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Preliminary factorization of a Shapovalov determinant

Statement

For β∈Q+, the nonzero Shapovalov determinant Dβ(λ) is a polynomial in λ whose top homogeneous part is, up to a nonzero scalar,

∏α∈Φ+⟨λ,α∨⟩∑n≥1K(β−nα).

Every irreducible factor of Dβ is proportional to ⟨λ+ρ,α∨⟩−n for some α∈Φ+ and n∈Z>0 with nα≤β. Consequently there are uniquely determined nonnegative integers mα,n(β) such that

Dβ(λ)≐∏α∈Φ+∏n≥1(⟨λ+ρ,α∨⟩−n)mα,n(β),

and mα,n(β)=0 when nα≰β.

Facts & Assumptions

Given: The PBW realization The PBW model of a Verma module, the determinant The Shapovalov determinant on a weight space, and the Casimir scalar The quadratic Casimir eigenvalue on a highest-weight module is (λ,λ+2ρ). Here γ≤β means β−γ∈Q+.

[F1]

The Shapovalov radical is the unique maximal proper submodule (The Shapovalov radical is the maximal submodule); every nonzero Verma submodule contains a singular vector (Every nonzero Verma submodule contains a singular vector).

[F2]

A singular vector of weight λ−γ gives a nonzero Verma map from M(λ−γ) (The universal property of Verma modules).

[F3]

Every root is Weyl-conjugate to a simple root, simple roots form an integral basis of Q, and Weyl reflections preserve Q (Finite Weyl positive roots and simple reflections).

Proof

technique · direct
1.1

Choose root vectors in opposite root spaces with nonzero pairing and PBW monomial bases in weight β. In the product of a positive and a negative PBW monomial, a factor of λ arises only when commuting a positive root vector with its opposite and retaining their Cartan bracket. A maximal-degree contribution pairs every root factor this way. The PBW order makes those maximal-degree pairings diagonal: an unequal pair of exponent vectors leaves a root vector, or requires a non-Cartan commutator and loses at least one degree. For exponent vector (kα) the diagonal coefficient is a nonzero constant times ∏α⟨λ,α∨⟩kα. Hence the determinant's top part is the product of these diagonal terms and is nonzero.

givenalgebra
2.1

Across all PBW monomials of weight β, the total number of occurrences of α is ∑n≥1K(β−nα): count a monomial with kα copies once for each 1≤n≤kα. This gives the displayed top part and its total degree.

step 1.1algebra
3.1

The polynomial of step 2.1 is nonzero. Suppose Dβ(λ)=0. A vector v in its kernel belongs to the radical. The space U(n+)v is finite dimensional because only finitely many weights of M(λ) lie above λ−β. Choose a nonzero vector in it of maximum weight height. It is singular, lies in the proper radical, and has weight λ−γ with 0<γ≤β. By [F2] and the Casimir scalar, the source and target have equal eigenvalues, giving 2(λ+ρ,γ)=(γ,γ). Thus the zero set of Dβ lies in the finite union of affine hyperplanes Hγ defined by these equations, 0<γ≤β.

F1F2step 2.1algebra
4.1

Every irreducible polynomial factor P of Dβ is proportional to one of the linear equations of the Hγ. Here is an elementary divisibility justification. If P divided none of their product F, choose a variable x in which P has positive degree. Over the fraction field of the other variables, P and F are coprime; clearing a Bézout identity's denominators gives AP+BF=g, with A,B polynomials and g a nonzero polynomial in the other variables. Choose values of those variables where g and the leading coefficient of P in x are nonzero. The specialized positive-degree polynomial P has a complex root, at which F≠0 by the identity, contradicting step 3.1. If P has no other variables, the same argument is the ordinary one-variable fact. Thus P divides F, and irreducibility makes it proportional to one of its linear factors.

step 3.1algebra
5.1

The highest homogeneous part of a factor Hγ is the linear form (λ,γ). Since the product of the factors' highest parts is the top part in step 2.1, unique factorization forces this linear form to be proportional to ⟨λ,α∨⟩ for some positive root α. Hence γ=cα for a positive rational c (both lie in the root lattice and positive cone). The equation of Hγ becomes ⟨λ+ρ,α∨⟩=c.

step 2.1step 4.1algebra
6.1

By [F3], every root is primitive in the root lattice Q: an integral lattice automorphism carries it to a simple basis vector. Therefore c in step 5.1 is a positive integer n. Substituting γ=nα into the equation of Hγ gives the stated affine factor, while γ≤β gives the support restriction. Distinct pairs (α,n) give distinct affine hyperplanes; unique factorization supplies the exponents.

F3step 5.1algebra∎

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