Marchenko equation

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:

${\displaystyle K(r,r^{\prime })+g(r,r^{\prime })+\int _{r}^{\infty }K(r,r^{\prime \prime })g(r^{\prime \prime },r^{\prime })\mathrm {d} r^{\prime \prime }=0}$

Where ${\displaystyle g(r,r^{\prime })\,}$is a symmetric kernel, such that ${\displaystyle g(r,r^{\prime })=g(r^{\prime },r),\,}$which is computed from the scattering data. Solving the Marchenko equation, one obtains the kernel of the transformation operator ${\displaystyle K(r,r^{\prime })}$ 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

Suppose that for a potential ${\displaystyle u(x)}$ for the Schrödinger operator ${\displaystyle L=-{\frac {d^{2}}{dx^{2}}}+u(x)}$, one has the scattering data ${\displaystyle (r(k),\{\chi _{1},\cdots ,\chi _{N}\})}$, where ${\displaystyle r(k)}$ are the reflection coefficients from continuous scattering, given as a function ${\displaystyle r:\mathbb {R} \rightarrow \mathbb {C} }$, and the real parameters ${\displaystyle \chi _{1},\cdots ,\chi _{N}>0}$ are from the discrete bound spectrum.^[1]

Then defining

where the ${\displaystyle \beta _{n}}$ are non-zero constants, solving the GLM equation for ${\displaystyle K}$ allows the potential to be recovered using the formula

See also

• Lax pair

References

• Marchenko, V. A. (2011). Sturm–Liouville Operators and Applications (2nd ed.). Providence: American Mathematical Society. ISBN 978-0-8218-5316-0. MR 2798059.