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Virasoro Verma modules have a unique simple highest-weight quotient

Statement

Let Vir be the Virasoro algebra with basis {Ln:n∈Z}∪{C} and commutator convention of def-virasoro-algebra; the countable basis of the Witt modes is fixed by def-witt-algebra. Put

b=span⁡{Ln:n≥0}⊕CC.

For c,h∈C, let Cc,h be the one-dimensional b-representation on which L0 acts by h, C by c, and each Ln for n>0 by zero. These scalars satisfy the restricted Virasoro brackets, as verified below. Define the induced Verma module

M(c,h)=U(Vir)⊗U(b)Cc,h,v=1⊗1,

with Vir acting by left multiplication on the first factor. Then M(c,h) has a unique simple highest-weight quotient

L(c,h)=M(c,h)/J,

where J is the sum of all proper Vir-submodules of M(c,h). Choose a PBW order with all negative modes first, then L0,C, then positive modes. The ordered negative-mode monomials on v form a basis of M(c,h); L0 acts on a monomial L−n1⋯L−nrv by h+∑ini. In particular, the weight-h space is Cv, and all other weights lie in h+Z>0.

Facts & Assumptions

Given: The Virasoro and Witt mode conventions and the scalar parameters c,h∈C in the Statement.

[F1]

Virasoro algebra in the Lm convention fixes [Lm,Ln]=(m−n)Lm+n+112(m3−m)δm+n,0C, with C central.

[F2]

Witt algebra of Laurent polynomial vector fields realizes the Witt modes as dn=−zn+1∂z on the Laurent-polynomial algebra; their span is the Witt algebra W in the Virasoro direct sum.

[F3]

Representations of Lie algebras: a representation is a linear action satisfying the Lie bracket relation.

[F4]

Highest-weight vector and module for Virasoro: v is highest weight of weight h and charge c when Lnv=0 for n>0, L0v=hv, and Cv=cv; its generated module is spanned by finite words in the Virasoro modes.

[F5]

The universal enveloping algebra as a tensor quotient constructs U(g) by imposing xy−yx=[x,y].

[F6]

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

1.1F1F3algebra

The subspace b is a Lie subalgebra: for m,n≥0, the bracket in [F1] is again in b; the central term can occur only when m=n=0, when its coefficient is zero. On Cc,h, brackets of two positive modes and brackets of L0 with a positive mode act by zero, as do all brackets with C. Thus the stated scalar action satisfies [F3] and defines a one-dimensional b-representation.

2.1F5step 1.1algebra

The inclusion b↪Vir induces U(b)→U(Vir) by the quotient construction [F5]. Form M(c,h) and v as in the Statement. The balanced tensor relation gives Lnv=0 for n>0, L0v=hv, and Cv=cv.

3.1F1F2F4F5F6step 2.1algebra

The modes Ln are linearly independent: if a finite sum ∑nanLn is zero, projection to W gives ∑nandn=0; applying this derivation to z gives −∑nanzn+1=0, so Laurent-monomial independence forces every an=0. The direct-sum definition of Vir also makes C independent. Thus {Ln:n∈Z}∪{C} is a supplied countable basis. Order it with all negative modes first, then L0,C, then positive modes. This puts a basis of b last. Applying [F6] to this ordered basis and to the basis of b shows that U(b)→U(Vir) is injective and that the PBW basis of U(Vir) factors uniquely as a negative-mode monomial followed by a b-monomial. Tensoring over U(b) evaluates the latter monomial on Cc,h, leaving exactly the ordered negative-mode monomials on v as a basis of M(c,h). The empty monomial v is therefore nonzero, and the equalities in step 2.1 with [F4] show that it is a highest-weight vector. By [F1], [L0,L−n]=nL−n; hence the monomial has weight h+∑ini. Only the empty monomial has weight h, so Mh=Cv and every other basis vector has weight h+N for an integer N>0.

4.1F4step 3.1algebra

Every submodule S⊆M(c,h) is stable under L0. Each vector is a finite sum of distinct L0-eigencomponents by the basis in step 3.1; polynomial interpolation in L0 projects any such vector onto each component, so every submodule is graded. If a proper submodule contained a vector with nonzero weight-h component, the same projection would put a nonzero multiple of v in S. Since v generates M(c,h), this would force S=M(c,h), a contradiction. Thus every proper submodule lies in the sum of the positive-level spaces. Their sum J also lies there and is proper because it misses v.

5.1F4step 4.1algebra∎

The quotient M(c,h)/J is nonzero because v∉J. If a submodule of this quotient is nonzero and proper, its preimage is a proper submodule of M(c,h) strictly containing J, contradicting the definition of J 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 J and, because J is proper, maximality forces that kernel to equal J. Therefore this is the unique simple highest-weight quotient.

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