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gates_numpy.py
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gates_numpy.py
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import numpy as np
import qiskit
from qiskit.extensions.unitary import UnitaryGate
from qiskit.circuit.library.standard_gates import RZZGate
def cphase_gate(theta):
return np.matrix([
[
1,
0,
0,
0
],
[
0,
1,
0,
0
],
[
0,
0,
1,
0
],
[
0,
0,
0,
np.cos(theta) + 1j*np.sin(theta)
]])
def cnot_gate():
return np.matrix([
[
1,
0,
0,
0
],
[
0,
1,
0,
0
],
[
0,
0,
0,
1
],
[
0,
0,
1,
0
]])
def fsim_gate(theta, phi):
return np.matrix([
[
1,
0,
0,
0
],
[
0,
np.cos(theta),
-1j * np.sin(theta),
0
],
[
0,
-1j * np.sin(theta),
np.cos(theta),
0
],
[
0,
0,
0,
np.cos(phi) - 1j*np.sin(phi)
]])
def xy_gate(theta):
return np.matrix([
[
1,
0,
0,
0
],
[
0,
np.cos(theta/2),
1j * np.sin(theta/2),
0
],
[
0,
1j * np.sin(theta/2),
np.cos(theta/2),
0
],
[
0,
0,
0,
1
]
])
def cz_gate():
return np.matrix([[1, 0, 0, 0],
[0, 1, 0, 0],
[0, 0, 1, 0],
[0, 0, 0, -1]])
def rzz_unitary(theta):
return np.array([[np.exp(-1j*theta/2), 0, 0, 0],
[0, np.exp(1j*theta/2), 0, 0],
[0, 0, np.exp(1j*theta/2), 0],
[0, 0, 0, np.exp(-1j*theta/2)]], dtype=complex)
def get_gate_unitary_qiskit(gate_op):
# Let's assume all the default unitary matrices in qiskit, which has different endianness from our
# convention, so we will need to reverse the qubit order when we apply our decomposition pass.
# if isinstance(gate_op, qiskit.circuit.library.standard_gates.x.CXGate):
# return cnot_gate()
# elif isinstance(gate_op, qiskit.circuit.library.standard_gates.z.CZGate):
# return cz_gate()
if isinstance(gate_op, UnitaryGate):
return gate_op.to_matrix()
elif isinstance(gate_op, RZZGate):
return rzz_unitary(gate_op.params[0])
else:
return gate_op.to_matrix()