Short-depth circuits for efficient expectation-value estimation

A. Roggero, A. Baroni

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13 Scopus citations

Abstract

The evaluation of expectation values TrρO for some pure state ρ and Hermitian operator O is of central importance in a variety of quantum algorithms. Near-optimal techniques have been developed in the past and require a number of measurements N approaching the Heisenberg limit N=O1/ϵ as a function of target accuracy ϵ. The use of quantum phase estimation (QPE) requires, however, long circuit depths C=O1/ϵ making its implementation difficult on near-term noisy devices. The more direct strategy of operator averaging is usually preferred as it can be performed using N=O1/ϵ2 measurements and no additional gates aside from those needed for the state preparation. In this work we use a simple but realistic model to describe the bound state of a neutron and a proton (the deuteron) to show that the latter strategy can require an overly large number of measurements in order to achieve a prefixed relative target accuracy ϵr. We propose to overcome this problem using a single step of QPE and classical postprocessing. This approach leads to a circuit depth C=Oϵμ (with μ≥0) and to a number of measurements N=O1/ϵ2+ν for 0<ν≤1 and a much smaller prefactor. We provide detailed descriptions of two implementations of our strategy for ν=1 and ν≈0.5 and derive appropriate conditions that a particular problem instance has to satisfy in order for our method to provide an advantage.

Original languageEnglish
Article number022328
JournalPhysical Review A
Volume101
Issue number2
DOIs
StatePublished - Feb 2020
Externally publishedYes

Funding

We wish to thank N. Klco and R. Schiavilla for helpful discussions regarding the subject of this work. We also thank A. Matsuura of Intel Labs for useful conversations and for encouragements. The work of A.R. was supported by the US Department of Energy, Office of Science, Office of Advanced Scientific Computing Research (ASCR) quantum algorithm teams program under field work Proposal No. ERKJ333 and by US Department of Energy Grant No. DE-FG02-00ER41132. We are also grateful to the T2 group at Los Alamos National Laboratory for the hospitality while working on this project thanks in part to funds from the US Department of Energy, Office of Science, HEP Contract No. DE-KA2401032. A.B. acknowledges support from US Department of Energy, Office of Science, Office of Nuclear Physics, under Awards No. DE-SC0010300 and No. DE-SC0019647.

FundersFunder number
Office of Nuclear PhysicsDE-SC0010300
US Department of Energy
Office of Science
Advanced Scientific Computing ResearchERKJ333

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