Feingold–Peres off-diagonal variance conjecture

From papers

Let ϕn\phi_n be Laplacian eigenfunctions with wavenumbers knk_n, let A^\hat{A} be multiplication by a test function, and define the mean wavenumber spacing by

Δk(E):=2πE1/2vol(Ω).\Delta_k(E):=\frac{2\pi}{E^{1/2}\operatorname{vol}(\Omega)}.

For a fixed ωR\omega\in\mathbb{R}, define

VA(E;ω):=Δk(E)2ϵ(E)NL(E)m,n:En[E,E+L(E)]kmknωϵ(E)ϕn,A^ϕm2.V_A(E;\omega):=\frac{\Delta_k(E)}{2\epsilon(E)N_L(E)}\sum_{\substack{m,n:E_n\in[E,E+L(E)]\\|k_m-k_n-\omega|\leq\epsilon(E)}}|\langle\phi_n,\hat{A}\phi_m\rangle|^2.

Feingold–Peres off-diagonal variance conjecture. For ergodic flow, as EE\to\infty,

VA(E;ω)C~A(ω)vol(Ω)E1/2,V_A(E;\omega)\sim\frac{\widetilde{C}_A(\omega)}{\operatorname{vol}(\Omega)}E^{-1/2},

where 0<ϵ(E)=O(E1/4)0<\epsilon(E)=O(E^{-1/4}). This predicts the high-energy variance of off-diagonal matrix elements in a frequency window. It is supported by heuristic arguments and numerical tests, but is not established in the generality stated.

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Sources & referencesView supporting material

Primary source

Alex H. Barnett, “Asymptotic rate of quantum ergodicity in chaotic Euclidean billiards”, arXiv:math-ph/0512030 (2006).

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