Understand
We show that excitations of interacting quantum particles in lattice models always propagate with a finite speed of sound.
- Our argument is simple yet general and shows that by focusing on the physically relevant observables one can generally expect a bounded speed of information propagation.
- The argument applies equally to quantum spins, bosons such as in the Bose-Hubbard model, fermions, anyons, and general mixtures thereof, on arbitrary lattices of any dimension.
- It also pertains to dissipative dynamics on the lattice, and generalizes to the continuum for quantum fields.
Built on
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A. Albus, F. Illuminati, and J. Eisert, Phys. Rev. A 68
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M. B. Hastings, Phys. Rev. B 69
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M. Cramer and J. Eisert, New J. Phys. 8
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There are two ways to obtain better bounds on the velocity. First, we can bound x y ≤ 1 2 ( λ x + y / λ ) \sqrt{xy}\leq\frac{1}{2}(\lambda x+y/\lambda) , which gives a velocity bound λ v 0 + 𝒟 τ / λ \lambda v_{0}+\mathcal{D}\tau/\lambda for any λ > 0 \lambda>0 . Second, one can solve the non-linear differential inequality ( 4
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Then
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