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|---|---|---|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
top = QuantumCircuit(1)
top.x(0);
bottom = QuantumCircuit(2)
bottom.cry(0.2, 0, 1);
tensored = bottom.tensor(top)
tensored.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumRegister, ClassicalRegister, QuantumCircuit
from qiskit.dagcircuit import DAGCircuit
from qiskit.converters import circuit_to_dag
from qiskit.circuit.library.standard_gates import CHGate, U2Gate, CXGate
from qiskit.converters import dag_to_circuit
q = QuantumRegister(3, 'q')
c = ClassicalRegister(3, 'c')
circ = QuantumCircuit(q, c)
circ.h(q[0])
circ.cx(q[0], q[1])
circ.measure(q[0], c[0])
circ.rz(0.5, q[1]).c_if(c, 2)
dag = circuit_to_dag(circ)
circuit = dag_to_circuit(dag)
circuit.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import pulse
d0 = pulse.DriveChannel(0)
x90 = pulse.Gaussian(10, 0.1, 3)
x180 = pulse.Gaussian(10, 0.2, 3)
with pulse.build() as hahn_echo:
with pulse.align_equispaced(duration=100):
pulse.play(x90, d0)
pulse.play(x180, d0)
pulse.play(x90, d0)
hahn_echo.draw()
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
import numpy as np
from qiskit import pulse
d0 = pulse.DriveChannel(0)
x90 = pulse.Gaussian(10, 0.1, 3)
x180 = pulse.Gaussian(10, 0.2, 3)
def udd10_pos(j):
return np.sin(np.pi*j/(2*10 + 2))**2
with pulse.build() as udd_sched:
pulse.play(x90, d0)
with pulse.align_func(duration=300, func=udd10_pos):
for _ in range(10):
pulse.play(x180, d0)
pulse.play(x90, d0)
udd_sched.draw()
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.transpiler.passes import RemoveBarriers
circuit = QuantumCircuit(1)
circuit.x(0)
circuit.barrier()
circuit.h(0)
circuit = RemoveBarriers()(circuit)
circuit.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumRegister, ClassicalRegister, QuantumCircuit
from qiskit.tools.visualization import circuit_drawer
q = QuantumRegister(1)
c = ClassicalRegister(1)
qc = QuantumCircuit(q, c)
qc.h(q)
qc.measure(q, c)
circuit_drawer(qc, output='mpl', style={'backgroundcolor': '#EEEEEE'})
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumRegister, ClassicalRegister, QuantumCircuit
from qiskit.dagcircuit import DAGCircuit
from qiskit.converters import circuit_to_dag
from qiskit.visualization import dag_drawer
q = QuantumRegister(3, 'q')
c = ClassicalRegister(3, 'c')
circ = QuantumCircuit(q, c)
circ.h(q[0])
circ.cx(q[0], q[1])
circ.measure(q[0], c[0])
circ.rz(0.5, q[1]).c_if(c, 2)
dag = circuit_to_dag(circ)
dag_drawer(dag)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.quantum_info import Statevector
from qiskit.visualization import plot_bloch_multivector
qc = QuantumCircuit(2)
qc.h(0)
qc.x(1)
state = Statevector(qc)
plot_bloch_multivector(state)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.quantum_info import Statevector
from qiskit.visualization import plot_bloch_multivector
qc = QuantumCircuit(2)
qc.h(0)
qc.x(1)
# You can reverse the order of the qubits.
from qiskit.quantum_info import DensityMatrix
qc = QuantumCircuit(2)
qc.h([0, 1])
qc.t(1)
qc.s(0)
qc.cx(0,1)
matrix = DensityMatrix(qc)
plot_bloch_multivector(matrix, title='My Bloch Spheres', reverse_bits=True)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
import numpy as np
from qiskit import QuantumCircuit, transpile
from qiskit.providers.fake_provider import FakeVigoV2
from qiskit.visualization import plot_circuit_layout
from qiskit.tools.monitor import job_monitor
from qiskit.providers.fake_provider import FakeVigoV2
import matplotlib.pyplot as plt
ghz = QuantumCircuit(3, 3)
ghz.h(0)
for idx in range(1,3):
ghz.cx(0,idx)
ghz.measure(range(3), range(3))
backend = FakeVigoV2()
new_circ_lv3 = transpile(ghz, backend=backend, optimization_level=3)
plot_circuit_layout(new_circ_lv3, backend)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, execute
from qiskit.visualization import plot_error_map
from qiskit.providers.fake_provider import FakeVigoV2
backend = FakeVigoV2()
plot_error_map(backend)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, execute
from qiskit.providers.fake_provider import FakeVigoV2
from qiskit.visualization import plot_gate_map
backend = FakeVigoV2()
plot_gate_map(backend)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
# You can choose different colors for the real and imaginary parts of the density matrix.
from qiskit import QuantumCircuit
from qiskit.quantum_info import DensityMatrix
from qiskit.visualization import plot_state_city
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
state = DensityMatrix(qc)
plot_state_city(state, color=['midnightblue', 'crimson'], title="New State City")
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
# You can make the bars more transparent to better see the ones that are behind
# if they overlap.
import numpy as np
from qiskit.quantum_info import Statevector
from qiskit.visualization import plot_state_city
from qiskit import QuantumCircuit
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
qc = QuantumCircuit(2)
qc.h([0, 1])
qc.cz(0,1)
qc.ry(np.pi/3, 0)
qc.rx(np.pi/5, 1)
state = Statevector(qc)
plot_state_city(state, alpha=0.6)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
import numpy as np
from qiskit import QuantumCircuit
from qiskit.quantum_info import DensityMatrix
from qiskit.visualization import plot_state_hinton
qc = QuantumCircuit(2)
qc.h([0, 1])
qc.cz(0,1)
qc.ry(np.pi/3 , 0)
qc.rx(np.pi/5, 1)
state = DensityMatrix(qc)
plot_state_hinton(state, title="New Hinton Plot")
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
# You can set a color for all the bars.
from qiskit import QuantumCircuit
from qiskit.quantum_info import Statevector
from qiskit.visualization import plot_state_paulivec
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
state = Statevector(qc)
plot_state_paulivec(state, color='midnightblue', title="New PauliVec plot")
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
# If you introduce a list with less colors than bars, the color of the bars will
# alternate following the sequence from the list.
import numpy as np
from qiskit.quantum_info import DensityMatrix
from qiskit import QuantumCircuit
from qiskit.visualization import plot_state_paulivec
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
qc = QuantumCircuit(2)
qc.h([0, 1])
qc.cz(0, 1)
qc.ry(np.pi/3, 0)
qc.rx(np.pi/5, 1)
matrix = DensityMatrix(qc)
plot_state_paulivec(matrix, color=['crimson', 'midnightblue', 'seagreen'])
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.quantum_info import Statevector
from qiskit.visualization import plot_state_qsphere
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
state = Statevector(qc)
plot_state_qsphere(state)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
# You can show the phase of each state and use
# degrees instead of radians
from qiskit.quantum_info import DensityMatrix
import numpy as np
from qiskit import QuantumCircuit
from qiskit.visualization import plot_state_qsphere
qc = QuantumCircuit(2)
qc.h([0, 1])
qc.cz(0,1)
qc.ry(np.pi/3, 0)
qc.rx(np.pi/5, 1)
qc.z(1)
matrix = DensityMatrix(qc)
plot_state_qsphere(matrix,
show_state_phases = True, use_degrees = True)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile, schedule
from qiskit.visualization.pulse_v2 import draw
from qiskit.providers.fake_provider import FakeBoeblingen
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
qc.measure_all()
qc = transpile(qc, FakeBoeblingen(), layout_method='trivial')
sched = schedule(qc, FakeBoeblingen())
draw(sched, backend=FakeBoeblingen())
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile, schedule
from qiskit.visualization.pulse_v2 import draw, IQXSimple
from qiskit.providers.fake_provider import FakeBoeblingen
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
qc.measure_all()
qc = transpile(qc, FakeBoeblingen(), layout_method='trivial')
sched = schedule(qc, FakeBoeblingen())
draw(sched, style=IQXSimple(), backend=FakeBoeblingen())
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile, schedule
from qiskit.visualization.pulse_v2 import draw, IQXDebugging
from qiskit.providers.fake_provider import FakeBoeblingen
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
qc.measure_all()
qc = transpile(qc, FakeBoeblingen(), layout_method='trivial')
sched = schedule(qc, FakeBoeblingen())
draw(sched, style=IQXDebugging(), backend=FakeBoeblingen())
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile, schedule
from qiskit.visualization.timeline import draw
from qiskit.providers.fake_provider import FakeBoeblingen
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0,1)
qc = transpile(qc, FakeBoeblingen(), scheduling_method='alap', layout_method='trivial')
draw(qc)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile, schedule
from qiskit.visualization.timeline import draw, IQXSimple
from qiskit.providers.fake_provider import FakeBoeblingen
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0,1)
qc = transpile(qc, FakeBoeblingen(), scheduling_method='alap', layout_method='trivial')
draw(qc, style=IQXSimple())
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile, schedule
from qiskit.visualization.timeline import draw, IQXDebugging
from qiskit.providers.fake_provider import FakeBoeblingen
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0,1)
qc = transpile(qc, FakeBoeblingen(), scheduling_method='alap', layout_method='trivial')
draw(qc, style=IQXDebugging())
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit.algorithms.optimizers import SLSQP
from qiskit.circuit.library import TwoLocal
num_qubits = 2
ansatz = TwoLocal(num_qubits, "ry", "cz")
optimizer = SLSQP(maxiter=1000)
ansatz.decompose().draw("mpl", style="iqx")
from qiskit.primitives import Estimator
estimator = Estimator()
from qiskit.algorithms.minimum_eigensolvers import VQE
vqe = VQE(estimator, ansatz, optimizer)
from qiskit.quantum_info import SparsePauliOp
H2_op = SparsePauliOp.from_list([
("II", -1.052373245772859),
("IZ", 0.39793742484318045),
("ZI", -0.39793742484318045),
("ZZ", -0.01128010425623538),
("XX", 0.18093119978423156)
])
result = vqe.compute_minimum_eigenvalue(H2_op)
print(result)
from qiskit.algorithms.optimizers import SPSA
estimator = Estimator(options={"shots": 1000})
vqe.estimator = estimator
vqe.optimizer = SPSA(maxiter=100)
result = vqe.compute_minimum_eigenvalue(operator=H2_op)
print(result)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit.quantum_info import SparsePauliOp
H2_op = SparsePauliOp.from_list(
[
("II", -1.052373245772859),
("IZ", 0.39793742484318045),
("ZI", -0.39793742484318045),
("ZZ", -0.01128010425623538),
("XX", 0.18093119978423156),
]
)
from qiskit.primitives import Estimator
estimator = Estimator()
import numpy as np
from qiskit.algorithms.minimum_eigensolvers import VQE
from qiskit.algorithms.optimizers import COBYLA, L_BFGS_B, SLSQP
from qiskit.circuit.library import TwoLocal
from qiskit.utils import algorithm_globals
# we will iterate over these different optimizers
optimizers = [COBYLA(maxiter=80), L_BFGS_B(maxiter=60), SLSQP(maxiter=60)]
converge_counts = np.empty([len(optimizers)], dtype=object)
converge_vals = np.empty([len(optimizers)], dtype=object)
for i, optimizer in enumerate(optimizers):
print("\rOptimizer: {} ".format(type(optimizer).__name__), end="")
algorithm_globals.random_seed = 50
ansatz = TwoLocal(rotation_blocks="ry", entanglement_blocks="cz")
counts = []
values = []
def store_intermediate_result(eval_count, parameters, mean, std):
counts.append(eval_count)
values.append(mean)
vqe = VQE(estimator, ansatz, optimizer, callback=store_intermediate_result)
result = vqe.compute_minimum_eigenvalue(operator=H2_op)
converge_counts[i] = np.asarray(counts)
converge_vals[i] = np.asarray(values)
print("\rOptimization complete ");
import pylab
pylab.rcParams["figure.figsize"] = (12, 8)
for i, optimizer in enumerate(optimizers):
pylab.plot(converge_counts[i], converge_vals[i], label=type(optimizer).__name__)
pylab.xlabel("Eval count")
pylab.ylabel("Energy")
pylab.title("Energy convergence for various optimizers")
pylab.legend(loc="upper right");
from qiskit.algorithms.minimum_eigensolvers import NumPyMinimumEigensolver
from qiskit.opflow import PauliSumOp
numpy_solver = NumPyMinimumEigensolver()
result = numpy_solver.compute_minimum_eigenvalue(operator=PauliSumOp(H2_op))
ref_value = result.eigenvalue.real
print(f"Reference value: {ref_value:.5f}")
pylab.rcParams["figure.figsize"] = (12, 8)
for i, optimizer in enumerate(optimizers):
pylab.plot(
converge_counts[i],
abs(ref_value - converge_vals[i]),
label=type(optimizer).__name__,
)
pylab.xlabel("Eval count")
pylab.ylabel("Energy difference from solution reference value")
pylab.title("Energy convergence for various optimizers")
pylab.yscale("log")
pylab.legend(loc="upper right");
from qiskit.algorithms.gradients import FiniteDiffEstimatorGradient
estimator = Estimator()
gradient = FiniteDiffEstimatorGradient(estimator, epsilon=0.01)
algorithm_globals.random_seed = 50
ansatz = TwoLocal(rotation_blocks="ry", entanglement_blocks="cz")
optimizer = SLSQP(maxiter=100)
counts = []
values = []
def store_intermediate_result(eval_count, parameters, mean, std):
counts.append(eval_count)
values.append(mean)
vqe = VQE(
estimator, ansatz, optimizer, callback=store_intermediate_result, gradient=gradient
)
result = vqe.compute_minimum_eigenvalue(operator=H2_op)
print(f"Value using Gradient: {result.eigenvalue.real:.5f}")
pylab.rcParams["figure.figsize"] = (12, 8)
pylab.plot(counts, values, label=type(optimizer).__name__)
pylab.xlabel("Eval count")
pylab.ylabel("Energy")
pylab.title("Energy convergence using Gradient")
pylab.legend(loc="upper right");
print(result)
cost_function_evals = result.cost_function_evals
initial_pt = result.optimal_point
estimator1 = Estimator()
gradient1 = FiniteDiffEstimatorGradient(estimator, epsilon=0.01)
ansatz1 = TwoLocal(rotation_blocks="ry", entanglement_blocks="cz")
optimizer1 = SLSQP(maxiter=1000)
vqe1 = VQE(
estimator1, ansatz1, optimizer1, gradient=gradient1, initial_point=initial_pt
)
result1 = vqe1.compute_minimum_eigenvalue(operator=H2_op)
print(result1)
cost_function_evals1 = result1.cost_function_evals
print()
print(
f"cost_function_evals is {cost_function_evals1} with initial point versus {cost_function_evals} without it."
)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit.quantum_info import SparsePauliOp
H2_op = SparsePauliOp.from_list(
[
("II", -1.052373245772859),
("IZ", 0.39793742484318045),
("ZI", -0.39793742484318045),
("ZZ", -0.01128010425623538),
("XX", 0.18093119978423156),
]
)
print(f"Number of qubits: {H2_op.num_qubits}")
from qiskit.algorithms import NumPyMinimumEigensolver
from qiskit.opflow import PauliSumOp
numpy_solver = NumPyMinimumEigensolver()
result = numpy_solver.compute_minimum_eigenvalue(operator=PauliSumOp(H2_op))
ref_value = result.eigenvalue.real
print(f"Reference value: {ref_value:.5f}")
# define ansatz and optimizer
from qiskit.circuit.library import TwoLocal
from qiskit.algorithms.optimizers import SPSA
iterations = 125
ansatz = TwoLocal(rotation_blocks="ry", entanglement_blocks="cz")
spsa = SPSA(maxiter=iterations)
# define callback
# note: Re-run this cell to restart lists before training
counts = []
values = []
def store_intermediate_result(eval_count, parameters, mean, std):
counts.append(eval_count)
values.append(mean)
# define Aer Estimator for noiseless statevector simulation
from qiskit.utils import algorithm_globals
from qiskit_aer.primitives import Estimator as AerEstimator
seed = 170
algorithm_globals.random_seed = seed
noiseless_estimator = AerEstimator(
run_options={"seed": seed, "shots": 1024},
transpile_options={"seed_transpiler": seed},
)
# instantiate and run VQE
from qiskit.algorithms.minimum_eigensolvers import VQE
vqe = VQE(
noiseless_estimator, ansatz, optimizer=spsa, callback=store_intermediate_result
)
result = vqe.compute_minimum_eigenvalue(operator=H2_op)
print(f"VQE on Aer qasm simulator (no noise): {result.eigenvalue.real:.5f}")
print(
f"Delta from reference energy value is {(result.eigenvalue.real - ref_value):.5f}"
)
import pylab
pylab.rcParams["figure.figsize"] = (12, 4)
pylab.plot(counts, values)
pylab.xlabel("Eval count")
pylab.ylabel("Energy")
pylab.title("Convergence with no noise")
from qiskit_aer.noise import NoiseModel
from qiskit.providers.fake_provider import FakeVigo
# fake providers contain data from real IBM Quantum devices stored in Qiskit Terra,
# and are useful for extracting realistic noise models.
device = FakeVigo()
coupling_map = device.configuration().coupling_map
noise_model = NoiseModel.from_backend(device)
print(noise_model)
noisy_estimator = AerEstimator(
backend_options={
"method": "density_matrix",
"coupling_map": coupling_map,
"noise_model": noise_model,
},
run_options={"seed": seed, "shots": 1024},
transpile_options={"seed_transpiler": seed},
)
# re-start callback variables
counts = []
values = []
vqe.estimator = noisy_estimator
result1 = vqe.compute_minimum_eigenvalue(operator=H2_op)
print(f"VQE on Aer qasm simulator (with noise): {result1.eigenvalue.real:.5f}")
print(
f"Delta from reference energy value is {(result1.eigenvalue.real - ref_value):.5f}"
)
if counts or values:
pylab.rcParams["figure.figsize"] = (12, 4)
pylab.plot(counts, values)
pylab.xlabel("Eval count")
pylab.ylabel("Energy")
pylab.title("Convergence with noise")
print(f"Reference value: {ref_value:.5f}")
print(f"VQE on Aer qasm simulator (no noise): {result.eigenvalue.real:.5f}")
print(f"VQE on Aer qasm simulator (with noise): {result1.eigenvalue.real:.5f}")
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit.quantum_info import SparsePauliOp
H2_op = SparsePauliOp.from_list(
[
("II", -1.052373245772859),
("IZ", 0.39793742484318045),
("ZI", -0.39793742484318045),
("ZZ", -0.01128010425623538),
("XX", 0.18093119978423156),
]
)
from qiskit.circuit.library import TwoLocal
from qiskit.algorithms.optimizers import SLSQP
ansatz = TwoLocal(3, rotation_blocks=["ry", "rz"], entanglement_blocks="cz", reps=1)
optimizer = SLSQP()
ansatz.decompose().draw('mpl')
from qiskit.primitives import Sampler, Estimator
from qiskit.algorithms.state_fidelities import ComputeUncompute
estimator = Estimator()
sampler = Sampler()
fidelity = ComputeUncompute(sampler)
k = 3
betas = [33, 33, 33]
counts = []
values = []
steps = []
def callback(eval_count, params, value, meta, step):
counts.append(eval_count)
values.append(value)
steps.append(step)
from qiskit.algorithms.eigensolvers import VQD
vqd = VQD(estimator, fidelity, ansatz, optimizer, k=k, betas=betas, callback=callback)
result = vqd.compute_eigenvalues(operator = H2_op)
vqd_values = result.optimal_values
print(vqd_values)
import numpy as np
import pylab
pylab.rcParams["figure.figsize"] = (12, 8)
steps = np.asarray(steps)
counts = np.asarray(counts)
values = np.asarray(values)
for i in range(1,4):
_counts = counts[np.where(steps == i)]
_values = values[np.where(steps == i)]
pylab.plot(_counts, _values, label=f"State {i-1}")
pylab.xlabel("Eval count")
pylab.ylabel("Energy")
pylab.title("Energy convergence for each computed state")
pylab.legend(loc="upper right");
from qiskit.algorithms.eigensolvers import NumPyEigensolver
from qiskit.opflow import PauliSumOp
exact_solver = NumPyEigensolver(k=3)
exact_result = exact_solver.compute_eigenvalues(PauliSumOp(H2_op))
ref_values = exact_result.eigenvalues
print(f"Reference values: {ref_values}")
print(f"VQD values: {vqd_values}")
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from __future__ import annotations
import numpy as np
import networkx as nx
num_nodes = 4
w = np.array([[0., 1., 1., 0.],
[1., 0., 1., 1.],
[1., 1., 0., 1.],
[0., 1., 1., 0.]])
G = nx.from_numpy_array(w)
layout = nx.random_layout(G, seed=10)
colors = ['r', 'g', 'b', 'y']
nx.draw(G, layout, node_color=colors)
labels = nx.get_edge_attributes(G, 'weight')
nx.draw_networkx_edge_labels(G, pos=layout, edge_labels=labels);
def objective_value(x: np.ndarray, w: np.ndarray) -> float:
"""Compute the value of a cut.
Args:
x: Binary string as numpy array.
w: Adjacency matrix.
Returns:
Value of the cut.
"""
X = np.outer(x, (1 - x))
w_01 = np.where(w != 0, 1, 0)
return np.sum(w_01 * X)
def bitfield(n: int, L: int) -> list[int]:
result = np.binary_repr(n, L)
return [int(digit) for digit in result] # [2:] to chop off the "0b" part
# use the brute-force way to generate the oracle
L = num_nodes
max = 2**L
sol = np.inf
for i in range(max):
cur = bitfield(i, L)
how_many_nonzero = np.count_nonzero(cur)
if how_many_nonzero * 2 != L: # not balanced
continue
cur_v = objective_value(np.array(cur), w)
if cur_v < sol:
sol = cur_v
print(f'Objective value computed by the brute-force method is {sol}')
from qiskit.quantum_info import Pauli, SparsePauliOp
def get_operator(weight_matrix: np.ndarray) -> tuple[SparsePauliOp, float]:
r"""Generate Hamiltonian for the graph partitioning
Notes:
Goals:
1 Separate the vertices into two set of the same size.
2 Make sure the number of edges between the two set is minimized.
Hamiltonian:
H = H_A + H_B
H_A = sum\_{(i,j)\in E}{(1-ZiZj)/2}
H_B = (sum_{i}{Zi})^2 = sum_{i}{Zi^2}+sum_{i!=j}{ZiZj}
H_A is for achieving goal 2 and H_B is for achieving goal 1.
Args:
weight_matrix: Adjacency matrix.
Returns:
Operator for the Hamiltonian
A constant shift for the obj function.
"""
num_nodes = len(weight_matrix)
pauli_list = []
coeffs = []
shift = 0
for i in range(num_nodes):
for j in range(i):
if weight_matrix[i, j] != 0:
x_p = np.zeros(num_nodes, dtype=bool)
z_p = np.zeros(num_nodes, dtype=bool)
z_p[i] = True
z_p[j] = True
pauli_list.append(Pauli((z_p, x_p)))
coeffs.append(-0.5)
shift += 0.5
for i in range(num_nodes):
for j in range(num_nodes):
if i != j:
x_p = np.zeros(num_nodes, dtype=bool)
z_p = np.zeros(num_nodes, dtype=bool)
z_p[i] = True
z_p[j] = True
pauli_list.append(Pauli((z_p, x_p)))
coeffs.append(1.0)
else:
shift += 1
return SparsePauliOp(pauli_list, coeffs=coeffs), shift
qubit_op, offset = get_operator(w)
from qiskit.algorithms.minimum_eigensolvers import QAOA
from qiskit.algorithms.optimizers import COBYLA
from qiskit.circuit.library import TwoLocal
from qiskit.primitives import Sampler
from qiskit.quantum_info import Pauli, Statevector
from qiskit.result import QuasiDistribution
from qiskit.utils import algorithm_globals
sampler = Sampler()
def sample_most_likely(state_vector: QuasiDistribution | Statevector) -> np.ndarray:
"""Compute the most likely binary string from state vector.
Args:
state_vector: State vector or quasi-distribution.
Returns:
Binary string as an array of ints.
"""
if isinstance(state_vector, QuasiDistribution):
values = list(state_vector.values())
else:
values = state_vector
n = int(np.log2(len(values)))
k = np.argmax(np.abs(values))
x = bitfield(k, n)
x.reverse()
return np.asarray(x)
algorithm_globals.random_seed = 10598
optimizer = COBYLA()
qaoa = QAOA(sampler, optimizer, reps=2)
result = qaoa.compute_minimum_eigenvalue(qubit_op)
x = sample_most_likely(result.eigenstate)
print(x)
print(f'Objective value computed by QAOA is {objective_value(x, w)}')
from qiskit.algorithms.minimum_eigensolvers import NumPyMinimumEigensolver
from qiskit.quantum_info import Operator
npme = NumPyMinimumEigensolver()
result = npme.compute_minimum_eigenvalue(Operator(qubit_op))
x = sample_most_likely(result.eigenstate)
print(x)
print(f'Objective value computed by the NumPyMinimumEigensolver is {objective_value(x, w)}')
from qiskit.algorithms.minimum_eigensolvers import SamplingVQE
from qiskit.circuit.library import TwoLocal
from qiskit.utils import algorithm_globals
algorithm_globals.random_seed = 10598
optimizer = COBYLA()
ansatz = TwoLocal(qubit_op.num_qubits, "ry", "cz", reps=2, entanglement="linear")
sampling_vqe = SamplingVQE(sampler, ansatz, optimizer)
result = sampling_vqe.compute_minimum_eigenvalue(qubit_op)
x = sample_most_likely(result.eigenstate)
print(x)
print(f"Objective value computed by VQE is {objective_value(x, w)}")
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.algorithms import AmplificationProblem
# the state we desire to find is '11'
good_state = ['11']
# specify the oracle that marks the state '11' as a good solution
oracle = QuantumCircuit(2)
oracle.cz(0, 1)
# define Grover's algorithm
problem = AmplificationProblem(oracle, is_good_state=good_state)
# now we can have a look at the Grover operator that is used in running the algorithm
# (Algorithm circuits are wrapped in a gate to appear in composition as a block
# so we have to decompose() the op to see it expanded into its component gates.)
problem.grover_operator.decompose().draw(output='mpl')
from qiskit.algorithms import Grover
from qiskit.primitives import Sampler
grover = Grover(sampler=Sampler())
result = grover.amplify(problem)
print('Result type:', type(result))
print()
print('Success!' if result.oracle_evaluation else 'Failure!')
print('Top measurement:', result.top_measurement)
from qiskit.quantum_info import Statevector
oracle = Statevector.from_label('11')
problem = AmplificationProblem(oracle, is_good_state=['11'])
grover = Grover(sampler=Sampler())
result = grover.amplify(problem)
print('Result type:', type(result))
print()
print('Success!' if result.oracle_evaluation else 'Failure!')
print('Top measurement:', result.top_measurement)
problem.grover_operator.oracle.decompose().draw(output='mpl')
from qiskit.circuit.library.phase_oracle import PhaseOracle
from qiskit.exceptions import MissingOptionalLibraryError
# `Oracle` (`PhaseOracle`) as the `oracle` argument
expression = '(a & b)'
try:
oracle = PhaseOracle(expression)
problem = AmplificationProblem(oracle)
display(problem.grover_operator.oracle.decompose().draw(output='mpl'))
except MissingOptionalLibraryError as ex:
print(ex)
import numpy as np
# Specifying `state_preparation`
# to prepare a superposition of |01>, |10>, and |11>
oracle = QuantumCircuit(3)
oracle.ccz(0, 1, 2)
theta = 2 * np.arccos(1 / np.sqrt(3))
state_preparation = QuantumCircuit(3)
state_preparation.ry(theta, 0)
state_preparation.ch(0,1)
state_preparation.x(1)
state_preparation.h(2)
# we only care about the first two bits being in state 1, thus add both possibilities for the last qubit
problem = AmplificationProblem(oracle, state_preparation=state_preparation, is_good_state=['110', '111'])
# state_preparation
print('state preparation circuit:')
problem.grover_operator.state_preparation.draw(output='mpl')
grover = Grover(sampler=Sampler())
result = grover.amplify(problem)
print('Success!' if result.oracle_evaluation else 'Failure!')
print('Top measurement:', result.top_measurement)
oracle = QuantumCircuit(5)
oracle.ccz(0, 1, 2)
oracle.draw(output='mpl')
from qiskit.circuit.library import GroverOperator
grover_op = GroverOperator(oracle, insert_barriers=True)
grover_op.decompose().draw(output='mpl')
grover_op = GroverOperator(oracle, reflection_qubits=[0, 1, 2], insert_barriers=True)
grover_op.decompose().draw(output='mpl')
# a list of binary strings good state
oracle = QuantumCircuit(2)
oracle.cz(0, 1)
good_state = ['11', '00']
problem = AmplificationProblem(oracle, is_good_state=good_state)
print(problem.is_good_state('11'))
# a list of integer good state
oracle = QuantumCircuit(2)
oracle.cz(0, 1)
good_state = [0, 1]
problem = AmplificationProblem(oracle, is_good_state=good_state)
print(problem.is_good_state('11'))
from qiskit.quantum_info import Statevector
# `Statevector` good state
oracle = QuantumCircuit(2)
oracle.cz(0, 1)
good_state = Statevector.from_label('11')
problem = AmplificationProblem(oracle, is_good_state=good_state)
print(problem.is_good_state('11'))
# Callable good state
def callable_good_state(bitstr):
if bitstr == "11":
return True
return False
oracle = QuantumCircuit(2)
oracle.cz(0, 1)
problem = AmplificationProblem(oracle, is_good_state=good_state)
print(problem.is_good_state('11'))
# integer iteration
oracle = QuantumCircuit(2)
oracle.cz(0, 1)
problem = AmplificationProblem(oracle, is_good_state=['11'])
grover = Grover(iterations=1)
# list iteration
oracle = QuantumCircuit(2)
oracle.cz(0, 1)
problem = AmplificationProblem(oracle, is_good_state=['11'])
grover = Grover(iterations=[1, 2, 3])
# using sample_from_iterations
oracle = QuantumCircuit(2)
oracle.cz(0, 1)
problem = AmplificationProblem(oracle, is_good_state=['11'])
grover = Grover(iterations=[1, 2, 3], sample_from_iterations=True)
iterations = Grover.optimal_num_iterations(num_solutions=1, num_qubits=8)
iterations
def to_DIAMACS_CNF_format(bit_rep):
return [index+1 if val==1 else -1 * (index + 1) for index, val in enumerate(bit_rep)]
oracle = QuantumCircuit(2)
oracle.cz(0, 1)
problem = AmplificationProblem(oracle, is_good_state=['11'], post_processing=to_DIAMACS_CNF_format)
problem.post_processing([1, 0, 1])
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
input_3sat_instance = '''
c example DIMACS-CNF 3-SAT
p cnf 3 5
-1 -2 -3 0
1 -2 3 0
1 2 -3 0
1 -2 -3 0
-1 2 3 0
'''
import os
import tempfile
from qiskit.exceptions import MissingOptionalLibraryError
from qiskit.circuit.library.phase_oracle import PhaseOracle
fp = tempfile.NamedTemporaryFile(mode='w+t', delete=False)
fp.write(input_3sat_instance)
file_name = fp.name
fp.close()
oracle = None
try:
oracle = PhaseOracle.from_dimacs_file(file_name)
except MissingOptionalLibraryError as ex:
print(ex)
finally:
os.remove(file_name)
from qiskit.algorithms import AmplificationProblem
problem = None
if oracle is not None:
problem = AmplificationProblem(oracle, is_good_state=oracle.evaluate_bitstring)
from qiskit.algorithms import Grover
from qiskit.primitives import Sampler
grover = Grover(sampler=Sampler())
result = None
if problem is not None:
result = grover.amplify(problem)
print(result.assignment)
from qiskit.tools.visualization import plot_histogram
if result is not None:
display(plot_histogram(result.circuit_results[0]))
expression = '(w ^ x) & ~(y ^ z) & (x & y & z)'
try:
oracle = PhaseOracle(expression)
problem = AmplificationProblem(oracle, is_good_state=oracle.evaluate_bitstring)
grover = Grover(sampler=Sampler())
result = grover.amplify(problem)
display(plot_histogram(result.circuit_results[0]))
except MissingOptionalLibraryError as ex:
print(ex)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
qc = QuantumCircuit(1, 1)
qc.h(0)
qc.measure(0,0)
qc.x(0).c_if(0, 0)
qc.draw(output='mpl')
from qiskit import QuantumRegister, ClassicalRegister
q = QuantumRegister(3, 'q')
c = ClassicalRegister(3, 'c')
qc = QuantumCircuit(q, c)
qc.h([0, 1, 2])
qc.barrier()
qc.measure(q, c)
qc.draw('mpl')
print(bin(3))
print(bin(7))
qc.x(2).c_if(c, 3) # for the 011 case
qc.x(2).c_if(c, 7) # for the 111 case
qc.draw(output='mpl')
nq = 2
m = 2
q = QuantumRegister(nq, 'q')
c = ClassicalRegister(m, 'c')
qc_S = QuantumCircuit(q,c)
qc_S.h(0)
qc_S.x(1)
qc_S.draw('mpl')
from math import pi
cu_circ = QuantumCircuit(2)
cu_circ.cp(pi/2, 0, 1)
cu_circ.draw('mpl')
for _ in range(2 ** (m - 1)):
qc_S.cp(pi/2, 0, 1)
qc_S.draw('mpl')
def x_measurement(qc, qubit, cbit):
"""Measure 'qubit' in the X-basis, and store the result in 'cbit'"""
qc.h(qubit)
qc.measure(qubit, cbit)
x_measurement(qc_S, q[0], c[0])
qc_S.draw('mpl')
qc_S.reset(0)
qc_S.h(0)
qc_S.draw('mpl')
qc_S.p(-pi/2, 0).c_if(c, 1)
qc_S.draw('mpl')
## 2^t c-U operations (with t=m-2)
for _ in range(2 ** (m - 2)):
qc_S.cp(pi/2, 0, 1)
x_measurement(qc_S, q[0], c[1])
qc_S.draw('mpl')
import matplotlib.pyplot as plt
from qiskit.tools.visualization import plot_histogram
from qiskit_aer.primitives import Sampler
sampler = Sampler()
job = sampler.run(qc_S)
result = job.result()
dist0 = result.quasi_dists[0]
key_new = [str(key/2**m) for key in list(dist0.keys())]
dist1 = dict(zip(key_new, dist0.values()))
fig, ax = plt.subplots(1,2)
plot_histogram(dist0, ax=ax[0])
plot_histogram(dist1, ax=ax[1])
plt.tight_layout()
nq = 3 # number of qubits
m = 3 # number of classical bits
q = QuantumRegister(nq,'q')
c = ClassicalRegister(m,'c')
qc = QuantumCircuit(q,c)
qc.h(0)
qc.x([1, 2])
qc.draw('mpl')
cu_circ = QuantumCircuit(nq)
cu_circ.mcp(pi/4, [0, 1], 2)
cu_circ.draw('mpl')
for _ in range(2 ** (m - 1)):
qc.mcp(pi/4, [0, 1], 2)
qc.draw('mpl')
x_measurement(qc, q[0], c[0])
qc.draw('mpl')
qc.reset(0)
qc.h(0)
qc.draw('mpl')
qc.p(-pi/2, 0).c_if(c, 1)
qc.draw('mpl')
for _ in range(2 ** (m - 2)):
qc.mcp(pi/4, [0, 1], 2)
x_measurement(qc, q[0], c[1])
qc.draw('mpl')
# initialization of qubit q0
qc.reset(0)
qc.h(0)
# phase correction
qc.p(-pi/4, 0).c_if(c, 1)
qc.p(-pi/2, 0).c_if(c, 2)
qc.p(-3*pi/2, 0).c_if(c, 3)
# c-U operations
for _ in range(2 ** (m - 3)):
qc.mcp(pi/4, [0, 1], 2)
# X measurement
qc.h(0)
qc.measure(0, 2)
qc.draw('mpl')
result = sampler.run(qc).result()
dist0 = result.quasi_dists[0]
key_new = [str(key/2**m) for key in list(dist0.keys())]
dist1 = dict(zip(key_new, dist0.values()))
fig, ax = plt.subplots(1,2)
plot_histogram(dist0, ax=ax[0])
plot_histogram(dist1, ax=ax[1])
plt.tight_layout()
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
import numpy as np
from qiskit import QuantumCircuit
# Create a Quantum Circuit acting on a quantum register of three qubits
circ = QuantumCircuit(3)
# Add a H gate on qubit 0, putting this qubit in superposition.
circ.h(0)
# Add a CX (CNOT) gate on control qubit 0 and target qubit 1, putting
# the qubits in a Bell state.
circ.cx(0, 1)
# Add a CX (CNOT) gate on control qubit 0 and target qubit 2, putting
# the qubits in a GHZ state.
circ.cx(0, 2)
circ.draw('mpl')
from qiskit.quantum_info import Statevector
# Set the intial state of the simulator to the ground state using from_int
state = Statevector.from_int(0, 2**3)
# Evolve the state by the quantum circuit
state = state.evolve(circ)
#draw using latex
state.draw('latex')
from qiskit.visualization import array_to_latex
#Alternative way of representing in latex
array_to_latex(state)
state.draw('qsphere')
state.draw('hinton')
from qiskit.quantum_info import Operator
U = Operator(circ)
# Show the results
U.data
# Create a Quantum Circuit
meas = QuantumCircuit(3, 3)
meas.barrier(range(3))
# map the quantum measurement to the classical bits
meas.measure(range(3), range(3))
# The Qiskit circuit object supports composition.
# Here the meas has to be first and front=True (putting it before)
# as compose must put a smaller circuit into a larger one.
qc = meas.compose(circ, range(3), front=True)
#drawing the circuit
qc.draw('mpl')
# Adding the transpiler to reduce the circuit to QASM instructions
# supported by the backend
from qiskit import transpile
# Use AerSimulator
from qiskit_aer import AerSimulator
backend = AerSimulator()
# First we have to transpile the quantum circuit
# to the low-level QASM instructions used by the
# backend
qc_compiled = transpile(qc, backend)
# Execute the circuit on the qasm simulator.
# We've set the number of repeats of the circuit
# to be 1024, which is the default.
job_sim = backend.run(qc_compiled, shots=1024)
# Grab the results from the job.
result_sim = job_sim.result()
counts = result_sim.get_counts(qc_compiled)
print(counts)
from qiskit.visualization import plot_histogram
plot_histogram(counts)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
import numpy as np
from qiskit import *
# Create a Quantum Circuit acting on a quantum register of three qubits
circ = QuantumCircuit(3)
# Add a H gate on qubit $q_{0}$, putting this qubit in superposition.
circ.h(0)
# Add a CX (CNOT) gate on control qubit $q_{0}$ and target qubit $q_{1}$, putting
# the qubits in a Bell state.
circ.cx(0, 1)
# Add a CX (CNOT) gate on control qubit $q_{0}$ and target qubit $q_{2}$, putting
# the qubits in a GHZ state.
circ.cx(0, 2)
circ.draw('mpl')
# Import Aer
from qiskit import Aer
# Run the quantum circuit on a statevector simulator backend
backend = Aer.get_backend('statevector_simulator')
# Create a Quantum Program for execution
job = backend.run(circ)
result = job.result()
outputstate = result.get_statevector(circ, decimals=3)
print(outputstate)
from qiskit.visualization import plot_state_city
plot_state_city(outputstate)
# Run the quantum circuit on a unitary simulator backend
backend = Aer.get_backend('unitary_simulator')
job = backend.run(circ)
result = job.result()
# Show the results
print(result.get_unitary(circ, decimals=3))
# Create a Quantum Circuit
meas = QuantumCircuit(3, 3)
meas.barrier(range(3))
# map the quantum measurement to the classical bits
meas.measure(range(3), range(3))
# The Qiskit circuit object supports composition using
# the compose method.
circ.add_register(meas.cregs[0])
qc = circ.compose(meas)
#drawing the circuit
qc.draw()
# Use Aer's qasm_simulator
backend_sim = Aer.get_backend('qasm_simulator')
# Execute the circuit on the qasm simulator.
# We've set the number of repeats of the circuit
# to be 1024, which is the default.
job_sim = backend_sim.run(transpile(qc, backend_sim), shots=1024)
# Grab the results from the job.
result_sim = job_sim.result()
counts = result_sim.get_counts(qc)
print(counts)
from qiskit.visualization import plot_histogram
plot_histogram(counts)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import *
from qiskit.visualization import plot_histogram
# quantum circuit to make a Bell state
bell = QuantumCircuit(2, 2)
bell.h(0)
bell.cx(0, 1)
meas = QuantumCircuit(2, 2)
meas.measure([0,1], [0,1])
# execute the quantum circuit
backend = BasicAer.get_backend('qasm_simulator') # the device to run on
circ = bell.compose(meas)
result = backend.run(transpile(circ, backend), shots=1000).result()
counts = result.get_counts(circ)
print(counts)
plot_histogram(counts)
# Execute 2-qubit Bell state again
second_result = backend.run(transpile(circ, backend), shots=1000).result()
second_counts = second_result.get_counts(circ)
# Plot results with legend
legend = ['First execution', 'Second execution']
plot_histogram([counts, second_counts], legend=legend)
plot_histogram([counts, second_counts], legend=legend, sort='desc', figsize=(15,12),
color=['orange', 'black'], bar_labels=False)
from qiskit.visualization import plot_state_city, plot_bloch_multivector
from qiskit.visualization import plot_state_paulivec, plot_state_hinton
from qiskit.visualization import plot_state_qsphere
# execute the quantum circuit
backend = BasicAer.get_backend('statevector_simulator') # the device to run on
result = backend.run(transpile(bell, backend)).result()
psi = result.get_statevector(bell)
plot_state_city(psi)
plot_state_hinton(psi)
plot_state_qsphere(psi)
plot_state_paulivec(psi)
plot_bloch_multivector(psi)
plot_state_city(psi, title="My City", color=['black', 'orange'])
plot_state_hinton(psi, title="My Hinton")
plot_state_paulivec(psi, title="My Paulivec", color=['purple', 'orange', 'green'])
plot_bloch_multivector(psi, title="My Bloch Spheres")
from qiskit.visualization import plot_bloch_vector
plot_bloch_vector([0,1,0])
plot_bloch_vector([0,1,0], title='My Bloch Sphere')
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
# Useful additional packages
import matplotlib.pyplot as plt
import numpy as np
from math import pi
from qiskit import QuantumCircuit, ClassicalRegister, QuantumRegister, transpile
from qiskit.tools.visualization import circuit_drawer
from qiskit.quantum_info import state_fidelity
from qiskit import BasicAer
backend = BasicAer.get_backend('unitary_simulator')
q = QuantumRegister(1)
qc = QuantumCircuit(q)
qc.u(pi/2,pi/4,pi/8,q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.p(pi/2,q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.id(q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.x(q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.y(q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.z(q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.h(q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.s(q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.sdg(q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.t(q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.tdg(q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.rx(pi/2,q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.ry(pi/2,q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.rz(pi/2,q)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
q = QuantumRegister(2)
qc = QuantumCircuit(q)
qc.cx(q[0],q[1])
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.cy(q[0],q[1])
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.cz(q[0],q[1])
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.ch(q[0],q[1])
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.crz(pi/2,q[0],q[1])
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.cp(pi/2,q[0], q[1])
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.cu(pi/2, pi/2, pi/2, 0, q[0], q[1])
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.swap(q[0], q[1])
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
q = QuantumRegister(3)
qc = QuantumCircuit(q)
qc.ccx(q[0], q[1], q[2])
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
qc = QuantumCircuit(q)
qc.cswap(q[0], q[1], q[2])
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_unitary(qc, decimals=3)
q = QuantumRegister(1)
c = ClassicalRegister(1)
qc = QuantumCircuit(q, c)
qc.measure(q, c)
qc.draw()
backend = BasicAer.get_backend('qasm_simulator')
job = backend.run(transpile(qc, backend))
job.result().get_counts(qc)
qc = QuantumCircuit(q, c)
qc.h(q)
qc.measure(q, c)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_counts(qc)
qc = QuantumCircuit(q, c)
qc.reset(q[0])
qc.measure(q, c)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_counts(qc)
qc = QuantumCircuit(q, c)
qc.h(q)
qc.reset(q[0])
qc.measure(q, c)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_counts(qc)
qc = QuantumCircuit(q, c)
qc.x(q[0]).c_if(c, 0)
qc.measure(q,c)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_counts(qc)
qc = QuantumCircuit(q, c)
qc.h(q)
qc.measure(q,c)
qc.x(q[0]).c_if(c, 0)
qc.measure(q,c)
qc.draw()
job = backend.run(transpile(qc, backend))
job.result().get_counts(qc)
# Initializing a three-qubit quantum state
import math
desired_vector = [
1 / math.sqrt(16) * complex(0, 1),
1 / math.sqrt(8) * complex(1, 0),
1 / math.sqrt(16) * complex(1, 1),
0,
0,
1 / math.sqrt(8) * complex(1, 2),
1 / math.sqrt(16) * complex(1, 0),
0]
q = QuantumRegister(3)
qc = QuantumCircuit(q)
qc.initialize(desired_vector, [q[0],q[1],q[2]])
qc.draw()
backend = BasicAer.get_backend('statevector_simulator')
job = backend.run(transpile(qc, backend))
qc_state = job.result().get_statevector(qc)
qc_state
state_fidelity(desired_vector,qc_state)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
import numpy as np
from qiskit import *
from qiskit.circuit import Gate
my_gate = Gate(name='my_gate', num_qubits=2, params=[])
qr = QuantumRegister(3, 'q')
circ = QuantumCircuit(qr)
circ.append(my_gate, [qr[0], qr[1]])
circ.append(my_gate, [qr[1], qr[2]])
circ.draw()
# Build a sub-circuit
sub_q = QuantumRegister(2)
sub_circ = QuantumCircuit(sub_q, name='sub_circ')
sub_circ.h(sub_q[0])
sub_circ.crz(1, sub_q[0], sub_q[1])
sub_circ.barrier()
sub_circ.id(sub_q[1])
sub_circ.u(1, 2, -2, sub_q[0])
# Convert to a gate and stick it into an arbitrary place in the bigger circuit
sub_inst = sub_circ.to_instruction()
qr = QuantumRegister(3, 'q')
circ = QuantumCircuit(qr)
circ.h(qr[0])
circ.cx(qr[0], qr[1])
circ.cx(qr[1], qr[2])
circ.append(sub_inst, [qr[1], qr[2]])
circ.draw()
decomposed_circ = circ.decompose() # Does not modify original circuit
decomposed_circ.draw()
from qiskit.circuit import Parameter
theta = Parameter('θ')
n = 5
qc = QuantumCircuit(5, 1)
qc.h(0)
for i in range(n-1):
qc.cx(i, i+1)
qc.barrier()
qc.rz(theta, range(5))
qc.barrier()
for i in reversed(range(n-1)):
qc.cx(i, i+1)
qc.h(0)
qc.measure(0, 0)
qc.draw('mpl')
print(qc.parameters)
import numpy as np
theta_range = np.linspace(0, 2 * np.pi, 128)
circuits = [qc.bind_parameters({theta: theta_val})
for theta_val in theta_range]
circuits[-1].draw()
backend = BasicAer.get_backend('qasm_simulator')
job = backend.run(transpile(circuits, backend))
counts = job.result().get_counts()
import matplotlib.pyplot as plt
fig = plt.figure(figsize=(8,6))
ax = fig.add_subplot(111)
ax.plot(theta_range, list(map(lambda c: c.get('0', 0), counts)), '.-', label='0')
ax.plot(theta_range, list(map(lambda c: c.get('1', 0), counts)), '.-', label='1')
ax.set_xticks([i * np.pi / 2 for i in range(5)])
ax.set_xticklabels(['0', r'$\frac{\pi}{2}$', r'$\pi$', r'$\frac{3\pi}{2}$', r'$2\pi$'], fontsize=14)
ax.set_xlabel('θ', fontsize=14)
ax.set_ylabel('Counts', fontsize=14)
ax.legend(fontsize=14)
import time
from itertools import combinations
from qiskit.compiler import assemble
from qiskit.test.mock import FakeVigo
start = time.time()
qcs = []
theta_range = np.linspace(0, 2*np.pi, 32)
for n in theta_range:
qc = QuantumCircuit(5)
for k in range(8):
for i,j in combinations(range(5), 2):
qc.cx(i,j)
qc.rz(n, range(5))
for i,j in combinations(range(5), 2):
qc.cx(i,j)
qcs.append(qc)
compiled_circuits = transpile(qcs, backend=FakeVigo())
qobj = assemble(compiled_circuits, backend=FakeVigo())
end = time.time()
print('Time compiling over set of bound circuits: ', end-start)
start = time.time()
qc = QuantumCircuit(5)
theta = Parameter('theta')
for k in range(8):
for i,j in combinations(range(5), 2):
qc.cx(i,j)
qc.rz(theta, range(5))
for i,j in combinations(range(5), 2):
qc.cx(i,j)
transpiled_qc = transpile(qc, backend=FakeVigo())
qobj = assemble([transpiled_qc.bind_parameters({theta: n})
for n in theta_range], backend=FakeVigo())
end = time.time()
print('Time compiling over parameterized circuit, then binding: ', end-start)
phi = Parameter('phi')
sub_circ1 = QuantumCircuit(2, name='sc_1')
sub_circ1.rz(phi, 0)
sub_circ1.rx(phi, 1)
sub_circ2 = QuantumCircuit(2, name='sc_2')
sub_circ2.rx(phi, 0)
sub_circ2.rz(phi, 1)
qc = QuantumCircuit(4)
qr = qc.qregs[0]
qc.append(sub_circ1.to_instruction(), [qr[0], qr[1]])
qc.append(sub_circ2.to_instruction(), [qr[0], qr[1]])
qc.append(sub_circ2.to_instruction(), [qr[2], qr[3]])
print(qc.draw())
# The following raises an error: "QiskitError: 'Name conflict on adding parameter: phi'"
# phi2 = Parameter('phi')
# qc.u3(0.1, phi2, 0.3, 0)
p = Parameter('p')
qc = QuantumCircuit(3, name='oracle')
qc.rz(p, 0)
qc.cx(0, 1)
qc.rz(p, 1)
qc.cx(1, 2)
qc.rz(p, 2)
theta = Parameter('theta')
phi = Parameter('phi')
gamma = Parameter('gamma')
qr = QuantumRegister(9)
larger_qc = QuantumCircuit(qr)
larger_qc.append(qc.to_instruction({p: theta}), qr[0:3])
larger_qc.append(qc.to_instruction({p: phi}), qr[3:6])
larger_qc.append(qc.to_instruction({p: gamma}), qr[6:9])
print(larger_qc.draw())
print(larger_qc.decompose().draw())
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
import numpy as np
from qiskit import QuantumCircuit, ClassicalRegister, QuantumRegister
from qiskit import BasicAer
from qiskit.compiler import transpile
from qiskit.quantum_info.operators import Operator, Pauli
from qiskit.quantum_info import process_fidelity
from qiskit.extensions import RXGate, XGate, CXGate
XX = Operator([[0, 0, 0, 1], [0, 0, 1, 0], [0, 1, 0, 0], [1, 0, 0, 0]])
XX
XX.data
input_dim, output_dim = XX.dim
input_dim, output_dim
op = Operator(np.random.rand(2 ** 1, 2 ** 2))
print('Input dimensions:', op.input_dims())
print('Output dimensions:', op.output_dims())
op = Operator(np.random.rand(6, 6))
print('Input dimensions:', op.input_dims())
print('Output dimensions:', op.output_dims())
# Force input dimension to be (4,) rather than (2, 2)
op = Operator(np.random.rand(2 ** 1, 2 ** 2), input_dims=[4])
print('Input dimensions:', op.input_dims())
print('Output dimensions:', op.output_dims())
# Specify system is a qubit and qutrit
op = Operator(np.random.rand(6, 6),
input_dims=[2, 3], output_dims=[2, 3])
print('Input dimensions:', op.input_dims())
print('Output dimensions:', op.output_dims())
print('Dimension of input system 0:', op.input_dims([0]))
print('Dimension of input system 1:', op.input_dims([1]))
# Create an Operator from a Pauli object
pauliXX = Pauli('XX')
Operator(pauliXX)
# Create an Operator for a Gate object
Operator(CXGate())
# Create an operator from a parameterized Gate object
Operator(RXGate(np.pi / 2))
# Create an operator from a QuantumCircuit object
circ = QuantumCircuit(10)
circ.h(0)
for j in range(1, 10):
circ.cx(j-1, j)
# Convert circuit to an operator by implicit unitary simulation
Operator(circ)
# Create an operator
XX = Operator(Pauli('XX'))
# Add to a circuit
circ = QuantumCircuit(2, 2)
circ.append(XX, [0, 1])
circ.measure([0,1], [0,1])
circ.draw('mpl')
backend = BasicAer.get_backend('qasm_simulator')
circ = transpile(circ, backend, basis_gates=['u1','u2','u3','cx'])
job = backend.run(circ)
job.result().get_counts(0)
# Add to a circuit
circ2 = QuantumCircuit(2, 2)
circ2.append(Pauli('XX'), [0, 1])
circ2.measure([0,1], [0,1])
circ2.draw()
A = Operator(Pauli('X'))
B = Operator(Pauli('Z'))
A.tensor(B)
A = Operator(Pauli('X'))
B = Operator(Pauli('Z'))
A.expand(B)
A = Operator(Pauli('X'))
B = Operator(Pauli('Z'))
A.compose(B)
A = Operator(Pauli('X'))
B = Operator(Pauli('Z'))
A.compose(B, front=True)
# Compose XZ with an 3-qubit identity operator
op = Operator(np.eye(2 ** 3))
XZ = Operator(Pauli('XZ'))
op.compose(XZ, qargs=[0, 2])
# Compose YX in front of the previous operator
op = Operator(np.eye(2 ** 3))
YX = Operator(Pauli('YX'))
op.compose(XZ, qargs=[0, 2], front=True)
XX = Operator(Pauli('XX'))
YY = Operator(Pauli('YY'))
ZZ = Operator(Pauli('ZZ'))
op = 0.5 * (XX + YY - 3 * ZZ)
op
op.is_unitary()
# Compose with a matrix passed as a list
Operator(np.eye(2)).compose([[0, 1], [1, 0]])
Operator(Pauli('X')) == Operator(XGate())
Operator(XGate()) == np.exp(1j * 0.5) * Operator(XGate())
# Two operators which differ only by phase
op_a = Operator(XGate())
op_b = np.exp(1j * 0.5) * Operator(XGate())
# Compute process fidelity
F = process_fidelity(op_a, op_b)
print('Process fidelity =', F)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, ClassicalRegister, QuantumRegister
# Build a quantum circuit
circuit = QuantumCircuit(3, 3)
circuit.x(1)
circuit.h(range(3))
circuit.cx(0, 1)
circuit.measure(range(3), range(3));
print(circuit)
circuit.draw()
# Matplotlib Drawing
circuit.draw(output='mpl')
# Draw a new circuit with barriers and more registers
q_a = QuantumRegister(3, name='qa')
q_b = QuantumRegister(5, name='qb')
c_a = ClassicalRegister(3)
c_b = ClassicalRegister(5)
circuit = QuantumCircuit(q_a, q_b, c_a, c_b)
circuit.x(q_a[1])
circuit.x(q_b[1])
circuit.x(q_b[2])
circuit.x(q_b[4])
circuit.barrier()
circuit.h(q_a)
circuit.barrier(q_a)
circuit.h(q_b)
circuit.cswap(q_b[0], q_b[1], q_b[2])
circuit.cswap(q_b[2], q_b[3], q_b[4])
circuit.cswap(q_b[3], q_b[4], q_b[0])
circuit.barrier(q_b)
circuit.measure(q_a, c_a)
circuit.measure(q_b, c_b);
# Draw the circuit
circuit.draw(output='mpl')
# Draw the circuit with reversed bit order
circuit.draw(output='mpl', reverse_bits=True)
# Draw the circuit without barriers
circuit.draw(output='mpl', plot_barriers=False)
# Draw the circuit without barriers and reverse bit order
circuit.draw(output='mpl', plot_barriers=False, reverse_bits=True)
# Set line length to 80 for above circuit
circuit.draw(output='text')
# Change the background color in mpl
style = {'backgroundcolor': 'lightgreen'}
circuit.draw(output='mpl', style=style)
# Scale the mpl output to 1/2 the normal size
circuit.draw(output='mpl', scale=0.5)
from qiskit.tools.visualization import circuit_drawer
circuit_drawer(circuit, output='mpl', plot_barriers=False)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.compiler import transpile
from qiskit.transpiler import PassManager
circ = QuantumCircuit(3)
circ.ccx(0, 1, 2)
circ.draw(output='mpl')
from qiskit.transpiler.passes import Unroller
pass_ = Unroller(['u1', 'u2', 'u3', 'cx'])
pm = PassManager(pass_)
new_circ = pm.run(circ)
new_circ.draw(output='mpl')
from qiskit.transpiler import passes
[pass_ for pass_ in dir(passes) if pass_[0].isupper()]
from qiskit.transpiler import CouplingMap, Layout
from qiskit.transpiler.passes import BasicSwap, LookaheadSwap, StochasticSwap
coupling = [[0, 1], [1, 2], [2, 3], [3, 4], [4, 5], [5, 6]]
circuit = QuantumCircuit(7)
circuit.h(3)
circuit.cx(0, 6)
circuit.cx(6, 0)
circuit.cx(0, 1)
circuit.cx(3, 1)
circuit.cx(3, 0)
coupling_map = CouplingMap(couplinglist=coupling)
bs = BasicSwap(coupling_map=coupling_map)
pass_manager = PassManager(bs)
basic_circ = pass_manager.run(circuit)
ls = LookaheadSwap(coupling_map=coupling_map)
pass_manager = PassManager(ls)
lookahead_circ = pass_manager.run(circuit)
ss = StochasticSwap(coupling_map=coupling_map)
pass_manager = PassManager(ss)
stochastic_circ = pass_manager.run(circuit)
circuit.draw(output='mpl')
basic_circ.draw(output='mpl')
lookahead_circ.draw(output='mpl')
stochastic_circ.draw(output='mpl')
import math
from qiskit.providers.fake_provider import FakeTokyo
backend = FakeTokyo() # mimics the tokyo device in terms of coupling map and basis gates
qc = QuantumCircuit(10)
random_state = [
1 / math.sqrt(4) * complex(0, 1),
1 / math.sqrt(8) * complex(1, 0),
0,
0,
0,
0,
0,
0,
1 / math.sqrt(8) * complex(1, 0),
1 / math.sqrt(8) * complex(0, 1),
0,
0,
0,
0,
1 / math.sqrt(4) * complex(1, 0),
1 / math.sqrt(8) * complex(1, 0)]
qc.initialize(random_state, range(4))
qc.draw()
optimized_0 = transpile(qc, backend=backend, seed_transpiler=11, optimization_level=0)
print('gates = ', optimized_0.count_ops())
print('depth = ', optimized_0.depth())
optimized_1 = transpile(qc, backend=backend, seed_transpiler=11, optimization_level=1)
print('gates = ', optimized_1.count_ops())
print('depth = ', optimized_1.depth())
optimized_2 = transpile(qc, backend=backend, seed_transpiler=11, optimization_level=2)
print('gates = ', optimized_2.count_ops())
print('depth = ', optimized_2.depth())
optimized_3 = transpile(qc, backend=backend, seed_transpiler=11, optimization_level=3)
print('gates = ', optimized_3.count_ops())
print('depth = ', optimized_3.depth())
from qiskit import QuantumRegister, ClassicalRegister, QuantumCircuit
from qiskit.dagcircuit import DAGCircuit
q = QuantumRegister(3, 'q')
c = ClassicalRegister(3, 'c')
circ = QuantumCircuit(q, c)
circ.h(q[0])
circ.cx(q[0], q[1])
circ.measure(q[0], c[0])
circ.rz(0.5, q[1]).c_if(c, 2)
circ.draw(output='mpl')
from qiskit.converters import circuit_to_dag
from qiskit.tools.visualization import dag_drawer
dag = circuit_to_dag(circ)
dag_drawer(dag)
dag.op_nodes()
node = dag.op_nodes()[3]
print("node name: ", node.name)
print("node op: ", node.op)
print("node qargs: ", node.qargs)
print("node cargs: ", node.cargs)
print("node condition: ", node.op.condition)
from qiskit.circuit.library import HGate
dag.apply_operation_back(HGate(), qargs=[q[0]])
dag_drawer(dag)
from qiskit.circuit.library import CCXGate
dag.apply_operation_front(CCXGate(), qargs=[q[0], q[1], q[2]], cargs=[])
dag_drawer(dag)
from qiskit.circuit.library import CHGate, U2Gate, CXGate
mini_dag = DAGCircuit()
p = QuantumRegister(2, "p")
mini_dag.add_qreg(p)
mini_dag.apply_operation_back(CHGate(), qargs=[p[1], p[0]])
mini_dag.apply_operation_back(U2Gate(0.1, 0.2), qargs=[p[1]])
# substitute the cx node with the above mini-dag
cx_node = dag.op_nodes(op=CXGate).pop()
dag.substitute_node_with_dag(node=cx_node, input_dag=mini_dag, wires=[p[0], p[1]])
dag_drawer(dag)
from qiskit.converters import dag_to_circuit
circuit = dag_to_circuit(dag)
circuit.draw(output='mpl')
from copy import copy
from qiskit.transpiler.basepasses import TransformationPass
from qiskit.transpiler import Layout
from qiskit.circuit.library import SwapGate
class BasicSwap(TransformationPass):
"""Maps (with minimum effort) a DAGCircuit onto a `coupling_map` adding swap gates."""
def __init__(self,
coupling_map,
initial_layout=None):
"""Maps a DAGCircuit onto a `coupling_map` using swap gates.
Args:
coupling_map (CouplingMap): Directed graph represented a coupling map.
initial_layout (Layout): initial layout of qubits in mapping
"""
super().__init__()
self.coupling_map = coupling_map
self.initial_layout = initial_layout
def run(self, dag):
"""Runs the BasicSwap pass on `dag`.
Args:
dag (DAGCircuit): DAG to map.
Returns:
DAGCircuit: A mapped DAG.
Raises:
TranspilerError: if the coupling map or the layout are not
compatible with the DAG.
"""
new_dag = DAGCircuit()
for qreg in dag.qregs.values():
new_dag.add_qreg(qreg)
for creg in dag.cregs.values():
new_dag.add_creg(creg)
if self.initial_layout is None:
if self.property_set["layout"]:
self.initial_layout = self.property_set["layout"]
else:
self.initial_layout = Layout.generate_trivial_layout(*dag.qregs.values())
if len(dag.qubits) != len(self.initial_layout):
raise TranspilerError('The layout does not match the amount of qubits in the DAG')
if len(self.coupling_map.physical_qubits) != len(self.initial_layout):
raise TranspilerError(
"Mappers require to have the layout to be the same size as the coupling map")
canonical_register = dag.qregs['q']
trivial_layout = Layout.generate_trivial_layout(canonical_register)
current_layout = trivial_layout.copy()
for layer in dag.serial_layers():
subdag = layer['graph']
for gate in subdag.two_qubit_ops():
physical_q0 = current_layout[gate.qargs[0]]
physical_q1 = current_layout[gate.qargs[1]]
if self.coupling_map.distance(physical_q0, physical_q1) != 1:
# Insert a new layer with the SWAP(s).
swap_layer = DAGCircuit()
swap_layer.add_qreg(canonical_register)
path = self.coupling_map.shortest_undirected_path(physical_q0, physical_q1)
for swap in range(len(path) - 2):
connected_wire_1 = path[swap]
connected_wire_2 = path[swap + 1]
qubit_1 = current_layout[connected_wire_1]
qubit_2 = current_layout[connected_wire_2]
# create the swap operation
swap_layer.apply_operation_back(SwapGate(),
qargs=[qubit_1, qubit_2],
cargs=[])
# layer insertion
order = current_layout.reorder_bits(new_dag.qubits)
new_dag.compose(swap_layer, qubits=order)
# update current_layout
for swap in range(len(path) - 2):
current_layout.swap(path[swap], path[swap + 1])
order = current_layout.reorder_bits(new_dag.qubits)
new_dag.compose(subdag, qubits=order)
return new_dag
q = QuantumRegister(7, 'q')
in_circ = QuantumCircuit(q)
in_circ.h(q[0])
in_circ.cx(q[0], q[4])
in_circ.cx(q[2], q[3])
in_circ.cx(q[6], q[1])
in_circ.cx(q[5], q[0])
in_circ.rz(0.1, q[2])
in_circ.cx(q[5], q[0])
from qiskit.transpiler import PassManager
from qiskit.transpiler import CouplingMap
from qiskit import BasicAer
pm = PassManager()
coupling = [[0, 1], [1, 2], [2, 3], [3, 4], [4, 5], [5, 6]]
coupling_map = CouplingMap(couplinglist=coupling)
pm.append([BasicSwap(coupling_map)])
out_circ = pm.run(in_circ)
in_circ.draw(output='mpl')
out_circ.draw(output='mpl')
import logging
logging.basicConfig(level='DEBUG')
from qiskit.providers.fake_provider import FakeTenerife
log_circ = QuantumCircuit(2, 2)
log_circ.h(0)
log_circ.h(1)
log_circ.h(1)
log_circ.x(1)
log_circ.cx(0, 1)
log_circ.measure([0,1], [0,1])
backend = FakeTenerife()
transpile(log_circ, backend);
logging.getLogger('qiskit.transpiler').setLevel('INFO')
transpile(log_circ, backend);
# Change log level back to DEBUG
logging.getLogger('qiskit.transpiler').setLevel('DEBUG')
# Transpile multiple circuits
circuits = [log_circ, log_circ]
transpile(circuits, backend);
formatter = logging.Formatter('%(name)s - %(processName)-10s - %(levelname)s: %(message)s')
handler = logging.getLogger().handlers[0]
handler.setFormatter(formatter)
transpile(circuits, backend);
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
circ = QuantumCircuit(2, 2)
circ.h(0)
circ.cx(0, 1)
circ.measure(0, 0)
circ.measure(1, 1)
circ.draw('mpl')
from qiskit import pulse
from qiskit.pulse.library import Gaussian
from qiskit.providers.fake_provider import FakeValencia
backend = FakeValencia()
with pulse.build(backend, name='hadamard') as h_q0:
pulse.play(Gaussian(duration=128, amp=0.1, sigma=16), pulse.drive_channel(0))
h_q0.draw()
circ.add_calibration('h', [0], h_q0)
from qiskit import transpile
from qiskit.providers.fake_provider import FakeHanoi
backend = FakeHanoi()
circ = transpile(circ, backend)
print(backend.configuration().basis_gates)
circ.draw('mpl', idle_wires=False)
from qiskit import QuantumCircuit
from qiskit.circuit import Gate
circ = QuantumCircuit(1, 1)
custom_gate = Gate('my_custom_gate', 1, [3.14, 1])
# 3.14 is an arbitrary parameter for demonstration
circ.append(custom_gate, [0])
circ.measure(0, 0)
circ.draw('mpl')
with pulse.build(backend, name='custom') as my_schedule:
pulse.play(Gaussian(duration=64, amp=0.2, sigma=8), pulse.drive_channel(0))
circ.add_calibration('my_custom_gate', [0], my_schedule, [3.14, 1])
# Alternatively: circ.add_calibration(custom_gate, [0], my_schedule)
circ = transpile(circ, backend)
circ.draw('mpl', idle_wires=False)
circ = QuantumCircuit(2, 2)
circ.append(custom_gate, [1])
from qiskit import QiskitError
try:
circ = transpile(circ, backend)
except QiskitError as e:
print(e)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import pulse
with pulse.build(name='my_example') as my_program:
# Add instructions here
pass
my_program
from qiskit.pulse import DriveChannel
channel = DriveChannel(0)
from qiskit.providers.fake_provider import FakeValencia
backend = FakeValencia()
with pulse.build(backend=backend, name='backend_aware') as backend_aware_program:
channel = pulse.drive_channel(0)
print(pulse.num_qubits())
# Raises an error as backend only has 5 qubits
#pulse.drive_channel(100)
with pulse.build(backend) as delay_5dt:
pulse.delay(5, channel)
from qiskit.pulse import library
amp = 1
sigma = 10
num_samples = 128
gaus = pulse.library.Gaussian(num_samples, amp, sigma,
name="Parametric Gaus")
gaus.draw()
import numpy as np
times = np.arange(num_samples)
gaussian_samples = np.exp(-1/2 *((times - num_samples / 2) ** 2 / sigma**2))
gaus = library.Waveform(gaussian_samples, name="WF Gaus")
gaus.draw()
gaus = library.gaussian(duration=num_samples, amp=amp, sigma=sigma, name="Lib Gaus")
gaus.draw()
with pulse.build() as schedule:
pulse.play(gaus, channel)
schedule.draw()
with pulse.build() as schedule:
pulse.play([0.001*i for i in range(160)], channel)
schedule.draw()
with pulse.build(backend) as schedule:
pulse.set_frequency(4.5e9, channel)
with pulse.build(backend) as schedule:
pulse.shift_phase(np.pi, channel)
from qiskit.pulse import Acquire, AcquireChannel, MemorySlot
with pulse.build(backend) as schedule:
pulse.acquire(1200, pulse.acquire_channel(0), MemorySlot(0))
with pulse.build(backend, name='Left align example') as program:
with pulse.align_left():
gaussian_pulse = library.gaussian(100, 0.5, 20)
pulse.play(gaussian_pulse, pulse.drive_channel(0))
pulse.play(gaussian_pulse, pulse.drive_channel(1))
pulse.play(gaussian_pulse, pulse.drive_channel(1))
program.draw()
with pulse.build(backend, name='Right align example') as program:
with pulse.align_right():
gaussian_pulse = library.gaussian(100, 0.5, 20)
pulse.play(gaussian_pulse, pulse.drive_channel(0))
pulse.play(gaussian_pulse, pulse.drive_channel(1))
pulse.play(gaussian_pulse, pulse.drive_channel(1))
program.draw()
with pulse.build(backend, name='example') as program:
gaussian_pulse = library.gaussian(100, 0.5, 20)
with pulse.align_equispaced(2*gaussian_pulse.duration):
pulse.play(gaussian_pulse, pulse.drive_channel(0))
pulse.play(gaussian_pulse, pulse.drive_channel(1))
pulse.play(gaussian_pulse, pulse.drive_channel(1))
program.draw()
with pulse.build(backend, name='example') as program:
with pulse.align_sequential():
gaussian_pulse = library.gaussian(100, 0.5, 20)
pulse.play(gaussian_pulse, pulse.drive_channel(0))
pulse.play(gaussian_pulse, pulse.drive_channel(1))
pulse.play(gaussian_pulse, pulse.drive_channel(1))
program.draw()
with pulse.build(backend, name='Offset example') as program:
with pulse.phase_offset(3.14, pulse.drive_channel(0)):
pulse.play(gaussian_pulse, pulse.drive_channel(0))
with pulse.frequency_offset(10e6, pulse.drive_channel(0)):
pulse.play(gaussian_pulse, pulse.drive_channel(0))
program.draw()
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
circ = QuantumCircuit(2, 2)
circ.h(0)
circ.cx(0, 1)
circ.measure([0, 1], [0, 1])
circ.draw("mpl")
from qiskit import transpile, schedule as build_schedule
from qiskit.providers.fake_provider import FakeHanoi
backend = FakeHanoi()
transpiled_circ = transpile(circ, backend) # Undefined Hadamard is replaced by U1
schedule = build_schedule(transpiled_circ, backend)
schedule.draw()
from qiskit import pulse
with pulse.build() as h_q0:
pulse.play(pulse.library.Gaussian(duration=256, amp=0.2, sigma=50, name='custom'),
pulse.DriveChannel(0))
circ.add_calibration('h', [0], h_q0)
schedule = build_schedule(circ, backend)
schedule.draw()
circ = QuantumCircuit(2, 2)
circ.x(0)
circ.x(0)
circ.x(1)
circ.measure([0, 1], [0, 1])
circ.draw("mpl")
schedule = build_schedule(circ, backend, method="as_late_as_possible")
schedule.filter(channels=[pulse.DriveChannel(0), pulse.DriveChannel(1)]).draw()
schedule = build_schedule(circ, backend, method="as_soon_as_possible")
schedule.filter(channels=[pulse.DriveChannel(0), pulse.DriveChannel(1)]).draw()
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit.providers.fake_provider import FakeHanoi
backend = FakeHanoi()
config = backend.configuration()
# Basic Features
print("This backend is called {0}, and is on version {1}. It has {2} qubit{3}. It "
"{4} OpenPulse programs. The basis gates supported on this device are {5}."
"".format(config.backend_name,
config.backend_version,
config.n_qubits,
'' if config.n_qubits == 1 else 's',
'supports' if config.open_pulse else 'does not support',
config.basis_gates))
config.dt # units of seconds
config.meas_levels
config.dtm
config.meas_map
config.drive(0)
config.measure(0)
config.acquire(0)
props = backend.properties()
def describe_qubit(qubit, properties):
"""Print a string describing some of reported properties of the given qubit."""
# Conversion factors from standard SI units
us = 1e6
ns = 1e9
GHz = 1e-9
print("Qubit {0} has a \n"
" - T1 time of {1} microseconds\n"
" - T2 time of {2} microseconds\n"
" - U2 gate error of {3}\n"
" - U2 gate duration of {4} nanoseconds\n"
" - resonant frequency of {5} GHz".format(
qubit,
properties.t1(qubit) * us,
properties.t2(qubit) * us,
properties.gate_error('sx', qubit),
properties.gate_length('sx', qubit) * ns,
properties.frequency(qubit) * GHz))
describe_qubit(0, props)
defaults = backend.defaults()
q0_freq = defaults.qubit_freq_est[0] # Hz
q0_meas_freq = defaults.meas_freq_est[0] # Hz
GHz = 1e-9
print("DriveChannel(0) defaults to a modulation frequency of {} GHz.".format(q0_freq * GHz))
print("MeasureChannel(0) defaults to a modulation frequency of {} GHz.".format(q0_meas_freq * GHz))
calibrations = defaults.instruction_schedule_map
print(calibrations)
measure_schedule = calibrations.get('measure', range(config.n_qubits))
measure_schedule.draw(backend=backend)
# You can use `has` to see if an operation is defined. Ex: Does qubit 3 have an x gate defined?
calibrations.has('x', 3)
# Some circuit operations take parameters. U1 takes a rotation angle:
calibrations.get('u1', 0, P0=3.1415)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit.opflow import I, X, Y, Z
print(I, X, Y, Z)
print(1.5 * I)
print(2.5 * X)
print(X + 2.0 * Y)
print(X^Y^Z)
print(X @ Y @ Z)
print((X + Y) @ (Y + Z))
print((X + Y) ^ (Y + Z))
(I, X)
2.0 * X^Y^Z
print(1.1 * ((1.2 * X)^(Y + (1.3 * Z))))
from qiskit.opflow import (StateFn, Zero, One, Plus, Minus, H,
DictStateFn, VectorStateFn, CircuitStateFn, OperatorStateFn)
print(Zero, One)
print(Plus, Minus)
print(Zero.eval('0'))
print(Zero.eval('1'))
print(One.eval('1'))
print(Plus.eval('0'))
print(Minus.eval('1'))
One.adjoint()
~One
(2.0 + 3.0j) * Zero
print(Zero + One)
import math
v_zero_one = (Zero + One) / math.sqrt(2)
print(v_zero_one)
print(Plus + Minus)
print(~One @ One)
(~One @ One).eval()
(~v_zero_one @ v_zero_one).eval()
(~Minus @ One).eval()
print((~One).compose(One))
(~One).eval(One)
print(Zero^Plus)
print((Zero^Plus).to_circuit_op())
print(600 * ((One^5) + (Zero^5)))
print((One^Zero)^3)
print(((Plus^Minus)^2).to_matrix_op())
print(((Plus^One)^2).to_circuit_op())
print(((Plus^One)^2).to_matrix_op().sample())
print(StateFn({'0':1}))
print(StateFn({'0':1}) == Zero)
print(StateFn([0,1,1,0]))
from qiskit.circuit.library import RealAmplitudes
print(StateFn(RealAmplitudes(2)))
from qiskit.opflow import X, Y, Z, I, CX, T, H, S, PrimitiveOp
X
print(X.eval('0'))
X.eval('0').eval('1')
print(CX)
print(CX.to_matrix().real) # The imaginary part vanishes.
CX.eval('01') # 01 is the one in decimal. We get the first column.
CX.eval('01').eval('11') # This returns element with (zero-based) index (1, 3)
print(X @ One)
(X @ One).eval()
X.eval(One)
print(((~One^2) @ (CX.eval('01'))).eval())
print(((H^5) @ ((CX^2)^I) @ (I^(CX^2)))**2)
print((((H^5) @ ((CX^2)^I) @ (I^(CX^2)))**2) @ (Minus^5))
print(((H^I^I)@(X^I^I)@Zero))
print(~One @ Minus)
from qiskit.opflow import ListOp
print((~ListOp([One, Zero]) @ ListOp([One, Zero])))
print((~ListOp([One, Zero]) @ ListOp([One, Zero])).reduce())
print(StateFn(Z).adjoint())
StateFn(Z).adjoint()
print(StateFn(Z).adjoint().eval(Zero))
print(StateFn(Z).adjoint().eval(One))
print(StateFn(Z).adjoint().eval(Plus))
import numpy as np
from qiskit.opflow import I, X, Y, Z, H, CX, Zero, ListOp, PauliExpectation, PauliTrotterEvolution, CircuitSampler, MatrixEvolution, Suzuki
from qiskit.circuit import Parameter
from qiskit import Aer
two_qubit_H2 = (-1.0523732 * I^I) + \
(0.39793742 * I^Z) + \
(-0.3979374 * Z^I) + \
(-0.0112801 * Z^Z) + \
(0.18093119 * X^X)
print(two_qubit_H2)
evo_time = Parameter('θ')
evolution_op = (evo_time*two_qubit_H2).exp_i()
print(evolution_op) # Note, EvolvedOps print as exponentiations
print(repr(evolution_op))
h2_measurement = StateFn(two_qubit_H2).adjoint()
print(h2_measurement)
bell = CX @ (I ^ H) @ Zero
print(bell)
evo_and_meas = h2_measurement @ evolution_op @ bell
print(evo_and_meas)
trotterized_op = PauliTrotterEvolution(trotter_mode=Suzuki(order=2, reps=1)).convert(evo_and_meas)
# We can also set trotter_mode='suzuki' or leave it empty to default to first order Trotterization.
print(trotterized_op)
bound = trotterized_op.bind_parameters({evo_time: .5})
bound[1].to_circuit().draw()
# Note that XX was the only non-diagonal measurement in our H2 Observable
print(PauliExpectation(group_paulis=False).convert(h2_measurement))
print(PauliExpectation().convert(h2_measurement))
diagonalized_meas_op = PauliExpectation().convert(trotterized_op)
print(diagonalized_meas_op)
evo_time_points = list(range(8))
h2_trotter_expectations = diagonalized_meas_op.bind_parameters({evo_time: evo_time_points})
h2_trotter_expectations.eval()
sampler = CircuitSampler(backend=Aer.get_backend('aer_simulator'))
# sampler.quantum_instance.run_config.shots = 1000
sampled_trotter_exp_op = sampler.convert(h2_trotter_expectations)
sampled_trotter_energies = sampled_trotter_exp_op.eval()
print('Sampled Trotterized energies:\n {}'.format(np.real(sampled_trotter_energies)))
print('Before:\n')
print(h2_trotter_expectations.reduce()[0][0])
print('\nAfter:\n')
print(sampled_trotter_exp_op[0][0])
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
#General imports
import numpy as np
#Operator Imports
from qiskit.opflow import Z, X, I, StateFn, CircuitStateFn, SummedOp
from qiskit.opflow.gradients import Gradient, NaturalGradient, QFI, Hessian
#Circuit imports
from qiskit.circuit import QuantumCircuit, QuantumRegister, Parameter, ParameterVector, ParameterExpression
from qiskit.circuit.library import EfficientSU2
# Instantiate the quantum state
a = Parameter('a')
b = Parameter('b')
q = QuantumRegister(1)
qc = QuantumCircuit(q)
qc.h(q)
qc.rz(a, q[0])
qc.rx(b, q[0])
# Instantiate the Hamiltonian observable
H = (2 * X) + Z
# Combine the Hamiltonian observable and the state
op = ~StateFn(H) @ CircuitStateFn(primitive=qc, coeff=1.)
# Print the operator corresponding to the expectation value
print(op)
params = [a, b]
# Define the values to be assigned to the parameters
value_dict = {a: np.pi / 4, b: np.pi}
# Convert the operator and the gradient target params into the respective operator
grad = Gradient().convert(operator = op, params = params)
# Print the operator corresponding to the Gradient
print(grad)
# Assign the parameters and evaluate the gradient
grad_result = grad.assign_parameters(value_dict).eval()
print('Gradient', grad_result)
# Define the Hamiltonian with fixed coefficients
H = 0.5 * X - 1 * Z
# Define the parameters w.r.t. we want to compute the gradients
params = [a, b]
# Define the values to be assigned to the parameters
value_dict = { a: np.pi / 4, b: np.pi}
# Combine the Hamiltonian observable and the state into an expectation value operator
op = ~StateFn(H) @ CircuitStateFn(primitive=qc, coeff=1.)
print(op)
# Convert the expectation value into an operator corresponding to the gradient w.r.t. the state parameters using
# the parameter shift method.
state_grad = Gradient(grad_method='param_shift').convert(operator=op, params=params)
# Print the operator corresponding to the gradient
print(state_grad)
# Assign the parameters and evaluate the gradient
state_grad_result = state_grad.assign_parameters(value_dict).eval()
print('State gradient computed with parameter shift', state_grad_result)
# Convert the expectation value into an operator corresponding to the gradient w.r.t. the state parameter using
# the linear combination of unitaries method.
state_grad = Gradient(grad_method='lin_comb').convert(operator=op, params=params)
# Print the operator corresponding to the gradient
print(state_grad)
# Assign the parameters and evaluate the gradient
state_grad_result = state_grad.assign_parameters(value_dict).eval()
print('State gradient computed with the linear combination method', state_grad_result)
# Convert the expectation value into an operator corresponding to the gradient w.r.t. the state parameter using
# the finite difference method.
state_grad = Gradient(grad_method='fin_diff').convert(operator=op, params=params)
# Print the operator corresponding to the gradient
print(state_grad)
# Assign the parameters and evaluate the gradient
state_grad_result = state_grad.assign_parameters(value_dict).eval()
print('State gradient computed with finite difference', state_grad_result)
# Besides the method to compute the circuit gradients resp. QFI, a regularization method can be chosen:
# `ridge` or `lasso` with automatic parameter search or `perturb_diag_elements` or `perturb_diag`
# which perturb the diagonal elements of the QFI.
nat_grad = NaturalGradient(grad_method='lin_comb', qfi_method='lin_comb_full', regularization='ridge').convert(
operator=op, params=params)
# Assign the parameters and evaluate the gradient
nat_grad_result = nat_grad.assign_parameters(value_dict).eval()
print('Natural gradient computed with linear combination of unitaries', nat_grad_result)
# Instantiate the Hamiltonian observable
H = X
# Instantiate the quantum state with two parameters
a = Parameter('a')
b = Parameter('b')
q = QuantumRegister(1)
qc = QuantumCircuit(q)
qc.h(q)
qc.rz(a, q[0])
qc.rx(b, q[0])
# Combine the Hamiltonian observable and the state
op = ~StateFn(H) @ CircuitStateFn(primitive=qc, coeff=1.)
# Convert the operator and the hessian target coefficients into the respective operator
hessian = Hessian().convert(operator = op, params = [a, b])
# Define the values to be assigned to the parameters
value_dict = {a: np.pi / 4, b: np.pi/4}
# Assign the parameters and evaluate the Hessian w.r.t. the Hamiltonian coefficients
hessian_result = hessian.assign_parameters(value_dict).eval()
print('Hessian \n', np.real(np.array(hessian_result)))
# Define parameters
params = [a, b]
# Get the operator object representing the Hessian
state_hess = Hessian(hess_method='param_shift').convert(operator=op, params=params)
# Assign the parameters and evaluate the Hessian
hessian_result = state_hess.assign_parameters(value_dict).eval()
print('Hessian computed using the parameter shift method\n', (np.array(hessian_result)))
# Get the operator object representing the Hessian
state_hess = Hessian(hess_method='lin_comb').convert(operator=op, params=params)
# Assign the parameters and evaluate the Hessian
hessian_result = state_hess.assign_parameters(value_dict).eval()
print('Hessian computed using the linear combination of unitaries method\n', (np.array(hessian_result)))
# Get the operator object representing the Hessian using finite difference
state_hess = Hessian(hess_method='fin_diff').convert(operator=op, params=params)
# Assign the parameters and evaluate the Hessian
hessian_result = state_hess.assign_parameters(value_dict).eval()
print('Hessian computed with finite difference\n', (np.array(hessian_result)))
# Wrap the quantum circuit into a CircuitStateFn
state = CircuitStateFn(primitive=qc, coeff=1.)
# Convert the state and the parameters into the operator object that represents the QFI
qfi = QFI(qfi_method='lin_comb_full').convert(operator=state, params=params)
# Define the values for which the QFI is to be computed
values_dict = {a: np.pi / 4, b: 0.1}
# Assign the parameters and evaluate the QFI
qfi_result = qfi.assign_parameters(values_dict).eval()
print('full QFI \n', np.real(np.array(qfi_result)))
# Convert the state and the parameters into the operator object that represents the QFI
# and set the approximation to 'block_diagonal'
qfi = QFI('overlap_block_diag').convert(operator=state, params=params)
# Assign the parameters and evaluate the QFI
qfi_result = qfi.assign_parameters(values_dict).eval()
print('Block-diagonal QFI \n', np.real(np.array(qfi_result)))
# Convert the state and the parameters into the operator object that represents the QFI
# and set the approximation to 'diagonal'
qfi = QFI('overlap_diag').convert(operator=state, params=params)
# Assign the parameters and evaluate the QFI
qfi_result = qfi.assign_parameters(values_dict).eval()
print('Diagonal QFI \n', np.real(np.array(qfi_result)))
# Execution Imports
from qiskit import Aer
from qiskit.utils import QuantumInstance
# Algorithm Imports
from qiskit.algorithms import VQE
from qiskit.algorithms.optimizers import CG
from qiskit.opflow import I, X, Z
from qiskit.circuit import QuantumCircuit, ParameterVector
from scipy.optimize import minimize
# Instantiate the system Hamiltonian
h2_hamiltonian = -1.05 * (I ^ I) + 0.39 * (I ^ Z) - 0.39 * (Z ^ I) - 0.01 * (Z ^ Z) + 0.18 * (X ^ X)
# This is the target energy
h2_energy = -1.85727503
# Define the Ansatz
wavefunction = QuantumCircuit(2)
params = ParameterVector('theta', length=8)
it = iter(params)
wavefunction.ry(next(it), 0)
wavefunction.ry(next(it), 1)
wavefunction.rz(next(it), 0)
wavefunction.rz(next(it), 1)
wavefunction.cx(0, 1)
wavefunction.ry(next(it), 0)
wavefunction.ry(next(it), 1)
wavefunction.rz(next(it), 0)
wavefunction.rz(next(it), 1)
# Define the expectation value corresponding to the energy
op = ~StateFn(h2_hamiltonian) @ StateFn(wavefunction)
grad = Gradient(grad_method='lin_comb')
qi_sv = QuantumInstance(Aer.get_backend('aer_simulator_statevector'),
shots=1,
seed_simulator=2,
seed_transpiler=2)
#Conjugate Gradient algorithm
optimizer = CG(maxiter=50)
# Gradient callable
vqe = VQE(wavefunction, optimizer=optimizer, gradient=grad, quantum_instance=qi_sv)
result = vqe.compute_minimum_eigenvalue(h2_hamiltonian)
print('Result:', result.optimal_value, 'Reference:', h2_energy)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
import numpy as np
# Import Qiskit
from qiskit import QuantumCircuit
from qiskit import Aer, transpile
from qiskit.tools.visualization import plot_histogram, plot_state_city
import qiskit.quantum_info as qi
Aer.backends()
simulator = Aer.get_backend('aer_simulator')
# Create circuit
circ = QuantumCircuit(2)
circ.h(0)
circ.cx(0, 1)
circ.measure_all()
# Transpile for simulator
simulator = Aer.get_backend('aer_simulator')
circ = transpile(circ, simulator)
# Run and get counts
result = simulator.run(circ).result()
counts = result.get_counts(circ)
plot_histogram(counts, title='Bell-State counts')
# Run and get memory
result = simulator.run(circ, shots=10, memory=True).result()
memory = result.get_memory(circ)
print(memory)
# Increase shots to reduce sampling variance
shots = 10000
# Stabilizer simulation method
sim_stabilizer = Aer.get_backend('aer_simulator_stabilizer')
job_stabilizer = sim_stabilizer.run(circ, shots=shots)
counts_stabilizer = job_stabilizer.result().get_counts(0)
# Statevector simulation method
sim_statevector = Aer.get_backend('aer_simulator_statevector')
job_statevector = sim_statevector.run(circ, shots=shots)
counts_statevector = job_statevector.result().get_counts(0)
# Density Matrix simulation method
sim_density = Aer.get_backend('aer_simulator_density_matrix')
job_density = sim_density.run(circ, shots=shots)
counts_density = job_density.result().get_counts(0)
# Matrix Product State simulation method
sim_mps = Aer.get_backend('aer_simulator_matrix_product_state')
job_mps = sim_mps.run(circ, shots=shots)
counts_mps = job_mps.result().get_counts(0)
plot_histogram([counts_stabilizer, counts_statevector, counts_density, counts_mps],
title='Counts for different simulation methods',
legend=['stabilizer', 'statevector',
'density_matrix', 'matrix_product_state'])
from qiskit_aer import AerError
# Initialize a GPU backend
# Note that the cloud instance for tutorials does not have a GPU
# so this will raise an exception.
try:
simulator_gpu = Aer.get_backend('aer_simulator')
simulator_gpu.set_options(device='GPU')
except AerError as e:
print(e)
# Configure a single-precision statevector simulator backend
simulator = Aer.get_backend('aer_simulator_statevector')
simulator.set_options(precision='single')
# Run and get counts
result = simulator.run(circ).result()
counts = result.get_counts(circ)
print(counts)
# Construct quantum circuit without measure
circ = QuantumCircuit(2)
circ.h(0)
circ.cx(0, 1)
circ.save_statevector()
# Transpile for simulator
simulator = Aer.get_backend('aer_simulator')
circ = transpile(circ, simulator)
# Run and get statevector
result = simulator.run(circ).result()
statevector = result.get_statevector(circ)
plot_state_city(statevector, title='Bell state')
# Construct quantum circuit without measure
circ = QuantumCircuit(2)
circ.h(0)
circ.cx(0, 1)
circ.save_unitary()
# Transpile for simulator
simulator = Aer.get_backend('aer_simulator')
circ = transpile(circ, simulator)
# Run and get unitary
result = simulator.run(circ).result()
unitary = result.get_unitary(circ)
print("Circuit unitary:\n", np.asarray(unitary).round(5))
# Construct quantum circuit without measure
steps = 5
circ = QuantumCircuit(1)
for i in range(steps):
circ.save_statevector(label=f'psi_{i}')
circ.rx(i * np.pi / steps, 0)
circ.save_statevector(label=f'psi_{steps}')
# Transpile for simulator
simulator = Aer.get_backend('aer_simulator')
circ = transpile(circ, simulator)
# Run and get saved data
result = simulator.run(circ).result()
data = result.data(0)
data
# Generate a random statevector
num_qubits = 2
psi = qi.random_statevector(2 ** num_qubits, seed=100)
# Set initial state to generated statevector
circ = QuantumCircuit(num_qubits)
circ.set_statevector(psi)
circ.save_state()
# Transpile for simulator
simulator = Aer.get_backend('aer_simulator')
circ = transpile(circ, simulator)
# Run and get saved data
result = simulator.run(circ).result()
result.data(0)
# Use initilize instruction to set initial state
circ = QuantumCircuit(num_qubits)
circ.initialize(psi, range(num_qubits))
circ.save_state()
# Transpile for simulator
simulator = Aer.get_backend('aer_simulator')
circ = transpile(circ, simulator)
# Run and get result data
result = simulator.run(circ).result()
result.data(0)
num_qubits = 2
rho = qi.random_density_matrix(2 ** num_qubits, seed=100)
circ = QuantumCircuit(num_qubits)
circ.set_density_matrix(rho)
circ.save_state()
# Transpile for simulator
simulator = Aer.get_backend('aer_simulator')
circ = transpile(circ, simulator)
# Run and get saved data
result = simulator.run(circ).result()
result.data(0)
# Generate a random Clifford C
num_qubits = 2
stab = qi.random_clifford(num_qubits, seed=100)
# Set initial state to stabilizer state C|0>
circ = QuantumCircuit(num_qubits)
circ.set_stabilizer(stab)
circ.save_state()
# Transpile for simulator
simulator = Aer.get_backend('aer_simulator')
circ = transpile(circ, simulator)
# Run and get saved data
result = simulator.run(circ).result()
result.data(0)
# Generate a random unitary
num_qubits = 2
unitary = qi.random_unitary(2 ** num_qubits, seed=100)
# Set initial state to unitary
circ = QuantumCircuit(num_qubits)
circ.set_unitary(unitary)
circ.save_state()
# Transpile for simulator
simulator = Aer.get_backend('aer_simulator')
circ = transpile(circ, simulator)
# Run and get saved data
result = simulator.run(circ).result()
result.data(0)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import IBMQ, transpile
from qiskit import QuantumCircuit
from qiskit_aer import AerSimulator
from qiskit.tools.visualization import plot_histogram
from qiskit.providers.fake_provider import FakeVigo
device_backend = FakeVigo()
# Construct quantum circuit
circ = QuantumCircuit(3, 3)
circ.h(0)
circ.cx(0, 1)
circ.cx(1, 2)
circ.measure([0, 1, 2], [0, 1, 2])
sim_ideal = AerSimulator()
# Execute and get counts
result = sim_ideal.run(transpile(circ, sim_ideal)).result()
counts = result.get_counts(0)
plot_histogram(counts, title='Ideal counts for 3-qubit GHZ state')
sim_vigo = AerSimulator.from_backend(device_backend)
# Transpile the circuit for the noisy basis gates
tcirc = transpile(circ, sim_vigo)
# Execute noisy simulation and get counts
result_noise = sim_vigo.run(tcirc).result()
counts_noise = result_noise.get_counts(0)
plot_histogram(counts_noise,
title="Counts for 3-qubit GHZ state with device noise model")
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
import numpy as np
from qiskit import QuantumCircuit, transpile
from qiskit.quantum_info import Kraus, SuperOp
from qiskit_aer import AerSimulator
from qiskit.tools.visualization import plot_histogram
# Import from Qiskit Aer noise module
from qiskit_aer.noise import (NoiseModel, QuantumError, ReadoutError,
pauli_error, depolarizing_error, thermal_relaxation_error)
# Construct a 1-qubit bit-flip and phase-flip errors
p_error = 0.05
bit_flip = pauli_error([('X', p_error), ('I', 1 - p_error)])
phase_flip = pauli_error([('Z', p_error), ('I', 1 - p_error)])
print(bit_flip)
print(phase_flip)
# Compose two bit-flip and phase-flip errors
bitphase_flip = bit_flip.compose(phase_flip)
print(bitphase_flip)
# Tensor product two bit-flip and phase-flip errors with
# bit-flip on qubit-0, phase-flip on qubit-1
error2 = phase_flip.tensor(bit_flip)
print(error2)
# Convert to Kraus operator
bit_flip_kraus = Kraus(bit_flip)
print(bit_flip_kraus)
# Convert to Superoperator
phase_flip_sop = SuperOp(phase_flip)
print(phase_flip_sop)
# Convert back to a quantum error
print(QuantumError(bit_flip_kraus))
# Check conversion is equivalent to original error
QuantumError(bit_flip_kraus) == bit_flip
# Measurement miss-assignement probabilities
p0given1 = 0.1
p1given0 = 0.05
ReadoutError([[1 - p1given0, p1given0], [p0given1, 1 - p0given1]])
# Create an empty noise model
noise_model = NoiseModel()
# Add depolarizing error to all single qubit u1, u2, u3 gates
error = depolarizing_error(0.05, 1)
noise_model.add_all_qubit_quantum_error(error, ['u1', 'u2', 'u3'])
# Print noise model info
print(noise_model)
# Create an empty noise model
noise_model = NoiseModel()
# Add depolarizing error to all single qubit u1, u2, u3 gates on qubit 0 only
error = depolarizing_error(0.05, 1)
noise_model.add_quantum_error(error, ['u1', 'u2', 'u3'], [0])
# Print noise model info
print(noise_model)
# System Specification
n_qubits = 4
circ = QuantumCircuit(n_qubits)
# Test Circuit
circ.h(0)
for qubit in range(n_qubits - 1):
circ.cx(qubit, qubit + 1)
circ.measure_all()
print(circ)
# Ideal simulator and execution
sim_ideal = AerSimulator()
result_ideal = sim_ideal.run(circ).result()
plot_histogram(result_ideal.get_counts(0))
# Example error probabilities
p_reset = 0.03
p_meas = 0.1
p_gate1 = 0.05
# QuantumError objects
error_reset = pauli_error([('X', p_reset), ('I', 1 - p_reset)])
error_meas = pauli_error([('X',p_meas), ('I', 1 - p_meas)])
error_gate1 = pauli_error([('X',p_gate1), ('I', 1 - p_gate1)])
error_gate2 = error_gate1.tensor(error_gate1)
# Add errors to noise model
noise_bit_flip = NoiseModel()
noise_bit_flip.add_all_qubit_quantum_error(error_reset, "reset")
noise_bit_flip.add_all_qubit_quantum_error(error_meas, "measure")
noise_bit_flip.add_all_qubit_quantum_error(error_gate1, ["u1", "u2", "u3"])
noise_bit_flip.add_all_qubit_quantum_error(error_gate2, ["cx"])
print(noise_bit_flip)
# Create noisy simulator backend
sim_noise = AerSimulator(noise_model=noise_bit_flip)
# Transpile circuit for noisy basis gates
circ_tnoise = transpile(circ, sim_noise)
# Run and get counts
result_bit_flip = sim_noise.run(circ_tnoise).result()
counts_bit_flip = result_bit_flip.get_counts(0)
# Plot noisy output
plot_histogram(counts_bit_flip)
# T1 and T2 values for qubits 0-3
T1s = np.random.normal(50e3, 10e3, 4) # Sampled from normal distribution mean 50 microsec
T2s = np.random.normal(70e3, 10e3, 4) # Sampled from normal distribution mean 50 microsec
# Truncate random T2s <= T1s
T2s = np.array([min(T2s[j], 2 * T1s[j]) for j in range(4)])
# Instruction times (in nanoseconds)
time_u1 = 0 # virtual gate
time_u2 = 50 # (single X90 pulse)
time_u3 = 100 # (two X90 pulses)
time_cx = 300
time_reset = 1000 # 1 microsecond
time_measure = 1000 # 1 microsecond
# QuantumError objects
errors_reset = [thermal_relaxation_error(t1, t2, time_reset)
for t1, t2 in zip(T1s, T2s)]
errors_measure = [thermal_relaxation_error(t1, t2, time_measure)
for t1, t2 in zip(T1s, T2s)]
errors_u1 = [thermal_relaxation_error(t1, t2, time_u1)
for t1, t2 in zip(T1s, T2s)]
errors_u2 = [thermal_relaxation_error(t1, t2, time_u2)
for t1, t2 in zip(T1s, T2s)]
errors_u3 = [thermal_relaxation_error(t1, t2, time_u3)
for t1, t2 in zip(T1s, T2s)]
errors_cx = [[thermal_relaxation_error(t1a, t2a, time_cx).expand(
thermal_relaxation_error(t1b, t2b, time_cx))
for t1a, t2a in zip(T1s, T2s)]
for t1b, t2b in zip(T1s, T2s)]
# Add errors to noise model
noise_thermal = NoiseModel()
for j in range(4):
noise_thermal.add_quantum_error(errors_reset[j], "reset", [j])
noise_thermal.add_quantum_error(errors_measure[j], "measure", [j])
noise_thermal.add_quantum_error(errors_u1[j], "u1", [j])
noise_thermal.add_quantum_error(errors_u2[j], "u2", [j])
noise_thermal.add_quantum_error(errors_u3[j], "u3", [j])
for k in range(4):
noise_thermal.add_quantum_error(errors_cx[j][k], "cx", [j, k])
print(noise_thermal)
# Run the noisy simulation
sim_thermal = AerSimulator(noise_model=noise_thermal)
# Transpile circuit for noisy basis gates
circ_tthermal = transpile(circ, sim_thermal)
# Run and get counts
result_thermal = sim_thermal.run(circ_tthermal).result()
counts_thermal = result_thermal.get_counts(0)
# Plot noisy output
plot_histogram(counts_thermal)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import transpile, QuantumCircuit
import qiskit.quantum_info as qi
from qiskit_aer import AerSimulator
from qiskit_aer.noise import NoiseModel, amplitude_damping_error
from qiskit.tools.visualization import plot_histogram
# CNOT matrix operator with qubit-0 as control and qubit-1 as target
cx_op = qi.Operator([[1, 0, 0, 0],
[0, 0, 0, 1],
[0, 0, 1, 0],
[0, 1, 0, 0]])
# iSWAP matrix operator
iswap_op = qi.Operator([[1, 0, 0, 0],
[0, 0, 1j, 0],
[0, 1j, 0, 0],
[0, 0, 0, 1]])
# CNOT in terms of iSWAP and single-qubit gates
cx_circ = QuantumCircuit(2, name='cx<iSWAP>')
# Add gates
cx_circ.sdg(1)
cx_circ.h(1)
cx_circ.sdg(0)
cx_circ.unitary(iswap_op, [0, 1], label='iswap')
cx_circ.sdg(0)
cx_circ.h(0)
cx_circ.sdg(0)
cx_circ.unitary(iswap_op, [0, 1], label='iswap')
cx_circ.s(1)
print(cx_circ)
# Simulate the unitary for the circuit using Operator:
unitary = qi.Operator(cx_circ)
print(unitary)
f_ave = qi.average_gate_fidelity(cx_op, unitary)
print("Average Gate Fidelity: F = {:f}".format(f_ave))
'unitary' in AerSimulator().configuration().basis_gates
# Error parameters
param_q0 = 0.05 # damping parameter for qubit-0
param_q1 = 0.1 # damping parameter for qubit-1
# Construct the error
qerror_q0 = amplitude_damping_error(param_q0)
qerror_q1 = amplitude_damping_error(param_q1)
iswap_error = qerror_q1.tensor(qerror_q0)
# Build the noise model by adding the error to the "iswap" gate
noise_model = NoiseModel()
noise_model.add_all_qubit_quantum_error(iswap_error, 'iswap')
noise_model.add_basis_gates(['unitary'])
print(noise_model.basis_gates)
# Bell state circuit where iSWAPS should be inserted at barrier locations
bell_circ = QuantumCircuit(2, 2, name='bell')
bell_circ.h(0)
bell_circ.append(cx_circ, [0, 1])
bell_circ.measure([0,1], [0,1])
print(bell_circ)
# Create ideal simulator backend and transpile circuit
sim_ideal = AerSimulator()
tbell_circ = transpile(bell_circ, sim_ideal)
ideal_result = sim_ideal.run(tbell_circ).result()
ideal_counts = ideal_result.get_counts(0)
plot_histogram(ideal_counts,
title='Ideal output for iSWAP bell-state preparation')
# Create noisy simulator and transpile circuit
sim_noise = AerSimulator(noise_model=noise_model)
tbell_circ_noise = transpile(bell_circ, sim_noise)
# Run on the simulator without noise
noise_result = sim_noise.run(tbell_circ_noise).result()
noise_counts = noise_result.get_counts(bell_circ)
plot_histogram(noise_counts,
title='Noisy output for iSWAP bell-state preparation')
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit_aer.utils import approximate_quantum_error, approximate_noise_model
import numpy as np
# Import Aer QuantumError functions that will be used
from qiskit_aer.noise import amplitude_damping_error, reset_error, pauli_error
from qiskit.quantum_info import Kraus
gamma = 0.23
error = amplitude_damping_error(gamma)
results = approximate_quantum_error(error, operator_string="reset")
print(results)
p = (1 + gamma - np.sqrt(1 - gamma)) / 2
q = 0
print("")
print("Expected results:")
print("P(0) = {}".format(1-(p+q)))
print("P(1) = {}".format(p))
print("P(2) = {}".format(q))
gamma = 0.23
K0 = np.array([[1,0],[0,np.sqrt(1-gamma)]])
K1 = np.array([[0,np.sqrt(gamma)],[0,0]])
results = approximate_quantum_error(Kraus([K0, K1]), operator_string="reset")
print(results)
reset_to_0 = Kraus([np.array([[1,0],[0,0]]), np.array([[0,1],[0,0]])])
reset_to_1 = Kraus([np.array([[0,0],[1,0]]), np.array([[0,0],[0,1]])])
reset_kraus = [reset_to_0, reset_to_1]
gamma = 0.23
error = amplitude_damping_error(gamma)
results = approximate_quantum_error(error, operator_list=reset_kraus)
print(results)
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile
from qiskit_aer import AerSimulator
from qiskit.tools.visualization import plot_histogram
import random
circ = QuantumCircuit(40, 40)
# Initialize with a Hadamard layer
circ.h(range(40))
# Apply some random CNOT and T gates
qubit_indices = [i for i in range(40)]
for i in range(10):
control, target, t = random.sample(qubit_indices, 3)
circ.cx(control, target)
circ.t(t)
circ.measure(range(40), range(40))
# Create statevector method simulator
statevector_simulator = AerSimulator(method='statevector')
# Transpile circuit for backend
tcirc = transpile(circ, statevector_simulator)
# Try and run circuit
statevector_result = statevector_simulator.run(tcirc, shots=1).result()
print('This succeeded?: {}'.format(statevector_result.success))
print('Why not? {}'.format(statevector_result.status))
# Create extended stabilizer method simulator
extended_stabilizer_simulator = AerSimulator(method='extended_stabilizer')
# Transpile circuit for backend
tcirc = transpile(circ, extended_stabilizer_simulator)
extended_stabilizer_result = extended_stabilizer_simulator.run(tcirc, shots=1).result()
print('This succeeded?: {}'.format(extended_stabilizer_result.success))
small_circ = QuantumCircuit(2, 2)
small_circ.h(0)
small_circ.cx(0, 1)
small_circ.t(0)
small_circ.measure([0, 1], [0, 1])
# This circuit should give 00 or 11 with equal probability...
expected_results ={'00': 50, '11': 50}
tsmall_circ = transpile(small_circ, extended_stabilizer_simulator)
result = extended_stabilizer_simulator.run(
tsmall_circ, shots=100).result()
counts = result.get_counts(0)
print('100 shots in {}s'.format(result.time_taken))
plot_histogram([expected_results, counts],
legend=['Expected', 'Extended Stabilizer'])
# Add runtime options for extended stabilizer simulator
opts = {'extended_stabilizer_approximation_error': 0.03}
reduced_error = extended_stabilizer_simulator.run(
tsmall_circ, shots=100, **opts).result()
reduced_error_counts = reduced_error.get_counts(0)
print('100 shots in {}s'.format(reduced_error.time_taken))
plot_histogram([expected_results, reduced_error_counts],
legend=['Expected', 'Extended Stabilizer'])
print("The circuit above, with 100 shots at precision 0.03 "
"and default mixing time, needed {}s".format(int(reduced_error.time_taken)))
opts = {
'extended_stabilizer_approximation_error': 0.03,
'extended_stabilizer_mixing_time': 100
}
optimized = extended_stabilizer_simulator.run(
tsmall_circ, shots=100, **opts).result()
print('Dialing down the mixing time, we completed in just {}s'.format(optimized.time_taken))
# We set these options here only to make the example run more quickly.
opts = {'extended_stabilizer_mixing_time': 100}
multishot = extended_stabilizer_simulator.run(
tcirc, shots=100, **opts).result()
print("100 shots took {} s".format(multishot.time_taken))
opts = {
'extended_stabilizer_measure_sampling': True,
'extended_stabilizer_mixing_time': 100
}
measure_sampling = extended_stabilizer_simulator.run(
circ, shots=100, **opts).result()
print("With the optimization, 100 shots took {} s".format(result.time_taken))
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
import numpy as np
# Import Qiskit
from qiskit import QuantumCircuit, transpile
from qiskit_aer import AerSimulator
# Construct quantum circuit
circ = QuantumCircuit(2, 2)
circ.h(0)
circ.cx(0, 1)
circ.measure([0,1], [0,1])
# Select the AerSimulator from the Aer provider
simulator = AerSimulator(method='matrix_product_state')
# Run and get counts, using the matrix_product_state method
tcirc = transpile(circ, simulator)
result = simulator.run(tcirc).result()
counts = result.get_counts(0)
counts
circ = QuantumCircuit(2, 2)
circ.h(0)
circ.cx(0, 1)
# Define a snapshot that shows the current state vector
circ.save_statevector(label='my_sv')
circ.save_matrix_product_state(label='my_mps')
circ.measure([0,1], [0,1])
# Execute and get saved data
tcirc = transpile(circ, simulator)
result = simulator.run(tcirc).result()
data = result.data(0)
#print the result data
data
num_qubits = 50
circ = QuantumCircuit(num_qubits, num_qubits)
# Create EPR state
circ.h(0)
for i in range (0, num_qubits-1):
circ.cx(i, i+1)
# Measure
circ.measure(range(num_qubits), range(num_qubits))
tcirc = transpile(circ, simulator)
result = simulator.run(tcirc).result()
print("Time taken: {} sec".format(result.time_taken))
result.get_counts()
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, ClassicalRegister, QuantumRegister, execute, assemble, Aer
from qiskit.tools.visualization import plot_histogram
from math import pi
import matplotlib.pyplot as plt
q = QuantumRegister(1,'q')
c = ClassicalRegister(1,'c')
qc = QuantumCircuit(q, c)
qc.h(0)
qc.measure(0,0)
qc.x(0).c_if(c, 0)
qc.draw(output='mpl')
q = QuantumRegister(3,'q')
c = ClassicalRegister(3,'c')
qc = QuantumCircuit(q, c)
qc.h(q[0])
qc.h(q[1])
qc.h(q[2])
qc.barrier()
qc.measure(q,c)
qc.draw('mpl')
print(bin(3))
print(bin(7))
q = QuantumRegister(3,'q')
c = ClassicalRegister(3,'c')
qc = QuantumCircuit(q, c)
qc.h(0)
qc.h(1)
qc.h(2)
qc.barrier()
qc.measure(q,c)
qc.x(2).c_if(c, 3) # for the 011 case
qc.x(2).c_if(c, 7) # for the 111 case
qc.draw(output='mpl')
nq = 2
m = 2
q = QuantumRegister(nq,'q')
c = ClassicalRegister(m,'c')
qc_S = QuantumCircuit(q,c)
qc_S.h(0)
qc_S.x(1)
qc_S.draw('mpl')
cu_circ = QuantumCircuit(2)
cu_circ.cp(pi/2,0,1)
cu_circ.draw('mpl')
for _ in range(2**(m-1)):
qc_S.cp(pi/2,0,1)
qc_S.draw('mpl')
def x_measurement(qc, qubit, cbit):
"""Measure 'qubit' in the X-basis, and store the result in 'cbit'"""
qc.h(qubit)
qc.measure(qubit, cbit)
x_measurement(qc_S, q[0], c[0])
qc_S.draw('mpl')
qc_S.reset(0)
qc_S.h(0)
qc_S.draw('mpl')
qc_S.p(-pi/2,0).c_if(c,1)
qc_S.draw('mpl')
## 2^t c-U operations (with t=m-2)
for _ in range(2**(m-2)):
qc_S.cp(pi/2,0,1)
x_measurement(qc_S, q[0], c[1])
qc_S.draw('mpl')
sim = Aer.get_backend('qasm_simulator')
count0 = execute(qc_S, sim).result().get_counts()
key_new = [str(int(key,2)/2**m) for key in list(count0.keys())]
count1 = dict(zip(key_new, count0.values()))
fig, ax = plt.subplots(1,2)
plot_histogram(count0, ax=ax[0])
plot_histogram(count1, ax=ax[1])
plt.tight_layout()
nq = 3 # number of qubits
m = 3 # number of classical bits
q = QuantumRegister(nq,'q')
c = ClassicalRegister(m,'c')
qc = QuantumCircuit(q,c)
qc.h(0)
qc.x([1,2])
qc.draw('mpl')
cu_circ = QuantumCircuit(nq)
cu_circ.mcp(pi/4,[0,1],2)
cu_circ.draw('mpl')
for _ in range(2**(m-1)):
qc.mcp(pi/4,[0,1],2)
qc.draw('mpl')
x_measurement(qc, q[0], c[0])
qc.draw('mpl')
qc.reset(0)
qc.h(0)
qc.draw('mpl')
qc.p(-pi/2,0).c_if(c,1)
qc.draw('mpl')
for _ in range(2**(m-2)):
qc.mcp(pi/4,[0,1],2)
x_measurement(qc, q[0], c[1])
qc.draw('mpl')
# initialization of qubit q0
qc.reset(0)
qc.h(0)
# phase correction
qc.p(-pi/4,0).c_if(c,1)
qc.p(-pi/2,0).c_if(c,2)
qc.p(-3*pi/4,0).c_if(c,3)
# c-U operations
for _ in range(2**(m-3)):
qc.mcp(pi/4,[0,1],2)
# X measurement
qc.h(0)
qc.measure(0,2)
qc.draw('mpl')
count0 = execute(qc, sim).result().get_counts()
key_new = [str(int(key,2)/2**m) for key in list(count0.keys())]
count1 = dict(zip(key_new, count0.values()))
fig, ax = plt.subplots(1,2)
plot_histogram(count0, ax=ax[0])
plot_histogram(count1, ax=ax[1])
fig.tight_layout()
import qiskit.tools.jupyter
%qiskit_version_table
%qiskit_copyright
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile, schedule
from qiskit.visualization.timeline import draw, IQXSimple
from qiskit.providers.fake_provider import FakeBoeblingen
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0,1)
qc = transpile(qc, FakeBoeblingen(), scheduling_method='alap', layout_method='trivial')
draw(qc, style=IQXSimple())
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
# If you introduce a list with less colors than bars, the color of the bars will
# alternate following the sequence from the list.
import numpy as np
from qiskit.quantum_info import DensityMatrix
from qiskit import QuantumCircuit
from qiskit.visualization import plot_state_paulivec
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
qc = QuantumCircuit(2)
qc.h([0, 1])
qc.cz(0, 1)
qc.ry(np.pi/3, 0)
qc.rx(np.pi/5, 1)
matrix = DensityMatrix(qc)
plot_state_paulivec(matrix, color=['crimson', 'midnightblue', 'seagreen'])
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.quantum_info import Operator
from qiskit.transpiler.passes import UnitarySynthesis
circuit = QuantumCircuit(1)
circuit.rx(0.8, 0)
unitary = Operator(circuit).data
unitary_circ = QuantumCircuit(1)
unitary_circ.unitary(unitary, [0])
synth = UnitarySynthesis(basis_gates=["h", "s"], method="sk")
out = synth(unitary_circ)
out.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
# You can choose different colors for the real and imaginary parts of the density matrix.
from qiskit import QuantumCircuit
from qiskit.quantum_info import DensityMatrix
from qiskit.visualization import plot_state_city
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
state = DensityMatrix(qc)
plot_state_city(state, color=['midnightblue', 'crimson'], title="New State City")
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.quantum_info import Clifford, random_clifford
qc = QuantumCircuit(3)
cliff = random_clifford(2)
qc.append(cliff, [0, 1])
qc.ccx(0, 1, 2)
qc.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit.circuit.library import MCXGate
gate = MCXGate(4)
from qiskit import QuantumCircuit
circuit = QuantumCircuit(5)
circuit.append(gate, [0, 1, 4, 2, 3])
circuit.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile
ghz = QuantumCircuit(15)
ghz.h(0)
ghz.cx(0, range(1, 15))
ghz.draw(output='mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile
from qiskit.visualization import plot_circuit_layout
from qiskit.providers.fake_provider import FakeVigo
backend = FakeVigo()
ghz = QuantumCircuit(3, 3)
ghz.h(0)
ghz.cx(0,range(1,3))
ghz.barrier()
ghz.measure(range(3), range(3))
# Virtual -> physical
# 0 -> 3
# 1 -> 4
# 2 -> 2
my_ghz = transpile(ghz, backend, initial_layout=[3, 4, 2])
plot_circuit_layout(my_ghz, backend)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.quantum_info import Statevector
from qiskit.visualization import plot_bloch_multivector
qc = QuantumCircuit(2)
qc.h(0)
qc.x(1)
# You can reverse the order of the qubits.
from qiskit.quantum_info import DensityMatrix
qc = QuantumCircuit(2)
qc.h([0, 1])
qc.t(1)
qc.s(0)
qc.cx(0,1)
matrix = DensityMatrix(qc)
plot_bloch_multivector(matrix, title='My Bloch Spheres', reverse_bits=True)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import BasicAer, transpile, QuantumRegister, ClassicalRegister, QuantumCircuit
qr = QuantumRegister(1)
cr = ClassicalRegister(1)
qc = QuantumCircuit(qr, cr)
qc.h(0)
qc.measure(0, 0)
qc.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile
from qiskit.visualization import plot_circuit_layout
from qiskit.providers.fake_provider import FakeVigo
backend = FakeVigo()
ghz = QuantumCircuit(3, 3)
ghz.h(0)
ghz.cx(0,range(1,3))
ghz.barrier()
ghz.measure(range(3), range(3))
ghz.draw(output='mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import transpile
from qiskit import QuantumCircuit
from qiskit.providers.fake_provider import FakeVigoV2
backend = FakeVigoV2()
qc = QuantumCircuit(2, 1)
qc.h(0)
qc.x(1)
qc.cp(np.pi/4, 0, 1)
qc.h(0)
qc.measure([0], [0])
qc_basis = transpile(qc, backend)
qc_basis.draw(output='mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile
from qiskit.visualization import plot_circuit_layout
from qiskit.providers.fake_provider import FakeVigo
backend = FakeVigo()
ghz = QuantumCircuit(3, 3)
ghz.h(0)
ghz.cx(0,range(1,3))
ghz.barrier()
ghz.measure(range(3), range(3))
new_circ_lv3 = transpile(ghz, backend=backend, optimization_level=3)
plot_circuit_layout(new_circ_lv3, backend)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile, schedule
from qiskit.visualization.pulse_v2 import draw, IQXSimple
from qiskit.providers.fake_provider import FakeBoeblingen
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
qc.measure_all()
qc = transpile(qc, FakeBoeblingen(), layout_method='trivial')
sched = schedule(qc, FakeBoeblingen())
draw(sched, style=IQXSimple(), backend=FakeBoeblingen())
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
import numpy as np
from qiskit import pulse
d0 = pulse.DriveChannel(0)
x90 = pulse.Gaussian(10, 0.1, 3)
x180 = pulse.Gaussian(10, 0.2, 3)
def udd10_pos(j):
return np.sin(np.pi*j/(2*10 + 2))**2
with pulse.build() as udd_sched:
pulse.play(x90, d0)
with pulse.align_func(duration=300, func=udd10_pos):
for _ in range(10):
pulse.play(x180, d0)
pulse.play(x90, d0)
udd_sched.draw()
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumRegister, ClassicalRegister, QuantumCircuit
qr = QuantumRegister(3, 'q')
anc = QuantumRegister(1, 'ancilla')
cr = ClassicalRegister(3, 'c')
qc = QuantumCircuit(qr, anc, cr)
qc.x(anc[0])
qc.h(anc[0])
qc.h(qr[0:3])
qc.cx(qr[0:3], anc[0])
qc.h(qr[0:3])
qc.barrier(qr)
qc.measure(qr, cr)
qc.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumRegister, ClassicalRegister, QuantumCircuit
q = QuantumRegister(1)
c = ClassicalRegister(1)
qc = QuantumCircuit(q, c)
qc.h(q)
qc.measure(q, c)
qc.draw(output='mpl', style={'backgroundcolor': '#EEEEEE'})
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, execute
from qiskit.visualization import plot_error_map
from qiskit.providers.fake_provider import FakeVigoV2
backend = FakeVigoV2()
plot_error_map(backend)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
top = QuantumCircuit(1)
top.x(0);
bottom = QuantumCircuit(2)
bottom.cry(0.2, 0, 1);
tensored = bottom.tensor(top)
tensored.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import pulse
dc = pulse.DriveChannel
d0, d1, d2, d3, d4 = dc(0), dc(1), dc(2), dc(3), dc(4)
with pulse.build(name='pulse_programming_in') as pulse_prog:
pulse.play([1, 1, 1, 0, 0, 1, 1, 1, 0, 1, 1, 1, 0, 1, 0, 1, 0, 1, 1, 1, 0, 1, 1, 1], d0)
pulse.play([1, 0, 1, 0, 0, 0, 1, 0, 0, 1, 0, 0, 0, 1, 1, 0, 0, 0, 1, 0, 0, 0, 1, 0], d1)
pulse.play([1, 0, 1, 0, 0, 0, 1, 0, 0, 1, 1, 1, 0, 1, 0, 0, 0, 0, 1, 0, 0, 0, 1, 0], d2)
pulse.play([1, 0, 1, 0, 0, 0, 1, 0, 0, 0, 0, 1, 0, 1, 1, 0, 0, 0, 1, 0, 0, 0, 1, 0], d3)
pulse.play([1, 1, 1, 1, 0, 1, 1, 1, 0, 1, 1, 1, 0, 1, 0, 1, 0, 1, 1, 1, 0, 0, 1, 0], d4)
pulse_prog.draw()
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit.visualization.timeline import draw as timeline_draw
from qiskit import QuantumCircuit, transpile
from qiskit.providers.fake_provider import FakeBoeblingen
backend = FakeBoeblingen()
ghz = QuantumCircuit(5)
ghz.h(0)
ghz.cx(0,range(1,5))
circ = transpile(ghz, backend, scheduling_method="asap")
timeline_draw(circ)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
qc = QuantumCircuit(12)
for idx in range(5):
qc.h(idx)
qc.cx(idx, idx+5)
qc.cx(1, 7)
qc.x(8)
qc.cx(1, 9)
qc.x(7)
qc.cx(1, 11)
qc.swap(6, 11)
qc.swap(6, 9)
qc.swap(6, 10)
qc.x(6)
qc.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import pulse
d0 = pulse.DriveChannel(0)
d1 = pulse.DriveChannel(1)
with pulse.build() as pulse_prog:
with pulse.align_right():
# this pulse will start at t=0
pulse.play(pulse.Constant(100, 1.0), d0)
# this pulse will start at t=80
pulse.play(pulse.Constant(20, 1.0), d1)
pulse_prog.draw()
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.quantum_info import Statevector
from qiskit.visualization import plot_bloch_multivector
qc = QuantumCircuit(2)
qc.h(0)
qc.x(1)
state = Statevector(qc)
plot_bloch_multivector(state)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
# You can make the bars more transparent to better see the ones that are behind
# if they overlap.
import numpy as np
from qiskit.quantum_info import Statevector
from qiskit.visualization import plot_state_city
from qiskit import QuantumCircuit
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
qc = QuantumCircuit(2)
qc.h([0, 1])
qc.cz(0,1)
qc.ry(np.pi/3, 0)
qc.rx(np.pi/5, 1)
state = Statevector(qc)
plot_state_city(state, alpha=0.6)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import execute, pulse
d0 = pulse.DriveChannel(0)
with pulse.build() as pulse_prog:
pulse.play(pulse.Constant(100, 1.0), d0)
pulse_prog.draw()
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile
from qiskit.providers.fake_provider import FakeBoeblingen
backend = FakeBoeblingen()
ghz = QuantumCircuit(5)
ghz.h(0)
ghz.cx(0,range(1,5))
circ = transpile(ghz, backend, scheduling_method="asap")
circ.draw(output='mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
import matplotlib.pyplot as plt
from qiskit import QuantumCircuit, transpile
from qiskit.providers.fake_provider import FakeAuckland
backend = FakeAuckland()
ghz = QuantumCircuit(15)
ghz.h(0)
ghz.cx(0, range(1, 15))
ghz.draw(output='mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumRegister, ClassicalRegister, QuantumCircuit
q = QuantumRegister(1)
c = ClassicalRegister(1)
qc = QuantumCircuit(q, c)
qc.h(q)
qc.measure(q, c)
qc.draw(output='mpl', style={'backgroundcolor': '#EEEEEE'})
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumRegister, ClassicalRegister, QuantumCircuit
from qiskit.dagcircuit import DAGCircuit
from qiskit.converters import circuit_to_dag
from qiskit.circuit.library.standard_gates import CHGate, U2Gate, CXGate
from qiskit.converters import dag_to_circuit
q = QuantumRegister(3, 'q')
c = ClassicalRegister(3, 'c')
circ = QuantumCircuit(q, c)
circ.h(q[0])
circ.cx(q[0], q[1])
circ.measure(q[0], c[0])
circ.rz(0.5, q[1]).c_if(c, 2)
dag = circuit_to_dag(circ)
circuit = dag_to_circuit(dag)
circuit.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import pulse
d0 = pulse.DriveChannel(0)
x90 = pulse.Gaussian(10, 0.1, 3)
x180 = pulse.Gaussian(10, 0.2, 3)
with pulse.build() as hahn_echo:
with pulse.align_equispaced(duration=100):
pulse.play(x90, d0)
pulse.play(x180, d0)
pulse.play(x90, d0)
hahn_echo.draw()
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
# You can set a color for all the bars.
from qiskit import QuantumCircuit
from qiskit.quantum_info import Statevector
from qiskit.visualization import plot_state_paulivec
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
state = Statevector(qc)
plot_state_paulivec(state, color='midnightblue', title="New PauliVec plot")
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.transpiler.passes import RemoveBarriers
circuit = QuantumCircuit(1)
circuit.x(0)
circuit.barrier()
circuit.h(0)
circuit = RemoveBarriers()(circuit)
circuit.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.quantum_info import DensityMatrix
from qiskit.visualization import plot_state_city
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0,1)
# plot using a DensityMatrix
state = DensityMatrix(qc)
plot_state_city(state)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, QuantumRegister, ClassicalRegister
from qiskit.circuit.quantumcircuitdata import CircuitInstruction
from qiskit.circuit import Measure
from qiskit.circuit.library import HGate, CXGate
qr = QuantumRegister(2)
cr = ClassicalRegister(2)
instructions = [
CircuitInstruction(HGate(), [qr[0]], []),
CircuitInstruction(CXGate(), [qr[0], qr[1]], []),
CircuitInstruction(Measure(), [qr[0]], [cr[0]]),
CircuitInstruction(Measure(), [qr[1]], [cr[1]]),
]
circuit = QuantumCircuit.from_instructions(instructions)
circuit.draw("mpl")
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumRegister, ClassicalRegister, QuantumCircuit
q = QuantumRegister(1)
c = ClassicalRegister(1)
qc = QuantumCircuit(q, c)
qc.h(q)
qc.measure(q, c)
qc.draw(output='mpl', style={'backgroundcolor': '#EEEEEE'})
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, transpile, schedule
from qiskit.visualization.timeline import draw
from qiskit.providers.fake_provider import FakeBoeblingen
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0,1)
qc = transpile(qc, FakeBoeblingen(), scheduling_method='alap', layout_method='trivial')
draw(qc)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit, execute
from qiskit.providers.fake_provider import FakeVigoV2
from qiskit.visualization import plot_gate_map
backend = FakeVigoV2()
plot_gate_map(backend)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.quantum_info import Statevector
from qiskit.visualization import plot_state_qsphere
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)
state = Statevector(qc)
plot_state_qsphere(state)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
ghz = QuantumCircuit(5)
ghz.h(0)
ghz.cx(0,range(1,5))
ghz.draw(output='mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
# Create a circuit with a register of three qubits
circ = QuantumCircuit(3)
# H gate on qubit 0, putting this qubit in a superposition of |0> + |1>.
circ.h(0)
# A CX (CNOT) gate on control qubit 0 and target qubit 1 generating a Bell state.
circ.cx(0, 1)
# CX (CNOT) gate on control qubit 0 and target qubit 2 resulting in a GHZ state.
circ.cx(0, 2)
# Draw the circuit
circ.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
qc = QuantumCircuit(2, 2)
qc.h(0)
qc.cx(0, 1)
qc.measure([0, 1], [0, 1])
qc.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import ClassicalRegister, QuantumRegister, QuantumCircuit
qr = QuantumRegister(2)
cr = ClassicalRegister(2)
qc = QuantumCircuit(qr, cr)
qc.h(range(2))
qc.measure(range(2), range(2))
# apply x gate if the classical register has the value 2 (10 in binary)
qc.x(0).c_if(cr, 2)
# apply y gate if bit 0 is set to 1
qc.y(1).c_if(0, 1)
qc.draw('mpl')
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
from qiskit import QuantumCircuit
from qiskit.quantum_info import Statevector
from qiskit.visualization import plot_state_city
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0,1)
# plot using a Statevector
state = Statevector(qc)
plot_state_city(state)
|
https://github.com/qiskit-community/qiskit-translations-staging
|
qiskit-community
|
import numpy as np
from qiskit import QuantumCircuit
from qiskit.quantum_info import DensityMatrix
from qiskit.visualization import plot_state_hinton
qc = QuantumCircuit(2)
qc.h([0, 1])
qc.cz(0,1)
qc.ry(np.pi/3 , 0)
qc.rx(np.pi/5, 1)
state = DensityMatrix(qc)
plot_state_hinton(state, title="New Hinton Plot")
|
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