Scalable Distributed Memory Implementation of the Quasi-Adiabatic Propagator Path Integral

TL;DR

This paper introduces a scalable distributed memory implementation of the MACGIC-QUAPI method for simulating dissipative quantum dynamics in structured non-Markovian environments, enabling large-scale, accurate simulations of complex quantum systems.

Contribution

It develops a distributed memory version of MACGIC-QUAPI with a new pre-merging algorithm, allowing efficient large-scale quantum dynamics simulations while maintaining accuracy.

Findings

Demonstrates efficient large-scale simulations of structured environments.

Reveals resonance splitting and sidebands due to strong system-environment coupling.

Shows the method's applicability to non-perturbative quantum dynamics.

Abstract

The accurate simulation of dissipative quantum dynamics subject to a non-Markovian environment poses persistent numerical challenges, in particular for structured environments where sharp mode resonances induce long-time system bath correlations. We present a scalable distributed memory implementation of the Mask Assisted Coarse Graining of Influence Coefficients (MACGIC) - Quasi-Adiabatic Propagator Path Integral (-QUAPI) method that exploits the memory resources of multiple compute nodes and mitigates the memory bottleneck of the method via a new pre-merging algorithm while preserving numerical accuracy. The distributed memory implementation spreads the paths over the computing nodes by means of the MPI protocoll and efficient high level path management is achieved via an implementation based on hash maps. The efficiency of the new implementation is demonstrated in large-scale dissipative quantum dynamics simulations that account for the coupling to a structured non-Markovian environment containing a sharp resonance, a setup for which convergence properties are investigated in depth. Broad applicability and the non-perturbative nature of the simulation method is illustrated via the tuning of the mode resonance frequency of the structured environment with respect to the system frequency. The simulations reveal a splitting of resonances due to strong system-environment interaction and the emergence of sidebands due to multi-excitations of the bosonic mode that are not accounted for in perturbative approaches. The simulations demonstrate the versatility of the new MACGIC-QUAPI method in the presence of strong non-Markovian system bath correlations.