Second Josephson excitations beyond mean field as a toy model for thermal pressure: exact quantum dynamics and the quantum phase model

TL;DR

This paper investigates a four-mode Bose-Hubbard model beyond mean field, revealing a second Josephson excitation and its relation to thermal pressure, with exact quantum dynamics aligning with classical predictions across various parameters.

Contribution

It introduces a detailed analysis of second Josephson excitations beyond mean field and connects them to thermal pressure using a quantum phase model.

Findings

Good agreement between quantum and mean field dynamics over many parameters

Second Josephson frequency becomes imaginary indicating instability

High-energy quasiparticles localize, modeling thermal pressure

Abstract

A simple four-mode Bose-Hubbard model with intrinsic time scale separation can be considered as a paradigm for mesoscopic quantum systems in thermal contact. In our previous work we showed that in addition to coherent particle exchange, a novel slow collective excitation can be identified by a series of Holstein-Primakoff transformations. This resonant energy exchange mode is not predicted by linear Bogoliubov theory, and its frequency is sensitive to interactions among Bogoliubov quasi-particles; it may be referred to as a second Josephson oscillation, in analogy to the second sound mode of liquid Helium II. In this paper we will explore this system beyond the Gross-Pitaevskii mean field regime. We directly compare the classical mean field dynamics to the exact full quantum many-particle dynamics and show good agreement over a large range of the system parameters. The second Josephson frequency becomes imaginary for stronger interactions, however, indicating dynamical instability of the symmetric state. By means of a generalized quantum phase model for the full four-mode system, we then show that, in this regime, high-energy Bogoliubov quasiparticles tend to accumulate in one pair of sites, while the actual particles preferentially occupy the opposite pair. We interpret this as a simple model for thermal pressure.