43 research outputs found

    Resonance expansions of massless Dirac fields propagating in the exterior of a de Sitter-Reissner-Nordstr\"om black hole

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    We give an expansion of the solution of the evolution equation for the massless Dirac fields in the outer region of de Sitter-Reissner-Nordstr\"om black hole in terms of resonances. By means of this method we describe the decay of local energy for compactly supported data. The proof uses the cut-off resolvent estimates for the semi-classical Schr\"odinger operators from Bony and H\"afner, 2008. The method extends to the Dirac operators on spherically symmetric asymptotically hyperbolic manifolds.Comment: The paper is continuation of arXiv:1407.3654 and generalizes arXiv:0706.0350 to the Dirac field

    An Inverse Problem for Trapping Point Resonances

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    We consider semi-classical Schr{\"o}dinger operator P(h)=−h2Δ+V(x) P(h)=-h^2\Delta +V(x) in Rn{\mathbb R}^n such that the analytic potential VV has a non-degenerate critical point x0=0x_0=0 with critical value E0E_0 and we can define resonances in some fixed neighborhood of E0E_0 when h>0h>0 is small enough. If the eigenvalues of the Hessian are \zz-independent the resonances in hδh^\delta-neighborhood of E0E_0 (δ>0\delta >0) can be calculated explicitly as the eigenvalues of the semi-classical Birkhoff normal form. Assuming that potential is symmetric with respect to reflections about the coordinate axes we show that the classical Birkhoff normal form determines the Taylor series of the potential at x0.x_0. As a consequence, the resonances in a hδh^\delta-neighborhood of E0E_0 determine the first NN terms in the Taylor series of VV at x0.x_0. The proof uses the recent inverse spectral results of V. Guillemin and A. Uribe

    Periodic Jacobi operator with finitely supported perturbations: the inverse resonance problem

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    We consider a periodic Jacobi operator HH with finitely supported perturbations on Z.{\Bbb Z}. We solve the inverse resonance problem: we prove that the mapping from finitely supported perturbations to the scattering data: the inverse of the transmission coefficient and the Jost function on the right half-axis, is one-to-one and onto. We consider the problem of reconstruction of the scattering data from all eigenvalues, resonances and the set of zeros of R−(λ)+1,R_-(\lambda)+1, where R−R_- is the reflection coefficient

    Resonances for Dirac operators on the half-line

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    We consider the 1D Dirac operator on the half-line with compactly supported potentials. We study resonances as the poles of scattering matrix or equivalently as the zeros of modified Fredholm determinant. We obtain the following properties of the resonances: 1) asymptotics of counting function, 2) estimates on the resonances and the forbidden domain.Comment: arXiv admin note: text overlap with arXiv:1302.463

    Resonances for 1D massless Dirac operators

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    We consider the 1D massless Dirac operator on the real line with compactly supported potentials. We study resonances as the poles of scattering matrix or equivalently as the zeros of modified Fredholm determinant. We obtain the following properties of the resonances: 1) asymptotics of counting function, 2) estimates on the resonances and the forbidden domain, 3) the trace formula in terms of resonances.Comment: 23 page

    Resonances for the radial Dirac operators

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    We consider the radial Dirac operator with compactly supported potentials. We study resonances as the poles of scattering matrix or equivalently as the zeros of modified Fredholm determinant. We obtain the following properties of the resonances: 1) asymptotics of counting function, 2) in the massless case we get the trace formula in terms of resonances.Comment: 36 pages. arXiv admin note: substantial text overlap with arXiv:1307.247
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