Nonrelativistic Levinson’s theorem in D dimensions

Shi Hai Dong, Zhong Qi Ma

Producción científica: Contribución a una revistaArtículorevisión exhaustiva

2 Citas (Scopus)

Resumen

The Levinson theorem for the Schrödinger equation with a spherically symmetric potential in D dimensions is uniformly established by the Sturm-Liouville theorem. It is shown that the Levinson theorem for the cases without a half bound state does not depend on the spatial dimension D, namely, the phase-shift [Formula Presented] of the scattering state with angular momentum l at zero momentum is equal to the total number [Formula Presented] of bound states multiplied by [Formula Presented] When a half bound state occurs the Levinson theorem may be modified.

Idioma originalInglés
Páginas (desde-hasta)6
Número de páginas1
PublicaciónPhysical Review A - Atomic, Molecular, and Optical Physics
Volumen65
N.º4
DOI
EstadoPublicada - 2002
Publicado de forma externa

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