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In mathematical physics, more specifically the one-dimensional inverse scattering problem, the Marchenko equation (or Gelfand-Levitan-Marchenko equation or GLM equation), named after Israel Gelfand, Boris Levitan and Vladimir Marchenko, is derived by computing the Fourier transform of the scattering relation:

Where is a symmetric kernel, such that which is computed from the scattering data. Solving the Marchenko equation, one obtains the kernel of the transformation operator from which the potential can be read off. This equation is derived from the Gelfand–Levitan integral equation, using the Povzner–Levitan representation.

Application to scattering theory

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Suppose that for a potential   for the Schrödinger operator  , one has the scattering data  , where   are the reflection coefficients from continuous scattering, given as a function  , and the real parameters   are from the discrete bound spectrum.[1]

Then defining   where the   are non-zero constants, solving the GLM equation   for   allows the potential to be recovered using the formula  

See also

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Notes

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  1. ^ Dunajski 2009, pp. 30–31.

References

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  • Dunajski, Maciej (2009). Solitons, Instantons, and Twistors. Oxford; New York: OUP Oxford. ISBN 978-0-19-857063-9. OCLC 320199531.
  • Marchenko, V. A. (2011). Sturm–Liouville Operators and Applications (2nd ed.). Providence: American Mathematical Society. ISBN 978-0-8218-5316-0. MR 2798059.
  • Kay, Irvin W. (1955). The inverse scattering problem. New York: Courant Institute of Mathematical Sciences, New York University. OCLC 1046812324.
  • Levinson, Norman (1953). "Certain Explicit Relationships between Phase Shift and Scattering Potential". Physical Review. 89 (4): 755–757. Bibcode:1953PhRv...89..755L. doi:10.1103/PhysRev.89.755. ISSN 0031-899X.