The off-diagonal Eigenstate Thermalization Hypothesis

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Consider energy eigenstates ∣Ei⟩|E_i\rangle and ∣Ej⟩|E_j\rangle of a finite isolated system, and define the matrix elements of an operator O^\hat{O} by

Oij=⟨Ei∣O^∣Ej⟩.O_{ij}=\langle E_i|\hat{O}|E_j\rangle.

For i≠ji\ne j, write Oij=ΔijO_{ij}=\Delta_{ij}, and let ⟨⋯ ⟩n\langle\cdots\rangle_n denote averages over nearby energy levels of ii and jj. Let Δi\Delta_i be the diagonal fluctuation described by the diagonal ETH statement.

Eigenstate Thermalization Hypothesis. The local statistics of the off-diagonal matrix elements satisfy

⟨∣Oij∣2⟩n=⟨Δi2⟩nF(Ei,Ej),\langle|O_{ij}|^2\rangle_n=\langle\Delta_i^2\rangle_n F(E_i,E_j),

where FF is of order unity for Ei=EjE_i=E_j and tends to zero as ∣Ei−Ej∣|E_i-E_j| becomes large.

This extension of ETH controls off-diagonal matrix elements and is relevant to dynamical correlation functions and the approach to equilibrium. The source does not state a resolution status for this formulation.

References

Primary source

Joshua M. Deutsch, “Eigenstate Thermalization Hypothesis”, arXiv:1805.01616 (2018).

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