The multiplicity of a weight in a finite-dimensional irreducible representation of a simple Lie
algebra
can be computed via Kostant’s weight multiplicity formula. This formula consists
of an alternating sum over the Weyl group (a finite group) and involves a
partition function known as Kostant’s partition function. Motivated by the
observation that, in practice, most terms in the sum are zero, our main results
describe the elements of the Weyl alternation sets. The Weyl alternation
sets are subsets of the Weyl group, which contributes nontrivially to the
multiplicity of a weight in a highest-weight representation of the Lie algebras
,
,
, and the exceptional
Lie algebra
.
By taking a geometric approach, we extend the work of Harris, Lescinsky, and Mabie
on ,
to provide visualizations of these Weyl alternation sets for all pairs of integral weights
and
of the
Lie algebras considered.