2015
DOI: 10.1016/j.wavemoti.2015.01.004
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Osculations of spectral lines in a layered medium

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Cited by 19 publications
(13 citation statements)
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“…Maznev and Every (2011) go beyond normal modes and discuss leaky modes as well. The phenomenon exists in combination with osculation points of dispersion curves (Kausel et al 2015) and according to Maznev and Every (2011) can be partly understood by consideration of mode degeneracy and hybridization. Malischewsky et al (2017) and Malischewsky and Forbriger (2020) report that the condition of a single-valued dispersion relation can as well be violated for simple seismic structures of a layer on top of a half-space.…”
Section: Reported Cases From Engineeringmentioning
confidence: 99%
“…Maznev and Every (2011) go beyond normal modes and discuss leaky modes as well. The phenomenon exists in combination with osculation points of dispersion curves (Kausel et al 2015) and according to Maznev and Every (2011) can be partly understood by consideration of mode degeneracy and hybridization. Malischewsky et al (2017) and Malischewsky and Forbriger (2020) report that the condition of a single-valued dispersion relation can as well be violated for simple seismic structures of a layer on top of a half-space.…”
Section: Reported Cases From Engineeringmentioning
confidence: 99%
“…(7,9) and for Eqs. (8,10). Namely, , and Solutions are given by equating the product of the two determinants to zero.…”
Section: Traction-free Platementioning
confidence: 99%
“…One notorious characteristic is an extremely high Poisson ratio in the uppermost layers together with a very high impedance contrast between the layers and the subsoil. Investigating the socalled osculations of dispersion curves (Kausel et al, 2015) we have casually discovered unusual higher-mode Rayleigh waves because of the equivocal behaviour of their dispersion curves in a certain frequency range. Following Furumura and Kennett (1998) the dominant seismic phases at regional distances are usually the crustal P g and L g phases and the recorded L g phase can be regarded either as a superposition of multiply reflected S waves in the crust or as a sum of a number of higher surface wave modes sampled at the free surface of the crust.…”
Section: Equivocalness Of Dispersion Curvesmentioning
confidence: 99%