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The simple modules of SL_2 and its fundamental representation

Example

Assume the Axiom of Choice inherited from the named suppliers. Let k be a field and G=SL2 with its diagonal maximal torus T2, upper triangular Borel B and root datum X(T2)=Zχ, α=2χ, α∨=χ∨ (The root datum of a split reductive group, Structure of SL_2 and root coordinates). The fundamental weight is ω=χ, the dominant characters are X(T2)+={mω:m≥0}, and Dominant weights classify the simple rational representations of a split reductive group attaches to each m≥0 exactly one simple module L(m), with L(0) the trivial representation and L(1)=k2 the standard representation (Weights, dominant weights and the highest-weight order of a rational representation). For every m, L(m)mχ is one-dimensional and all other weights of L(m) belong to {mχ,(m−2)χ,…,−mχ}, each with multiplicity at most one; in particular dim⁡kL(m)≤m+1. If p=char⁡(k)>0, the vectors e1p,e2p span a two-dimensional simple submodule of the symmetric power Sp(k2) with highest weight pχ, so this submodule is isomorphic to L(p), realized as the Frobenius twist of the standard module L(1) through g⋅eip=(g⋅ei)p.

Facts & Assumptions

Given: AC; a field k, G=SL2 with diagonal torus T2, upper triangular Borel B=T2⋉U+, root groups U+={(1 a0 1)} and U−={(1 0a 1)}, and a prime p=char⁡(k)>0 in the last part.

[F1]

Root coordinates of SL2. X(T2)=Zχ, Φ={±2χ}, α=2χ, α∨=χ∨ with ⟨χ,α∨⟩=1, the Weyl group is {1,sα} acting by sα(χ)=χ−⟨χ,α∨⟩α=−χ, uα(a)=(1 a0 1), u−α(a)=(1 0a 1), and SL2 is generated by U+ and U− (Structure of SL_2 and root coordinates, The root datum of a split reductive group).

[F2]

Classification of simple modules. The map sending a simple rational representation of G to its highest weight is a bijection onto X(T2)+; we write L(m) for the simple module of highest weight mχ (Dominant weights classify the simple rational representations of a split reductive group, Weights, dominant weights and the highest-weight order of a rational representation).

[F3]

Simple modules and primitive vectors. Every simple rational representation V of G contains a primitive vector v, unique up to a nonzero scalar, whose weight is the highest weight λ of V; one has Vλ=kv, every weight μ of V satisfies μ=λ−∑mαα with mα≥0, and the set of weights is stable under the Weyl group (Simple rational representations have a unique highest weight, The normalizer of the torus permutes weight spaces).

[F4]

Modules generated by a primitive vector. If a rational representation W of G is generated as a G-module by a primitive vector v of weight λ, then W is generated as a U−-module by v, and W=kv⊕⨁μ<λWμ with Wλ=kv (Modules generated by a primitive vector, Primitive vectors for a Borel pair).

[F5]

Root-group expansion. For a weight vector v∈Vλ and any root β there are vi∈Vλ+iβ with uβ(c)⋅v=v+∑i≥1civi, finitely many nonzero (Expansion of a root-group translate of a weight vector).

[F6]

Weight decompositions. The weight spaces of a rational T2-representation are the eigenspaces of the diagonalizable group T2, and every subrepresentation is the direct sum of its intersections with those weight spaces; in particular a nonzero subrepresentation contains a nonzero weight vector (Representations of diagonalizable groups split into character eigenspaces, Rational representations and comodules of an affine group scheme).

[F7]

Symmetric powers. For a k-vector space V, Sp(V) is the quotient of V⊗p by the symmetric relations, with basis e1ae2p−a (0≤a≤p) when V=k2; a representation of G on V induces a rational representation on Sp(V) by functoriality, and in characteristic p the Frobenius identity (x+y)p=xp+yp and the binomial expansion hold (Symmetric algebra of a vector space, Rational representations and comodules of an affine group scheme).

For the basis assertion, the maps e1↦x, e2↦y identify S(k2) with k[x,y]: the map from the tensor algebra kills the commutator relations, and the inverse sends x,y to the commuting generators e1,e2. Both composites fix the generators, hence are identities. The degree-p monomials therefore form the stated basis. The substitution action of any g∈SL2(R) preserves degree and respects the group law; its coefficients are polynomials in the matrix entries, so each symmetric-power action is rational.

Verification

Given: AC; a field k, G=SL2 with diagonal torus T2, upper triangular Borel B=T2⋉U+, root groups U±, and a prime p=char⁡(k)>0 in the last part.

Proof technique: direct.

1.1F1F2

With the identification X(T2)=Zχ of [F1], the fundamental weight is ω=χ and X(T2)+={mχ:m≥0}, so [F2] gives the simple modules L(m)=V(mχ) for m≥0. The trivial representation is one-dimensional hence simple with highest weight 0, so L(0) is the trivial representation. The standard representation k2 is simple: for any nonzero v=(a,b) one has (a 0b a−1)e1=v when a≠0 and (0 −b−1b 0)e1=v when a=0, so the submodule generated by any nonzero vector is all of k2; moreover e1 is fixed by U+ and is a T2-eigenvector of weight χ, so e1 is primitive of weight χ=ω and k2≅L(1) by [F2].

1.2F3F4F5

Fix m≥0 and let v∈L(m) be a primitive vector of weight mχ, which exists and is unique up to scalar by [F3]. By [F4] L(m) is generated as a U−-module by v, and U−=U−α≅Ga. By [F5] write u−α(c)⋅v=∑i≥0civi, where v0=v, vi∈L(m)(m−2i)χ, and only finitely many vi are nonzero. Let W=span⁡k{vi:i≥0}. For every k-algebra R and a∈R, the group law gives u−α(a)⋅(u−α(c)⋅v)=u−α(a+c)⋅v; comparing coefficients of cj in these polynomial expressions yields u−α(a)⋅vj=∑i≥j(ij)ai−jvi, so WR is stable under every U−(R)-point. Thus W is a U−-submodule containing v, and [F4] implies L(m)=W. The weights (m−2i)χ are distinct, so this is a direct sum of one-dimensional spaces kvi for the nonzero coefficients; hence every weight space of L(m) has dimension at most one.

1.3F7given

Assume now p=char⁡(k)>0 and put W=ke1p⊕ke2p⊆Sp(k2). For g∈SL2(R) with ge1=ae1+ce2, the multinomial expansion in characteristic p gives g⋅e1p=(ae1+ce2)p=ape1p+cpe2p∈WR, and likewise g⋅e2p=(be1+de2)p=bpe1p+dpe2p∈WR; thus W is a G-submodule of Sp(k2), of dimension two because e1p,e2p are distinct basis monomials. The same computation is the identity g⋅eip=(g⋅ei)p.

2.1F1F3step 1.2

If vi≠0, then (m−2i)χ is a weight of L(m), so by the Weyl-group stability of [F3] and sα(χ)=−χ of [F1], the character (2i−m)χ is again a weight; by [F3] applied to L(m) it has the form (m−2j)χ with j≥0, so 2i−m=m−2j, that is i+j=m and 0≤i≤m. Hence at most m+1 of the vectors vi are nonzero and dim⁡kL(m)≤m+1; every weight other than mχ lies in {(m−2)χ,…,−mχ} with multiplicity at most one.

2.2F1F6F7step 1.3

The submodule W is T2-stable with weight spaces ke1p of weight pχ and ke2p of weight −pχ. Let S⊆W be a nonzero submodule; by [F6] S contains a nonzero weight vector, hence a nonzero multiple of e1p or of e2p. If e1p∈S, then u−α(1)⋅e1p=e1p+e2p∈S and hence e2p∈S; if e2p∈S, then uα(1)⋅e2p=e2p+e1p∈S and hence e1p∈S. In both cases S=W, so W is simple.

3.1F2F3step 1.3step 2.2∎

Finally e1p is fixed by U+ and is a T2-eigenvector of weight pχ, so it is a primitive vector of weight pχ in the simple module W; the submodule it generates is contained in W by step 1.3 and contains it by step 2.2, so it is all of W, and pχ is dominant. By the classification [F2] the simple module with highest weight pχ=pω is L(p), whence W≅L(p). In the basis e1p,e2p of W, step 1.3 gives the entrywise p-th powers of the standard representation matrices. These are the action matrices of the Frobenius twist L(1)(p). The k-linear map sending its two basis vectors to e1p,e2p is therefore a G-module isomorphism onto W, over every field k of characteristic p.

Remarks

  • The first part of the verification is the standard weight analysis of the simple SL2-modules: the U−-orbit of a highest weight vector has one nonzero coefficient in each admissible weight space, so the weight spaces are one-dimensional and the weights lie between mχ and −mχ.
  • The computation g⋅eip=(g⋅ei)p shows that the p-th symmetric power always contains the Frobenius twist L(1)(p)≅L(p). For 0≤m<p, Sm(k2) is simple: a nonzero submodule contains a weight monomial e1ae2m−a by [F6]; the coefficient of tm−a in its universal U+-translate is e1m, so the submodule contains e1m. The universal U−-translate of e1m has coefficients (mi)e1m−ie2i, all nonzero because m<p, so the submodule is the whole symmetric power. Coefficients belong to the submodule by its coaction criterion, rather than by interpolation over k.

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