蕨类 发表于 2025-3-25 06:14:35
Some Explicit Examples,he solution to the inverse scattering problem is illustrated with various explicit examples, and it is demonstrated how the potential, boundary condition, and other relevant quantities are constructed from a given scattering data set. The use of Levinson’s theorem and the generalized Fourier map is使迷醉 发表于 2025-3-25 07:31:43
http://reply.papertrans.cn/29/2807/280637/280637_22.pngIntentional 发表于 2025-3-25 13:05:32
http://reply.papertrans.cn/29/2807/280637/280637_23.pngGlossy 发表于 2025-3-25 16:53:31
https://doi.org/10.1007/978-3-662-58125-4om a given scattering matrix without having the bound-state information. From the given scattering matrix alone we show how to construct a scattering data set belonging to the Marchenko class so that the constructed scattering data set can be used as input into a properly posed inverse scattering pr听写 发表于 2025-3-25 23:47:57
http://reply.papertrans.cn/29/2807/280637/280637_25.png轻推 发表于 2025-3-26 03:29:03
http://reply.papertrans.cn/29/2807/280637/280637_26.png加剧 发表于 2025-3-26 04:49:14
0066-5452 g theory through explicit examples.Indicates how the inverseAuthored by two experts in the field who have been long-time collaborators, this monograph treats the scattering and inverse scattering problems for the matrix Schrödinger equation on the half line with the general selfadjoint boundary condaverse 发表于 2025-3-26 10:10:42
Book 2021he matrix Schrödinger equation on the half line with the general selfadjoint boundary condition. The existence, uniqueness, construction, and characterization aspects are treated with mathematical rigor, and physical insight is provided to make the material accessible to mathematicians, physicists,干旱 发表于 2025-3-26 15:57:12
http://reply.papertrans.cn/29/2807/280637/280637_29.pngConsensus 发表于 2025-3-26 18:12:19
Direct Scattering II, that the scattering matrix defined in terms of the Jost matrix coincides with the scattering matrix derived from the scattering operator. Various other topics are considered such as the properties of the spectral shift function, trace formulas of Buslaev–Faddeev type, and a Bargmann–Birman–Schwinger bound on the number of bound states.