English

Fundamental Weights, Permutation Weights and Weyl Character Formula

Mathematical Physics 2008-11-26 v2 High Energy Physics - Theory Group Theory math.MP Representation Theory

Abstract

For a finite Lie algebra GNG_N of rank N, the Weyl orbits W(Λ++)W(\Lambda^{++}) of strictly dominant weights Λ++\Lambda^{++} contain dimW(GN)dimW(G_N) number of weights where dimW(GN)dimW(G_N) is the dimension of its Weyl group W(GN)W(G_N). For any W(Λ++)W(\Lambda^{++}), there is a very peculiar subset (Λ++)\wp(\Lambda^{++}) for which we always have dim(Λ++)=dimW(GN)/dimW(AN1). dim\wp(\Lambda^{++})=dimW(G_N)/dimW(A_{N-1}) . For any dominant weight Λ+ \Lambda^+ , the elements of (Λ+)\wp(\Lambda^+) are called {\bf Permutation Weights}. It is shown that there is a one-to-one correspondence between elements of (Λ++)\wp(\Lambda^{++}) and (ρ)\wp(\rho) where ρ\rho is the Weyl vector of GNG_N. The concept of signature factor which enters in Weyl character formula can be relaxed in such a way that signatures are preserved under this one-to-one correspondence in the sense that corresponding permutation weights have the same signature. Once the permutation weights and their signatures are specified for a dominant Λ+\Lambda^+, calculation of the character ChR(Λ+)ChR(\Lambda^+) for irreducible representation R(Λ+)R(\Lambda^+) will then be provided by ANA_N multiplicity rules governing generalized Schur functions. The main idea is again to express everything in terms of the so-called {\bf Fundamental Weights} with which we obtain a quite relevant specialization in applications of Weyl character formula.

Cite

@article{arxiv.math-ph/9806014,
  title  = {Fundamental Weights, Permutation Weights and Weyl Character Formula},
  author = {Hasan R. Karadayi and Meltem Gungormez},
  journal= {arXiv preprint arXiv:math-ph/9806014},
  year   = {2008}
}

Comments

6 pages, no figures, TeX, as will appear in Journal of Physics A:Mathematical and General