Abstract

Quantum simulation has wide applications in quantum chemistry and physics. Recently, scientists have begun exploring the use of randomized methods for accelerating quantum simulation. Among them, a simple and powerful technique, called qDRIFT, is known to generate random product formulas for which the average quantum channel approximates the ideal evolution. qDRIFT achieves a gate count that does not explicitly depend on the number of terms in the Hamiltonian, which contrasts with Suzuki formulas. This work aims to understand the origin of this speed-up by comprehensively analyzing a single realization of the random product formula produced by qDRIFT. The main results prove that a typical realization of the randomized product formula approximates the ideal unitary evolution up to a small diamond-norm error. The gate complexity is already independent of the number of terms in the Hamiltonian, but it depends on the system size and the sum of the interaction strengths in the Hamiltonian. Remarkably, the same random evolution starting from an arbitrary, but fixed, input state yields a much shorter circuit suitable for that input state. In contrast, in deterministic settings, such an improvement usually requires initial state knowledge. The proofs depend on concentration inequalities for vector and matrix martingales, and the framework is applicable to other randomized product formulas. Our bounds are saturated by certain commuting Hamiltonians.

Highlights

  • Simulating complex quantum systems is one of the most promising applications for quantum computers

  • This work aims to understand the origin of this speedup by comprehensively analyzing a single realization of the random product formula produced by QDRIFT

  • This work shows interesting characteristics of randomization that might help to further improve quantum simulation. (a) By studying typical unitary instances of QDRFIT, we have shown that L independence of QDRIFT attributes to randomly sampling terms; mixing different realizations is not essential. (b) Gate complexities can be reduced substantially by restricting attention to a particular input state or/and target observable

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Summary

Introduction

Simulating complex quantum systems is one of the most promising applications for quantum computers. This task has many applications, such as developing new pharmaceuticals, catalysts, and materials [1,2,3], as well as solving linear algebra problems [4,5,6]. The task of digital quantum (dynamics) simulation can be phrased as a compiling problem: approximate a given unitary, say a Hamiltonian evolution U = e−iHt, by a product of “simple” unitaries gk:. Several cost functions make sense in this context, but we focus on the gate complexity, i.e., the number N of simple gates [8] on the right-hand side of Eq (1)

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