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Preliminary factorization of a Shapovalov determinant
Statement
For , the nonzero Shapovalov determinant is a polynomial in whose top homogeneous part is, up to a nonzero scalar,
Every irreducible factor of is proportional to for some and with . Consequently there are uniquely determined nonnegative integers such that
and when .
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 . Here means .
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).
A singular vector of weight gives a nonzero Verma map from (The universal property of Verma modules).
Every root is Weyl-conjugate to a simple root, simple roots form an integral basis of , and Weyl reflections preserve (Finite Weyl positive roots and simple reflections).
Proof
Choose root vectors in opposite root spaces with nonzero pairing and PBW monomial bases in weight . In the product of a positive and a negative PBW monomial, a factor of 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 the diagonal coefficient is a nonzero constant times . Hence the determinant's top part is the product of these diagonal terms and is nonzero.
Across all PBW monomials of weight , the total number of occurrences of is : count a monomial with copies once for each . This gives the displayed top part and its total degree.
The polynomial of step 2.1 is nonzero. Suppose . A vector in its kernel belongs to the radical. The space is finite dimensional because only finitely many weights of lie above . Choose a nonzero vector in it of maximum weight height. It is singular, lies in the proper radical, and has weight with . By [F2] and the Casimir scalar, the source and target have equal eigenvalues, giving . Thus the zero set of lies in the finite union of affine hyperplanes defined by these equations, .
Every irreducible polynomial factor of is proportional to one of the linear equations of the . Here is an elementary divisibility justification. If divided none of their product , choose a variable in which has positive degree. Over the fraction field of the other variables, and are coprime; clearing a Bézout identity's denominators gives , with polynomials and a nonzero polynomial in the other variables. Choose values of those variables where and the leading coefficient of in are nonzero. The specialized positive-degree polynomial has a complex root, at which by the identity, contradicting step 3.1. If has no other variables, the same argument is the ordinary one-variable fact. Thus divides , and irreducibility makes it proportional to one of its linear factors.
The highest homogeneous part of a factor is the linear form . 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 for some positive root . Hence for a positive rational (both lie in the root lattice and positive cone). The equation of becomes .
By [F3], every root is primitive in the root lattice : an integral lattice automorphism carries it to a simple basis vector. Therefore in step 5.1 is a positive integer . Substituting into the equation of gives the stated affine factor, while gives the support restriction. Distinct pairs give distinct affine hyperplanes; unique factorization supplies the exponents.
Depends on
- The Shapovalov determinant on a weight space
- The PBW model of a Verma module
- The Shapovalov radical is the maximal submodule
- Every nonzero Verma submodule contains a singular vector
- The universal property of Verma modules
- The quadratic Casimir eigenvalue on a highest-weight module is $(\lambda,\lambda+2\rho)$
- Finite Weyl positive roots and simple reflections
- Root reflections and the Weyl group action
- The Weyl vector rho for a chosen positive system
Used by
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Sources
- Pavel Etingof, Representations of Lie Groups, Exercise 8.15(iv)–(v), pp. 45–46 (standard reference, not scraped)