The Weyl-law conjecture for Love waves in layered elastic half-spaces

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Let n⩾3n\geqslant3, let y∈[1/C∞,1/C0)y\in[1/C_\infty,1/C_0), and let C~1⩽⋯⩽C~n+1\widetilde{C}_1\leqslant\cdots\leqslant\widetilde{C}_{n+1} be the nondecreasing reordering of the parameters C1,…,Cn+1C_1,\ldots,C_{n+1}, with associated sequences ν~p\tilde{\nu}_p and T~p\widetilde{T}_p. Let N(ω,y)N(\omega,y) denote the counting function for the Love-wave problem. Weyl-law conjecture. As ω\omega goes to +∞+\infty, one has

N(ω,y)∼ωπ∑p=1j∣ν~p(y)∣T~p,N(\omega,y)\sim\frac{\omega}{\pi}\sum_{p=1}^{j}|\tilde{\nu}_p(y)|\widetilde{T}_p,

if y∈[1/C~j+1,1/C~j)y\in[1/\widetilde{C}_{j+1},1/\widetilde{C}_j). This conjecture extends the proved asymptotic formula to the whole interval [1/C∞,1/C0)[1/C_\infty,1/C_0) without assuming C0<C~2C_0<\widetilde{C}_2, thereby allowing several of the CjC_j to equal C0:=min⁡jCjC_0:=\min_j C_j.

References

Primary source

Maarten V. de Hoop, Josselin Garnier, Alexei Iantchenko and Julien Ricaud, “Inverse problem for Love waves in a layered, elastic half-space”, arXiv:2302.08173 (2023).

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