In view of extending the shell model to highly deformed states of heavy nuclei, we discuss the evaluation of the Green's function for the Schrodinger equation in three dimensions with a smooth potential, in the limit of large quantum numbers. Such an evaluation is possible only after smoothing over
On the large-time asymptotics of Green's function for internal gravity waves
โ Scribed by V.A. Borovikov
- Publisher
- Elsevier Science
- Year
- 1997
- Tongue
- English
- Weight
- 1022 KB
- Volume
- 26
- Category
- Article
- ISSN
- 0165-2125
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โฆ Synopsis
We study Green's function for the internal gravity waves in a horizontally uniform fluid. The exact representation of Green's function is found for the half-space z > 0 under the assumptions that the square of Briinta-V&still frequency N'(z) = cont. z, and the boundary condition at z = 0 is zero. The large-time asymptotics of this function contain two terms of the form t~'/~A(r, z, ZO) exp i(to(r, z, ~0)). This result suggests that in the general case the large-time asymptotics of Green's function contain analogous terms. The analogs of the eikonal equation for o and the transport equation for A are obtained and solved. This enables us to formulate an algorithm for calculating the asymptotics of Green's function in the general case. Under an additional assumption that N2 has a unique maximum, these asymptotics are justified for the case of internal waves propagating in a waveguide layer, when as 1.~1 + 03, N2(z) + 0. In order to prove this we employ the well-known representation of Green's function as a sum of normal modes as obtained by the method of separation of variables. The appropriate eigenvalues and eigenfunctions are replaced by their WKB-asymptotics, and the Poisson summation formula is used. The resulting integrals are evaluated by applying the stationary phase method.
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