Source code for pennylane.resource.measurement

# Copyright 2018-2022 Xanadu Quantum Technologies Inc.

# Licensed under the Apache License, Version 2.0 (the "License");
# you may not use this file except in compliance with the License.
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"""
This module contains the functions needed for estimating the number of measurements and the error
for computing expectation values.
"""
import numpy as np


[docs]def estimate_shots(coeffs, variances=None, error=0.0016): r"""Estimate the number of measurements required to compute an expectation value with a target error. See also :func:`estimate_error`. Args: coeffs (list[tensor_like]): list of coefficient groups variances (list[float]): variances of the Pauli word groups error (float): target error in computing the expectation value Returns: int: the number of measurements **Example** >>> coeffs = [np.array([-0.32707061, 0.7896887]), np.array([0.18121046])] >>> qml.resource.estimate_shots(coeffs) 419218 .. details:: :title: Theory An estimation for the number of measurements :math:`M` required to predict the expectation value of an observable :math:`H = \sum_i A_i`, with :math:`A = \sum_j c_j O_j` representing a linear combination of Pauli words, can be obtained following Eq. (34) of [`PRX Quantum 2, 040320 (2021) <https://journals.aps.org/prxquantum/abstract/10.1103/PRXQuantum.2.040320>`_] as .. math:: M = \frac{\left ( \sum_i \sqrt{\text{Var}(A_i)} \right )^2}{\epsilon^2}, with :math:`\epsilon` and :math:`\text{Var}(A)` denoting the target error in computing :math:`\left \langle H \right \rangle` and the variance in computing :math:`\left \langle A \right \rangle`, respectively. It has been shown in Eq. (10) of [`arXiv:2201.01471v3 <https://arxiv.org/abs/2201.01471v3>`_] that the variances can be computed from the covariances between the Pauli words as .. math:: \text{Var}(A_i) = \sum_{jk} c_j c_k \text{Cov}(O_j, O_k), where .. math:: \text{Cov}(O_j, O_k) = \left \langle O_j O_k \right \rangle - \left \langle O_j \right \rangle \left \langle O_k \right \rangle. The values of :math:`\text{Cov}(O_j, O_k)` are not known a priori and should be either computed from affordable classical methods, such as the configuration interaction with singles and doubles (CISD), or approximated with other methods. If the variances are not provided to the function as input, they will be approximated following Eqs. (6-7) of [`Phys. Rev. Research 4, 033154, 2022 <https://journals.aps.org/prresearch/abstract/10.1103/PhysRevResearch.4.033154>`_] by assuming :math:`\text{Cov}(O_j, O_k) =0` for :math:`j \neq k` and using :math:`\text{Var}(O_i) \leq 1` from .. math:: \text{Var}(O_i) = \left \langle O_i^2 \right \rangle - \left \langle O_i \right \rangle^2 = 1 - \left \langle O_i \right \rangle^2. This approximation gives .. math:: M \approx \frac{\left ( \sum_i \sqrt{\sum_j c_{ij}^2} \right )^2}{\epsilon^2}, where :math:`i` and :math:`j` run over the observable groups and the Pauli words inside the group, respectively. """ if variances: return int(np.ceil(np.sum(np.sqrt(variances)) ** 2 / error**2)) group_sum = [np.sum(coeff**2) for coeff in coeffs] return int(np.ceil(np.sum(np.sqrt(group_sum)) ** 2 / error**2))
[docs]def estimate_error(coeffs, variances=None, shots=1000): r"""Estimate the error in computing an expectation value with a given number of measurements. See also :func:`estimate_shots`. Args: coeffs (list[tensor_like]): list of coefficient groups variances (list[float]): variances of the Pauli word groups shots (int): the number of measurements Returns: float: target error in computing the expectation value **Example** >>> coeffs = [np.array([-0.32707061, 0.7896887]), np.array([0.18121046])] >>> qml.resource.estimate_error(coeffs, shots=100000) 0.00327597 .. details:: :title: Theory An estimation for the error :math:`\epsilon` in predicting the expectation value of an observable :math:`H = \sum_i A_i` with :math:`A = \sum_j c_j O_j` representing a linear combination of Pauli words can be obtained following Eq. (34) of [`PRX Quantum 2, 040320 (2021) <https://journals.aps.org/prxquantum/abstract/10.1103/PRXQuantum.2.040320>`_] as .. math:: \epsilon = \frac{\sum_i \sqrt{\text{Var}(A_i)}}{\sqrt{M}}, with :math:`M` and :math:`\text{Var}(A)` denoting the number of measurements and the variance in computing :math:`\left \langle A \right \rangle`, respectively. It has been shown in Eq. (10) of [`arXiv:2201.01471v3 <https://arxiv.org/abs/2201.01471v3>`_] that the variances can be computed from the covariances between the Pauli words as .. math:: \text{Var}(A_i) = \sum_{jk} c_j c_k \text{Cov}(O_j, O_k), where .. math:: \text{Cov}(O_j, O_k) = \left \langle O_j O_k \right \rangle - \left \langle O_j \right \rangle \left \langle O_k \right \rangle. The values of :math:`\text{Cov}(O_j, O_k)` are not known a priori and should be either computed from affordable classical methods, such as the configuration interaction with singles and doubles (CISD), or approximated with other methods. If the variances are not provided to the function as input, they will be approximated following Eqs. (6-7) of [`Phys. Rev. Research 4, 033154, 2022 <https://journals.aps.org/prresearch/abstract/10.1103/PhysRevResearch.4.033154>`_] by assuming :math:`\text{Cov}(O_j, O_k) =0` for :math:`j \neq k` and using :math:`\text{Var}(O_i) \leq 1` from .. math:: \text{Var}(O_i) = \left \langle O_i^2 \right \rangle - \left \langle O_i \right \rangle^2 = 1 - \left \langle O_i \right \rangle^2. This approximation gives .. math:: \epsilon \approx \frac{\sum_i \sqrt{\sum_j c_{ij}^2}}{\sqrt{M}}, where :math:`i` and :math:`j` run over the observable groups and the Pauli words inside the group, respectively. """ if variances: return np.sum(np.sqrt(variances)) / np.sqrt(shots) group_sum = [np.sum(coeff**2) for coeff in coeffs] return np.sum(np.sqrt(group_sum)) / np.sqrt(shots)