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Energy Concentration and Sommerfeld Condition for Helmholtz Equation with Variable Index at Infinity
Authors:Benoit Perthame  Luis Vega
Institution:(1) UMR 7598 LJLL, BC187, Université Pierre et Marie Curie-Paris 6, 4, place Jussieu, F-75252 Paris cedex 5, France;(2) Institut Universitaire de France, Paris cedex 5, France;(3) Universidad del Pais Vasco, Apdo. 644, 48080 Bilbao, Spain
Abstract:We consider the Helmholtz equation with a variable index of refraction n(x), which is not necessarily constant at infinity but can have an angular dependency like 
$$n(x)\rightarrow n_{\infty} (x/|x|)$$
as 
$$|x| \rightarrow \infty$$
. Under some appropriate assumptions on this convergence and on n we prove that the Sommerfeld condition at infinity still holds true under the explicit form

$$\int_{{\rm \mathbb{R}}^{d}}\left| \nabla u-in^{1/2}_{\infty}u\frac{x}{\mid x \mid}\right|^{2}\frac{dx}{\mid x \mid}<+\infty.$$
It is a very striking and unexpected feature that the index n appears in this formula and not the gradient of the phase as established by Saito in S] and broadly used numerically. This apparent contradiction is clarified by the existence of some extra estimates on the energy decay. In particular we prove that

$$\int_{{\rm \mathbb{R}}^{d}}\left|\nabla_{\omega}n_{\infty}\left(\frac{x}{\mid x \mid}\right)\right|^{2}\frac{{\mid u \mid}^2}{\mid x \mid}dx<+\infty.$$
In fact our main contribution is to show that this can be interpreted as a concentration of the energy along the critical lines of n . In other words, the Sommerfeld condition hides the main physical effect arising for a variable n at infinity; energy concentration on lines rather than dispersion in all directions. Received: March 2006, Revision: July 2006, Accepted: July 2006
Keywords: and phrases:" target="_blank"> and phrases:  Helmholtz equation  Energy concentration  Sommerfeld condition  index of refraction
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