def trotter_step(
self,
qubits: Sequence[cirq.QubitId],
time: float,
control_qubit: Optional[cirq.QubitId] = None) -> cirq.OP_TREE:
n_qubits = len(qubits)
# Simulate the one-body terms for half of the full time
yield (cirq.RotZGate(rads=-0.5 * self.orbital_energies[i] * time).on(
qubits[i]) for i in range(n_qubits))
# Rotate to the computational basis
yield bogoliubov_transform(qubits, self.basis_change_matrix)
# Simulate the two-body terms for the full time
def two_body_interaction(p, q, a, b) -> cirq.OP_TREE:
yield cirq.Rot11Gate(rads=-2 * self.hamiltonian.two_body[p, q] *
time).on(a, b)
yield swap_network(qubits, two_body_interaction)
# The qubit ordering has been reversed
qubits = qubits[::-1]
# Rotate back to the basis in which the one-body term is diagonal
yield cirq.inverse(
bogoliubov_transform(qubits, self.basis_change_matrix))
# Simulate the one-body terms for half of the full time
yield (cirq.RotZGate(rads=-0.5 * self.orbital_energies[i] * time).on(
qubits[i]) for i in range(n_qubits))
def test_z_matrix():
assert np.allclose(
cirq.RotZGate(half_turns=1).matrix(), np.array([[1, 0], [0, -1]]))
assert np.allclose(
cirq.RotZGate(half_turns=0.5).matrix(), np.array([[1, 0], [0, 1j]]))
assert np.allclose(
cirq.RotZGate(half_turns=0).matrix(), np.array([[1, 0], [0, 1]]))
assert np.allclose(
cirq.RotZGate(half_turns=-0.5).matrix(), np.array([[1, 0], [0, -1j]]))
def test_single_qubit_matrix_to_gates_fuzz_half_turns_merge_z_gates(
pre_turns, post_turns):
intended_effect = cirq.dot(
cirq.RotZGate(half_turns=2 * pre_turns).matrix(), cirq.X.matrix(),
cirq.RotZGate(half_turns=2 * post_turns).matrix())
gates = cirq.single_qubit_matrix_to_gates(intended_effect, tolerance=1e-7)
assert len(gates) <= 2
assert_gates_implement_unitary(gates, intended_effect, atol=1e-6)
def test_single_qubit_matrix_to_native_gates_fuzz_half_turns_always_one_gate(
pre_turns, post_turns):
intended_effect = cirq.dot(
cirq.RotZGate(half_turns=2 * pre_turns).matrix(), cirq.X.matrix(),
cirq.RotZGate(half_turns=2 * post_turns).matrix())
gates = decompositions.single_qubit_matrix_to_native_gates(
intended_effect, tolerance=0.0001)
assert len(gates) == 1
assert_gates_implement_unitary(gates, intended_effect)
def operations(self, qubits: Sequence[cirq.QubitId]) -> cirq.OP_TREE:
"""Produce the operations of the ansatz circuit."""
n_qubits = len(qubits)
param_set = set(self.params())
for i in range(self.iterations):
# Change to the basis in which the one-body term is diagonal
yield bogoliubov_transform(
qubits, self.one_body_basis_change_matrix.T.conj())
# Simulate the one-body terms.
for p in range(n_qubits):
u_symbol = LetterWithSubscripts('U', p, i)
if u_symbol in param_set:
yield cirq.RotZGate(half_turns=u_symbol).on(qubits[p])
# Simulate each singular vector of the two-body terms.
prior_basis_matrix = self.one_body_basis_change_matrix
for j in range(len(self.eigenvalues)):
# Get the basis change matrix.
basis_change_matrix = self.basis_change_matrices[j]
# Merge previous basis change matrix with the inverse of the
# current one
merged_basis_change_matrix = numpy.dot(
prior_basis_matrix, basis_change_matrix.T.conj())
yield bogoliubov_transform(qubits, merged_basis_change_matrix)
# Simulate the off-diagonal two-body terms.
def two_body_interaction(p, q, a, b) -> cirq.OP_TREE:
v_symbol = LetterWithSubscripts('V', p, q, j, i)
if v_symbol in param_set:
yield cirq.Rot11Gate(half_turns=v_symbol).on(a, b)
yield swap_network(qubits, two_body_interaction)
qubits = qubits[::-1]
# Simulate the diagonal two-body terms.
for p in range(n_qubits):
u_symbol = LetterWithSubscripts('U', p, j, i)
if u_symbol in param_set:
yield cirq.RotZGate(half_turns=u_symbol).on(qubits[p])
# Update prior basis change matrix.
prior_basis_matrix = basis_change_matrix
# Undo final basis transformation.
yield bogoliubov_transform(qubits, prior_basis_matrix)
def test_ignores_czs_separated_by_parameterized():
a, b = cirq.LineQubit.range(2)
assert_optimizes(
before=cirq.Circuit([
cirq.Moment([cirq.CZ(a, b)]),
cirq.Moment([cirq.RotZGate(half_turns=cirq.Symbol('boo'))(a)]),
cirq.Moment([cirq.CZ(a, b)]),
]),
expected=cirq.Circuit([
cirq.Moment([cirq.CZ(a, b)]),
cirq.Moment([cirq.RotZGate(half_turns=cirq.Symbol('boo'))(a)]),
cirq.Moment([cirq.CZ(a, b)]),
]))
def trotter_step(
self,
qubits: Sequence[cirq.QubitId],
time: float,
control_qubit: Optional[cirq.QubitId] = None) -> cirq.OP_TREE:
n_qubits = len(qubits)
# Change to the basis in which the one-body term is diagonal
yield bogoliubov_transform(qubits,
self.one_body_basis_change_matrix.T.conj())
# Simulate the one-body terms.
for p in range(n_qubits):
yield cirq.RotZGate(rads=-self.one_body_energies[p] * time).on(
qubits[p])
# Simulate each singular vector of the two-body terms.
prior_basis_matrix = self.one_body_basis_change_matrix
for j in range(len(self.eigenvalues)):
# Get the two-body coefficients and basis change matrix.
two_body_coefficients = self.scaled_density_density_matrices[j]
basis_change_matrix = self.basis_change_matrices[j]
# Merge previous basis change matrix with the inverse of the
# current one
merged_basis_change_matrix = numpy.dot(
prior_basis_matrix, basis_change_matrix.T.conj())
yield bogoliubov_transform(qubits, merged_basis_change_matrix)
# Simulate the off-diagonal two-body terms.
yield swap_network(
qubits, lambda p, q, a, b: cirq.Rot11Gate(
rads=-2 * two_body_coefficients[p, q] * time).on(a, b))
qubits = qubits[::-1]
# Simulate the diagonal two-body terms.
for p in range(n_qubits):
yield cirq.RotZGate(rads=-two_body_coefficients[p, p] *
time).on(qubits[p])
# Update prior basis change matrix
prior_basis_matrix = basis_change_matrix
# Undo final basis transformation
yield bogoliubov_transform(qubits, prior_basis_matrix)
def _slater_basis_change(
qubits: Sequence[cirq.QubitId], transformation_matrix: numpy.ndarray,
initially_occupied_orbitals: Optional[Sequence[int]]) -> cirq.OP_TREE:
n_qubits = len(qubits)
if initially_occupied_orbitals is None:
decomposition, diagonal = givens_decomposition_square(
transformation_matrix)
circuit_description = list(reversed(decomposition))
# The initial state is not a computational basis state so the
# phases left on the diagonal in the decomposition matter
yield (cirq.RotZGate(rads=numpy.angle(diagonal[j])).on(qubits[j])
for j in range(n_qubits))
else:
initially_occupied_orbitals = cast(Sequence[int],
initially_occupied_orbitals)
transformation_matrix = transformation_matrix[list(
initially_occupied_orbitals)]
n_occupied = len(initially_occupied_orbitals)
# Flip bits so that the first n_occupied are 1 and the rest 0
initially_occupied_orbitals_set = set(initially_occupied_orbitals)
yield (cirq.X(qubits[j]) for j in range(n_qubits)
if (j < n_occupied) != (j in initially_occupied_orbitals_set))
circuit_description = slater_determinant_preparation_circuit(
transformation_matrix)
yield _ops_from_givens_rotations_circuit_description(
qubits, circuit_description)
def rot_z_layer(h, half_turns):
"""Yields Z rotations by half_turns conditioned on the field h."""
gate = cirq.RotZGate(half_turns=half_turns)
for i, h_row in enumerate(h):
for j, h_ij in enumerate(h_row):
if h_ij == 1:
yield gate(cirq.GridQubit(i, j))
def _gaussian_basis_change(
qubits: Sequence[cirq.QubitId], transformation_matrix: numpy.ndarray,
initially_occupied_orbitals: Optional[Sequence[int]]) -> cirq.OP_TREE:
n_qubits = len(qubits)
# Rearrange the transformation matrix because the OpenFermion routine
# expects it to describe annihilation operators rather than creation
# operators
left_block = transformation_matrix[:, :n_qubits]
right_block = transformation_matrix[:, n_qubits:]
transformation_matrix = numpy.block(
[numpy.conjugate(right_block),
numpy.conjugate(left_block)])
decomposition, left_decomposition, _, left_diagonal = (
fermionic_gaussian_decomposition(transformation_matrix))
if (initially_occupied_orbitals is not None
and len(initially_occupied_orbitals) == 0):
# Starting with the vacuum state yields additional symmetry
circuit_description = list(reversed(decomposition))
else:
if initially_occupied_orbitals is None:
# The initial state is not a computational basis state so the
# phases left on the diagonal in the Givens decomposition matter
yield (cirq.RotZGate(rads=numpy.angle(left_diagonal[j])).on(
qubits[j]) for j in range(n_qubits))
circuit_description = list(reversed(decomposition +
left_decomposition))
yield _ops_from_givens_rotations_circuit_description(
qubits, circuit_description)
def test_arbitrary_xyz_repr():
cirq.testing.assert_equivalent_repr(
cirq.RotXGate(half_turns=0.1, global_shift_in_half_turns=0.2))
cirq.testing.assert_equivalent_repr(
cirq.RotYGate(half_turns=0.1, global_shift_in_half_turns=0.2))
cirq.testing.assert_equivalent_repr(
cirq.RotZGate(half_turns=0.1, global_shift_in_half_turns=0.2))
def test_text_diagrams():
a = cirq.NamedQubit('a')
b = cirq.NamedQubit('b')
circuit = Circuit.from_ops(
cirq.SWAP(a, b),
cirq.X(a),
cirq.Y(a),
cirq.Z(a),
cirq.RotZGate(half_turns=cirq.Symbol('x')).on(a),
cirq.CZ(a, b),
cirq.CNOT(a, b),
cirq.CNOT(b, a),
cirq.H(a),
cirq.ISWAP(a, b),
cirq.ISWAP(a, b)**-1)
assert circuit.to_text_diagram().strip() == """
a: ───×───X───Y───Z───Z^x───@───@───X───H───iSwap───iSwap──────
│ │ │ │ │ │
b: ───×─────────────────────@───X───@───────iSwap───iSwap^-1───
""".strip()
assert circuit.to_text_diagram(use_unicode_characters=False).strip() == """
a: ---swap---X---Y---Z---Z^x---@---@---X---H---iSwap---iSwap------
| | | | | |
b: ---swap---------------------@---X---@-------iSwap---iSwap^-1---
""".strip()
def trotter_step(
self,
qubits: Sequence[cirq.QubitId],
time: float,
control_qubit: Optional[cirq.QubitId] = None) -> cirq.OP_TREE:
n_qubits = len(qubits)
# Apply one- and two-body interactions for the full time
def one_and_two_body_interaction(p, q, a, b) -> cirq.OP_TREE:
yield ControlledXXYYGate(
duration=self.hamiltonian.one_body[p, q].real * time).on(
control_qubit, a, b)
yield ControlledYXXYGate(
duration=self.hamiltonian.one_body[p, q].imag * time).on(
control_qubit, a, b)
yield Rot111Gate(rads=-2 * self.hamiltonian.two_body[p, q] *
time).on(control_qubit, a, b)
yield swap_network(qubits,
one_and_two_body_interaction,
fermionic=True)
qubits = qubits[::-1]
# Apply one-body potential for the full time
yield (cirq.Rot11Gate(rads=-self.hamiltonian.one_body[i, i].real *
time).on(control_qubit, qubits[i])
for i in range(n_qubits))
# Apply phase from constant term
yield cirq.RotZGate(rads=-self.hamiltonian.constant *
time).on(control_qubit)
def test_rot_gates_eq():
eq = cirq.testing.EqualsTester()
gates = [
cirq.RotXGate, cirq.RotYGate, cirq.RotZGate, cirq.CNotGate,
cirq.Rot11Gate
]
for gate in gates:
eq.add_equality_group(gate(half_turns=3.5), gate(half_turns=-0.5),
gate(rads=-np.pi / 2), gate(degs=-90))
eq.make_equality_group(lambda: gate(half_turns=0))
eq.make_equality_group(lambda: gate(half_turns=0.5))
eq.add_equality_group(cirq.RotXGate(), cirq.RotXGate(half_turns=1), cirq.X)
eq.add_equality_group(cirq.RotYGate(), cirq.RotYGate(half_turns=1), cirq.Y)
eq.add_equality_group(cirq.RotZGate(), cirq.RotZGate(half_turns=1), cirq.Z)
eq.add_equality_group(
cirq.RotZGate(half_turns=1, global_shift_in_half_turns=-0.5),
cirq.RotZGate(half_turns=5, global_shift_in_half_turns=-0.5))
eq.add_equality_group(
cirq.RotZGate(half_turns=3, global_shift_in_half_turns=-0.5))
eq.add_equality_group(
cirq.RotZGate(half_turns=1, global_shift_in_half_turns=-0.1))
eq.add_equality_group(
cirq.RotZGate(half_turns=5, global_shift_in_half_turns=-0.1))
eq.add_equality_group(cirq.CNotGate(), cirq.CNotGate(half_turns=1),
cirq.CNOT)
eq.add_equality_group(cirq.Rot11Gate(), cirq.Rot11Gate(half_turns=1),
cirq.CZ)
def operations(self, qubits: Sequence[cirq.QubitId]) -> cirq.OP_TREE:
"""Produce the operations of the ansatz circuit."""
# TODO implement asymmetric ansatzes?
for i in range(self.iterations):
suffix = '-{}'.format(i) if self.iterations > 1 else ''
# Apply one- and two-body interactions with a swap network that
# reverses the order of the modes
def one_and_two_body_interaction(p, q, a, b) -> cirq.OP_TREE:
if 'T{}_{}'.format(p, q) + suffix in self.params:
yield XXYYGate(
half_turns=self.params['T{}_{}'.format(p, q) +
suffix]).on(a, b)
if 'W{}_{}'.format(p, q) + suffix in self.params:
yield YXXYGate(
half_turns=self.params['W{}_{}'.format(p, q) +
suffix]).on(a, b)
if 'V{}_{}'.format(p, q) + suffix in self.params:
yield cirq.Rot11Gate(
half_turns=self.params['V{}_{}'.format(p, q) +
suffix]).on(a, b)
yield swap_network(qubits,
one_and_two_body_interaction,
fermionic=True)
qubits = qubits[::-1]
# Apply one-body potential
yield (cirq.RotZGate(half_turns=self.params['U{}'.format(p) +
suffix]).on(qubits[p])
for p in range(len(qubits))
if 'U{}'.format(p) + suffix in self.params)
# Apply one- and two-body interactions again. This time, reorder
# them so that the entire iteration is symmetric
def one_and_two_body_interaction_reversed_order(p, q, a,
b) -> cirq.OP_TREE:
if 'V{}_{}'.format(p, q) + suffix in self.params:
yield cirq.Rot11Gate(
half_turns=self.params['V{}_{}'.format(p, q) +
suffix]).on(a, b)
if 'W{}_{}'.format(p, q) + suffix in self.params:
yield YXXYGate(
half_turns=self.params['W{}_{}'.format(p, q) +
suffix]).on(a, b)
if 'T{}_{}'.format(p, q) + suffix in self.params:
yield XXYYGate(
half_turns=self.params['T{}_{}'.format(p, q) +
suffix]).on(a, b)
yield swap_network(qubits,
one_and_two_body_interaction_reversed_order,
fermionic=True,
offset=True)
qubits = qubits[::-1]
def test_parameterizable_effect():
q = cirq.NamedQubit('q')
r = cirq.ParamResolver({'a': 0.5})
op1 = cirq.GateOperation(cirq.RotZGate(half_turns=cirq.Symbol('a')), [q])
assert cirq.is_parameterized(op1)
op2 = cirq.resolve_parameters(op1, r)
assert not cirq.is_parameterized(op2)
assert op2 == cirq.S.on(q)
def operations(self, qubits: Sequence[cirq.QubitId]) -> cirq.OP_TREE:
"""Produce the operations of the ansatz circuit."""
# TODO implement asymmetric ansatz
# Change to the basis in which the one-body term is diagonal
yield cirq.inverse(
bogoliubov_transform(qubits, self.basis_change_matrix))
for i in range(self.iterations):
suffix = '-{}'.format(i) if self.iterations > 1 else ''
# Simulate one-body terms
yield (cirq.RotZGate(half_turns=self.params['U{}'.format(p) +
suffix]).on(qubits[p])
for p in range(len(qubits))
if 'U{}'.format(p) + suffix in self.params)
# Rotate to the computational basis
yield bogoliubov_transform(qubits, self.basis_change_matrix)
# Simulate the two-body terms
def two_body_interaction(p, q, a, b) -> cirq.OP_TREE:
if 'V{}_{}'.format(p, q) + suffix in self.params:
yield cirq.Rot11Gate(
half_turns=self.params['V{}_{}'.format(p, q) +
suffix]).on(a, b)
yield swap_network(qubits, two_body_interaction)
qubits = qubits[::-1]
# Rotate back to the basis in which the one-body term is diagonal
yield cirq.inverse(
bogoliubov_transform(qubits, self.basis_change_matrix))
# Simulate one-body terms again
yield (cirq.RotZGate(half_turns=self.params['U{}'.format(p) +
suffix]).on(qubits[p])
for p in range(len(qubits))
if 'U{}'.format(p) + suffix in self.params)
# Rotate to the computational basis
yield bogoliubov_transform(qubits, self.basis_change_matrix)
def operations(self, qubits: Sequence[cirq.QubitId]) -> cirq.OP_TREE:
"""Produce the operations of the ansatz circuit."""
# TODO implement asymmetric ansatz
param_set = set(self.params())
# Change to the basis in which the one-body term is diagonal
yield cirq.inverse(
bogoliubov_transform(qubits, self.basis_change_matrix))
for i in range(self.iterations):
# Simulate one-body terms
for p in range(len(qubits)):
u_symbol = LetterWithSubscripts('U', p, i)
if u_symbol in param_set:
yield cirq.RotZGate(half_turns=u_symbol).on(qubits[p])
# Rotate to the computational basis
yield bogoliubov_transform(qubits, self.basis_change_matrix)
# Simulate the two-body terms
def two_body_interaction(p, q, a, b) -> cirq.OP_TREE:
v_symbol = LetterWithSubscripts('V', p, q, i)
if v_symbol in param_set:
yield cirq.Rot11Gate(half_turns=v_symbol).on(a, b)
yield swap_network(qubits, two_body_interaction)
qubits = qubits[::-1]
# Rotate back to the basis in which the one-body term is diagonal
yield cirq.inverse(
bogoliubov_transform(qubits, self.basis_change_matrix))
# Simulate one-body terms again
for p in range(len(qubits)):
u_symbol = LetterWithSubscripts('U', p, i)
if u_symbol in param_set:
yield cirq.RotZGate(half_turns=u_symbol).on(qubits[p])
# Rotate to the computational basis
yield bogoliubov_transform(qubits, self.basis_change_matrix)
def _rot(self, qubit, params):
"""Helper function that returns an arbitrary rotation of the form
R = Rz(params[2]) * Ry(params[1]) * Rx(params[0])
on the qubit, e.g. R |qubit>.
Note that order is reversed when put into the circuit. The circuit is:
|qubit>---Rx(params[0])---Ry(params[1])---Rz(params[2])---
"""
rx = cirq.RotXGate(half_turns=params[0])
ry = cirq.RotYGate(half_turns=params[1])
rz = cirq.RotZGate(half_turns=params[2])
yield (rx(qubit), ry(qubit), rz(qubit))
def operations(self, qubits: Sequence[cirq.QubitId]) -> cirq.OP_TREE:
"""Produce the operations of the ansatz circuit."""
# TODO implement asymmetric ansatz
param_set = set(self.params())
for i in range(self.iterations):
# Apply one- and two-body interactions with a swap network that
# reverses the order of the modes
def one_and_two_body_interaction(p, q, a, b) -> cirq.OP_TREE:
t_symbol = LetterWithSubscripts('T', p, q, i)
w_symbol = LetterWithSubscripts('W', p, q, i)
v_symbol = LetterWithSubscripts('V', p, q, i)
if t_symbol in param_set:
yield XXYYGate(half_turns=t_symbol).on(a, b)
if w_symbol in param_set:
yield YXXYGate(half_turns=w_symbol).on(a, b)
if v_symbol in param_set:
yield cirq.Rot11Gate(half_turns=v_symbol).on(a, b)
yield swap_network(qubits,
one_and_two_body_interaction,
fermionic=True)
qubits = qubits[::-1]
# Apply one-body potential
for p in range(len(qubits)):
u_symbol = LetterWithSubscripts('U', p, i)
if u_symbol in param_set:
yield cirq.RotZGate(half_turns=u_symbol).on(qubits[p])
# Apply one- and two-body interactions again. This time, reorder
# them so that the entire iteration is symmetric
def one_and_two_body_interaction_reversed_order(p, q, a,
b) -> cirq.OP_TREE:
t_symbol = LetterWithSubscripts('T', p, q, i)
w_symbol = LetterWithSubscripts('W', p, q, i)
v_symbol = LetterWithSubscripts('V', p, q, i)
if v_symbol in param_set:
yield cirq.Rot11Gate(half_turns=v_symbol).on(a, b)
if w_symbol in param_set:
yield YXXYGate(half_turns=w_symbol).on(a, b)
if t_symbol in param_set:
yield XXYYGate(half_turns=t_symbol).on(a, b)
yield swap_network(qubits,
one_and_two_body_interaction_reversed_order,
fermionic=True,
offset=True)
qubits = qubits[::-1]
def trotter_step(
self,
qubits: Sequence[cirq.QubitId],
time: float,
control_qubit: Optional[cirq.QubitId] = None) -> cirq.OP_TREE:
n_qubits = len(qubits)
# Apply one- and two-body interactions for half of the full time
def one_and_two_body_interaction(p, q, a, b) -> cirq.OP_TREE:
yield XXYYGate(duration=0.5 *
self.hamiltonian.one_body[p, q].real * time).on(
a, b)
yield YXXYGate(duration=0.5 *
self.hamiltonian.one_body[p, q].imag * time).on(
a, b)
yield cirq.Rot11Gate(rads=-self.hamiltonian.two_body[p, q] *
time).on(a, b)
yield swap_network(qubits,
one_and_two_body_interaction,
fermionic=True)
qubits = qubits[::-1]
# Apply one-body potential for the full time
yield (cirq.RotZGate(rads=-self.hamiltonian.one_body[i, i].real *
time).on(qubits[i]) for i in range(n_qubits))
# Apply one- and two-body interactions for half of the full time
# This time, reorder the operations so that the entire Trotter step is
# symmetric
def one_and_two_body_interaction_reverse_order(p, q, a,
b) -> cirq.OP_TREE:
yield cirq.Rot11Gate(rads=-self.hamiltonian.two_body[p, q] *
time).on(a, b)
yield YXXYGate(duration=0.5 *
self.hamiltonian.one_body[p, q].imag * time).on(
a, b)
yield XXYYGate(duration=0.5 *
self.hamiltonian.one_body[p, q].real * time).on(
a, b)
yield swap_network(qubits,
one_and_two_body_interaction_reverse_order,
fermionic=True,
offset=True)
def test_parameterizable_effect():
q = cirq.NamedQubit('q')
r = cirq.ParamResolver({'a': 0.5})
# If the gate isn't parameterizable, you get a type error.
op0 = cirq.GateOperation(cirq.Gate(), [q])
assert not cirq.can_cast(cirq.ParameterizableEffect, op0)
with pytest.raises(TypeError):
_ = op0.is_parameterized()
with pytest.raises(TypeError):
_ = op0.with_parameters_resolved_by(r)
op1 = cirq.GateOperation(cirq.RotZGate(half_turns=cirq.Symbol('a')), [q])
assert cirq.can_cast(cirq.ParameterizableEffect, op1)
assert op1.is_parameterized()
op2 = op1.with_parameters_resolved_by(r)
assert not op2.is_parameterized()
assert op2 == cirq.S.on(q)
def rot_z_layer(h, half_turns):
"""Yields Z rotations by half_turns conditioned on the field h."""
for (i, j), h_ij in np.ndenumerate(h):
yield cirq.RotZGate(half_turns=(h_ij * half_turns))(cirq.GridQubit(
i, j))
def trotter_step(
self,
qubits: Sequence[cirq.QubitId],
time: float,
control_qubit: Optional[cirq.QubitId]=None
) -> cirq.OP_TREE:
n_qubits = len(qubits)
# Simulate the off-diagonal one-body terms.
yield swap_network(
qubits,
lambda p, q, a, b: ControlledXXYYGate(duration=
self.one_body_coefficients[p, q].real * time).on(
control_qubit, a, b),
fermionic=True)
qubits = qubits[::-1]
# Simulate the diagonal one-body terms.
yield (cirq.Rot11Gate(rads=
-self.one_body_coefficients[j, j].real * time).on(
control_qubit, qubits[j])
for j in range(n_qubits))
# Simulate each singular vector of the two-body terms.
prior_basis_matrix = numpy.identity(n_qubits, complex)
for j in range(len(self.eigenvalues)):
# Get the basis change matrix and its inverse.
two_body_coefficients = self.scaled_density_density_matrices[j]
basis_change_matrix = self.basis_change_matrices[j]
# If the basis change matrix is unitary, merge rotations.
# Otherwise, you must simulate two basis rotations.
is_unitary = cirq.is_unitary(basis_change_matrix)
if is_unitary:
inverse_basis_matrix = numpy.conjugate(
numpy.transpose(basis_change_matrix))
merged_basis_matrix = numpy.dot(prior_basis_matrix,
inverse_basis_matrix)
yield bogoliubov_transform(qubits, merged_basis_matrix)
else:
# TODO add LiH test to cover this.
# coverage: ignore
if j:
yield bogoliubov_transform(qubits, prior_basis_matrix)
yield cirq.inverse(
bogoliubov_transform(qubits, basis_change_matrix))
# Simulate the off-diagonal two-body terms.
yield swap_network(
qubits,
lambda p, q, a, b: Rot111Gate(rads=
-2 * two_body_coefficients[p, q] * time).on(
control_qubit, a, b))
qubits = qubits[::-1]
# Simulate the diagonal two-body terms.
yield (cirq.Rot11Gate(rads=
-two_body_coefficients[k, k] * time).on(
control_qubit, qubits[k])
for k in range(n_qubits))
# Undo basis transformation non-unitary case.
# Else, set basis change matrix to prior matrix for merging.
if is_unitary:
prior_basis_matrix = basis_change_matrix
else:
# TODO add LiH test to cover this.
# coverage: ignore
yield bogoliubov_transform(qubits, basis_change_matrix)
prior_basis_matrix = numpy.identity(n_qubits, complex)
# Undo final basis transformation in unitary case.
if is_unitary:
yield bogoliubov_transform(qubits, prior_basis_matrix)
# Apply phase from constant term
yield cirq.RotZGate(rads=-self.constant * time).on(control_qubit)
def test_z_init():
z = cirq.RotZGate(half_turns=5)
assert z.half_turns == 1
def test_z_extrapolate():
assert cirq.RotZGate(half_turns=1)**0.5 == cirq.RotZGate(half_turns=0.5)
assert cirq.Z**-0.25 == cirq.RotZGate(half_turns=1.75)
assert cirq.RotZGate(half_turns=0.5).phase_by(
0.25, 0) == cirq.RotZGate(half_turns=0.5)