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Add Google-specific variant for noise properties. (quantumlib#5082)
This PR provides an implementation of `SuperconductingQubitsNoiseProperties` for Google hardware. Now that SQNP is an abstract type, this is a prerequisite for re-enabling calibration-to-noise tools. This is part 3 of quantumlib#4666; part 2 was quantumlib#4964. Remaining steps include: - Reinstatement of calibration_to_noise_properties using new types - Reinstatement of compare_generated_noise_to_metrics using new types
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cirq-google/cirq_google/devices/google_noise_properties.py
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# Copyright 2022 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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"""Class for representing noise on a Google device.""" | ||
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from dataclasses import dataclass, field | ||
from typing import Dict, List, Set, Type | ||
import numpy as np | ||
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import cirq, cirq_google | ||
from cirq import _compat, devices | ||
from cirq.devices import noise_utils | ||
from cirq.transformers.heuristic_decompositions import gate_tabulation_math_utils | ||
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SINGLE_QUBIT_GATES: Set[Type['cirq.Gate']] = { | ||
cirq.ZPowGate, | ||
cirq.PhasedXZGate, | ||
cirq.MeasurementGate, | ||
cirq.ResetChannel, | ||
} | ||
SYMMETRIC_TWO_QUBIT_GATES: Set[Type['cirq.Gate']] = { | ||
cirq_google.SycamoreGate, | ||
cirq.FSimGate, | ||
cirq.PhasedFSimGate, | ||
cirq.ISwapPowGate, | ||
cirq.CZPowGate, | ||
} | ||
ASYMMETRIC_TWO_QUBIT_GATES: Set[Type['cirq.Gate']] = set() | ||
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@dataclass | ||
class GoogleNoiseProperties(devices.SuperconductingQubitsNoiseProperties): | ||
"""Noise-defining properties for a Google device. | ||
Inherited args: | ||
gate_times_ns: Dict[type, float] of gate types to their duration on | ||
quantum hardware. Used with t(1|phi)_ns to specify thermal noise. | ||
t1_ns: Dict[cirq.Qid, float] of qubits to their T_1 time, in ns. | ||
tphi_ns: Dict[cirq.Qid, float] of qubits to their T_phi time, in ns. | ||
readout_errors: Dict[cirq.Qid, np.ndarray] of qubits to their readout | ||
errors in matrix form: [P(read |1> from |0>), P(read |0> from |1>)]. | ||
Used to prepend amplitude damping errors to measurements. | ||
gate_pauli_errors: dict of noise_utils.OpIdentifiers (a gate and the qubits it | ||
targets) to the Pauli error for that operation. Used to construct | ||
depolarizing error. Keys in this dict must have defined qubits. | ||
validate: If True, verifies that t1 and tphi qubits sets match, and | ||
that all symmetric two-qubit gates have errors which are | ||
symmetric over the qubits they affect. Defaults to True. | ||
Additional args: | ||
fsim_errors: Dict[noise_utils.OpIdentifier, cirq.PhasedFSimGate] of gate types | ||
(potentially on specific qubits) to the PhasedFSim fix-up operation | ||
for that gate. Defaults to no-op for all gates. | ||
""" | ||
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fsim_errors: Dict[noise_utils.OpIdentifier, cirq.PhasedFSimGate] = field(default_factory=dict) | ||
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def __post_init__(self): | ||
super().__post_init__() | ||
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# validate two qubit gate errors. | ||
self._validate_symmetric_errors('fsim_errors') | ||
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@classmethod | ||
def single_qubit_gates(cls) -> Set[type]: | ||
return SINGLE_QUBIT_GATES | ||
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@classmethod | ||
def symmetric_two_qubit_gates(cls) -> Set[type]: | ||
return SYMMETRIC_TWO_QUBIT_GATES | ||
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@classmethod | ||
def asymmetric_two_qubit_gates(cls) -> Set[type]: | ||
return ASYMMETRIC_TWO_QUBIT_GATES | ||
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@_compat.cached_property | ||
def _depolarizing_error(self) -> Dict[noise_utils.OpIdentifier, float]: | ||
depol_errors = super()._depolarizing_error | ||
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def extract_entangling_error(match_id: noise_utils.OpIdentifier): | ||
"""Gets the entangling error component of depol_errors[match_id].""" | ||
unitary_err = cirq.unitary(self.fsim_errors[match_id]) | ||
fid = gate_tabulation_math_utils.unitary_entanglement_fidelity(unitary_err, np.eye(4)) | ||
return 1 - fid | ||
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# Subtract entangling angle error. | ||
for op_id in depol_errors: | ||
if op_id.gate_type not in self.two_qubit_gates(): | ||
continue | ||
if op_id in self.fsim_errors: | ||
depol_errors[op_id] -= extract_entangling_error(op_id) | ||
continue | ||
# Find the closest matching supertype, if one is provided. | ||
# Gateset has similar behavior, but cannot be used here | ||
# because depol_errors is a dict, not a set. | ||
match_id = None | ||
candidate_parents = [ | ||
parent_id for parent_id in self.fsim_errors if op_id.is_proper_subtype_of(parent_id) | ||
] | ||
for parent_id in candidate_parents: | ||
if match_id is None or parent_id.is_proper_subtype_of(match_id): | ||
match_id = parent_id | ||
if match_id is not None: | ||
depol_errors[op_id] -= extract_entangling_error(match_id) | ||
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return depol_errors | ||
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def build_noise_models(self) -> List['cirq.NoiseModel']: | ||
"""Construct all NoiseModels associated with NoiseProperties.""" | ||
noise_models = super().build_noise_models() | ||
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# Insert entangling gate coherent errors after thermal error. | ||
if self.fsim_errors: | ||
fsim_ops = {op_id: gate.on(*op_id.qubits) for op_id, gate in self.fsim_errors.items()} | ||
noise_models.insert(1, devices.InsertionNoiseModel(ops_added=fsim_ops)) | ||
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return noise_models | ||
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class NoiseModelFromGoogleNoiseProperties(devices.NoiseModelFromNoiseProperties): | ||
"""A noise model defined from noise properties of a Google device.""" | ||
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def is_virtual(self, op: cirq.Operation) -> bool: | ||
return isinstance(op.gate, cirq.ZPowGate) and cirq_google.PhysicalZTag not in op.tags | ||
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# noisy_moments is implemented by the superclass. |
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