The resonance concentration conjecture near the pressure line

Let N(Ω):=NP(h)(Ω)N(\Omega):=N_{P(h)}(\Omega) be the resonance counting function, and let PE(s)\mathcal P_E(s) be the topological pressure. Resonance concentration conjecture. For every γ>PE(1)/2\gamma>\mathcal P_E(1)/2, there exists ϵ0>0\epsilon_0>0 such that for every ϵ<ϵ0\epsilon<\epsilon_0,

limh0N([Eh,E+h]ih2[PE(1)ϵ,PE(1)+ϵ])N([Eh,E+h]ih[0,γ])=1.\lim_{h\to0}\frac{N\left([E-h,E+h]-\frac{i h}{2}[\mathcal P_E(1)-\epsilon,\mathcal P_E(1)+\epsilon]\right)}{N([E-h,E+h]-ih[0,\gamma])}=1.

The claim asserts that asymptotically almost all resonances in the indicated window concentrate near the pressure line; the source presents it as open.

Sources & referencesView supporting material

Primary source

Maciej Zworski, “Mathematical Study of Scattering Resonances”, arXiv:1609.03550 (2017).

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