An inverse problem for the wave equation with one measurement and the pseudorandom noise

preprint2010arXivOpen access

Abstract

We consider the wave equation $(\p_t^2-Δ_g)u(t,x)=f(t,x)$, in Rn\R^n, u∣R−×Rn=0u|_{\R_-\times \R^n}=0, where the metric g=(gjk(x))j,k=1ng=(g_{jk}(x))_{j,k=1}^n is known outside an open and bounded set M⊂RnM\subset \R^n with smooth boundary $\p M$. We define a deterministic source f(t,x)f(t,x) called the pseudorandom noise as a sum of point sources, f(t,x)=∑j=1∞ajδxj(x)δ(t)f(t,x)=\sum_{j=1}^\infty a_jδ_{x_j}(x)δ(t), where the points xj, j∈Z+x_j,\ j\in\Z_+, form a dense set on $\p M$. We show that when the weights aja_j are chosen appropriately, $u|_{\R\times \p M}$ determines the scattering relation on $\p M$, that is, it determines for all geodesics which pass through MM the travel times together with the entering and exit points and directions. The wave u(t,x)u(t,x) contains the singularities produced by all point sources, but when aj=λ−λja_j=λ^{-λ^{j}} for some λ>1λ>1, we can trace back the point source that produced a given singularity in the data. This gives us the distance in (Rn,g)(\R^n, g) between a source point xjx_j and an arbitrary point $y \in \p M$. In particular, if (Mˉ,g)(\bar M,g) is a simple Riemannian manifold and gg is conformally Euclidian in Mˉ\bar M, these distances are known to determine the metric gg in MM. In the case when (Mˉ,g)(\bar M,g) is non-simple we present a more detailed analysis of the wave fronts yielding the scattering relation on $\p M$.

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