Python gates.CZ屬性代碼示例

# 需要導入模塊: from pyquil import gates [as 別名]
# 或者: from pyquil.gates import CZ [as 別名]
def test_gates_in_isa(isa_dict):
    isa = ISA.from_dict(isa_dict)
    gates = gates_in_isa(isa)
    for q in [0, 1, 2]:
        for g in [
            I(q),
            RX(np.pi / 2, q),
            RX(-np.pi / 2, q),
            RX(np.pi, q),
            RX(-np.pi, q),
            RZ(THETA, q),
        ]:
            assert g in gates

    assert CZ(0, 1) in gates
    assert CZ(1, 0) in gates
    assert ISWAP(1, 2) in gates
    assert ISWAP(2, 1) in gates
    assert CPHASE(THETA, 2, 0) in gates
    assert CPHASE(THETA, 0, 2) in gates 

# 需要導入模塊: from pyquil import gates [as 別名]
# 或者: from pyquil.gates import CZ [as 別名]
def _random_2q_programs(n_progs=3):
    """Generate random programs that consist of single qubit rotations, a CZ, and single
    qubit rotations.
    """
    r = random.Random(52)

    def RI(qubit, angle):
        # throw away angle so we can randomly choose the identity
        return I(qubit)

    def _random_1q_gate(qubit):
        return r.choice([RI, RX, RY, RZ])(qubit=qubit, angle=r.uniform(0, 2 * pi))

    for _ in range(n_progs):
        prog = Program()
        prog += _random_1q_gate(0)
        prog += _random_1q_gate(1)
        prog += CZ(0, 1)
        prog += _random_1q_gate(0)
        prog += _random_1q_gate(1)
        yield prog 

# 需要導入模塊: from pyquil import gates [as 別名]
# 或者: from pyquil.gates import CZ [as 別名]
def CNOT_X_basis(control, target) -> Program:
    """
    The CNOT in the X basis, i.e.

    ::

        CNOTX = |+X+| * I + |-X-| * Z

    where ``|+>`` and ``|->`` are the +/- eigenstate of the Pauli X operator, and ``*`` denotes a
    tensor product.

    :param control: qubit label
    :param target: qubit label
    :return: program
    """
    prog = Program()
    prog += H(control)
    prog += CZ(control, target)
    prog += H(control)
    return prog 

# 需要導入模塊: from pyquil import gates [as 別名]
# 或者: from pyquil.gates import CZ [as 別名]
def generate_cz_phase_ramsey_experiments(cz_qubits: Sequence[int], measure_qubit: int,
                                         angles: Sequence[float]) -> List[ObservablesExperiment]:
    """
    Return ObservablesExperiments containing programs that constitute a CZ phase ramsey experiment.

    :param cz_qubits: the qubits participating in the cz gate
    :param measure_qubit: Which qubit to measure.
    :param angles: A list of angles at which to make a measurement
    :return: ObservablesExperiments which can be run to estimate the effective RZ rotation
        applied to a single qubit during the application of a CZ gate.
    """
    expts = []
    for angle in angles:
        settings = []
        program = Program()
        # apply CZ, possibly inducing an effective RZ on measure qubit by some angle
        program += CZ(*cz_qubits)
        # apply phase to measure_qubit akin to T2 experiment
        program += RZ(angle, measure_qubit)
        settings = [ExperimentSetting(minusY(measure_qubit), PauliTerm('Y', measure_qubit))]

        expts.append(ObservablesExperiment([settings], program))

    return expts 

# 需要導入模塊: from pyquil import gates [as 別名]
# 或者: from pyquil.gates import CZ [as 別名]
def test_lifted_gate_modified():
    test_unitary = lifted_gate(RZ(np.pi / 4, 0).dagger(), 1)
    true_unitary = mat.RZ(-np.pi / 4)
    assert np.allclose(test_unitary, true_unitary)

    test_unitary = lifted_gate(X(0).dagger().controlled(1), 2)
    true_unitary = lifted_gate(CNOT(1, 0), 2)
    other_true = mat.CNOT
    assert np.allclose(test_unitary, true_unitary)
    assert np.allclose(other_true, true_unitary)

    test_unitary = lifted_gate(X(1).dagger().controlled(0).dagger().dagger(), 2)
    true_unitary = lifted_gate(CNOT(0, 1), 2)
    assert np.allclose(test_unitary, true_unitary)

    test_unitary = lifted_gate(X(0).dagger().controlled(1).dagger().dagger().controlled(2), 3)
    true_unitary = lifted_gate(CCNOT(1, 2, 0), 3)
    other_true = mat.CCNOT
    assert np.allclose(test_unitary, true_unitary)
    assert np.allclose(other_true, true_unitary)

    test_unitary = lifted_gate(RY(np.pi / 4, 0).dagger().controlled(2).dagger().dagger(), 3)
    ry_part = lifted_gate(RY(-np.pi / 4, 0), 1)
    zero = np.eye(2)
    zero[1, 1] = 0
    one = np.eye(2)
    one[0, 0] = 0
    true_unitary = np.kron(zero, np.eye(4)) + np.kron(one, np.kron(np.eye(2), ry_part))
    assert np.allclose(test_unitary, true_unitary)

    test_unitary = lifted_gate(PHASE(0.0, 1).forked(0, [np.pi]), 2)
    true_unitary = lifted_gate(CZ(0, 1), 2)
    assert np.allclose(test_unitary, true_unitary)

    test_unitary = lifted_gate(PHASE(0.0, 2).forked(1, [0.0]).forked(0, [0.0, np.pi]), 3)
    true_unitary = lifted_gate(CZ(1, 2).controlled(0), 3)
    assert np.allclose(test_unitary, true_unitary) 

# 需要導入模塊: from pyquil import gates [as 別名]
# 或者: from pyquil.gates import CZ [as 別名]
def test_noise_helpers():
    gates = RX(np.pi / 2, 0), RX(-np.pi / 2, 1), I(1), CZ(0, 1)
    prog = Program(*gates)
    inferred_gates = _get_program_gates(prog)
    assert set(inferred_gates) == set(gates) 

# 需要導入模塊: from pyquil import gates [as 別名]
# 或者: from pyquil.gates import CZ [as 別名]
def test_apply_noise_model_perturbed_angles():
    eps = 1e-15
    p = Program(RX(np.pi / 2 + eps, 0), RX(np.pi / 2 - eps, 1), CZ(0, 1), RX(np.pi / 2 + eps, 1))
    noise_model = _decoherence_noise_model(_get_program_gates(p))
    pnoisy = apply_noise_model(p, noise_model)
    for i in pnoisy:
        if isinstance(i, DefGate):
            pass
        elif isinstance(i, Pragma):
            assert i.command in ["ADD-KRAUS", "READOUT-POVM"]
        elif isinstance(i, Gate):
            assert i.name in NO_NOISE or not i.params 

# 需要導入模塊: from pyquil import gates [as 別名]
# 或者: from pyquil.gates import CZ [as 別名]
def _CNOT(q1, q2):
    """
    A CNOT in terms of RX(+-pi/2), RZ(theta), and CZ

    .. note:
        This uses two of :py:func:`_H`, so it picks up twice the global phase.
        Don't control this gate.

    """
    p = Program()
    p.inst(_H(q2))
    p.inst(CZ(q1, q2))
    p.inst(_H(q2))
    return p 

# 需要導入模塊: from pyquil import gates [as 別名]
# 或者: from pyquil.gates import CZ [as 別名]
def _CCNOT(q1, q2, q3):
    """
    A CCNOT in terms of RX(+-pi/2), RZ(theta), and CZ

    .. note:
        Don't control this gate.

    """
    p = Program()
    p.inst(_H(q3))
    p.inst(_CNOT(q2, q3))
    p.inst(_T(q3, dagger=True))
    p.inst(_SWAP(q2, q3))
    p.inst(_CNOT(q1, q2))
    p.inst(_T(q2))
    p.inst(_CNOT(q3, q2))
    p.inst(_T(q2, dagger=True))
    p.inst(_CNOT(q1, q2))
    p.inst(_SWAP(q2, q3))
    p.inst(_T(q2))
    p.inst(_T(q3))
    p.inst(_CNOT(q1, q2))
    p.inst(_H(q3))
    p.inst(_T(q1))
    p.inst(_T(q2, dagger=True))
    p.inst(_CNOT(q1, q2))

    return p 

# 需要導入模塊: from pyquil import gates [as 別名]
# 或者: from pyquil.gates import CZ [as 別名]
def twoq_rb_gateset(q1: int, q2: int) -> Iterable[Gate]:
    """
    Yield the gateset for 2-qubit randomized benchmarking.

    This is two 1-q gatesets and ``CZ``.

    :param q1: The first qubit.
    :param q2: The second qubit.
    """
    yield from oneq_rb_gateset(q1)
    yield from oneq_rb_gateset(q2)
    yield CZ(q1, q2) 

# 需要導入模塊: from pyquil import gates [as 別名]
# 或者: from pyquil.gates import CZ [as 別名]
def test_decoherence_noise():
    prog = Program(RX(np.pi / 2, 0), CZ(0, 1), RZ(np.pi, 0))
    gates = _get_program_gates(prog)
    m1 = _decoherence_noise_model(gates, T1=INFINITY, T2=INFINITY, ro_fidelity=1.0)

    # with no readout error, assignment_probs = identity matrix
    assert np.allclose(m1.assignment_probs[0], np.eye(2))
    assert np.allclose(m1.assignment_probs[1], np.eye(2))
    for g in m1.gates:
        # with infinite coherence time all kraus maps should only have a single, unitary kraus op
        assert len(g.kraus_ops) == 1
        (k0,) = g.kraus_ops
        # check unitarity
        k0dk0 = k0.dot(k0.conjugate().transpose())
        assert np.allclose(k0dk0, np.eye(k0dk0.shape[0]))

    # verify that selective (by qubit) dephasing and readout infidelity is working
    m2 = _decoherence_noise_model(gates, T1=INFINITY, T2={0: 30e-6}, ro_fidelity={0: 0.95, 1: 1.0})
    assert np.allclose(m2.assignment_probs[0], [[0.95, 0.05], [0.05, 0.95]])
    assert np.allclose(m2.assignment_probs[1], np.eye(2))
    for g in m2.gates:
        if 0 in g.targets:
            # single dephasing (no damping) channel on qc 0, no noise on qc1 -> 2 Kraus ops
            assert len(g.kraus_ops) == 2
        else:
            assert len(g.kraus_ops) == 1

    # verify that combined T1 and T2 will lead to 4 outcome Kraus map.
    m3 = _decoherence_noise_model(gates, T1={0: 30e-6}, T2={0: 30e-6})
    for g in m3.gates:
        if 0 in g.targets:
            # damping (implies dephasing) channel on qc 0, no noise on qc1 -> 4 Kraus ops
            assert len(g.kraus_ops) == 4
        else:
            assert len(g.kraus_ops) == 1

    # verify that gate names are translated
    new_prog = apply_noise_model(prog, m3)

    # check that headers have been embedded
    headers = _noise_model_program_header(m3)
    assert all(
        (isinstance(i, Pragma) and i.command in ["ADD-KRAUS", "READOUT-POVM"])
        or isinstance(i, DefGate)
        for i in headers
    )
    assert headers.out() in new_prog.out()

    # verify that high-level add_decoherence_noise reproduces new_prog
    new_prog2 = add_decoherence_noise(prog, T1={0: 30e-6}, T2={0: 30e-6})
    assert new_prog == new_prog2 

# 需要導入模塊: from pyquil import gates [as 別名]
# 或者: from pyquil.gates import CZ [as 別名]
def create_graph_state(graph: nx.Graph, use_pragmas=False):
    """
    Write a program to create a graph state according to the specified graph

    A graph state involves Hadamarding all your qubits and then applying a CZ for each
    edge in the graph. A graph state and the ability to measure it however you want gives
    you universal quantum computation. Some good references are [MBQC]_ and [MBCS]_.

    Similar to a Bell state / GHZ state, we can try to prepare a graph state and measure
    how well we've done according to expected parities.

    .. [MBQC] A One-Way Quantum Computer.
           Raussendorf et al.
           Phys. Rev. Lett. 86, 5188 (2001).
           https://doi.org/10.1103/PhysRevLett.86.5188
           https://arxiv.org/abs/quant-ph/0010033

    .. [MBCS] Measurement-based quantum computation with cluster states.
           Raussendorf et al.
           Phys. Rev. A 68, 022312 (2003).
           https://dx.doi.org/10.1103/PhysRevA.68.022312
           https://arxiv.org/abs/quant-ph/0301052

    :param graph: The graph. Nodes are used as arguments to gates, so they should be qubit-like.
    :param use_pragmas: Use COMMUTING_BLOCKS pragmas to hint at the compiler
    :return: A program that constructs a graph state.
    """
    program = Program()
    for q in graph.nodes:
        program += H(q)

    if use_pragmas:
        program += Pragma('COMMUTING_BLOCKS')
    for a, b in graph.edges:
        if use_pragmas:
            program += Pragma('BLOCK')
        program += CZ(a, b)
        if use_pragmas:
            program += Pragma('END_BLOCK')
    if use_pragmas:
        program += Pragma('END_COMMUTING_BLOCKS')

    return program