2020
DOI: 10.2140/paa.2020.2.385
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Scattering resonances on truncated cones

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Cited by 3 publications
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“…2 /.g j ' j / D 0 to a Bessel equation by change of variables. For a detailed treatment on this solution on a single Fourier mode, we refer to [3]. By the functional calculus on product cones, f ./g.r; / D r Now, what we can compute by the asymptotic expansion of Bessel functions is the principal symbol of the conormal solution u j at N ¹r C r 0 D tº (as we will do in the later part of this section); for now we write these principal symbols P j .t; r; r 0 ; /' j .…”
Section: Diffraction Coefficient On Product Conesmentioning
confidence: 99%
“…2 /.g j ' j / D 0 to a Bessel equation by change of variables. For a detailed treatment on this solution on a single Fourier mode, we refer to [3]. By the functional calculus on product cones, f ./g.r; / D r Now, what we can compute by the asymptotic expansion of Bessel functions is the principal symbol of the conormal solution u j at N ¹r C r 0 D tº (as we will do in the later part of this section); for now we write these principal symbols P j .t; r; r 0 ; /' j .…”
Section: Diffraction Coefficient On Product Conesmentioning
confidence: 99%