On the quantum dynamics of long-ranged Bose-Hubbard Hamiltonians
Marius Lemm, Carla Rubiliani, Jingxuan Zhang
TL;DR
The paper tackles the challenge of understanding quantum dynamics in long-range Bose-Hubbard systems with power-law decays, aiming to prove propagation bounds that are uniform in the thermodynamic limit. It develops and applies a multiscale ASTLO (adiabatic space-time localization observables) framework to handle unbounded, long-range hopping and interactions, delivering a sharp uniform particle transport bound for exponents $\\alpha>d+1$ and a thermodynamically stable Lieb-Robinson bound under particle-free shell conditions. A key methodological advance is the logarithmically renormalized ASTLO and a multiscale induction that yields rigorous control over all moments and a light-cone approximation, establishing fixed-speed propagation independent of the total particle number. The results strengthen the locality intuition for long-range, strongly interacting bosonic systems and provide a versatile toolkit for analyzing macroscopic quantum dynamics in high-dimensional, strongly coupled settings. The findings have potential implications for quantum simulations with ultracold atoms in optical lattices, where long-range effects and large system sizes are relevant, and they contribute to the rigorous foundations of dynamical locality in many-body quantum physics.
Abstract
We study the quantum dynamics generated by Bose-Hubbard Hamiltonians with long-ranged (power law) terms. We prove two ballistic propagation bounds for suitable initial states: (i) A bound on all moments of the local particle number for all power law exponents $α>d+1$ in $d$ dimensions, the sharp condition. (ii) The first thermodynamically stable Lieb-Robinson bound (LRB) for these Hamiltonians. To handle the long-ranged and unbounded terms, we further develop the multiscale ASTLO (adiabatic space time localization observables) method introduced in our recent work [arXiv:2310.14896].
