Pöschl–Teller potential

In mathematical physics, a PöschlTeller potential, named after the physicists Herta Pöschl[1] (credited as G. Pöschl) and Edward Teller, is a special class of potentials for which the one-dimensional Schrödinger equation can be solved in terms of Special functions.

Definition

In its symmetric form is explicitly given by[2]

Symmetric PöschlTeller potential: . It shows the eigenvalues for μ=1, 2, 3, 4, 5, 6.

and the solutions of the time-independent Schrödinger equation

with this potential can be found by virtue of the substitution , which yields

.

Thus the solutions are just the Legendre functions with , and , . Moreover, eigenvalues and scattering data can be explicitly computed.[3] In the special case of integer , the potential is reflectionless and such potentials also arise as the N-soliton solutions of the Korteweg-de Vries equation.[4]

The more general form of the potential is given by[2]

See also

References list

  1. "Edward Teller Biographical Memoir." by Stephen B. Libby and Andrew M. Sessler, 2009 (published in Edward Teller Centennial Symposium: modern physics and the scientific legacy of Edward Teller, World Scientific, 2010.
  2. 1 2 Pöschl, G.; Teller, E. (1933). "Bemerkungen zur Quantenmechanik des anharmonischen Oszillators". Zeitschrift für Physik. 83 (3–4): 143–151. Bibcode:1933ZPhy...83..143P. doi:10.1007/BF01331132.
  3. Siegfried Flügge Practical Quantum Mechanics (Springer, 1998)
  4. Lekner, John (2007). "Reflectionless eigenstates of the sech2 potential". American Journal of Physics. 875 (12): 1151–1157. Bibcode:2007AmJPh..75.1151L. doi:10.1119/1.2787015.
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