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Overlaps between the irreducible representations of two SO(7) subgroups of SO(8) used in the quark model of the atomic f shell

B R Judd, G M S Lister and N Vaeck

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In his studies of f electrons in atoms, Racah introduced the group SO(7) and its subgroup G2, with irreducible representations (irreps) W and U. By using a quarklike basis, these groups can be conveniently embedded in SO(8). This larger group, with irreps V, possesses two other SO(7) groups as subgroups that themselves contain G2 as a common subgroup. One of them, SO(7)' (with irreps W'), has been used to derive new selection rules on operators of physical interest. We describe methods for calculating the overlaps (VWU mod VW' U), the ultimate aim being to facilitate the transformations between SO(7) and SO(7)'. A table of relevant 6-U symbols (the G2 generalizations of 6-j symbols) is given. When V possesses null triality (that is, when the symbols labelling the open ends of the Dynkin diagram for SO(8) are equal), an undetermined phase in the overlaps can be used to generate matrix representations of S3, the permutation group on three objects. A brief table of zero overlaps is given. A remarkable factorization of the overlaps ((4310)W(40) I(4310)W'(40)) is noted, where (4310) is the irrep of SO(8) with dimension 25725.


PACS

02.20.-a Group theory

12.39.-x Phenomenological quark models

MSC

20Cxx Representation theory of groups (See also 19A22 (for representation rings and Burnside rings))

20Bxx Permutation groups

Subjects

Mathematical physics

Particle physics and field theory

Dates

Issue 19 (7 October 1993)



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