Samplex 입출력

import matplotlib.pyplot as plt
import numpy as np
from qiskit.circuit import ClassicalRegister, Parameter, QuantumCircuit, QuantumRegister
from qiskit.quantum_info import Operator, Pauli, PauliLindbladMap

from samplomatic import ChangeBasis, InjectNoise, Twirl, build

# our circuit has two classical registers named alpha and beta
circuit = QuantumCircuit(
    QuantumRegister(4), alpha := ClassicalRegister(3, "alpha"), beta := ClassicalRegister(1, "beta")
)

# the first box is only twirled
with circuit.box([Twirl()]):
    for idx in range(4):
        circuit.rx(Parameter(f"a{idx}"), idx)
    circuit.cz(0, 1)
    circuit.cz(1, 2)

# the second box is twirled, and has noise injected
with circuit.box([Twirl(), InjectNoise(ref="ref1", modifier_ref="mod_ref1")]):
    circuit.h(1)
    circuit.cz(1, 2)

# the third box is twirled, and has different noise injected
with circuit.box([Twirl(), InjectNoise(ref="ref2", modifier_ref="mod_ref2")]):
    circuit.rx(0.1, range(4))
    circuit.cz(0, 1)
    circuit.cz(1, 2)

# the fourth box is the same as the second, but with a different modifer ref
with circuit.box([Twirl(), InjectNoise(ref="ref1", modifier_ref="mod_ref3")]):
    circuit.h(1)
    circuit.cz(1, 2)

circuit.barrier()

# the final two boxes twirl, and add a basis change in one case
with circuit.box([Twirl(), ChangeBasis(ref="conclude")]):
    circuit.measure(range(3), alpha)

with circuit.box([Twirl()]):
    circuit.measure([3], beta)

circuit.draw("mpl")

template, samplex = build(circuit)

template.draw("mpl", fold=100)

samplex.draw()

print(samplex)

samplex.inputs().specs

for spec in samplex.outputs().get_specs("flips"):
    print(spec.name, spec.shape, spec.dtype)

inputs = samplex.inputs().bind(
    # bind() concatenates nested dicts with a '.' so that we can
    # set 'pauli_lindblad_maps.noise0/1' as follows. note that the
    # names 'ref1' and 'ref2' derive from the names in the InjectNoise
    # annotation.
    pauli_lindblad_maps={
        "ref1": PauliLindbladMap.identity(2),
        "ref2": PauliLindbladMap.identity(4),
    },
    # likewise, we can set all basis changes as follows, where
    # the name 'conclude' comes from our basis change annotation
    basis_changes={"conclude": [0, 1, 2]},
    # we must provide values for all parameters in the original circuit
    parameter_values=np.linspace(0, 1, 4),
)

outputs = samplex.sample(inputs, num_randomizations=3)
print(outputs)

inputs = (
    samplex.inputs()
    .bind(
        pauli_lindblad_maps={
            "ref1": PauliLindbladMap.identity(2),
            "ref2": PauliLindbladMap.identity(4),
        }
    )
    .bind(parameter_values=np.linspace(0, 1, 4))
)

# once the final requirement is bound, fully_bound becomes True
print("Fully bound?", inputs.fully_bound)
inputs["basis_changes.conclude"] = [0, 2, 3]
print("Fully bound?", inputs.fully_bound)

# setting optional values does not affect whether the interface is fully bound
inputs["noise_scales.mod_ref1"] = 3
print("Fully bound?", inputs.fully_bound)

print("(num_randomizations, num_template_params) =", outputs["parameter_values"].shape)
print(outputs["parameter_values"][0, :])

inputs = {
    "pauli_lindblad_maps": {
        "ref1": PauliLindbladMap.identity(2),
        "ref2": PauliLindbladMap.identity(4),
    },
    "basis_changes": {"conclude": [0, 1, 2]},
    "parameter_values": np.linspace(0, 1, 4),
}
outputs = samplex.sample(inputs, num_randomizations=3)

# up to precision loss, these are equivalent via automatic type coersion of array inputs
samplex.inputs()["parameter_values"] = [1, 2, 8, 9]
samplex.inputs()["parameter_values"] = np.array([1, 2, 8, 9], dtype=np.float16)

print("All free dimensions:", outputs.free_dimensions)
print("Current constraints:", outputs.bound_dimensions)

# both the PauliLindbladMap and the local scales imply 2 terms, so that the free dimension
# 'num_terms_noise2' is satisfied
inputs = samplex.inputs().bind(
    pauli_lindblad_maps={"ref2": PauliLindbladMap.from_list([("XXYZ", 0.1), ("IIXX", 0.2)])},
    local_scales={"mod_ref2": [1, 2]},
)
print("All free dimensions:", inputs.free_dimensions)
print("Current constraints:", inputs.bound_dimensions)

box_of_interest = circuit[1]
qubit_ordering_convention = [qubit for qubit in circuit.qubits if qubit in box_of_interest.qubits]
qubit_ordering_convention

samplex.inputs().bind(
    pauli_lindblad_maps={
        "ref1": (noise1 := PauliLindbladMap.from_sparse_list([("X", [1], 0.12)], num_qubits=2))
    }
)
noise1

samplex.inputs().bind(basis_changes={"conclude": (basis_change := [2, 3, 1])})
basis_change

inputs = samplex.inputs().bind(
    pauli_lindblad_maps={
        "ref1": PauliLindbladMap.identity(2),
        "ref2": PauliLindbladMap.identity(4),
    },
    basis_changes={"conclude": [0, 0, 0]},
    parameter_values=np.linspace(0, 1, 4),
)

outputs = samplex.sample(inputs, num_randomizations=3)

bound_template = template.assign_parameters(outputs["parameter_values"][2])
bound_template.draw("mpl", fold=1000)

from samplomatic.utils import unbox

# Operator requires that we unpack all of the boxes first
unboxed = unbox(circuit).assign_parameters(inputs["parameter_values"])
# We want to plot unitary matrix amplitudes, so we need to remove the non-unitary measurements
unboxed.remove_final_measurements()
unboxed_unitary = Operator(unboxed)

# Plot magnitudes of the unitary matrix represenation of the circuit
plt.subplot(1, 4, 1)
plt.imshow(np.abs(unboxed_unitary))
plt.title("Base Circuit")

# For each randomization we sampled, plot the unitary matrix representation
for idx in range(3):
    bound_template = template.assign_parameters(outputs["parameter_values"][idx])
    bound_template.remove_final_measurements()

    # The example does measurement twirling by compiling random bitflip gates before the
    # measurements, so we need to undo these at the operator level for each randomization.
    # We do this by casting them to Paulis and composing with the bound circuit's unitary
    alpha_flips = Pauli(([0, 0, 0], outputs["measurement_flips.alpha"][idx, 0]))
    beta_flips = Pauli(([0], outputs["measurement_flips.beta"][idx, 0]))
    flips = beta_flips ^ alpha_flips
    bound_unitary = Operator(bound_template) & flips

    # Plot magnitudes of the unitary matrix represenation of the circuit
    plt.subplot(1, 4, idx + 2)
    plt.imshow(np.abs(bound_unitary))
    plt.title(f"Randomization {idx}")

plt.tight_layout()

from qiskit.primitives import StatevectorEstimator as Estimator
from qiskit.primitives import StatevectorSampler as Sampler
from qiskit.primitives.containers import BitArray

# simulate some expectation values direction from the base circuit
estimator_job = Estimator().run([(unboxed, ["IZII", "IIZI", "IIIZ"])])
evs = estimator_job.result()[0].data["evs"]

# get the sampler data from each randomization, and do bitflip correction
sampler_job = Sampler().run([(template, outputs["parameter_values"])], shots=10_000)
alpha_data = sampler_job.result()[0].data["alpha"]
alpha_data ^= BitArray.from_bool_array(outputs["measurement_flips.alpha"], "little")

# compare the results
print("  EVs from base circuit:", evs)
print("EVs from randomizations:", alpha_data.expectation_values(["ZII", "IZI", "IIZ"]))