Proper quantization rule

We find a proper quantization rule, $\int _{x_{A}}^{x_{B}}k(x){\rm d}x-\int _{x_{0A}}^{x_{0B}}k_{0}(x){\rm d}x=n\pi $, where n is the number of the nodes of wave function$\psi (x) $. By this rule the energy spectra of a solvable system can be determined from its ground-state energy only. Particularl...

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Bibliographic Details
Published inEurophysics letters Vol. 89; no. 1; p. 10003
Main Authors Qiang, Wen-Chao, Dong, Shi-Hai
Format Journal Article
LanguageEnglish
Published IOP Publishing 01.01.2010
EDP Sciences
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Summary:We find a proper quantization rule, $\int _{x_{A}}^{x_{B}}k(x){\rm d}x-\int _{x_{0A}}^{x_{0B}}k_{0}(x){\rm d}x=n\pi $, where n is the number of the nodes of wave function$\psi (x) $. By this rule the energy spectra of a solvable system can be determined from its ground-state energy only. Particularly, we study three solvable quantum systems —modified Rosen-Morse potential, symmetric trigonometric Rosen-Morse potential and Manning-Rosen potential in D dimensions— with the proper quantization rule, and show that the previous complicated and tedious calculations can be greatly simplified. This proper quantization rule applies to any exactly solvable potential, and one can easily obtain its energy spectra with the rule. This work is dedicated to Professor Zhong-Qi Ma on the occasion of his 70th birthday.
Bibliography:istex:D59AEAC6E82F75D31D6D539507AD2C7FF68B97A3
publisher-ID:epl12372
ark:/67375/80W-XXH7SX0Q-R
ObjectType-Article-2
SourceType-Scholarly Journals-1
ObjectType-Feature-1
content type line 23
ISSN:0295-5075
1286-4854
DOI:10.1209/0295-5075/89/10003