O(3) shift operators: The general analysis
O(3) shift operators are constructed in terms of tensor operators T (j,μ) and the O(3) generators. These are of type B k l , k=−j,...,j, where B k l raises l by k, l (l+1) being the eigenvalue of the O(3) Casimir operator. Various convenient normalizations of these operators are constructed, and the...
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Veröffentlicht in: | Journal of mathematical physics 1978-10, Vol.19 (10), p.2068-2078 |
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Hauptverfasser: | , |
Format: | Artikel |
Sprache: | eng |
Online-Zugang: | Volltext |
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Zusammenfassung: | O(3) shift operators are constructed in terms of tensor operators T (j,μ) and the O(3) generators. These are of type B
k
l
, k=−j,...,j, where B
k
l
raises l by k, l (l+1) being the eigenvalue of the O(3) Casimir operator. Various convenient normalizations of these operators are constructed, and their properties and uses considered. |
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ISSN: | 0022-2488 1089-7658 |
DOI: | 10.1063/1.523587 |