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High frequency wave propagation for the viscoelastic wave equation with singular memory

Abstract

We study high-frequency propagation for a viscoelastic wave equation with spatially dependent hereditary memory in relative-history form. The kernel may have the integrable singularity m(s,x)=sp−1m(s,x), 0<p<1; the regular case p=1 is included. Using the half-amplitude propagation distance and corresponding travel time as units, the wavelength h≪1 yields the memory factor ε=h1−p. We construct exact solutions with full two-scale geometric-optics expansions in powers hk+(1−p)ℓ. Memory modifies the propagation geometry through the instantaneous modulus σ+ε∫0∞m(s,·) d s, while the kernel singularity contributes Cp=Γ(p)eiπp/2 to the leading transport equation. For 0<p<1, this produces fractional scales, frequency-dependent attenuation, and a dispersive phase correction; for p=1, the fractional hierarchy disappears, attenuation is frequency independent, and the transport phase correction vanishes. We also derive a local damped wave equation whose incoming high-frequency solutions approximate the hereditary solutions with O(h) error in semiclassical Ck norms. Exterior observations for all incident directions and 0<h≪1 uniquely recover σm and the full temporal jet of m at s=0, which determine the expansion modulo O(h∞). Finally, a contraction-semigroup argument gives well-posedness and arbitrary finite-order Sobolev regularity for spatially dependent weakly singular kernels and prescribed full prehistory, with explicit compatibility conditions and estimates uniform in ε. These estimates justify the geometric-optics construction.

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BibTeX
@misc{grebnev2026high,
  title = {{High frequency wave propagation for the viscoelastic wave equation with singular memory}},
  author = {Haim Grebnev and Plamen Stefanov},
  howpublished = {arXiv},
  year = {2026},
  month = aug,
  doi = {10.48550/arxiv.2608.30138},
  eprint = {2608.30138},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2608.30138},
}
RIS
TY  - UNPB
TI  - High frequency wave propagation for the viscoelastic wave equation with singular memory
AU  - Haim Grebnev
AU  - Plamen Stefanov
PY  - 2026
DA  - 2026/08/31
PB  - arXiv
DO  - 10.48550/arxiv.2608.30138
UR  - https://arxiv.org/abs/2608.30138
AB  - We study high-frequency propagation for a viscoelastic wave equation with spatially dependent hereditary memory in relative-history form. The kernel may have the integrable singularity m(s,x)=s^p−1m(s,x), 0<p<1; the regular case p=1 is included. Using the half-amplitude propagation distance and corresponding travel time as units, the wavelength h≪1 yields the memory factor ε=h^1−p. We construct exact solutions with full two-scale geometric-optics expansions in powers h^k+(1−p)ℓ. Memory modifies the propagation geometry through the instantaneous modulus σ+ε∫_0^∞m(s,·) d s, while the kernel singularity contributes C_p=Γ(p)e^iπp/2 to the leading transport equation. For 0<p<1, this produces fractional scales, frequency-dependent attenuation, and a dispersive phase correction; for p=1, the fractional hierarchy disappears, attenuation is frequency independent, and the transport phase correction vanishes. We also derive a local damped wave equation whose incoming high-frequency solutions approximate the hereditary solutions with O(h) error in semiclassical C^k norms. Exterior observations for all incident directions and 0<h≪1 uniquely recover σ_m and the full temporal jet of m at s=0, which determine the expansion modulo O(h^∞). Finally, a contraction-semigroup argument gives well-posedness and arbitrary finite-order Sobolev regularity for spatially dependent weakly singular kernels and prescribed full prehistory, with explicit compatibility conditions and estimates uniform in ε. These estimates justify the geometric-optics construction.
ER  -