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Lagrange-mesh calculations in momentum space

Gwendolyn Lacroix*, Claude Semay, and Fabien Buisseret

  • Service de Physique Nucléaire et Subnucléaire, Université de Mons, Académie universitaire Wallonie-Bruxelles, Place du Parc 20, 7000 Mons, Belgium

  • *gwendolyn.lacroix@umons.ac.be
  • claude.semay@umons.ac.be
  • Haute École Louvain en Hainaut, Chaussée de Binche 159, 7000 Mons, Belgium; fabien.buisseret@umons.ac.be

Phys. Rev. E 86, 026705 – Published 8 August, 2012

DOI: https://doi.org/10.1103/PhysRevE.86.026705

Abstract

The Lagrange-mesh method is a powerful method to solve eigenequations written in configuration space. It is very easy to implement and very accurate. Using a Gauss quadrature rule, the method requires only the evaluation of the potential at some mesh points. The eigenfunctions are expanded in terms of regularized Lagrange functions which vanish at all mesh points except one. It is shown that this method can be adapted to solve eigenequations written in momentum space, keeping the convenience and the accuracy of the original technique. In particular, the kinetic operator is a diagonal matrix. Observables and wave functions in both configuration space and momentum space can also be easily computed with good accuracy using only eigenfunctions computed in the momentum space. The method is tested with Gaussian and Yukawa potentials, requiring, respectively, a small and a large mesh to reach convergence. Corresponding wave functions in both spaces are compared with each other using the Fourier transform.

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