AbstractThe inverse scattering problem for the perturbed wave equation (1) □u + V(x)u = 0 in Ω=Rn (n = odd ⩾ 3) is considered. Here the potentials V(x) are real, smooth, with compact support and non-negative. We apply the Lax and Phillips theory, together with some properties of solutions of a Dirichlet problem associated with the operator −Δ + V(x) to show, in a very simple way, that the scattering operator S(V) associated with (1) determines uniquely the scatterer, provided that a fixed sign condition on the potentials is satisfied. We also show that the map V → S(V) is once-differentiable
We develop a soliton perturbation theory for the non-degenerate 3×3 eigenvalue operator, with obviou...
Let $A(β,α,k)$ be the scattering amplitude corresponding to a real-valued potential which vanishes o...
AbstractConsider the equation □u + q(t. x)u = 0, x∈R3, with a time-dependent potential q(t, x) compa...
AbstractThe inverse scattering problem for the perturbed wave equation (1) □u + V(x)u = 0 in Ω=Rn (n...
AbstractWe consider finite energy solutions of the perturbed wave equation with “impurities” which d...
AbstractWe consider a linear perturbation for the wave equation □u = 0 in Ω = E3 by “repulsive” smoo...
The inverse problem for quantum and acoustic scatterings has been investi-gated extensively. Little ...
AbstractWe consider finite energy solutions of the perturbed wave equation with “impurities” which d...
We develop a soliton perturbation theory for the non-degenerate 3 × 3 eigenvalue operator, with obvi...
We develop a soliton perturbation theory for the non-degenerate 3 × 3 eigenvalue operator, with obvi...
2010 Mathematics Subject Classification: 37K40, 35Q15, 35Q51, 37K15.The inverse scattering transform...
This thesis considers certain mathematical formulation of the scattering phenomena. Scattering is a ...
Let H0 be the Laplace operator with Dirichlet conditions in L2(Ω), Ω = Rn × (0, pi), n ≥ 2, V being ...
Let H0 be the Laplace operator with Dirichlet conditions in L2(Ω), Ω = Rn × (0, pi), n ≥ 2, V being ...
We consider the recovery of a potential associated with a semi-linear wave equation on Rn+1, n≥1. We...
We develop a soliton perturbation theory for the non-degenerate 3×3 eigenvalue operator, with obviou...
Let $A(β,α,k)$ be the scattering amplitude corresponding to a real-valued potential which vanishes o...
AbstractConsider the equation □u + q(t. x)u = 0, x∈R3, with a time-dependent potential q(t, x) compa...
AbstractThe inverse scattering problem for the perturbed wave equation (1) □u + V(x)u = 0 in Ω=Rn (n...
AbstractWe consider finite energy solutions of the perturbed wave equation with “impurities” which d...
AbstractWe consider a linear perturbation for the wave equation □u = 0 in Ω = E3 by “repulsive” smoo...
The inverse problem for quantum and acoustic scatterings has been investi-gated extensively. Little ...
AbstractWe consider finite energy solutions of the perturbed wave equation with “impurities” which d...
We develop a soliton perturbation theory for the non-degenerate 3 × 3 eigenvalue operator, with obvi...
We develop a soliton perturbation theory for the non-degenerate 3 × 3 eigenvalue operator, with obvi...
2010 Mathematics Subject Classification: 37K40, 35Q15, 35Q51, 37K15.The inverse scattering transform...
This thesis considers certain mathematical formulation of the scattering phenomena. Scattering is a ...
Let H0 be the Laplace operator with Dirichlet conditions in L2(Ω), Ω = Rn × (0, pi), n ≥ 2, V being ...
Let H0 be the Laplace operator with Dirichlet conditions in L2(Ω), Ω = Rn × (0, pi), n ≥ 2, V being ...
We consider the recovery of a potential associated with a semi-linear wave equation on Rn+1, n≥1. We...
We develop a soliton perturbation theory for the non-degenerate 3×3 eigenvalue operator, with obviou...
Let $A(β,α,k)$ be the scattering amplitude corresponding to a real-valued potential which vanishes o...
AbstractConsider the equation □u + q(t. x)u = 0, x∈R3, with a time-dependent potential q(t, x) compa...