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Add PhaseEstimator and related classes
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# This code is part of Qiskit. | ||
# | ||
# (C) Copyright IBM 2020. | ||
# | ||
# This code is licensed under the Apache License, Version 2.0. You may | ||
# obtain a copy of this license in the LICENSE.txt file in the root directory | ||
# of this source tree or at http://www.apache.org/licenses/LICENSE-2.0. | ||
# | ||
# Any modifications or derivative works of this code must retain this | ||
# copyright notice, and modified files need to carry a notice indicating | ||
# that they have been altered from the originals. | ||
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"""Phase Estimators.""" | ||
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from .phase_estimator import PhaseEstimator | ||
from .phase_estimation import PhaseEstimation | ||
from .phase_estimation_result import PhaseEstimationResult | ||
from .phase_estimation_scale import PhaseEstimationScale | ||
from .hamiltonian_phase_estimation import HamiltonianPhaseEstimation | ||
from .hamiltonian_phase_estimation_result import HamiltonianPhaseEstimationResult | ||
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__all__ = [ | ||
'PhaseEstimator', | ||
'PhaseEstimation', | ||
'PhaseEstimationResult', | ||
'PhaseEstimationScale', | ||
'HamiltonianPhaseEstimation', | ||
'HamiltonianPhaseEstimationResult' | ||
] |
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qiskit/algorithms/phase_estimators/hamiltonian_phase_estimation.py
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# This code is part of Qiskit. | ||
# | ||
# (C) Copyright IBM 2020. | ||
# | ||
# This code is licensed under the Apache License, Version 2.0. You may | ||
# obtain a copy of this license in the LICENSE.txt file in the root directory | ||
# of this source tree or at http://www.apache.org/licenses/LICENSE-2.0. | ||
# | ||
# Any modifications or derivative works of this code must retain this | ||
# copyright notice, and modified files need to carry a notice indicating | ||
# that they have been altered from the originals. | ||
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"""Phase estimation for the spectrum of a Hamiltonian""" | ||
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from typing import Optional, Union | ||
from qiskit import QuantumCircuit | ||
from qiskit.utils import QuantumInstance | ||
from qiskit.opflow import EvolutionBase, OperatorBase, SummedOp | ||
from qiskit.providers import BaseBackend, Backend | ||
from .phase_estimation import PhaseEstimation | ||
from . import phase_estimation_scale | ||
from .hamiltonian_phase_estimation_result import HamiltonianPhaseEstimationResult | ||
from .phase_estimation_scale import PhaseEstimationScale | ||
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class HamiltonianPhaseEstimation(PhaseEstimation): | ||
r"""Run the Quantum Phase Estimation algorithm to find the eigenvalues of a Hermitian operator. | ||
This class is nearly the same as :class:`~qiskit.algorithms.PhaseEstimator`, differing only | ||
in that the input in that class is a unitary operator, whereas here the input is a Hermitian | ||
operator from which a unitary will be obtained by scaling and exponentiating. The scaling is | ||
performed in order to prevent the phases from wrapping around :math:`2\pi`. This class uses and | ||
works together with :class:`~qiskit.algorithms.PhaseEstimationScale` to manage scaling the | ||
Hamiltonian and the phases that are obtained by the QPE algorithm. This includes setting, or | ||
computing, a bound on the eigenvalues of the operator, using this bound to obtain a scale | ||
factor, scaling the operator, and shifting and scaling the measured phases to recover the | ||
eigenvalues. | ||
Note that, although we speak of "evolving" the state according the the Hamiltonian, in the | ||
present algorithm, we are not actually considering time evolution. Rather, the role of time is | ||
played by the scaling factor, which is chosen to best extract the eigenvalues of the | ||
Hamiltonian. | ||
A few of the ideas in the algorithm may be found in Ref. [1]. | ||
**Reference:** | ||
[1]: Quantum phase estimation of multiple eigenvalues for small-scale (noisy) experiments | ||
T.E. O'Brien, B. Tarasinski, B.M. Terhal | ||
https://arxiv.org/abs/1809.09697 | ||
""" | ||
def __init__(self, | ||
num_evaluation_qubits: int, | ||
hamiltonian: OperatorBase, | ||
evolution: EvolutionBase, | ||
state_preparation: Optional[QuantumCircuit] = None, | ||
bound: Optional[float] = None, | ||
quantum_instance: Optional[Union[QuantumInstance, | ||
BaseBackend, Backend]] = None) -> None: | ||
""" | ||
Args: | ||
num_evaluation_qubits: The number of qubits used in estimating the phase. The | ||
phase will be estimated as a binary string with this many | ||
bits. | ||
hamiltonian: a Hamiltonian or Hermitian operator | ||
evolution: An evolution object that generates a unitary from `hamiltonian`. | ||
state_preparation: The circuit that prepares the state whose eigenphase will be | ||
measured. If this parameter is omitted, no preparation circuit | ||
will be run and input state will be the all-zero state in the | ||
computational basis. | ||
bound: An upper bound on the absolute value of the eigenvalues of | ||
`hamiltonian`. If omitted, then `hamiltonian` must be a Pauli sum, in which case | ||
then a bound will be computed. | ||
quantum_instance: The quantum instance on which the circuit will be run. | ||
Raises: | ||
ValueError: if `bound` is `None` and `hamiltonian` is not a Pauli sum (i.e. a | ||
`SummedOp` whose terms are `PauliOp`s.) | ||
""" | ||
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self._evolution = evolution | ||
self._bound = bound | ||
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# The term propto the identity is removed from hamiltonian. | ||
# The coefficient of this term will be added to the eigenvalues. | ||
id_coefficient, hamiltonian_no_id = _remove_identity(hamiltonian) | ||
self._hamiltonian = hamiltonian_no_id | ||
self._id_coefficient = id_coefficient | ||
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self._set_scale() | ||
unitary = self._get_unitary() | ||
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super().__init__(num_evaluation_qubits, | ||
unitary=unitary, | ||
pe_circuit=None, | ||
num_unitary_qubits=None, | ||
state_preparation=state_preparation, | ||
quantum_instance=quantum_instance) | ||
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def _set_scale(self) -> None: | ||
if self._bound is None: | ||
pe_scale = phase_estimation_scale.from_pauli_sum(self._hamiltonian) | ||
self._pe_scale = pe_scale | ||
else: | ||
self._pe_scale = PhaseEstimationScale(self._bound) | ||
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def _get_unitary(self) -> QuantumCircuit: | ||
"""Evolve the Hamiltonian to obtain a unitary. | ||
Apply the scaling to the Hamiltonian that has been computed from an eigenvalue bound | ||
and compute the unitary by applying the evolution object. | ||
""" | ||
# scale so that phase does not wrap. | ||
scaled_hamiltonian = -self._pe_scale.scale * self._hamiltonian | ||
unitary = self._evolution.convert(scaled_hamiltonian.exp_i()) | ||
if not isinstance(unitary, QuantumCircuit): | ||
unitary_circuit = unitary.to_circuit() | ||
else: | ||
unitary_circuit = unitary | ||
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# Decomposing twice allows some 1Q Hamiltonians to give correct results | ||
# when using MatrixEvolution(), that otherwise would give incorrect results. | ||
# It does not break any others that we tested. | ||
return unitary_circuit.decompose().decompose() | ||
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def _run(self) -> HamiltonianPhaseEstimationResult: | ||
"""Run the circuit and return and return `HamiltonianPhaseEstimationResult`. | ||
""" | ||
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circuit_result = self._quantum_instance.execute(self.construct_circuit()) | ||
phases = self._compute_phases(circuit_result) | ||
return HamiltonianPhaseEstimationResult( | ||
self._num_evaluation_qubits, phases=phases, id_coefficient=self._id_coefficient, | ||
circuit_result=circuit_result, phase_estimation_scale=self._pe_scale) | ||
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def _remove_identity(pauli_sum): | ||
"""Remove any identity operators from `pauli_sum`. Return | ||
the sum of the coefficients of the identities and the new operator. | ||
""" | ||
idcoeff = 0.0 | ||
ops = [] | ||
for op in pauli_sum: | ||
p = op.primitive | ||
if p.x.any() or p.z.any(): | ||
ops.append(op) | ||
else: | ||
idcoeff += op.coeff | ||
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return idcoeff, SummedOp(ops) |
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qiskit/algorithms/phase_estimators/hamiltonian_phase_estimation_result.py
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# This code is part of Qiskit. | ||
# | ||
# (C) Copyright IBM 2020. | ||
# | ||
# This code is licensed under the Apache License, Version 2.0. You may | ||
# obtain a copy of this license in the LICENSE.txt file in the root directory | ||
# of this source tree or at http://www.apache.org/licenses/LICENSE-2.0. | ||
# | ||
# Any modifications or derivative works of this code must retain this | ||
# copyright notice, and modified files need to carry a notice indicating | ||
# that they have been altered from the originals. | ||
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"""Result from running HamiltonianPhaseEstimation""" | ||
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from typing import Dict, Union, cast | ||
import numpy | ||
from qiskit.result import Result | ||
from .phase_estimation_result import PhaseEstimationResult | ||
from .phase_estimation_scale import PhaseEstimationScale | ||
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class HamiltonianPhaseEstimationResult(PhaseEstimationResult): | ||
"""Store and manipulate results from running `HamiltonianPhaseEstimation`. | ||
This API of this class is nearly the same as `PhaseEstimatorResult`, differing only in | ||
the presence of an additional keyword argument in the methods. If `scaled` | ||
is `False`, then the phases are not translated and scaled to recover the | ||
eigenvalues of the Hamiltonian. Instead `phi` in :math:`[0, 1)` is returned, | ||
as is the case when then unitary is not derived from a Hamiltonian. | ||
""" | ||
def __init__(self, num_evaluation_qubits: int, circuit_result: Result, | ||
phase_estimation_scale: PhaseEstimationScale, | ||
id_coefficient: float, | ||
phases: Union[numpy.ndarray, Dict[str, float]]) -> None: | ||
""" | ||
Args: | ||
num_evaluation_qubits: number of qubits in phase-readout register. | ||
circuit_result: result object returned by method running circuit. | ||
phase_estimation_scale: object used to scale phases to obtain eigenvalues. | ||
id_coefficient: The coefficient of the identity term in the Hamiltonian. | ||
Eigenvalues are computed without this term so that the | ||
coefficient must added to give correct eigenvalues. | ||
This is done automatically when retrieving eigenvalues. | ||
phases: ndarray or dict of phases and frequencies determined by QPE. | ||
""" | ||
self._phase_estimation_scale = phase_estimation_scale | ||
self._id_coefficient = id_coefficient | ||
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super().__init__(num_evaluation_qubits, circuit_result, phases) | ||
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# pylint: disable=arguments-differ | ||
def filter_phases(self, cutoff: float = 0.0, scaled: bool = True, # type: ignore | ||
as_float: bool = True) -> Dict[Union[str, float], float]: | ||
"""Filter phases as does `PhaseEstimatorResult.filter_phases`, with | ||
the addition that `phi` is shifted and translated to return eigenvalues | ||
of the Hamiltonian. | ||
Args: | ||
cutoff: Minimum weight of number of counts required to keep a bit string. | ||
The default value is `0.0`. | ||
scaled: If False, return `phi` in :math:`[0, 1)` rather than the eigenvalues of | ||
the Hamiltonian. | ||
as_float: If `True`, returned keys are floats in :math:`[0.0, 1.0)`. If `False` | ||
returned keys are bit strings. | ||
Raises: | ||
ValueError: if as_float` is `False` and `scaled` is `True`. | ||
Returns: | ||
A dict of filtered phases. | ||
""" | ||
if scaled and not as_float: | ||
raise ValueError('`as_float` must be `True` if `scaled` is `True`.') | ||
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phases = super().filter_phases(cutoff, as_float=as_float) | ||
if scaled: | ||
return cast(Dict, self._phase_estimation_scale.scale_phases(phases, | ||
self._id_coefficient)) | ||
else: | ||
return cast(Dict, phases) | ||
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@property | ||
def most_likely_eigenvalue(self) -> float: | ||
"""The most likely eigenvalue of the Hamiltonian. | ||
This method calls `most_likely_phase` and scales the result to | ||
obtain an eigenvalue. | ||
Returns: | ||
The most likely eigenvalue of the Hamiltonian. | ||
""" | ||
phase = super().most_likely_phase | ||
return self._phase_estimation_scale.scale_phase(phase, self._id_coefficient) |
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