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z.py
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z.py
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# This code is part of Qiskit.
#
# (C) Copyright IBM 2017.
#
# This code is licensed under the Apache License, Version 2.0. You may
# obtain a copy of this license in the LICENSE.txt file in the root directory
# of this source tree or at http://www.apache.org/licenses/LICENSE-2.0.
#
# Any modifications or derivative works of this code must retain this
# copyright notice, and modified files need to carry a notice indicating
# that they have been altered from the originals.
"""Z, CZ and CCZ gates."""
from math import pi
from typing import Optional, Union
import numpy
from qiskit.circuit._utils import with_gate_array, with_controlled_gate_array
from qiskit.circuit.singleton import SingletonGate, SingletonControlledGate, stdlib_singleton_key
from qiskit.circuit.quantumregister import QuantumRegister
from qiskit._accelerate.circuit import StandardGate
from .p import PhaseGate
_Z_ARRAY = [[1, 0], [0, -1]]
@with_gate_array(_Z_ARRAY)
class ZGate(SingletonGate):
r"""The single-qubit Pauli-Z gate (:math:`\sigma_z`).
Can be applied to a :class:`~qiskit.circuit.QuantumCircuit`
with the :meth:`~qiskit.circuit.QuantumCircuit.z` method.
**Matrix Representation:**
.. math::
Z = \begin{pmatrix}
1 & 0 \\
0 & -1
\end{pmatrix}
**Circuit symbol:**
.. parsed-literal::
┌───┐
q_0: ┤ Z ├
└───┘
Equivalent to a :math:`\pi` radian rotation about the Z axis.
.. note::
A global phase difference exists between the definitions of
:math:`RZ(\pi)` and :math:`Z`.
.. math::
RZ(\pi) = \begin{pmatrix}
-i & 0 \\
0 & i
\end{pmatrix}
= -i Z
The gate is equivalent to a phase flip.
.. math::
|0\rangle \rightarrow |0\rangle \\
|1\rangle \rightarrow -|1\rangle
"""
_standard_gate = StandardGate.ZGate
def __init__(self, label: Optional[str] = None, *, duration=None, unit="dt"):
"""Create new Z gate."""
super().__init__("z", 1, [], label=label, duration=duration, unit=unit)
_singleton_lookup_key = stdlib_singleton_key()
def _define(self):
# pylint: disable=cyclic-import
from qiskit.circuit.quantumcircuit import QuantumCircuit
from .u1 import U1Gate
q = QuantumRegister(1, "q")
qc = QuantumCircuit(q, name=self.name)
rules = [(U1Gate(pi), [q[0]], [])]
for instr, qargs, cargs in rules:
qc._append(instr, qargs, cargs)
self.definition = qc
def control(
self,
num_ctrl_qubits: int = 1,
label: Optional[str] = None,
ctrl_state: Optional[Union[str, int]] = None,
annotated: bool = False,
):
"""Return a (multi-)controlled-Z gate.
One control returns a CZ gate.
Args:
num_ctrl_qubits: number of control qubits.
label: An optional label for the gate [Default: ``None``]
ctrl_state: control state expressed as integer,
string (e.g.``'110'``), or ``None``. If ``None``, use all 1s.
annotated: indicates whether the controlled gate should be implemented
as an annotated gate.
Returns:
ControlledGate: controlled version of this gate.
"""
if not annotated and num_ctrl_qubits == 1:
gate = CZGate(label=label, ctrl_state=ctrl_state, _base_label=self.label)
else:
gate = super().control(
num_ctrl_qubits=num_ctrl_qubits,
label=label,
ctrl_state=ctrl_state,
annotated=annotated,
)
return gate
def inverse(self, annotated: bool = False):
"""Return inverted Z gate (itself).
Args:
annotated: when set to ``True``, this is typically used to return an
:class:`.AnnotatedOperation` with an inverse modifier set instead of a concrete
:class:`.Gate`. However, for this class this argument is ignored as this gate
is self-inverse.
Returns:
ZGate: inverse gate (self-inverse).
"""
return ZGate() # self-inverse
def power(self, exponent: float, annotated: bool = False):
return PhaseGate(numpy.pi * exponent)
def __eq__(self, other):
return isinstance(other, ZGate)
@with_controlled_gate_array(_Z_ARRAY, num_ctrl_qubits=1)
class CZGate(SingletonControlledGate):
r"""Controlled-Z gate.
This is a Clifford and symmetric gate.
Can be applied to a :class:`~qiskit.circuit.QuantumCircuit`
with the :meth:`~qiskit.circuit.QuantumCircuit.cz` method.
**Circuit symbol:**
.. parsed-literal::
q_0: ─■─
│
q_1: ─■─
**Matrix representation:**
.. math::
CZ\ q_0, q_1 =
I \otimes |0\rangle\langle 0| + Z \otimes |1\rangle\langle 1| =
\begin{pmatrix}
1 & 0 & 0 & 0 \\
0 & 1 & 0 & 0 \\
0 & 0 & 1 & 0 \\
0 & 0 & 0 & -1
\end{pmatrix}
In the computational basis, this gate flips the phase of
the target qubit if the control qubit is in the :math:`|1\rangle` state.
"""
_standard_gate = StandardGate.CZGate
def __init__(
self,
label: Optional[str] = None,
ctrl_state: Optional[Union[str, int]] = None,
*,
duration=None,
unit="dt",
_base_label=None,
):
"""Create new CZ gate."""
super().__init__(
"cz",
2,
[],
label=label,
num_ctrl_qubits=1,
ctrl_state=ctrl_state,
base_gate=ZGate(label=_base_label),
duration=duration,
unit=unit,
)
_singleton_lookup_key = stdlib_singleton_key(num_ctrl_qubits=1)
def _define(self):
"""
gate cz a,b { h b; cx a,b; h b; }
"""
# pylint: disable=cyclic-import
from qiskit.circuit.quantumcircuit import QuantumCircuit
from .h import HGate
from .x import CXGate
q = QuantumRegister(2, "q")
qc = QuantumCircuit(q, name=self.name)
rules = [(HGate(), [q[1]], []), (CXGate(), [q[0], q[1]], []), (HGate(), [q[1]], [])]
for instr, qargs, cargs in rules:
qc._append(instr, qargs, cargs)
self.definition = qc
def inverse(self, annotated: bool = False):
"""Return inverted CZ gate (itself).
Args:
annotated: when set to ``True``, this is typically used to return an
:class:`.AnnotatedOperation` with an inverse modifier set instead of a concrete
:class:`.Gate`. However, for this class this argument is ignored as this gate
is self-inverse.
Returns:
CZGate: inverse gate (self-inverse).
"""
return CZGate(ctrl_state=self.ctrl_state) # self-inverse
def __eq__(self, other):
return isinstance(other, CZGate) and self.ctrl_state == other.ctrl_state
@with_controlled_gate_array(_Z_ARRAY, num_ctrl_qubits=2, cached_states=(3,))
class CCZGate(SingletonControlledGate):
r"""CCZ gate.
This is a symmetric gate.
Can be applied to a :class:`~qiskit.circuit.QuantumCircuit`
with the :meth:`~qiskit.circuit.QuantumCircuit.ccz` method.
**Circuit symbol:**
.. parsed-literal::
q_0: ─■─
│
q_1: ─■─
│
q_2: ─■─
**Matrix representation:**
.. math::
CCZ\ q_0, q_1, q_2 =
I \otimes I \otimes |0\rangle\langle 0| + CZ \otimes |1\rangle\langle 1| =
\begin{pmatrix}
1 & 0 & 0 & 0 & 0 & 0 & 0 & 0 \\
0 & 1 & 0 & 0 & 0 & 0 & 0 & 0 \\
0 & 0 & 1 & 0 & 0 & 0 & 0 & 0 \\
0 & 0 & 0 & 1 & 0 & 0 & 0 & 0 \\
0 & 0 & 0 & 0 & 1 & 0 & 0 & 0 \\
0 & 0 & 0 & 0 & 0 & 1 & 0 & 0 \\
0 & 0 & 0 & 0 & 0 & 0 & 1 & 0 \\
0 & 0 & 0 & 0 & 0 & 0 & 0 & -1
\end{pmatrix}
In the computational basis, this gate flips the phase of
the target qubit if the control qubits are in the :math:`|11\rangle` state.
"""
_standard_gate = StandardGate.CCZGate
def __init__(
self,
label: Optional[str] = None,
ctrl_state: Optional[Union[str, int]] = None,
*,
duration=None,
unit="dt",
_base_label=None,
):
"""Create new CCZ gate."""
super().__init__(
"ccz",
3,
[],
label=label,
num_ctrl_qubits=2,
ctrl_state=ctrl_state,
base_gate=ZGate(label=_base_label),
duration=duration,
unit=unit,
)
_singleton_lookup_key = stdlib_singleton_key(num_ctrl_qubits=2)
def _define(self):
"""
gate ccz a,b,c { h c; ccx a,b,c; h c; }
"""
# pylint: disable=cyclic-import
from qiskit.circuit.quantumcircuit import QuantumCircuit
from .h import HGate
from .x import CCXGate
q = QuantumRegister(3, "q")
qc = QuantumCircuit(q, name=self.name)
rules = [(HGate(), [q[2]], []), (CCXGate(), [q[0], q[1], q[2]], []), (HGate(), [q[2]], [])]
for instr, qargs, cargs in rules:
qc._append(instr, qargs, cargs)
self.definition = qc
def inverse(self, annotated: bool = False):
"""Return inverted CCZ gate (itself).
Args:
annotated: when set to ``True``, this is typically used to return an
:class:`.AnnotatedOperation` with an inverse modifier set instead of a concrete
:class:`.Gate`. However, for this class this argument is ignored as this gate
is self-inverse.
Returns:
CCZGate: inverse gate (self-inverse).
"""
return CCZGate(ctrl_state=self.ctrl_state) # self-inverse
def __eq__(self, other):
return isinstance(other, CCZGate) and self.ctrl_state == other.ctrl_state