B R Judd et al 1993 J. Phys. A: Math. Gen. 26 4991 doi:10.1088/0305-4470/26/19/028
B R Judd, G M S Lister and N Vaeck
Show affiliationsIn 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.
20Cxx Representation theory of groups (See also 19A22 (for representation rings and Burnside rings))
Issue 19 (7 October 1993)
B R Judd et al 1993 J. Phys. A: Math. Gen. 26 4991
Y S Ji et al 2009 J. Phys.: Conf. Ser. 165 012015
Giorgio Riccobene 2008 J. Phys.: Conf. Ser. 136 022053
J Ellis 2008 J. Phys.: Conf. Ser. 110 012001
Consuelo Escudero and Eduardo A Jaime 2007 J. Phys.: Conf. Ser. 90 012021
K Ohki et al 2008 J. Phys.: Conf. Ser. 97 012142
B Hillmer et al 2007 J. Phys.: Conf. Ser. 75 012002
Harald Müllejans et al 2009 Meas. Sci. Technol. 20 075101
Michael Wang et al 2007 Environ. Res. Lett. 2 024001
S Cui and Z W Chen 2009 IOP Conf. Ser.: Mater. Sci. Eng. 4 012019