1997
DOI: 10.1088/0305-4470/30/5/024
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Eigenvalues of Casimir invariants for unitary irreps of

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Cited by 2 publications
(4 citation statements)
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“…We now aim to prove the following weaker version of the Theorem above, using the Lemma: Proof: From the decomposition (73) this is enough to prove part (i) of the proposition. As to the second part we proceed as in the proof of Theorem 2 and suppose 0 = w + ∈ V ⊗ V (Λ) is also a maximal weight vector of the same weight ν.…”
Section: Appendix Bmentioning
confidence: 99%
See 1 more Smart Citation
“…We now aim to prove the following weaker version of the Theorem above, using the Lemma: Proof: From the decomposition (73) this is enough to prove part (i) of the proposition. As to the second part we proceed as in the proof of Theorem 2 and suppose 0 = w + ∈ V ⊗ V (Λ) is also a maximal weight vector of the same weight ν.…”
Section: Appendix Bmentioning
confidence: 99%
“…Note that strictly speaking, this formula is only valid on the Zariski dense subset as mentioned earlier. For more on the general case, see [72,73]. In graded index notation, we furthermore have γr = (−1)…”
Section: Corollarymentioning
confidence: 99%
“…( 32). Now by using the relations (30,31,50) and looking only for those terms which give a vector proportional to X h we find that…”
Section: Highest Weight Propertymentioning
confidence: 99%
“…A general theorem states [29] that tensor products of type I unitary representations are always completely reducible into representations which are also of type I. Moreover, since the module which acts for the impurity spaces is typical it follows from [31] (see Proposition 2) that all the modules occuring in the decomposition of the tensor product space are in fact typical.…”
Section: Highest Weight Propertymentioning
confidence: 99%