Concentration bounds for quantum states with finite correlation length on quantum spin lattice systems

Abstract:

We consider the problem of determining the energy distribution of quantum states that satisfy exponential decay of correlation and product states, with respect to a quantum local Hamiltonian on a spin lattice. For a quantum state on a D-dimensional lattice that has correlation length σ and has average energy e with respect to a given local Hamiltonian (with n local terms, each of which has norm at most 1), we show that the overlap of this state with eigenspace of energy f is at most $\exp {(-({(e-f)}^{2}\sigma )}^{\tfrac{1}{D+1}}/{n}^{\tfrac{1}{D+1}}D\sigma )$. This bound holds whenever $| e-f| \gt {2}^{D}\sqrt{n\sigma }$. Thus, on a one-dimensional lattice, the tail of the energy distribution decays exponentially with the energy. For product states, we improve above result to obtain a Gaussian decay in energy, even for quantum spin systems without an underlying lattice structure. Given a product state on a collection of spins which has average energy e with respect to a local Hamiltonian (with n local terms and each local term overlapping with at most m other local terms), we show that the overlap of this state with eigenspace of energy f is at most $\exp (-{(e-f)}^{2}/{{nm}}^{2})$. This bound holds whenever $| e-f| \gt m\sqrt{n}$.
Last updated on 11/16/2021