English

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

Analysis of PDEs 2010-11-12 v1

Abstract

We consider the wave equation (\pt2Δg)u(t,x)=f(t,x)(\p_t^2-\Delta_g)u(t,x)=f(t,x), in Rn\R^n, uR×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 MRnM\subset \R^n with smooth boundary \pM\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=1ajδxj(x)δ(t)f(t,x)=\sum_{j=1}^\infty a_j\delta_{x_j}(x)\delta(t), where the points xj, jZ+x_j,\ j\in\Z_+, form a dense set on \pM\p M. We show that when the weights aja_j are chosen appropriately, uR×\pMu|_{\R\times \p M} determines the scattering relation on \pM\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=λλja_j=\lambda^{-\lambda^{j}} for some λ>1\lambda>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\pMy \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 \pM\p M.

Keywords

Cite

@article{arxiv.1011.2527,
  title  = {An inverse problem for the wave equation with one measurement and the pseudorandom noise},
  author = {Tapio Helin and Matti Lassas and Lauri Oksanen},
  journal= {arXiv preprint arXiv:1011.2527},
  year   = {2010}
}