Alphabeta Math
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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(Ch⊕Ce)Cλ, realised concretely as U(sl2)/Jλ with Jλ the left ideal generated by e and h−λ(h) (Universal enveloping algebra, Highest-weight vectors and modules). Then M(λ) has basis vk=fk⋅v0, k≥0, on which h⋅vk=(λ(h)−2k)vk,f⋅vk=vk+1,e⋅vk=k(λ(h)−k+1)vk−1; 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 v−1=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 Ch⊕Ce, 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 e⋅v0=0 and h⋅v0=λ(h)v0, and fk⋅v0 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]=kfk−1(h−(k−1)) holds for every k≥1, by induction from [e,f]=h and [h,f]=−2f. [L1]

[L4]

A finite-dimensional irreducible sl2-module of highest weight m≥0 is isomorphic to V(m) of All irreducible finite-dimensional sl2 modules.

Verification

technique · direct
1.1L1L2

The relations h↦λ(h) and e↦0 define a character χλ:U(Ch⊕Ce)→C. By PBW, multiplication is a linear isomorphism U(Cf)⊗U(Ch⊕Ce)⟶U(sl2). Tensoring this factorisation over U(Ch⊕Ce) with the one-dimensional module Cλ identifies M(λ) linearly with U(Cf). Thus the classes of fk, k≥0, are a basis of M(λ).

2.1L2L3step 1.1

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

3.1step 2.1

If λ(h)∉Z≥0, then e⋅vk≠0 for every k≥1. Given 0≠w=∑k=0Nckvk, choose the largest K with cK≠0. For k<K one has eKvk=0, whereas eKvK=K!∏j=1K(λ(h)−j+1)v0≠0. Thus eKw is a nonzero multiple of v0. Hence v0∈U(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.

3.2step 2.1

If λ(h)=n is a nonnegative integer, then e⋅vn+1=0 by step 2.1, and K=∑k≥n+1Cvk is a nonzero proper submodule. Let N be a submodule not contained in K, and choose a finite nonzero sum w=∑ckvk∈N∖K. Since the h-eigenvalues n−2k are pairwise distinct, a polynomial in h isolates from this finite sum a nonzero term cjvj∈N with j≤n. Then ejvj=j!∏r=1j(n−r+1)v0≠0, so v0∈N 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.

4.1L4step 3.2

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 n−2k and operators f,e acting by vk↦vk+1 and vk↦k(n−k+1)vk−1; hence the quotient is the finite-dimensional simple module V(n) by [L4].

5.1A1step 1.1step 2.1step 3.1step 3.2step 4.1∎

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)∈Z≥0, in which case that quotient is V(λ(h)); this proves all the assertions.

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