def test_random(self):
# Create random DiagonalCoulombHamiltonian.
n_qubits = 8
random.seed(n_qubits)
one_body = numpy.zeros((n_qubits, n_qubits), float)
two_body = numpy.zeros((n_qubits, n_qubits), float)
for p in range(8):
for q in range(p, 8):
one_body[p, q] = random.random()
two_body[p, q] = random.random()
one_body += one_body.T
two_body += two_body.T
diagonal_operator = DiagonalCoulombHamiltonian(
one_body, two_body, random.random())
# Compute the lambda norm using expensive (reliable) method.
qubit_operator = jordan_wigner(diagonal_operator)
del qubit_operator.terms[()]
reliable_norm = qubit_operator.induced_norm()
# Compute the lambda norm using the method under test.
test_norm = lambda_norm(diagonal_operator)
# Third norm.
third_norm = 0.
for term, coefficient in qubit_operator.terms.items():
third_norm += abs(coefficient)
# Test.
self.assertAlmostEqual(third_norm, reliable_norm)
self.assertAlmostEqual(test_norm, reliable_norm)
def random_diagonal_coulomb_hamiltonian(n_qubits, real=False):
"""Generate a random instance of DiagonalCoulombHamiltonian.
Args:
n_qubits: The number of qubits
real: Whether to use only real numbers in the one-body term
"""
one_body = random_hermitian_matrix(n_qubits, real=real)
two_body = random_hermitian_matrix(n_qubits, real=True)
constant = numpy.random.randn()
return DiagonalCoulombHamiltonian(one_body, two_body, constant)
def get_diagonal_coulomb_hamiltonian(fermion_operator, n_qubits=None):
"""Convert a FermionOperator to a DiagonalCoulombHamiltonian."""
if not isinstance(fermion_operator, FermionOperator):
raise TypeError('Input must be a FermionOperator.')
if n_qubits is None:
n_qubits = count_qubits(fermion_operator)
if n_qubits < count_qubits(fermion_operator):
raise ValueError('Invalid number of qubits specified.')
fermion_operator = normal_ordered(fermion_operator)
constant = 0.
one_body = numpy.zeros((n_qubits, n_qubits), complex)
two_body = numpy.zeros((n_qubits, n_qubits), float)
for term, coefficient in fermion_operator.terms.items():
# Ignore this term if the coefficient is zero
if abs(coefficient) < EQ_TOLERANCE:
continue
if len(term) == 0:
constant = coefficient
else:
actions = [operator[1] for operator in term]
if actions == [1, 0]:
p, q = [operator[0] for operator in term]
one_body[p, q] = coefficient
elif actions == [1, 1, 0, 0]:
p, q, r, s = [operator[0] for operator in term]
if p == r and q == s:
if abs(numpy.imag(coefficient)) > EQ_TOLERANCE:
raise ValueError(
'FermionOperator does not map to '
'DiagonalCoulombHamiltonian (not Hermitian).')
coefficient = numpy.real(coefficient)
two_body[p, q] = -.5 * coefficient
two_body[q, p] = -.5 * coefficient
else:
raise ValueError('FermionOperator does not map to '
'DiagonalCoulombHamiltonian '
'(contains terms with indices '
'{}).'.format((p, q, r, s)))
else:
raise ValueError('FermionOperator does not map to '
'DiagonalCoulombHamiltonian (contains terms '
'with action {}.'.format(tuple(actions)))
# Check that the operator is Hermitian
if not is_hermitian(one_body):
raise ValueError(
'FermionOperator does not map to DiagonalCoulombHamiltonian '
'(not Hermitian).')
return DiagonalCoulombHamiltonian(one_body, two_body, constant)
def test_diagonal_coulomb_hamiltonian(self):
n_qubits = 5
one_body = random_hermitian_matrix(n_qubits, real=False)
two_body = random_hermitian_matrix(n_qubits, real=True)
constant = numpy.random.randn()
op = DiagonalCoulombHamiltonian(one_body, two_body, constant)
op1 = get_sparse_operator(op)
op2 = get_sparse_operator(jordan_wigner(get_fermion_operator(op)))
diff = op1 - op2
discrepancy = 0.
if diff.nnz:
discrepancy = max(abs(diff.data))
self.assertAlmostEqual(discrepancy, 0.)
def get_diagonal_coulomb_hamiltonian(fermion_operator,
n_qubits=None,
ignore_incompatible_terms=False):
r"""Convert a FermionOperator to a DiagonalCoulombHamiltonian.
Args:
fermion_operator(FermionOperator): The operator to convert.
n_qubits(int): Optionally specify the total number of qubits in the
system
ignore_incompatible_terms(bool): This flag determines the behavior
of this method when it encounters terms that are not represented
by the DiagonalCoulombHamiltonian class, namely, terms that are
not quadratic and not quartic of the form
a^\dagger_p a_p a^\dagger_q a_q. If set to True, this method will
simply ignore those terms. If False, then this method will raise
an error if it encounters such a term. The default setting is False.
"""
if not isinstance(fermion_operator, FermionOperator):
raise TypeError('Input must be a FermionOperator.')
if n_qubits is None:
n_qubits = count_qubits(fermion_operator)
if n_qubits < count_qubits(fermion_operator):
raise ValueError('Invalid number of qubits specified.')
fermion_operator = normal_ordered(fermion_operator)
constant = 0.
one_body = numpy.zeros((n_qubits, n_qubits), complex)
two_body = numpy.zeros((n_qubits, n_qubits), float)
for term, coefficient in fermion_operator.terms.items():
# Ignore this term if the coefficient is zero
if abs(coefficient) < EQ_TOLERANCE:
continue
if len(term) == 0:
constant = coefficient
else:
actions = [operator[1] for operator in term]
if actions == [1, 0]:
p, q = [operator[0] for operator in term]
one_body[p, q] = coefficient
elif actions == [1, 1, 0, 0]:
p, q, r, s = [operator[0] for operator in term]
if p == r and q == s:
if abs(numpy.imag(coefficient)) > EQ_TOLERANCE:
raise ValueError(
'FermionOperator does not map to '
'DiagonalCoulombHamiltonian (not Hermitian).')
coefficient = numpy.real(coefficient)
two_body[p, q] = -.5 * coefficient
two_body[q, p] = -.5 * coefficient
elif not ignore_incompatible_terms:
raise ValueError('FermionOperator does not map to '
'DiagonalCoulombHamiltonian '
'(contains terms with indices '
'{}).'.format((p, q, r, s)))
elif not ignore_incompatible_terms:
raise ValueError('FermionOperator does not map to '
'DiagonalCoulombHamiltonian (contains terms '
'with action {}.'.format(tuple(actions)))
# Check that the operator is Hermitian
if not is_hermitian(one_body):
raise ValueError(
'FermionOperator does not map to DiagonalCoulombHamiltonian '
'(not Hermitian).')
return DiagonalCoulombHamiltonian(one_body, two_body, constant)
