
Simulations
contributed
Tue, 1 Sep 2026, 11:00 - 12:30
- Quantum simulation of chemistry via quantum fast multipole methodDominic Berry (Macquarie University); Kianna Wan (Stanford University); Andrew Baczewski (Sandia National Laboratories); Elliot Eklund (University of Sydney); Arkin Tikku (University of Sydney); Ryan Babbush (Google Quantum AI)[abstract]Abstract: Here we describe an approach for simulating quantum chemistry on quantum computers with significantly lower asymptotic complexity than prior work. The approach uses a real-space first-quantised representation of the molecular Hamiltonian which we propagate using high-order product formulae. Essential for this low complexity is the use of a technique similar to the fast multipole method for computing the Coulomb operator with O(eta) complexity for a simulation with eta particles. We show how to modify this algorithm so that it can be implemented on a quantum computer. We ultimately demonstrate an approach with t(eta^{4/3} N^{1/3} + eta^{1/3} N^{2/3})(eta Nt/epsilon)^o(1) gate complexity, where N is the number of grid points, epsilon is target precision, and t is the duration of time evolution. This is roughly a speedup by O(eta) over most prior algorithms. We provide lower complexity than all prior work for N<eta^7 (the regime of practical interest), with only first-quantised interaction-picture simulations providing better performance for N>eta^7. As with the classical fast multipole method, large numbers eta>10^3 would be needed to realise this advantage.
- Quantum lower bounds for simulating fluid dynamicsAbtin Ameri (MIT); Joseph Carolan (University of Maryland); Andrew M. Childs (University of Maryland); Hari Krovi (IBM Quantum)[abstract]Abstract: Developing quantum algorithms to simulate fluid dynamics has become an active area of research, as accelerating fluid simulations could have significant impact in industry and fundamental science. While many approaches have been proposed for simulating fluid dynamics on quantum computers, it is largely unclear whether these algorithms will provide any speedup over existing classical approaches. In this paper we give evidence that quantum computers cannot significantly outperform classical simulations of fluid dynamics in general. We study two models of fluids: the Korteweg-de Vries (KdV) equation, which models shallow water waves, and the incompressible Euler equations, which model ideal, inviscid fluids. We show that any quantum algorithm simulating the KdV equation or the Euler equations for time T requires Ω(T^2) and exp(Ω(T)) copies of the initial state in the worst case, respectively. These lower bounds hold for the task of preparing the final state, and similar bounds hold for history state preparation. We prove the lower bound for the KdV equation by investigating divergence of solitons. For the Euler equations, we show that instabilities can accelerate state discrimination.
- Rapid Mixing of Quantum Gibbs Samplers for Weakly-Interacting Quantum SystemsŠtěpán Šmíd (Imperial College London); Richard Meister (Imperial College London); Mario Berta (RWTH Aachen University); Roberto Bondesan (Imperial College London)[abstract]Abstract: Dissipative quantum algorithms for state preparation in many-body systems are increasingly recognised as promising candidates for achieving large quantum advantages in application-relevant tasks. Recent advances in algorithmic, detailed-balance Lindbladians enable the efficient simulation of open-system dynamics converging towards desired target states. However, the overall complexity of such schemes is governed by system-size dependent mixing times. In this work, we analyse algorithmic Lindbladians for Gibbs state preparation and prove that they exhibit rapid mixing, i.e., convergence in time poly-logarithmic in the system size. We first establish this for non-interacting spin systems, free fermions, and free bosons, and then show that these rapid mixing results are stable under perturbations, covering weakly interacting qudits and perturbed non-hopping fermions. Further, we adapt the techniques from separable qudits to the fermionic setting and prove rapid mixing of the strongly-interacting regime of the Fermi-Hubbard model. Our results constitute the first efficient mixing bounds for non-commuting qudit models and bosonic systems at arbitrary temperatures. Compared to prior spectral-gap-based results for fermions, we achieve exponentially faster mixing, further featuring explicit constants on the maximal allowed interaction strength. This not only improves the overall polynomial runtime for quantum Gibbs state preparation, but also enhances robustness against noise. Our analysis relies on oscillator norm techniques from mathematical physics, where we introduce tailored variants adapted to specific Lindbladians - an innovation that we expect to significantly broaden the scope of these methods.
