The problem of representing a diatomic (true) Rydberg-Klein-Rees potential U ' by an analytical function U" is discussed. The perturbed Morse function is in the form U" = U M + Cb, y", where the Morse potential is U M = Dy2, y = 1exp( -a(rre)). The problem is reduced to determination of the coeffici
A generalized Morse function as cleavage potential
✍ Scribed by J.Å. Schweitz; O. Vingsbo
- Publisher
- Elsevier Science
- Year
- 1971
- Weight
- 531 KB
- Volume
- 8
- Category
- Article
- ISSN
- 0025-5416
No coin nor oath required. For personal study only.
📜 SIMILAR VOLUMES
The problem of the representation of the RKR (or IPA) diatomic potential by a simple analytic function is considered. This old problem has for a fairly good solution the Coxon-Hajigeorgiou function U(x) = D(lexp( -fn(x)I2 withf,(x) = Ck=, a,P. The problem of the determination of the disposable param
The Schroedinger equation with a momentum-dependent potential has been solved to yield the single-particle energies for neutrons and protons in bound nuclear systems. A nonlocal nucleon-nucleus potential is reduced to a momentum-dependent potential which is further transformed to an energy-dependen