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_slater_determinants.py
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_slater_determinants.py
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# Licensed under the Apache License, Version 2.0 (the "License");
# you may not use this file except in compliance with the License.
# You may obtain a copy of the License at
#
# http://www.apache.org/licenses/LICENSE-2.0
#
# Unless required by applicable law or agreed to in writing, software
# distributed under the License is distributed on an "AS IS" BASIS,
# WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied.
# See the License for the specific language governing permissions and
# limitations under the License.
"""This module contains functions for compiling circuits to prepare
Slater determinants and fermionic Gaussian states."""
from __future__ import absolute_import
import numpy
from openfermion.config import EQ_TOLERANCE
from openfermion.ops import QuadraticHamiltonian
from openfermion.ops._quadratic_hamiltonian import swap_columns
def gaussian_state_preparation_circuit(
quadratic_hamiltonian, occupied_orbitals=None):
"""Obtain the description of a circuit which prepares a fermionic Gaussian
state.
Fermionic Gaussian states can be regarded as eigenstates of quadratic
Hamiltonians. If the Hamiltonian conserves particle number, then these are
just Slater determinants. See arXiv:1711.05395 for a detailed description
of how this procedure works.
The circuit description is returned as a sequence of elementary
operations; operations that can be performed in parallel are grouped
together. Each elementary operation is either
- the string 'pht', indicating the operation
.. math::
a_N + a_N^\dagger,
the particle-hole transformation on the last fermionic mode, or
- a tuple :math:`(i, j, \\theta, \\varphi)`, indicating the operation
.. math::
\exp[i \\varphi a_j^\dagger a_j]
\exp[\\theta (a_i^\dagger a_j - a_j^\dagger a_i)],
a Givens rotation of modes :math:`i` and :math:`j` by angles
:math:`\\theta` and :math:`\\varphi`.
Args:
quadratic_hamiltonian(QuadraticHamiltonian):
The Hamiltonian whose eigenstate is desired.
occupied_orbitals(list):
A list of integers representing the indices of the occupied
orbitals in the desired Gaussian state. If this is None
(the default), then it is assumed that the ground state is
desired, i.e., the orbitals with negative energies are filled.
Returns
-------
circuit_description (list[tuple]):
A list of operations describing the circuit. Each operation
is a tuple of objects describing elementary operations that
can be performed in parallel. Each elementary operation
is either the string 'pht', indicating a particle-hole
transformation on the last fermionic mode, or a tuple of
the form :math:`(i, j, \\theta, \\varphi)`,
indicating a Givens rotation
of modes :math:`i` and :math:`j` by angles :math:`\\theta`
and :math:`\\varphi`.
start_orbitals (list):
The occupied orbitals to start with. This describes the
initial state that the circuit should be applied to: it should
be a Slater determinant (in the computational basis) with these
orbitals filled.
"""
if not isinstance(quadratic_hamiltonian, QuadraticHamiltonian):
raise ValueError('Input must be an instance of QuadraticHamiltonian.')
if quadratic_hamiltonian.conserves_particle_number:
# The Hamiltonian conserves particle number, so we don't need
# to use the most general procedure.
hermitian_matrix = quadratic_hamiltonian.combined_hermitian_part
energies, diagonalizing_unitary = numpy.linalg.eigh(hermitian_matrix)
if occupied_orbitals is None:
# The ground state is desired, so we fill the orbitals that have
# negative energy
num_negative_energies = numpy.count_nonzero(
energies < -EQ_TOLERANCE)
occupied_orbitals = range(num_negative_energies)
# Get the unitary rows which represent the Slater determinant
slater_determinant_matrix = diagonalizing_unitary.T[occupied_orbitals]
# Get the circuit description
circuit_description = slater_determinant_preparation_circuit(
slater_determinant_matrix)
start_orbitals = range(len(occupied_orbitals))
else:
# The Hamiltonian does not conserve particle number, so we
# need to use the most general procedure.
diagonalizing_unitary = (
quadratic_hamiltonian.diagonalizing_bogoliubov_transform())
# Get the unitary rows which represent the Gaussian unitary
gaussian_unitary_matrix = diagonalizing_unitary[
quadratic_hamiltonian.n_qubits:]
# Get the circuit description
decomposition, left_decomposition, diagonal, left_diagonal = (
fermionic_gaussian_decomposition(gaussian_unitary_matrix))
if occupied_orbitals is None:
# The ground state is desired, so the circuit should be applied
# to the vaccuum state
start_orbitals = []
circuit_description = list(reversed(decomposition))
else:
start_orbitals = occupied_orbitals
# The circuit won't be applied to the ground state, so we need to
# use left_decomposition
circuit_description = list(reversed(
decomposition + left_decomposition))
return circuit_description, start_orbitals
def slater_determinant_preparation_circuit(slater_determinant_matrix):
"""Obtain the description of a circuit which prepares a Slater determinant.
The input is an :math:`N_f \\times N` matrix :math:`Q` with orthonormal
rows. Such a matrix describes the Slater determinant
.. math::
b^\dagger_1 \cdots b^\dagger_{N_f} \lvert \\text{vac} \\rangle,
where
.. math::
b^\dagger_j = \sum_{k = 1}^N Q_{jk} a^\dagger_k.
The output is the description of a circuit which prepares this
Slater determinant, up to a global phase.
The starting state which the circuit should be applied to
is a Slater determinant (in the computational basis) with
the first :math:`N_f` orbitals filled.
Args:
slater_determinant_matrix: The matrix :math:`Q` which describes the
Slater determinant to be prepared.
Returns:
circuit_description:
A list of operations describing the circuit. Each operation
is a tuple of elementary operations that can be performed in
parallel. Each elementary operation is a tuple of the form
:math:`(i, j, \\theta, \\varphi)`, indicating a Givens rotation
of modes :math:`i` and :math:`j` by angles :math:`\\theta`
and :math:`\\varphi`.
"""
decomposition, left_unitary, diagonal = givens_decomposition(
slater_determinant_matrix)
circuit_description = list(reversed(decomposition))
return circuit_description
def fermionic_gaussian_decomposition(unitary_rows):
"""Decompose a matrix into a sequence of Givens rotations and
particle-hole transformations on the last fermionic mode.
The input is an :math:`N \\times 2N` matrix :math:`W` with orthonormal
rows. Furthermore, :math:`W` must have the block form
.. math::
W = ( W_1 \hspace{4pt} W_2 )
where :math:`W_1` and :math:`W_2` satisfy
.. math::
W_1 W_1^\dagger + W_2 W_2^\dagger &= I
W_1 W_2^T + W_2 W_1^T &= 0.
Then :math:`W` can be decomposed as
.. math::
V W U^\dagger = ( 0 \hspace{6pt} D )
where :math:`V` and :math:`U` are unitary matrices and :math:`D`
is a diagonal unitary matrix. Furthermore, :math:`U` can be decomposed
as follows:
.. math::
U = B G_{k} \cdots B G_3 G_2 B G_1 B,
where each :math:`G_i` is a Givens rotation, and :math:`B` represents
swapping the :math:`N`-th column with the :math:`2N`-th column,
which corresponds to a particle-hole transformation
on the last fermionic mode. This particle-hole transformation maps
:math:`a^\dagger_N` to :math:`a_N` and vice versa, while leaving the
other fermionic ladder operators invariant.
The decomposition of :math:`U` is returned as a list of tuples of objects
describing rotations and particle-hole transformations. The list looks
something like [('pht', ), (G_1, ), ('pht', G_2), ... ].
The objects within a tuple are either the string 'pht', which indicates
a particle-hole transformation on the last fermionic mode, or a tuple
of the form :math:`(i, j, \\theta, \\varphi)`, which indicates a
Givens rotation of rows :math:`i` and :math:`j` by angles
:math:`\\theta` and :math:`\\varphi`.
The matrix :math:`V^T D^*` can also be decomposed as a sequence of
Givens rotations. This decomposition is needed for a circuit that
prepares an excited state.
Args:
unitary_rows(ndarray): A matrix with orthonormal rows and
additional structure described above.
Returns
-------
decomposition (list[tuple]):
The decomposition of :math:`U`.
left_decomposition (list[tuple]):
The decomposition of :math:`V^T D^*`.
diagonal (ndarray):
A list of the nonzero entries of :math:`D`.
left_diagonal (ndarray):
A list of the nonzero entries left from the decomposition
of :math:`V^T D^*`.
"""
current_matrix = numpy.copy(unitary_rows)
n, p = current_matrix.shape
# Check that p = 2 * n
if p != 2 * n:
raise ValueError('The input matrix must have twice as many columns '
'as rows.')
# Check that left and right parts of unitary_rows satisfy the constraints
# necessary for the transformed fermionic operators to satisfy
# the fermionic anticommutation relations
left_part = unitary_rows[:, :n]
right_part = unitary_rows[:, n:]
constraint_matrix_1 = (left_part.dot(left_part.T.conj()) +
right_part.dot(right_part.T.conj()))
constraint_matrix_2 = (left_part.dot(right_part.T) +
right_part.dot(left_part.T))
discrepancy_1 = numpy.amax(abs(constraint_matrix_1 - numpy.eye(n)))
discrepancy_2 = numpy.amax(abs(constraint_matrix_2))
if discrepancy_1 > EQ_TOLERANCE or discrepancy_2 > EQ_TOLERANCE:
raise ValueError('The input matrix does not satisfy the constraints '
'necessary for a proper transformation of the '
'fermionic ladder operators.')
# Compute left_unitary using Givens rotations
left_unitary = numpy.eye(n, dtype=complex)
for k in range(n - 1):
# Zero out entries in column k
for l in range(n - 1 - k):
# Zero out entry in row l if needed
if abs(current_matrix[l, k]) > EQ_TOLERANCE:
givens_rotation = givens_matrix_elements(
current_matrix[l, k], current_matrix[l + 1, k])
# Apply Givens rotation
givens_rotate(current_matrix, givens_rotation, l, l + 1)
givens_rotate(left_unitary, givens_rotation, l, l + 1)
# Initialize list to store decomposition of current_matrix
decomposition = []
# There are 2 * n - 1 iterations (that is the circuit depth)
for k in range(2 * n - 1):
# Initialize the list of parallel operations to perform
# in this iteration
parallel_ops = []
# Perform a particle-hole transformation if necessary
if k % 2 == 0 and abs(current_matrix[k // 2, n - 1]) > EQ_TOLERANCE:
parallel_ops.append('pht')
swap_columns(current_matrix, n - 1, 2 * n - 1)
# Get the (row, column) indices of elements to zero out in parallel.
if k < n:
end_row = k
end_column = n - 1 - k
else:
end_row = n - 1
end_column = k - (n - 1)
column_indices = range(end_column, n - 1, 2)
row_indices = range(end_row, end_row - len(column_indices), -1)
indices_to_zero_out = zip(row_indices, column_indices)
for i, j in indices_to_zero_out:
# Compute the Givens rotation to zero out the (i, j) element,
# if needed
left_element = current_matrix[i, j].conj()
if abs(left_element) > EQ_TOLERANCE:
# We actually need to perform a Givens rotation
right_element = current_matrix[i, j + 1].conj()
givens_rotation = givens_matrix_elements(left_element,
right_element)
# Add the parameters to the list
theta = numpy.arcsin(numpy.real(givens_rotation[1, 0]))
phi = numpy.angle(givens_rotation[1, 1])
parallel_ops.append((j, j + 1, theta, phi))
# Update the matrix
double_givens_rotate(current_matrix, givens_rotation,
j, j + 1, which='col')
# If the current list of parallel operations is not empty,
# append it to the list,
if parallel_ops:
decomposition.append(tuple(parallel_ops))
# Get the diagonal entries
diagonal = current_matrix[range(n), range(n, 2 * n)]
# Compute the decomposition of left_unitary^T * diagonal^*
current_matrix = left_unitary.T
for k in range(n):
current_matrix[:, k] *= diagonal[k].conj()
left_decomposition = []
for k in range(2 * (n - 1) - 1):
# Initialize the list of parallel operations to perform
# in this iteration
parallel_ops = []
# Get the (row, column) indices of elements to zero out in parallel.
if k < n - 1:
start_row = 0
start_column = n - 1 - k
else:
start_row = k - (n - 2)
start_column = k - (n - 3)
column_indices = range(start_column, n, 2)
row_indices = range(start_row, start_row + len(column_indices))
indices_to_zero_out = zip(row_indices, column_indices)
for i, j in indices_to_zero_out:
# Compute the Givens rotation to zero out the (i, j) element,
# if needed
right_element = current_matrix[i, j].conj()
if abs(right_element) > EQ_TOLERANCE:
# We actually need to perform a Givens rotation
left_element = current_matrix[i, j - 1].conj()
givens_rotation = givens_matrix_elements(left_element,
right_element,
which='right')
# Add the parameters to the list
theta = numpy.arcsin(numpy.real(givens_rotation[1, 0]))
phi = numpy.angle(givens_rotation[1, 1])
parallel_ops.append((j - 1, j, theta, phi))
# Update the matrix
givens_rotate(current_matrix, givens_rotation,
j - 1, j, which='col')
# If the current list of parallel operations is not empty,
# append it to the list,
if parallel_ops:
left_decomposition.append(tuple(parallel_ops))
# Get the diagonal entries
left_diagonal = current_matrix[range(n), range(n)]
return decomposition, left_decomposition, diagonal, left_diagonal
def givens_decomposition(unitary_rows):
"""Decompose a matrix into a sequence of Givens rotations.
The input is an :math:`m \\times n` matrix :math:`Q` with :math:`m \leq n`.
The rows of :math:`Q` are orthonormal.
:math:`Q` can be decomposed as follows:
.. math::
V Q U^\dagger = D
where :math:`V` and :math:`U` are unitary matrices, and :math:`D`
is an :math:`m \\times n` matrix with the
first :math:`m` columns forming a diagonal matrix and the rest of the
columns being zero. Furthermore, we can decompose :math:`U` as
.. math::
U = G_k ... G_1
where :math:`G_1, \\ldots, G_k` are complex Givens rotations.
A Givens rotation is a rotation within the two-dimensional subspace
spanned by two coordinate axes. Within the two relevant coordinate
axes, a Givens rotation has the form
.. math::
\\begin{pmatrix}
\\cos(\\theta) & -e^{i \\varphi} \\sin(\\theta) \\\\
\\sin(\\theta) & e^{i \\varphi} \\cos(\\theta)
\\end{pmatrix}.
Args:
unitary_rows: A numpy array or matrix with orthonormal rows,
representing the matrix Q.
Returns
-------
givens_rotations (list[tuple]):
A list of tuples of objects describing Givens
rotations. The list looks like [(G_1, ), (G_2, G_3), ... ].
The Givens rotations within a tuple can be implemented in parallel.
The description of a Givens rotation is itself a tuple of the
form :math:`(i, j, \\theta, \\varphi)`, which represents a
Givens rotation of coordinates
:math:`i` and :math:`j` by angles :math:`\\theta` and
:math:`\\varphi`.
left_unitary (ndarray):
An :math:`m \\times m` numpy array representing the matrix
:math:`V`.
diagonal (ndarray):
A list of the nonzero entries of :math:`D`.
"""
current_matrix = numpy.copy(unitary_rows)
m, n = current_matrix.shape
# Check that m <= n
if m > n:
raise ValueError('The input m x n matrix must have m <= n')
# Compute left_unitary using Givens rotations
left_unitary = numpy.eye(m, dtype=complex)
for k in reversed(range(n - m + 1, n)):
# Zero out entries in column k
for l in range(m - n + k):
# Zero out entry in row l if needed
if abs(current_matrix[l, k]) > EQ_TOLERANCE:
givens_rotation = givens_matrix_elements(
current_matrix[l, k], current_matrix[l + 1, k])
# Apply Givens rotation
givens_rotate(current_matrix, givens_rotation, l, l + 1)
givens_rotate(left_unitary, givens_rotation, l, l + 1)
# Compute the decomposition of current_matrix into Givens rotations
givens_rotations = []
# If m = n (the matrix is square) then we don't need to perform any
# Givens rotations!
if m != n:
# Get the maximum number of simultaneous rotations that
# will be performed
max_simul_rotations = min(m, n - m)
# There are n - 1 iterations (the circuit depth is n - 1)
for k in range(n - 1):
# Get the (row, column) indices of elements to zero out in
# parallel.
if k < max_simul_rotations - 1:
# There are k + 1 elements to zero out
start_row = 0
end_row = k + 1
start_column = n - m - k
end_column = start_column + 2 * (k + 1)
elif k > n - 1 - max_simul_rotations:
# There are n - 1 - k elements to zero out
start_row = m - (n - 1 - k)
end_row = m
start_column = m - (n - 1 - k) + 1
end_column = start_column + 2 * (n - 1 - k)
else:
# There are max_simul_rotations elements to zero out
if max_simul_rotations == m:
start_row = 0
end_row = m
start_column = n - m - k
end_column = start_column + 2 * m
else:
start_row = k + 1 - max_simul_rotations
end_row = k + 1
start_column = k + 1 - max_simul_rotations + 1
end_column = start_column + 2 * max_simul_rotations
row_indices = range(start_row, end_row)
column_indices = range(start_column, end_column, 2)
indices_to_zero_out = zip(row_indices, column_indices)
parallel_rotations = []
for i, j in indices_to_zero_out:
# Compute the Givens rotation to zero out the (i, j) element,
# if needed
right_element = current_matrix[i, j].conj()
if abs(right_element) > EQ_TOLERANCE:
# We actually need to perform a Givens rotation
left_element = current_matrix[i, j - 1].conj()
givens_rotation = givens_matrix_elements(
left_element, right_element, which='right')
# Add the parameters to the list
theta = numpy.arcsin(numpy.real(givens_rotation[1, 0]))
phi = numpy.angle(givens_rotation[1, 1])
parallel_rotations.append((j - 1, j, theta, phi))
# Update the matrix
givens_rotate(current_matrix, givens_rotation,
j - 1, j, which='col')
# If the current list of parallel operations is not empty,
# append it to the list,
if parallel_rotations:
givens_rotations.append(tuple(parallel_rotations))
# Get the diagonal entries
diagonal = current_matrix.diagonal()
return givens_rotations, left_unitary, diagonal
def givens_matrix_elements(a, b, which='left'):
"""Compute the matrix elements of the Givens rotation that zeroes out one
of two row entries.
If `which='left'` then returns a matrix G such that
G * [a b]^T= [0 r]^T
otherwise, returns a matrix G such that
G * [a b]^T= [r 0]^T
where r is a complex number.
Args:
a(complex or float): A complex number representing the upper row entry
b(complex or float): A complex number representing the lower row entry
which(string): Either 'left' or 'right', indicating whether to
zero out the left element (first argument) or right element
(second argument). Default is `left`.
Returns:
G(ndarray): A 2 x 2 numpy array representing the matrix G.
The numbers in the first column of G are real.
"""
# Handle case that a is zero
if abs(a) < EQ_TOLERANCE:
cosine = 1.
sine = 0.
phase = 1.
# Handle case that b is zero and a is nonzero
elif abs(b) < EQ_TOLERANCE:
cosine = 0.
sine = 1.
phase = 1.
# Handle case that a and b are both nonzero
else:
denominator = numpy.sqrt(abs(a) ** 2 + abs(b) ** 2)
cosine = abs(b) / denominator
sine = abs(a) / denominator
sign_b = b / abs(b)
sign_a = a / abs(a)
phase = sign_a * sign_b.conjugate()
# If phase is a real number, convert it to a float
if numpy.isreal(phase):
phase = numpy.real(phase)
# Construct matrix and return
if which == 'left':
# We want to zero out a
if numpy.isreal(a) and numpy.isreal(b):
givens_rotation = numpy.array([[cosine, -phase * sine],
[phase * sine, cosine]])
else:
givens_rotation = numpy.array([[cosine, -phase * sine],
[sine, phase * cosine]])
elif which == 'right':
# We want to zero out b
if numpy.isreal(a) and numpy.isreal(b):
givens_rotation = numpy.array([[sine, phase * cosine],
[-phase * cosine, sine]])
else:
givens_rotation = numpy.array([[sine, phase * cosine],
[cosine, -phase * sine]])
else:
raise ValueError('"which" must be equal to "left" or "right".')
return givens_rotation
def givens_rotate(operator, givens_rotation, i, j, which='row'):
"""Apply a Givens rotation to coordinates i and j of an operator."""
if which == 'row':
# Rotate rows i and j
row_i = operator[i].copy()
row_j = operator[j].copy()
operator[i] = (givens_rotation[0, 0] * row_i +
givens_rotation[0, 1] * row_j)
operator[j] = (givens_rotation[1, 0] * row_i +
givens_rotation[1, 1] * row_j)
elif which == 'col':
# Rotate columns i and j
col_i = operator[:, i].copy()
col_j = operator[:, j].copy()
operator[:, i] = (givens_rotation[0, 0] * col_i +
givens_rotation[0, 1].conj() * col_j)
operator[:, j] = (givens_rotation[1, 0] * col_i +
givens_rotation[1, 1].conj() * col_j)
else:
raise ValueError('"which" must be equal to "row" or "col".')
def double_givens_rotate(operator, givens_rotation, i, j, which='row'):
"""Apply a double Givens rotation.
Applies a Givens rotation to coordinates i and j and the the conjugate
Givens rotation to coordinates n + i and n + j, where
n = dim(operator) / 2. dim(operator) must be even.
"""
m, p = operator.shape
if which == 'row':
if m % 2 != 0:
raise ValueError('To apply a double Givens rotation on rows, '
'the number of rows must be even.')
n = m // 2
# Rotate rows i and j
givens_rotate(operator[:n], givens_rotation, i, j, which='row')
# Rotate rows n + i and n + j
givens_rotate(operator[n:], givens_rotation.conj(), i, j, which='row')
elif which == 'col':
if p % 2 != 0:
raise ValueError('To apply a double Givens rotation on columns, '
'the number of columns must be even.')
n = p // 2
# Rotate columns i and j
givens_rotate(operator[:, :n], givens_rotation, i, j, which='col')
# Rotate cols n + i and n + j
givens_rotate(operator[:, n:], givens_rotation.conj(), i, j,
which='col')
else:
raise ValueError('"which" must be equal to "row" or "col".')