Pöschl–Teller potential

Short description: Quantum mechanical potential

In mathematical physics, a Pöschl–Teller potential is a special class of potentials for which the one-dimensional Schrödinger equation can be solved in terms of special functions. It is named after the physicists Gertrud Pöschl and Edward Teller who developed it in 1933.

Definition

In its symmetric form is explicitly given by

Symmetric Pöschl–Teller potential: $-\frac{\lambda (\lambda +1)}{2}{\mathrm{sech}}^2(x)$. It shows the eigenvalues for μ=1, 2, 3, 4, 5, 6.

$V(x)=-\frac{\lambda (\lambda +1)}{2}{\mathrm{s}\mathrm{e}\mathrm{c}\mathrm{h}}^2(x)$

and the solutions of the time-independent Schrödinger equation

$-\frac{1}{2}{\psi }^{″}(x)+V(x)\psi (x)=E\psi (x)$

with this potential can be found by virtue of the substitution $u=\mathrm{t}\mathrm{a}\mathrm{n}\mathrm{h}\mathrm{(}\mathrm{x}\mathrm{)}$, which yields

$[(1-u^2){\psi }^{\prime }(u)]+\lambda (\lambda +1)\psi (u)+\frac{2E}{1-u^2}\psi (u)=0$.

Thus the solutions $\psi (u)$ are just the Legendre functions $P_{\lambda }^{\mu }(\tanh (x))$ with $E=-\frac{{\mu }^2}{2}$, and $\lambda =1,2,3\cdots$, $\mu =1,2,\cdots ,\lambda -1,\lambda$. Moreover, eigenvalues and scattering data can be explicitly computed. In the special case of integer $\lambda$, the potential is reflectionless and such potentials also arise as the N-soliton solutions of the Korteweg–De Vries equation.

The more general form of the potential is given by

$V(x)=-\frac{\lambda (\lambda +1)}{2}{\mathrm{s}\mathrm{e}\mathrm{c}\mathrm{h}}^2(x)-\frac{\nu (\nu +1)}{2}{\mathrm{c}\mathrm{s}\mathrm{c}\mathrm{h}}^2(x).$

Rosen–Morse potential

Nathan Rosen and Philip M. Morse introduced related potential is given by introducing an additional term:

$V(x)=-\frac{\lambda (\lambda +1)}{2}{\mathrm{s}\mathrm{e}\mathrm{c}\mathrm{h}}^2(x)-g\tanh x.$

See also

• Morse potential
• Trigonometric Rosen–Morse potential

External links

• Eigenstates for Pöschl-Teller Potentials