Hydrogenic Radial Functions via Supersymmetry

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An application of supersymmetric quantum mechanics enables all the bound-state radial functions for the hydrogen atom to be evaluated using first-order differential operators, without any explicit reference to Laguerre polynomials.
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Contributed by: S. M. Blinder (March 2011)
Open content licensed under CC BY-NC-SA
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Supersymmetric quantum mechanics can be applied to the solution of the hydrogenic radial equation, treated as a pseudo-one-dimensional problem in the variable with effective Hamiltonians denoted
. There exist two partner Hamiltonians for each value of
, which can be written
and
, with
and
. The superpotential
is given by
. With
as defined above,
. The lowest-energy eigenstate of
has no partner eigenstate, but all higher-energy eigenstates have degenerate supersymmetric partners. These can be labeled by increasing values of the principal quantum number
, beginning with
. The composite pattern for all
-values leads to the characteristic degeneracies for
in a pure Coulomb field, associated with a higher symmetry than would be implied by spherical invariance alone.
Snapshots 1–3: the 1 ground state is nondegenerate and is annihilated by either operator
or
Snapshots 4–6: the 3 state is transformed to 3
by
Reference: A. Valance, T. J. Morgan, and H. Bergeron, "Eigensolution of the Coulomb Hamiltonian via Supersymmetry," American Journal of Physics, 58(5), 1990 pp. 487–491.
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