Work over with a finite-dimensional semisimple Lie algebra . Choose a Cartan subalgebra , its root system , a positive system and its simple roots. Let be the Weyl group, generated by the corresponding root reflections, and put , the Weyl vector. The finite-dimensional irreducible highest-weight representation is indexed by a dominant integral weight .
If is the weight lattice, its group ring has formal symbols with multiplication . The formal character is
where is a weight space. For a weight , define the Weyl alternant ; the sign is the determinant of on the real root span, equivalently the parity of its expression in simple reflections.
The Weyl character formula is
The second denominator is the Weyl denominator formula. The quotient can initially be taken in the fraction field of the group ring; the formula says it is the finite character on the left, so its apparent singularities are removable. The shifts by make strictly dominant.
Let and identify the real weight and Cartan spaces using a Weyl group-invariant positive inner product. For a regular , meaning for every root, specialize to . Then the value of the formal character at is , but both Weyl alternants in the Weyl character formula vanish there. We compute their leading terms instead of substituting into that zero-over-zero expression.
Expand
For every root reflection , replacing by changes the sign of , by replacing with in the sum. Replacing by also changes its sign, by replacing with . Thus the polynomial vanishes whenever or lies on any reflecting hyperplane. It is divisible by in its first variables and by in its second variables. Distinct positive roots give distinct linear factors; each product has degree .
The polynomial has degree in each group of variables. Therefore for , and for it has the form
with a constant independent of both variables. At , the Weyl denominator formula gives
Consequently . For strictly dominant , its leading coefficient is nonzero, and the ratio of the two Weyl alternants tends to
The coroot is , so the root-length factors cancel in each ratio. This proves the Weyl dimension formula by the lowest-degree alternant proof of the Weyl dimension formula, including the limiting step.