For bosons on a lattice, the mean-field approximation error far from the initial condensate is bounded by any inverse power of the distance for times up to a distance-dependent light cone.
Upper bounds in non-autonomous quantum dynamics
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abstract
We prove upper bounds on outside probabilities for generic non-autonomous Schr\"odinger operators on lattices of arbitrary dimension. Our approach is based on a combination of commutator method originated in scattering theory and novel monotonicity estimate for certain mollified asymptotic observables that track the spacetime localization of evolving states. Sub-ballistic upper bounds are obtained, assuming that momentum vanishes sufficiently fast in the front of the wavepackets. A special case gives a refinement of the general ballistic upper bound of Radin-Simon's, showing that the evolution of wavepackets are effectively confined to a strictly linear light cone with explicitly bounded slope. All results apply to long-range Hamiltonian with polynomial decaying off-diagonal terms and can be extended, via a frozen-coefficient argument, to generic nonlinear Schr\"odinger equations on lattices.
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Local enhancement of the mean-field approximation for bosons
For bosons on a lattice, the mean-field approximation error far from the initial condensate is bounded by any inverse power of the distance for times up to a distance-dependent light cone.