Abstract
The acoustic propagator is the self-adjoint operatorH=-∇·c(x)2∇, defined inL2(Q), whereQ⊆R2is a band of finite width, given byQ={(x, z), x∈R, 0≤z≤Γ}. The wave velocitycdepends only on the horizontal coordinatex, and is a measurable bounded function, converging toc±>0 asx→±∞. It is proved that the resolvent operatorR(z)=(H-z)-1, Imz≠0, can be extended continuously to the closed upper (or lower) half-plane, in a suitable weighted-L2topology ("Limiting Absorption Principle"). In particular, this continuity holds at the thresholdλ=0. It follows as a corollary thatHhas no point spectrum.
| Original language | English |
|---|---|
| Pages (from-to) | 115-135 |
| Number of pages | 21 |
| Journal | Journal of Differential Equations |
| Volume | 136 |
| Issue number | 1 |
| DOIs | |
| State | Published - 1 May 1997 |
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