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Create workflow for Z-phase calibration (#6728)
This calibration workflow is created for excitation preserving 2-qubit gates and assumes an error model that can be described with small random z-rotations ``` 0: ───Rz(a)───two_qubit_gate───Rz(c)─── │ 1: ───Rz(b)───two_qubit_gate───Rz(d)─── ``` for some small angles a, b, c, and d. --- when the error model doesn't apply the workflow may give absured numbers (e.g. fidilities $\notin [0, 1]$). The fidilities can be slightly outside the $[0, 1]$ interval because it's a statistical estimate as can be seen in the following figure which compares the estimated fidelity of a CZ surrounded by random z rotations before and after calibration ![image](https://github.com/user-attachments/assets/40e7cedb-179b-416b-8796-94d1da44012b) test notebook: https://colab.sandbox.google.com/drive/10gZ5dggYKH_xSsCJFpg__GakxvoaZDIi
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# Copyright 2024 The Cirq Developers | ||
# | ||
# Licensed under the Apache License, Version 2.0 (the "License"); | ||
# you may not use this file except in compliance with the License. | ||
# You may obtain a copy of the License at | ||
# | ||
# https://www.apache.org/licenses/LICENSE-2.0 | ||
# | ||
# Unless required by applicable law or agreed to in writing, software | ||
# distributed under the License is distributed on an "AS IS" BASIS, | ||
# WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied. | ||
# See the License for the specific language governing permissions and | ||
# limitations under the License. | ||
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"""Provides a method to do z-phase calibration for excitation-preserving gates.""" | ||
from typing import Union, Optional, Sequence, Tuple, Dict, TYPE_CHECKING | ||
import multiprocessing | ||
import multiprocessing.pool | ||
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import matplotlib.pyplot as plt | ||
import numpy as np | ||
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from cirq.experiments import xeb_fitting | ||
from cirq.experiments.two_qubit_xeb import parallel_xeb_workflow | ||
from cirq import ops | ||
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if TYPE_CHECKING: | ||
import cirq | ||
import pandas as pd | ||
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def z_phase_calibration_workflow( | ||
sampler: 'cirq.Sampler', | ||
qubits: Optional[Sequence['cirq.GridQubit']] = None, | ||
two_qubit_gate: 'cirq.Gate' = ops.CZ, | ||
options: Optional[xeb_fitting.XEBPhasedFSimCharacterizationOptions] = None, | ||
n_repetitions: int = 10**4, | ||
n_combinations: int = 10, | ||
n_circuits: int = 20, | ||
cycle_depths: Sequence[int] = tuple(np.arange(3, 100, 20)), | ||
random_state: 'cirq.RANDOM_STATE_OR_SEED_LIKE' = None, | ||
atol: float = 1e-3, | ||
num_workers_or_pool: Union[int, 'multiprocessing.pool.Pool'] = -1, | ||
) -> Tuple[xeb_fitting.XEBCharacterizationResult, 'pd.DataFrame']: | ||
"""Perform z-phase calibration for excitation-preserving gates. | ||
For a given excitation-preserving two-qubit gate we assume an error model that can be described | ||
using Z-rotations: | ||
0: ───Rz(a)───two_qubit_gate───Rz(c)─── | ||
│ | ||
1: ───Rz(b)───two_qubit_gate───Rz(d)─── | ||
for some angles a, b, c, and d. | ||
Since the two-qubit gate is a excitation-preserving-gate, it can be represented by an FSimGate | ||
and the effect of rotations turns it into a PhasedFSimGate. Using XEB-data we find the | ||
PhasedFSimGate parameters that minimize the infidelity of the gate. | ||
References: | ||
- https://arxiv.org/abs/2001.08343 | ||
- https://arxiv.org/abs/2010.07965 | ||
- https://arxiv.org/abs/1910.11333 | ||
Args: | ||
sampler: The quantum engine or simulator to run the circuits. | ||
qubits: Qubits to use. If none, use all qubits on the sampler's device. | ||
two_qubit_gate: The entangling gate to use. | ||
options: The XEB-fitting options. If None, calibrate only the three phase angles | ||
(chi, gamma, zeta) using the representation of a two-qubit gate as an FSimGate | ||
for the initial guess. | ||
n_repetitions: The number of repetitions to use. | ||
n_combinations: The number of combinations to generate. | ||
n_circuits: The number of circuits to generate. | ||
cycle_depths: The cycle depths to use. | ||
random_state: The random state to use. | ||
atol: Absolute tolerance to be used by the minimizer. | ||
num_workers_or_pool: An optional multi-processing pool or number of workers. | ||
A zero value means no multiprocessing. | ||
A positive integer value will create a pool with the given number of workers. | ||
A negative value will create pool with maximum number of workers. | ||
Returns: | ||
- An `XEBCharacterizationResult` object that contains the calibration result. | ||
- A `pd.DataFrame` comparing the before and after fidelities. | ||
""" | ||
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pool: Optional['multiprocessing.pool.Pool'] = None | ||
local_pool = False | ||
if isinstance(num_workers_or_pool, multiprocessing.pool.Pool): | ||
pool = num_workers_or_pool # pragma: no cover | ||
elif num_workers_or_pool != 0: | ||
pool = multiprocessing.Pool(num_workers_or_pool if num_workers_or_pool > 0 else None) | ||
local_pool = True | ||
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fids_df_0, circuits, sampled_df = parallel_xeb_workflow( | ||
sampler=sampler, | ||
qubits=qubits, | ||
entangling_gate=two_qubit_gate, | ||
n_repetitions=n_repetitions, | ||
cycle_depths=cycle_depths, | ||
n_circuits=n_circuits, | ||
n_combinations=n_combinations, | ||
random_state=random_state, | ||
pool=pool, | ||
) | ||
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if options is None: | ||
options = xeb_fitting.XEBPhasedFSimCharacterizationOptions( | ||
characterize_chi=True, | ||
characterize_gamma=True, | ||
characterize_zeta=True, | ||
characterize_theta=False, | ||
characterize_phi=False, | ||
).with_defaults_from_gate(two_qubit_gate) | ||
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p_circuits = [ | ||
xeb_fitting.parameterize_circuit(circuit, options, ops.GateFamily(two_qubit_gate)) | ||
for circuit in circuits | ||
] | ||
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result = xeb_fitting.characterize_phased_fsim_parameters_with_xeb_by_pair( | ||
sampled_df=sampled_df, | ||
parameterized_circuits=p_circuits, | ||
cycle_depths=cycle_depths, | ||
options=options, | ||
fatol=atol, | ||
xatol=atol, | ||
pool=pool, | ||
) | ||
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before_after = xeb_fitting.before_and_after_characterization( | ||
fids_df_0, characterization_result=result | ||
) | ||
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if local_pool: | ||
assert isinstance(pool, multiprocessing.pool.Pool) | ||
pool.close() | ||
return result, before_after | ||
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def calibrate_z_phases( | ||
sampler: 'cirq.Sampler', | ||
qubits: Optional[Sequence['cirq.GridQubit']] = None, | ||
two_qubit_gate: 'cirq.Gate' = ops.CZ, | ||
options: Optional[xeb_fitting.XEBPhasedFSimCharacterizationOptions] = None, | ||
n_repetitions: int = 10**4, | ||
n_combinations: int = 10, | ||
n_circuits: int = 20, | ||
cycle_depths: Sequence[int] = tuple(np.arange(3, 100, 20)), | ||
random_state: 'cirq.RANDOM_STATE_OR_SEED_LIKE' = None, | ||
atol: float = 1e-3, | ||
num_workers_or_pool: Union[int, 'multiprocessing.pool.Pool'] = -1, | ||
) -> Dict[Tuple['cirq.Qid', 'cirq.Qid'], 'cirq.PhasedFSimGate']: | ||
"""Perform z-phase calibration for excitation-preserving gates. | ||
For a given excitation-preserving two-qubit gate we assume an error model that can be described | ||
using Z-rotations: | ||
0: ───Rz(a)───two_qubit_gate───Rz(c)─── | ||
│ | ||
1: ───Rz(b)───two_qubit_gate───Rz(d)─── | ||
for some angles a, b, c, and d. | ||
Since the two-qubit gate is a excitation-preserving gate, it can be represented by an FSimGate | ||
and the effect of rotations turns it into a PhasedFSimGate. Using XEB-data we find the | ||
PhasedFSimGate parameters that minimize the infidelity of the gate. | ||
References: | ||
- https://arxiv.org/abs/2001.08343 | ||
- https://arxiv.org/abs/2010.07965 | ||
- https://arxiv.org/abs/1910.11333 | ||
Args: | ||
sampler: The quantum engine or simulator to run the circuits. | ||
qubits: Qubits to use. If none, use all qubits on the sampler's device. | ||
two_qubit_gate: The entangling gate to use. | ||
options: The XEB-fitting options. If None, calibrate only the three phase angles | ||
(chi, gamma, zeta) using the representation of a two-qubit gate as an FSimGate | ||
for the initial guess. | ||
n_repetitions: The number of repetitions to use. | ||
n_combinations: The number of combinations to generate. | ||
n_circuits: The number of circuits to generate. | ||
cycle_depths: The cycle depths to use. | ||
random_state: The random state to use. | ||
atol: Absolute tolerance to be used by the minimizer. | ||
num_workers_or_pool: An optional multi-processing pool or number of workers. | ||
A zero value means no multiprocessing. | ||
A positive integer value will create a pool with the given number of workers. | ||
A negative value will create pool with maximum number of workers. | ||
Returns: | ||
- A dictionary mapping qubit pairs to the calibrated PhasedFSimGates. | ||
""" | ||
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if options is None: | ||
options = xeb_fitting.XEBPhasedFSimCharacterizationOptions( | ||
characterize_chi=True, | ||
characterize_gamma=True, | ||
characterize_zeta=True, | ||
characterize_theta=False, | ||
characterize_phi=False, | ||
).with_defaults_from_gate(two_qubit_gate) | ||
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result, _ = z_phase_calibration_workflow( | ||
sampler=sampler, | ||
qubits=qubits, | ||
two_qubit_gate=two_qubit_gate, | ||
options=options, | ||
n_repetitions=n_repetitions, | ||
n_combinations=n_combinations, | ||
n_circuits=n_circuits, | ||
cycle_depths=cycle_depths, | ||
random_state=random_state, | ||
atol=atol, | ||
num_workers_or_pool=num_workers_or_pool, | ||
) | ||
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gates = {} | ||
for pair, params in result.final_params.items(): | ||
params['theta'] = params.get('theta', options.theta_default or 0) | ||
params['phi'] = params.get('phi', options.phi_default or 0) | ||
params['zeta'] = params.get('zeta', options.zeta_default or 0) | ||
params['chi'] = params.get('chi', options.chi_default or 0) | ||
params['gamma'] = params.get('gamma', options.gamma_default or 0) | ||
gates[pair] = ops.PhasedFSimGate(**params) | ||
return gates | ||
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def plot_z_phase_calibration_result( | ||
before_after_df: 'pd.DataFrame', | ||
axes: Optional[np.ndarray[Sequence[Sequence['plt.Axes']], np.dtype[np.object_]]] = None, | ||
pairs: Optional[Sequence[Tuple['cirq.Qid', 'cirq.Qid']]] = None, | ||
*, | ||
with_error_bars: bool = False, | ||
) -> np.ndarray[Sequence[Sequence['plt.Axes']], np.dtype[np.object_]]: | ||
"""A helper method to plot the result of running z-phase calibration. | ||
Note that the plotted fidelity is a statistical estimate of the true fidelity and as a result | ||
may be outside the [0, 1] range. | ||
Args: | ||
before_after_df: The second return object of running `z_phase_calibration_workflow`. | ||
axes: And ndarray of the axes to plot on. | ||
The number of axes is expected to be >= number of qubit pairs. | ||
pairs: If provided, only the given pairs are plotted. | ||
with_error_bars: Whether to add error bars or not. | ||
The width of the bar is an upper bound on standard variation of the estimated fidelity. | ||
""" | ||
if pairs is None: | ||
pairs = before_after_df.index | ||
if axes is None: | ||
# Create a 16x9 rectangle. | ||
ncols = int(np.ceil(np.sqrt(9 / 16 * len(pairs)))) | ||
nrows = (len(pairs) + ncols - 1) // ncols | ||
_, axes = plt.subplots(nrows=nrows, ncols=ncols) | ||
axes = axes if isinstance(axes, np.ndarray) else np.array(axes) | ||
for pair, ax in zip(pairs, axes.flatten()): | ||
row = before_after_df.loc[[pair]].iloc[0] | ||
ax.errorbar( | ||
row.cycle_depths_0, | ||
row.fidelities_0, | ||
yerr=row.layer_fid_std_0 * with_error_bars, | ||
label='original', | ||
) | ||
ax.errorbar( | ||
row.cycle_depths_0, | ||
row.fidelities_c, | ||
yerr=row.layer_fid_std_c * with_error_bars, | ||
label='calibrated', | ||
) | ||
ax.axhline(1, linestyle='--') | ||
ax.set_xlabel('cycle depth') | ||
ax.set_ylabel('fidelity estimate') | ||
ax.set_title('-'.join(str(q) for q in pair)) | ||
ax.legend() | ||
return axes |
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