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3RNN/Lib/site-packages/scipy/linalg/_matfuncs.py

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2024-05-26 19:49:15 +02:00
#
# Author: Travis Oliphant, March 2002
#
from itertools import product
import numpy as np
from numpy import (dot, diag, prod, logical_not, ravel, transpose,
conjugate, absolute, amax, sign, isfinite, triu)
# Local imports
from scipy.linalg import LinAlgError, bandwidth
from ._misc import norm
from ._basic import solve, inv
from ._decomp_svd import svd
from ._decomp_schur import schur, rsf2csf
from ._expm_frechet import expm_frechet, expm_cond
from ._matfuncs_sqrtm import sqrtm
from ._matfuncs_expm import pick_pade_structure, pade_UV_calc
# deprecated imports to be removed in SciPy 1.13.0
from numpy import single # noqa: F401
__all__ = ['expm', 'cosm', 'sinm', 'tanm', 'coshm', 'sinhm', 'tanhm', 'logm',
'funm', 'signm', 'sqrtm', 'fractional_matrix_power', 'expm_frechet',
'expm_cond', 'khatri_rao']
eps = np.finfo('d').eps
feps = np.finfo('f').eps
_array_precision = {'i': 1, 'l': 1, 'f': 0, 'd': 1, 'F': 0, 'D': 1}
###############################################################################
# Utility functions.
def _asarray_square(A):
"""
Wraps asarray with the extra requirement that the input be a square matrix.
The motivation is that the matfuncs module has real functions that have
been lifted to square matrix functions.
Parameters
----------
A : array_like
A square matrix.
Returns
-------
out : ndarray
An ndarray copy or view or other representation of A.
"""
A = np.asarray(A)
if len(A.shape) != 2 or A.shape[0] != A.shape[1]:
raise ValueError('expected square array_like input')
return A
def _maybe_real(A, B, tol=None):
"""
Return either B or the real part of B, depending on properties of A and B.
The motivation is that B has been computed as a complicated function of A,
and B may be perturbed by negligible imaginary components.
If A is real and B is complex with small imaginary components,
then return a real copy of B. The assumption in that case would be that
the imaginary components of B are numerical artifacts.
Parameters
----------
A : ndarray
Input array whose type is to be checked as real vs. complex.
B : ndarray
Array to be returned, possibly without its imaginary part.
tol : float
Absolute tolerance.
Returns
-------
out : real or complex array
Either the input array B or only the real part of the input array B.
"""
# Note that booleans and integers compare as real.
if np.isrealobj(A) and np.iscomplexobj(B):
if tol is None:
tol = {0: feps*1e3, 1: eps*1e6}[_array_precision[B.dtype.char]]
if np.allclose(B.imag, 0.0, atol=tol):
B = B.real
return B
###############################################################################
# Matrix functions.
def fractional_matrix_power(A, t):
"""
Compute the fractional power of a matrix.
Proceeds according to the discussion in section (6) of [1]_.
Parameters
----------
A : (N, N) array_like
Matrix whose fractional power to evaluate.
t : float
Fractional power.
Returns
-------
X : (N, N) array_like
The fractional power of the matrix.
References
----------
.. [1] Nicholas J. Higham and Lijing lin (2011)
"A Schur-Pade Algorithm for Fractional Powers of a Matrix."
SIAM Journal on Matrix Analysis and Applications,
32 (3). pp. 1056-1078. ISSN 0895-4798
Examples
--------
>>> import numpy as np
>>> from scipy.linalg import fractional_matrix_power
>>> a = np.array([[1.0, 3.0], [1.0, 4.0]])
>>> b = fractional_matrix_power(a, 0.5)
>>> b
array([[ 0.75592895, 1.13389342],
[ 0.37796447, 1.88982237]])
>>> np.dot(b, b) # Verify square root
array([[ 1., 3.],
[ 1., 4.]])
"""
# This fixes some issue with imports;
# this function calls onenormest which is in scipy.sparse.
A = _asarray_square(A)
import scipy.linalg._matfuncs_inv_ssq
return scipy.linalg._matfuncs_inv_ssq._fractional_matrix_power(A, t)
def logm(A, disp=True):
"""
Compute matrix logarithm.
The matrix logarithm is the inverse of
expm: expm(logm(`A`)) == `A`
Parameters
----------
A : (N, N) array_like
Matrix whose logarithm to evaluate
disp : bool, optional
Print warning if error in the result is estimated large
instead of returning estimated error. (Default: True)
Returns
-------
logm : (N, N) ndarray
Matrix logarithm of `A`
errest : float
(if disp == False)
1-norm of the estimated error, ||err||_1 / ||A||_1
References
----------
.. [1] Awad H. Al-Mohy and Nicholas J. Higham (2012)
"Improved Inverse Scaling and Squaring Algorithms
for the Matrix Logarithm."
SIAM Journal on Scientific Computing, 34 (4). C152-C169.
ISSN 1095-7197
.. [2] Nicholas J. Higham (2008)
"Functions of Matrices: Theory and Computation"
ISBN 978-0-898716-46-7
.. [3] Nicholas J. Higham and Lijing lin (2011)
"A Schur-Pade Algorithm for Fractional Powers of a Matrix."
SIAM Journal on Matrix Analysis and Applications,
32 (3). pp. 1056-1078. ISSN 0895-4798
Examples
--------
>>> import numpy as np
>>> from scipy.linalg import logm, expm
>>> a = np.array([[1.0, 3.0], [1.0, 4.0]])
>>> b = logm(a)
>>> b
array([[-1.02571087, 2.05142174],
[ 0.68380725, 1.02571087]])
>>> expm(b) # Verify expm(logm(a)) returns a
array([[ 1., 3.],
[ 1., 4.]])
"""
A = _asarray_square(A)
# Avoid circular import ... this is OK, right?
import scipy.linalg._matfuncs_inv_ssq
F = scipy.linalg._matfuncs_inv_ssq._logm(A)
F = _maybe_real(A, F)
errtol = 1000*eps
# TODO use a better error approximation
errest = norm(expm(F)-A, 1) / norm(A, 1)
if disp:
if not isfinite(errest) or errest >= errtol:
print("logm result may be inaccurate, approximate err =", errest)
return F
else:
return F, errest
def expm(A):
"""Compute the matrix exponential of an array.
Parameters
----------
A : ndarray
Input with last two dimensions are square ``(..., n, n)``.
Returns
-------
eA : ndarray
The resulting matrix exponential with the same shape of ``A``
Notes
-----
Implements the algorithm given in [1], which is essentially a Pade
approximation with a variable order that is decided based on the array
data.
For input with size ``n``, the memory usage is in the worst case in the
order of ``8*(n**2)``. If the input data is not of single and double
precision of real and complex dtypes, it is copied to a new array.
For cases ``n >= 400``, the exact 1-norm computation cost, breaks even with
1-norm estimation and from that point on the estimation scheme given in
[2] is used to decide on the approximation order.
References
----------
.. [1] Awad H. Al-Mohy and Nicholas J. Higham, (2009), "A New Scaling
and Squaring Algorithm for the Matrix Exponential", SIAM J. Matrix
Anal. Appl. 31(3):970-989, :doi:`10.1137/09074721X`
.. [2] Nicholas J. Higham and Francoise Tisseur (2000), "A Block Algorithm
for Matrix 1-Norm Estimation, with an Application to 1-Norm
Pseudospectra." SIAM J. Matrix Anal. Appl. 21(4):1185-1201,
:doi:`10.1137/S0895479899356080`
Examples
--------
>>> import numpy as np
>>> from scipy.linalg import expm, sinm, cosm
Matrix version of the formula exp(0) = 1:
>>> expm(np.zeros((3, 2, 2)))
array([[[1., 0.],
[0., 1.]],
<BLANKLINE>
[[1., 0.],
[0., 1.]],
<BLANKLINE>
[[1., 0.],
[0., 1.]]])
Euler's identity (exp(i*theta) = cos(theta) + i*sin(theta))
applied to a matrix:
>>> a = np.array([[1.0, 2.0], [-1.0, 3.0]])
>>> expm(1j*a)
array([[ 0.42645930+1.89217551j, -2.13721484-0.97811252j],
[ 1.06860742+0.48905626j, -1.71075555+0.91406299j]])
>>> cosm(a) + 1j*sinm(a)
array([[ 0.42645930+1.89217551j, -2.13721484-0.97811252j],
[ 1.06860742+0.48905626j, -1.71075555+0.91406299j]])
"""
a = np.asarray(A)
if a.size == 1 and a.ndim < 2:
return np.array([[np.exp(a.item())]])
if a.ndim < 2:
raise LinAlgError('The input array must be at least two-dimensional')
if a.shape[-1] != a.shape[-2]:
raise LinAlgError('Last 2 dimensions of the array must be square')
n = a.shape[-1]
# Empty array
if min(*a.shape) == 0:
return np.empty_like(a)
# Scalar case
if a.shape[-2:] == (1, 1):
return np.exp(a)
if not np.issubdtype(a.dtype, np.inexact):
a = a.astype(np.float64)
elif a.dtype == np.float16:
a = a.astype(np.float32)
# An explicit formula for 2x2 case exists (formula (2.2) in [1]). However, without
# Kahan's method, numerical instabilities can occur (See gh-19584). Hence removed
# here until we have a more stable implementation.
n = a.shape[-1]
eA = np.empty(a.shape, dtype=a.dtype)
# working memory to hold intermediate arrays
Am = np.empty((5, n, n), dtype=a.dtype)
# Main loop to go through the slices of an ndarray and passing to expm
for ind in product(*[range(x) for x in a.shape[:-2]]):
aw = a[ind]
lu = bandwidth(aw)
if not any(lu): # a is diagonal?
eA[ind] = np.diag(np.exp(np.diag(aw)))
continue
# Generic/triangular case; copy the slice into scratch and send.
# Am will be mutated by pick_pade_structure
Am[0, :, :] = aw
m, s = pick_pade_structure(Am)
if s != 0: # scaling needed
Am[:4] *= [[[2**(-s)]], [[4**(-s)]], [[16**(-s)]], [[64**(-s)]]]
pade_UV_calc(Am, n, m)
eAw = Am[0]
if s != 0: # squaring needed
if (lu[1] == 0) or (lu[0] == 0): # lower/upper triangular
# This branch implements Code Fragment 2.1 of [1]
diag_aw = np.diag(aw)
# einsum returns a writable view
np.einsum('ii->i', eAw)[:] = np.exp(diag_aw * 2**(-s))
# super/sub diagonal
sd = np.diag(aw, k=-1 if lu[1] == 0 else 1)
for i in range(s-1, -1, -1):
eAw = eAw @ eAw
# diagonal
np.einsum('ii->i', eAw)[:] = np.exp(diag_aw * 2.**(-i))
exp_sd = _exp_sinch(diag_aw * (2.**(-i))) * (sd * 2**(-i))
if lu[1] == 0: # lower
np.einsum('ii->i', eAw[1:, :-1])[:] = exp_sd
else: # upper
np.einsum('ii->i', eAw[:-1, 1:])[:] = exp_sd
else: # generic
for _ in range(s):
eAw = eAw @ eAw
# Zero out the entries from np.empty in case of triangular input
if (lu[0] == 0) or (lu[1] == 0):
eA[ind] = np.triu(eAw) if lu[0] == 0 else np.tril(eAw)
else:
eA[ind] = eAw
return eA
def _exp_sinch(x):
# Higham's formula (10.42), might overflow, see GH-11839
lexp_diff = np.diff(np.exp(x))
l_diff = np.diff(x)
mask_z = l_diff == 0.
lexp_diff[~mask_z] /= l_diff[~mask_z]
lexp_diff[mask_z] = np.exp(x[:-1][mask_z])
return lexp_diff
def cosm(A):
"""
Compute the matrix cosine.
This routine uses expm to compute the matrix exponentials.
Parameters
----------
A : (N, N) array_like
Input array
Returns
-------
cosm : (N, N) ndarray
Matrix cosine of A
Examples
--------
>>> import numpy as np
>>> from scipy.linalg import expm, sinm, cosm
Euler's identity (exp(i*theta) = cos(theta) + i*sin(theta))
applied to a matrix:
>>> a = np.array([[1.0, 2.0], [-1.0, 3.0]])
>>> expm(1j*a)
array([[ 0.42645930+1.89217551j, -2.13721484-0.97811252j],
[ 1.06860742+0.48905626j, -1.71075555+0.91406299j]])
>>> cosm(a) + 1j*sinm(a)
array([[ 0.42645930+1.89217551j, -2.13721484-0.97811252j],
[ 1.06860742+0.48905626j, -1.71075555+0.91406299j]])
"""
A = _asarray_square(A)
if np.iscomplexobj(A):
return 0.5*(expm(1j*A) + expm(-1j*A))
else:
return expm(1j*A).real
def sinm(A):
"""
Compute the matrix sine.
This routine uses expm to compute the matrix exponentials.
Parameters
----------
A : (N, N) array_like
Input array.
Returns
-------
sinm : (N, N) ndarray
Matrix sine of `A`
Examples
--------
>>> import numpy as np
>>> from scipy.linalg import expm, sinm, cosm
Euler's identity (exp(i*theta) = cos(theta) + i*sin(theta))
applied to a matrix:
>>> a = np.array([[1.0, 2.0], [-1.0, 3.0]])
>>> expm(1j*a)
array([[ 0.42645930+1.89217551j, -2.13721484-0.97811252j],
[ 1.06860742+0.48905626j, -1.71075555+0.91406299j]])
>>> cosm(a) + 1j*sinm(a)
array([[ 0.42645930+1.89217551j, -2.13721484-0.97811252j],
[ 1.06860742+0.48905626j, -1.71075555+0.91406299j]])
"""
A = _asarray_square(A)
if np.iscomplexobj(A):
return -0.5j*(expm(1j*A) - expm(-1j*A))
else:
return expm(1j*A).imag
def tanm(A):
"""
Compute the matrix tangent.
This routine uses expm to compute the matrix exponentials.
Parameters
----------
A : (N, N) array_like
Input array.
Returns
-------
tanm : (N, N) ndarray
Matrix tangent of `A`
Examples
--------
>>> import numpy as np
>>> from scipy.linalg import tanm, sinm, cosm
>>> a = np.array([[1.0, 3.0], [1.0, 4.0]])
>>> t = tanm(a)
>>> t
array([[ -2.00876993, -8.41880636],
[ -2.80626879, -10.42757629]])
Verify tanm(a) = sinm(a).dot(inv(cosm(a)))
>>> s = sinm(a)
>>> c = cosm(a)
>>> s.dot(np.linalg.inv(c))
array([[ -2.00876993, -8.41880636],
[ -2.80626879, -10.42757629]])
"""
A = _asarray_square(A)
return _maybe_real(A, solve(cosm(A), sinm(A)))
def coshm(A):
"""
Compute the hyperbolic matrix cosine.
This routine uses expm to compute the matrix exponentials.
Parameters
----------
A : (N, N) array_like
Input array.
Returns
-------
coshm : (N, N) ndarray
Hyperbolic matrix cosine of `A`
Examples
--------
>>> import numpy as np
>>> from scipy.linalg import tanhm, sinhm, coshm
>>> a = np.array([[1.0, 3.0], [1.0, 4.0]])
>>> c = coshm(a)
>>> c
array([[ 11.24592233, 38.76236492],
[ 12.92078831, 50.00828725]])
Verify tanhm(a) = sinhm(a).dot(inv(coshm(a)))
>>> t = tanhm(a)
>>> s = sinhm(a)
>>> t - s.dot(np.linalg.inv(c))
array([[ 2.72004641e-15, 4.55191440e-15],
[ 0.00000000e+00, -5.55111512e-16]])
"""
A = _asarray_square(A)
return _maybe_real(A, 0.5 * (expm(A) + expm(-A)))
def sinhm(A):
"""
Compute the hyperbolic matrix sine.
This routine uses expm to compute the matrix exponentials.
Parameters
----------
A : (N, N) array_like
Input array.
Returns
-------
sinhm : (N, N) ndarray
Hyperbolic matrix sine of `A`
Examples
--------
>>> import numpy as np
>>> from scipy.linalg import tanhm, sinhm, coshm
>>> a = np.array([[1.0, 3.0], [1.0, 4.0]])
>>> s = sinhm(a)
>>> s
array([[ 10.57300653, 39.28826594],
[ 13.09608865, 49.86127247]])
Verify tanhm(a) = sinhm(a).dot(inv(coshm(a)))
>>> t = tanhm(a)
>>> c = coshm(a)
>>> t - s.dot(np.linalg.inv(c))
array([[ 2.72004641e-15, 4.55191440e-15],
[ 0.00000000e+00, -5.55111512e-16]])
"""
A = _asarray_square(A)
return _maybe_real(A, 0.5 * (expm(A) - expm(-A)))
def tanhm(A):
"""
Compute the hyperbolic matrix tangent.
This routine uses expm to compute the matrix exponentials.
Parameters
----------
A : (N, N) array_like
Input array
Returns
-------
tanhm : (N, N) ndarray
Hyperbolic matrix tangent of `A`
Examples
--------
>>> import numpy as np
>>> from scipy.linalg import tanhm, sinhm, coshm
>>> a = np.array([[1.0, 3.0], [1.0, 4.0]])
>>> t = tanhm(a)
>>> t
array([[ 0.3428582 , 0.51987926],
[ 0.17329309, 0.86273746]])
Verify tanhm(a) = sinhm(a).dot(inv(coshm(a)))
>>> s = sinhm(a)
>>> c = coshm(a)
>>> t - s.dot(np.linalg.inv(c))
array([[ 2.72004641e-15, 4.55191440e-15],
[ 0.00000000e+00, -5.55111512e-16]])
"""
A = _asarray_square(A)
return _maybe_real(A, solve(coshm(A), sinhm(A)))
def funm(A, func, disp=True):
"""
Evaluate a matrix function specified by a callable.
Returns the value of matrix-valued function ``f`` at `A`. The
function ``f`` is an extension of the scalar-valued function `func`
to matrices.
Parameters
----------
A : (N, N) array_like
Matrix at which to evaluate the function
func : callable
Callable object that evaluates a scalar function f.
Must be vectorized (eg. using vectorize).
disp : bool, optional
Print warning if error in the result is estimated large
instead of returning estimated error. (Default: True)
Returns
-------
funm : (N, N) ndarray
Value of the matrix function specified by func evaluated at `A`
errest : float
(if disp == False)
1-norm of the estimated error, ||err||_1 / ||A||_1
Notes
-----
This function implements the general algorithm based on Schur decomposition
(Algorithm 9.1.1. in [1]_).
If the input matrix is known to be diagonalizable, then relying on the
eigendecomposition is likely to be faster. For example, if your matrix is
Hermitian, you can do
>>> from scipy.linalg import eigh
>>> def funm_herm(a, func, check_finite=False):
... w, v = eigh(a, check_finite=check_finite)
... ## if you further know that your matrix is positive semidefinite,
... ## you can optionally guard against precision errors by doing
... # w = np.maximum(w, 0)
... w = func(w)
... return (v * w).dot(v.conj().T)
References
----------
.. [1] Gene H. Golub, Charles F. van Loan, Matrix Computations 4th ed.
Examples
--------
>>> import numpy as np
>>> from scipy.linalg import funm
>>> a = np.array([[1.0, 3.0], [1.0, 4.0]])
>>> funm(a, lambda x: x*x)
array([[ 4., 15.],
[ 5., 19.]])
>>> a.dot(a)
array([[ 4., 15.],
[ 5., 19.]])
"""
A = _asarray_square(A)
# Perform Shur decomposition (lapack ?gees)
T, Z = schur(A)
T, Z = rsf2csf(T, Z)
n, n = T.shape
F = diag(func(diag(T))) # apply function to diagonal elements
F = F.astype(T.dtype.char) # e.g., when F is real but T is complex
minden = abs(T[0, 0])
# implement Algorithm 11.1.1 from Golub and Van Loan
# "matrix Computations."
for p in range(1, n):
for i in range(1, n-p+1):
j = i + p
s = T[i-1, j-1] * (F[j-1, j-1] - F[i-1, i-1])
ksl = slice(i, j-1)
val = dot(T[i-1, ksl], F[ksl, j-1]) - dot(F[i-1, ksl], T[ksl, j-1])
s = s + val
den = T[j-1, j-1] - T[i-1, i-1]
if den != 0.0:
s = s / den
F[i-1, j-1] = s
minden = min(minden, abs(den))
F = dot(dot(Z, F), transpose(conjugate(Z)))
F = _maybe_real(A, F)
tol = {0: feps, 1: eps}[_array_precision[F.dtype.char]]
if minden == 0.0:
minden = tol
err = min(1, max(tol, (tol/minden)*norm(triu(T, 1), 1)))
if prod(ravel(logical_not(isfinite(F))), axis=0):
err = np.inf
if disp:
if err > 1000*tol:
print("funm result may be inaccurate, approximate err =", err)
return F
else:
return F, err
def signm(A, disp=True):
"""
Matrix sign function.
Extension of the scalar sign(x) to matrices.
Parameters
----------
A : (N, N) array_like
Matrix at which to evaluate the sign function
disp : bool, optional
Print warning if error in the result is estimated large
instead of returning estimated error. (Default: True)
Returns
-------
signm : (N, N) ndarray
Value of the sign function at `A`
errest : float
(if disp == False)
1-norm of the estimated error, ||err||_1 / ||A||_1
Examples
--------
>>> from scipy.linalg import signm, eigvals
>>> a = [[1,2,3], [1,2,1], [1,1,1]]
>>> eigvals(a)
array([ 4.12488542+0.j, -0.76155718+0.j, 0.63667176+0.j])
>>> eigvals(signm(a))
array([-1.+0.j, 1.+0.j, 1.+0.j])
"""
A = _asarray_square(A)
def rounded_sign(x):
rx = np.real(x)
if rx.dtype.char == 'f':
c = 1e3*feps*amax(x)
else:
c = 1e3*eps*amax(x)
return sign((absolute(rx) > c) * rx)
result, errest = funm(A, rounded_sign, disp=0)
errtol = {0: 1e3*feps, 1: 1e3*eps}[_array_precision[result.dtype.char]]
if errest < errtol:
return result
# Handle signm of defective matrices:
# See "E.D.Denman and J.Leyva-Ramos, Appl.Math.Comp.,
# 8:237-250,1981" for how to improve the following (currently a
# rather naive) iteration process:
# a = result # sometimes iteration converges faster but where??
# Shifting to avoid zero eigenvalues. How to ensure that shifting does
# not change the spectrum too much?
vals = svd(A, compute_uv=False)
max_sv = np.amax(vals)
# min_nonzero_sv = vals[(vals>max_sv*errtol).tolist().count(1)-1]
# c = 0.5/min_nonzero_sv
c = 0.5/max_sv
S0 = A + c*np.identity(A.shape[0])
prev_errest = errest
for i in range(100):
iS0 = inv(S0)
S0 = 0.5*(S0 + iS0)
Pp = 0.5*(dot(S0, S0)+S0)
errest = norm(dot(Pp, Pp)-Pp, 1)
if errest < errtol or prev_errest == errest:
break
prev_errest = errest
if disp:
if not isfinite(errest) or errest >= errtol:
print("signm result may be inaccurate, approximate err =", errest)
return S0
else:
return S0, errest
def khatri_rao(a, b):
r"""
Khatri-rao product
A column-wise Kronecker product of two matrices
Parameters
----------
a : (n, k) array_like
Input array
b : (m, k) array_like
Input array
Returns
-------
c: (n*m, k) ndarray
Khatri-rao product of `a` and `b`.
See Also
--------
kron : Kronecker product
Notes
-----
The mathematical definition of the Khatri-Rao product is:
.. math::
(A_{ij} \bigotimes B_{ij})_{ij}
which is the Kronecker product of every column of A and B, e.g.::
c = np.vstack([np.kron(a[:, k], b[:, k]) for k in range(b.shape[1])]).T
Examples
--------
>>> import numpy as np
>>> from scipy import linalg
>>> a = np.array([[1, 2, 3], [4, 5, 6]])
>>> b = np.array([[3, 4, 5], [6, 7, 8], [2, 3, 9]])
>>> linalg.khatri_rao(a, b)
array([[ 3, 8, 15],
[ 6, 14, 24],
[ 2, 6, 27],
[12, 20, 30],
[24, 35, 48],
[ 8, 15, 54]])
"""
a = np.asarray(a)
b = np.asarray(b)
if not (a.ndim == 2 and b.ndim == 2):
raise ValueError("The both arrays should be 2-dimensional.")
if not a.shape[1] == b.shape[1]:
raise ValueError("The number of columns for both arrays "
"should be equal.")
# c = np.vstack([np.kron(a[:, k], b[:, k]) for k in range(b.shape[1])]).T
c = a[..., :, np.newaxis, :] * b[..., np.newaxis, :, :]
return c.reshape((-1,) + c.shape[2:])
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