Representation Functions for SU(3)
- 1 October 1969
- journal article
- research article
- Published by AIP Publishing in Journal of Mathematical Physics
- Vol. 10 (10) , 1968-1970
- https://doi.org/10.1063/1.1664791
Abstract
``Euler'' decomposition for SU(3) has been found by analytic continuation from the ``Euler'' decomposition of SU(2, 1), which is based on the factorization SU(2, 1) = SU(2) × Au × A × SU(2) derived by Hillion [Au ∼ U(1) and A is one‐parameter subgroup of the V‐spin subgroup.] For the degenerate case the SU(3) representation functions can be found by transforming to a new basis where the V‐spin subgroup is diagonal. The result is a sum of products, each product containing two D‐functions, one d‐function, and an exponential function exp [imχ]. As is well known, every representation D(p, q) can be reduced from the direct product D(p, 0) × D(q, q). The nondegenerate representation functions can then be directly written down using the SU(3) CG coefficients, which are relatively simple for the above‐mentioned case.Keywords
This publication has 3 references indexed in Scilit:
- Some unitary representations ofSU p,q groupsIl Nuovo Cimento A (1971-1996), 1967
- Polynominal Bases and Isoscalar Factors for SU(3)Journal of Mathematical Physics, 1966
- On the Representations of the Semisimple Lie Groups. IIJournal of Mathematical Physics, 1963