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1: 33.22 Particle Scattering and Atomic and Molecular Spectra
At positive energies E > 0 , ρ 0 , and:
Attractive potentials: Z 1 Z 2 < 0 , η < 0 .
R = m e c α 2 / ( 2 ) .
Attractive potentials: Z 1 Z 2 < 0 , r > 0 .
Attractive potentials: Z 1 Z 2 < 0 , κ < 0 .
2: Bibliography B
  • E. Bank and M. E. H. Ismail (1985) The attractive Coulomb potential polynomials. Constr. Approx. 1 (2), pp. 103–119.
  • 3: Bibliography S
  • M. J. Seaton (2002a) Coulomb functions for attractive and repulsive potentials and for positive and negative energies. Comput. Phys. Comm. 146 (2), pp. 225–249.
  • 4: 18.39 Applications in the Physical Sciences
    The Schrödinger equation with potentialBound state solutions to the relativistic Dirac Equation, for this same problem of a single electron attracted by a nucleus with Z protons, involve Laguerre polynomials of fractional index. … These cases correspond to the two distinct orthogonality conditions of (18.35.6) and (18.35.6_3). … In the attractive case (18.35.6_4) for the discrete parts of the weight function where with x k < 1 , are also simplified: …The weight functions for both the attractive and repulsive cases are now unit normalized, see Bank and Ismail (1985), and Ismail (2009). …