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Implement quantum phase estimation algorithms (Qiskit#5642)
* Add PhaseEstimator and related classes * Fix linter complaints * Update qiskit/algorithms/phase_estimators/hamiltonian_phase_estimation.py Co-authored-by: Julien Gacon <gaconju@gmail.com> * Fix indentation in doc string * Fix more indentation in doc string * Comment on reasons for removing identity term from Hamiltonian * Replace mistaken description "water" by "H2" * Add default phase shift of 0.0 for identity term * Remove function call from default arg Replace default arg with None, and then set the desired default in the body of the function. * Refactor _run and rename to _result Move all common code out of _run for HamiltonianPhaseEstimation and PhaseEstimation, and rename _run to _result, because it only creates the result class. * Move some inputs and calculation to estimate method * Add cutoff to filter in test_from_bound * An unknown change in the past three weeks caused tests to fail with the default filter threshold of 0 (no filtering). I added a small cutoff so that the tests pass again. * Fix linter complaints * Fix linter complaints * Allow PauliSumOp as input Hamiltonian * Make suggested changes * Move module method to classmethod * Fix indentation * Refactor scale_phase scale_phases * Make HamiltonianPhaseEstimation have a hasa rather than isa use of PE * Remove all computation from PhaseEstimator * Remove ability to set number of computation qubits in PhaseEstimator.estimate() * update to current algorithm paradigm + small fixes * make algorithms stateless (store no problem information) * fix lint and docstrings * fix cyclic imports * Use PauliTrotterEvolution by default in HamiltonianPhaseEstimation * Make HamiltonianPhaseEstmation take a StateFn for state preparation * Add method most_likely_phase to HamiltonianPhaseEstimation * Allow PauliOp as input unitary to HPE * Allow MatrixOp as input Hermitian op to HPE * Fix linter complaints * fix evolution = None case * refactor tests slightly * be explicit about which evolution is used * combine tests using ddt * add some linebreaks * fix import order * Improve docstrings for PE and HPE * attempt to fix sphinx * attempt to fix sphinx #2 * attempt no. 3 to fix sphinx * layout, don't use function calls in defaults * trailing comma Co-authored-by: Julien Gacon <gaconju@gmail.com>
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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, PauliTrotterEvolution, OperatorBase, | ||
SummedOp, PauliOp, MatrixOp, PauliSumOp, StateFn) | ||
from qiskit.providers import BaseBackend | ||
from .phase_estimation import PhaseEstimation | ||
from .hamiltonian_phase_estimation_result import HamiltonianPhaseEstimationResult | ||
from .phase_estimation_scale import PhaseEstimationScale | ||
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class HamiltonianPhaseEstimation: | ||
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.PhaseEstimation`, 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`. | ||
The problem of estimating eigenvalues :math:`\lambda_j` of the Hermitian operator | ||
:math:`H` is solved by running a circuit representing | ||
.. math:: | ||
\exp(i b H) |\psi\rangle = \sum_j \exp(i b \lambda_j) c_j |\lambda_j\rangle, | ||
where the input state is | ||
.. math:: | ||
|\psi\rangle = \sum_j c_j |\lambda_j\rangle, | ||
and :math:`\lambda_j` are the eigenvalues of :math:`H`. | ||
Here, :math:`b` is a scaling factor sufficiently large to map positive :math:`\lambda` to | ||
:math:`[0,\pi)` and negative :math:`\lambda` to :math:`[\pi,2\pi)`. Each time the circuit is | ||
run, one measures a phase corresponding to :math:`lambda_j` with probability :math:`|c_j|^2`. | ||
If :math:`H` is a Pauli sum, the bound :math:`b` is computed from the sum of the absolute | ||
values of the coefficients of the terms. There is no way to reliably recover eigenvalues | ||
from phases very near the endpoints of these intervals. Because of this you should be aware | ||
that for degenerate cases, such as :math:`H=Z`, the eigenvalues :math:`\pm 1` will be | ||
mapped to the same phase, :math:`\pi`, and so cannot be distinguished. In this case, you need | ||
to specify a larger bound as an argument to the method ``estimate``. | ||
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 | ||
`arXiv:1809.09697 <https://arxiv.org/abs/1809.09697>`_ | ||
""" | ||
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def __init__(self, | ||
num_evaluation_qubits: int, | ||
quantum_instance: Optional[Union[QuantumInstance, BaseBackend]] = 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. | ||
quantum_instance: The quantum instance on which the circuit will be run. | ||
""" | ||
self._phase_estimation = PhaseEstimation( | ||
num_evaluation_qubits=num_evaluation_qubits, | ||
quantum_instance=quantum_instance) | ||
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def _get_scale(self, hamiltonian, bound=None) -> None: | ||
if bound is None: | ||
return PhaseEstimationScale.from_pauli_sum(hamiltonian) | ||
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return PhaseEstimationScale(bound) | ||
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def _get_unitary(self, hamiltonian, pe_scale, evolution) -> 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 = -pe_scale.scale * hamiltonian | ||
unitary = 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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# pylint: disable=arguments-differ | ||
def estimate(self, hamiltonian: OperatorBase, | ||
state_preparation: Optional[StateFn] = None, | ||
evolution: Optional[EvolutionBase] = None, | ||
bound: Optional[float] = None) -> HamiltonianPhaseEstimationResult: | ||
"""Run the Hamiltonian phase estimation algorithm. | ||
Args: | ||
hamiltonian: A Hermitian operator. | ||
state_preparation: The ``StateFn`` to be prepared, 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. | ||
evolution: An evolution converter that generates a unitary from ``hamiltonian``. If | ||
``None``, then the default ``PauliTrotterEvolution`` is used. | ||
bound: An upper bound on the absolute value of the eigenvalues of | ||
``hamiltonian``. If omitted, then ``hamiltonian`` must be a Pauli sum, or a | ||
``PauliOp``, in which case a bound will be computed. If ``hamiltonian`` | ||
is a ``MatrixOp``, then ``bound`` may not be ``None``. The tighter the bound, | ||
the higher the resolution of computed phases. | ||
Returns: | ||
HamiltonianPhaseEstimationResult instance containing the result of the estimation | ||
and diagnostic information. | ||
Raises: | ||
ValueError: If ``bound`` is ``None`` and ``hamiltonian`` is not a Pauli sum, i.e. a | ||
``PauliSumOp`` or a ``SummedOp`` whose terms are of type ``PauliOp``. | ||
TypeError: If ``evolution`` is not of type ``EvolutionBase``. | ||
""" | ||
if evolution is None: | ||
evolution = PauliTrotterEvolution() | ||
elif not isinstance(evolution, EvolutionBase): | ||
raise TypeError(f'Expecting type EvolutionBase, got {type(evolution)}') | ||
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if isinstance(hamiltonian, PauliSumOp): | ||
hamiltonian = hamiltonian.to_pauli_op() | ||
elif isinstance(hamiltonian, PauliOp): | ||
hamiltonian = SummedOp([hamiltonian]) | ||
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if isinstance(hamiltonian, SummedOp): | ||
# remove identitiy terms | ||
# The term propto the identity is removed from hamiltonian. | ||
# This is done for three reasons: | ||
# 1. Work around an unknown bug that otherwise causes the energies to be wrong in some | ||
# cases. | ||
# 2. Allow working with a simpler Hamiltonian, one with fewer terms. | ||
# 3. Tighten the bound on the eigenvalues so that the spectrum is better resolved, i.e. | ||
# occupies more of the range of values representable by the qubit register. | ||
# The coefficient of this term will be added to the eigenvalues. | ||
id_coefficient, hamiltonian_no_id = _remove_identity(hamiltonian) | ||
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# get the rescaling object | ||
pe_scale = self._get_scale(hamiltonian_no_id, bound) | ||
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# get the unitary | ||
unitary = self._get_unitary(hamiltonian_no_id, pe_scale, evolution) | ||
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elif isinstance(hamiltonian, MatrixOp): | ||
if bound is None: | ||
raise ValueError('bound must be specified if Hermitian operator is MatrixOp') | ||
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# Do not subtract an identity term from the matrix, so do not compensate. | ||
id_coefficient = 0.0 | ||
pe_scale = self._get_scale(hamiltonian, bound) | ||
unitary = self._get_unitary(hamiltonian, pe_scale, evolution) | ||
else: | ||
raise TypeError(f'Hermitian operator of type {type(hamiltonian)} not supported.') | ||
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if state_preparation is not None: | ||
state_preparation = state_preparation.to_circuit_op().to_circuit() | ||
# run phase estimation | ||
phase_estimation_result = self._phase_estimation.estimate( | ||
unitary=unitary, state_preparation=state_preparation) | ||
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return HamiltonianPhaseEstimationResult( | ||
phase_estimation_result=phase_estimation_result, | ||
id_coefficient=id_coefficient, | ||
phase_estimation_scale=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 | ||
from qiskit.algorithms.algorithm_result import AlgorithmResult | ||
from .phase_estimation_result import PhaseEstimationResult | ||
from .phase_estimation_scale import PhaseEstimationScale | ||
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class HamiltonianPhaseEstimationResult(AlgorithmResult): | ||
"""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. | ||
This class is meant to be instantiated via `HamiltonianPhaseEstimation.estimate`. | ||
""" | ||
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def __init__(self, | ||
phase_estimation_result: PhaseEstimationResult, | ||
phase_estimation_scale: PhaseEstimationScale, | ||
id_coefficient: float, | ||
) -> None: | ||
""" | ||
Args: | ||
phase_estimation_result: The result object returned by PhaseEstimation.estimate. | ||
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. | ||
""" | ||
super().__init__() | ||
self._phase_estimation_scale = phase_estimation_scale | ||
self._id_coefficient = id_coefficient | ||
self._phase_estimation_result = phase_estimation_result | ||
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# pylint: disable=arguments-differ | ||
def filter_phases(self, cutoff: float = 0.0, scaled: bool = True, | ||
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 = self._phase_estimation_result.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_phase(self) -> float: | ||
"""The most likely phase of the unitary corresponding to the Hamiltonian. | ||
Returns: | ||
The most likely phase. | ||
""" | ||
return self._phase_estimation_result.most_likely_phase | ||
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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 = self._phase_estimation_result.most_likely_phase | ||
return self._phase_estimation_scale.scale_phase(phase, self._id_coefficient) |
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