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Improving the t^{D−1} Lieb–Robinson scaling for the standard Bose–Hubbard model (p=2) in low dimensions

Determine whether, for the standard Bose–Hubbard model with quadratic on-site interaction (p = 2) in spatial dimensions D ≤ 3 and for broad classes of initial states, the known Lieb–Robinson bound with velocity scaling v ∼ t^{D−1} can be qualitatively improved to a strictly smaller time exponent (e.g., v ∼ t^α with α < D−1).

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Background

The paper improves known bounds under higher-order on-site repulsion and translation invariance, but explicitly notes that the most relevant p=2 case lies beyond the current techniques. For p=2 in low dimensions, whether the general v ∼ t{D−1} upper bound can be tightened remains unsettled.

Clarifying this would delineate the true light-cone structure for the standard Bose–Hubbard model in physically relevant dimensions and for broad initial-state classes.

References

it is not clear at all, even at a physical level, if the LRB from can be improved for the original Bose-Hubbard model with $p=2$ in the most interesting regime of $D\leq 3$ for a broad class of initial states.

Enhanced Lieb-Robinson bounds for a class of Bose-Hubbard type Hamiltonians (2405.04672 - Kuwahara et al., 7 May 2024) in Discussion, Section 1.3