Efficient Quantum Simulation Algorithms in the Path Integral Formulation

TL;DR

This paper introduces new quantum algorithms for simulating systems using path integral formulations, demonstrating efficiency improvements and potential applications to quantum field theories.

Contribution

It presents three novel quantum algorithms based on path integrals, including Hamiltonian and Lagrangian formulations, with rigorous derivations and complexity analyses.

Findings

Hamiltonian path integral method scales as $t^{o(1)}/\epsilon^{o(1)}$

Long-time path integral approach scales as $O(1/\sqrt{\epsilon})$

Lagrangian simulation scales as $\widetilde{O}(\eta D t^2/\epsilon)$ for systems with $\eta$ particles

Abstract

We provide a new paradigm for quantum simulation that is based on path integration that allows quantum speedups to be observed for problems that are more naturally expressed using the path integral formalism rather than the conventional sparse Hamiltonian formalism. We provide two novel quantum algorithms based on Hamiltonian versions of the path integral formulation and another for Lagrangians of the form $\frac{m}{2}\dot{x}^2 - V(x)$. This Lagrangian path integral algorithm is based on a new rigorous derivation of a discrete version of the Lagrangian path integral. Our first Hamiltonian path integral method breaks up the paths into short timesteps. It is efficient under appropriate sparsity assumptions and requires a number of queries to oracles that give the eigenvalues and overlaps between the eigenvectors of the Hamiltonian terms that scales as $t^{o(1)}/\epsilon^{o(1)}$ for simulation time $t$ and error $\epsilon$. The second approach uses long-time path integrals for near-adiabatic systems and has query complexity that scales as $O(1/\sqrt{\epsilon})$ if the energy eigenvalue gaps and simulation time is sufficiently long. Finally, we show that our Lagrangian simulation algorithm requires a number of queries to an oracle that computes the discrete Lagrangian that scales for a system with $\eta$ particles in $D+1$ dimensions, in the continuum limit, as $\widetilde{O}(\eta D t^2/\epsilon)$ if $V(x)$ is bounded and finite and the wave function obeys appropriate position and momentum cutoffs. This shows that Lagrangian dynamics can be efficiently simulated on quantum computers and opens up the possibility for quantum field theories for which the Hamiltonian is unknown to be efficiently simulated on quantum computers.