Pöschl–Teller potential
In mathematical physics, a Pöschl–Teller 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]
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
- ↑ "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.
- 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.
- ↑ Siegfried Flügge Practical Quantum Mechanics (Springer, 1998)
- ↑ 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.