Baryon octupole moments

European Physical Journal A

Volumn 35, Issue 3, 2008, Pages 267-269

  Buchmann, A J ^a   Henley, E M ^b  

^a UNIVERSITY OF TÜBINGEN   (Germany)

^b UNIVERSITY OF WASHINGTON   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 42449096721     PISSN: 14346001     EISSN: None     Source Type: Journal    
DOI: 10.1140/epja/i2007-10565-4     Document Type: Article

References (17)

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14. If two of these had the same particle index, spin commutation relations would reduce them to a single Pauli matrix.
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16. For ground-state baryons an allowed operator ω must transform according to one of the irreducible representations found in the product 56 × 56 = 1 + 35 + 405 + 2695. Here, the 1, 35, 405, and 2695 dimensional representations, are respectively connected with zero-, one-, two-, and three-body operators. Because the 2695 occurs only once, there is a unique three-quark magnetic octupole operator.
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