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Implement quantum phase estimation algorithms (Qiskit#5642)
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* 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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jlapeyre and Cryoris authored Mar 25, 2021
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21 changes: 21 additions & 0 deletions qiskit/algorithms/__init__.py
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QAOA
VQE
Phase Estimators
++++++++++++++++
Algorithms that estimate the phases of eigenstates of a unitary.
.. autosummary::
:toctree: ../stubs/
:nosignatures:
HamiltonianPhaseEstimation
HamiltonianPhaseEstimationResult
PhaseEstimationScale
PhaseEstimation
PhaseEstimationResult
Exceptions
==========
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from .minimum_eigen_solvers import (VQE, VQEResult, QAOA,
NumPyMinimumEigensolver,
MinimumEigensolver, MinimumEigensolverResult)
from .phase_estimators import (HamiltonianPhaseEstimation, HamiltonianPhaseEstimationResult,
PhaseEstimationScale, PhaseEstimation, PhaseEstimationResult)
from .exceptions import AlgorithmError

__all__ = [
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'NumPyMinimumEigensolver',
'MinimumEigensolver',
'MinimumEigensolverResult',
'HamiltonianPhaseEstimation',
'HamiltonianPhaseEstimationResult',
'PhaseEstimationScale',
'PhaseEstimation',
'PhaseEstimationResult',
'AlgorithmError',
]
29 changes: 29 additions & 0 deletions qiskit/algorithms/phase_estimators/__init__.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.

"""Phase Estimators."""

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

__all__ = [
'PhaseEstimator',
'PhaseEstimation',
'PhaseEstimationResult',
'PhaseEstimationScale',
'HamiltonianPhaseEstimation',
'HamiltonianPhaseEstimationResult'
]
211 changes: 211 additions & 0 deletions 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.

"""Phase estimation for the spectrum of a Hamiltonian"""

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


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>`_
"""

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)

def _get_scale(self, hamiltonian, bound=None) -> None:
if bound is None:
return PhaseEstimationScale.from_pauli_sum(hamiltonian)

return PhaseEstimationScale(bound)

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

# 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()

# 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)}')

if isinstance(hamiltonian, PauliSumOp):
hamiltonian = hamiltonian.to_pauli_op()
elif isinstance(hamiltonian, PauliOp):
hamiltonian = SummedOp([hamiltonian])

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)

# get the rescaling object
pe_scale = self._get_scale(hamiltonian_no_id, bound)

# get the unitary
unitary = self._get_unitary(hamiltonian_no_id, pe_scale, evolution)

elif isinstance(hamiltonian, MatrixOp):
if bound is None:
raise ValueError('bound must be specified if Hermitian operator is MatrixOp')

# 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.')

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)

return HamiltonianPhaseEstimationResult(
phase_estimation_result=phase_estimation_result,
id_coefficient=id_coefficient,
phase_estimation_scale=pe_scale)


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

return idcoeff, SummedOp(ops)
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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.

"""Result from running HamiltonianPhaseEstimation"""


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


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`.
"""

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

# 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`.')

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)

@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

@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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