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Verma modules for sl2

Example

Assume the Axiom of Choice. Let sl2=sl2(C) have basis e,f,h with [e,f]=h, [h,e]=2e, [h,f]=2f (The special linear Lie algebra sl_2), and for every linear functional λ(Ch) let M(λ) be the induced module U(sl2)U(ChCe)Cλ, realised concretely as U(sl2)/Jλ with Jλ the left ideal generated by e and hλ(h) (Universal enveloping algebra, Highest-weight vectors and modules). Then M(λ) has basis vk=fkv0, k0, on which hvk=(λ(h)2k)vk,fvk=vk+1,evk=k(λ(h)k+1)vk1; it is infinite-dimensional, and it has a finite-dimensional simple quotient exactly when λ(h) is a nonnegative integer. In that case the quotient is V(n) of All irreducible finite-dimensional sl2 modules with n=λ(h).

Set v1=0 in the displayed action formula. The one-dimensional Borel module Cλ has h acting by λ(h) and e acting by zero.

Facts & Assumptions

Given: The Axiom of Choice, sl2 with its basis, a functional λ(Ch) determined by the scalar nλ=λ(h), the Borel subalgebra ChCe, and the quotient module M(λ) with generator v0=1+Jλ.

[A1]

The Axiom of Choice (The Axiom of Choice) is inherited from the cited general definitions of highest weight and dominant integral weight. The explicit rank-one calculations and supplied-basis PBW argument make no further use of choice.

[L1]

The monomials fahbec in the ordered basis (f,h,e) form a basis of U(sl2); moreover U(sl2)=U(Cf)U(Ch)U(Ce) as a linear span (Poincaré–Birkhoff–Witt theorem).

[L2]

In M(λ) one has ev0=0 and hv0=λ(h)v0, and fkv0 is the class of fk; the module is generated by v0 (Highest-weight vectors and modules).

[L3]

In U(sl2) the commutation identity [e,fk]=kfk1(h(k1)) holds for every k1, by induction from [e,f]=h and [h,f]=2f. [L1]

[L4]

A finite-dimensional irreducible sl2-module of highest weight m0 is isomorphic to V(m) of All irreducible finite-dimensional sl2 modules.

Verification

technique · direct
1.1

The relations hλ(h) and e0 define a character χλ:U(ChCe)C. By PBW, multiplication is a linear isomorphism U(Cf)U(ChCe)U(sl2). Tensoring this factorisation over U(ChCe) with the one-dimensional module Cλ identifies M(λ) linearly with U(Cf). Thus the classes of fk, k0, are a basis of M(λ).

L1L2
2.1

Therefore M(λ) is infinite-dimensional, and the action on vk=fkv0 is hvk=(λ(h)2k)vk (eigenvalue computation), fvk=vk+1, and evk=[e,fk]v0=k(λ(h)k+1)vk1 by [L3]; in particular evk=0 exactly when k=0 or λ(h)=k1.

L2L3step 1.1
3.1

If λ(h)Z0, then evk0 for every k1. Given 0w=k=0Nckvk, choose the largest K with cK0. For k<K one has eKvk=0, whereas eKvK=K!j=1K(λ(h)j+1)v00. Thus eKw is a nonzero multiple of v0. Hence v0U(sl2)w, so every nonzero submodule is all of M(λ). The module is therefore simple and infinite-dimensional and has no nonzero finite-dimensional quotient.

step 2.1
3.2

If λ(h)=n is a nonnegative integer, then evn+1=0 by step 2.1, and K=kn+1Cvk is a nonzero proper submodule. Let N be a submodule not contained in K, and choose a finite nonzero sum w=ckvkNK. Since the h-eigenvalues n2k are pairwise distinct, a polynomial in h isolates from this finite sum a nonzero term cjvjN with jn. Then ejvj=j!r=1j(nr+1)v00, so v0N and N=M(λ). Consequently every proper submodule lies in K; hence K is the unique maximal proper submodule and M(λ)/K is the unique simple quotient.

step 2.1
4.1

On M(λ)/K the classes of v0,,vn satisfy exactly the relations of V(n) from All irreducible finite-dimensional sl2 modules, with h-eigenvalues n2k and operators f,e acting by vkvk+1 and vkk(nk+1)vk1; hence the quotient is the finite-dimensional simple module V(n) by [L4].

L4step 3.2
5.1

Collecting steps 1.1–4.1, M(λ) is an infinite-dimensional highest weight module of highest weight λ, and it has a finite-dimensional simple quotient exactly for λ(h)Z0, in which case that quotient is V(λ(h)); this proves all the assertions.

A1step 1.1step 2.1step 3.1step 3.2step 4.1

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