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 original | Inglés |
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Páginas (desde-hasta) | 6 |
Número de páginas | 1 |
Publicación | Physical Review A - Atomic, Molecular, and Optical Physics |
Volumen | 65 |
N.º | 4 |
DOI | |
Estado | Publicada - 2002 |
Publicado de forma externa | Sí |