The fractal Weyl law for resonance lower bounds

Let N(Ω):=NP(h)(Ω)N(\Omega):=N_{P(h)}(\Omega) be the resonance counting function, and let δE\delta_E be the trapped-set dimension parameter defined in the source. Fractal Weyl law conjecture. If dimM=2\dim M=2, then

limh0hδEN([Eh,E+h]ih[0,γ])=vE(γ),\lim_{h\to0}h^{\delta_E}N([E-h,E+h]-ih[0,\gamma])=v_E(\gamma),

where vE(γ)>0v_E(\gamma)>0 for sufficiently large γ\gamma. If dimM>2\dim M>2, then

lim suph0hδEN([Eh,E+h]ih[0,γ])>0\limsup_{h\to0}h^{\delta_E}N([E-h,E+h]-ih[0,\gamma])>0

for sufficiently large γ\gamma. This conjecture seeks a lower bound matching the fractal Weyl upper bound; the source says that only special toy models had been proved.

Sources & referencesView supporting material

Primary source

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

Additional references

4 papers in this index state this conjecture (2005–2016). The statement above is taken from the most recent of them; the others are arXiv:1305.4850, arXiv:nlin/0608069, arXiv:math-ph/0506056.

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