Source code for thewalrus._montrealer
"""
Montrealer Python interface
* Yanic Cardin and Nicolás Quesada. "Photon-number moments and cumulants of Gaussian states"
`arxiv:12212.06067 (2023) <https://arxiv.org/abs/2212.06067>`_
"""
import numpy as np
import numba
from thewalrus.quantum.conversions import Xmat
from thewalrus.charpoly import powertrace
from ._hafnian import nb_ix
from ._torontonian import tor_input_checks
@numba.jit(nopython=True, cache=True)
def dec2bin(num, n): # pragma: no cover
"""Helper function to convert an integer into an element of the power-set of ``n`` objects.
Args:
num (int): label to convert
n (int): number of elements in the set
Returns:
(array): array containing the labels of the elements to be selected
"""
digits = np.zeros((n), dtype=type(num))
nn = num
counter = -1
while nn >= 1:
digits[counter] = nn % 2
counter -= 1
nn //= 2
return np.nonzero(digits)[0]
@numba.jit(nopython=True)
def montrealer(Sigma): # pragma: no cover
"""Calculates the loop-montrealer of the zero-displacement Gaussian state with the given complex covariance matrix.
Args:
Sigma (array): adjacency matrix of the Gaussian state
Returns:
(np.complex128): the montrealer of ``Sigma``
"""
n = len(Sigma) // 2
tot_num = 2**n
val = np.complex128(0)
for p in numba.prange(tot_num):
pos = dec2bin(p, n)
lenpos = len(pos)
pos = np.concatenate((pos, n + pos))
submat = nb_ix(Sigma, pos, pos)
sign = (-1) ** (lenpos + 1)
val += (sign) * powertrace(submat, n + 1)[-1]
return (-1) ** (n + 1) * val / (2 * n)
@numba.jit(nopython=True)
def power_loop(Sigma, zeta, n): # pragma: no cover
"""Auxiliary function to calculate the product ``np.conj(zeta) @ Sigma^{n-1} @ zeta``.
Args:
Sigma (array): square complex matrix
zeta (array): complex vector
n (int): sought after power
Returns:
(np.complex128 or np.float64): the product np.conj(zeta) @ Sigma^{n-1} @ zeta
"""
vec = zeta
for _ in range(n - 1):
vec = Sigma @ vec
return np.conj(zeta) @ vec
@numba.jit(nopython=True, cache=True)
def lmontrealer(Sigma, zeta): # pragma: no cover
"""Calculates the loop-montrealer of the displaced Gaussian state with the given complex covariance matrix and vector of displacements.
Args:
Sigma (array): complex Glauber covariance matrix of the Gaussian state
zeta (array): vector of displacements
Returns:
(np.complex128): the montrealer of ``Sigma``
"""
n = len(Sigma) // 2
tot_num = 2**n
val = np.complex128(0)
val_loops = np.complex128(0)
for p in numba.prange(tot_num):
pos = dec2bin(p, n)
lenpos = len(pos)
pos = np.concatenate((pos, n + pos))
subvec = zeta[pos]
submat = nb_ix(Sigma, pos, pos)
sign = (-1) ** (lenpos + 1)
val_loops += sign * power_loop(submat, subvec, n)
val += sign * powertrace(submat, n + 1)[-1]
return (-1) ** (n + 1) * (val / (2 * n) + val_loops / 2)
[docs]
def lmtl(A, zeta):
"""Returns the montrealer of an NxN matrix and an N-length vector.
Args:
A (array): an NxN array of even dimensions
zeta (array): an N-length vector of even dimensions
Returns:
np.float64 or np.complex128: the loop montrealer of matrix A, vector zeta
"""
tor_input_checks(A, zeta)
n = len(A) // 2
Sigma = Xmat(n) @ A
return lmontrealer(Sigma, zeta)
[docs]
def mtl(A):
"""Returns the montrealer of an NxN matrix.
Args:
A (array): an NxN array of even dimensions.
Returns:
np.float64 or np.complex128: the montrealer of matrix ``A``
"""
tor_input_checks(A)
n = len(A) // 2
Sigma = Xmat(n) @ A
return montrealer(Sigma)
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