qiskit.circuit.library.standard_gates.rzx のソースコード

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"""Two-qubit ZX-rotation gate."""
import math
from typing import Optional
from qiskit.circuit.gate import Gate
from qiskit.circuit.quantumregister import QuantumRegister
from qiskit.circuit.parameterexpression import ParameterValueType


[ドキュメント]class RZXGate(Gate): r"""A parametric 2-qubit :math:`Z \otimes X` interaction (rotation about ZX). This gate is maximally entangling at :math:`\theta = \pi/2`. The cross-resonance gate (CR) for superconducting qubits implements a ZX interaction (however other terms are also present in an experiment). Can be applied to a :class:`~qiskit.circuit.QuantumCircuit` with the :meth:`~qiskit.circuit.QuantumCircuit.rzx` method. **Circuit Symbol:** .. parsed-literal:: ┌─────────┐ q_0: ┤0 ├ │ Rzx(θ) │ q_1: ┤1 ├ └─────────┘ **Matrix Representation:** .. math:: \newcommand{\th}{\frac{\theta}{2}} R_{ZX}(\theta)\ q_0, q_1 = \exp\left(-i \frac{\theta}{2} X{\otimes}Z\right) = \begin{pmatrix} \cos\left(\th\right) & 0 & -i\sin\left(\th\right) & 0 \\ 0 & \cos\left(\th\right) & 0 & i\sin\left(\th\right) \\ -i\sin\left(\th\right) & 0 & \cos\left(\th\right) & 0 \\ 0 & i\sin\left(\th\right) & 0 & \cos\left(\th\right) \end{pmatrix} .. note:: In Qiskit's convention, higher qubit indices are more significant (little endian convention). In the above example we apply the gate on (q_0, q_1) which results in the :math:`X \otimes Z` tensor order. Instead, if we apply it on (q_1, q_0), the matrix will be :math:`Z \otimes X`: .. parsed-literal:: ┌─────────┐ q_0: ┤1 ├ │ Rzx(θ) │ q_1: ┤0 ├ └─────────┘ .. math:: \newcommand{\th}{\frac{\theta}{2}} R_{ZX}(\theta)\ q_1, q_0 = exp(-i \frac{\theta}{2} Z{\otimes}X) = \begin{pmatrix} \cos(\th) & -i\sin(\th) & 0 & 0 \\ -i\sin(\th) & \cos(\th) & 0 & 0 \\ 0 & 0 & \cos(\th) & i\sin(\th) \\ 0 & 0 & i\sin(\th) & \cos(\th) \end{pmatrix} This is a direct sum of RX rotations, so this gate is equivalent to a uniformly controlled (multiplexed) RX gate: .. math:: R_{ZX}(\theta)\ q_1, q_0 = \begin{pmatrix} RX(\theta) & 0 \\ 0 & RX(-\theta) \end{pmatrix} **Examples:** .. math:: R_{ZX}(\theta = 0) = I .. math:: R_{ZX}(\theta = 2\pi) = -I .. math:: R_{ZX}(\theta = \pi) = -i Z \otimes X .. math:: RZX(\theta = \frac{\pi}{2}) = \frac{1}{\sqrt{2}} \begin{pmatrix} 1 & 0 & -i & 0 \\ 0 & 1 & 0 & i \\ -i & 0 & 1 & 0 \\ 0 & i & 0 & 1 \end{pmatrix} """ def __init__(self, theta: ParameterValueType, label: Optional[str] = None): """Create new RZX gate.""" super().__init__("rzx", 2, [theta], label=label) def _define(self): """ gate rzx(theta) a, b { h b; cx a, b; u1(theta) b; cx a, b; h b;} """ # pylint: disable=cyclic-import from qiskit.circuit.quantumcircuit import QuantumCircuit from .h import HGate from .x import CXGate from .rz import RZGate # q_0: ───────■─────────────■─────── # ┌───┐┌─┴─┐┌───────┐┌─┴─┐┌───┐ # q_1: ┤ H ├┤ X ├┤ Rz(0) ├┤ X ├┤ H ├ # └───┘└───┘└───────┘└───┘└───┘ theta = self.params[0] q = QuantumRegister(2, "q") qc = QuantumCircuit(q, name=self.name) rules = [ (HGate(), [q[1]], []), (CXGate(), [q[0], q[1]], []), (RZGate(theta), [q[1]], []), (CXGate(), [q[0], q[1]], []), (HGate(), [q[1]], []), ] for instr, qargs, cargs in rules: qc._append(instr, qargs, cargs) self.definition = qc
[ドキュメント] def inverse(self): """Return inverse RZX gate (i.e. with the negative rotation angle).""" return RZXGate(-self.params[0])
def __array__(self, dtype=None): """Return a numpy.array for the RZX gate.""" import numpy half_theta = float(self.params[0]) / 2 cos = math.cos(half_theta) isin = 1j * math.sin(half_theta) return numpy.array( [[cos, 0, -isin, 0], [0, cos, 0, isin], [-isin, 0, cos, 0], [0, isin, 0, cos]], dtype=dtype, )
[ドキュメント] def power(self, exponent: float): """Raise gate to a power.""" (theta,) = self.params return RZXGate(exponent * theta)