Group Theory in Physics 1997
DOI: 10.1016/b978-012189800-7/50006-6
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Group Theory in Quantum Mechanical Calculations

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Cited by 66 publications
(134 citation statements)
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“…Let Φ be the representation over End(H N sym ) associated with φ s . Since End(H N sym ) ∼ = H N sym ⊗ H N * sym one has Φ ∼ = φ s ⊗ φ * s , the tensor product or two totally symmetric SU (d)-irreps, therefore in the decomposition of Φ each SU (d)-irrep appears once [12]. As A U i = 0 simply means that the F i 's transform according to the adjoint representation, one must have…”
Section: B Algebraic Approachmentioning
confidence: 99%
“…Let Φ be the representation over End(H N sym ) associated with φ s . Since End(H N sym ) ∼ = H N sym ⊗ H N * sym one has Φ ∼ = φ s ⊗ φ * s , the tensor product or two totally symmetric SU (d)-irreps, therefore in the decomposition of Φ each SU (d)-irrep appears once [12]. As A U i = 0 simply means that the F i 's transform according to the adjoint representation, one must have…”
Section: B Algebraic Approachmentioning
confidence: 99%
“…The first step is to choose a Cartan subalgebra h of g, which is by definition just a Cartan subalgebra of its even part g0: its dimension is called the rank of g. (If g0 has a non-trivial center z 0 and a semisimple part g ss 0 , so that g0 = z0 ⊕ g ss 0 , then h = z0 ⊕ h ss , where h ss is a Cartan subalgebra of g ss 0 .) As in the case of ordinary semisimple Lie algebras, the specific choice of Cartan subalgebra is irrelevant, since they are all conjugate [14,15]. This gives rise to the root system ∆ = ∆ 0 ∪ ∆ 1 of g, where the set ∆ 0 of even roots is just the root system of g0, as an ordinary reductive Lie algebra, and the set ∆ 1 of odd roots is just the weight system of g1, as a g0-module.…”
Section: Basic Classical Lie Superalgebrasmentioning
confidence: 99%
“…Note, again, that this property is not guaranteed automatically, as it would be for ordinary semisimple Lie algebras, according to Cartan's criterion for semisimplicity. In fact, it turns out that an even, graded symmetric, invariant bilinear form on a simple Lie superalgebra is either non-degenerate or identically zero [14,15] and that, in particular, the Killing form of a simple Lie superalgebra defined by the supertrace operation in the adjoint representation may vanish identically. Moreover, there are simple Lie superalgebras whose Killing form vanishes identically but which are still basic because they admit some other non-degenerate, even, graded symmetric, invariant bilinear form.…”
Section: Basic Classical Lie Superalgebrasmentioning
confidence: 99%
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