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Virasoro Verma modules have a unique simple highest-weight quotient
Statement
Let be the Virasoro algebra with basis and commutator convention of def-virasoro-algebra; the countable basis of the Witt modes is fixed by def-witt-algebra. Put
For , let be the one-dimensional -representation on which acts by , by , and each for by zero. These scalars satisfy the restricted Virasoro brackets, as verified below. Define the induced Verma module
with acting by left multiplication on the first factor. Then has a unique simple highest-weight quotient
where is the sum of all proper -submodules of . Choose a PBW order with all negative modes first, then , then positive modes. The ordered negative-mode monomials on form a basis of ; acts on a monomial by . In particular, the weight- space is , and all other weights lie in .
Statement references
Facts & Assumptions
Given: The Virasoro and Witt mode conventions and the scalar parameters in the Statement.
Virasoro algebra in the convention fixes , with central.
Witt algebra of Laurent polynomial vector fields realizes the Witt modes as on the Laurent-polynomial algebra; their span is the Witt algebra in the Virasoro direct sum.
Representations of Lie algebras: a representation is a linear action satisfying the Lie bracket relation.
Highest-weight vector and module for Virasoro: is highest weight of weight and charge when for , , and ; its generated module is spanned by finite words in the Virasoro modes.
The universal enveloping algebra as a tensor quotient constructs by imposing .
PBW for countably presented Kac Moody Lie algebras: for a complex Lie algebra with a supplied countable ordered basis, the ordered monomials form a basis of its universal enveloping algebra, and the Lie algebra embeds in it.
Proof
The subspace is a Lie subalgebra: for , the bracket in [F1] is again in ; the central term can occur only when , when its coefficient is zero. On , brackets of two positive modes and brackets of with a positive mode act by zero, as do all brackets with . Thus the stated scalar action satisfies [F3] and defines a one-dimensional -representation.
The inclusion induces by the quotient construction [F5]. Form and as in the Statement. The balanced tensor relation gives for , , and .
The modes are linearly independent: if a finite sum is zero, projection to gives ; applying this derivation to gives , so Laurent-monomial independence forces every . The direct-sum definition of Vir also makes independent. Thus is a supplied countable basis. Order it with all negative modes first, then , then positive modes. This puts a basis of last. Applying [F6] to this ordered basis and to the basis of shows that is injective and that the PBW basis of factors uniquely as a negative-mode monomial followed by a -monomial. Tensoring over evaluates the latter monomial on , leaving exactly the ordered negative-mode monomials on as a basis of . The empty monomial is therefore nonzero, and the equalities in step 2.1 with [F4] show that it is a highest-weight vector. By [F1], ; hence the monomial has weight . Only the empty monomial has weight , so and every other basis vector has weight for an integer .
Every submodule is stable under . Each vector is a finite sum of distinct -eigencomponents by the basis in step 3.1; polynomial interpolation in projects any such vector onto each component, so every submodule is graded. If a proper submodule contained a vector with nonzero weight- component, the same projection would put a nonzero multiple of in . Since generates , this would force , a contradiction. Thus every proper submodule lies in the sum of the positive-level spaces. Their sum also lies there and is proper because it misses .
The quotient is nonzero because . If a submodule of this quotient is nonzero and proper, its preimage is a proper submodule of strictly containing , contradicting the definition of as the sum of all proper submodules. Hence the quotient is simple and highest weight. The kernel of any simple quotient is a maximal proper submodule, so it is contained in and, because is proper, maximality forces that kernel to equal . Therefore this is the unique simple highest-weight quotient.