{ "id": "2109.11267", "version": "v1", "published": "2021-09-23T10:12:14.000Z", "updated": "2021-09-23T10:12:14.000Z", "title": "Scattering by finely-layered obstacles: frequency-explicit bounds and homogenization", "authors": [ "Théophile Chaumont-Frelet", "Euan A. Spence" ], "categories": [ "math.AP" ], "abstract": "We consider the scalar Helmholtz equation with variable, discontinuous coefficients, modelling transmission of acoustic waves through an anisotropic penetrable obstacle. We first prove a well-posedness result and a frequency-explicit bound on the solution operator, with both valid for sufficiently-large frequency and for a class of coefficients that satisfy certain monotonicity conditions in one spatial direction, and are only assumed to be bounded (i.e., $L^\\infty$) in the other spatial directions. This class of coefficients therefore includes coefficients modelling transmission by penetrable obstacles with a (potentially large) number of layers (in 2-d) or fibres (in 3-d). Importantly, the frequency-explicit bound holds uniformly for all coefficients in this class; this uniformity allows us to consider highly-oscillatory coefficients and study the limiting behaviour when the period of oscillations goes to zero. In particular, we bound the $H^1$ error committed by the first-order bulk correction to the homogenized transmission problem, with this bound explicit in both the period of oscillations of the coefficients and the frequency of the Helmholtz equation; to our knowledge, this is the first homogenization result for the Helmholtz equation that is explicit in these two quantities and valid without the assumption that the frequency is small.", "revisions": [ { "version": "v1", "updated": "2021-09-23T10:12:14.000Z" } ], "analyses": { "keywords": [ "coefficients", "finely-layered obstacles", "spatial direction", "modelling transmission", "penetrable obstacle" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }