Feingold–Peres off-diagonal variance conjecture

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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 ω∈R\omega\in\mathbb{R}, define

VA(E;ω):=Δk(E)2ϵ(E)NL(E)∑m,n:En∈[E,E+L(E)]∣km−kn−ω∣≤ϵ(E)∣⟨ϕn,A^ϕm⟩∣2.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 E→∞E\to\infty,

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

where 0<ϵ(E)=O(E−1/4)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.

References

Primary source

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

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