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.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/__init__.py

@@ -0,0 +1,107 @@
+"""
+=============================================
+Integration and ODEs (:mod:`scipy.integrate`)
+=============================================
+
+.. currentmodule:: scipy.integrate
+
+Integrating functions, given function object
+============================================
+
+.. autosummary::
+   :toctree: generated/
+
+   quad          -- General purpose integration
+   quad_vec      -- General purpose integration of vector-valued functions
+   dblquad       -- General purpose double integration
+   tplquad       -- General purpose triple integration
+   nquad         -- General purpose N-D integration
+   fixed_quad    -- Integrate func(x) using Gaussian quadrature of order n
+   quadrature    -- Integrate with given tolerance using Gaussian quadrature
+   romberg       -- Integrate func using Romberg integration
+   newton_cotes  -- Weights and error coefficient for Newton-Cotes integration
+   IntegrationWarning -- Warning on issues during integration
+   AccuracyWarning  -- Warning on issues during quadrature integration
+
+Integrating functions, given fixed samples
+==========================================
+
+.. autosummary::
+   :toctree: generated/
+
+   trapezoid            -- Use trapezoidal rule to compute integral.
+   cumulative_trapezoid -- Use trapezoidal rule to cumulatively compute integral.
+   simpson              -- Use Simpson's rule to compute integral from samples.
+   romb                 -- Use Romberg Integration to compute integral from
+                        -- (2**k + 1) evenly-spaced samples.
+
+.. seealso::
+
+   :mod:`scipy.special` for orthogonal polynomials (special) for Gaussian
+   quadrature roots and weights for other weighting factors and regions.
+
+Solving initial value problems for ODE systems
+==============================================
+
+The solvers are implemented as individual classes, which can be used directly
+(low-level usage) or through a convenience function.
+
+.. autosummary::
+   :toctree: generated/
+
+   solve_ivp     -- Convenient function for ODE integration.
+   RK23          -- Explicit Runge-Kutta solver of order 3(2).
+   RK45          -- Explicit Runge-Kutta solver of order 5(4).
+   DOP853        -- Explicit Runge-Kutta solver of order 8.
+   Radau         -- Implicit Runge-Kutta solver of order 5.
+   BDF           -- Implicit multi-step variable order (1 to 5) solver.
+   LSODA         -- LSODA solver from ODEPACK Fortran package.
+   OdeSolver     -- Base class for ODE solvers.
+   DenseOutput   -- Local interpolant for computing a dense output.
+   OdeSolution   -- Class which represents a continuous ODE solution.
+
+
+Old API
+-------
+
+These are the routines developed earlier for SciPy. They wrap older solvers
+implemented in Fortran (mostly ODEPACK). While the interface to them is not
+particularly convenient and certain features are missing compared to the new
+API, the solvers themselves are of good quality and work fast as compiled
+Fortran code. In some cases, it might be worth using this old API.
+
+.. autosummary::
+   :toctree: generated/
+
+   odeint        -- General integration of ordinary differential equations.
+   ode           -- Integrate ODE using VODE and ZVODE routines.
+   complex_ode   -- Convert a complex-valued ODE to real-valued and integrate.
+
+
+Solving boundary value problems for ODE systems
+===============================================
+
+.. autosummary::
+   :toctree: generated/
+
+   solve_bvp     -- Solve a boundary value problem for a system of ODEs.
+"""  # noqa: E501
+
+
+from ._quadrature import *
+from ._odepack_py import *
+from ._quadpack_py import *
+from ._ode import *
+from ._bvp import solve_bvp
+from ._ivp import (solve_ivp, OdeSolution, DenseOutput,
+                   OdeSolver, RK23, RK45, DOP853, Radau, BDF, LSODA)
+from ._quad_vec import quad_vec
+
+# Deprecated namespaces, to be removed in v2.0.0
+from . import dop, lsoda, vode, odepack, quadpack
+
+__all__ = [s for s in dir() if not s.startswith('_')]
+
+from scipy._lib._testutils import PytestTester
+test = PytestTester(__name__)
+del PytestTester

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/_ivp/__init__.py

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+"""Suite of ODE solvers implemented in Python."""
+from .ivp import solve_ivp
+from .rk import RK23, RK45, DOP853
+from .radau import Radau
+from .bdf import BDF
+from .lsoda import LSODA
+from .common import OdeSolution
+from .base import DenseOutput, OdeSolver

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/_ivp/base.py

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+import numpy as np
+
+
+def check_arguments(fun, y0, support_complex):
+    """Helper function for checking arguments common to all solvers."""
+    y0 = np.asarray(y0)
+    if np.issubdtype(y0.dtype, np.complexfloating):
+        if not support_complex:
+            raise ValueError("`y0` is complex, but the chosen solver does "
+                             "not support integration in a complex domain.")
+        dtype = complex
+    else:
+        dtype = float
+    y0 = y0.astype(dtype, copy=False)
+
+    if y0.ndim != 1:
+        raise ValueError("`y0` must be 1-dimensional.")
+
+    def fun_wrapped(t, y):
+        return np.asarray(fun(t, y), dtype=dtype)
+
+    return fun_wrapped, y0
+
+
+class OdeSolver:
+    """Base class for ODE solvers.
+
+    In order to implement a new solver you need to follow the guidelines:
+
+        1. A constructor must accept parameters presented in the base class
+           (listed below) along with any other parameters specific to a solver.
+        2. A constructor must accept arbitrary extraneous arguments
+           ``**extraneous``, but warn that these arguments are irrelevant
+           using `common.warn_extraneous` function. Do not pass these
+           arguments to the base class.
+        3. A solver must implement a private method `_step_impl(self)` which
+           propagates a solver one step further. It must return tuple
+           ``(success, message)``, where ``success`` is a boolean indicating
+           whether a step was successful, and ``message`` is a string
+           containing description of a failure if a step failed or None
+           otherwise.
+        4. A solver must implement a private method `_dense_output_impl(self)`,
+           which returns a `DenseOutput` object covering the last successful
+           step.
+        5. A solver must have attributes listed below in Attributes section.
+           Note that ``t_old`` and ``step_size`` are updated automatically.
+        6. Use `fun(self, t, y)` method for the system rhs evaluation, this
+           way the number of function evaluations (`nfev`) will be tracked
+           automatically.
+        7. For convenience, a base class provides `fun_single(self, t, y)` and
+           `fun_vectorized(self, t, y)` for evaluating the rhs in
+           non-vectorized and vectorized fashions respectively (regardless of
+           how `fun` from the constructor is implemented). These calls don't
+           increment `nfev`.
+        8. If a solver uses a Jacobian matrix and LU decompositions, it should
+           track the number of Jacobian evaluations (`njev`) and the number of
+           LU decompositions (`nlu`).
+        9. By convention, the function evaluations used to compute a finite
+           difference approximation of the Jacobian should not be counted in
+           `nfev`, thus use `fun_single(self, t, y)` or
+           `fun_vectorized(self, t, y)` when computing a finite difference
+           approximation of the Jacobian.
+
+    Parameters
+    ----------
+    fun : callable
+        Right-hand side of the system. The calling signature is ``fun(t, y)``.
+        Here ``t`` is a scalar and there are two options for ndarray ``y``.
+        It can either have shape (n,), then ``fun`` must return array_like with
+        shape (n,). Or, alternatively, it can have shape (n, n_points), then
+        ``fun`` must return array_like with shape (n, n_points) (each column
+        corresponds to a single column in ``y``). The choice between the two
+        options is determined by `vectorized` argument (see below).
+    t0 : float
+        Initial time.
+    y0 : array_like, shape (n,)
+        Initial state.
+    t_bound : float
+        Boundary time --- the integration won't continue beyond it. It also
+        determines the direction of the integration.
+    vectorized : bool
+        Whether `fun` is implemented in a vectorized fashion.
+    support_complex : bool, optional
+        Whether integration in a complex domain should be supported.
+        Generally determined by a derived solver class capabilities.
+        Default is False.
+
+    Attributes
+    ----------
+    n : int
+        Number of equations.
+    status : string
+        Current status of the solver: 'running', 'finished' or 'failed'.
+    t_bound : float
+        Boundary time.
+    direction : float
+        Integration direction: +1 or -1.
+    t : float
+        Current time.
+    y : ndarray
+        Current state.
+    t_old : float
+        Previous time. None if no steps were made yet.
+    step_size : float
+        Size of the last successful step. None if no steps were made yet.
+    nfev : int
+        Number of the system's rhs evaluations.
+    njev : int
+        Number of the Jacobian evaluations.
+    nlu : int
+        Number of LU decompositions.
+    """
+    TOO_SMALL_STEP = "Required step size is less than spacing between numbers."
+
+    def __init__(self, fun, t0, y0, t_bound, vectorized,
+                 support_complex=False):
+        self.t_old = None
+        self.t = t0
+        self._fun, self.y = check_arguments(fun, y0, support_complex)
+        self.t_bound = t_bound
+        self.vectorized = vectorized
+
+        if vectorized:
+            def fun_single(t, y):
+                return self._fun(t, y[:, None]).ravel()
+            fun_vectorized = self._fun
+        else:
+            fun_single = self._fun
+
+            def fun_vectorized(t, y):
+                f = np.empty_like(y)
+                for i, yi in enumerate(y.T):
+                    f[:, i] = self._fun(t, yi)
+                return f
+
+        def fun(t, y):
+            self.nfev += 1
+            return self.fun_single(t, y)
+
+        self.fun = fun
+        self.fun_single = fun_single
+        self.fun_vectorized = fun_vectorized
+
+        self.direction = np.sign(t_bound - t0) if t_bound != t0 else 1
+        self.n = self.y.size
+        self.status = 'running'
+
+        self.nfev = 0
+        self.njev = 0
+        self.nlu = 0
+
+    @property
+    def step_size(self):
+        if self.t_old is None:
+            return None
+        else:
+            return np.abs(self.t - self.t_old)
+
+    def step(self):
+        """Perform one integration step.
+
+        Returns
+        -------
+        message : string or None
+            Report from the solver. Typically a reason for a failure if
+            `self.status` is 'failed' after the step was taken or None
+            otherwise.
+        """
+        if self.status != 'running':
+            raise RuntimeError("Attempt to step on a failed or finished "
+                               "solver.")
+
+        if self.n == 0 or self.t == self.t_bound:
+            # Handle corner cases of empty solver or no integration.
+            self.t_old = self.t
+            self.t = self.t_bound
+            message = None
+            self.status = 'finished'
+        else:
+            t = self.t
+            success, message = self._step_impl()
+
+            if not success:
+                self.status = 'failed'
+            else:
+                self.t_old = t
+                if self.direction * (self.t - self.t_bound) >= 0:
+                    self.status = 'finished'
+
+        return message
+
+    def dense_output(self):
+        """Compute a local interpolant over the last successful step.
+
+        Returns
+        -------
+        sol : `DenseOutput`
+            Local interpolant over the last successful step.
+        """
+        if self.t_old is None:
+            raise RuntimeError("Dense output is available after a successful "
+                               "step was made.")
+
+        if self.n == 0 or self.t == self.t_old:
+            # Handle corner cases of empty solver and no integration.
+            return ConstantDenseOutput(self.t_old, self.t, self.y)
+        else:
+            return self._dense_output_impl()
+
+    def _step_impl(self):
+        raise NotImplementedError
+
+    def _dense_output_impl(self):
+        raise NotImplementedError
+
+
+class DenseOutput:
+    """Base class for local interpolant over step made by an ODE solver.
+
+    It interpolates between `t_min` and `t_max` (see Attributes below).
+    Evaluation outside this interval is not forbidden, but the accuracy is not
+    guaranteed.
+
+    Attributes
+    ----------
+    t_min, t_max : float
+        Time range of the interpolation.
+    """
+    def __init__(self, t_old, t):
+        self.t_old = t_old
+        self.t = t
+        self.t_min = min(t, t_old)
+        self.t_max = max(t, t_old)
+
+    def __call__(self, t):
+        """Evaluate the interpolant.
+
+        Parameters
+        ----------
+        t : float or array_like with shape (n_points,)
+            Points to evaluate the solution at.
+
+        Returns
+        -------
+        y : ndarray, shape (n,) or (n, n_points)
+            Computed values. Shape depends on whether `t` was a scalar or a
+            1-D array.
+        """
+        t = np.asarray(t)
+        if t.ndim > 1:
+            raise ValueError("`t` must be a float or a 1-D array.")
+        return self._call_impl(t)
+
+    def _call_impl(self, t):
+        raise NotImplementedError
+
+
+class ConstantDenseOutput(DenseOutput):
+    """Constant value interpolator.
+
+    This class used for degenerate integration cases: equal integration limits
+    or a system with 0 equations.
+    """
+    def __init__(self, t_old, t, value):
+        super().__init__(t_old, t)
+        self.value = value
+
+    def _call_impl(self, t):
+        if t.ndim == 0:
+            return self.value
+        else:
+            ret = np.empty((self.value.shape[0], t.shape[0]))
+            ret[:] = self.value[:, None]
+            return ret

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/_ivp/bdf.py

@@ -0,0 +1,470 @@
+import numpy as np
+from scipy.linalg import lu_factor, lu_solve
+from scipy.sparse import issparse, csc_matrix, eye
+from scipy.sparse.linalg import splu
+from scipy.optimize._numdiff import group_columns
+from .common import (validate_max_step, validate_tol, select_initial_step,
+                     norm, EPS, num_jac, validate_first_step,
+                     warn_extraneous)
+from .base import OdeSolver, DenseOutput
+
+
+MAX_ORDER = 5
+NEWTON_MAXITER = 4
+MIN_FACTOR = 0.2
+MAX_FACTOR = 10
+
+
+def compute_R(order, factor):
+    """Compute the matrix for changing the differences array."""
+    I = np.arange(1, order + 1)[:, None]
+    J = np.arange(1, order + 1)
+    M = np.zeros((order + 1, order + 1))
+    M[1:, 1:] = (I - 1 - factor * J) / I
+    M[0] = 1
+    return np.cumprod(M, axis=0)
+
+
+def change_D(D, order, factor):
+    """Change differences array in-place when step size is changed."""
+    R = compute_R(order, factor)
+    U = compute_R(order, 1)
+    RU = R.dot(U)
+    D[:order + 1] = np.dot(RU.T, D[:order + 1])
+
+
+def solve_bdf_system(fun, t_new, y_predict, c, psi, LU, solve_lu, scale, tol):
+    """Solve the algebraic system resulting from BDF method."""
+    d = 0
+    y = y_predict.copy()
+    dy_norm_old = None
+    converged = False
+    for k in range(NEWTON_MAXITER):
+        f = fun(t_new, y)
+        if not np.all(np.isfinite(f)):
+            break
+
+        dy = solve_lu(LU, c * f - psi - d)
+        dy_norm = norm(dy / scale)
+
+        if dy_norm_old is None:
+            rate = None
+        else:
+            rate = dy_norm / dy_norm_old
+
+        if (rate is not None and (rate >= 1 or
+                rate ** (NEWTON_MAXITER - k) / (1 - rate) * dy_norm > tol)):
+            break
+
+        y += dy
+        d += dy
+
+        if (dy_norm == 0 or
+                rate is not None and rate / (1 - rate) * dy_norm < tol):
+            converged = True
+            break
+
+        dy_norm_old = dy_norm
+
+    return converged, k + 1, y, d
+
+
+class BDF(OdeSolver):
+    """Implicit method based on backward-differentiation formulas.
+
+    This is a variable order method with the order varying automatically from
+    1 to 5. The general framework of the BDF algorithm is described in [1]_.
+    This class implements a quasi-constant step size as explained in [2]_.
+    The error estimation strategy for the constant-step BDF is derived in [3]_.
+    An accuracy enhancement using modified formulas (NDF) [2]_ is also implemented.
+
+    Can be applied in the complex domain.
+
+    Parameters
+    ----------
+    fun : callable
+        Right-hand side of the system. The calling signature is ``fun(t, y)``.
+        Here ``t`` is a scalar, and there are two options for the ndarray ``y``:
+        It can either have shape (n,); then ``fun`` must return array_like with
+        shape (n,). Alternatively it can have shape (n, k); then ``fun``
+        must return an array_like with shape (n, k), i.e. each column
+        corresponds to a single column in ``y``. The choice between the two
+        options is determined by `vectorized` argument (see below). The
+        vectorized implementation allows a faster approximation of the Jacobian
+        by finite differences (required for this solver).
+    t0 : float
+        Initial time.
+    y0 : array_like, shape (n,)
+        Initial state.
+    t_bound : float
+        Boundary time - the integration won't continue beyond it. It also
+        determines the direction of the integration.
+    first_step : float or None, optional
+        Initial step size. Default is ``None`` which means that the algorithm
+        should choose.
+    max_step : float, optional
+        Maximum allowed step size. Default is np.inf, i.e., the step size is not
+        bounded and determined solely by the solver.
+    rtol, atol : float and array_like, optional
+        Relative and absolute tolerances. The solver keeps the local error
+        estimates less than ``atol + rtol * abs(y)``. Here `rtol` controls a
+        relative accuracy (number of correct digits), while `atol` controls
+        absolute accuracy (number of correct decimal places). To achieve the
+        desired `rtol`, set `atol` to be smaller than the smallest value that
+        can be expected from ``rtol * abs(y)`` so that `rtol` dominates the
+        allowable error. If `atol` is larger than ``rtol * abs(y)`` the
+        number of correct digits is not guaranteed. Conversely, to achieve the
+        desired `atol` set `rtol` such that ``rtol * abs(y)`` is always smaller
+        than `atol`. If components of y have different scales, it might be
+        beneficial to set different `atol` values for different components by
+        passing array_like with shape (n,) for `atol`. Default values are
+        1e-3 for `rtol` and 1e-6 for `atol`.
+    jac : {None, array_like, sparse_matrix, callable}, optional
+        Jacobian matrix of the right-hand side of the system with respect to y,
+        required by this method. The Jacobian matrix has shape (n, n) and its
+        element (i, j) is equal to ``d f_i / d y_j``.
+        There are three ways to define the Jacobian:
+
+            * If array_like or sparse_matrix, the Jacobian is assumed to
+              be constant.
+            * If callable, the Jacobian is assumed to depend on both
+              t and y; it will be called as ``jac(t, y)`` as necessary.
+              For the 'Radau' and 'BDF' methods, the return value might be a
+              sparse matrix.
+            * If None (default), the Jacobian will be approximated by
+              finite differences.
+
+        It is generally recommended to provide the Jacobian rather than
+        relying on a finite-difference approximation.
+    jac_sparsity : {None, array_like, sparse matrix}, optional
+        Defines a sparsity structure of the Jacobian matrix for a
+        finite-difference approximation. Its shape must be (n, n). This argument
+        is ignored if `jac` is not `None`. If the Jacobian has only few non-zero
+        elements in *each* row, providing the sparsity structure will greatly
+        speed up the computations [4]_. A zero entry means that a corresponding
+        element in the Jacobian is always zero. If None (default), the Jacobian
+        is assumed to be dense.
+    vectorized : bool, optional
+        Whether `fun` is implemented in a vectorized fashion. Default is False.
+
+    Attributes
+    ----------
+    n : int
+        Number of equations.
+    status : string
+        Current status of the solver: 'running', 'finished' or 'failed'.
+    t_bound : float
+        Boundary time.
+    direction : float
+        Integration direction: +1 or -1.
+    t : float
+        Current time.
+    y : ndarray
+        Current state.
+    t_old : float
+        Previous time. None if no steps were made yet.
+    step_size : float
+        Size of the last successful step. None if no steps were made yet.
+    nfev : int
+        Number of evaluations of the right-hand side.
+    njev : int
+        Number of evaluations of the Jacobian.
+    nlu : int
+        Number of LU decompositions.
+
+    References
+    ----------
+    .. [1] G. D. Byrne, A. C. Hindmarsh, "A Polyalgorithm for the Numerical
+           Solution of Ordinary Differential Equations", ACM Transactions on
+           Mathematical Software, Vol. 1, No. 1, pp. 71-96, March 1975.
+    .. [2] L. F. Shampine, M. W. Reichelt, "THE MATLAB ODE SUITE", SIAM J. SCI.
+           COMPUTE., Vol. 18, No. 1, pp. 1-22, January 1997.
+    .. [3] E. Hairer, G. Wanner, "Solving Ordinary Differential Equations I:
+           Nonstiff Problems", Sec. III.2.
+    .. [4] A. Curtis, M. J. D. Powell, and J. Reid, "On the estimation of
+           sparse Jacobian matrices", Journal of the Institute of Mathematics
+           and its Applications, 13, pp. 117-120, 1974.
+    """
+    def __init__(self, fun, t0, y0, t_bound, max_step=np.inf,
+                 rtol=1e-3, atol=1e-6, jac=None, jac_sparsity=None,
+                 vectorized=False, first_step=None, **extraneous):
+        warn_extraneous(extraneous)
+        super().__init__(fun, t0, y0, t_bound, vectorized,
+                         support_complex=True)
+        self.max_step = validate_max_step(max_step)
+        self.rtol, self.atol = validate_tol(rtol, atol, self.n)
+        f = self.fun(self.t, self.y)
+        if first_step is None:
+            self.h_abs = select_initial_step(self.fun, self.t, self.y, f,
+                                             self.direction, 1,
+                                             self.rtol, self.atol)
+        else:
+            self.h_abs = validate_first_step(first_step, t0, t_bound)
+        self.h_abs_old = None
+        self.error_norm_old = None
+
+        self.newton_tol = max(10 * EPS / rtol, min(0.03, rtol ** 0.5))
+
+        self.jac_factor = None
+        self.jac, self.J = self._validate_jac(jac, jac_sparsity)
+        if issparse(self.J):
+            def lu(A):
+                self.nlu += 1
+                return splu(A)
+
+            def solve_lu(LU, b):
+                return LU.solve(b)
+
+            I = eye(self.n, format='csc', dtype=self.y.dtype)
+        else:
+            def lu(A):
+                self.nlu += 1
+                return lu_factor(A, overwrite_a=True)
+
+            def solve_lu(LU, b):
+                return lu_solve(LU, b, overwrite_b=True)
+
+            I = np.identity(self.n, dtype=self.y.dtype)
+
+        self.lu = lu
+        self.solve_lu = solve_lu
+        self.I = I
+
+        kappa = np.array([0, -0.1850, -1/9, -0.0823, -0.0415, 0])
+        self.gamma = np.hstack((0, np.cumsum(1 / np.arange(1, MAX_ORDER + 1))))
+        self.alpha = (1 - kappa) * self.gamma
+        self.error_const = kappa * self.gamma + 1 / np.arange(1, MAX_ORDER + 2)
+
+        D = np.empty((MAX_ORDER + 3, self.n), dtype=self.y.dtype)
+        D[0] = self.y
+        D[1] = f * self.h_abs * self.direction
+        self.D = D
+
+        self.order = 1
+        self.n_equal_steps = 0
+        self.LU = None
+
+    def _validate_jac(self, jac, sparsity):
+        t0 = self.t
+        y0 = self.y
+
+        if jac is None:
+            if sparsity is not None:
+                if issparse(sparsity):
+                    sparsity = csc_matrix(sparsity)
+                groups = group_columns(sparsity)
+                sparsity = (sparsity, groups)
+
+            def jac_wrapped(t, y):
+                self.njev += 1
+                f = self.fun_single(t, y)
+                J, self.jac_factor = num_jac(self.fun_vectorized, t, y, f,
+                                             self.atol, self.jac_factor,
+                                             sparsity)
+                return J
+            J = jac_wrapped(t0, y0)
+        elif callable(jac):
+            J = jac(t0, y0)
+            self.njev += 1
+            if issparse(J):
+                J = csc_matrix(J, dtype=y0.dtype)
+
+                def jac_wrapped(t, y):
+                    self.njev += 1
+                    return csc_matrix(jac(t, y), dtype=y0.dtype)
+            else:
+                J = np.asarray(J, dtype=y0.dtype)
+
+                def jac_wrapped(t, y):
+                    self.njev += 1
+                    return np.asarray(jac(t, y), dtype=y0.dtype)
+
+            if J.shape != (self.n, self.n):
+                raise ValueError("`jac` is expected to have shape {}, but "
+                                 "actually has {}."
+                                 .format((self.n, self.n), J.shape))
+        else:
+            if issparse(jac):
+                J = csc_matrix(jac, dtype=y0.dtype)
+            else:
+                J = np.asarray(jac, dtype=y0.dtype)
+
+            if J.shape != (self.n, self.n):
+                raise ValueError("`jac` is expected to have shape {}, but "
+                                 "actually has {}."
+                                 .format((self.n, self.n), J.shape))
+            jac_wrapped = None
+
+        return jac_wrapped, J
+
+    def _step_impl(self):
+        t = self.t
+        D = self.D
+
+        max_step = self.max_step
+        min_step = 10 * np.abs(np.nextafter(t, self.direction * np.inf) - t)
+        if self.h_abs > max_step:
+            h_abs = max_step
+            change_D(D, self.order, max_step / self.h_abs)
+            self.n_equal_steps = 0
+        elif self.h_abs < min_step:
+            h_abs = min_step
+            change_D(D, self.order, min_step / self.h_abs)
+            self.n_equal_steps = 0
+        else:
+            h_abs = self.h_abs
+
+        atol = self.atol
+        rtol = self.rtol
+        order = self.order
+
+        alpha = self.alpha
+        gamma = self.gamma
+        error_const = self.error_const
+
+        J = self.J
+        LU = self.LU
+        current_jac = self.jac is None
+
+        step_accepted = False
+        while not step_accepted:
+            if h_abs < min_step:
+                return False, self.TOO_SMALL_STEP
+
+            h = h_abs * self.direction
+            t_new = t + h
+
+            if self.direction * (t_new - self.t_bound) > 0:
+                t_new = self.t_bound
+                change_D(D, order, np.abs(t_new - t) / h_abs)
+                self.n_equal_steps = 0
+                LU = None
+
+            h = t_new - t
+            h_abs = np.abs(h)
+
+            y_predict = np.sum(D[:order + 1], axis=0)
+
+            scale = atol + rtol * np.abs(y_predict)
+            psi = np.dot(D[1: order + 1].T, gamma[1: order + 1]) / alpha[order]
+
+            converged = False
+            c = h / alpha[order]
+            while not converged:
+                if LU is None:
+                    LU = self.lu(self.I - c * J)
+
+                converged, n_iter, y_new, d = solve_bdf_system(
+                    self.fun, t_new, y_predict, c, psi, LU, self.solve_lu,
+                    scale, self.newton_tol)
+
+                if not converged:
+                    if current_jac:
+                        break
+                    J = self.jac(t_new, y_predict)
+                    LU = None
+                    current_jac = True
+
+            if not converged:
+                factor = 0.5
+                h_abs *= factor
+                change_D(D, order, factor)
+                self.n_equal_steps = 0
+                LU = None
+                continue
+
+            safety = 0.9 * (2 * NEWTON_MAXITER + 1) / (2 * NEWTON_MAXITER
+                                                       + n_iter)
+
+            scale = atol + rtol * np.abs(y_new)
+            error = error_const[order] * d
+            error_norm = norm(error / scale)
+
+            if error_norm > 1:
+                factor = max(MIN_FACTOR,
+                             safety * error_norm ** (-1 / (order + 1)))
+                h_abs *= factor
+                change_D(D, order, factor)
+                self.n_equal_steps = 0
+                # As we didn't have problems with convergence, we don't
+                # reset LU here.
+            else:
+                step_accepted = True
+
+        self.n_equal_steps += 1
+
+        self.t = t_new
+        self.y = y_new
+
+        self.h_abs = h_abs
+        self.J = J
+        self.LU = LU
+
+        # Update differences. The principal relation here is
+        # D^{j + 1} y_n = D^{j} y_n - D^{j} y_{n - 1}. Keep in mind that D
+        # contained difference for previous interpolating polynomial and
+        # d = D^{k + 1} y_n. Thus this elegant code follows.
+        D[order + 2] = d - D[order + 1]
+        D[order + 1] = d
+        for i in reversed(range(order + 1)):
+            D[i] += D[i + 1]
+
+        if self.n_equal_steps < order + 1:
+            return True, None
+
+        if order > 1:
+            error_m = error_const[order - 1] * D[order]
+            error_m_norm = norm(error_m / scale)
+        else:
+            error_m_norm = np.inf
+
+        if order < MAX_ORDER:
+            error_p = error_const[order + 1] * D[order + 2]
+            error_p_norm = norm(error_p / scale)
+        else:
+            error_p_norm = np.inf
+
+        error_norms = np.array([error_m_norm, error_norm, error_p_norm])
+        with np.errstate(divide='ignore'):
+            factors = error_norms ** (-1 / np.arange(order, order + 3))
+
+        delta_order = np.argmax(factors) - 1
+        order += delta_order
+        self.order = order
+
+        factor = min(MAX_FACTOR, safety * np.max(factors))
+        self.h_abs *= factor
+        change_D(D, order, factor)
+        self.n_equal_steps = 0
+        self.LU = None
+
+        return True, None
+
+    def _dense_output_impl(self):
+        return BdfDenseOutput(self.t_old, self.t, self.h_abs * self.direction,
+                              self.order, self.D[:self.order + 1].copy())
+
+
+class BdfDenseOutput(DenseOutput):
+    def __init__(self, t_old, t, h, order, D):
+        super().__init__(t_old, t)
+        self.order = order
+        self.t_shift = self.t - h * np.arange(self.order)
+        self.denom = h * (1 + np.arange(self.order))
+        self.D = D
+
+    def _call_impl(self, t):
+        if t.ndim == 0:
+            x = (t - self.t_shift) / self.denom
+            p = np.cumprod(x)
+        else:
+            x = (t - self.t_shift[:, None]) / self.denom[:, None]
+            p = np.cumprod(x, axis=0)
+
+        y = np.dot(self.D[1:].T, p)
+        if y.ndim == 1:
+            y += self.D[0]
+        else:
+            y += self.D[0, :, None]
+
+        return y

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/_ivp/common.py

@@ -0,0 +1,433 @@
+from itertools import groupby
+from warnings import warn
+import numpy as np
+from scipy.sparse import find, coo_matrix
+
+
+EPS = np.finfo(float).eps
+
+
+def validate_first_step(first_step, t0, t_bound):
+    """Assert that first_step is valid and return it."""
+    if first_step <= 0:
+        raise ValueError("`first_step` must be positive.")
+    if first_step > np.abs(t_bound - t0):
+        raise ValueError("`first_step` exceeds bounds.")
+    return first_step
+
+
+def validate_max_step(max_step):
+    """Assert that max_Step is valid and return it."""
+    if max_step <= 0:
+        raise ValueError("`max_step` must be positive.")
+    return max_step
+
+
+def warn_extraneous(extraneous):
+    """Display a warning for extraneous keyword arguments.
+
+    The initializer of each solver class is expected to collect keyword
+    arguments that it doesn't understand and warn about them. This function
+    prints a warning for each key in the supplied dictionary.
+
+    Parameters
+    ----------
+    extraneous : dict
+        Extraneous keyword arguments
+    """
+    if extraneous:
+        warn("The following arguments have no effect for a chosen solver: {}."
+             .format(", ".join("`{}`".format(x) for x in extraneous)))
+
+
+def validate_tol(rtol, atol, n):
+    """Validate tolerance values."""
+
+    if np.any(rtol < 100 * EPS):
+        warn("At least one element of `rtol` is too small. "
+             f"Setting `rtol = np.maximum(rtol, {100 * EPS})`.")
+        rtol = np.maximum(rtol, 100 * EPS)
+
+    atol = np.asarray(atol)
+    if atol.ndim > 0 and atol.shape != (n,):
+        raise ValueError("`atol` has wrong shape.")
+
+    if np.any(atol < 0):
+        raise ValueError("`atol` must be positive.")
+
+    return rtol, atol
+
+
+def norm(x):
+    """Compute RMS norm."""
+    return np.linalg.norm(x) / x.size ** 0.5
+
+
+def select_initial_step(fun, t0, y0, f0, direction, order, rtol, atol):
+    """Empirically select a good initial step.
+
+    The algorithm is described in [1]_.
+
+    Parameters
+    ----------
+    fun : callable
+        Right-hand side of the system.
+    t0 : float
+        Initial value of the independent variable.
+    y0 : ndarray, shape (n,)
+        Initial value of the dependent variable.
+    f0 : ndarray, shape (n,)
+        Initial value of the derivative, i.e., ``fun(t0, y0)``.
+    direction : float
+        Integration direction.
+    order : float
+        Error estimator order. It means that the error controlled by the
+        algorithm is proportional to ``step_size ** (order + 1)`.
+    rtol : float
+        Desired relative tolerance.
+    atol : float
+        Desired absolute tolerance.
+
+    Returns
+    -------
+    h_abs : float
+        Absolute value of the suggested initial step.
+
+    References
+    ----------
+    .. [1] E. Hairer, S. P. Norsett G. Wanner, "Solving Ordinary Differential
+           Equations I: Nonstiff Problems", Sec. II.4.
+    """
+    if y0.size == 0:
+        return np.inf
+
+    scale = atol + np.abs(y0) * rtol
+    d0 = norm(y0 / scale)
+    d1 = norm(f0 / scale)
+    if d0 < 1e-5 or d1 < 1e-5:
+        h0 = 1e-6
+    else:
+        h0 = 0.01 * d0 / d1
+
+    y1 = y0 + h0 * direction * f0
+    f1 = fun(t0 + h0 * direction, y1)
+    d2 = norm((f1 - f0) / scale) / h0
+
+    if d1 <= 1e-15 and d2 <= 1e-15:
+        h1 = max(1e-6, h0 * 1e-3)
+    else:
+        h1 = (0.01 / max(d1, d2)) ** (1 / (order + 1))
+
+    return min(100 * h0, h1)
+
+
+class OdeSolution:
+    """Continuous ODE solution.
+
+    It is organized as a collection of `DenseOutput` objects which represent
+    local interpolants. It provides an algorithm to select a right interpolant
+    for each given point.
+
+    The interpolants cover the range between `t_min` and `t_max` (see
+    Attributes below). Evaluation outside this interval is not forbidden, but
+    the accuracy is not guaranteed.
+
+    When evaluating at a breakpoint (one of the values in `ts`) a segment with
+    the lower index is selected.
+
+    Parameters
+    ----------
+    ts : array_like, shape (n_segments + 1,)
+        Time instants between which local interpolants are defined. Must
+        be strictly increasing or decreasing (zero segment with two points is
+        also allowed).
+    interpolants : list of DenseOutput with n_segments elements
+        Local interpolants. An i-th interpolant is assumed to be defined
+        between ``ts[i]`` and ``ts[i + 1]``.
+
+    Attributes
+    ----------
+    t_min, t_max : float
+        Time range of the interpolation.
+    """
+    def __init__(self, ts, interpolants):
+        ts = np.asarray(ts)
+        d = np.diff(ts)
+        # The first case covers integration on zero segment.
+        if not ((ts.size == 2 and ts[0] == ts[-1])
+                or np.all(d > 0) or np.all(d < 0)):
+            raise ValueError("`ts` must be strictly increasing or decreasing.")
+
+        self.n_segments = len(interpolants)
+        if ts.shape != (self.n_segments + 1,):
+            raise ValueError("Numbers of time stamps and interpolants "
+                             "don't match.")
+
+        self.ts = ts
+        self.interpolants = interpolants
+        if ts[-1] >= ts[0]:
+            self.t_min = ts[0]
+            self.t_max = ts[-1]
+            self.ascending = True
+            self.ts_sorted = ts
+        else:
+            self.t_min = ts[-1]
+            self.t_max = ts[0]
+            self.ascending = False
+            self.ts_sorted = ts[::-1]
+
+    def _call_single(self, t):
+        # Here we preserve a certain symmetry that when t is in self.ts,
+        # then we prioritize a segment with a lower index.
+        if self.ascending:
+            ind = np.searchsorted(self.ts_sorted, t, side='left')
+        else:
+            ind = np.searchsorted(self.ts_sorted, t, side='right')
+
+        segment = min(max(ind - 1, 0), self.n_segments - 1)
+        if not self.ascending:
+            segment = self.n_segments - 1 - segment
+
+        return self.interpolants[segment](t)
+
+    def __call__(self, t):
+        """Evaluate the solution.
+
+        Parameters
+        ----------
+        t : float or array_like with shape (n_points,)
+            Points to evaluate at.
+
+        Returns
+        -------
+        y : ndarray, shape (n_states,) or (n_states, n_points)
+            Computed values. Shape depends on whether `t` is a scalar or a
+            1-D array.
+        """
+        t = np.asarray(t)
+
+        if t.ndim == 0:
+            return self._call_single(t)
+
+        order = np.argsort(t)
+        reverse = np.empty_like(order)
+        reverse[order] = np.arange(order.shape[0])
+        t_sorted = t[order]
+
+        # See comment in self._call_single.
+        if self.ascending:
+            segments = np.searchsorted(self.ts_sorted, t_sorted, side='left')
+        else:
+            segments = np.searchsorted(self.ts_sorted, t_sorted, side='right')
+        segments -= 1
+        segments[segments < 0] = 0
+        segments[segments > self.n_segments - 1] = self.n_segments - 1
+        if not self.ascending:
+            segments = self.n_segments - 1 - segments
+
+        ys = []
+        group_start = 0
+        for segment, group in groupby(segments):
+            group_end = group_start + len(list(group))
+            y = self.interpolants[segment](t_sorted[group_start:group_end])
+            ys.append(y)
+            group_start = group_end
+
+        ys = np.hstack(ys)
+        ys = ys[:, reverse]
+
+        return ys
+
+
+NUM_JAC_DIFF_REJECT = EPS ** 0.875
+NUM_JAC_DIFF_SMALL = EPS ** 0.75
+NUM_JAC_DIFF_BIG = EPS ** 0.25
+NUM_JAC_MIN_FACTOR = 1e3 * EPS
+NUM_JAC_FACTOR_INCREASE = 10
+NUM_JAC_FACTOR_DECREASE = 0.1
+
+
+def num_jac(fun, t, y, f, threshold, factor, sparsity=None):
+    """Finite differences Jacobian approximation tailored for ODE solvers.
+
+    This function computes finite difference approximation to the Jacobian
+    matrix of `fun` with respect to `y` using forward differences.
+    The Jacobian matrix has shape (n, n) and its element (i, j) is equal to
+    ``d f_i / d y_j``.
+
+    A special feature of this function is the ability to correct the step
+    size from iteration to iteration. The main idea is to keep the finite
+    difference significantly separated from its round-off error which
+    approximately equals ``EPS * np.abs(f)``. It reduces a possibility of a
+    huge error and assures that the estimated derivative are reasonably close
+    to the true values (i.e., the finite difference approximation is at least
+    qualitatively reflects the structure of the true Jacobian).
+
+    Parameters
+    ----------
+    fun : callable
+        Right-hand side of the system implemented in a vectorized fashion.
+    t : float
+        Current time.
+    y : ndarray, shape (n,)
+        Current state.
+    f : ndarray, shape (n,)
+        Value of the right hand side at (t, y).
+    threshold : float
+        Threshold for `y` value used for computing the step size as
+        ``factor * np.maximum(np.abs(y), threshold)``. Typically, the value of
+        absolute tolerance (atol) for a solver should be passed as `threshold`.
+    factor : ndarray with shape (n,) or None
+        Factor to use for computing the step size. Pass None for the very
+        evaluation, then use the value returned from this function.
+    sparsity : tuple (structure, groups) or None
+        Sparsity structure of the Jacobian, `structure` must be csc_matrix.
+
+    Returns
+    -------
+    J : ndarray or csc_matrix, shape (n, n)
+        Jacobian matrix.
+    factor : ndarray, shape (n,)
+        Suggested `factor` for the next evaluation.
+    """
+    y = np.asarray(y)
+    n = y.shape[0]
+    if n == 0:
+        return np.empty((0, 0)), factor
+
+    if factor is None:
+        factor = np.full(n, EPS ** 0.5)
+    else:
+        factor = factor.copy()
+
+    # Direct the step as ODE dictates, hoping that such a step won't lead to
+    # a problematic region. For complex ODEs it makes sense to use the real
+    # part of f as we use steps along real axis.
+    f_sign = 2 * (np.real(f) >= 0).astype(float) - 1
+    y_scale = f_sign * np.maximum(threshold, np.abs(y))
+    h = (y + factor * y_scale) - y
+
+    # Make sure that the step is not 0 to start with. Not likely it will be
+    # executed often.
+    for i in np.nonzero(h == 0)[0]:
+        while h[i] == 0:
+            factor[i] *= 10
+            h[i] = (y[i] + factor[i] * y_scale[i]) - y[i]
+
+    if sparsity is None:
+        return _dense_num_jac(fun, t, y, f, h, factor, y_scale)
+    else:
+        structure, groups = sparsity
+        return _sparse_num_jac(fun, t, y, f, h, factor, y_scale,
+                               structure, groups)
+
+
+def _dense_num_jac(fun, t, y, f, h, factor, y_scale):
+    n = y.shape[0]
+    h_vecs = np.diag(h)
+    f_new = fun(t, y[:, None] + h_vecs)
+    diff = f_new - f[:, None]
+    max_ind = np.argmax(np.abs(diff), axis=0)
+    r = np.arange(n)
+    max_diff = np.abs(diff[max_ind, r])
+    scale = np.maximum(np.abs(f[max_ind]), np.abs(f_new[max_ind, r]))
+
+    diff_too_small = max_diff < NUM_JAC_DIFF_REJECT * scale
+    if np.any(diff_too_small):
+        ind, = np.nonzero(diff_too_small)
+        new_factor = NUM_JAC_FACTOR_INCREASE * factor[ind]
+        h_new = (y[ind] + new_factor * y_scale[ind]) - y[ind]
+        h_vecs[ind, ind] = h_new
+        f_new = fun(t, y[:, None] + h_vecs[:, ind])
+        diff_new = f_new - f[:, None]
+        max_ind = np.argmax(np.abs(diff_new), axis=0)
+        r = np.arange(ind.shape[0])
+        max_diff_new = np.abs(diff_new[max_ind, r])
+        scale_new = np.maximum(np.abs(f[max_ind]), np.abs(f_new[max_ind, r]))
+
+        update = max_diff[ind] * scale_new < max_diff_new * scale[ind]
+        if np.any(update):
+            update, = np.nonzero(update)
+            update_ind = ind[update]
+            factor[update_ind] = new_factor[update]
+            h[update_ind] = h_new[update]
+            diff[:, update_ind] = diff_new[:, update]
+            scale[update_ind] = scale_new[update]
+            max_diff[update_ind] = max_diff_new[update]
+
+    diff /= h
+
+    factor[max_diff < NUM_JAC_DIFF_SMALL * scale] *= NUM_JAC_FACTOR_INCREASE
+    factor[max_diff > NUM_JAC_DIFF_BIG * scale] *= NUM_JAC_FACTOR_DECREASE
+    factor = np.maximum(factor, NUM_JAC_MIN_FACTOR)
+
+    return diff, factor
+
+
+def _sparse_num_jac(fun, t, y, f, h, factor, y_scale, structure, groups):
+    n = y.shape[0]
+    n_groups = np.max(groups) + 1
+    h_vecs = np.empty((n_groups, n))
+    for group in range(n_groups):
+        e = np.equal(group, groups)
+        h_vecs[group] = h * e
+    h_vecs = h_vecs.T
+
+    f_new = fun(t, y[:, None] + h_vecs)
+    df = f_new - f[:, None]
+
+    i, j, _ = find(structure)
+    diff = coo_matrix((df[i, groups[j]], (i, j)), shape=(n, n)).tocsc()
+    max_ind = np.array(abs(diff).argmax(axis=0)).ravel()
+    r = np.arange(n)
+    max_diff = np.asarray(np.abs(diff[max_ind, r])).ravel()
+    scale = np.maximum(np.abs(f[max_ind]),
+                       np.abs(f_new[max_ind, groups[r]]))
+
+    diff_too_small = max_diff < NUM_JAC_DIFF_REJECT * scale
+    if np.any(diff_too_small):
+        ind, = np.nonzero(diff_too_small)
+        new_factor = NUM_JAC_FACTOR_INCREASE * factor[ind]
+        h_new = (y[ind] + new_factor * y_scale[ind]) - y[ind]
+        h_new_all = np.zeros(n)
+        h_new_all[ind] = h_new
+
+        groups_unique = np.unique(groups[ind])
+        groups_map = np.empty(n_groups, dtype=int)
+        h_vecs = np.empty((groups_unique.shape[0], n))
+        for k, group in enumerate(groups_unique):
+            e = np.equal(group, groups)
+            h_vecs[k] = h_new_all * e
+            groups_map[group] = k
+        h_vecs = h_vecs.T
+
+        f_new = fun(t, y[:, None] + h_vecs)
+        df = f_new - f[:, None]
+        i, j, _ = find(structure[:, ind])
+        diff_new = coo_matrix((df[i, groups_map[groups[ind[j]]]],
+                               (i, j)), shape=(n, ind.shape[0])).tocsc()
+
+        max_ind_new = np.array(abs(diff_new).argmax(axis=0)).ravel()
+        r = np.arange(ind.shape[0])
+        max_diff_new = np.asarray(np.abs(diff_new[max_ind_new, r])).ravel()
+        scale_new = np.maximum(
+            np.abs(f[max_ind_new]),
+            np.abs(f_new[max_ind_new, groups_map[groups[ind]]]))
+
+        update = max_diff[ind] * scale_new < max_diff_new * scale[ind]
+        if np.any(update):
+            update, = np.nonzero(update)
+            update_ind = ind[update]
+            factor[update_ind] = new_factor[update]
+            h[update_ind] = h_new[update]
+            diff[:, update_ind] = diff_new[:, update]
+            scale[update_ind] = scale_new[update]
+            max_diff[update_ind] = max_diff_new[update]
+
+    diff.data /= np.repeat(h, np.diff(diff.indptr))
+
+    factor[max_diff < NUM_JAC_DIFF_SMALL * scale] *= NUM_JAC_FACTOR_INCREASE
+    factor[max_diff > NUM_JAC_DIFF_BIG * scale] *= NUM_JAC_FACTOR_DECREASE
+    factor = np.maximum(factor, NUM_JAC_MIN_FACTOR)
+
+    return diff, factor

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/_ivp/dop853_coefficients.py

@@ -0,0 +1,193 @@
+import numpy as np
+
+N_STAGES = 12
+N_STAGES_EXTENDED = 16
+INTERPOLATOR_POWER = 7
+
+C = np.array([0.0,
+              0.526001519587677318785587544488e-01,
+              0.789002279381515978178381316732e-01,
+              0.118350341907227396726757197510,
+              0.281649658092772603273242802490,
+              0.333333333333333333333333333333,
+              0.25,
+              0.307692307692307692307692307692,
+              0.651282051282051282051282051282,
+              0.6,
+              0.857142857142857142857142857142,
+              1.0,
+              1.0,
+              0.1,
+              0.2,
+              0.777777777777777777777777777778])
+
+A = np.zeros((N_STAGES_EXTENDED, N_STAGES_EXTENDED))
+A[1, 0] = 5.26001519587677318785587544488e-2
+
+A[2, 0] = 1.97250569845378994544595329183e-2
+A[2, 1] = 5.91751709536136983633785987549e-2
+
+A[3, 0] = 2.95875854768068491816892993775e-2
+A[3, 2] = 8.87627564304205475450678981324e-2
+
+A[4, 0] = 2.41365134159266685502369798665e-1
+A[4, 2] = -8.84549479328286085344864962717e-1
+A[4, 3] = 9.24834003261792003115737966543e-1
+
+A[5, 0] = 3.7037037037037037037037037037e-2
+A[5, 3] = 1.70828608729473871279604482173e-1
+A[5, 4] = 1.25467687566822425016691814123e-1
+
+A[6, 0] = 3.7109375e-2
+A[6, 3] = 1.70252211019544039314978060272e-1
+A[6, 4] = 6.02165389804559606850219397283e-2
+A[6, 5] = -1.7578125e-2
+
+A[7, 0] = 3.70920001185047927108779319836e-2
+A[7, 3] = 1.70383925712239993810214054705e-1
+A[7, 4] = 1.07262030446373284651809199168e-1
+A[7, 5] = -1.53194377486244017527936158236e-2
+A[7, 6] = 8.27378916381402288758473766002e-3
+
+A[8, 0] = 6.24110958716075717114429577812e-1
+A[8, 3] = -3.36089262944694129406857109825
+A[8, 4] = -8.68219346841726006818189891453e-1
+A[8, 5] = 2.75920996994467083049415600797e1
+A[8, 6] = 2.01540675504778934086186788979e1
+A[8, 7] = -4.34898841810699588477366255144e1
+
+A[9, 0] = 4.77662536438264365890433908527e-1
+A[9, 3] = -2.48811461997166764192642586468
+A[9, 4] = -5.90290826836842996371446475743e-1
+A[9, 5] = 2.12300514481811942347288949897e1
+A[9, 6] = 1.52792336328824235832596922938e1
+A[9, 7] = -3.32882109689848629194453265587e1
+A[9, 8] = -2.03312017085086261358222928593e-2
+
+A[10, 0] = -9.3714243008598732571704021658e-1
+A[10, 3] = 5.18637242884406370830023853209
+A[10, 4] = 1.09143734899672957818500254654
+A[10, 5] = -8.14978701074692612513997267357
+A[10, 6] = -1.85200656599969598641566180701e1
+A[10, 7] = 2.27394870993505042818970056734e1
+A[10, 8] = 2.49360555267965238987089396762
+A[10, 9] = -3.0467644718982195003823669022
+
+A[11, 0] = 2.27331014751653820792359768449
+A[11, 3] = -1.05344954667372501984066689879e1
+A[11, 4] = -2.00087205822486249909675718444
+A[11, 5] = -1.79589318631187989172765950534e1
+A[11, 6] = 2.79488845294199600508499808837e1
+A[11, 7] = -2.85899827713502369474065508674
+A[11, 8] = -8.87285693353062954433549289258
+A[11, 9] = 1.23605671757943030647266201528e1
+A[11, 10] = 6.43392746015763530355970484046e-1
+
+A[12, 0] = 5.42937341165687622380535766363e-2
+A[12, 5] = 4.45031289275240888144113950566
+A[12, 6] = 1.89151789931450038304281599044
+A[12, 7] = -5.8012039600105847814672114227
+A[12, 8] = 3.1116436695781989440891606237e-1
+A[12, 9] = -1.52160949662516078556178806805e-1
+A[12, 10] = 2.01365400804030348374776537501e-1
+A[12, 11] = 4.47106157277725905176885569043e-2
+
+A[13, 0] = 5.61675022830479523392909219681e-2
+A[13, 6] = 2.53500210216624811088794765333e-1
+A[13, 7] = -2.46239037470802489917441475441e-1
+A[13, 8] = -1.24191423263816360469010140626e-1
+A[13, 9] = 1.5329179827876569731206322685e-1
+A[13, 10] = 8.20105229563468988491666602057e-3
+A[13, 11] = 7.56789766054569976138603589584e-3
+A[13, 12] = -8.298e-3
+
+A[14, 0] = 3.18346481635021405060768473261e-2
+A[14, 5] = 2.83009096723667755288322961402e-2
+A[14, 6] = 5.35419883074385676223797384372e-2
+A[14, 7] = -5.49237485713909884646569340306e-2
+A[14, 10] = -1.08347328697249322858509316994e-4
+A[14, 11] = 3.82571090835658412954920192323e-4
+A[14, 12] = -3.40465008687404560802977114492e-4
+A[14, 13] = 1.41312443674632500278074618366e-1
+
+A[15, 0] = -4.28896301583791923408573538692e-1
+A[15, 5] = -4.69762141536116384314449447206
+A[15, 6] = 7.68342119606259904184240953878
+A[15, 7] = 4.06898981839711007970213554331
+A[15, 8] = 3.56727187455281109270669543021e-1
+A[15, 12] = -1.39902416515901462129418009734e-3
+A[15, 13] = 2.9475147891527723389556272149
+A[15, 14] = -9.15095847217987001081870187138
+
+
+B = A[N_STAGES, :N_STAGES]
+
+E3 = np.zeros(N_STAGES + 1)
+E3[:-1] = B.copy()
+E3[0] -= 0.244094488188976377952755905512
+E3[8] -= 0.733846688281611857341361741547
+E3[11] -= 0.220588235294117647058823529412e-1
+
+E5 = np.zeros(N_STAGES + 1)
+E5[0] = 0.1312004499419488073250102996e-1
+E5[5] = -0.1225156446376204440720569753e+1
+E5[6] = -0.4957589496572501915214079952
+E5[7] = 0.1664377182454986536961530415e+1
+E5[8] = -0.3503288487499736816886487290
+E5[9] = 0.3341791187130174790297318841
+E5[10] = 0.8192320648511571246570742613e-1
+E5[11] = -0.2235530786388629525884427845e-1
+
+# First 3 coefficients are computed separately.
+D = np.zeros((INTERPOLATOR_POWER - 3, N_STAGES_EXTENDED))
+D[0, 0] = -0.84289382761090128651353491142e+1
+D[0, 5] = 0.56671495351937776962531783590
+D[0, 6] = -0.30689499459498916912797304727e+1
+D[0, 7] = 0.23846676565120698287728149680e+1
+D[0, 8] = 0.21170345824450282767155149946e+1
+D[0, 9] = -0.87139158377797299206789907490
+D[0, 10] = 0.22404374302607882758541771650e+1
+D[0, 11] = 0.63157877876946881815570249290
+D[0, 12] = -0.88990336451333310820698117400e-1
+D[0, 13] = 0.18148505520854727256656404962e+2
+D[0, 14] = -0.91946323924783554000451984436e+1
+D[0, 15] = -0.44360363875948939664310572000e+1
+
+D[1, 0] = 0.10427508642579134603413151009e+2
+D[1, 5] = 0.24228349177525818288430175319e+3
+D[1, 6] = 0.16520045171727028198505394887e+3
+D[1, 7] = -0.37454675472269020279518312152e+3
+D[1, 8] = -0.22113666853125306036270938578e+2
+D[1, 9] = 0.77334326684722638389603898808e+1
+D[1, 10] = -0.30674084731089398182061213626e+2
+D[1, 11] = -0.93321305264302278729567221706e+1
+D[1, 12] = 0.15697238121770843886131091075e+2
+D[1, 13] = -0.31139403219565177677282850411e+2
+D[1, 14] = -0.93529243588444783865713862664e+1
+D[1, 15] = 0.35816841486394083752465898540e+2
+
+D[2, 0] = 0.19985053242002433820987653617e+2
+D[2, 5] = -0.38703730874935176555105901742e+3
+D[2, 6] = -0.18917813819516756882830838328e+3
+D[2, 7] = 0.52780815920542364900561016686e+3
+D[2, 8] = -0.11573902539959630126141871134e+2
+D[2, 9] = 0.68812326946963000169666922661e+1
+D[2, 10] = -0.10006050966910838403183860980e+1
+D[2, 11] = 0.77771377980534432092869265740
+D[2, 12] = -0.27782057523535084065932004339e+1
+D[2, 13] = -0.60196695231264120758267380846e+2
+D[2, 14] = 0.84320405506677161018159903784e+2
+D[2, 15] = 0.11992291136182789328035130030e+2
+
+D[3, 0] = -0.25693933462703749003312586129e+2
+D[3, 5] = -0.15418974869023643374053993627e+3
+D[3, 6] = -0.23152937917604549567536039109e+3
+D[3, 7] = 0.35763911791061412378285349910e+3
+D[3, 8] = 0.93405324183624310003907691704e+2
+D[3, 9] = -0.37458323136451633156875139351e+2
+D[3, 10] = 0.10409964950896230045147246184e+3
+D[3, 11] = 0.29840293426660503123344363579e+2
+D[3, 12] = -0.43533456590011143754432175058e+2
+D[3, 13] = 0.96324553959188282948394950600e+2
+D[3, 14] = -0.39177261675615439165231486172e+2
+D[3, 15] = -0.14972683625798562581422125276e+3

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/_ivp/ivp.py

@@ -0,0 +1,678 @@
+import inspect
+import numpy as np
+from .bdf import BDF
+from .radau import Radau
+from .rk import RK23, RK45, DOP853
+from .lsoda import LSODA
+from scipy.optimize import OptimizeResult
+from .common import EPS, OdeSolution
+from .base import OdeSolver
+
+
+METHODS = {'RK23': RK23,
+           'RK45': RK45,
+           'DOP853': DOP853,
+           'Radau': Radau,
+           'BDF': BDF,
+           'LSODA': LSODA}
+
+
+MESSAGES = {0: "The solver successfully reached the end of the integration interval.",
+            1: "A termination event occurred."}
+
+
+class OdeResult(OptimizeResult):
+    pass
+
+
+def prepare_events(events):
+    """Standardize event functions and extract is_terminal and direction."""
+    if callable(events):
+        events = (events,)
+
+    if events is not None:
+        is_terminal = np.empty(len(events), dtype=bool)
+        direction = np.empty(len(events))
+        for i, event in enumerate(events):
+            try:
+                is_terminal[i] = event.terminal
+            except AttributeError:
+                is_terminal[i] = False
+
+            try:
+                direction[i] = event.direction
+            except AttributeError:
+                direction[i] = 0
+    else:
+        is_terminal = None
+        direction = None
+
+    return events, is_terminal, direction
+
+
+def solve_event_equation(event, sol, t_old, t):
+    """Solve an equation corresponding to an ODE event.
+
+    The equation is ``event(t, y(t)) = 0``, here ``y(t)`` is known from an
+    ODE solver using some sort of interpolation. It is solved by
+    `scipy.optimize.brentq` with xtol=atol=4*EPS.
+
+    Parameters
+    ----------
+    event : callable
+        Function ``event(t, y)``.
+    sol : callable
+        Function ``sol(t)`` which evaluates an ODE solution between `t_old`
+        and  `t`.
+    t_old, t : float
+        Previous and new values of time. They will be used as a bracketing
+        interval.
+
+    Returns
+    -------
+    root : float
+        Found solution.
+    """
+    from scipy.optimize import brentq
+    return brentq(lambda t: event(t, sol(t)), t_old, t,
+                  xtol=4 * EPS, rtol=4 * EPS)
+
+
+def handle_events(sol, events, active_events, is_terminal, t_old, t):
+    """Helper function to handle events.
+
+    Parameters
+    ----------
+    sol : DenseOutput
+        Function ``sol(t)`` which evaluates an ODE solution between `t_old`
+        and  `t`.
+    events : list of callables, length n_events
+        Event functions with signatures ``event(t, y)``.
+    active_events : ndarray
+        Indices of events which occurred.
+    is_terminal : ndarray, shape (n_events,)
+        Which events are terminal.
+    t_old, t : float
+        Previous and new values of time.
+
+    Returns
+    -------
+    root_indices : ndarray
+        Indices of events which take zero between `t_old` and `t` and before
+        a possible termination.
+    roots : ndarray
+        Values of t at which events occurred.
+    terminate : bool
+        Whether a terminal event occurred.
+    """
+    roots = [solve_event_equation(events[event_index], sol, t_old, t)
+             for event_index in active_events]
+
+    roots = np.asarray(roots)
+
+    if np.any(is_terminal[active_events]):
+        if t > t_old:
+            order = np.argsort(roots)
+        else:
+            order = np.argsort(-roots)
+        active_events = active_events[order]
+        roots = roots[order]
+        t = np.nonzero(is_terminal[active_events])[0][0]
+        active_events = active_events[:t + 1]
+        roots = roots[:t + 1]
+        terminate = True
+    else:
+        terminate = False
+
+    return active_events, roots, terminate
+
+
+def find_active_events(g, g_new, direction):
+    """Find which event occurred during an integration step.
+
+    Parameters
+    ----------
+    g, g_new : array_like, shape (n_events,)
+        Values of event functions at a current and next points.
+    direction : ndarray, shape (n_events,)
+        Event "direction" according to the definition in `solve_ivp`.
+
+    Returns
+    -------
+    active_events : ndarray
+        Indices of events which occurred during the step.
+    """
+    g, g_new = np.asarray(g), np.asarray(g_new)
+    up = (g <= 0) & (g_new >= 0)
+    down = (g >= 0) & (g_new <= 0)
+    either = up | down
+    mask = (up & (direction > 0) |
+            down & (direction < 0) |
+            either & (direction == 0))
+
+    return np.nonzero(mask)[0]
+
+
+def solve_ivp(fun, t_span, y0, method='RK45', t_eval=None, dense_output=False,
+              events=None, vectorized=False, args=None, **options):
+    """Solve an initial value problem for a system of ODEs.
+
+    This function numerically integrates a system of ordinary differential
+    equations given an initial value::
+
+        dy / dt = f(t, y)
+        y(t0) = y0
+
+    Here t is a 1-D independent variable (time), y(t) is an
+    N-D vector-valued function (state), and an N-D
+    vector-valued function f(t, y) determines the differential equations.
+    The goal is to find y(t) approximately satisfying the differential
+    equations, given an initial value y(t0)=y0.
+
+    Some of the solvers support integration in the complex domain, but note
+    that for stiff ODE solvers, the right-hand side must be
+    complex-differentiable (satisfy Cauchy-Riemann equations [11]_).
+    To solve a problem in the complex domain, pass y0 with a complex data type.
+    Another option always available is to rewrite your problem for real and
+    imaginary parts separately.
+
+    Parameters
+    ----------
+    fun : callable
+        Right-hand side of the system. The calling signature is ``fun(t, y)``.
+        Here `t` is a scalar, and there are two options for the ndarray `y`:
+        It can either have shape (n,); then `fun` must return array_like with
+        shape (n,). Alternatively, it can have shape (n, k); then `fun`
+        must return an array_like with shape (n, k), i.e., each column
+        corresponds to a single column in `y`. The choice between the two
+        options is determined by `vectorized` argument (see below). The
+        vectorized implementation allows a faster approximation of the Jacobian
+        by finite differences (required for stiff solvers).
+    t_span : 2-member sequence
+        Interval of integration (t0, tf). The solver starts with t=t0 and
+        integrates until it reaches t=tf. Both t0 and tf must be floats
+        or values interpretable by the float conversion function.
+    y0 : array_like, shape (n,)
+        Initial state. For problems in the complex domain, pass `y0` with a
+        complex data type (even if the initial value is purely real).
+    method : string or `OdeSolver`, optional
+        Integration method to use:
+
+            * 'RK45' (default): Explicit Runge-Kutta method of order 5(4) [1]_.
+              The error is controlled assuming accuracy of the fourth-order
+              method, but steps are taken using the fifth-order accurate
+              formula (local extrapolation is done). A quartic interpolation
+              polynomial is used for the dense output [2]_. Can be applied in
+              the complex domain.
+            * 'RK23': Explicit Runge-Kutta method of order 3(2) [3]_. The error
+              is controlled assuming accuracy of the second-order method, but
+              steps are taken using the third-order accurate formula (local
+              extrapolation is done). A cubic Hermite polynomial is used for the
+              dense output. Can be applied in the complex domain.
+            * 'DOP853': Explicit Runge-Kutta method of order 8 [13]_.
+              Python implementation of the "DOP853" algorithm originally
+              written in Fortran [14]_. A 7-th order interpolation polynomial
+              accurate to 7-th order is used for the dense output.
+              Can be applied in the complex domain.
+            * 'Radau': Implicit Runge-Kutta method of the Radau IIA family of
+              order 5 [4]_. The error is controlled with a third-order accurate
+              embedded formula. A cubic polynomial which satisfies the
+              collocation conditions is used for the dense output.
+            * 'BDF': Implicit multi-step variable-order (1 to 5) method based
+              on a backward differentiation formula for the derivative
+              approximation [5]_. The implementation follows the one described
+              in [6]_. A quasi-constant step scheme is used and accuracy is
+              enhanced using the NDF modification. Can be applied in the
+              complex domain.
+            * 'LSODA': Adams/BDF method with automatic stiffness detection and
+              switching [7]_, [8]_. This is a wrapper of the Fortran solver
+              from ODEPACK.
+
+        Explicit Runge-Kutta methods ('RK23', 'RK45', 'DOP853') should be used
+        for non-stiff problems and implicit methods ('Radau', 'BDF') for
+        stiff problems [9]_. Among Runge-Kutta methods, 'DOP853' is recommended
+        for solving with high precision (low values of `rtol` and `atol`).
+
+        If not sure, first try to run 'RK45'. If it makes unusually many
+        iterations, diverges, or fails, your problem is likely to be stiff and
+        you should use 'Radau' or 'BDF'. 'LSODA' can also be a good universal
+        choice, but it might be somewhat less convenient to work with as it
+        wraps old Fortran code.
+
+        You can also pass an arbitrary class derived from `OdeSolver` which
+        implements the solver.
+    t_eval : array_like or None, optional
+        Times at which to store the computed solution, must be sorted and lie
+        within `t_span`. If None (default), use points selected by the solver.
+    dense_output : bool, optional
+        Whether to compute a continuous solution. Default is False.
+    events : callable, or list of callables, optional
+        Events to track. If None (default), no events will be tracked.
+        Each event occurs at the zeros of a continuous function of time and
+        state. Each function must have the signature ``event(t, y)`` and return
+        a float. The solver will find an accurate value of `t` at which
+        ``event(t, y(t)) = 0`` using a root-finding algorithm. By default, all
+        zeros will be found. The solver looks for a sign change over each step,
+        so if multiple zero crossings occur within one step, events may be
+        missed. Additionally each `event` function might have the following
+        attributes:
+
+            terminal: bool, optional
+                Whether to terminate integration if this event occurs.
+                Implicitly False if not assigned.
+            direction: float, optional
+                Direction of a zero crossing. If `direction` is positive,
+                `event` will only trigger when going from negative to positive,
+                and vice versa if `direction` is negative. If 0, then either
+                direction will trigger event. Implicitly 0 if not assigned.
+
+        You can assign attributes like ``event.terminal = True`` to any
+        function in Python.
+    vectorized : bool, optional
+        Whether `fun` is implemented in a vectorized fashion. Default is False.
+    args : tuple, optional
+        Additional arguments to pass to the user-defined functions.  If given,
+        the additional arguments are passed to all user-defined functions.
+        So if, for example, `fun` has the signature ``fun(t, y, a, b, c)``,
+        then `jac` (if given) and any event functions must have the same
+        signature, and `args` must be a tuple of length 3.
+    **options
+        Options passed to a chosen solver. All options available for already
+        implemented solvers are listed below.
+    first_step : float or None, optional
+        Initial step size. Default is `None` which means that the algorithm
+        should choose.
+    max_step : float, optional
+        Maximum allowed step size. Default is np.inf, i.e., the step size is not
+        bounded and determined solely by the solver.
+    rtol, atol : float or array_like, optional
+        Relative and absolute tolerances. The solver keeps the local error
+        estimates less than ``atol + rtol * abs(y)``. Here `rtol` controls a
+        relative accuracy (number of correct digits), while `atol` controls
+        absolute accuracy (number of correct decimal places). To achieve the
+        desired `rtol`, set `atol` to be smaller than the smallest value that
+        can be expected from ``rtol * abs(y)`` so that `rtol` dominates the
+        allowable error. If `atol` is larger than ``rtol * abs(y)`` the
+        number of correct digits is not guaranteed. Conversely, to achieve the
+        desired `atol` set `rtol` such that ``rtol * abs(y)`` is always smaller
+        than `atol`. If components of y have different scales, it might be
+        beneficial to set different `atol` values for different components by
+        passing array_like with shape (n,) for `atol`. Default values are
+        1e-3 for `rtol` and 1e-6 for `atol`.
+    jac : array_like, sparse_matrix, callable or None, optional
+        Jacobian matrix of the right-hand side of the system with respect
+        to y, required by the 'Radau', 'BDF' and 'LSODA' method. The
+        Jacobian matrix has shape (n, n) and its element (i, j) is equal to
+        ``d f_i / d y_j``.  There are three ways to define the Jacobian:
+
+            * If array_like or sparse_matrix, the Jacobian is assumed to
+              be constant. Not supported by 'LSODA'.
+            * If callable, the Jacobian is assumed to depend on both
+              t and y; it will be called as ``jac(t, y)``, as necessary.
+              For 'Radau' and 'BDF' methods, the return value might be a
+              sparse matrix.
+            * If None (default), the Jacobian will be approximated by
+              finite differences.
+
+        It is generally recommended to provide the Jacobian rather than
+        relying on a finite-difference approximation.
+    jac_sparsity : array_like, sparse matrix or None, optional
+        Defines a sparsity structure of the Jacobian matrix for a finite-
+        difference approximation. Its shape must be (n, n). This argument
+        is ignored if `jac` is not `None`. If the Jacobian has only few
+        non-zero elements in *each* row, providing the sparsity structure
+        will greatly speed up the computations [10]_. A zero entry means that
+        a corresponding element in the Jacobian is always zero. If None
+        (default), the Jacobian is assumed to be dense.
+        Not supported by 'LSODA', see `lband` and `uband` instead.
+    lband, uband : int or None, optional
+        Parameters defining the bandwidth of the Jacobian for the 'LSODA'
+        method, i.e., ``jac[i, j] != 0 only for i - lband <= j <= i + uband``.
+        Default is None. Setting these requires your jac routine to return the
+        Jacobian in the packed format: the returned array must have ``n``
+        columns and ``uband + lband + 1`` rows in which Jacobian diagonals are
+        written. Specifically ``jac_packed[uband + i - j , j] = jac[i, j]``.
+        The same format is used in `scipy.linalg.solve_banded` (check for an
+        illustration).  These parameters can be also used with ``jac=None`` to
+        reduce the number of Jacobian elements estimated by finite differences.
+    min_step : float, optional
+        The minimum allowed step size for 'LSODA' method.
+        By default `min_step` is zero.
+
+    Returns
+    -------
+    Bunch object with the following fields defined:
+    t : ndarray, shape (n_points,)
+        Time points.
+    y : ndarray, shape (n, n_points)
+        Values of the solution at `t`.
+    sol : `OdeSolution` or None
+        Found solution as `OdeSolution` instance; None if `dense_output` was
+        set to False.
+    t_events : list of ndarray or None
+        Contains for each event type a list of arrays at which an event of
+        that type event was detected. None if `events` was None.
+    y_events : list of ndarray or None
+        For each value of `t_events`, the corresponding value of the solution.
+        None if `events` was None.
+    nfev : int
+        Number of evaluations of the right-hand side.
+    njev : int
+        Number of evaluations of the Jacobian.
+    nlu : int
+        Number of LU decompositions.
+    status : int
+        Reason for algorithm termination:
+
+            * -1: Integration step failed.
+            *  0: The solver successfully reached the end of `tspan`.
+            *  1: A termination event occurred.
+
+    message : string
+        Human-readable description of the termination reason.
+    success : bool
+        True if the solver reached the interval end or a termination event
+        occurred (``status >= 0``).
+
+    References
+    ----------
+    .. [1] J. R. Dormand, P. J. Prince, "A family of embedded Runge-Kutta
+           formulae", Journal of Computational and Applied Mathematics, Vol. 6,
+           No. 1, pp. 19-26, 1980.
+    .. [2] L. W. Shampine, "Some Practical Runge-Kutta Formulas", Mathematics
+           of Computation,, Vol. 46, No. 173, pp. 135-150, 1986.
+    .. [3] P. Bogacki, L.F. Shampine, "A 3(2) Pair of Runge-Kutta Formulas",
+           Appl. Math. Lett. Vol. 2, No. 4. pp. 321-325, 1989.
+    .. [4] E. Hairer, G. Wanner, "Solving Ordinary Differential Equations II:
+           Stiff and Differential-Algebraic Problems", Sec. IV.8.
+    .. [5] `Backward Differentiation Formula
+            <https://en.wikipedia.org/wiki/Backward_differentiation_formula>`_
+            on Wikipedia.
+    .. [6] L. F. Shampine, M. W. Reichelt, "THE MATLAB ODE SUITE", SIAM J. SCI.
+           COMPUTE., Vol. 18, No. 1, pp. 1-22, January 1997.
+    .. [7] A. C. Hindmarsh, "ODEPACK, A Systematized Collection of ODE
+           Solvers," IMACS Transactions on Scientific Computation, Vol 1.,
+           pp. 55-64, 1983.
+    .. [8] L. Petzold, "Automatic selection of methods for solving stiff and
+           nonstiff systems of ordinary differential equations", SIAM Journal
+           on Scientific and Statistical Computing, Vol. 4, No. 1, pp. 136-148,
+           1983.
+    .. [9] `Stiff equation <https://en.wikipedia.org/wiki/Stiff_equation>`_ on
+           Wikipedia.
+    .. [10] A. Curtis, M. J. D. Powell, and J. Reid, "On the estimation of
+            sparse Jacobian matrices", Journal of the Institute of Mathematics
+            and its Applications, 13, pp. 117-120, 1974.
+    .. [11] `Cauchy-Riemann equations
+             <https://en.wikipedia.org/wiki/Cauchy-Riemann_equations>`_ on
+             Wikipedia.
+    .. [12] `Lotka-Volterra equations
+            <https://en.wikipedia.org/wiki/Lotka%E2%80%93Volterra_equations>`_
+            on Wikipedia.
+    .. [13] E. Hairer, S. P. Norsett G. Wanner, "Solving Ordinary Differential
+            Equations I: Nonstiff Problems", Sec. II.
+    .. [14] `Page with original Fortran code of DOP853
+            <http://www.unige.ch/~hairer/software.html>`_.
+
+    Examples
+    --------
+    Basic exponential decay showing automatically chosen time points.
+
+    >>> import numpy as np
+    >>> from scipy.integrate import solve_ivp
+    >>> def exponential_decay(t, y): return -0.5 * y
+    >>> sol = solve_ivp(exponential_decay, [0, 10], [2, 4, 8])
+    >>> print(sol.t)
+    [ 0.          0.11487653  1.26364188  3.06061781  4.81611105  6.57445806
+      8.33328988 10.        ]
+    >>> print(sol.y)
+    [[2.         1.88836035 1.06327177 0.43319312 0.18017253 0.07483045
+      0.03107158 0.01350781]
+     [4.         3.7767207  2.12654355 0.86638624 0.36034507 0.14966091
+      0.06214316 0.02701561]
+     [8.         7.5534414  4.25308709 1.73277247 0.72069014 0.29932181
+      0.12428631 0.05403123]]
+
+    Specifying points where the solution is desired.
+
+    >>> sol = solve_ivp(exponential_decay, [0, 10], [2, 4, 8],
+    ...                 t_eval=[0, 1, 2, 4, 10])
+    >>> print(sol.t)
+    [ 0  1  2  4 10]
+    >>> print(sol.y)
+    [[2.         1.21305369 0.73534021 0.27066736 0.01350938]
+     [4.         2.42610739 1.47068043 0.54133472 0.02701876]
+     [8.         4.85221478 2.94136085 1.08266944 0.05403753]]
+
+    Cannon fired upward with terminal event upon impact. The ``terminal`` and
+    ``direction`` fields of an event are applied by monkey patching a function.
+    Here ``y[0]`` is position and ``y[1]`` is velocity. The projectile starts
+    at position 0 with velocity +10. Note that the integration never reaches
+    t=100 because the event is terminal.
+
+    >>> def upward_cannon(t, y): return [y[1], -0.5]
+    >>> def hit_ground(t, y): return y[0]
+    >>> hit_ground.terminal = True
+    >>> hit_ground.direction = -1
+    >>> sol = solve_ivp(upward_cannon, [0, 100], [0, 10], events=hit_ground)
+    >>> print(sol.t_events)
+    [array([40.])]
+    >>> print(sol.t)
+    [0.00000000e+00 9.99900010e-05 1.09989001e-03 1.10988901e-02
+     1.11088891e-01 1.11098890e+00 1.11099890e+01 4.00000000e+01]
+
+    Use `dense_output` and `events` to find position, which is 100, at the apex
+    of the cannonball's trajectory. Apex is not defined as terminal, so both
+    apex and hit_ground are found. There is no information at t=20, so the sol
+    attribute is used to evaluate the solution. The sol attribute is returned
+    by setting ``dense_output=True``. Alternatively, the `y_events` attribute
+    can be used to access the solution at the time of the event.
+
+    >>> def apex(t, y): return y[1]
+    >>> sol = solve_ivp(upward_cannon, [0, 100], [0, 10],
+    ...                 events=(hit_ground, apex), dense_output=True)
+    >>> print(sol.t_events)
+    [array([40.]), array([20.])]
+    >>> print(sol.t)
+    [0.00000000e+00 9.99900010e-05 1.09989001e-03 1.10988901e-02
+     1.11088891e-01 1.11098890e+00 1.11099890e+01 4.00000000e+01]
+    >>> print(sol.sol(sol.t_events[1][0]))
+    [100.   0.]
+    >>> print(sol.y_events)
+    [array([[-5.68434189e-14, -1.00000000e+01]]), array([[1.00000000e+02, 1.77635684e-15]])]
+
+    As an example of a system with additional parameters, we'll implement
+    the Lotka-Volterra equations [12]_.
+
+    >>> def lotkavolterra(t, z, a, b, c, d):
+    ...     x, y = z
+    ...     return [a*x - b*x*y, -c*y + d*x*y]
+    ...
+
+    We pass in the parameter values a=1.5, b=1, c=3 and d=1 with the `args`
+    argument.
+
+    >>> sol = solve_ivp(lotkavolterra, [0, 15], [10, 5], args=(1.5, 1, 3, 1),
+    ...                 dense_output=True)
+
+    Compute a dense solution and plot it.
+
+    >>> t = np.linspace(0, 15, 300)
+    >>> z = sol.sol(t)
+    >>> import matplotlib.pyplot as plt
+    >>> plt.plot(t, z.T)
+    >>> plt.xlabel('t')
+    >>> plt.legend(['x', 'y'], shadow=True)
+    >>> plt.title('Lotka-Volterra System')
+    >>> plt.show()
+
+    """
+    if method not in METHODS and not (
+            inspect.isclass(method) and issubclass(method, OdeSolver)):
+        raise ValueError("`method` must be one of {} or OdeSolver class."
+                         .format(METHODS))
+
+    t0, tf = map(float, t_span)
+
+    if args is not None:
+        # Wrap the user's fun (and jac, if given) in lambdas to hide the
+        # additional parameters.  Pass in the original fun as a keyword
+        # argument to keep it in the scope of the lambda.
+        try:
+            _ = [*(args)]
+        except TypeError as exp:
+            suggestion_tuple = (
+                "Supplied 'args' cannot be unpacked. Please supply `args`"
+                f" as a tuple (e.g. `args=({args},)`)"
+            )
+            raise TypeError(suggestion_tuple) from exp
+
+        fun = lambda t, x, fun=fun: fun(t, x, *args)
+        jac = options.get('jac')
+        if callable(jac):
+            options['jac'] = lambda t, x: jac(t, x, *args)
+
+    if t_eval is not None:
+        t_eval = np.asarray(t_eval)
+        if t_eval.ndim != 1:
+            raise ValueError("`t_eval` must be 1-dimensional.")
+
+        if np.any(t_eval < min(t0, tf)) or np.any(t_eval > max(t0, tf)):
+            raise ValueError("Values in `t_eval` are not within `t_span`.")
+
+        d = np.diff(t_eval)
+        if tf > t0 and np.any(d <= 0) or tf < t0 and np.any(d >= 0):
+            raise ValueError("Values in `t_eval` are not properly sorted.")
+
+        if tf > t0:
+            t_eval_i = 0
+        else:
+            # Make order of t_eval decreasing to use np.searchsorted.
+            t_eval = t_eval[::-1]
+            # This will be an upper bound for slices.
+            t_eval_i = t_eval.shape[0]
+
+    if method in METHODS:
+        method = METHODS[method]
+
+    solver = method(fun, t0, y0, tf, vectorized=vectorized, **options)
+
+    if t_eval is None:
+        ts = [t0]
+        ys = [y0]
+    elif t_eval is not None and dense_output:
+        ts = []
+        ti = [t0]
+        ys = []
+    else:
+        ts = []
+        ys = []
+
+    interpolants = []
+
+    events, is_terminal, event_dir = prepare_events(events)
+
+    if events is not None:
+        if args is not None:
+            # Wrap user functions in lambdas to hide the additional parameters.
+            # The original event function is passed as a keyword argument to the
+            # lambda to keep the original function in scope (i.e., avoid the
+            # late binding closure "gotcha").
+            events = [lambda t, x, event=event: event(t, x, *args)
+                      for event in events]
+        g = [event(t0, y0) for event in events]
+        t_events = [[] for _ in range(len(events))]
+        y_events = [[] for _ in range(len(events))]
+    else:
+        t_events = None
+        y_events = None
+
+    status = None
+    while status is None:
+        message = solver.step()
+
+        if solver.status == 'finished':
+            status = 0
+        elif solver.status == 'failed':
+            status = -1
+            break
+
+        t_old = solver.t_old
+        t = solver.t
+        y = solver.y
+
+        if dense_output:
+            sol = solver.dense_output()
+            interpolants.append(sol)
+        else:
+            sol = None
+
+        if events is not None:
+            g_new = [event(t, y) for event in events]
+            active_events = find_active_events(g, g_new, event_dir)
+            if active_events.size > 0:
+                if sol is None:
+                    sol = solver.dense_output()
+
+                root_indices, roots, terminate = handle_events(
+                    sol, events, active_events, is_terminal, t_old, t)
+
+                for e, te in zip(root_indices, roots):
+                    t_events[e].append(te)
+                    y_events[e].append(sol(te))
+
+                if terminate:
+                    status = 1
+                    t = roots[-1]
+                    y = sol(t)
+
+            g = g_new
+
+        if t_eval is None:
+            ts.append(t)
+            ys.append(y)
+        else:
+            # The value in t_eval equal to t will be included.
+            if solver.direction > 0:
+                t_eval_i_new = np.searchsorted(t_eval, t, side='right')
+                t_eval_step = t_eval[t_eval_i:t_eval_i_new]
+            else:
+                t_eval_i_new = np.searchsorted(t_eval, t, side='left')
+                # It has to be done with two slice operations, because
+                # you can't slice to 0th element inclusive using backward
+                # slicing.
+                t_eval_step = t_eval[t_eval_i_new:t_eval_i][::-1]
+
+            if t_eval_step.size > 0:
+                if sol is None:
+                    sol = solver.dense_output()
+                ts.append(t_eval_step)
+                ys.append(sol(t_eval_step))
+                t_eval_i = t_eval_i_new
+
+        if t_eval is not None and dense_output:
+            ti.append(t)
+
+    message = MESSAGES.get(status, message)
+
+    if t_events is not None:
+        t_events = [np.asarray(te) for te in t_events]
+        y_events = [np.asarray(ye) for ye in y_events]
+
+    if t_eval is None:
+        ts = np.array(ts)
+        ys = np.vstack(ys).T
+    elif ts:
+        ts = np.hstack(ts)
+        ys = np.hstack(ys)
+
+    if dense_output:
+        if t_eval is None:
+            sol = OdeSolution(ts, interpolants)
+        else:
+            sol = OdeSolution(ti, interpolants)
+    else:
+        sol = None
+
+    return OdeResult(t=ts, y=ys, sol=sol, t_events=t_events, y_events=y_events,
+                     nfev=solver.nfev, njev=solver.njev, nlu=solver.nlu,
+                     status=status, message=message, success=status >= 0)

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/_ivp/lsoda.py

@@ -0,0 +1,192 @@
+import numpy as np
+from scipy.integrate import ode
+from .common import validate_tol, validate_first_step, warn_extraneous
+from .base import OdeSolver, DenseOutput
+
+
+class LSODA(OdeSolver):
+    """Adams/BDF method with automatic stiffness detection and switching.
+
+    This is a wrapper to the Fortran solver from ODEPACK [1]_. It switches
+    automatically between the nonstiff Adams method and the stiff BDF method.
+    The method was originally detailed in [2]_.
+
+    Parameters
+    ----------
+    fun : callable
+        Right-hand side of the system. The calling signature is ``fun(t, y)``.
+        Here ``t`` is a scalar, and there are two options for the ndarray ``y``:
+        It can either have shape (n,); then ``fun`` must return array_like with
+        shape (n,). Alternatively it can have shape (n, k); then ``fun``
+        must return an array_like with shape (n, k), i.e. each column
+        corresponds to a single column in ``y``. The choice between the two
+        options is determined by `vectorized` argument (see below). The
+        vectorized implementation allows a faster approximation of the Jacobian
+        by finite differences (required for this solver).
+    t0 : float
+        Initial time.
+    y0 : array_like, shape (n,)
+        Initial state.
+    t_bound : float
+        Boundary time - the integration won't continue beyond it. It also
+        determines the direction of the integration.
+    first_step : float or None, optional
+        Initial step size. Default is ``None`` which means that the algorithm
+        should choose.
+    min_step : float, optional
+        Minimum allowed step size. Default is 0.0, i.e., the step size is not
+        bounded and determined solely by the solver.
+    max_step : float, optional
+        Maximum allowed step size. Default is np.inf, i.e., the step size is not
+        bounded and determined solely by the solver.
+    rtol, atol : float and array_like, optional
+        Relative and absolute tolerances. The solver keeps the local error
+        estimates less than ``atol + rtol * abs(y)``. Here `rtol` controls a
+        relative accuracy (number of correct digits), while `atol` controls
+        absolute accuracy (number of correct decimal places). To achieve the
+        desired `rtol`, set `atol` to be smaller than the smallest value that
+        can be expected from ``rtol * abs(y)`` so that `rtol` dominates the
+        allowable error. If `atol` is larger than ``rtol * abs(y)`` the
+        number of correct digits is not guaranteed. Conversely, to achieve the
+        desired `atol` set `rtol` such that ``rtol * abs(y)`` is always smaller
+        than `atol`. If components of y have different scales, it might be
+        beneficial to set different `atol` values for different components by
+        passing array_like with shape (n,) for `atol`. Default values are
+        1e-3 for `rtol` and 1e-6 for `atol`.
+    jac : None or callable, optional
+        Jacobian matrix of the right-hand side of the system with respect to
+        ``y``. The Jacobian matrix has shape (n, n) and its element (i, j) is
+        equal to ``d f_i / d y_j``. The function will be called as
+        ``jac(t, y)``. If None (default), the Jacobian will be
+        approximated by finite differences. It is generally recommended to
+        provide the Jacobian rather than relying on a finite-difference
+        approximation.
+    lband, uband : int or None
+        Parameters defining the bandwidth of the Jacobian,
+        i.e., ``jac[i, j] != 0 only for i - lband <= j <= i + uband``. Setting
+        these requires your jac routine to return the Jacobian in the packed format:
+        the returned array must have ``n`` columns and ``uband + lband + 1``
+        rows in which Jacobian diagonals are written. Specifically
+        ``jac_packed[uband + i - j , j] = jac[i, j]``. The same format is used
+        in `scipy.linalg.solve_banded` (check for an illustration).
+        These parameters can be also used with ``jac=None`` to reduce the
+        number of Jacobian elements estimated by finite differences.
+    vectorized : bool, optional
+        Whether `fun` is implemented in a vectorized fashion. A vectorized
+        implementation offers no advantages for this solver. Default is False.
+
+    Attributes
+    ----------
+    n : int
+        Number of equations.
+    status : string
+        Current status of the solver: 'running', 'finished' or 'failed'.
+    t_bound : float
+        Boundary time.
+    direction : float
+        Integration direction: +1 or -1.
+    t : float
+        Current time.
+    y : ndarray
+        Current state.
+    t_old : float
+        Previous time. None if no steps were made yet.
+    nfev : int
+        Number of evaluations of the right-hand side.
+    njev : int
+        Number of evaluations of the Jacobian.
+
+    References
+    ----------
+    .. [1] A. C. Hindmarsh, "ODEPACK, A Systematized Collection of ODE
+           Solvers," IMACS Transactions on Scientific Computation, Vol 1.,
+           pp. 55-64, 1983.
+    .. [2] L. Petzold, "Automatic selection of methods for solving stiff and
+           nonstiff systems of ordinary differential equations", SIAM Journal
+           on Scientific and Statistical Computing, Vol. 4, No. 1, pp. 136-148,
+           1983.
+    """
+    def __init__(self, fun, t0, y0, t_bound, first_step=None, min_step=0.0,
+                 max_step=np.inf, rtol=1e-3, atol=1e-6, jac=None, lband=None,
+                 uband=None, vectorized=False, **extraneous):
+        warn_extraneous(extraneous)
+        super().__init__(fun, t0, y0, t_bound, vectorized)
+
+        if first_step is None:
+            first_step = 0  # LSODA value for automatic selection.
+        else:
+            first_step = validate_first_step(first_step, t0, t_bound)
+
+        first_step *= self.direction
+
+        if max_step == np.inf:
+            max_step = 0  # LSODA value for infinity.
+        elif max_step <= 0:
+            raise ValueError("`max_step` must be positive.")
+
+        if min_step < 0:
+            raise ValueError("`min_step` must be nonnegative.")
+
+        rtol, atol = validate_tol(rtol, atol, self.n)
+
+        solver = ode(self.fun, jac)
+        solver.set_integrator('lsoda', rtol=rtol, atol=atol, max_step=max_step,
+                              min_step=min_step, first_step=first_step,
+                              lband=lband, uband=uband)
+        solver.set_initial_value(y0, t0)
+
+        # Inject t_bound into rwork array as needed for itask=5.
+        solver._integrator.rwork[0] = self.t_bound
+        solver._integrator.call_args[4] = solver._integrator.rwork
+
+        self._lsoda_solver = solver
+
+    def _step_impl(self):
+        solver = self._lsoda_solver
+        integrator = solver._integrator
+
+        # From lsoda.step and lsoda.integrate itask=5 means take a single
+        # step and do not go past t_bound.
+        itask = integrator.call_args[2]
+        integrator.call_args[2] = 5
+        solver._y, solver.t = integrator.run(
+            solver.f, solver.jac or (lambda: None), solver._y, solver.t,
+            self.t_bound, solver.f_params, solver.jac_params)
+        integrator.call_args[2] = itask
+
+        if solver.successful():
+            self.t = solver.t
+            self.y = solver._y
+            # From LSODA Fortran source njev is equal to nlu.
+            self.njev = integrator.iwork[12]
+            self.nlu = integrator.iwork[12]
+            return True, None
+        else:
+            return False, 'Unexpected istate in LSODA.'
+
+    def _dense_output_impl(self):
+        iwork = self._lsoda_solver._integrator.iwork
+        rwork = self._lsoda_solver._integrator.rwork
+
+        order = iwork[14]
+        h = rwork[11]
+        yh = np.reshape(rwork[20:20 + (order + 1) * self.n],
+                        (self.n, order + 1), order='F').copy()
+
+        return LsodaDenseOutput(self.t_old, self.t, h, order, yh)
+
+
+class LsodaDenseOutput(DenseOutput):
+    def __init__(self, t_old, t, h, order, yh):
+        super().__init__(t_old, t)
+        self.h = h
+        self.yh = yh
+        self.p = np.arange(order + 1)
+
+    def _call_impl(self, t):
+        if t.ndim == 0:
+            x = ((t - self.t) / self.h) ** self.p
+        else:
+            x = ((t - self.t) / self.h) ** self.p[:, None]
+
+        return np.dot(self.yh, x)

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/_ivp/radau.py

@@ -0,0 +1,565 @@
+import numpy as np
+from scipy.linalg import lu_factor, lu_solve
+from scipy.sparse import csc_matrix, issparse, eye
+from scipy.sparse.linalg import splu
+from scipy.optimize._numdiff import group_columns
+from .common import (validate_max_step, validate_tol, select_initial_step,
+                     norm, num_jac, EPS, warn_extraneous,
+                     validate_first_step)
+from .base import OdeSolver, DenseOutput
+
+S6 = 6 ** 0.5
+
+# Butcher tableau. A is not used directly, see below.
+C = np.array([(4 - S6) / 10, (4 + S6) / 10, 1])
+E = np.array([-13 - 7 * S6, -13 + 7 * S6, -1]) / 3
+
+# Eigendecomposition of A is done: A = T L T**-1. There is 1 real eigenvalue
+# and a complex conjugate pair. They are written below.
+MU_REAL = 3 + 3 ** (2 / 3) - 3 ** (1 / 3)
+MU_COMPLEX = (3 + 0.5 * (3 ** (1 / 3) - 3 ** (2 / 3))
+              - 0.5j * (3 ** (5 / 6) + 3 ** (7 / 6)))
+
+# These are transformation matrices.
+T = np.array([
+    [0.09443876248897524, -0.14125529502095421, 0.03002919410514742],
+    [0.25021312296533332, 0.20412935229379994, -0.38294211275726192],
+    [1, 1, 0]])
+TI = np.array([
+    [4.17871859155190428, 0.32768282076106237, 0.52337644549944951],
+    [-4.17871859155190428, -0.32768282076106237, 0.47662355450055044],
+    [0.50287263494578682, -2.57192694985560522, 0.59603920482822492]])
+# These linear combinations are used in the algorithm.
+TI_REAL = TI[0]
+TI_COMPLEX = TI[1] + 1j * TI[2]
+
+# Interpolator coefficients.
+P = np.array([
+    [13/3 + 7*S6/3, -23/3 - 22*S6/3, 10/3 + 5 * S6],
+    [13/3 - 7*S6/3, -23/3 + 22*S6/3, 10/3 - 5 * S6],
+    [1/3, -8/3, 10/3]])
+
+
+NEWTON_MAXITER = 6  # Maximum number of Newton iterations.
+MIN_FACTOR = 0.2  # Minimum allowed decrease in a step size.
+MAX_FACTOR = 10  # Maximum allowed increase in a step size.
+
+
+def solve_collocation_system(fun, t, y, h, Z0, scale, tol,
+                             LU_real, LU_complex, solve_lu):
+    """Solve the collocation system.
+
+    Parameters
+    ----------
+    fun : callable
+        Right-hand side of the system.
+    t : float
+        Current time.
+    y : ndarray, shape (n,)
+        Current state.
+    h : float
+        Step to try.
+    Z0 : ndarray, shape (3, n)
+        Initial guess for the solution. It determines new values of `y` at
+        ``t + h * C`` as ``y + Z0``, where ``C`` is the Radau method constants.
+    scale : ndarray, shape (n)
+        Problem tolerance scale, i.e. ``rtol * abs(y) + atol``.
+    tol : float
+        Tolerance to which solve the system. This value is compared with
+        the normalized by `scale` error.
+    LU_real, LU_complex
+        LU decompositions of the system Jacobians.
+    solve_lu : callable
+        Callable which solves a linear system given a LU decomposition. The
+        signature is ``solve_lu(LU, b)``.
+
+    Returns
+    -------
+    converged : bool
+        Whether iterations converged.
+    n_iter : int
+        Number of completed iterations.
+    Z : ndarray, shape (3, n)
+        Found solution.
+    rate : float
+        The rate of convergence.
+    """
+    n = y.shape[0]
+    M_real = MU_REAL / h
+    M_complex = MU_COMPLEX / h
+
+    W = TI.dot(Z0)
+    Z = Z0
+
+    F = np.empty((3, n))
+    ch = h * C
+
+    dW_norm_old = None
+    dW = np.empty_like(W)
+    converged = False
+    rate = None
+    for k in range(NEWTON_MAXITER):
+        for i in range(3):
+            F[i] = fun(t + ch[i], y + Z[i])
+
+        if not np.all(np.isfinite(F)):
+            break
+
+        f_real = F.T.dot(TI_REAL) - M_real * W[0]
+        f_complex = F.T.dot(TI_COMPLEX) - M_complex * (W[1] + 1j * W[2])
+
+        dW_real = solve_lu(LU_real, f_real)
+        dW_complex = solve_lu(LU_complex, f_complex)
+
+        dW[0] = dW_real
+        dW[1] = dW_complex.real
+        dW[2] = dW_complex.imag
+
+        dW_norm = norm(dW / scale)
+        if dW_norm_old is not None:
+            rate = dW_norm / dW_norm_old
+
+        if (rate is not None and (rate >= 1 or
+                rate ** (NEWTON_MAXITER - k) / (1 - rate) * dW_norm > tol)):
+            break
+
+        W += dW
+        Z = T.dot(W)
+
+        if (dW_norm == 0 or
+                rate is not None and rate / (1 - rate) * dW_norm < tol):
+            converged = True
+            break
+
+        dW_norm_old = dW_norm
+
+    return converged, k + 1, Z, rate
+
+
+def predict_factor(h_abs, h_abs_old, error_norm, error_norm_old):
+    """Predict by which factor to increase/decrease the step size.
+
+    The algorithm is described in [1]_.
+
+    Parameters
+    ----------
+    h_abs, h_abs_old : float
+        Current and previous values of the step size, `h_abs_old` can be None
+        (see Notes).
+    error_norm, error_norm_old : float
+        Current and previous values of the error norm, `error_norm_old` can
+        be None (see Notes).
+
+    Returns
+    -------
+    factor : float
+        Predicted factor.
+
+    Notes
+    -----
+    If `h_abs_old` and `error_norm_old` are both not None then a two-step
+    algorithm is used, otherwise a one-step algorithm is used.
+
+    References
+    ----------
+    .. [1] E. Hairer, S. P. Norsett G. Wanner, "Solving Ordinary Differential
+           Equations II: Stiff and Differential-Algebraic Problems", Sec. IV.8.
+    """
+    if error_norm_old is None or h_abs_old is None or error_norm == 0:
+        multiplier = 1
+    else:
+        multiplier = h_abs / h_abs_old * (error_norm_old / error_norm) ** 0.25
+
+    with np.errstate(divide='ignore'):
+        factor = min(1, multiplier) * error_norm ** -0.25
+
+    return factor
+
+
+class Radau(OdeSolver):
+    """Implicit Runge-Kutta method of Radau IIA family of order 5.
+
+    The implementation follows [1]_. The error is controlled with a
+    third-order accurate embedded formula. A cubic polynomial which satisfies
+    the collocation conditions is used for the dense output.
+
+    Parameters
+    ----------
+    fun : callable
+        Right-hand side of the system. The calling signature is ``fun(t, y)``.
+        Here ``t`` is a scalar, and there are two options for the ndarray ``y``:
+        It can either have shape (n,); then ``fun`` must return array_like with
+        shape (n,). Alternatively it can have shape (n, k); then ``fun``
+        must return an array_like with shape (n, k), i.e., each column
+        corresponds to a single column in ``y``. The choice between the two
+        options is determined by `vectorized` argument (see below). The
+        vectorized implementation allows a faster approximation of the Jacobian
+        by finite differences (required for this solver).
+    t0 : float
+        Initial time.
+    y0 : array_like, shape (n,)
+        Initial state.
+    t_bound : float
+        Boundary time - the integration won't continue beyond it. It also
+        determines the direction of the integration.
+    first_step : float or None, optional
+        Initial step size. Default is ``None`` which means that the algorithm
+        should choose.
+    max_step : float, optional
+        Maximum allowed step size. Default is np.inf, i.e., the step size is not
+        bounded and determined solely by the solver.
+    rtol, atol : float and array_like, optional
+        Relative and absolute tolerances. The solver keeps the local error
+        estimates less than ``atol + rtol * abs(y)``. HHere `rtol` controls a
+        relative accuracy (number of correct digits), while `atol` controls
+        absolute accuracy (number of correct decimal places). To achieve the
+        desired `rtol`, set `atol` to be smaller than the smallest value that
+        can be expected from ``rtol * abs(y)`` so that `rtol` dominates the
+        allowable error. If `atol` is larger than ``rtol * abs(y)`` the
+        number of correct digits is not guaranteed. Conversely, to achieve the
+        desired `atol` set `rtol` such that ``rtol * abs(y)`` is always smaller
+        than `atol`. If components of y have different scales, it might be
+        beneficial to set different `atol` values for different components by
+        passing array_like with shape (n,) for `atol`. Default values are
+        1e-3 for `rtol` and 1e-6 for `atol`.
+    jac : {None, array_like, sparse_matrix, callable}, optional
+        Jacobian matrix of the right-hand side of the system with respect to
+        y, required by this method. The Jacobian matrix has shape (n, n) and
+        its element (i, j) is equal to ``d f_i / d y_j``.
+        There are three ways to define the Jacobian:
+
+            * If array_like or sparse_matrix, the Jacobian is assumed to
+              be constant.
+            * If callable, the Jacobian is assumed to depend on both
+              t and y; it will be called as ``jac(t, y)`` as necessary.
+              For the 'Radau' and 'BDF' methods, the return value might be a
+              sparse matrix.
+            * If None (default), the Jacobian will be approximated by
+              finite differences.
+
+        It is generally recommended to provide the Jacobian rather than
+        relying on a finite-difference approximation.
+    jac_sparsity : {None, array_like, sparse matrix}, optional
+        Defines a sparsity structure of the Jacobian matrix for a
+        finite-difference approximation. Its shape must be (n, n). This argument
+        is ignored if `jac` is not `None`. If the Jacobian has only few non-zero
+        elements in *each* row, providing the sparsity structure will greatly
+        speed up the computations [2]_. A zero entry means that a corresponding
+        element in the Jacobian is always zero. If None (default), the Jacobian
+        is assumed to be dense.
+    vectorized : bool, optional
+        Whether `fun` is implemented in a vectorized fashion. Default is False.
+
+    Attributes
+    ----------
+    n : int
+        Number of equations.
+    status : string
+        Current status of the solver: 'running', 'finished' or 'failed'.
+    t_bound : float
+        Boundary time.
+    direction : float
+        Integration direction: +1 or -1.
+    t : float
+        Current time.
+    y : ndarray
+        Current state.
+    t_old : float
+        Previous time. None if no steps were made yet.
+    step_size : float
+        Size of the last successful step. None if no steps were made yet.
+    nfev : int
+        Number of evaluations of the right-hand side.
+    njev : int
+        Number of evaluations of the Jacobian.
+    nlu : int
+        Number of LU decompositions.
+
+    References
+    ----------
+    .. [1] E. Hairer, G. Wanner, "Solving Ordinary Differential Equations II:
+           Stiff and Differential-Algebraic Problems", Sec. IV.8.
+    .. [2] A. Curtis, M. J. D. Powell, and J. Reid, "On the estimation of
+           sparse Jacobian matrices", Journal of the Institute of Mathematics
+           and its Applications, 13, pp. 117-120, 1974.
+    """
+    def __init__(self, fun, t0, y0, t_bound, max_step=np.inf,
+                 rtol=1e-3, atol=1e-6, jac=None, jac_sparsity=None,
+                 vectorized=False, first_step=None, **extraneous):
+        warn_extraneous(extraneous)
+        super().__init__(fun, t0, y0, t_bound, vectorized)
+        self.y_old = None
+        self.max_step = validate_max_step(max_step)
+        self.rtol, self.atol = validate_tol(rtol, atol, self.n)
+        self.f = self.fun(self.t, self.y)
+        # Select initial step assuming the same order which is used to control
+        # the error.
+        if first_step is None:
+            self.h_abs = select_initial_step(
+                self.fun, self.t, self.y, self.f, self.direction,
+                3, self.rtol, self.atol)
+        else:
+            self.h_abs = validate_first_step(first_step, t0, t_bound)
+        self.h_abs_old = None
+        self.error_norm_old = None
+
+        self.newton_tol = max(10 * EPS / rtol, min(0.03, rtol ** 0.5))
+        self.sol = None
+
+        self.jac_factor = None
+        self.jac, self.J = self._validate_jac(jac, jac_sparsity)
+        if issparse(self.J):
+            def lu(A):
+                self.nlu += 1
+                return splu(A)
+
+            def solve_lu(LU, b):
+                return LU.solve(b)
+
+            I = eye(self.n, format='csc')
+        else:
+            def lu(A):
+                self.nlu += 1
+                return lu_factor(A, overwrite_a=True)
+
+            def solve_lu(LU, b):
+                return lu_solve(LU, b, overwrite_b=True)
+
+            I = np.identity(self.n)
+
+        self.lu = lu
+        self.solve_lu = solve_lu
+        self.I = I
+
+        self.current_jac = True
+        self.LU_real = None
+        self.LU_complex = None
+        self.Z = None
+
+    def _validate_jac(self, jac, sparsity):
+        t0 = self.t
+        y0 = self.y
+
+        if jac is None:
+            if sparsity is not None:
+                if issparse(sparsity):
+                    sparsity = csc_matrix(sparsity)
+                groups = group_columns(sparsity)
+                sparsity = (sparsity, groups)
+
+            def jac_wrapped(t, y, f):
+                self.njev += 1
+                J, self.jac_factor = num_jac(self.fun_vectorized, t, y, f,
+                                             self.atol, self.jac_factor,
+                                             sparsity)
+                return J
+            J = jac_wrapped(t0, y0, self.f)
+        elif callable(jac):
+            J = jac(t0, y0)
+            self.njev = 1
+            if issparse(J):
+                J = csc_matrix(J)
+
+                def jac_wrapped(t, y, _=None):
+                    self.njev += 1
+                    return csc_matrix(jac(t, y), dtype=float)
+
+            else:
+                J = np.asarray(J, dtype=float)
+
+                def jac_wrapped(t, y, _=None):
+                    self.njev += 1
+                    return np.asarray(jac(t, y), dtype=float)
+
+            if J.shape != (self.n, self.n):
+                raise ValueError("`jac` is expected to have shape {}, but "
+                                 "actually has {}."
+                                 .format((self.n, self.n), J.shape))
+        else:
+            if issparse(jac):
+                J = csc_matrix(jac)
+            else:
+                J = np.asarray(jac, dtype=float)
+
+            if J.shape != (self.n, self.n):
+                raise ValueError("`jac` is expected to have shape {}, but "
+                                 "actually has {}."
+                                 .format((self.n, self.n), J.shape))
+            jac_wrapped = None
+
+        return jac_wrapped, J
+
+    def _step_impl(self):
+        t = self.t
+        y = self.y
+        f = self.f
+
+        max_step = self.max_step
+        atol = self.atol
+        rtol = self.rtol
+
+        min_step = 10 * np.abs(np.nextafter(t, self.direction * np.inf) - t)
+        if self.h_abs > max_step:
+            h_abs = max_step
+            h_abs_old = None
+            error_norm_old = None
+        elif self.h_abs < min_step:
+            h_abs = min_step
+            h_abs_old = None
+            error_norm_old = None
+        else:
+            h_abs = self.h_abs
+            h_abs_old = self.h_abs_old
+            error_norm_old = self.error_norm_old
+
+        J = self.J
+        LU_real = self.LU_real
+        LU_complex = self.LU_complex
+
+        current_jac = self.current_jac
+        jac = self.jac
+
+        rejected = False
+        step_accepted = False
+        message = None
+        while not step_accepted:
+            if h_abs < min_step:
+                return False, self.TOO_SMALL_STEP
+
+            h = h_abs * self.direction
+            t_new = t + h
+
+            if self.direction * (t_new - self.t_bound) > 0:
+                t_new = self.t_bound
+
+            h = t_new - t
+            h_abs = np.abs(h)
+
+            if self.sol is None:
+                Z0 = np.zeros((3, y.shape[0]))
+            else:
+                Z0 = self.sol(t + h * C).T - y
+
+            scale = atol + np.abs(y) * rtol
+
+            converged = False
+            while not converged:
+                if LU_real is None or LU_complex is None:
+                    LU_real = self.lu(MU_REAL / h * self.I - J)
+                    LU_complex = self.lu(MU_COMPLEX / h * self.I - J)
+
+                converged, n_iter, Z, rate = solve_collocation_system(
+                    self.fun, t, y, h, Z0, scale, self.newton_tol,
+                    LU_real, LU_complex, self.solve_lu)
+
+                if not converged:
+                    if current_jac:
+                        break
+
+                    J = self.jac(t, y, f)
+                    current_jac = True
+                    LU_real = None
+                    LU_complex = None
+
+            if not converged:
+                h_abs *= 0.5
+                LU_real = None
+                LU_complex = None
+                continue
+
+            y_new = y + Z[-1]
+            ZE = Z.T.dot(E) / h
+            error = self.solve_lu(LU_real, f + ZE)
+            scale = atol + np.maximum(np.abs(y), np.abs(y_new)) * rtol
+            error_norm = norm(error / scale)
+            safety = 0.9 * (2 * NEWTON_MAXITER + 1) / (2 * NEWTON_MAXITER
+                                                       + n_iter)
+
+            if rejected and error_norm > 1:
+                error = self.solve_lu(LU_real, self.fun(t, y + error) + ZE)
+                error_norm = norm(error / scale)
+
+            if error_norm > 1:
+                factor = predict_factor(h_abs, h_abs_old,
+                                        error_norm, error_norm_old)
+                h_abs *= max(MIN_FACTOR, safety * factor)
+
+                LU_real = None
+                LU_complex = None
+                rejected = True
+            else:
+                step_accepted = True
+
+        recompute_jac = jac is not None and n_iter > 2 and rate > 1e-3
+
+        factor = predict_factor(h_abs, h_abs_old, error_norm, error_norm_old)
+        factor = min(MAX_FACTOR, safety * factor)
+
+        if not recompute_jac and factor < 1.2:
+            factor = 1
+        else:
+            LU_real = None
+            LU_complex = None
+
+        f_new = self.fun(t_new, y_new)
+        if recompute_jac:
+            J = jac(t_new, y_new, f_new)
+            current_jac = True
+        elif jac is not None:
+            current_jac = False
+
+        self.h_abs_old = self.h_abs
+        self.error_norm_old = error_norm
+
+        self.h_abs = h_abs * factor
+
+        self.y_old = y
+
+        self.t = t_new
+        self.y = y_new
+        self.f = f_new
+
+        self.Z = Z
+
+        self.LU_real = LU_real
+        self.LU_complex = LU_complex
+        self.current_jac = current_jac
+        self.J = J
+
+        self.t_old = t
+        self.sol = self._compute_dense_output()
+
+        return step_accepted, message
+
+    def _compute_dense_output(self):
+        Q = np.dot(self.Z.T, P)
+        return RadauDenseOutput(self.t_old, self.t, self.y_old, Q)
+
+    def _dense_output_impl(self):
+        return self.sol
+
+
+class RadauDenseOutput(DenseOutput):
+    def __init__(self, t_old, t, y_old, Q):
+        super().__init__(t_old, t)
+        self.h = t - t_old
+        self.Q = Q
+        self.order = Q.shape[1] - 1
+        self.y_old = y_old
+
+    def _call_impl(self, t):
+        x = (t - self.t_old) / self.h
+        if t.ndim == 0:
+            p = np.tile(x, self.order + 1)
+            p = np.cumprod(p)
+        else:
+            p = np.tile(x, (self.order + 1, 1))
+            p = np.cumprod(p, axis=0)
+        # Here we don't multiply by h, not a mistake.
+        y = np.dot(self.Q, p)
+        if y.ndim == 2:
+            y += self.y_old[:, None]
+        else:
+            y += self.y_old
+
+        return y

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/_ivp/rk.py

@@ -0,0 +1,587 @@
+import numpy as np
+from .base import OdeSolver, DenseOutput
+from .common import (validate_max_step, validate_tol, select_initial_step,
+                     norm, warn_extraneous, validate_first_step)
+from . import dop853_coefficients
+
+# Multiply steps computed from asymptotic behaviour of errors by this.
+SAFETY = 0.9
+
+MIN_FACTOR = 0.2  # Minimum allowed decrease in a step size.
+MAX_FACTOR = 10  # Maximum allowed increase in a step size.
+
+
+def rk_step(fun, t, y, f, h, A, B, C, K):
+    """Perform a single Runge-Kutta step.
+
+    This function computes a prediction of an explicit Runge-Kutta method and
+    also estimates the error of a less accurate method.
+
+    Notation for Butcher tableau is as in [1]_.
+
+    Parameters
+    ----------
+    fun : callable
+        Right-hand side of the system.
+    t : float
+        Current time.
+    y : ndarray, shape (n,)
+        Current state.
+    f : ndarray, shape (n,)
+        Current value of the derivative, i.e., ``fun(x, y)``.
+    h : float
+        Step to use.
+    A : ndarray, shape (n_stages, n_stages)
+        Coefficients for combining previous RK stages to compute the next
+        stage. For explicit methods the coefficients at and above the main
+        diagonal are zeros.
+    B : ndarray, shape (n_stages,)
+        Coefficients for combining RK stages for computing the final
+        prediction.
+    C : ndarray, shape (n_stages,)
+        Coefficients for incrementing time for consecutive RK stages.
+        The value for the first stage is always zero.
+    K : ndarray, shape (n_stages + 1, n)
+        Storage array for putting RK stages here. Stages are stored in rows.
+        The last row is a linear combination of the previous rows with
+        coefficients
+
+    Returns
+    -------
+    y_new : ndarray, shape (n,)
+        Solution at t + h computed with a higher accuracy.
+    f_new : ndarray, shape (n,)
+        Derivative ``fun(t + h, y_new)``.
+
+    References
+    ----------
+    .. [1] E. Hairer, S. P. Norsett G. Wanner, "Solving Ordinary Differential
+           Equations I: Nonstiff Problems", Sec. II.4.
+    """
+    K[0] = f
+    for s, (a, c) in enumerate(zip(A[1:], C[1:]), start=1):
+        dy = np.dot(K[:s].T, a[:s]) * h
+        K[s] = fun(t + c * h, y + dy)
+
+    y_new = y + h * np.dot(K[:-1].T, B)
+    f_new = fun(t + h, y_new)
+
+    K[-1] = f_new
+
+    return y_new, f_new
+
+
+class RungeKutta(OdeSolver):
+    """Base class for explicit Runge-Kutta methods."""
+    C: np.ndarray = NotImplemented
+    A: np.ndarray = NotImplemented
+    B: np.ndarray = NotImplemented
+    E: np.ndarray = NotImplemented
+    P: np.ndarray = NotImplemented
+    order: int = NotImplemented
+    error_estimator_order: int = NotImplemented
+    n_stages: int = NotImplemented
+
+    def __init__(self, fun, t0, y0, t_bound, max_step=np.inf,
+                 rtol=1e-3, atol=1e-6, vectorized=False,
+                 first_step=None, **extraneous):
+        warn_extraneous(extraneous)
+        super().__init__(fun, t0, y0, t_bound, vectorized,
+                         support_complex=True)
+        self.y_old = None
+        self.max_step = validate_max_step(max_step)
+        self.rtol, self.atol = validate_tol(rtol, atol, self.n)
+        self.f = self.fun(self.t, self.y)
+        if first_step is None:
+            self.h_abs = select_initial_step(
+                self.fun, self.t, self.y, self.f, self.direction,
+                self.error_estimator_order, self.rtol, self.atol)
+        else:
+            self.h_abs = validate_first_step(first_step, t0, t_bound)
+        self.K = np.empty((self.n_stages + 1, self.n), dtype=self.y.dtype)
+        self.error_exponent = -1 / (self.error_estimator_order + 1)
+        self.h_previous = None
+
+    def _estimate_error(self, K, h):
+        return np.dot(K.T, self.E) * h
+
+    def _estimate_error_norm(self, K, h, scale):
+        return norm(self._estimate_error(K, h) / scale)
+
+    def _step_impl(self):
+        t = self.t
+        y = self.y
+
+        max_step = self.max_step
+        rtol = self.rtol
+        atol = self.atol
+
+        min_step = 10 * np.abs(np.nextafter(t, self.direction * np.inf) - t)
+
+        if self.h_abs > max_step:
+            h_abs = max_step
+        elif self.h_abs < min_step:
+            h_abs = min_step
+        else:
+            h_abs = self.h_abs
+
+        step_accepted = False
+        step_rejected = False
+
+        while not step_accepted:
+            if h_abs < min_step:
+                return False, self.TOO_SMALL_STEP
+
+            h = h_abs * self.direction
+            t_new = t + h
+
+            if self.direction * (t_new - self.t_bound) > 0:
+                t_new = self.t_bound
+
+            h = t_new - t
+            h_abs = np.abs(h)
+
+            y_new, f_new = rk_step(self.fun, t, y, self.f, h, self.A,
+                                   self.B, self.C, self.K)
+            scale = atol + np.maximum(np.abs(y), np.abs(y_new)) * rtol
+            error_norm = self._estimate_error_norm(self.K, h, scale)
+
+            if error_norm < 1:
+                if error_norm == 0:
+                    factor = MAX_FACTOR
+                else:
+                    factor = min(MAX_FACTOR,
+                                 SAFETY * error_norm ** self.error_exponent)
+
+                if step_rejected:
+                    factor = min(1, factor)
+
+                h_abs *= factor
+
+                step_accepted = True
+            else:
+                h_abs *= max(MIN_FACTOR,
+                             SAFETY * error_norm ** self.error_exponent)
+                step_rejected = True
+
+        self.h_previous = h
+        self.y_old = y
+
+        self.t = t_new
+        self.y = y_new
+
+        self.h_abs = h_abs
+        self.f = f_new
+
+        return True, None
+
+    def _dense_output_impl(self):
+        Q = self.K.T.dot(self.P)
+        return RkDenseOutput(self.t_old, self.t, self.y_old, Q)
+
+
+class RK23(RungeKutta):
+    """Explicit Runge-Kutta method of order 3(2).
+
+    This uses the Bogacki-Shampine pair of formulas [1]_. The error is controlled
+    assuming accuracy of the second-order method, but steps are taken using the
+    third-order accurate formula (local extrapolation is done). A cubic Hermite
+    polynomial is used for the dense output.
+
+    Can be applied in the complex domain.
+
+    Parameters
+    ----------
+    fun : callable
+        Right-hand side of the system. The calling signature is ``fun(t, y)``.
+        Here ``t`` is a scalar and there are two options for ndarray ``y``.
+        It can either have shape (n,), then ``fun`` must return array_like with
+        shape (n,). Or alternatively it can have shape (n, k), then ``fun``
+        must return array_like with shape (n, k), i.e. each column
+        corresponds to a single column in ``y``. The choice between the two
+        options is determined by `vectorized` argument (see below).
+    t0 : float
+        Initial time.
+    y0 : array_like, shape (n,)
+        Initial state.
+    t_bound : float
+        Boundary time - the integration won't continue beyond it. It also
+        determines the direction of the integration.
+    first_step : float or None, optional
+        Initial step size. Default is ``None`` which means that the algorithm
+        should choose.
+    max_step : float, optional
+        Maximum allowed step size. Default is np.inf, i.e., the step size is not
+        bounded and determined solely by the solver.
+    rtol, atol : float and array_like, optional
+        Relative and absolute tolerances. The solver keeps the local error
+        estimates less than ``atol + rtol * abs(y)``. Here `rtol` controls a
+        relative accuracy (number of correct digits), while `atol` controls
+        absolute accuracy (number of correct decimal places). To achieve the
+        desired `rtol`, set `atol` to be smaller than the smallest value that
+        can be expected from ``rtol * abs(y)`` so that `rtol` dominates the
+        allowable error. If `atol` is larger than ``rtol * abs(y)`` the
+        number of correct digits is not guaranteed. Conversely, to achieve the
+        desired `atol` set `rtol` such that ``rtol * abs(y)`` is always smaller
+        than `atol`. If components of y have different scales, it might be
+        beneficial to set different `atol` values for different components by
+        passing array_like with shape (n,) for `atol`. Default values are
+        1e-3 for `rtol` and 1e-6 for `atol`.
+    vectorized : bool, optional
+        Whether `fun` is implemented in a vectorized fashion. Default is False.
+
+    Attributes
+    ----------
+    n : int
+        Number of equations.
+    status : string
+        Current status of the solver: 'running', 'finished' or 'failed'.
+    t_bound : float
+        Boundary time.
+    direction : float
+        Integration direction: +1 or -1.
+    t : float
+        Current time.
+    y : ndarray
+        Current state.
+    t_old : float
+        Previous time. None if no steps were made yet.
+    step_size : float
+        Size of the last successful step. None if no steps were made yet.
+    nfev : int
+        Number evaluations of the system's right-hand side.
+    njev : int
+        Number of evaluations of the Jacobian. Is always 0 for this solver as it does not use the Jacobian.
+    nlu : int
+        Number of LU decompositions. Is always 0 for this solver.
+
+    References
+    ----------
+    .. [1] P. Bogacki, L.F. Shampine, "A 3(2) Pair of Runge-Kutta Formulas",
+           Appl. Math. Lett. Vol. 2, No. 4. pp. 321-325, 1989.
+    """
+    order = 3
+    error_estimator_order = 2
+    n_stages = 3
+    C = np.array([0, 1/2, 3/4])
+    A = np.array([
+        [0, 0, 0],
+        [1/2, 0, 0],
+        [0, 3/4, 0]
+    ])
+    B = np.array([2/9, 1/3, 4/9])
+    E = np.array([5/72, -1/12, -1/9, 1/8])
+    P = np.array([[1, -4 / 3, 5 / 9],
+                  [0, 1, -2/3],
+                  [0, 4/3, -8/9],
+                  [0, -1, 1]])
+
+
+class RK45(RungeKutta):
+    """Explicit Runge-Kutta method of order 5(4).
+
+    This uses the Dormand-Prince pair of formulas [1]_. The error is controlled
+    assuming accuracy of the fourth-order method accuracy, but steps are taken
+    using the fifth-order accurate formula (local extrapolation is done).
+    A quartic interpolation polynomial is used for the dense output [2]_.
+
+    Can be applied in the complex domain.
+
+    Parameters
+    ----------
+    fun : callable
+        Right-hand side of the system. The calling signature is ``fun(t, y)``.
+        Here ``t`` is a scalar, and there are two options for the ndarray ``y``:
+        It can either have shape (n,); then ``fun`` must return array_like with
+        shape (n,). Alternatively it can have shape (n, k); then ``fun``
+        must return an array_like with shape (n, k), i.e., each column
+        corresponds to a single column in ``y``. The choice between the two
+        options is determined by `vectorized` argument (see below).
+    t0 : float
+        Initial time.
+    y0 : array_like, shape (n,)
+        Initial state.
+    t_bound : float
+        Boundary time - the integration won't continue beyond it. It also
+        determines the direction of the integration.
+    first_step : float or None, optional
+        Initial step size. Default is ``None`` which means that the algorithm
+        should choose.
+    max_step : float, optional
+        Maximum allowed step size. Default is np.inf, i.e., the step size is not
+        bounded and determined solely by the solver.
+    rtol, atol : float and array_like, optional
+        Relative and absolute tolerances. The solver keeps the local error
+        estimates less than ``atol + rtol * abs(y)``. Here `rtol` controls a
+        relative accuracy (number of correct digits), while `atol` controls
+        absolute accuracy (number of correct decimal places). To achieve the
+        desired `rtol`, set `atol` to be smaller than the smallest value that
+        can be expected from ``rtol * abs(y)`` so that `rtol` dominates the
+        allowable error. If `atol` is larger than ``rtol * abs(y)`` the
+        number of correct digits is not guaranteed. Conversely, to achieve the
+        desired `atol` set `rtol` such that ``rtol * abs(y)`` is always smaller
+        than `atol`. If components of y have different scales, it might be
+        beneficial to set different `atol` values for different components by
+        passing array_like with shape (n,) for `atol`. Default values are
+        1e-3 for `rtol` and 1e-6 for `atol`.
+    vectorized : bool, optional
+        Whether `fun` is implemented in a vectorized fashion. Default is False.
+
+    Attributes
+    ----------
+    n : int
+        Number of equations.
+    status : string
+        Current status of the solver: 'running', 'finished' or 'failed'.
+    t_bound : float
+        Boundary time.
+    direction : float
+        Integration direction: +1 or -1.
+    t : float
+        Current time.
+    y : ndarray
+        Current state.
+    t_old : float
+        Previous time. None if no steps were made yet.
+    step_size : float
+        Size of the last successful step. None if no steps were made yet.
+    nfev : int
+        Number evaluations of the system's right-hand side.
+    njev : int
+        Number of evaluations of the Jacobian. Is always 0 for this solver as it does not use the Jacobian.
+    nlu : int
+        Number of LU decompositions. Is always 0 for this solver.
+
+    References
+    ----------
+    .. [1] J. R. Dormand, P. J. Prince, "A family of embedded Runge-Kutta
+           formulae", Journal of Computational and Applied Mathematics, Vol. 6,
+           No. 1, pp. 19-26, 1980.
+    .. [2] L. W. Shampine, "Some Practical Runge-Kutta Formulas", Mathematics
+           of Computation,, Vol. 46, No. 173, pp. 135-150, 1986.
+    """
+    order = 5
+    error_estimator_order = 4
+    n_stages = 6
+    C = np.array([0, 1/5, 3/10, 4/5, 8/9, 1])
+    A = np.array([
+        [0, 0, 0, 0, 0],
+        [1/5, 0, 0, 0, 0],
+        [3/40, 9/40, 0, 0, 0],
+        [44/45, -56/15, 32/9, 0, 0],
+        [19372/6561, -25360/2187, 64448/6561, -212/729, 0],
+        [9017/3168, -355/33, 46732/5247, 49/176, -5103/18656]
+    ])
+    B = np.array([35/384, 0, 500/1113, 125/192, -2187/6784, 11/84])
+    E = np.array([-71/57600, 0, 71/16695, -71/1920, 17253/339200, -22/525,
+                  1/40])
+    # Corresponds to the optimum value of c_6 from [2]_.
+    P = np.array([
+        [1, -8048581381/2820520608, 8663915743/2820520608,
+         -12715105075/11282082432],
+        [0, 0, 0, 0],
+        [0, 131558114200/32700410799, -68118460800/10900136933,
+         87487479700/32700410799],
+        [0, -1754552775/470086768, 14199869525/1410260304,
+         -10690763975/1880347072],
+        [0, 127303824393/49829197408, -318862633887/49829197408,
+         701980252875 / 199316789632],
+        [0, -282668133/205662961, 2019193451/616988883, -1453857185/822651844],
+        [0, 40617522/29380423, -110615467/29380423, 69997945/29380423]])
+
+
+class DOP853(RungeKutta):
+    """Explicit Runge-Kutta method of order 8.
+
+    This is a Python implementation of "DOP853" algorithm originally written
+    in Fortran [1]_, [2]_. Note that this is not a literate translation, but
+    the algorithmic core and coefficients are the same.
+
+    Can be applied in the complex domain.
+
+    Parameters
+    ----------
+    fun : callable
+        Right-hand side of the system. The calling signature is ``fun(t, y)``.
+        Here, ``t`` is a scalar, and there are two options for the ndarray ``y``:
+        It can either have shape (n,); then ``fun`` must return array_like with
+        shape (n,). Alternatively it can have shape (n, k); then ``fun``
+        must return an array_like with shape (n, k), i.e. each column
+        corresponds to a single column in ``y``. The choice between the two
+        options is determined by `vectorized` argument (see below).
+    t0 : float
+        Initial time.
+    y0 : array_like, shape (n,)
+        Initial state.
+    t_bound : float
+        Boundary time - the integration won't continue beyond it. It also
+        determines the direction of the integration.
+    first_step : float or None, optional
+        Initial step size. Default is ``None`` which means that the algorithm
+        should choose.
+    max_step : float, optional
+        Maximum allowed step size. Default is np.inf, i.e. the step size is not
+        bounded and determined solely by the solver.
+    rtol, atol : float and array_like, optional
+        Relative and absolute tolerances. The solver keeps the local error
+        estimates less than ``atol + rtol * abs(y)``. Here `rtol` controls a
+        relative accuracy (number of correct digits), while `atol` controls
+        absolute accuracy (number of correct decimal places). To achieve the
+        desired `rtol`, set `atol` to be smaller than the smallest value that
+        can be expected from ``rtol * abs(y)`` so that `rtol` dominates the
+        allowable error. If `atol` is larger than ``rtol * abs(y)`` the
+        number of correct digits is not guaranteed. Conversely, to achieve the
+        desired `atol` set `rtol` such that ``rtol * abs(y)`` is always smaller
+        than `atol`. If components of y have different scales, it might be
+        beneficial to set different `atol` values for different components by
+        passing array_like with shape (n,) for `atol`. Default values are
+        1e-3 for `rtol` and 1e-6 for `atol`.
+    vectorized : bool, optional
+        Whether `fun` is implemented in a vectorized fashion. Default is False.
+
+    Attributes
+    ----------
+    n : int
+        Number of equations.
+    status : string
+        Current status of the solver: 'running', 'finished' or 'failed'.
+    t_bound : float
+        Boundary time.
+    direction : float
+        Integration direction: +1 or -1.
+    t : float
+        Current time.
+    y : ndarray
+        Current state.
+    t_old : float
+        Previous time. None if no steps were made yet.
+    step_size : float
+        Size of the last successful step. None if no steps were made yet.
+    nfev : int
+        Number evaluations of the system's right-hand side.
+    njev : int
+        Number of evaluations of the Jacobian. Is always 0 for this solver
+        as it does not use the Jacobian.
+    nlu : int
+        Number of LU decompositions. Is always 0 for this solver.
+
+    References
+    ----------
+    .. [1] E. Hairer, S. P. Norsett G. Wanner, "Solving Ordinary Differential
+           Equations I: Nonstiff Problems", Sec. II.
+    .. [2] `Page with original Fortran code of DOP853
+            <http://www.unige.ch/~hairer/software.html>`_.
+    """
+    n_stages = dop853_coefficients.N_STAGES
+    order = 8
+    error_estimator_order = 7
+    A = dop853_coefficients.A[:n_stages, :n_stages]
+    B = dop853_coefficients.B
+    C = dop853_coefficients.C[:n_stages]
+    E3 = dop853_coefficients.E3
+    E5 = dop853_coefficients.E5
+    D = dop853_coefficients.D
+
+    A_EXTRA = dop853_coefficients.A[n_stages + 1:]
+    C_EXTRA = dop853_coefficients.C[n_stages + 1:]
+
+    def __init__(self, fun, t0, y0, t_bound, max_step=np.inf,
+                 rtol=1e-3, atol=1e-6, vectorized=False,
+                 first_step=None, **extraneous):
+        super().__init__(fun, t0, y0, t_bound, max_step, rtol, atol,
+                         vectorized, first_step, **extraneous)
+        self.K_extended = np.empty((dop853_coefficients.N_STAGES_EXTENDED,
+                                    self.n), dtype=self.y.dtype)
+        self.K = self.K_extended[:self.n_stages + 1]
+
+    def _estimate_error(self, K, h):  # Left for testing purposes.
+        err5 = np.dot(K.T, self.E5)
+        err3 = np.dot(K.T, self.E3)
+        denom = np.hypot(np.abs(err5), 0.1 * np.abs(err3))
+        correction_factor = np.ones_like(err5)
+        mask = denom > 0
+        correction_factor[mask] = np.abs(err5[mask]) / denom[mask]
+        return h * err5 * correction_factor
+
+    def _estimate_error_norm(self, K, h, scale):
+        err5 = np.dot(K.T, self.E5) / scale
+        err3 = np.dot(K.T, self.E3) / scale
+        err5_norm_2 = np.linalg.norm(err5)**2
+        err3_norm_2 = np.linalg.norm(err3)**2
+        if err5_norm_2 == 0 and err3_norm_2 == 0:
+            return 0.0
+        denom = err5_norm_2 + 0.01 * err3_norm_2
+        return np.abs(h) * err5_norm_2 / np.sqrt(denom * len(scale))
+
+    def _dense_output_impl(self):
+        K = self.K_extended
+        h = self.h_previous
+        for s, (a, c) in enumerate(zip(self.A_EXTRA, self.C_EXTRA),
+                                   start=self.n_stages + 1):
+            dy = np.dot(K[:s].T, a[:s]) * h
+            K[s] = self.fun(self.t_old + c * h, self.y_old + dy)
+
+        F = np.empty((dop853_coefficients.INTERPOLATOR_POWER, self.n),
+                     dtype=self.y_old.dtype)
+
+        f_old = K[0]
+        delta_y = self.y - self.y_old
+
+        F[0] = delta_y
+        F[1] = h * f_old - delta_y
+        F[2] = 2 * delta_y - h * (self.f + f_old)
+        F[3:] = h * np.dot(self.D, K)
+
+        return Dop853DenseOutput(self.t_old, self.t, self.y_old, F)
+
+
+class RkDenseOutput(DenseOutput):
+    def __init__(self, t_old, t, y_old, Q):
+        super().__init__(t_old, t)
+        self.h = t - t_old
+        self.Q = Q
+        self.order = Q.shape[1] - 1
+        self.y_old = y_old
+
+    def _call_impl(self, t):
+        x = (t - self.t_old) / self.h
+        if t.ndim == 0:
+            p = np.tile(x, self.order + 1)
+            p = np.cumprod(p)
+        else:
+            p = np.tile(x, (self.order + 1, 1))
+            p = np.cumprod(p, axis=0)
+        y = self.h * np.dot(self.Q, p)
+        if y.ndim == 2:
+            y += self.y_old[:, None]
+        else:
+            y += self.y_old
+
+        return y
+
+
+class Dop853DenseOutput(DenseOutput):
+    def __init__(self, t_old, t, y_old, F):
+        super().__init__(t_old, t)
+        self.h = t - t_old
+        self.F = F
+        self.y_old = y_old
+
+    def _call_impl(self, t):
+        x = (t - self.t_old) / self.h
+
+        if t.ndim == 0:
+            y = np.zeros_like(self.y_old)
+        else:
+            x = x[:, None]
+            y = np.zeros((len(x), len(self.y_old)), dtype=self.y_old.dtype)
+
+        for i, f in enumerate(reversed(self.F)):
+            y += f
+            if i % 2 == 0:
+                y *= x
+            else:
+                y *= 1 - x
+        y += self.y_old
+
+        return y.T

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/_ivp/tests/test_rk.py

@@ -0,0 +1,37 @@
+import pytest
+from numpy.testing import assert_allclose, assert_
+import numpy as np
+from scipy.integrate import RK23, RK45, DOP853
+from scipy.integrate._ivp import dop853_coefficients
+
+
+@pytest.mark.parametrize("solver", [RK23, RK45, DOP853])
+def test_coefficient_properties(solver):
+    assert_allclose(np.sum(solver.B), 1, rtol=1e-15)
+    assert_allclose(np.sum(solver.A, axis=1), solver.C, rtol=1e-14)
+
+
+def test_coefficient_properties_dop853():
+    assert_allclose(np.sum(dop853_coefficients.B), 1, rtol=1e-15)
+    assert_allclose(np.sum(dop853_coefficients.A, axis=1),
+                    dop853_coefficients.C,
+                    rtol=1e-14)
+
+
+@pytest.mark.parametrize("solver_class", [RK23, RK45, DOP853])
+def test_error_estimation(solver_class):
+    step = 0.2
+    solver = solver_class(lambda t, y: y, 0, [1], 1, first_step=step)
+    solver.step()
+    error_estimate = solver._estimate_error(solver.K, step)
+    error = solver.y - np.exp([step])
+    assert_(np.abs(error) < np.abs(error_estimate))
+
+
+@pytest.mark.parametrize("solver_class", [RK23, RK45, DOP853])
+def test_error_estimation_complex(solver_class):
+    h = 0.2
+    solver = solver_class(lambda t, y: 1j * y, 0, [1j], 1, first_step=h)
+    solver.step()
+    err_norm = solver._estimate_error_norm(solver.K, h, scale=[1])
+    assert np.isrealobj(err_norm)

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/_odepack_py.py

@@ -0,0 +1,260 @@
+# Author: Travis Oliphant
+
+__all__ = ['odeint']
+
+import numpy as np
+from . import _odepack
+from copy import copy
+import warnings
+
+
+class ODEintWarning(Warning):
+    pass
+
+
+_msgs = {2: "Integration successful.",
+         1: "Nothing was done; the integration time was 0.",
+         -1: "Excess work done on this call (perhaps wrong Dfun type).",
+         -2: "Excess accuracy requested (tolerances too small).",
+         -3: "Illegal input detected (internal error).",
+         -4: "Repeated error test failures (internal error).",
+         -5: "Repeated convergence failures (perhaps bad Jacobian or tolerances).",
+         -6: "Error weight became zero during problem.",
+         -7: "Internal workspace insufficient to finish (internal error).",
+         -8: "Run terminated (internal error)."
+         }
+
+
+def odeint(func, y0, t, args=(), Dfun=None, col_deriv=0, full_output=0,
+           ml=None, mu=None, rtol=None, atol=None, tcrit=None, h0=0.0,
+           hmax=0.0, hmin=0.0, ixpr=0, mxstep=0, mxhnil=0, mxordn=12,
+           mxords=5, printmessg=0, tfirst=False):
+    """
+    Integrate a system of ordinary differential equations.
+
+    .. note:: For new code, use `scipy.integrate.solve_ivp` to solve a
+              differential equation.
+
+    Solve a system of ordinary differential equations using lsoda from the
+    FORTRAN library odepack.
+
+    Solves the initial value problem for stiff or non-stiff systems
+    of first order ode-s::
+
+        dy/dt = func(y, t, ...)  [or func(t, y, ...)]
+
+    where y can be a vector.
+
+    .. note:: By default, the required order of the first two arguments of
+              `func` are in the opposite order of the arguments in the system
+              definition function used by the `scipy.integrate.ode` class and
+              the function `scipy.integrate.solve_ivp`. To use a function with
+              the signature ``func(t, y, ...)``, the argument `tfirst` must be
+              set to ``True``.
+
+    Parameters
+    ----------
+    func : callable(y, t, ...) or callable(t, y, ...)
+        Computes the derivative of y at t.
+        If the signature is ``callable(t, y, ...)``, then the argument
+        `tfirst` must be set ``True``.
+    y0 : array
+        Initial condition on y (can be a vector).
+    t : array
+        A sequence of time points for which to solve for y. The initial
+        value point should be the first element of this sequence.
+        This sequence must be monotonically increasing or monotonically
+        decreasing; repeated values are allowed.
+    args : tuple, optional
+        Extra arguments to pass to function.
+    Dfun : callable(y, t, ...) or callable(t, y, ...)
+        Gradient (Jacobian) of `func`.
+        If the signature is ``callable(t, y, ...)``, then the argument
+        `tfirst` must be set ``True``.
+    col_deriv : bool, optional
+        True if `Dfun` defines derivatives down columns (faster),
+        otherwise `Dfun` should define derivatives across rows.
+    full_output : bool, optional
+        True if to return a dictionary of optional outputs as the second output
+    printmessg : bool, optional
+        Whether to print the convergence message
+    tfirst : bool, optional
+        If True, the first two arguments of `func` (and `Dfun`, if given)
+        must ``t, y`` instead of the default ``y, t``.
+
+        .. versionadded:: 1.1.0
+
+    Returns
+    -------
+    y : array, shape (len(t), len(y0))
+        Array containing the value of y for each desired time in t,
+        with the initial value `y0` in the first row.
+    infodict : dict, only returned if full_output == True
+        Dictionary containing additional output information
+
+        =======  ============================================================
+        key      meaning
+        =======  ============================================================
+        'hu'     vector of step sizes successfully used for each time step
+        'tcur'   vector with the value of t reached for each time step
+                 (will always be at least as large as the input times)
+        'tolsf'  vector of tolerance scale factors, greater than 1.0,
+                 computed when a request for too much accuracy was detected
+        'tsw'    value of t at the time of the last method switch
+                 (given for each time step)
+        'nst'    cumulative number of time steps
+        'nfe'    cumulative number of function evaluations for each time step
+        'nje'    cumulative number of jacobian evaluations for each time step
+        'nqu'    a vector of method orders for each successful step
+        'imxer'  index of the component of largest magnitude in the
+                 weighted local error vector (e / ewt) on an error return, -1
+                 otherwise
+        'lenrw'  the length of the double work array required
+        'leniw'  the length of integer work array required
+        'mused'  a vector of method indicators for each successful time step:
+                 1: adams (nonstiff), 2: bdf (stiff)
+        =======  ============================================================
+
+    Other Parameters
+    ----------------
+    ml, mu : int, optional
+        If either of these are not None or non-negative, then the
+        Jacobian is assumed to be banded. These give the number of
+        lower and upper non-zero diagonals in this banded matrix.
+        For the banded case, `Dfun` should return a matrix whose
+        rows contain the non-zero bands (starting with the lowest diagonal).
+        Thus, the return matrix `jac` from `Dfun` should have shape
+        ``(ml + mu + 1, len(y0))`` when ``ml >=0`` or ``mu >=0``.
+        The data in `jac` must be stored such that ``jac[i - j + mu, j]``
+        holds the derivative of the `i`th equation with respect to the `j`th
+        state variable.  If `col_deriv` is True, the transpose of this
+        `jac` must be returned.
+    rtol, atol : float, optional
+        The input parameters `rtol` and `atol` determine the error
+        control performed by the solver.  The solver will control the
+        vector, e, of estimated local errors in y, according to an
+        inequality of the form ``max-norm of (e / ewt) <= 1``,
+        where ewt is a vector of positive error weights computed as
+        ``ewt = rtol * abs(y) + atol``.
+        rtol and atol can be either vectors the same length as y or scalars.
+        Defaults to 1.49012e-8.
+    tcrit : ndarray, optional
+        Vector of critical points (e.g., singularities) where integration
+        care should be taken.
+    h0 : float, (0: solver-determined), optional
+        The step size to be attempted on the first step.
+    hmax : float, (0: solver-determined), optional
+        The maximum absolute step size allowed.
+    hmin : float, (0: solver-determined), optional
+        The minimum absolute step size allowed.
+    ixpr : bool, optional
+        Whether to generate extra printing at method switches.
+    mxstep : int, (0: solver-determined), optional
+        Maximum number of (internally defined) steps allowed for each
+        integration point in t.
+    mxhnil : int, (0: solver-determined), optional
+        Maximum number of messages printed.
+    mxordn : int, (0: solver-determined), optional
+        Maximum order to be allowed for the non-stiff (Adams) method.
+    mxords : int, (0: solver-determined), optional
+        Maximum order to be allowed for the stiff (BDF) method.
+
+    See Also
+    --------
+    solve_ivp : solve an initial value problem for a system of ODEs
+    ode : a more object-oriented integrator based on VODE
+    quad : for finding the area under a curve
+
+    Examples
+    --------
+    The second order differential equation for the angle `theta` of a
+    pendulum acted on by gravity with friction can be written::
+
+        theta''(t) + b*theta'(t) + c*sin(theta(t)) = 0
+
+    where `b` and `c` are positive constants, and a prime (') denotes a
+    derivative. To solve this equation with `odeint`, we must first convert
+    it to a system of first order equations. By defining the angular
+    velocity ``omega(t) = theta'(t)``, we obtain the system::
+
+        theta'(t) = omega(t)
+        omega'(t) = -b*omega(t) - c*sin(theta(t))
+
+    Let `y` be the vector [`theta`, `omega`]. We implement this system
+    in Python as:
+
+    >>> import numpy as np
+    >>> def pend(y, t, b, c):
+    ...     theta, omega = y
+    ...     dydt = [omega, -b*omega - c*np.sin(theta)]
+    ...     return dydt
+    ...
+
+    We assume the constants are `b` = 0.25 and `c` = 5.0:
+
+    >>> b = 0.25
+    >>> c = 5.0
+
+    For initial conditions, we assume the pendulum is nearly vertical
+    with `theta(0)` = `pi` - 0.1, and is initially at rest, so
+    `omega(0)` = 0.  Then the vector of initial conditions is
+
+    >>> y0 = [np.pi - 0.1, 0.0]
+
+    We will generate a solution at 101 evenly spaced samples in the interval
+    0 <= `t` <= 10.  So our array of times is:
+
+    >>> t = np.linspace(0, 10, 101)
+
+    Call `odeint` to generate the solution. To pass the parameters
+    `b` and `c` to `pend`, we give them to `odeint` using the `args`
+    argument.
+
+    >>> from scipy.integrate import odeint
+    >>> sol = odeint(pend, y0, t, args=(b, c))
+
+    The solution is an array with shape (101, 2). The first column
+    is `theta(t)`, and the second is `omega(t)`. The following code
+    plots both components.
+
+    >>> import matplotlib.pyplot as plt
+    >>> plt.plot(t, sol[:, 0], 'b', label='theta(t)')
+    >>> plt.plot(t, sol[:, 1], 'g', label='omega(t)')
+    >>> plt.legend(loc='best')
+    >>> plt.xlabel('t')
+    >>> plt.grid()
+    >>> plt.show()
+    """
+
+    if ml is None:
+        ml = -1  # changed to zero inside function call
+    if mu is None:
+        mu = -1  # changed to zero inside function call
+
+    dt = np.diff(t)
+    if not ((dt >= 0).all() or (dt <= 0).all()):
+        raise ValueError("The values in t must be monotonically increasing "
+                         "or monotonically decreasing; repeated values are "
+                         "allowed.")
+
+    t = copy(t)
+    y0 = copy(y0)
+    output = _odepack.odeint(func, y0, t, args, Dfun, col_deriv, ml, mu,
+                             full_output, rtol, atol, tcrit, h0, hmax, hmin,
+                             ixpr, mxstep, mxhnil, mxordn, mxords,
+                             int(bool(tfirst)))
+    if output[-1] < 0:
+        warning_msg = _msgs[output[-1]] + " Run with full_output = 1 to get quantitative information."
+        warnings.warn(warning_msg, ODEintWarning)
+    elif printmessg:
+        warning_msg = _msgs[output[-1]]
+        warnings.warn(warning_msg, ODEintWarning)
+
+    if full_output:
+        output[1]['message'] = _msgs[output[-1]]
+
+    output = output[:-1]
+    if len(output) == 1:
+        return output[0]
+    else:
+        return output

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/_quad_vec.py

@@ -0,0 +1,653 @@
+import sys
+import copy
+import heapq
+import collections
+import functools
+
+import numpy as np
+
+from scipy._lib._util import MapWrapper, _FunctionWrapper
+
+
+class LRUDict(collections.OrderedDict):
+    def __init__(self, max_size):
+        self.__max_size = max_size
+
+    def __setitem__(self, key, value):
+        existing_key = (key in self)
+        super().__setitem__(key, value)
+        if existing_key:
+            self.move_to_end(key)
+        elif len(self) > self.__max_size:
+            self.popitem(last=False)
+
+    def update(self, other):
+        # Not needed below
+        raise NotImplementedError()
+
+
+class SemiInfiniteFunc:
+    """
+    Argument transform from (start, +-oo) to (0, 1)
+    """
+    def __init__(self, func, start, infty):
+        self._func = func
+        self._start = start
+        self._sgn = -1 if infty < 0 else 1
+
+        # Overflow threshold for the 1/t**2 factor
+        self._tmin = sys.float_info.min**0.5
+
+    def get_t(self, x):
+        z = self._sgn * (x - self._start) + 1
+        if z == 0:
+            # Can happen only if point not in range
+            return np.inf
+        return 1 / z
+
+    def __call__(self, t):
+        if t < self._tmin:
+            return 0.0
+        else:
+            x = self._start + self._sgn * (1 - t) / t
+            f = self._func(x)
+            return self._sgn * (f / t) / t
+
+
+class DoubleInfiniteFunc:
+    """
+    Argument transform from (-oo, oo) to (-1, 1)
+    """
+    def __init__(self, func):
+        self._func = func
+
+        # Overflow threshold for the 1/t**2 factor
+        self._tmin = sys.float_info.min**0.5
+
+    def get_t(self, x):
+        s = -1 if x < 0 else 1
+        return s / (abs(x) + 1)
+
+    def __call__(self, t):
+        if abs(t) < self._tmin:
+            return 0.0
+        else:
+            x = (1 - abs(t)) / t
+            f = self._func(x)
+            return (f / t) / t
+
+
+def _max_norm(x):
+    return np.amax(abs(x))
+
+
+def _get_sizeof(obj):
+    try:
+        return sys.getsizeof(obj)
+    except TypeError:
+        # occurs on pypy
+        if hasattr(obj, '__sizeof__'):
+            return int(obj.__sizeof__())
+        return 64
+
+
+class _Bunch:
+    def __init__(self, **kwargs):
+        self.__keys = kwargs.keys()
+        self.__dict__.update(**kwargs)
+
+    def __repr__(self):
+        return "_Bunch({})".format(", ".join("{}={}".format(k, repr(self.__dict__[k]))
+                                             for k in self.__keys))
+
+
+def quad_vec(f, a, b, epsabs=1e-200, epsrel=1e-8, norm='2', cache_size=100e6, limit=10000,
+             workers=1, points=None, quadrature=None, full_output=False,
+             *, args=()):
+    r"""Adaptive integration of a vector-valued function.
+
+    Parameters
+    ----------
+    f : callable
+        Vector-valued function f(x) to integrate.
+    a : float
+        Initial point.
+    b : float
+        Final point.
+    epsabs : float, optional
+        Absolute tolerance.
+    epsrel : float, optional
+        Relative tolerance.
+    norm : {'max', '2'}, optional
+        Vector norm to use for error estimation.
+    cache_size : int, optional
+        Number of bytes to use for memoization.
+    limit : float or int, optional
+        An upper bound on the number of subintervals used in the adaptive
+        algorithm.
+    workers : int or map-like callable, optional
+        If `workers` is an integer, part of the computation is done in
+        parallel subdivided to this many tasks (using
+        :class:`python:multiprocessing.pool.Pool`).
+        Supply `-1` to use all cores available to the Process.
+        Alternatively, supply a map-like callable, such as
+        :meth:`python:multiprocessing.pool.Pool.map` for evaluating the
+        population in parallel.
+        This evaluation is carried out as ``workers(func, iterable)``.
+    points : list, optional
+        List of additional breakpoints.
+    quadrature : {'gk21', 'gk15', 'trapezoid'}, optional
+        Quadrature rule to use on subintervals.
+        Options: 'gk21' (Gauss-Kronrod 21-point rule),
+        'gk15' (Gauss-Kronrod 15-point rule),
+        'trapezoid' (composite trapezoid rule).
+        Default: 'gk21' for finite intervals and 'gk15' for (semi-)infinite
+    full_output : bool, optional
+        Return an additional ``info`` dictionary.
+    args : tuple, optional
+        Extra arguments to pass to function, if any.
+
+        .. versionadded:: 1.8.0
+
+    Returns
+    -------
+    res : {float, array-like}
+        Estimate for the result
+    err : float
+        Error estimate for the result in the given norm
+    info : dict
+        Returned only when ``full_output=True``.
+        Info dictionary. Is an object with the attributes:
+
+            success : bool
+                Whether integration reached target precision.
+            status : int
+                Indicator for convergence, success (0),
+                failure (1), and failure due to rounding error (2).
+            neval : int
+                Number of function evaluations.
+            intervals : ndarray, shape (num_intervals, 2)
+                Start and end points of subdivision intervals.
+            integrals : ndarray, shape (num_intervals, ...)
+                Integral for each interval.
+                Note that at most ``cache_size`` values are recorded,
+                and the array may contains *nan* for missing items.
+            errors : ndarray, shape (num_intervals,)
+                Estimated integration error for each interval.
+
+    Notes
+    -----
+    The algorithm mainly follows the implementation of QUADPACK's
+    DQAG* algorithms, implementing global error control and adaptive
+    subdivision.
+
+    The algorithm here has some differences to the QUADPACK approach:
+
+    Instead of subdividing one interval at a time, the algorithm
+    subdivides N intervals with largest errors at once. This enables
+    (partial) parallelization of the integration.
+
+    The logic of subdividing "next largest" intervals first is then
+    not implemented, and we rely on the above extension to avoid
+    concentrating on "small" intervals only.
+
+    The Wynn epsilon table extrapolation is not used (QUADPACK uses it
+    for infinite intervals). This is because the algorithm here is
+    supposed to work on vector-valued functions, in an user-specified
+    norm, and the extension of the epsilon algorithm to this case does
+    not appear to be widely agreed. For max-norm, using elementwise
+    Wynn epsilon could be possible, but we do not do this here with
+    the hope that the epsilon extrapolation is mainly useful in
+    special cases.
+
+    References
+    ----------
+    [1] R. Piessens, E. de Doncker, QUADPACK (1983).
+
+    Examples
+    --------
+    We can compute integrations of a vector-valued function:
+
+    >>> from scipy.integrate import quad_vec
+    >>> import numpy as np
+    >>> import matplotlib.pyplot as plt
+    >>> alpha = np.linspace(0.0, 2.0, num=30)
+    >>> f = lambda x: x**alpha
+    >>> x0, x1 = 0, 2
+    >>> y, err = quad_vec(f, x0, x1)
+    >>> plt.plot(alpha, y)
+    >>> plt.xlabel(r"$\alpha$")
+    >>> plt.ylabel(r"$\int_{0}^{2} x^\alpha dx$")
+    >>> plt.show()
+
+    """
+    a = float(a)
+    b = float(b)
+
+    if args:
+        if not isinstance(args, tuple):
+            args = (args,)
+
+        # create a wrapped function to allow the use of map and Pool.map
+        f = _FunctionWrapper(f, args)
+
+    # Use simple transformations to deal with integrals over infinite
+    # intervals.
+    kwargs = dict(epsabs=epsabs,
+                  epsrel=epsrel,
+                  norm=norm,
+                  cache_size=cache_size,
+                  limit=limit,
+                  workers=workers,
+                  points=points,
+                  quadrature='gk15' if quadrature is None else quadrature,
+                  full_output=full_output)
+    if np.isfinite(a) and np.isinf(b):
+        f2 = SemiInfiniteFunc(f, start=a, infty=b)
+        if points is not None:
+            kwargs['points'] = tuple(f2.get_t(xp) for xp in points)
+        return quad_vec(f2, 0, 1, **kwargs)
+    elif np.isfinite(b) and np.isinf(a):
+        f2 = SemiInfiniteFunc(f, start=b, infty=a)
+        if points is not None:
+            kwargs['points'] = tuple(f2.get_t(xp) for xp in points)
+        res = quad_vec(f2, 0, 1, **kwargs)
+        return (-res[0],) + res[1:]
+    elif np.isinf(a) and np.isinf(b):
+        sgn = -1 if b < a else 1
+
+        # NB. explicitly split integral at t=0, which separates
+        # the positive and negative sides
+        f2 = DoubleInfiniteFunc(f)
+        if points is not None:
+            kwargs['points'] = (0,) + tuple(f2.get_t(xp) for xp in points)
+        else:
+            kwargs['points'] = (0,)
+
+        if a != b:
+            res = quad_vec(f2, -1, 1, **kwargs)
+        else:
+            res = quad_vec(f2, 1, 1, **kwargs)
+
+        return (res[0]*sgn,) + res[1:]
+    elif not (np.isfinite(a) and np.isfinite(b)):
+        raise ValueError("invalid integration bounds a={}, b={}".format(a, b))
+
+    norm_funcs = {
+        None: _max_norm,
+        'max': _max_norm,
+        '2': np.linalg.norm
+    }
+    if callable(norm):
+        norm_func = norm
+    else:
+        norm_func = norm_funcs[norm]
+
+    parallel_count = 128
+    min_intervals = 2
+
+    try:
+        _quadrature = {None: _quadrature_gk21,
+                       'gk21': _quadrature_gk21,
+                       'gk15': _quadrature_gk15,
+                       'trapz': _quadrature_trapezoid,  # alias for backcompat
+                       'trapezoid': _quadrature_trapezoid}[quadrature]
+    except KeyError as e:
+        raise ValueError("unknown quadrature {!r}".format(quadrature)) from e
+
+    # Initial interval set
+    if points is None:
+        initial_intervals = [(a, b)]
+    else:
+        prev = a
+        initial_intervals = []
+        for p in sorted(points):
+            p = float(p)
+            if not (a < p < b) or p == prev:
+                continue
+            initial_intervals.append((prev, p))
+            prev = p
+        initial_intervals.append((prev, b))
+
+    global_integral = None
+    global_error = None
+    rounding_error = None
+    interval_cache = None
+    intervals = []
+    neval = 0
+
+    for x1, x2 in initial_intervals:
+        ig, err, rnd = _quadrature(x1, x2, f, norm_func)
+        neval += _quadrature.num_eval
+
+        if global_integral is None:
+            if isinstance(ig, (float, complex)):
+                # Specialize for scalars
+                if norm_func in (_max_norm, np.linalg.norm):
+                    norm_func = abs
+
+            global_integral = ig
+            global_error = float(err)
+            rounding_error = float(rnd)
+
+            cache_count = cache_size // _get_sizeof(ig)
+            interval_cache = LRUDict(cache_count)
+        else:
+            global_integral += ig
+            global_error += err
+            rounding_error += rnd
+
+        interval_cache[(x1, x2)] = copy.copy(ig)
+        intervals.append((-err, x1, x2))
+
+    heapq.heapify(intervals)
+
+    CONVERGED = 0
+    NOT_CONVERGED = 1
+    ROUNDING_ERROR = 2
+    NOT_A_NUMBER = 3
+
+    status_msg = {
+        CONVERGED: "Target precision reached.",
+        NOT_CONVERGED: "Target precision not reached.",
+        ROUNDING_ERROR: "Target precision could not be reached due to rounding error.",
+        NOT_A_NUMBER: "Non-finite values encountered."
+    }
+
+    # Process intervals
+    with MapWrapper(workers) as mapwrapper:
+        ier = NOT_CONVERGED
+
+        while intervals and len(intervals) < limit:
+            # Select intervals with largest errors for subdivision
+            tol = max(epsabs, epsrel*norm_func(global_integral))
+
+            to_process = []
+            err_sum = 0
+
+            for j in range(parallel_count):
+                if not intervals:
+                    break
+
+                if j > 0 and err_sum > global_error - tol/8:
+                    # avoid unnecessary parallel splitting
+                    break
+
+                interval = heapq.heappop(intervals)
+
+                neg_old_err, a, b = interval
+                old_int = interval_cache.pop((a, b), None)
+                to_process.append(((-neg_old_err, a, b, old_int), f, norm_func, _quadrature))
+                err_sum += -neg_old_err
+
+            # Subdivide intervals
+            for dint, derr, dround_err, subint, dneval in mapwrapper(_subdivide_interval, to_process):
+                neval += dneval
+                global_integral += dint
+                global_error += derr
+                rounding_error += dround_err
+                for x in subint:
+                    x1, x2, ig, err = x
+                    interval_cache[(x1, x2)] = ig
+                    heapq.heappush(intervals, (-err, x1, x2))
+
+            # Termination check
+            if len(intervals) >= min_intervals:
+                tol = max(epsabs, epsrel*norm_func(global_integral))
+                if global_error < tol/8:
+                    ier = CONVERGED
+                    break
+                if global_error < rounding_error:
+                    ier = ROUNDING_ERROR
+                    break
+
+            if not (np.isfinite(global_error) and np.isfinite(rounding_error)):
+                ier = NOT_A_NUMBER
+                break
+
+    res = global_integral
+    err = global_error + rounding_error
+
+    if full_output:
+        res_arr = np.asarray(res)
+        dummy = np.full(res_arr.shape, np.nan, dtype=res_arr.dtype)
+        integrals = np.array([interval_cache.get((z[1], z[2]), dummy)
+                                      for z in intervals], dtype=res_arr.dtype)
+        errors = np.array([-z[0] for z in intervals])
+        intervals = np.array([[z[1], z[2]] for z in intervals])
+
+        info = _Bunch(neval=neval,
+                      success=(ier == CONVERGED),
+                      status=ier,
+                      message=status_msg[ier],
+                      intervals=intervals,
+                      integrals=integrals,
+                      errors=errors)
+        return (res, err, info)
+    else:
+        return (res, err)
+
+
+def _subdivide_interval(args):
+    interval, f, norm_func, _quadrature = args
+    old_err, a, b, old_int = interval
+
+    c = 0.5 * (a + b)
+
+    # Left-hand side
+    if getattr(_quadrature, 'cache_size', 0) > 0:
+        f = functools.lru_cache(_quadrature.cache_size)(f)
+
+    s1, err1, round1 = _quadrature(a, c, f, norm_func)
+    dneval = _quadrature.num_eval
+    s2, err2, round2 = _quadrature(c, b, f, norm_func)
+    dneval += _quadrature.num_eval
+    if old_int is None:
+        old_int, _, _ = _quadrature(a, b, f, norm_func)
+        dneval += _quadrature.num_eval
+
+    if getattr(_quadrature, 'cache_size', 0) > 0:
+        dneval = f.cache_info().misses
+
+    dint = s1 + s2 - old_int
+    derr = err1 + err2 - old_err
+    dround_err = round1 + round2
+
+    subintervals = ((a, c, s1, err1), (c, b, s2, err2))
+    return dint, derr, dround_err, subintervals, dneval
+
+
+def _quadrature_trapezoid(x1, x2, f, norm_func):
+    """
+    Composite trapezoid quadrature
+    """
+    x3 = 0.5*(x1 + x2)
+    f1 = f(x1)
+    f2 = f(x2)
+    f3 = f(x3)
+
+    s2 = 0.25 * (x2 - x1) * (f1 + 2*f3 + f2)
+
+    round_err = 0.25 * abs(x2 - x1) * (float(norm_func(f1))
+                                       + 2*float(norm_func(f3))
+                                       + float(norm_func(f2))) * 2e-16
+
+    s1 = 0.5 * (x2 - x1) * (f1 + f2)
+    err = 1/3 * float(norm_func(s1 - s2))
+    return s2, err, round_err
+
+
+_quadrature_trapezoid.cache_size = 3 * 3
+_quadrature_trapezoid.num_eval = 3
+
+
+def _quadrature_gk(a, b, f, norm_func, x, w, v):
+    """
+    Generic Gauss-Kronrod quadrature
+    """
+
+    fv = [0.0]*len(x)
+
+    c = 0.5 * (a + b)
+    h = 0.5 * (b - a)
+
+    # Gauss-Kronrod
+    s_k = 0.0
+    s_k_abs = 0.0
+    for i in range(len(x)):
+        ff = f(c + h*x[i])
+        fv[i] = ff
+
+        vv = v[i]
+
+        # \int f(x)
+        s_k += vv * ff
+        # \int |f(x)|
+        s_k_abs += vv * abs(ff)
+
+    # Gauss
+    s_g = 0.0
+    for i in range(len(w)):
+        s_g += w[i] * fv[2*i + 1]
+
+    # Quadrature of abs-deviation from average
+    s_k_dabs = 0.0
+    y0 = s_k / 2.0
+    for i in range(len(x)):
+        # \int |f(x) - y0|
+        s_k_dabs += v[i] * abs(fv[i] - y0)
+
+    # Use similar error estimation as quadpack
+    err = float(norm_func((s_k - s_g) * h))
+    dabs = float(norm_func(s_k_dabs * h))
+    if dabs != 0 and err != 0:
+        err = dabs * min(1.0, (200 * err / dabs)**1.5)
+
+    eps = sys.float_info.epsilon
+    round_err = float(norm_func(50 * eps * h * s_k_abs))
+
+    if round_err > sys.float_info.min:
+        err = max(err, round_err)
+
+    return h * s_k, err, round_err
+
+
+def _quadrature_gk21(a, b, f, norm_func):
+    """
+    Gauss-Kronrod 21 quadrature with error estimate
+    """
+    # Gauss-Kronrod points
+    x = (0.995657163025808080735527280689003,
+         0.973906528517171720077964012084452,
+         0.930157491355708226001207180059508,
+         0.865063366688984510732096688423493,
+         0.780817726586416897063717578345042,
+         0.679409568299024406234327365114874,
+         0.562757134668604683339000099272694,
+         0.433395394129247190799265943165784,
+         0.294392862701460198131126603103866,
+         0.148874338981631210884826001129720,
+         0,
+         -0.148874338981631210884826001129720,
+         -0.294392862701460198131126603103866,
+         -0.433395394129247190799265943165784,
+         -0.562757134668604683339000099272694,
+         -0.679409568299024406234327365114874,
+         -0.780817726586416897063717578345042,
+         -0.865063366688984510732096688423493,
+         -0.930157491355708226001207180059508,
+         -0.973906528517171720077964012084452,
+         -0.995657163025808080735527280689003)
+
+    # 10-point weights
+    w = (0.066671344308688137593568809893332,
+         0.149451349150580593145776339657697,
+         0.219086362515982043995534934228163,
+         0.269266719309996355091226921569469,
+         0.295524224714752870173892994651338,
+         0.295524224714752870173892994651338,
+         0.269266719309996355091226921569469,
+         0.219086362515982043995534934228163,
+         0.149451349150580593145776339657697,
+         0.066671344308688137593568809893332)
+
+    # 21-point weights
+    v = (0.011694638867371874278064396062192,
+         0.032558162307964727478818972459390,
+         0.054755896574351996031381300244580,
+         0.075039674810919952767043140916190,
+         0.093125454583697605535065465083366,
+         0.109387158802297641899210590325805,
+         0.123491976262065851077958109831074,
+         0.134709217311473325928054001771707,
+         0.142775938577060080797094273138717,
+         0.147739104901338491374841515972068,
+         0.149445554002916905664936468389821,
+         0.147739104901338491374841515972068,
+         0.142775938577060080797094273138717,
+         0.134709217311473325928054001771707,
+         0.123491976262065851077958109831074,
+         0.109387158802297641899210590325805,
+         0.093125454583697605535065465083366,
+         0.075039674810919952767043140916190,
+         0.054755896574351996031381300244580,
+         0.032558162307964727478818972459390,
+         0.011694638867371874278064396062192)
+
+    return _quadrature_gk(a, b, f, norm_func, x, w, v)
+
+
+_quadrature_gk21.num_eval = 21
+
+
+def _quadrature_gk15(a, b, f, norm_func):
+    """
+    Gauss-Kronrod 15 quadrature with error estimate
+    """
+    # Gauss-Kronrod points
+    x = (0.991455371120812639206854697526329,
+         0.949107912342758524526189684047851,
+         0.864864423359769072789712788640926,
+         0.741531185599394439863864773280788,
+         0.586087235467691130294144838258730,
+         0.405845151377397166906606412076961,
+         0.207784955007898467600689403773245,
+         0.000000000000000000000000000000000,
+         -0.207784955007898467600689403773245,
+         -0.405845151377397166906606412076961,
+         -0.586087235467691130294144838258730,
+         -0.741531185599394439863864773280788,
+         -0.864864423359769072789712788640926,
+         -0.949107912342758524526189684047851,
+         -0.991455371120812639206854697526329)
+
+    # 7-point weights
+    w = (0.129484966168869693270611432679082,
+         0.279705391489276667901467771423780,
+         0.381830050505118944950369775488975,
+         0.417959183673469387755102040816327,
+         0.381830050505118944950369775488975,
+         0.279705391489276667901467771423780,
+         0.129484966168869693270611432679082)
+
+    # 15-point weights
+    v = (0.022935322010529224963732008058970,
+         0.063092092629978553290700663189204,
+         0.104790010322250183839876322541518,
+         0.140653259715525918745189590510238,
+         0.169004726639267902826583426598550,
+         0.190350578064785409913256402421014,
+         0.204432940075298892414161999234649,
+         0.209482141084727828012999174891714,
+         0.204432940075298892414161999234649,
+         0.190350578064785409913256402421014,
+         0.169004726639267902826583426598550,
+         0.140653259715525918745189590510238,
+         0.104790010322250183839876322541518,
+         0.063092092629978553290700663189204,
+         0.022935322010529224963732008058970)
+
+    return _quadrature_gk(a, b, f, norm_func, x, w, v)
+
+
+_quadrature_gk15.num_eval = 15

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/dop.py

@@ -0,0 +1,28 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+
+
+import warnings
+from . import _dop  # type: ignore
+
+
+__all__ = [  # noqa: F822
+    'dopri5',
+    'dop853'
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    if name not in __all__:
+        raise AttributeError(
+            "scipy.integrate.dop is deprecated and has no attribute "
+            f"{name}")
+
+    warnings.warn("The `scipy.integrate.dop` namespace is deprecated "
+                  "and will be removed in SciPy v2.0.0.",
+                  category=DeprecationWarning, stacklevel=2)
+
+    return getattr(_dop, name)

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/lsoda.py

@@ -0,0 +1,25 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+
+
+import warnings
+from . import _lsoda  # type: ignore
+
+
+__all__ = ['lsoda']  # noqa: F822
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    if name not in __all__:
+        raise AttributeError(
+            "scipy.integrate.lsoda is deprecated and has no attribute "
+            f"{name}.")
+
+    warnings.warn("The `scipy.integrate.lsoda` namespace is deprecated "
+                  "and will be removed in SciPy v2.0.0.",
+                  category=DeprecationWarning, stacklevel=2)
+
+    return getattr(_lsoda, name)

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/odepack.py

@@ -0,0 +1,25 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.integrate` namespace for importing the functions
+# included below.
+
+import warnings
+from . import _odepack_py
+
+__all__ = ['odeint', 'ODEintWarning']  # noqa: F822
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    if name not in __all__:
+        raise AttributeError(
+            "scipy.integrate.odepack is deprecated and has no attribute "
+            f"{name}. Try looking in scipy.integrate instead.")
+
+    warnings.warn(f"Please use `{name}` from the `scipy.integrate` namespace, "
+                  "the `scipy.integrate.odepack` namespace is deprecated.",
+                  category=DeprecationWarning, stacklevel=2)
+
+    return getattr(_odepack_py, name)

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/quadpack.py

@@ -0,0 +1,32 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.integrate` namespace for importing the functions
+# included below.
+
+import warnings
+from . import _quadpack_py
+
+__all__ = [  # noqa: F822
+    "quad",
+    "dblquad",
+    "tplquad",
+    "nquad",
+    "IntegrationWarning",
+    "error",
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    if name not in __all__:
+        raise AttributeError(
+            "scipy.integrate.quadpack is deprecated and has no attribute "
+            f"{name}. Try looking in scipy.integrate instead.")
+
+    warnings.warn(f"Please use `{name}` from the `scipy.integrate` namespace, "
+                  "the `scipy.integrate.quadpack` namespace is deprecated.",
+                  category=DeprecationWarning, stacklevel=2)
+
+    return getattr(_quadpack_py, name)

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/tests/test__quad_vec.py

@@ -0,0 +1,204 @@
+import pytest
+
+import numpy as np
+from numpy.testing import assert_allclose
+
+from scipy.integrate import quad_vec
+
+from multiprocessing.dummy import Pool
+
+
+quadrature_params = pytest.mark.parametrize(
+    'quadrature', [None, "gk15", "gk21", "trapezoid"])
+
+
+@quadrature_params
+def test_quad_vec_simple(quadrature):
+    n = np.arange(10)
+    f = lambda x: x**n
+    for epsabs in [0.1, 1e-3, 1e-6]:
+        if quadrature == 'trapezoid' and epsabs < 1e-4:
+            # slow: skip
+            continue
+
+        kwargs = dict(epsabs=epsabs, quadrature=quadrature)
+
+        exact = 2**(n+1)/(n + 1)
+
+        res, err = quad_vec(f, 0, 2, norm='max', **kwargs)
+        assert_allclose(res, exact, rtol=0, atol=epsabs)
+
+        res, err = quad_vec(f, 0, 2, norm='2', **kwargs)
+        assert np.linalg.norm(res - exact) < epsabs
+
+        res, err = quad_vec(f, 0, 2, norm='max', points=(0.5, 1.0), **kwargs)
+        assert_allclose(res, exact, rtol=0, atol=epsabs)
+
+        res, err, *rest = quad_vec(f, 0, 2, norm='max',
+                                   epsrel=1e-8,
+                                   full_output=True,
+                                   limit=10000,
+                                   **kwargs)
+        assert_allclose(res, exact, rtol=0, atol=epsabs)
+
+
+@quadrature_params
+def test_quad_vec_simple_inf(quadrature):
+    f = lambda x: 1 / (1 + np.float64(x)**2)
+
+    for epsabs in [0.1, 1e-3, 1e-6]:
+        if quadrature == 'trapezoid' and epsabs < 1e-4:
+            # slow: skip
+            continue
+
+        kwargs = dict(norm='max', epsabs=epsabs, quadrature=quadrature)
+
+        res, err = quad_vec(f, 0, np.inf, **kwargs)
+        assert_allclose(res, np.pi/2, rtol=0, atol=max(epsabs, err))
+
+        res, err = quad_vec(f, 0, -np.inf, **kwargs)
+        assert_allclose(res, -np.pi/2, rtol=0, atol=max(epsabs, err))
+
+        res, err = quad_vec(f, -np.inf, 0, **kwargs)
+        assert_allclose(res, np.pi/2, rtol=0, atol=max(epsabs, err))
+
+        res, err = quad_vec(f, np.inf, 0, **kwargs)
+        assert_allclose(res, -np.pi/2, rtol=0, atol=max(epsabs, err))
+
+        res, err = quad_vec(f, -np.inf, np.inf, **kwargs)
+        assert_allclose(res, np.pi, rtol=0, atol=max(epsabs, err))
+
+        res, err = quad_vec(f, np.inf, -np.inf, **kwargs)
+        assert_allclose(res, -np.pi, rtol=0, atol=max(epsabs, err))
+
+        res, err = quad_vec(f, np.inf, np.inf, **kwargs)
+        assert_allclose(res, 0, rtol=0, atol=max(epsabs, err))
+
+        res, err = quad_vec(f, -np.inf, -np.inf, **kwargs)
+        assert_allclose(res, 0, rtol=0, atol=max(epsabs, err))
+
+        res, err = quad_vec(f, 0, np.inf, points=(1.0, 2.0), **kwargs)
+        assert_allclose(res, np.pi/2, rtol=0, atol=max(epsabs, err))
+
+    f = lambda x: np.sin(x + 2) / (1 + x**2)
+    exact = np.pi / np.e * np.sin(2)
+    epsabs = 1e-5
+
+    res, err, info = quad_vec(f, -np.inf, np.inf, limit=1000, norm='max', epsabs=epsabs,
+                              quadrature=quadrature, full_output=True)
+    assert info.status == 1
+    assert_allclose(res, exact, rtol=0, atol=max(epsabs, 1.5 * err))
+
+
+def test_quad_vec_args():
+    f = lambda x, a: x * (x + a) * np.arange(3)
+    a = 2
+    exact = np.array([0, 4/3, 8/3])
+
+    res, err = quad_vec(f, 0, 1, args=(a,))
+    assert_allclose(res, exact, rtol=0, atol=1e-4)
+
+
+def _lorenzian(x):
+    return 1 / (1 + x**2)
+
+
+def test_quad_vec_pool():
+    f = _lorenzian
+    res, err = quad_vec(f, -np.inf, np.inf, norm='max', epsabs=1e-4, workers=4)
+    assert_allclose(res, np.pi, rtol=0, atol=1e-4)
+
+    with Pool(10) as pool:
+        f = lambda x: 1 / (1 + x**2)
+        res, err = quad_vec(f, -np.inf, np.inf, norm='max', epsabs=1e-4, workers=pool.map)
+        assert_allclose(res, np.pi, rtol=0, atol=1e-4)
+
+
+def _func_with_args(x, a):
+    return x * (x + a) * np.arange(3)
+
+
+@pytest.mark.parametrize('extra_args', [2, (2,)])
+@pytest.mark.parametrize('workers', [1, 10])
+def test_quad_vec_pool_args(extra_args, workers):
+    f = _func_with_args
+    exact = np.array([0, 4/3, 8/3])
+
+    res, err = quad_vec(f, 0, 1, args=extra_args, workers=workers)
+    assert_allclose(res, exact, rtol=0, atol=1e-4)
+
+    with Pool(workers) as pool:
+        res, err = quad_vec(f, 0, 1, args=extra_args, workers=pool.map)
+        assert_allclose(res, exact, rtol=0, atol=1e-4)
+
+
+@quadrature_params
+def test_num_eval(quadrature):
+    def f(x):
+        count[0] += 1
+        return x**5
+
+    count = [0]
+    res = quad_vec(f, 0, 1, norm='max', full_output=True, quadrature=quadrature)
+    assert res[2].neval == count[0]
+
+
+def test_info():
+    def f(x):
+        return np.ones((3, 2, 1))
+
+    res, err, info = quad_vec(f, 0, 1, norm='max', full_output=True)
+
+    assert info.success == True
+    assert info.status == 0
+    assert info.message == 'Target precision reached.'
+    assert info.neval > 0
+    assert info.intervals.shape[1] == 2
+    assert info.integrals.shape == (info.intervals.shape[0], 3, 2, 1)
+    assert info.errors.shape == (info.intervals.shape[0],)
+
+
+def test_nan_inf():
+    def f_nan(x):
+        return np.nan
+
+    def f_inf(x):
+        return np.inf if x < 0.1 else 1/x
+
+    res, err, info = quad_vec(f_nan, 0, 1, full_output=True)
+    assert info.status == 3
+
+    res, err, info = quad_vec(f_inf, 0, 1, full_output=True)
+    assert info.status == 3
+
+
+@pytest.mark.parametrize('a,b', [(0, 1), (0, np.inf), (np.inf, 0),
+                                 (-np.inf, np.inf), (np.inf, -np.inf)])
+def test_points(a, b):
+    # Check that initial interval splitting is done according to
+    # `points`, by checking that consecutive sets of 15 point (for
+    # gk15) function evaluations lie between `points`
+
+    points = (0, 0.25, 0.5, 0.75, 1.0)
+    points += tuple(-x for x in points)
+
+    quadrature_points = 15
+    interval_sets = []
+    count = 0
+
+    def f(x):
+        nonlocal count
+
+        if count % quadrature_points == 0:
+            interval_sets.append(set())
+
+        count += 1
+        interval_sets[-1].add(float(x))
+        return 0.0
+
+    quad_vec(f, a, b, points=points, quadrature='gk15', limit=0)
+
+    # Check that all point sets lie in a single `points` interval
+    for p in interval_sets:
+        j = np.searchsorted(sorted(points), tuple(p))
+        assert np.all(j == j[0])

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/tests/test_banded_ode_solvers.py

@@ -0,0 +1,218 @@
+import itertools
+import numpy as np
+from numpy.testing import assert_allclose
+from scipy.integrate import ode
+
+
+def _band_count(a):
+    """Returns ml and mu, the lower and upper band sizes of a."""
+    nrows, ncols = a.shape
+    ml = 0
+    for k in range(-nrows+1, 0):
+        if np.diag(a, k).any():
+            ml = -k
+            break
+    mu = 0
+    for k in range(nrows-1, 0, -1):
+        if np.diag(a, k).any():
+            mu = k
+            break
+    return ml, mu
+
+
+def _linear_func(t, y, a):
+    """Linear system dy/dt = a * y"""
+    return a.dot(y)
+
+
+def _linear_jac(t, y, a):
+    """Jacobian of a * y is a."""
+    return a
+
+
+def _linear_banded_jac(t, y, a):
+    """Banded Jacobian."""
+    ml, mu = _band_count(a)
+    bjac = [np.r_[[0] * k, np.diag(a, k)] for k in range(mu, 0, -1)]
+    bjac.append(np.diag(a))
+    for k in range(-1, -ml-1, -1):
+        bjac.append(np.r_[np.diag(a, k), [0] * (-k)])
+    return bjac
+
+
+def _solve_linear_sys(a, y0, tend=1, dt=0.1,
+                      solver=None, method='bdf', use_jac=True,
+                      with_jacobian=False, banded=False):
+    """Use scipy.integrate.ode to solve a linear system of ODEs.
+
+    a : square ndarray
+        Matrix of the linear system to be solved.
+    y0 : ndarray
+        Initial condition
+    tend : float
+        Stop time.
+    dt : float
+        Step size of the output.
+    solver : str
+        If not None, this must be "vode", "lsoda" or "zvode".
+    method : str
+        Either "bdf" or "adams".
+    use_jac : bool
+        Determines if the jacobian function is passed to ode().
+    with_jacobian : bool
+        Passed to ode.set_integrator().
+    banded : bool
+        Determines whether a banded or full jacobian is used.
+        If `banded` is True, `lband` and `uband` are determined by the
+        values in `a`.
+    """
+    if banded:
+        lband, uband = _band_count(a)
+    else:
+        lband = None
+        uband = None
+
+    if use_jac:
+        if banded:
+            r = ode(_linear_func, _linear_banded_jac)
+        else:
+            r = ode(_linear_func, _linear_jac)
+    else:
+        r = ode(_linear_func)
+
+    if solver is None:
+        if np.iscomplexobj(a):
+            solver = "zvode"
+        else:
+            solver = "vode"
+
+    r.set_integrator(solver,
+                     with_jacobian=with_jacobian,
+                     method=method,
+                     lband=lband, uband=uband,
+                     rtol=1e-9, atol=1e-10,
+                     )
+    t0 = 0
+    r.set_initial_value(y0, t0)
+    r.set_f_params(a)
+    r.set_jac_params(a)
+
+    t = [t0]
+    y = [y0]
+    while r.successful() and r.t < tend:
+        r.integrate(r.t + dt)
+        t.append(r.t)
+        y.append(r.y)
+
+    t = np.array(t)
+    y = np.array(y)
+    return t, y
+
+
+def _analytical_solution(a, y0, t):
+    """
+    Analytical solution to the linear differential equations dy/dt = a*y.
+
+    The solution is only valid if `a` is diagonalizable.
+
+    Returns a 2-D array with shape (len(t), len(y0)).
+    """
+    lam, v = np.linalg.eig(a)
+    c = np.linalg.solve(v, y0)
+    e = c * np.exp(lam * t.reshape(-1, 1))
+    sol = e.dot(v.T)
+    return sol
+
+
+def test_banded_ode_solvers():
+    # Test the "lsoda", "vode" and "zvode" solvers of the `ode` class
+    # with a system that has a banded Jacobian matrix.
+
+    t_exact = np.linspace(0, 1.0, 5)
+
+    # --- Real arrays for testing the "lsoda" and "vode" solvers ---
+
+    # lband = 2, uband = 1:
+    a_real = np.array([[-0.6, 0.1, 0.0, 0.0, 0.0],
+                       [0.2, -0.5, 0.9, 0.0, 0.0],
+                       [0.1, 0.1, -0.4, 0.1, 0.0],
+                       [0.0, 0.3, -0.1, -0.9, -0.3],
+                       [0.0, 0.0, 0.1, 0.1, -0.7]])
+
+    # lband = 0, uband = 1:
+    a_real_upper = np.triu(a_real)
+
+    # lband = 2, uband = 0:
+    a_real_lower = np.tril(a_real)
+
+    # lband = 0, uband = 0:
+    a_real_diag = np.triu(a_real_lower)
+
+    real_matrices = [a_real, a_real_upper, a_real_lower, a_real_diag]
+    real_solutions = []
+
+    for a in real_matrices:
+        y0 = np.arange(1, a.shape[0] + 1)
+        y_exact = _analytical_solution(a, y0, t_exact)
+        real_solutions.append((y0, t_exact, y_exact))
+
+    def check_real(idx, solver, meth, use_jac, with_jac, banded):
+        a = real_matrices[idx]
+        y0, t_exact, y_exact = real_solutions[idx]
+        t, y = _solve_linear_sys(a, y0,
+                                 tend=t_exact[-1],
+                                 dt=t_exact[1] - t_exact[0],
+                                 solver=solver,
+                                 method=meth,
+                                 use_jac=use_jac,
+                                 with_jacobian=with_jac,
+                                 banded=banded)
+        assert_allclose(t, t_exact)
+        assert_allclose(y, y_exact)
+
+    for idx in range(len(real_matrices)):
+        p = [['vode', 'lsoda'],  # solver
+             ['bdf', 'adams'],   # method
+             [False, True],      # use_jac
+             [False, True],      # with_jacobian
+             [False, True]]      # banded
+        for solver, meth, use_jac, with_jac, banded in itertools.product(*p):
+            check_real(idx, solver, meth, use_jac, with_jac, banded)
+
+    # --- Complex arrays for testing the "zvode" solver ---
+
+    # complex, lband = 2, uband = 1:
+    a_complex = a_real - 0.5j * a_real
+
+    # complex, lband = 0, uband = 0:
+    a_complex_diag = np.diag(np.diag(a_complex))
+
+    complex_matrices = [a_complex, a_complex_diag]
+    complex_solutions = []
+
+    for a in complex_matrices:
+        y0 = np.arange(1, a.shape[0] + 1) + 1j
+        y_exact = _analytical_solution(a, y0, t_exact)
+        complex_solutions.append((y0, t_exact, y_exact))
+
+    def check_complex(idx, solver, meth, use_jac, with_jac, banded):
+        a = complex_matrices[idx]
+        y0, t_exact, y_exact = complex_solutions[idx]
+        t, y = _solve_linear_sys(a, y0,
+                                 tend=t_exact[-1],
+                                 dt=t_exact[1] - t_exact[0],
+                                 solver=solver,
+                                 method=meth,
+                                 use_jac=use_jac,
+                                 with_jacobian=with_jac,
+                                 banded=banded)
+        assert_allclose(t, t_exact)
+        assert_allclose(y, y_exact)
+
+    for idx in range(len(complex_matrices)):
+        p = [['bdf', 'adams'],   # method
+             [False, True],      # use_jac
+             [False, True],      # with_jacobian
+             [False, True]]      # banded
+        for meth, use_jac, with_jac, banded in itertools.product(*p):
+            check_complex(idx, "zvode", meth, use_jac, with_jac, banded)

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/tests/test_bvp.py

@@ -0,0 +1,709 @@
+import sys
+
+try:
+    from StringIO import StringIO
+except ImportError:
+    from io import StringIO
+
+import numpy as np
+from numpy.testing import (assert_, assert_array_equal, assert_allclose,
+                           assert_equal)
+from pytest import raises as assert_raises
+
+from scipy.sparse import coo_matrix
+from scipy.special import erf
+from scipy.integrate._bvp import (modify_mesh, estimate_fun_jac,
+                                  estimate_bc_jac, compute_jac_indices,
+                                  construct_global_jac, solve_bvp)
+
+
+def exp_fun(x, y):
+    return np.vstack((y[1], y[0]))
+
+
+def exp_fun_jac(x, y):
+    df_dy = np.empty((2, 2, x.shape[0]))
+    df_dy[0, 0] = 0
+    df_dy[0, 1] = 1
+    df_dy[1, 0] = 1
+    df_dy[1, 1] = 0
+    return df_dy
+
+
+def exp_bc(ya, yb):
+    return np.hstack((ya[0] - 1, yb[0]))
+
+
+def exp_bc_complex(ya, yb):
+    return np.hstack((ya[0] - 1 - 1j, yb[0]))
+
+
+def exp_bc_jac(ya, yb):
+    dbc_dya = np.array([
+        [1, 0],
+        [0, 0]
+    ])
+    dbc_dyb = np.array([
+        [0, 0],
+        [1, 0]
+    ])
+    return dbc_dya, dbc_dyb
+
+
+def exp_sol(x):
+    return (np.exp(-x) - np.exp(x - 2)) / (1 - np.exp(-2))
+
+
+def sl_fun(x, y, p):
+    return np.vstack((y[1], -p[0]**2 * y[0]))
+
+
+def sl_fun_jac(x, y, p):
+    n, m = y.shape
+    df_dy = np.empty((n, 2, m))
+    df_dy[0, 0] = 0
+    df_dy[0, 1] = 1
+    df_dy[1, 0] = -p[0]**2
+    df_dy[1, 1] = 0
+
+    df_dp = np.empty((n, 1, m))
+    df_dp[0, 0] = 0
+    df_dp[1, 0] = -2 * p[0] * y[0]
+
+    return df_dy, df_dp
+
+
+def sl_bc(ya, yb, p):
+    return np.hstack((ya[0], yb[0], ya[1] - p[0]))
+
+
+def sl_bc_jac(ya, yb, p):
+    dbc_dya = np.zeros((3, 2))
+    dbc_dya[0, 0] = 1
+    dbc_dya[2, 1] = 1
+
+    dbc_dyb = np.zeros((3, 2))
+    dbc_dyb[1, 0] = 1
+
+    dbc_dp = np.zeros((3, 1))
+    dbc_dp[2, 0] = -1
+
+    return dbc_dya, dbc_dyb, dbc_dp
+
+
+def sl_sol(x, p):
+    return np.sin(p[0] * x)
+
+
+def emden_fun(x, y):
+    return np.vstack((y[1], -y[0]**5))
+
+
+def emden_fun_jac(x, y):
+    df_dy = np.empty((2, 2, x.shape[0]))
+    df_dy[0, 0] = 0
+    df_dy[0, 1] = 1
+    df_dy[1, 0] = -5 * y[0]**4
+    df_dy[1, 1] = 0
+    return df_dy
+
+
+def emden_bc(ya, yb):
+    return np.array([ya[1], yb[0] - (3/4)**0.5])
+
+
+def emden_bc_jac(ya, yb):
+    dbc_dya = np.array([
+        [0, 1],
+        [0, 0]
+    ])
+    dbc_dyb = np.array([
+        [0, 0],
+        [1, 0]
+    ])
+    return dbc_dya, dbc_dyb
+
+
+def emden_sol(x):
+    return (1 + x**2/3)**-0.5
+
+
+def undefined_fun(x, y):
+    return np.zeros_like(y)
+
+
+def undefined_bc(ya, yb):
+    return np.array([ya[0], yb[0] - 1])
+
+
+def big_fun(x, y):
+    f = np.zeros_like(y)
+    f[::2] = y[1::2]
+    return f
+
+
+def big_bc(ya, yb):
+    return np.hstack((ya[::2], yb[::2] - 1))
+
+
+def big_sol(x, n):
+    y = np.ones((2 * n, x.size))
+    y[::2] = x
+    return x
+
+
+def big_fun_with_parameters(x, y, p):
+    """ Big version of sl_fun, with two parameters.
+
+    The two differential equations represented by sl_fun are broadcast to the
+    number of rows of y, rotating between the parameters p[0] and p[1].
+    Here are the differential equations:
+
+        dy[0]/dt = y[1]
+        dy[1]/dt = -p[0]**2 * y[0]
+        dy[2]/dt = y[3]
+        dy[3]/dt = -p[1]**2 * y[2]
+        dy[4]/dt = y[5]
+        dy[5]/dt = -p[0]**2 * y[4]
+        dy[6]/dt = y[7]
+        dy[7]/dt = -p[1]**2 * y[6]
+        .
+        .
+        .
+
+    """
+    f = np.zeros_like(y)
+    f[::2] = y[1::2]
+    f[1::4] = -p[0]**2 * y[::4]
+    f[3::4] = -p[1]**2 * y[2::4]
+    return f
+
+
+def big_fun_with_parameters_jac(x, y, p):
+    # big version of sl_fun_jac, with two parameters
+    n, m = y.shape
+    df_dy = np.zeros((n, n, m))
+    df_dy[range(0, n, 2), range(1, n, 2)] = 1
+    df_dy[range(1, n, 4), range(0, n, 4)] = -p[0]**2
+    df_dy[range(3, n, 4), range(2, n, 4)] = -p[1]**2
+
+    df_dp = np.zeros((n, 2, m))
+    df_dp[range(1, n, 4), 0] = -2 * p[0] * y[range(0, n, 4)]
+    df_dp[range(3, n, 4), 1] = -2 * p[1] * y[range(2, n, 4)]
+
+    return df_dy, df_dp
+
+
+def big_bc_with_parameters(ya, yb, p):
+    # big version of sl_bc, with two parameters
+    return np.hstack((ya[::2], yb[::2], ya[1] - p[0], ya[3] - p[1]))
+
+
+def big_bc_with_parameters_jac(ya, yb, p):
+    # big version of sl_bc_jac, with two parameters
+    n = ya.shape[0]
+    dbc_dya = np.zeros((n + 2, n))
+    dbc_dyb = np.zeros((n + 2, n))
+
+    dbc_dya[range(n // 2), range(0, n, 2)] = 1
+    dbc_dyb[range(n // 2, n), range(0, n, 2)] = 1
+
+    dbc_dp = np.zeros((n + 2, 2))
+    dbc_dp[n, 0] = -1
+    dbc_dya[n, 1] = 1
+    dbc_dp[n + 1, 1] = -1
+    dbc_dya[n + 1, 3] = 1
+
+    return dbc_dya, dbc_dyb, dbc_dp
+
+
+def big_sol_with_parameters(x, p):
+    # big version of sl_sol, with two parameters
+    return np.vstack((np.sin(p[0] * x), np.sin(p[1] * x)))
+
+
+def shock_fun(x, y):
+    eps = 1e-3
+    return np.vstack((
+        y[1],
+        -(x * y[1] + eps * np.pi**2 * np.cos(np.pi * x) +
+          np.pi * x * np.sin(np.pi * x)) / eps
+    ))
+
+
+def shock_bc(ya, yb):
+    return np.array([ya[0] + 2, yb[0]])
+
+
+def shock_sol(x):
+    eps = 1e-3
+    k = np.sqrt(2 * eps)
+    return np.cos(np.pi * x) + erf(x / k) / erf(1 / k)
+
+
+def nonlin_bc_fun(x, y):
+    # laplace eq.
+    return np.stack([y[1], np.zeros_like(x)])
+
+
+def nonlin_bc_bc(ya, yb):
+    phiA, phipA = ya
+    phiC, phipC = yb
+
+    kappa, ioA, ioC, V, f = 1.64, 0.01, 1.0e-4, 0.5, 38.9
+
+    # Butler-Volmer Kinetics at Anode
+    hA = 0.0-phiA-0.0
+    iA = ioA * (np.exp(f*hA) - np.exp(-f*hA))
+    res0 = iA + kappa * phipA
+
+    # Butler-Volmer Kinetics at Cathode
+    hC = V - phiC - 1.0
+    iC = ioC * (np.exp(f*hC) - np.exp(-f*hC))
+    res1 = iC - kappa*phipC
+
+    return np.array([res0, res1])
+
+
+def nonlin_bc_sol(x):
+    return -0.13426436116763119 - 1.1308709 * x
+
+
+def test_modify_mesh():
+    x = np.array([0, 1, 3, 9], dtype=float)
+    x_new = modify_mesh(x, np.array([0]), np.array([2]))
+    assert_array_equal(x_new, np.array([0, 0.5, 1, 3, 5, 7, 9]))
+
+    x = np.array([-6, -3, 0, 3, 6], dtype=float)
+    x_new = modify_mesh(x, np.array([1], dtype=int), np.array([0, 2, 3]))
+    assert_array_equal(x_new, [-6, -5, -4, -3, -1.5, 0, 1, 2, 3, 4, 5, 6])
+
+
+def test_compute_fun_jac():
+    x = np.linspace(0, 1, 5)
+    y = np.empty((2, x.shape[0]))
+    y[0] = 0.01
+    y[1] = 0.02
+    p = np.array([])
+    df_dy, df_dp = estimate_fun_jac(lambda x, y, p: exp_fun(x, y), x, y, p)
+    df_dy_an = exp_fun_jac(x, y)
+    assert_allclose(df_dy, df_dy_an)
+    assert_(df_dp is None)
+
+    x = np.linspace(0, np.pi, 5)
+    y = np.empty((2, x.shape[0]))
+    y[0] = np.sin(x)
+    y[1] = np.cos(x)
+    p = np.array([1.0])
+    df_dy, df_dp = estimate_fun_jac(sl_fun, x, y, p)
+    df_dy_an, df_dp_an = sl_fun_jac(x, y, p)
+    assert_allclose(df_dy, df_dy_an)
+    assert_allclose(df_dp, df_dp_an)
+
+    x = np.linspace(0, 1, 10)
+    y = np.empty((2, x.shape[0]))
+    y[0] = (3/4)**0.5
+    y[1] = 1e-4
+    p = np.array([])
+    df_dy, df_dp = estimate_fun_jac(lambda x, y, p: emden_fun(x, y), x, y, p)
+    df_dy_an = emden_fun_jac(x, y)
+    assert_allclose(df_dy, df_dy_an)
+    assert_(df_dp is None)
+
+
+def test_compute_bc_jac():
+    ya = np.array([-1.0, 2])
+    yb = np.array([0.5, 3])
+    p = np.array([])
+    dbc_dya, dbc_dyb, dbc_dp = estimate_bc_jac(
+        lambda ya, yb, p: exp_bc(ya, yb), ya, yb, p)
+    dbc_dya_an, dbc_dyb_an = exp_bc_jac(ya, yb)
+    assert_allclose(dbc_dya, dbc_dya_an)
+    assert_allclose(dbc_dyb, dbc_dyb_an)
+    assert_(dbc_dp is None)
+
+    ya = np.array([0.0, 1])
+    yb = np.array([0.0, -1])
+    p = np.array([0.5])
+    dbc_dya, dbc_dyb, dbc_dp = estimate_bc_jac(sl_bc, ya, yb, p)
+    dbc_dya_an, dbc_dyb_an, dbc_dp_an = sl_bc_jac(ya, yb, p)
+    assert_allclose(dbc_dya, dbc_dya_an)
+    assert_allclose(dbc_dyb, dbc_dyb_an)
+    assert_allclose(dbc_dp, dbc_dp_an)
+
+    ya = np.array([0.5, 100])
+    yb = np.array([-1000, 10.5])
+    p = np.array([])
+    dbc_dya, dbc_dyb, dbc_dp = estimate_bc_jac(
+        lambda ya, yb, p: emden_bc(ya, yb), ya, yb, p)
+    dbc_dya_an, dbc_dyb_an = emden_bc_jac(ya, yb)
+    assert_allclose(dbc_dya, dbc_dya_an)
+    assert_allclose(dbc_dyb, dbc_dyb_an)
+    assert_(dbc_dp is None)
+
+
+def test_compute_jac_indices():
+    n = 2
+    m = 4
+    k = 2
+    i, j = compute_jac_indices(n, m, k)
+    s = coo_matrix((np.ones_like(i), (i, j))).toarray()
+    s_true = np.array([
+        [1, 1, 1, 1, 0, 0, 0, 0, 1, 1],
+        [1, 1, 1, 1, 0, 0, 0, 0, 1, 1],
+        [0, 0, 1, 1, 1, 1, 0, 0, 1, 1],
+        [0, 0, 1, 1, 1, 1, 0, 0, 1, 1],
+        [0, 0, 0, 0, 1, 1, 1, 1, 1, 1],
+        [0, 0, 0, 0, 1, 1, 1, 1, 1, 1],
+        [1, 1, 0, 0, 0, 0, 1, 1, 1, 1],
+        [1, 1, 0, 0, 0, 0, 1, 1, 1, 1],
+        [1, 1, 0, 0, 0, 0, 1, 1, 1, 1],
+        [1, 1, 0, 0, 0, 0, 1, 1, 1, 1],
+    ])
+    assert_array_equal(s, s_true)
+
+
+def test_compute_global_jac():
+    n = 2
+    m = 5
+    k = 1
+    i_jac, j_jac = compute_jac_indices(2, 5, 1)
+    x = np.linspace(0, 1, 5)
+    h = np.diff(x)
+    y = np.vstack((np.sin(np.pi * x), np.pi * np.cos(np.pi * x)))
+    p = np.array([3.0])
+
+    f = sl_fun(x, y, p)
+
+    x_middle = x[:-1] + 0.5 * h
+    y_middle = 0.5 * (y[:, :-1] + y[:, 1:]) - h/8 * (f[:, 1:] - f[:, :-1])
+
+    df_dy, df_dp = sl_fun_jac(x, y, p)
+    df_dy_middle, df_dp_middle = sl_fun_jac(x_middle, y_middle, p)
+    dbc_dya, dbc_dyb, dbc_dp = sl_bc_jac(y[:, 0], y[:, -1], p)
+
+    J = construct_global_jac(n, m, k, i_jac, j_jac, h, df_dy, df_dy_middle,
+                             df_dp, df_dp_middle, dbc_dya, dbc_dyb, dbc_dp)
+    J = J.toarray()
+
+    def J_block(h, p):
+        return np.array([
+            [h**2*p**2/12 - 1, -0.5*h, -h**2*p**2/12 + 1, -0.5*h],
+            [0.5*h*p**2, h**2*p**2/12 - 1, 0.5*h*p**2, 1 - h**2*p**2/12]
+        ])
+
+    J_true = np.zeros((m * n + k, m * n + k))
+    for i in range(m - 1):
+        J_true[i * n: (i + 1) * n, i * n: (i + 2) * n] = J_block(h[i], p[0])
+
+    J_true[:(m - 1) * n:2, -1] = p * h**2/6 * (y[0, :-1] - y[0, 1:])
+    J_true[1:(m - 1) * n:2, -1] = p * (h * (y[0, :-1] + y[0, 1:]) +
+                                       h**2/6 * (y[1, :-1] - y[1, 1:]))
+
+    J_true[8, 0] = 1
+    J_true[9, 8] = 1
+    J_true[10, 1] = 1
+    J_true[10, 10] = -1
+
+    assert_allclose(J, J_true, rtol=1e-10)
+
+    df_dy, df_dp = estimate_fun_jac(sl_fun, x, y, p)
+    df_dy_middle, df_dp_middle = estimate_fun_jac(sl_fun, x_middle, y_middle, p)
+    dbc_dya, dbc_dyb, dbc_dp = estimate_bc_jac(sl_bc, y[:, 0], y[:, -1], p)
+    J = construct_global_jac(n, m, k, i_jac, j_jac, h, df_dy, df_dy_middle,
+                             df_dp, df_dp_middle, dbc_dya, dbc_dyb, dbc_dp)
+    J = J.toarray()
+    assert_allclose(J, J_true, rtol=2e-8, atol=2e-8)
+
+
+def test_parameter_validation():
+    x = [0, 1, 0.5]
+    y = np.zeros((2, 3))
+    assert_raises(ValueError, solve_bvp, exp_fun, exp_bc, x, y)
+
+    x = np.linspace(0, 1, 5)
+    y = np.zeros((2, 4))
+    assert_raises(ValueError, solve_bvp, exp_fun, exp_bc, x, y)
+
+    fun = lambda x, y, p: exp_fun(x, y)
+    bc = lambda ya, yb, p: exp_bc(ya, yb)
+
+    y = np.zeros((2, x.shape[0]))
+    assert_raises(ValueError, solve_bvp, fun, bc, x, y, p=[1])
+
+    def wrong_shape_fun(x, y):
+        return np.zeros(3)
+
+    assert_raises(ValueError, solve_bvp, wrong_shape_fun, bc, x, y)
+
+    S = np.array([[0, 0]])
+    assert_raises(ValueError, solve_bvp, exp_fun, exp_bc, x, y, S=S)
+
+
+def test_no_params():
+    x = np.linspace(0, 1, 5)
+    x_test = np.linspace(0, 1, 100)
+    y = np.zeros((2, x.shape[0]))
+    for fun_jac in [None, exp_fun_jac]:
+        for bc_jac in [None, exp_bc_jac]:
+            sol = solve_bvp(exp_fun, exp_bc, x, y, fun_jac=fun_jac,
+                            bc_jac=bc_jac)
+
+            assert_equal(sol.status, 0)
+            assert_(sol.success)
+
+            assert_equal(sol.x.size, 5)
+
+            sol_test = sol.sol(x_test)
+
+            assert_allclose(sol_test[0], exp_sol(x_test), atol=1e-5)
+
+            f_test = exp_fun(x_test, sol_test)
+            r = sol.sol(x_test, 1) - f_test
+            rel_res = r / (1 + np.abs(f_test))
+            norm_res = np.sum(rel_res**2, axis=0)**0.5
+            assert_(np.all(norm_res < 1e-3))
+
+            assert_(np.all(sol.rms_residuals < 1e-3))
+            assert_allclose(sol.sol(sol.x), sol.y, rtol=1e-10, atol=1e-10)
+            assert_allclose(sol.sol(sol.x, 1), sol.yp, rtol=1e-10, atol=1e-10)
+
+
+def test_with_params():
+    x = np.linspace(0, np.pi, 5)
+    x_test = np.linspace(0, np.pi, 100)
+    y = np.ones((2, x.shape[0]))
+
+    for fun_jac in [None, sl_fun_jac]:
+        for bc_jac in [None, sl_bc_jac]:
+            sol = solve_bvp(sl_fun, sl_bc, x, y, p=[0.5], fun_jac=fun_jac,
+                            bc_jac=bc_jac)
+
+            assert_equal(sol.status, 0)
+            assert_(sol.success)
+
+            assert_(sol.x.size < 10)
+
+            assert_allclose(sol.p, [1], rtol=1e-4)
+
+            sol_test = sol.sol(x_test)
+
+            assert_allclose(sol_test[0], sl_sol(x_test, [1]),
+                            rtol=1e-4, atol=1e-4)
+
+            f_test = sl_fun(x_test, sol_test, [1])
+            r = sol.sol(x_test, 1) - f_test
+            rel_res = r / (1 + np.abs(f_test))
+            norm_res = np.sum(rel_res ** 2, axis=0) ** 0.5
+            assert_(np.all(norm_res < 1e-3))
+
+            assert_(np.all(sol.rms_residuals < 1e-3))
+            assert_allclose(sol.sol(sol.x), sol.y, rtol=1e-10, atol=1e-10)
+            assert_allclose(sol.sol(sol.x, 1), sol.yp, rtol=1e-10, atol=1e-10)
+
+
+def test_singular_term():
+    x = np.linspace(0, 1, 10)
+    x_test = np.linspace(0.05, 1, 100)
+    y = np.empty((2, 10))
+    y[0] = (3/4)**0.5
+    y[1] = 1e-4
+    S = np.array([[0, 0], [0, -2]])
+
+    for fun_jac in [None, emden_fun_jac]:
+        for bc_jac in [None, emden_bc_jac]:
+            sol = solve_bvp(emden_fun, emden_bc, x, y, S=S, fun_jac=fun_jac,
+                            bc_jac=bc_jac)
+
+            assert_equal(sol.status, 0)
+            assert_(sol.success)
+
+            assert_equal(sol.x.size, 10)
+
+            sol_test = sol.sol(x_test)
+            assert_allclose(sol_test[0], emden_sol(x_test), atol=1e-5)
+
+            f_test = emden_fun(x_test, sol_test) + S.dot(sol_test) / x_test
+            r = sol.sol(x_test, 1) - f_test
+            rel_res = r / (1 + np.abs(f_test))
+            norm_res = np.sum(rel_res ** 2, axis=0) ** 0.5
+
+            assert_(np.all(norm_res < 1e-3))
+            assert_allclose(sol.sol(sol.x), sol.y, rtol=1e-10, atol=1e-10)
+            assert_allclose(sol.sol(sol.x, 1), sol.yp, rtol=1e-10, atol=1e-10)
+
+
+def test_complex():
+    # The test is essentially the same as test_no_params, but boundary
+    # conditions are turned into complex.
+    x = np.linspace(0, 1, 5)
+    x_test = np.linspace(0, 1, 100)
+    y = np.zeros((2, x.shape[0]), dtype=complex)
+    for fun_jac in [None, exp_fun_jac]:
+        for bc_jac in [None, exp_bc_jac]:
+            sol = solve_bvp(exp_fun, exp_bc_complex, x, y, fun_jac=fun_jac,
+                            bc_jac=bc_jac)
+
+            assert_equal(sol.status, 0)
+            assert_(sol.success)
+
+            sol_test = sol.sol(x_test)
+
+            assert_allclose(sol_test[0].real, exp_sol(x_test), atol=1e-5)
+            assert_allclose(sol_test[0].imag, exp_sol(x_test), atol=1e-5)
+
+            f_test = exp_fun(x_test, sol_test)
+            r = sol.sol(x_test, 1) - f_test
+            rel_res = r / (1 + np.abs(f_test))
+            norm_res = np.sum(np.real(rel_res * np.conj(rel_res)),
+                              axis=0) ** 0.5
+            assert_(np.all(norm_res < 1e-3))
+
+            assert_(np.all(sol.rms_residuals < 1e-3))
+            assert_allclose(sol.sol(sol.x), sol.y, rtol=1e-10, atol=1e-10)
+            assert_allclose(sol.sol(sol.x, 1), sol.yp, rtol=1e-10, atol=1e-10)
+
+
+def test_failures():
+    x = np.linspace(0, 1, 2)
+    y = np.zeros((2, x.size))
+    res = solve_bvp(exp_fun, exp_bc, x, y, tol=1e-5, max_nodes=5)
+    assert_equal(res.status, 1)
+    assert_(not res.success)
+
+    x = np.linspace(0, 1, 5)
+    y = np.zeros((2, x.size))
+    res = solve_bvp(undefined_fun, undefined_bc, x, y)
+    assert_equal(res.status, 2)
+    assert_(not res.success)
+
+
+def test_big_problem():
+    n = 30
+    x = np.linspace(0, 1, 5)
+    y = np.zeros((2 * n, x.size))
+    sol = solve_bvp(big_fun, big_bc, x, y)
+
+    assert_equal(sol.status, 0)
+    assert_(sol.success)
+
+    sol_test = sol.sol(x)
+
+    assert_allclose(sol_test[0], big_sol(x, n))
+
+    f_test = big_fun(x, sol_test)
+    r = sol.sol(x, 1) - f_test
+    rel_res = r / (1 + np.abs(f_test))
+    norm_res = np.sum(np.real(rel_res * np.conj(rel_res)), axis=0) ** 0.5
+    assert_(np.all(norm_res < 1e-3))
+
+    assert_(np.all(sol.rms_residuals < 1e-3))
+    assert_allclose(sol.sol(sol.x), sol.y, rtol=1e-10, atol=1e-10)
+    assert_allclose(sol.sol(sol.x, 1), sol.yp, rtol=1e-10, atol=1e-10)
+
+
+def test_big_problem_with_parameters():
+    n = 30
+    x = np.linspace(0, np.pi, 5)
+    x_test = np.linspace(0, np.pi, 100)
+    y = np.ones((2 * n, x.size))
+
+    for fun_jac in [None, big_fun_with_parameters_jac]:
+        for bc_jac in [None, big_bc_with_parameters_jac]:
+            sol = solve_bvp(big_fun_with_parameters, big_bc_with_parameters, x,
+                            y, p=[0.5, 0.5], fun_jac=fun_jac, bc_jac=bc_jac)
+
+            assert_equal(sol.status, 0)
+            assert_(sol.success)
+
+            assert_allclose(sol.p, [1, 1], rtol=1e-4)
+
+            sol_test = sol.sol(x_test)
+
+            for isol in range(0, n, 4):
+                assert_allclose(sol_test[isol],
+                                big_sol_with_parameters(x_test, [1, 1])[0],
+                                rtol=1e-4, atol=1e-4)
+                assert_allclose(sol_test[isol + 2],
+                                big_sol_with_parameters(x_test, [1, 1])[1],
+                                rtol=1e-4, atol=1e-4)
+
+            f_test = big_fun_with_parameters(x_test, sol_test, [1, 1])
+            r = sol.sol(x_test, 1) - f_test
+            rel_res = r / (1 + np.abs(f_test))
+            norm_res = np.sum(rel_res ** 2, axis=0) ** 0.5
+            assert_(np.all(norm_res < 1e-3))
+
+            assert_(np.all(sol.rms_residuals < 1e-3))
+            assert_allclose(sol.sol(sol.x), sol.y, rtol=1e-10, atol=1e-10)
+            assert_allclose(sol.sol(sol.x, 1), sol.yp, rtol=1e-10, atol=1e-10)
+
+
+def test_shock_layer():
+    x = np.linspace(-1, 1, 5)
+    x_test = np.linspace(-1, 1, 100)
+    y = np.zeros((2, x.size))
+    sol = solve_bvp(shock_fun, shock_bc, x, y)
+
+    assert_equal(sol.status, 0)
+    assert_(sol.success)
+
+    assert_(sol.x.size < 110)
+
+    sol_test = sol.sol(x_test)
+    assert_allclose(sol_test[0], shock_sol(x_test), rtol=1e-5, atol=1e-5)
+
+    f_test = shock_fun(x_test, sol_test)
+    r = sol.sol(x_test, 1) - f_test
+    rel_res = r / (1 + np.abs(f_test))
+    norm_res = np.sum(rel_res ** 2, axis=0) ** 0.5
+
+    assert_(np.all(norm_res < 1e-3))
+    assert_allclose(sol.sol(sol.x), sol.y, rtol=1e-10, atol=1e-10)
+    assert_allclose(sol.sol(sol.x, 1), sol.yp, rtol=1e-10, atol=1e-10)
+
+
+def test_nonlin_bc():
+    x = np.linspace(0, 0.1, 5)
+    x_test = x
+    y = np.zeros([2, x.size])
+    sol = solve_bvp(nonlin_bc_fun, nonlin_bc_bc, x, y)
+
+    assert_equal(sol.status, 0)
+    assert_(sol.success)
+
+    assert_(sol.x.size < 8)
+
+    sol_test = sol.sol(x_test)
+    assert_allclose(sol_test[0], nonlin_bc_sol(x_test), rtol=1e-5, atol=1e-5)
+
+    f_test = nonlin_bc_fun(x_test, sol_test)
+    r = sol.sol(x_test, 1) - f_test
+    rel_res = r / (1 + np.abs(f_test))
+    norm_res = np.sum(rel_res ** 2, axis=0) ** 0.5
+
+    assert_(np.all(norm_res < 1e-3))
+    assert_allclose(sol.sol(sol.x), sol.y, rtol=1e-10, atol=1e-10)
+    assert_allclose(sol.sol(sol.x, 1), sol.yp, rtol=1e-10, atol=1e-10)
+
+
+def test_verbose():
+    # Smoke test that checks the printing does something and does not crash
+    x = np.linspace(0, 1, 5)
+    y = np.zeros((2, x.shape[0]))
+    for verbose in [0, 1, 2]:
+        old_stdout = sys.stdout
+        sys.stdout = StringIO()
+        try:
+            sol = solve_bvp(exp_fun, exp_bc, x, y, verbose=verbose)
+            text = sys.stdout.getvalue()
+        finally:
+            sys.stdout = old_stdout
+
+        assert_(sol.success)
+        if verbose == 0:
+            assert_(not text, text)
+        if verbose >= 1:
+            assert_("Solved in" in text, text)
+        if verbose >= 2:
+            assert_("Max residual" in text, text)

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/tests/test_integrate.py

@@ -0,0 +1,830 @@
+# Authors: Nils Wagner, Ed Schofield, Pauli Virtanen, John Travers
+"""
+Tests for numerical integration.
+"""
+import numpy as np
+from numpy import (arange, zeros, array, dot, sqrt, cos, sin, eye, pi, exp,
+                   allclose)
+
+from numpy.testing import (
+    assert_, assert_array_almost_equal,
+    assert_allclose, assert_array_equal, assert_equal, assert_warns)
+from pytest import raises as assert_raises
+from scipy.integrate import odeint, ode, complex_ode
+
+#------------------------------------------------------------------------------
+# Test ODE integrators
+#------------------------------------------------------------------------------
+
+
+class TestOdeint:
+    # Check integrate.odeint
+
+    def _do_problem(self, problem):
+        t = arange(0.0, problem.stop_t, 0.05)
+
+        # Basic case
+        z, infodict = odeint(problem.f, problem.z0, t, full_output=True)
+        assert_(problem.verify(z, t))
+
+        # Use tfirst=True
+        z, infodict = odeint(lambda t, y: problem.f(y, t), problem.z0, t,
+                             full_output=True, tfirst=True)
+        assert_(problem.verify(z, t))
+
+        if hasattr(problem, 'jac'):
+            # Use Dfun
+            z, infodict = odeint(problem.f, problem.z0, t, Dfun=problem.jac,
+                                 full_output=True)
+            assert_(problem.verify(z, t))
+
+            # Use Dfun and tfirst=True
+            z, infodict = odeint(lambda t, y: problem.f(y, t), problem.z0, t,
+                                 Dfun=lambda t, y: problem.jac(y, t),
+                                 full_output=True, tfirst=True)
+            assert_(problem.verify(z, t))
+
+    def test_odeint(self):
+        for problem_cls in PROBLEMS:
+            problem = problem_cls()
+            if problem.cmplx:
+                continue
+            self._do_problem(problem)
+
+
+class TestODEClass:
+
+    ode_class = None   # Set in subclass.
+
+    def _do_problem(self, problem, integrator, method='adams'):
+
+        # ode has callback arguments in different order than odeint
+        f = lambda t, z: problem.f(z, t)
+        jac = None
+        if hasattr(problem, 'jac'):
+            jac = lambda t, z: problem.jac(z, t)
+
+        integrator_params = {}
+        if problem.lband is not None or problem.uband is not None:
+            integrator_params['uband'] = problem.uband
+            integrator_params['lband'] = problem.lband
+
+        ig = self.ode_class(f, jac)
+        ig.set_integrator(integrator,
+                          atol=problem.atol/10,
+                          rtol=problem.rtol/10,
+                          method=method,
+                          **integrator_params)
+
+        ig.set_initial_value(problem.z0, t=0.0)
+        z = ig.integrate(problem.stop_t)
+
+        assert_array_equal(z, ig.y)
+        assert_(ig.successful(), (problem, method))
+        assert_(ig.get_return_code() > 0, (problem, method))
+        assert_(problem.verify(array([z]), problem.stop_t), (problem, method))
+
+
+class TestOde(TestODEClass):
+
+    ode_class = ode
+
+    def test_vode(self):
+        # Check the vode solver
+        for problem_cls in PROBLEMS:
+            problem = problem_cls()
+            if problem.cmplx:
+                continue
+            if not problem.stiff:
+                self._do_problem(problem, 'vode', 'adams')
+            self._do_problem(problem, 'vode', 'bdf')
+
+    def test_zvode(self):
+        # Check the zvode solver
+        for problem_cls in PROBLEMS:
+            problem = problem_cls()
+            if not problem.stiff:
+                self._do_problem(problem, 'zvode', 'adams')
+            self._do_problem(problem, 'zvode', 'bdf')
+
+    def test_lsoda(self):
+        # Check the lsoda solver
+        for problem_cls in PROBLEMS:
+            problem = problem_cls()
+            if problem.cmplx:
+                continue
+            self._do_problem(problem, 'lsoda')
+
+    def test_dopri5(self):
+        # Check the dopri5 solver
+        for problem_cls in PROBLEMS:
+            problem = problem_cls()
+            if problem.cmplx:
+                continue
+            if problem.stiff:
+                continue
+            if hasattr(problem, 'jac'):
+                continue
+            self._do_problem(problem, 'dopri5')
+
+    def test_dop853(self):
+        # Check the dop853 solver
+        for problem_cls in PROBLEMS:
+            problem = problem_cls()
+            if problem.cmplx:
+                continue
+            if problem.stiff:
+                continue
+            if hasattr(problem, 'jac'):
+                continue
+            self._do_problem(problem, 'dop853')
+
+    def test_concurrent_fail(self):
+        for sol in ('vode', 'zvode', 'lsoda'):
+            f = lambda t, y: 1.0
+
+            r = ode(f).set_integrator(sol)
+            r.set_initial_value(0, 0)
+
+            r2 = ode(f).set_integrator(sol)
+            r2.set_initial_value(0, 0)
+
+            r.integrate(r.t + 0.1)
+            r2.integrate(r2.t + 0.1)
+
+            assert_raises(RuntimeError, r.integrate, r.t + 0.1)
+
+    def test_concurrent_ok(self):
+        f = lambda t, y: 1.0
+
+        for k in range(3):
+            for sol in ('vode', 'zvode', 'lsoda', 'dopri5', 'dop853'):
+                r = ode(f).set_integrator(sol)
+                r.set_initial_value(0, 0)
+
+                r2 = ode(f).set_integrator(sol)
+                r2.set_initial_value(0, 0)
+
+                r.integrate(r.t + 0.1)
+                r2.integrate(r2.t + 0.1)
+                r2.integrate(r2.t + 0.1)
+
+                assert_allclose(r.y, 0.1)
+                assert_allclose(r2.y, 0.2)
+
+            for sol in ('dopri5', 'dop853'):
+                r = ode(f).set_integrator(sol)
+                r.set_initial_value(0, 0)
+
+                r2 = ode(f).set_integrator(sol)
+                r2.set_initial_value(0, 0)
+
+                r.integrate(r.t + 0.1)
+                r.integrate(r.t + 0.1)
+                r2.integrate(r2.t + 0.1)
+                r.integrate(r.t + 0.1)
+                r2.integrate(r2.t + 0.1)
+
+                assert_allclose(r.y, 0.3)
+                assert_allclose(r2.y, 0.2)
+
+
+class TestComplexOde(TestODEClass):
+
+    ode_class = complex_ode
+
+    def test_vode(self):
+        # Check the vode solver
+        for problem_cls in PROBLEMS:
+            problem = problem_cls()
+            if not problem.stiff:
+                self._do_problem(problem, 'vode', 'adams')
+            else:
+                self._do_problem(problem, 'vode', 'bdf')
+
+    def test_lsoda(self):
+        # Check the lsoda solver
+        for problem_cls in PROBLEMS:
+            problem = problem_cls()
+            self._do_problem(problem, 'lsoda')
+
+    def test_dopri5(self):
+        # Check the dopri5 solver
+        for problem_cls in PROBLEMS:
+            problem = problem_cls()
+            if problem.stiff:
+                continue
+            if hasattr(problem, 'jac'):
+                continue
+            self._do_problem(problem, 'dopri5')
+
+    def test_dop853(self):
+        # Check the dop853 solver
+        for problem_cls in PROBLEMS:
+            problem = problem_cls()
+            if problem.stiff:
+                continue
+            if hasattr(problem, 'jac'):
+                continue
+            self._do_problem(problem, 'dop853')
+
+
+class TestSolout:
+    # Check integrate.ode correctly handles solout for dopri5 and dop853
+    def _run_solout_test(self, integrator):
+        # Check correct usage of solout
+        ts = []
+        ys = []
+        t0 = 0.0
+        tend = 10.0
+        y0 = [1.0, 2.0]
+
+        def solout(t, y):
+            ts.append(t)
+            ys.append(y.copy())
+
+        def rhs(t, y):
+            return [y[0] + y[1], -y[1]**2]
+
+        ig = ode(rhs).set_integrator(integrator)
+        ig.set_solout(solout)
+        ig.set_initial_value(y0, t0)
+        ret = ig.integrate(tend)
+        assert_array_equal(ys[0], y0)
+        assert_array_equal(ys[-1], ret)
+        assert_equal(ts[0], t0)
+        assert_equal(ts[-1], tend)
+
+    def test_solout(self):
+        for integrator in ('dopri5', 'dop853'):
+            self._run_solout_test(integrator)
+
+    def _run_solout_after_initial_test(self, integrator):
+        # Check if solout works even if it is set after the initial value.
+        ts = []
+        ys = []
+        t0 = 0.0
+        tend = 10.0
+        y0 = [1.0, 2.0]
+
+        def solout(t, y):
+            ts.append(t)
+            ys.append(y.copy())
+
+        def rhs(t, y):
+            return [y[0] + y[1], -y[1]**2]
+
+        ig = ode(rhs).set_integrator(integrator)
+        ig.set_initial_value(y0, t0)
+        ig.set_solout(solout)
+        ret = ig.integrate(tend)
+        assert_array_equal(ys[0], y0)
+        assert_array_equal(ys[-1], ret)
+        assert_equal(ts[0], t0)
+        assert_equal(ts[-1], tend)
+
+    def test_solout_after_initial(self):
+        for integrator in ('dopri5', 'dop853'):
+            self._run_solout_after_initial_test(integrator)
+
+    def _run_solout_break_test(self, integrator):
+        # Check correct usage of stopping via solout
+        ts = []
+        ys = []
+        t0 = 0.0
+        tend = 10.0
+        y0 = [1.0, 2.0]
+
+        def solout(t, y):
+            ts.append(t)
+            ys.append(y.copy())
+            if t > tend/2.0:
+                return -1
+
+        def rhs(t, y):
+            return [y[0] + y[1], -y[1]**2]
+
+        ig = ode(rhs).set_integrator(integrator)
+        ig.set_solout(solout)
+        ig.set_initial_value(y0, t0)
+        ret = ig.integrate(tend)
+        assert_array_equal(ys[0], y0)
+        assert_array_equal(ys[-1], ret)
+        assert_equal(ts[0], t0)
+        assert_(ts[-1] > tend/2.0)
+        assert_(ts[-1] < tend)
+
+    def test_solout_break(self):
+        for integrator in ('dopri5', 'dop853'):
+            self._run_solout_break_test(integrator)
+
+
+class TestComplexSolout:
+    # Check integrate.ode correctly handles solout for dopri5 and dop853
+    def _run_solout_test(self, integrator):
+        # Check correct usage of solout
+        ts = []
+        ys = []
+        t0 = 0.0
+        tend = 20.0
+        y0 = [0.0]
+
+        def solout(t, y):
+            ts.append(t)
+            ys.append(y.copy())
+
+        def rhs(t, y):
+            return [1.0/(t - 10.0 - 1j)]
+
+        ig = complex_ode(rhs).set_integrator(integrator)
+        ig.set_solout(solout)
+        ig.set_initial_value(y0, t0)
+        ret = ig.integrate(tend)
+        assert_array_equal(ys[0], y0)
+        assert_array_equal(ys[-1], ret)
+        assert_equal(ts[0], t0)
+        assert_equal(ts[-1], tend)
+
+    def test_solout(self):
+        for integrator in ('dopri5', 'dop853'):
+            self._run_solout_test(integrator)
+
+    def _run_solout_break_test(self, integrator):
+        # Check correct usage of stopping via solout
+        ts = []
+        ys = []
+        t0 = 0.0
+        tend = 20.0
+        y0 = [0.0]
+
+        def solout(t, y):
+            ts.append(t)
+            ys.append(y.copy())
+            if t > tend/2.0:
+                return -1
+
+        def rhs(t, y):
+            return [1.0/(t - 10.0 - 1j)]
+
+        ig = complex_ode(rhs).set_integrator(integrator)
+        ig.set_solout(solout)
+        ig.set_initial_value(y0, t0)
+        ret = ig.integrate(tend)
+        assert_array_equal(ys[0], y0)
+        assert_array_equal(ys[-1], ret)
+        assert_equal(ts[0], t0)
+        assert_(ts[-1] > tend/2.0)
+        assert_(ts[-1] < tend)
+
+    def test_solout_break(self):
+        for integrator in ('dopri5', 'dop853'):
+            self._run_solout_break_test(integrator)
+
+
+#------------------------------------------------------------------------------
+# Test problems
+#------------------------------------------------------------------------------
+
+
+class ODE:
+    """
+    ODE problem
+    """
+    stiff = False
+    cmplx = False
+    stop_t = 1
+    z0 = []
+
+    lband = None
+    uband = None
+
+    atol = 1e-6
+    rtol = 1e-5
+
+
+class SimpleOscillator(ODE):
+    r"""
+    Free vibration of a simple oscillator::
+        m \ddot{u} + k u = 0, u(0) = u_0 \dot{u}(0) \dot{u}_0
+    Solution::
+        u(t) = u_0*cos(sqrt(k/m)*t)+\dot{u}_0*sin(sqrt(k/m)*t)/sqrt(k/m)
+    """
+    stop_t = 1 + 0.09
+    z0 = array([1.0, 0.1], float)
+
+    k = 4.0
+    m = 1.0
+
+    def f(self, z, t):
+        tmp = zeros((2, 2), float)
+        tmp[0, 1] = 1.0
+        tmp[1, 0] = -self.k / self.m
+        return dot(tmp, z)
+
+    def verify(self, zs, t):
+        omega = sqrt(self.k / self.m)
+        u = self.z0[0]*cos(omega*t) + self.z0[1]*sin(omega*t)/omega
+        return allclose(u, zs[:, 0], atol=self.atol, rtol=self.rtol)
+
+
+class ComplexExp(ODE):
+    r"""The equation :lm:`\dot u = i u`"""
+    stop_t = 1.23*pi
+    z0 = exp([1j, 2j, 3j, 4j, 5j])
+    cmplx = True
+
+    def f(self, z, t):
+        return 1j*z
+
+    def jac(self, z, t):
+        return 1j*eye(5)
+
+    def verify(self, zs, t):
+        u = self.z0 * exp(1j*t)
+        return allclose(u, zs, atol=self.atol, rtol=self.rtol)
+
+
+class Pi(ODE):
+    r"""Integrate 1/(t + 1j) from t=-10 to t=10"""
+    stop_t = 20
+    z0 = [0]
+    cmplx = True
+
+    def f(self, z, t):
+        return array([1./(t - 10 + 1j)])
+
+    def verify(self, zs, t):
+        u = -2j * np.arctan(10)
+        return allclose(u, zs[-1, :], atol=self.atol, rtol=self.rtol)
+
+
+class CoupledDecay(ODE):
+    r"""
+    3 coupled decays suited for banded treatment
+    (banded mode makes it necessary when N>>3)
+    """
+
+    stiff = True
+    stop_t = 0.5
+    z0 = [5.0, 7.0, 13.0]
+    lband = 1
+    uband = 0
+
+    lmbd = [0.17, 0.23, 0.29]  # fictitious decay constants
+
+    def f(self, z, t):
+        lmbd = self.lmbd
+        return np.array([-lmbd[0]*z[0],
+                         -lmbd[1]*z[1] + lmbd[0]*z[0],
+                         -lmbd[2]*z[2] + lmbd[1]*z[1]])
+
+    def jac(self, z, t):
+        # The full Jacobian is
+        #
+        #    [-lmbd[0]      0         0   ]
+        #    [ lmbd[0]  -lmbd[1]      0   ]
+        #    [    0      lmbd[1]  -lmbd[2]]
+        #
+        # The lower and upper bandwidths are lband=1 and uband=0, resp.
+        # The representation of this array in packed format is
+        #
+        #    [-lmbd[0]  -lmbd[1]  -lmbd[2]]
+        #    [ lmbd[0]   lmbd[1]      0   ]
+
+        lmbd = self.lmbd
+        j = np.zeros((self.lband + self.uband + 1, 3), order='F')
+
+        def set_j(ri, ci, val):
+            j[self.uband + ri - ci, ci] = val
+        set_j(0, 0, -lmbd[0])
+        set_j(1, 0, lmbd[0])
+        set_j(1, 1, -lmbd[1])
+        set_j(2, 1, lmbd[1])
+        set_j(2, 2, -lmbd[2])
+        return j
+
+    def verify(self, zs, t):
+        # Formulae derived by hand
+        lmbd = np.array(self.lmbd)
+        d10 = lmbd[1] - lmbd[0]
+        d21 = lmbd[2] - lmbd[1]
+        d20 = lmbd[2] - lmbd[0]
+        e0 = np.exp(-lmbd[0] * t)
+        e1 = np.exp(-lmbd[1] * t)
+        e2 = np.exp(-lmbd[2] * t)
+        u = np.vstack((
+            self.z0[0] * e0,
+            self.z0[1] * e1 + self.z0[0] * lmbd[0] / d10 * (e0 - e1),
+            self.z0[2] * e2 + self.z0[1] * lmbd[1] / d21 * (e1 - e2) +
+            lmbd[1] * lmbd[0] * self.z0[0] / d10 *
+            (1 / d20 * (e0 - e2) - 1 / d21 * (e1 - e2)))).transpose()
+        return allclose(u, zs, atol=self.atol, rtol=self.rtol)
+
+
+PROBLEMS = [SimpleOscillator, ComplexExp, Pi, CoupledDecay]
+
+#------------------------------------------------------------------------------
+
+
+def f(t, x):
+    dxdt = [x[1], -x[0]]
+    return dxdt
+
+
+def jac(t, x):
+    j = array([[0.0, 1.0],
+               [-1.0, 0.0]])
+    return j
+
+
+def f1(t, x, omega):
+    dxdt = [omega*x[1], -omega*x[0]]
+    return dxdt
+
+
+def jac1(t, x, omega):
+    j = array([[0.0, omega],
+               [-omega, 0.0]])
+    return j
+
+
+def f2(t, x, omega1, omega2):
+    dxdt = [omega1*x[1], -omega2*x[0]]
+    return dxdt
+
+
+def jac2(t, x, omega1, omega2):
+    j = array([[0.0, omega1],
+               [-omega2, 0.0]])
+    return j
+
+
+def fv(t, x, omega):
+    dxdt = [omega[0]*x[1], -omega[1]*x[0]]
+    return dxdt
+
+
+def jacv(t, x, omega):
+    j = array([[0.0, omega[0]],
+               [-omega[1], 0.0]])
+    return j
+
+
+class ODECheckParameterUse:
+    """Call an ode-class solver with several cases of parameter use."""
+
+    # solver_name must be set before tests can be run with this class.
+
+    # Set these in subclasses.
+    solver_name = ''
+    solver_uses_jac = False
+
+    def _get_solver(self, f, jac):
+        solver = ode(f, jac)
+        if self.solver_uses_jac:
+            solver.set_integrator(self.solver_name, atol=1e-9, rtol=1e-7,
+                                  with_jacobian=self.solver_uses_jac)
+        else:
+            # XXX Shouldn't set_integrator *always* accept the keyword arg
+            # 'with_jacobian', and perhaps raise an exception if it is set
+            # to True if the solver can't actually use it?
+            solver.set_integrator(self.solver_name, atol=1e-9, rtol=1e-7)
+        return solver
+
+    def _check_solver(self, solver):
+        ic = [1.0, 0.0]
+        solver.set_initial_value(ic, 0.0)
+        solver.integrate(pi)
+        assert_array_almost_equal(solver.y, [-1.0, 0.0])
+
+    def test_no_params(self):
+        solver = self._get_solver(f, jac)
+        self._check_solver(solver)
+
+    def test_one_scalar_param(self):
+        solver = self._get_solver(f1, jac1)
+        omega = 1.0
+        solver.set_f_params(omega)
+        if self.solver_uses_jac:
+            solver.set_jac_params(omega)
+        self._check_solver(solver)
+
+    def test_two_scalar_params(self):
+        solver = self._get_solver(f2, jac2)
+        omega1 = 1.0
+        omega2 = 1.0
+        solver.set_f_params(omega1, omega2)
+        if self.solver_uses_jac:
+            solver.set_jac_params(omega1, omega2)
+        self._check_solver(solver)
+
+    def test_vector_param(self):
+        solver = self._get_solver(fv, jacv)
+        omega = [1.0, 1.0]
+        solver.set_f_params(omega)
+        if self.solver_uses_jac:
+            solver.set_jac_params(omega)
+        self._check_solver(solver)
+
+    def test_warns_on_failure(self):
+        # Set nsteps small to ensure failure
+        solver = self._get_solver(f, jac)
+        solver.set_integrator(self.solver_name, nsteps=1)
+        ic = [1.0, 0.0]
+        solver.set_initial_value(ic, 0.0)
+        assert_warns(UserWarning, solver.integrate, pi)
+
+
+class TestDOPRI5CheckParameterUse(ODECheckParameterUse):
+    solver_name = 'dopri5'
+    solver_uses_jac = False
+
+
+class TestDOP853CheckParameterUse(ODECheckParameterUse):
+    solver_name = 'dop853'
+    solver_uses_jac = False
+
+
+class TestVODECheckParameterUse(ODECheckParameterUse):
+    solver_name = 'vode'
+    solver_uses_jac = True
+
+
+class TestZVODECheckParameterUse(ODECheckParameterUse):
+    solver_name = 'zvode'
+    solver_uses_jac = True
+
+
+class TestLSODACheckParameterUse(ODECheckParameterUse):
+    solver_name = 'lsoda'
+    solver_uses_jac = True
+
+
+def test_odeint_trivial_time():
+    # Test that odeint succeeds when given a single time point
+    # and full_output=True.  This is a regression test for gh-4282.
+    y0 = 1
+    t = [0]
+    y, info = odeint(lambda y, t: -y, y0, t, full_output=True)
+    assert_array_equal(y, np.array([[y0]]))
+
+
+def test_odeint_banded_jacobian():
+    # Test the use of the `Dfun`, `ml` and `mu` options of odeint.
+
+    def func(y, t, c):
+        return c.dot(y)
+
+    def jac(y, t, c):
+        return c
+
+    def jac_transpose(y, t, c):
+        return c.T.copy(order='C')
+
+    def bjac_rows(y, t, c):
+        jac = np.row_stack((np.r_[0, np.diag(c, 1)],
+                            np.diag(c),
+                            np.r_[np.diag(c, -1), 0],
+                            np.r_[np.diag(c, -2), 0, 0]))
+        return jac
+
+    def bjac_cols(y, t, c):
+        return bjac_rows(y, t, c).T.copy(order='C')
+
+    c = array([[-205, 0.01, 0.00, 0.0],
+               [0.1, -2.50, 0.02, 0.0],
+               [1e-3, 0.01, -2.0, 0.01],
+               [0.00, 0.00, 0.1, -1.0]])
+
+    y0 = np.ones(4)
+    t = np.array([0, 5, 10, 100])
+
+    # Use the full Jacobian.
+    sol1, info1 = odeint(func, y0, t, args=(c,), full_output=True,
+                         atol=1e-13, rtol=1e-11, mxstep=10000,
+                         Dfun=jac)
+
+    # Use the transposed full Jacobian, with col_deriv=True.
+    sol2, info2 = odeint(func, y0, t, args=(c,), full_output=True,
+                         atol=1e-13, rtol=1e-11, mxstep=10000,
+                         Dfun=jac_transpose, col_deriv=True)
+
+    # Use the banded Jacobian.
+    sol3, info3 = odeint(func, y0, t, args=(c,), full_output=True,
+                         atol=1e-13, rtol=1e-11, mxstep=10000,
+                         Dfun=bjac_rows, ml=2, mu=1)
+
+    # Use the transposed banded Jacobian, with col_deriv=True.
+    sol4, info4 = odeint(func, y0, t, args=(c,), full_output=True,
+                         atol=1e-13, rtol=1e-11, mxstep=10000,
+                         Dfun=bjac_cols, ml=2, mu=1, col_deriv=True)
+
+    assert_allclose(sol1, sol2, err_msg="sol1 != sol2")
+    assert_allclose(sol1, sol3, atol=1e-12, err_msg="sol1 != sol3")
+    assert_allclose(sol3, sol4, err_msg="sol3 != sol4")
+
+    # Verify that the number of jacobian evaluations was the same for the
+    # calls of odeint with a full jacobian and with a banded jacobian. This is
+    # a regression test--there was a bug in the handling of banded jacobians
+    # that resulted in an incorrect jacobian matrix being passed to the LSODA
+    # code.  That would cause errors or excessive jacobian evaluations.
+    assert_array_equal(info1['nje'], info2['nje'])
+    assert_array_equal(info3['nje'], info4['nje'])
+
+    # Test the use of tfirst
+    sol1ty, info1ty = odeint(lambda t, y, c: func(y, t, c), y0, t, args=(c,),
+                             full_output=True, atol=1e-13, rtol=1e-11,
+                             mxstep=10000,
+                             Dfun=lambda t, y, c: jac(y, t, c), tfirst=True)
+    # The code should execute the exact same sequence of floating point
+    # calculations, so these should be exactly equal. We'll be safe and use
+    # a small tolerance.
+    assert_allclose(sol1, sol1ty, rtol=1e-12, err_msg="sol1 != sol1ty")
+
+
+def test_odeint_errors():
+    def sys1d(x, t):
+        return -100*x
+
+    def bad1(x, t):
+        return 1.0/0
+
+    def bad2(x, t):
+        return "foo"
+
+    def bad_jac1(x, t):
+        return 1.0/0
+
+    def bad_jac2(x, t):
+        return [["foo"]]
+
+    def sys2d(x, t):
+        return [-100*x[0], -0.1*x[1]]
+
+    def sys2d_bad_jac(x, t):
+        return [[1.0/0, 0], [0, -0.1]]
+
+    assert_raises(ZeroDivisionError, odeint, bad1, 1.0, [0, 1])
+    assert_raises(ValueError, odeint, bad2, 1.0, [0, 1])
+
+    assert_raises(ZeroDivisionError, odeint, sys1d, 1.0, [0, 1], Dfun=bad_jac1)
+    assert_raises(ValueError, odeint, sys1d, 1.0, [0, 1], Dfun=bad_jac2)
+
+    assert_raises(ZeroDivisionError, odeint, sys2d, [1.0, 1.0], [0, 1],
+                  Dfun=sys2d_bad_jac)
+
+
+def test_odeint_bad_shapes():
+    # Tests of some errors that can occur with odeint.
+
+    def badrhs(x, t):
+        return [1, -1]
+
+    def sys1(x, t):
+        return -100*x
+
+    def badjac(x, t):
+        return [[0, 0, 0]]
+
+    # y0 must be at most 1-d.
+    bad_y0 = [[0, 0], [0, 0]]
+    assert_raises(ValueError, odeint, sys1, bad_y0, [0, 1])
+
+    # t must be at most 1-d.
+    bad_t = [[0, 1], [2, 3]]
+    assert_raises(ValueError, odeint, sys1, [10.0], bad_t)
+
+    # y0 is 10, but badrhs(x, t) returns [1, -1].
+    assert_raises(RuntimeError, odeint, badrhs, 10, [0, 1])
+
+    # shape of array returned by badjac(x, t) is not correct.
+    assert_raises(RuntimeError, odeint, sys1, [10, 10], [0, 1], Dfun=badjac)
+
+
+def test_repeated_t_values():
+    """Regression test for gh-8217."""
+
+    def func(x, t):
+        return -0.25*x
+
+    t = np.zeros(10)
+    sol = odeint(func, [1.], t)
+    assert_array_equal(sol, np.ones((len(t), 1)))
+
+    tau = 4*np.log(2)
+    t = [0]*9 + [tau, 2*tau, 2*tau, 3*tau]
+    sol = odeint(func, [1, 2], t, rtol=1e-12, atol=1e-12)
+    expected_sol = np.array([[1.0, 2.0]]*9 +
+                            [[0.5, 1.0],
+                             [0.25, 0.5],
+                             [0.25, 0.5],
+                             [0.125, 0.25]])
+    assert_allclose(sol, expected_sol)
+
+    # Edge case: empty t sequence.
+    sol = odeint(func, [1.], [])
+    assert_array_equal(sol, np.array([], dtype=np.float64).reshape((0, 1)))
+
+    # t values are not monotonic.
+    assert_raises(ValueError, odeint, func, [1.], [0, 1, 0.5, 0])
+    assert_raises(ValueError, odeint, func, [1, 2, 3], [0, -1, -2, 3])

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/tests/test_odeint_jac.py

@@ -0,0 +1,75 @@
+
+import numpy as np
+from numpy.testing import assert_equal, assert_allclose
+from scipy.integrate import odeint
+import scipy.integrate._test_odeint_banded as banded5x5
+
+
+def rhs(y, t):
+    dydt = np.zeros_like(y)
+    banded5x5.banded5x5(t, y, dydt)
+    return dydt
+
+
+def jac(y, t):
+    n = len(y)
+    jac = np.zeros((n, n), order='F')
+    banded5x5.banded5x5_jac(t, y, 1, 1, jac)
+    return jac
+
+
+def bjac(y, t):
+    n = len(y)
+    bjac = np.zeros((4, n), order='F')
+    banded5x5.banded5x5_bjac(t, y, 1, 1, bjac)
+    return bjac
+
+
+JACTYPE_FULL = 1
+JACTYPE_BANDED = 4
+
+
+def check_odeint(jactype):
+    if jactype == JACTYPE_FULL:
+        ml = None
+        mu = None
+        jacobian = jac
+    elif jactype == JACTYPE_BANDED:
+        ml = 2
+        mu = 1
+        jacobian = bjac
+    else:
+        raise ValueError("invalid jactype: %r" % (jactype,))
+
+    y0 = np.arange(1.0, 6.0)
+    # These tolerances must match the tolerances used in banded5x5.f.
+    rtol = 1e-11
+    atol = 1e-13
+    dt = 0.125
+    nsteps = 64
+    t = dt * np.arange(nsteps+1)
+
+    sol, info = odeint(rhs, y0, t,
+                       Dfun=jacobian, ml=ml, mu=mu,
+                       atol=atol, rtol=rtol, full_output=True)
+    yfinal = sol[-1]
+    odeint_nst = info['nst'][-1]
+    odeint_nfe = info['nfe'][-1]
+    odeint_nje = info['nje'][-1]
+
+    y1 = y0.copy()
+    # Pure Fortran solution. y1 is modified in-place.
+    nst, nfe, nje = banded5x5.banded5x5_solve(y1, nsteps, dt, jactype)
+
+    # It is likely that yfinal and y1 are *exactly* the same, but
+    # we'll be cautious and use assert_allclose.
+    assert_allclose(yfinal, y1, rtol=1e-12)
+    assert_equal((odeint_nst, odeint_nfe, odeint_nje), (nst, nfe, nje))
+
+
+def test_odeint_full_jac():
+    check_odeint(JACTYPE_FULL)
+
+
+def test_odeint_banded_jac():
+    check_odeint(JACTYPE_BANDED)

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/tests/test_quadpack.py

@@ -0,0 +1,675 @@
+import sys
+import math
+import numpy as np
+from numpy import sqrt, cos, sin, arctan, exp, log, pi, Inf
+from numpy.testing import (assert_,
+        assert_allclose, assert_array_less, assert_almost_equal)
+import pytest
+
+from scipy.integrate import quad, dblquad, tplquad, nquad
+from scipy.special import erf, erfc
+from scipy._lib._ccallback import LowLevelCallable
+
+import ctypes
+import ctypes.util
+from scipy._lib._ccallback_c import sine_ctypes
+
+import scipy.integrate._test_multivariate as clib_test
+
+
+def assert_quad(value_and_err, tabled_value, error_tolerance=1.5e-8):
+    value, err = value_and_err
+    assert_allclose(value, tabled_value, atol=err, rtol=0)
+    if error_tolerance is not None:
+        assert_array_less(err, error_tolerance)
+
+
+def get_clib_test_routine(name, restype, *argtypes):
+    ptr = getattr(clib_test, name)
+    return ctypes.cast(ptr, ctypes.CFUNCTYPE(restype, *argtypes))
+
+
+class TestCtypesQuad:
+    def setup_method(self):
+        if sys.platform == 'win32':
+            files = ['api-ms-win-crt-math-l1-1-0.dll']
+        elif sys.platform == 'darwin':
+            files = ['libm.dylib']
+        else:
+            files = ['libm.so', 'libm.so.6']
+
+        for file in files:
+            try:
+                self.lib = ctypes.CDLL(file)
+                break
+            except OSError:
+                pass
+        else:
+            # This test doesn't work on some Linux platforms (Fedora for
+            # example) that put an ld script in libm.so - see gh-5370
+            pytest.skip("Ctypes can't import libm.so")
+
+        restype = ctypes.c_double
+        argtypes = (ctypes.c_double,)
+        for name in ['sin', 'cos', 'tan']:
+            func = getattr(self.lib, name)
+            func.restype = restype
+            func.argtypes = argtypes
+
+    def test_typical(self):
+        assert_quad(quad(self.lib.sin, 0, 5), quad(math.sin, 0, 5)[0])
+        assert_quad(quad(self.lib.cos, 0, 5), quad(math.cos, 0, 5)[0])
+        assert_quad(quad(self.lib.tan, 0, 1), quad(math.tan, 0, 1)[0])
+
+    def test_ctypes_sine(self):
+        quad(LowLevelCallable(sine_ctypes), 0, 1)
+
+    def test_ctypes_variants(self):
+        sin_0 = get_clib_test_routine('_sin_0', ctypes.c_double,
+                                      ctypes.c_double, ctypes.c_void_p)
+
+        sin_1 = get_clib_test_routine('_sin_1', ctypes.c_double,
+                                      ctypes.c_int, ctypes.POINTER(ctypes.c_double),
+                                      ctypes.c_void_p)
+
+        sin_2 = get_clib_test_routine('_sin_2', ctypes.c_double,
+                                      ctypes.c_double)
+
+        sin_3 = get_clib_test_routine('_sin_3', ctypes.c_double,
+                                      ctypes.c_int, ctypes.POINTER(ctypes.c_double))
+
+        sin_4 = get_clib_test_routine('_sin_3', ctypes.c_double,
+                                      ctypes.c_int, ctypes.c_double)
+
+        all_sigs = [sin_0, sin_1, sin_2, sin_3, sin_4]
+        legacy_sigs = [sin_2, sin_4]
+        legacy_only_sigs = [sin_4]
+
+        # LowLevelCallables work for new signatures
+        for j, func in enumerate(all_sigs):
+            callback = LowLevelCallable(func)
+            if func in legacy_only_sigs:
+                pytest.raises(ValueError, quad, callback, 0, pi)
+            else:
+                assert_allclose(quad(callback, 0, pi)[0], 2.0)
+
+        # Plain ctypes items work only for legacy signatures
+        for j, func in enumerate(legacy_sigs):
+            if func in legacy_sigs:
+                assert_allclose(quad(func, 0, pi)[0], 2.0)
+            else:
+                pytest.raises(ValueError, quad, func, 0, pi)
+
+
+class TestMultivariateCtypesQuad:
+    def setup_method(self):
+        restype = ctypes.c_double
+        argtypes = (ctypes.c_int, ctypes.c_double)
+        for name in ['_multivariate_typical', '_multivariate_indefinite',
+                     '_multivariate_sin']:
+            func = get_clib_test_routine(name, restype, *argtypes)
+            setattr(self, name, func)
+
+    def test_typical(self):
+        # 1) Typical function with two extra arguments:
+        assert_quad(quad(self._multivariate_typical, 0, pi, (2, 1.8)),
+                    0.30614353532540296487)
+
+    def test_indefinite(self):
+        # 2) Infinite integration limits --- Euler's constant
+        assert_quad(quad(self._multivariate_indefinite, 0, Inf),
+                    0.577215664901532860606512)
+
+    def test_threadsafety(self):
+        # Ensure multivariate ctypes are threadsafe
+        def threadsafety(y):
+            return y + quad(self._multivariate_sin, 0, 1)[0]
+        assert_quad(quad(threadsafety, 0, 1), 0.9596976941318602)
+
+
+class TestQuad:
+    def test_typical(self):
+        # 1) Typical function with two extra arguments:
+        def myfunc(x, n, z):       # Bessel function integrand
+            return cos(n*x-z*sin(x))/pi
+        assert_quad(quad(myfunc, 0, pi, (2, 1.8)), 0.30614353532540296487)
+
+    def test_indefinite(self):
+        # 2) Infinite integration limits --- Euler's constant
+        def myfunc(x):           # Euler's constant integrand
+            return -exp(-x)*log(x)
+        assert_quad(quad(myfunc, 0, Inf), 0.577215664901532860606512)
+
+    def test_singular(self):
+        # 3) Singular points in region of integration.
+        def myfunc(x):
+            if 0 < x < 2.5:
+                return sin(x)
+            elif 2.5 <= x <= 5.0:
+                return exp(-x)
+            else:
+                return 0.0
+
+        assert_quad(quad(myfunc, 0, 10, points=[2.5, 5.0]),
+                    1 - cos(2.5) + exp(-2.5) - exp(-5.0))
+
+    def test_sine_weighted_finite(self):
+        # 4) Sine weighted integral (finite limits)
+        def myfunc(x, a):
+            return exp(a*(x-1))
+
+        ome = 2.0**3.4
+        assert_quad(quad(myfunc, 0, 1, args=20, weight='sin', wvar=ome),
+                    (20*sin(ome)-ome*cos(ome)+ome*exp(-20))/(20**2 + ome**2))
+
+    def test_sine_weighted_infinite(self):
+        # 5) Sine weighted integral (infinite limits)
+        def myfunc(x, a):
+            return exp(-x*a)
+
+        a = 4.0
+        ome = 3.0
+        assert_quad(quad(myfunc, 0, Inf, args=a, weight='sin', wvar=ome),
+                    ome/(a**2 + ome**2))
+
+    def test_cosine_weighted_infinite(self):
+        # 6) Cosine weighted integral (negative infinite limits)
+        def myfunc(x, a):
+            return exp(x*a)
+
+        a = 2.5
+        ome = 2.3
+        assert_quad(quad(myfunc, -Inf, 0, args=a, weight='cos', wvar=ome),
+                    a/(a**2 + ome**2))
+
+    def test_algebraic_log_weight(self):
+        # 6) Algebraic-logarithmic weight.
+        def myfunc(x, a):
+            return 1/(1+x+2**(-a))
+
+        a = 1.5
+        assert_quad(quad(myfunc, -1, 1, args=a, weight='alg',
+                         wvar=(-0.5, -0.5)),
+                    pi/sqrt((1+2**(-a))**2 - 1))
+
+    def test_cauchypv_weight(self):
+        # 7) Cauchy prinicpal value weighting w(x) = 1/(x-c)
+        def myfunc(x, a):
+            return 2.0**(-a)/((x-1)**2+4.0**(-a))
+
+        a = 0.4
+        tabledValue = ((2.0**(-0.4)*log(1.5) -
+                        2.0**(-1.4)*log((4.0**(-a)+16) / (4.0**(-a)+1)) -
+                        arctan(2.0**(a+2)) -
+                        arctan(2.0**a)) /
+                       (4.0**(-a) + 1))
+        assert_quad(quad(myfunc, 0, 5, args=0.4, weight='cauchy', wvar=2.0),
+                    tabledValue, error_tolerance=1.9e-8)
+
+    def test_b_less_than_a(self):
+        def f(x, p, q):
+            return p * np.exp(-q*x)
+
+        val_1, err_1 = quad(f, 0, np.inf, args=(2, 3))
+        val_2, err_2 = quad(f, np.inf, 0, args=(2, 3))
+        assert_allclose(val_1, -val_2, atol=max(err_1, err_2))
+
+    def test_b_less_than_a_2(self):
+        def f(x, s):
+            return np.exp(-x**2 / 2 / s) / np.sqrt(2.*s)
+
+        val_1, err_1 = quad(f, -np.inf, np.inf, args=(2,))
+        val_2, err_2 = quad(f, np.inf, -np.inf, args=(2,))
+        assert_allclose(val_1, -val_2, atol=max(err_1, err_2))
+
+    def test_b_less_than_a_3(self):
+        def f(x):
+            return 1.0
+
+        val_1, err_1 = quad(f, 0, 1, weight='alg', wvar=(0, 0))
+        val_2, err_2 = quad(f, 1, 0, weight='alg', wvar=(0, 0))
+        assert_allclose(val_1, -val_2, atol=max(err_1, err_2))
+
+    def test_b_less_than_a_full_output(self):
+        def f(x):
+            return 1.0
+
+        res_1 = quad(f, 0, 1, weight='alg', wvar=(0, 0), full_output=True)
+        res_2 = quad(f, 1, 0, weight='alg', wvar=(0, 0), full_output=True)
+        err = max(res_1[1], res_2[1])
+        assert_allclose(res_1[0], -res_2[0], atol=err)
+
+    def test_double_integral(self):
+        # 8) Double Integral test
+        def simpfunc(y, x):       # Note order of arguments.
+            return x+y
+
+        a, b = 1.0, 2.0
+        assert_quad(dblquad(simpfunc, a, b, lambda x: x, lambda x: 2*x),
+                    5/6.0 * (b**3.0-a**3.0))
+
+    def test_double_integral2(self):
+        def func(x0, x1, t0, t1):
+            return x0 + x1 + t0 + t1
+        g = lambda x: x
+        h = lambda x: 2 * x
+        args = 1, 2
+        assert_quad(dblquad(func, 1, 2, g, h, args=args),35./6 + 9*.5)
+
+    def test_double_integral3(self):
+        def func(x0, x1):
+            return x0 + x1 + 1 + 2
+        assert_quad(dblquad(func, 1, 2, 1, 2),6.)
+
+    @pytest.mark.parametrize(
+        "x_lower, x_upper, y_lower, y_upper, expected",
+        [
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain D = [-inf, 0] for all n.
+            (-np.inf, 0, -np.inf, 0, np.pi / 4),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain D = [-inf, -1] for each n (one at a time).
+            (-np.inf, -1, -np.inf, 0, np.pi / 4 * erfc(1)),
+            (-np.inf, 0, -np.inf, -1, np.pi / 4 * erfc(1)),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain D = [-inf, -1] for all n.
+            (-np.inf, -1, -np.inf, -1, np.pi / 4 * (erfc(1) ** 2)),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain D = [-inf, 1] for each n (one at a time).
+            (-np.inf, 1, -np.inf, 0, np.pi / 4 * (erf(1) + 1)),
+            (-np.inf, 0, -np.inf, 1, np.pi / 4 * (erf(1) + 1)),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain D = [-inf, 1] for all n.
+            (-np.inf, 1, -np.inf, 1, np.pi / 4 * ((erf(1) + 1) ** 2)),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain Dx = [-inf, -1] and Dy = [-inf, 1].
+            (-np.inf, -1, -np.inf, 1, np.pi / 4 * ((erf(1) + 1) * erfc(1))),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain Dx = [-inf, 1] and Dy = [-inf, -1].
+            (-np.inf, 1, -np.inf, -1, np.pi / 4 * ((erf(1) + 1) * erfc(1))),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain D = [0, inf] for all n.
+            (0, np.inf, 0, np.inf, np.pi / 4),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain D = [1, inf] for each n (one at a time).
+            (1, np.inf, 0, np.inf, np.pi / 4 * erfc(1)),
+            (0, np.inf, 1, np.inf, np.pi / 4 * erfc(1)),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain D = [1, inf] for all n.
+            (1, np.inf, 1, np.inf, np.pi / 4 * (erfc(1) ** 2)),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain D = [-1, inf] for each n (one at a time).
+            (-1, np.inf, 0, np.inf, np.pi / 4 * (erf(1) + 1)),
+            (0, np.inf, -1, np.inf, np.pi / 4 * (erf(1) + 1)),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain D = [-1, inf] for all n.
+            (-1, np.inf, -1, np.inf, np.pi / 4 * ((erf(1) + 1) ** 2)),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain Dx = [-1, inf] and Dy = [1, inf].
+            (-1, np.inf, 1, np.inf, np.pi / 4 * ((erf(1) + 1) * erfc(1))),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain Dx = [1, inf] and Dy = [-1, inf].
+            (1, np.inf, -1, np.inf, np.pi / 4 * ((erf(1) + 1) * erfc(1))),
+            # Multiple integration of a function in n = 2 variables: f(x, y, z)
+            # over domain D = [-inf, inf] for all n.
+            (-np.inf, np.inf, -np.inf, np.inf, np.pi)
+        ]
+    )
+    def test_double_integral_improper(
+            self, x_lower, x_upper, y_lower, y_upper, expected
+    ):
+        # The Gaussian Integral.
+        def f(x, y):
+            return np.exp(-x ** 2 - y ** 2)
+
+        assert_quad(
+            dblquad(f, x_lower, x_upper, y_lower, y_upper),
+            expected,
+            error_tolerance=3e-8
+        )
+
+    def test_triple_integral(self):
+        # 9) Triple Integral test
+        def simpfunc(z, y, x, t):      # Note order of arguments.
+            return (x+y+z)*t
+
+        a, b = 1.0, 2.0
+        assert_quad(tplquad(simpfunc, a, b,
+                            lambda x: x, lambda x: 2*x,
+                            lambda x, y: x - y, lambda x, y: x + y,
+                            (2.,)),
+                     2*8/3.0 * (b**4.0 - a**4.0))
+
+    @pytest.mark.parametrize(
+        "x_lower, x_upper, y_lower, y_upper, z_lower, z_upper, expected",
+        [
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [-inf, 0] for all n.
+            (-np.inf, 0, -np.inf, 0, -np.inf, 0, (np.pi ** (3 / 2)) / 8),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [-inf, -1] for each n (one at a time).
+            (-np.inf, -1, -np.inf, 0, -np.inf, 0,
+             (np.pi ** (3 / 2)) / 8 * erfc(1)),
+            (-np.inf, 0, -np.inf, -1, -np.inf, 0,
+             (np.pi ** (3 / 2)) / 8 * erfc(1)),
+            (-np.inf, 0, -np.inf, 0, -np.inf, -1,
+             (np.pi ** (3 / 2)) / 8 * erfc(1)),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [-inf, -1] for each n (two at a time).
+            (-np.inf, -1, -np.inf, -1, -np.inf, 0,
+             (np.pi ** (3 / 2)) / 8 * (erfc(1) ** 2)),
+            (-np.inf, -1, -np.inf, 0, -np.inf, -1,
+             (np.pi ** (3 / 2)) / 8 * (erfc(1) ** 2)),
+            (-np.inf, 0, -np.inf, -1, -np.inf, -1,
+             (np.pi ** (3 / 2)) / 8 * (erfc(1) ** 2)),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [-inf, -1] for all n.
+            (-np.inf, -1, -np.inf, -1, -np.inf, -1,
+             (np.pi ** (3 / 2)) / 8 * (erfc(1) ** 3)),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain Dx = [-inf, -1] and Dy = Dz = [-inf, 1].
+            (-np.inf, -1, -np.inf, 1, -np.inf, 1,
+             (np.pi ** (3 / 2)) / 8 * (((erf(1) + 1) ** 2) * erfc(1))),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain Dx = Dy = [-inf, -1] and Dz = [-inf, 1].
+            (-np.inf, -1, -np.inf, -1, -np.inf, 1,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) * (erfc(1) ** 2))),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain Dx = Dz = [-inf, -1] and Dy = [-inf, 1].
+            (-np.inf, -1, -np.inf, 1, -np.inf, -1,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) * (erfc(1) ** 2))),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain Dx = [-inf, 1] and Dy = Dz = [-inf, -1].
+            (-np.inf, 1, -np.inf, -1, -np.inf, -1,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) * (erfc(1) ** 2))),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain Dx = Dy = [-inf, 1] and Dz = [-inf, -1].
+            (-np.inf, 1, -np.inf, 1, -np.inf, -1,
+             (np.pi ** (3 / 2)) / 8 * (((erf(1) + 1) ** 2) * erfc(1))),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain Dx = Dz = [-inf, 1] and Dy = [-inf, -1].
+            (-np.inf, 1, -np.inf, -1, -np.inf, 1,
+             (np.pi ** (3 / 2)) / 8 * (((erf(1) + 1) ** 2) * erfc(1))),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [-inf, 1] for each n (one at a time).
+            (-np.inf, 1, -np.inf, 0, -np.inf, 0,
+             (np.pi ** (3 / 2)) / 8 * (erf(1) + 1)),
+            (-np.inf, 0, -np.inf, 1, -np.inf, 0,
+             (np.pi ** (3 / 2)) / 8 * (erf(1) + 1)),
+            (-np.inf, 0, -np.inf, 0, -np.inf, 1,
+             (np.pi ** (3 / 2)) / 8 * (erf(1) + 1)),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [-inf, 1] for each n (two at a time).
+            (-np.inf, 1, -np.inf, 1, -np.inf, 0,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) ** 2)),
+            (-np.inf, 1, -np.inf, 0, -np.inf, 1,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) ** 2)),
+            (-np.inf, 0, -np.inf, 1, -np.inf, 1,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) ** 2)),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [-inf, 1] for all n.
+            (-np.inf, 1, -np.inf, 1, -np.inf, 1,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) ** 3)),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [0, inf] for all n.
+            (0, np.inf, 0, np.inf, 0, np.inf, (np.pi ** (3 / 2)) / 8),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [1, inf] for each n (one at a time).
+            (1, np.inf, 0, np.inf, 0, np.inf,
+             (np.pi ** (3 / 2)) / 8 * erfc(1)),
+            (0, np.inf, 1, np.inf, 0, np.inf,
+             (np.pi ** (3 / 2)) / 8 * erfc(1)),
+            (0, np.inf, 0, np.inf, 1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * erfc(1)),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [1, inf] for each n (two at a time).
+            (1, np.inf, 1, np.inf, 0, np.inf,
+             (np.pi ** (3 / 2)) / 8 * (erfc(1) ** 2)),
+            (1, np.inf, 0, np.inf, 1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * (erfc(1) ** 2)),
+            (0, np.inf, 1, np.inf, 1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * (erfc(1) ** 2)),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [1, inf] for all n.
+            (1, np.inf, 1, np.inf, 1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * (erfc(1) ** 3)),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [-1, inf] for each n (one at a time).
+            (-1, np.inf, 0, np.inf, 0, np.inf,
+             (np.pi ** (3 / 2)) / 8 * (erf(1) + 1)),
+            (0, np.inf, -1, np.inf, 0, np.inf,
+             (np.pi ** (3 / 2)) / 8 * (erf(1) + 1)),
+            (0, np.inf, 0, np.inf, -1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * (erf(1) + 1)),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [-1, inf] for each n (two at a time).
+            (-1, np.inf, -1, np.inf, 0, np.inf,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) ** 2)),
+            (-1, np.inf, 0, np.inf, -1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) ** 2)),
+            (0, np.inf, -1, np.inf, -1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) ** 2)),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [-1, inf] for all n.
+            (-1, np.inf, -1, np.inf, -1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) ** 3)),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain Dx = [1, inf] and Dy = Dz = [-1, inf].
+            (1, np.inf, -1, np.inf, -1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * (((erf(1) + 1) ** 2) * erfc(1))),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain Dx = Dy = [1, inf] and Dz = [-1, inf].
+            (1, np.inf, 1, np.inf, -1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) * (erfc(1) ** 2))),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain Dx = Dz = [1, inf] and Dy = [-1, inf].
+            (1, np.inf, -1, np.inf, 1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) * (erfc(1) ** 2))),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain Dx = [-1, inf] and Dy = Dz = [1, inf].
+            (-1, np.inf, 1, np.inf, 1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * ((erf(1) + 1) * (erfc(1) ** 2))),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain Dx = Dy = [-1, inf] and Dz = [1, inf].
+            (-1, np.inf, -1, np.inf, 1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * (((erf(1) + 1) ** 2) * erfc(1))),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain Dx = Dz = [-1, inf] and Dy = [1, inf].
+            (-1, np.inf, 1, np.inf, -1, np.inf,
+             (np.pi ** (3 / 2)) / 8 * (((erf(1) + 1) ** 2) * erfc(1))),
+            # Multiple integration of a function in n = 3 variables: f(x, y, z)
+            # over domain D = [-inf, inf] for all n.
+            (-np.inf, np.inf, -np.inf, np.inf, -np.inf, np.inf,
+             np.pi ** (3 / 2)),
+        ],
+    )
+    def test_triple_integral_improper(
+            self,
+            x_lower,
+            x_upper,
+            y_lower,
+            y_upper,
+            z_lower,
+            z_upper,
+            expected
+    ):
+        # The Gaussian Integral.
+        def f(x, y, z):
+            return np.exp(-x ** 2 - y ** 2 - z ** 2)
+
+        assert_quad(
+            tplquad(f, x_lower, x_upper, y_lower, y_upper, z_lower, z_upper),
+            expected,
+            error_tolerance=6e-8
+        )
+
+    def test_complex(self):
+        def tfunc(x):
+            return np.exp(1j*x)
+
+        assert np.allclose(
+                    quad(tfunc, 0, np.pi/2, complex_func=True)[0],
+                    1+1j)
+
+        # We consider a divergent case in order to force quadpack
+        # to return an error message.  The output is compared
+        # against what is returned by explicit integration
+        # of the parts.
+        kwargs = {'a': 0, 'b': np.inf, 'full_output': True,
+                  'weight': 'cos', 'wvar': 1}
+        res_c = quad(tfunc, complex_func=True, **kwargs)
+        res_r = quad(lambda x: np.real(np.exp(1j*x)),
+                     complex_func=False,
+                     **kwargs)
+        res_i = quad(lambda x: np.imag(np.exp(1j*x)),
+                     complex_func=False,
+                     **kwargs)
+
+        np.testing.assert_equal(res_c[0], res_r[0] + 1j*res_i[0])
+        np.testing.assert_equal(res_c[1], res_r[1] + 1j*res_i[1])
+
+        assert len(res_c[2]['real']) == len(res_r[2:]) == 3
+        assert res_c[2]['real'][2] == res_r[4]
+        assert res_c[2]['real'][1] == res_r[3]
+        assert res_c[2]['real'][0]['lst'] == res_r[2]['lst']
+
+        assert len(res_c[2]['imag']) == len(res_i[2:]) == 1
+        assert res_c[2]['imag'][0]['lst'] == res_i[2]['lst']
+
+
+class TestNQuad:
+    def test_fixed_limits(self):
+        def func1(x0, x1, x2, x3):
+            val = (x0**2 + x1*x2 - x3**3 + np.sin(x0) +
+                   (1 if (x0 - 0.2*x3 - 0.5 - 0.25*x1 > 0) else 0))
+            return val
+
+        def opts_basic(*args):
+            return {'points': [0.2*args[2] + 0.5 + 0.25*args[0]]}
+
+        res = nquad(func1, [[0, 1], [-1, 1], [.13, .8], [-.15, 1]],
+                    opts=[opts_basic, {}, {}, {}], full_output=True)
+        assert_quad(res[:-1], 1.5267454070738635)
+        assert_(res[-1]['neval'] > 0 and res[-1]['neval'] < 4e5)
+
+    def test_variable_limits(self):
+        scale = .1
+
+        def func2(x0, x1, x2, x3, t0, t1):
+            val = (x0*x1*x3**2 + np.sin(x2) + 1 +
+                   (1 if x0 + t1*x1 - t0 > 0 else 0))
+            return val
+
+        def lim0(x1, x2, x3, t0, t1):
+            return [scale * (x1**2 + x2 + np.cos(x3)*t0*t1 + 1) - 1,
+                    scale * (x1**2 + x2 + np.cos(x3)*t0*t1 + 1) + 1]
+
+        def lim1(x2, x3, t0, t1):
+            return [scale * (t0*x2 + t1*x3) - 1,
+                    scale * (t0*x2 + t1*x3) + 1]
+
+        def lim2(x3, t0, t1):
+            return [scale * (x3 + t0**2*t1**3) - 1,
+                    scale * (x3 + t0**2*t1**3) + 1]
+
+        def lim3(t0, t1):
+            return [scale * (t0 + t1) - 1, scale * (t0 + t1) + 1]
+
+        def opts0(x1, x2, x3, t0, t1):
+            return {'points': [t0 - t1*x1]}
+
+        def opts1(x2, x3, t0, t1):
+            return {}
+
+        def opts2(x3, t0, t1):
+            return {}
+
+        def opts3(t0, t1):
+            return {}
+
+        res = nquad(func2, [lim0, lim1, lim2, lim3], args=(0, 0),
+                    opts=[opts0, opts1, opts2, opts3])
+        assert_quad(res, 25.066666666666663)
+
+    def test_square_separate_ranges_and_opts(self):
+        def f(y, x):
+            return 1.0
+
+        assert_quad(nquad(f, [[-1, 1], [-1, 1]], opts=[{}, {}]), 4.0)
+
+    def test_square_aliased_ranges_and_opts(self):
+        def f(y, x):
+            return 1.0
+
+        r = [-1, 1]
+        opt = {}
+        assert_quad(nquad(f, [r, r], opts=[opt, opt]), 4.0)
+
+    def test_square_separate_fn_ranges_and_opts(self):
+        def f(y, x):
+            return 1.0
+
+        def fn_range0(*args):
+            return (-1, 1)
+
+        def fn_range1(*args):
+            return (-1, 1)
+
+        def fn_opt0(*args):
+            return {}
+
+        def fn_opt1(*args):
+            return {}
+
+        ranges = [fn_range0, fn_range1]
+        opts = [fn_opt0, fn_opt1]
+        assert_quad(nquad(f, ranges, opts=opts), 4.0)
+
+    def test_square_aliased_fn_ranges_and_opts(self):
+        def f(y, x):
+            return 1.0
+
+        def fn_range(*args):
+            return (-1, 1)
+
+        def fn_opt(*args):
+            return {}
+
+        ranges = [fn_range, fn_range]
+        opts = [fn_opt, fn_opt]
+        assert_quad(nquad(f, ranges, opts=opts), 4.0)
+
+    def test_matching_quad(self):
+        def func(x):
+            return x**2 + 1
+
+        res, reserr = quad(func, 0, 4)
+        res2, reserr2 = nquad(func, ranges=[[0, 4]])
+        assert_almost_equal(res, res2)
+        assert_almost_equal(reserr, reserr2)
+
+    def test_matching_dblquad(self):
+        def func2d(x0, x1):
+            return x0**2 + x1**3 - x0 * x1 + 1
+
+        res, reserr = dblquad(func2d, -2, 2, lambda x: -3, lambda x: 3)
+        res2, reserr2 = nquad(func2d, [[-3, 3], (-2, 2)])
+        assert_almost_equal(res, res2)
+        assert_almost_equal(reserr, reserr2)
+
+    def test_matching_tplquad(self):
+        def func3d(x0, x1, x2, c0, c1):
+            return x0**2 + c0 * x1**3 - x0 * x1 + 1 + c1 * np.sin(x2)
+
+        res = tplquad(func3d, -1, 2, lambda x: -2, lambda x: 2,
+                      lambda x, y: -np.pi, lambda x, y: np.pi,
+                      args=(2, 3))
+        res2 = nquad(func3d, [[-np.pi, np.pi], [-2, 2], (-1, 2)], args=(2, 3))
+        assert_almost_equal(res, res2)
+
+    def test_dict_as_opts(self):
+        try:
+            nquad(lambda x, y: x * y, [[0, 1], [0, 1]], opts={'epsrel': 0.0001})
+        except TypeError:
+            assert False
+

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/tests/test_quadrature.py

@@ -0,0 +1,397 @@
+import pytest
+import numpy as np
+from numpy import cos, sin, pi
+from numpy.testing import (assert_equal, assert_almost_equal, assert_allclose,
+                           assert_, suppress_warnings)
+
+from scipy.integrate import (quadrature, romberg, romb, newton_cotes,
+                             cumulative_trapezoid, cumtrapz, trapz, trapezoid,
+                             quad, simpson, simps, fixed_quad, AccuracyWarning)
+from scipy.integrate._quadrature import _qmc_quad as qmc_quad
+from scipy import stats, special as sc
+
+
+class TestFixedQuad:
+    def test_scalar(self):
+        n = 4
+        expected = 1/(2*n)
+        got, _ = fixed_quad(lambda x: x**(2*n - 1), 0, 1, n=n)
+        # quadrature exact for this input
+        assert_allclose(got, expected, rtol=1e-12)
+
+    def test_vector(self):
+        n = 4
+        p = np.arange(1, 2*n)
+        expected = 1/(p + 1)
+        got, _ = fixed_quad(lambda x: x**p[:, None], 0, 1, n=n)
+        assert_allclose(got, expected, rtol=1e-12)
+
+
+class TestQuadrature:
+    def quad(self, x, a, b, args):
+        raise NotImplementedError
+
+    def test_quadrature(self):
+        # Typical function with two extra arguments:
+        def myfunc(x, n, z):       # Bessel function integrand
+            return cos(n*x-z*sin(x))/pi
+        val, err = quadrature(myfunc, 0, pi, (2, 1.8))
+        table_val = 0.30614353532540296487
+        assert_almost_equal(val, table_val, decimal=7)
+
+    def test_quadrature_rtol(self):
+        def myfunc(x, n, z):       # Bessel function integrand
+            return 1e90 * cos(n*x-z*sin(x))/pi
+        val, err = quadrature(myfunc, 0, pi, (2, 1.8), rtol=1e-10)
+        table_val = 1e90 * 0.30614353532540296487
+        assert_allclose(val, table_val, rtol=1e-10)
+
+    def test_quadrature_miniter(self):
+        # Typical function with two extra arguments:
+        def myfunc(x, n, z):       # Bessel function integrand
+            return cos(n*x-z*sin(x))/pi
+        table_val = 0.30614353532540296487
+        for miniter in [5, 52]:
+            val, err = quadrature(myfunc, 0, pi, (2, 1.8), miniter=miniter)
+            assert_almost_equal(val, table_val, decimal=7)
+            assert_(err < 1.0)
+
+    def test_quadrature_single_args(self):
+        def myfunc(x, n):
+            return 1e90 * cos(n*x-1.8*sin(x))/pi
+        val, err = quadrature(myfunc, 0, pi, args=2, rtol=1e-10)
+        table_val = 1e90 * 0.30614353532540296487
+        assert_allclose(val, table_val, rtol=1e-10)
+
+    def test_romberg(self):
+        # Typical function with two extra arguments:
+        def myfunc(x, n, z):       # Bessel function integrand
+            return cos(n*x-z*sin(x))/pi
+        val = romberg(myfunc, 0, pi, args=(2, 1.8))
+        table_val = 0.30614353532540296487
+        assert_almost_equal(val, table_val, decimal=7)
+
+    def test_romberg_rtol(self):
+        # Typical function with two extra arguments:
+        def myfunc(x, n, z):       # Bessel function integrand
+            return 1e19*cos(n*x-z*sin(x))/pi
+        val = romberg(myfunc, 0, pi, args=(2, 1.8), rtol=1e-10)
+        table_val = 1e19*0.30614353532540296487
+        assert_allclose(val, table_val, rtol=1e-10)
+
+    def test_romb(self):
+        assert_equal(romb(np.arange(17)), 128)
+
+    def test_romb_gh_3731(self):
+        # Check that romb makes maximal use of data points
+        x = np.arange(2**4+1)
+        y = np.cos(0.2*x)
+        val = romb(y)
+        val2, err = quad(lambda x: np.cos(0.2*x), x.min(), x.max())
+        assert_allclose(val, val2, rtol=1e-8, atol=0)
+
+        # should be equal to romb with 2**k+1 samples
+        with suppress_warnings() as sup:
+            sup.filter(AccuracyWarning, "divmax .4. exceeded")
+            val3 = romberg(lambda x: np.cos(0.2*x), x.min(), x.max(), divmax=4)
+        assert_allclose(val, val3, rtol=1e-12, atol=0)
+
+    def test_non_dtype(self):
+        # Check that we work fine with functions returning float
+        import math
+        valmath = romberg(math.sin, 0, 1)
+        expected_val = 0.45969769413185085
+        assert_almost_equal(valmath, expected_val, decimal=7)
+
+    def test_newton_cotes(self):
+        """Test the first few degrees, for evenly spaced points."""
+        n = 1
+        wts, errcoff = newton_cotes(n, 1)
+        assert_equal(wts, n*np.array([0.5, 0.5]))
+        assert_almost_equal(errcoff, -n**3/12.0)
+
+        n = 2
+        wts, errcoff = newton_cotes(n, 1)
+        assert_almost_equal(wts, n*np.array([1.0, 4.0, 1.0])/6.0)
+        assert_almost_equal(errcoff, -n**5/2880.0)
+
+        n = 3
+        wts, errcoff = newton_cotes(n, 1)
+        assert_almost_equal(wts, n*np.array([1.0, 3.0, 3.0, 1.0])/8.0)
+        assert_almost_equal(errcoff, -n**5/6480.0)
+
+        n = 4
+        wts, errcoff = newton_cotes(n, 1)
+        assert_almost_equal(wts, n*np.array([7.0, 32.0, 12.0, 32.0, 7.0])/90.0)
+        assert_almost_equal(errcoff, -n**7/1935360.0)
+
+    def test_newton_cotes2(self):
+        """Test newton_cotes with points that are not evenly spaced."""
+
+        x = np.array([0.0, 1.5, 2.0])
+        y = x**2
+        wts, errcoff = newton_cotes(x)
+        exact_integral = 8.0/3
+        numeric_integral = np.dot(wts, y)
+        assert_almost_equal(numeric_integral, exact_integral)
+
+        x = np.array([0.0, 1.4, 2.1, 3.0])
+        y = x**2
+        wts, errcoff = newton_cotes(x)
+        exact_integral = 9.0
+        numeric_integral = np.dot(wts, y)
+        assert_almost_equal(numeric_integral, exact_integral)
+
+    def test_simpson(self):
+        y = np.arange(17)
+        assert_equal(simpson(y), 128)
+        assert_equal(simpson(y, dx=0.5), 64)
+        assert_equal(simpson(y, x=np.linspace(0, 4, 17)), 32)
+
+        y = np.arange(4)
+        x = 2**y
+        assert_equal(simpson(y, x=x, even='avg'), 13.875)
+        assert_equal(simpson(y, x=x, even='first'), 13.75)
+        assert_equal(simpson(y, x=x, even='last'), 14)
+
+        # Tests for checking base case
+        x = np.array([3])
+        y = np.power(x, 2)
+        assert_equal(simpson(y, x=x, axis=0), 0.0)
+        assert_equal(simpson(y, x=x, axis=-1), 0.0)
+
+        x = np.array([3, 3, 3, 3])
+        y = np.power(x, 2)
+        assert_equal(simpson(y, x=x, axis=0), 0.0)
+        assert_equal(simpson(y, x=x, axis=-1), 0.0)
+
+        x = np.array([[1, 2, 4, 8], [1, 2, 4, 8], [1, 2, 4, 8]])
+        y = np.power(x, 2)
+        zero_axis = [0.0, 0.0, 0.0, 0.0]
+        default_axis = [175.75, 175.75, 175.75]
+        assert_equal(simpson(y, x=x, axis=0), zero_axis)
+        assert_equal(simpson(y, x=x, axis=-1), default_axis)
+
+        x = np.array([[1, 2, 4, 8], [1, 2, 4, 8], [1, 8, 16, 32]])
+        y = np.power(x, 2)
+        zero_axis = [0.0, 136.0, 1088.0, 8704.0]
+        default_axis = [175.75, 175.75, 11292.25]
+        assert_equal(simpson(y, x=x, axis=0), zero_axis)
+        assert_equal(simpson(y, x=x, axis=-1), default_axis)
+
+    @pytest.mark.parametrize('droplast', [False, True])
+    def test_simpson_2d_integer_no_x(self, droplast):
+        # The inputs are 2d integer arrays.  The results should be
+        # identical to the results when the inputs are floating point.
+        y = np.array([[2, 2, 4, 4, 8, 8, -4, 5],
+                      [4, 4, 2, -4, 10, 22, -2, 10]])
+        if droplast:
+            y = y[:, :-1]
+        result = simpson(y, axis=-1)
+        expected = simpson(np.array(y, dtype=np.float64), axis=-1)
+        assert_equal(result, expected)
+
+    def test_simps(self):
+        # Basic coverage test for the alias
+        y = np.arange(4)
+        x = 2**y
+        assert_equal(simpson(y, x=x, dx=0.5, even='first'),
+                     simps(y, x=x, dx=0.5, even='first'))
+
+
+class TestCumulative_trapezoid:
+    def test_1d(self):
+        x = np.linspace(-2, 2, num=5)
+        y = x
+        y_int = cumulative_trapezoid(y, x, initial=0)
+        y_expected = [0., -1.5, -2., -1.5, 0.]
+        assert_allclose(y_int, y_expected)
+
+        y_int = cumulative_trapezoid(y, x, initial=None)
+        assert_allclose(y_int, y_expected[1:])
+
+    def test_y_nd_x_nd(self):
+        x = np.arange(3 * 2 * 4).reshape(3, 2, 4)
+        y = x
+        y_int = cumulative_trapezoid(y, x, initial=0)
+        y_expected = np.array([[[0., 0.5, 2., 4.5],
+                                [0., 4.5, 10., 16.5]],
+                               [[0., 8.5, 18., 28.5],
+                                [0., 12.5, 26., 40.5]],
+                               [[0., 16.5, 34., 52.5],
+                                [0., 20.5, 42., 64.5]]])
+
+        assert_allclose(y_int, y_expected)
+
+        # Try with all axes
+        shapes = [(2, 2, 4), (3, 1, 4), (3, 2, 3)]
+        for axis, shape in zip([0, 1, 2], shapes):
+            y_int = cumulative_trapezoid(y, x, initial=3.45, axis=axis)
+            assert_equal(y_int.shape, (3, 2, 4))
+            y_int = cumulative_trapezoid(y, x, initial=None, axis=axis)
+            assert_equal(y_int.shape, shape)
+
+    def test_y_nd_x_1d(self):
+        y = np.arange(3 * 2 * 4).reshape(3, 2, 4)
+        x = np.arange(4)**2
+        # Try with all axes
+        ys_expected = (
+            np.array([[[4., 5., 6., 7.],
+                       [8., 9., 10., 11.]],
+                      [[40., 44., 48., 52.],
+                       [56., 60., 64., 68.]]]),
+            np.array([[[2., 3., 4., 5.]],
+                      [[10., 11., 12., 13.]],
+                      [[18., 19., 20., 21.]]]),
+            np.array([[[0.5, 5., 17.5],
+                       [4.5, 21., 53.5]],
+                      [[8.5, 37., 89.5],
+                       [12.5, 53., 125.5]],
+                      [[16.5, 69., 161.5],
+                       [20.5, 85., 197.5]]]))
+
+        for axis, y_expected in zip([0, 1, 2], ys_expected):
+            y_int = cumulative_trapezoid(y, x=x[:y.shape[axis]], axis=axis,
+                                         initial=None)
+            assert_allclose(y_int, y_expected)
+
+    def test_x_none(self):
+        y = np.linspace(-2, 2, num=5)
+
+        y_int = cumulative_trapezoid(y)
+        y_expected = [-1.5, -2., -1.5, 0.]
+        assert_allclose(y_int, y_expected)
+
+        y_int = cumulative_trapezoid(y, initial=1.23)
+        y_expected = [1.23, -1.5, -2., -1.5, 0.]
+        assert_allclose(y_int, y_expected)
+
+        y_int = cumulative_trapezoid(y, dx=3)
+        y_expected = [-4.5, -6., -4.5, 0.]
+        assert_allclose(y_int, y_expected)
+
+        y_int = cumulative_trapezoid(y, dx=3, initial=1.23)
+        y_expected = [1.23, -4.5, -6., -4.5, 0.]
+        assert_allclose(y_int, y_expected)
+
+    def test_cumtrapz(self):
+        # Basic coverage test for the alias
+        x = np.arange(3 * 2 * 4).reshape(3, 2, 4)
+        y = x
+        assert_allclose(cumulative_trapezoid(y, x, dx=0.5, axis=0, initial=0),
+                        cumtrapz(y, x, dx=0.5, axis=0, initial=0),
+                        rtol=1e-14)
+
+
+class TestTrapezoid():
+    """This function is tested in NumPy more extensive, just do some
+    basic due diligence here."""
+    def test_trapezoid(self):
+        y = np.arange(17)
+        assert_equal(trapezoid(y), 128)
+        assert_equal(trapezoid(y, dx=0.5), 64)
+        assert_equal(trapezoid(y, x=np.linspace(0, 4, 17)), 32)
+
+        y = np.arange(4)
+        x = 2**y
+        assert_equal(trapezoid(y, x=x, dx=0.1), 13.5)
+
+    def test_trapz(self):
+        # Basic coverage test for the alias
+        y = np.arange(4)
+        x = 2**y
+        assert_equal(trapezoid(y, x=x, dx=0.5, axis=0),
+                     trapz(y, x=x, dx=0.5, axis=0))
+
+
+class TestQMCQuad():
+    def test_input_validation(self):
+        message = "`func` must be callable."
+        with pytest.raises(TypeError, match=message):
+            qmc_quad("a duck", [0, 0], [1, 1])
+
+        message = "`func` must evaluate the integrand at points..."
+        with pytest.raises(ValueError, match=message):
+            qmc_quad(lambda: 1, [0, 0], [1, 1])
+
+        def func(x):
+            assert x.ndim == 1
+            return np.sum(x)
+        message = "Exception encountered when attempting vectorized call..."
+        with pytest.warns(UserWarning, match=message):
+            qmc_quad(func, [0, 0], [1, 1])
+
+        message = "`n_points` must be an integer."
+        with pytest.raises(TypeError, match=message):
+            qmc_quad(lambda x: 1, [0, 0], [1, 1], n_points=1024.5)
+
+        message = "`n_estimates` must be an integer."
+        with pytest.raises(TypeError, match=message):
+            qmc_quad(lambda x: 1, [0, 0], [1, 1], n_estimates=8.5)
+
+        message = "`qrng` must be an instance of scipy.stats.qmc.QMCEngine."
+        with pytest.raises(TypeError, match=message):
+            qmc_quad(lambda x: 1, [0, 0], [1, 1], qrng="a duck")
+
+        message = "`qrng` must be initialized with dimensionality equal to "
+        with pytest.raises(ValueError, match=message):
+            qmc_quad(lambda x: 1, [0, 0], [1, 1], qrng=stats.qmc.Sobol(1))
+
+        message = r"`log` must be boolean \(`True` or `False`\)."
+        with pytest.raises(TypeError, match=message):
+            qmc_quad(lambda x: 1, [0, 0], [1, 1], log=10)
+
+    def basic_test(self, n_points=2**8, n_estimates=8, signs=np.ones(2)):
+
+        ndim = 2
+        mean = np.zeros(ndim)
+        cov = np.eye(ndim)
+
+        def func(x):
+            return stats.multivariate_normal.pdf(x, mean, cov)
+
+        rng = np.random.default_rng(2879434385674690281)
+        qrng = stats.qmc.Sobol(ndim, seed=rng)
+        a = np.zeros(ndim)
+        b = np.ones(ndim) * signs
+        res = qmc_quad(func, a, b, n_points=n_points,
+                       n_estimates=n_estimates, args=(mean, cov), qrng=qrng)
+        ref = stats.multivariate_normal.cdf(b, mean, cov, lower_limit=a)
+        atol = sc.stdtrit(n_estimates-1, 0.995) * res.standard_error  # 99% CI
+        assert_allclose(res.integral, ref, atol=atol)
+        assert np.prod(signs)*res.integral > 0
+
+        rng = np.random.default_rng(2879434385674690281)
+        qrng = stats.qmc.Sobol(ndim, seed=rng)
+        logres = qmc_quad(lambda *args: np.log(func(*args)), a, b,
+                          n_points=n_points, n_estimates=n_estimates,
+                          args=(mean, cov), log=True, qrng=qrng)
+        assert_allclose(np.exp(logres.integral), res.integral)
+        assert np.imag(logres.integral) == (np.pi if np.prod(signs) < 0 else 0)
+
+    @pytest.mark.parametrize("n_points", [2**8, 2**12])
+    @pytest.mark.parametrize("n_estimates", [8, 16])
+    def test_basic(self, n_points, n_estimates):
+        self.basic_test(n_points, n_estimates)
+
+    @pytest.mark.parametrize("signs", [[1, 1], [-1, -1], [-1, 1], [1, -1]])
+    def test_sign(self, signs):
+        self.basic_test(signs=signs)
+
+    @pytest.mark.parametrize("log", [False, True])
+    def test_zero(self, log):
+        message = "A lower limit was equal to an upper limit, so"
+        with pytest.warns(UserWarning, match=message):
+            res = qmc_quad(lambda x: 1, [0, 0], [0, 1], log=log)
+        assert res.integral == (-np.inf if log else 0)
+        assert res.standard_error == 0
+
+    def test_flexible_input(self):
+        # check that qrng is not required
+        # also checks that for 1d problems, a and b can be scalars
+        def func(x):
+            return stats.norm.pdf(x, scale=2)
+
+        res = qmc_quad(func, 0, 1)
+        ref = stats.norm.cdf(1, scale=2) - stats.norm.cdf(0, scale=2)
+        assert_allclose(res.integral, ref, 1e-2)

.CondaPkg/env/lib/python3.11/site-packages/scipy/integrate/vode.py

@@ -0,0 +1,28 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+
+
+import warnings
+from . import _vode  # type: ignore
+
+
+__all__ = [  # noqa: F822
+    'dvode',
+    'zvode'
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    if name not in __all__:
+        raise AttributeError(
+            "scipy.integrate.vode is deprecated and has no attribute "
+            f"{name}.")
+
+    warnings.warn("The `scipy.integrate.vode` namespace is deprecated "
+                  "and will be removed in SciPy v2.0.0.",
+                  category=DeprecationWarning, stacklevel=2)
+
+    return getattr(_vode, name)