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Galois orbits classify simple modules after splitting base change

Statement

In ZFC, let A be a finite-dimensional semisimple unital F-algebra and let E/F be finite Galois with group Γ, such that B=EFA is split semisimple. There is a canonical bijection between simple left A-module isomorphism classes and Γ-orbits O of simple left B-module classes. For the class S corresponding to O there is a unique positive integer mS such that EFS[W]OWmS. Distinct simple A-modules have disjoint constituent sets, and every simple B-module occurs. For A=0, both sets of classes are empty.

In particular, let G be a finite group, let F have characteristic zero, and let E/F be a finite Galois extension which is a splitting field for G. The assertions apply to A=F[G] and B=E[G]. Neither algebraic closure of F nor multiplicity one is assumed. This is conditional on the given E; it makes no assertion about existence of a finite Galois splitting field.

Facts & Assumptions

[F1]

Canonical semilinear tensor actions and inverse-pullback twists are specified in Semilinear Galois actions, twists, and split central idempotents.

[F2]

Split primitive central idempotents correspond to simple classes, equivariantly, and their orbit sums descend: Orbit sums of primitive split central idempotents descend.

[F3]

The descended orbit idempotents are precisely the primitive central idempotents of A, with one simple type per block and D=EndA(S)op: Descended orbit idempotents are primitive and their blocks have one simple type.

[F4]

Nonzero semisimple rings are finite products of matrix rings over division rings: Wedderburn–Artin theorem for semisimple rings.

[F5]

The simple left modules of such a product are its factor column modules: Simple modules over a product of matrix rings over division rings.

[F6]

Tensoring over F commutes with direct sums, by the coordinate maps: Tensor products commute with arbitrary direct sums.

[F7]

Product bases describe tensors of free modules, also for empty bases: The elementary tensors of two bases form the product basis of the tensor product.

[F8]

The simple factors of two finite composition series agree with multiplicity: Jordan–Hölder theorem for modules.

[F9]

Finite-dimensional subspaces have finite bases, independent sets extend to bases, and a proper subspace has strictly smaller dimension: If dimFV=n and U is a linear subspace of V, then U is finite-dimensional, dimFUn, and dimFU=n if and only if U=V.

[F11]

Every nonzero field element has an inverse: Field.

[F12]

Finite sums in a commutative monoid include the empty sum 0: A finite sum in a commutative monoid indexed by an arbitrary finite set.

[F14]

Strong induction permits assuming all smaller natural-number cases: Strong (complete) induction.

[F15]

Linear G-actions and k[G]-module structures correspond, as do equivariant maps and module homomorphisms: For a commutative ring R, R-linear G-actions are exactly the compatible left R[G]-module structures.

[F16]

A splitting field for G has scalar endomorphisms for every irreducible representation: A splitting field for a finite group: every irreducible representation has scalar endomorphism ring.

[F17]

A module is semisimple when it is a direct sum of simple submodules, allowing the empty sum: Semisimple modules as direct sums of simple modules.

[F18]

A ring is semisimple when its left regular module is semisimple: A semisimple ring as a ring whose left regular module is semisimple.

[F19]

The group algebra has the group basis, with multiplication [g][h]=[gh]: The group ring R[G] is a unital R-algebra with basis G, and each gG is a unit of R[G].

Proof

Given: The algebra and field hypotheses in the statement; all modules are unital left modules.

1.1

If A=0, B=0 and every unital module is zero, since w=1w=0w=0. There are no simple classes, so the empty map is the asserted bijection. Henceforth take A0. By F2–F3, each orbit O gives a block AeOMnO(DO) with one simple type SO=DOnO, where nO1. F4–F5 show that these exhaust all simple A-modules with no repetition. In particular these simples are finite-dimensional, because each is a column left ideal of the finite-dimensional algebra.

F2F3F4F5algebra
1.2

For completeness, any finite-dimensional module M over Md(E) is a sum of column modules by an explicit map. The orthogonal Ejj give M=j=1dEjjM. Choose an E-basis (vt)t=1h of E11M by F9, and send the jth standard vector in column copy t to Ej1vt. Matrix multiplication EabEj1=δbjEa1 proves module linearity. Every xEjjM equals Ej1(E1jx), proving spanning. Applying E1j to a relation k,tλktEk1vt=0 gives tλjtvt=0, proving independence. Thus M(Ed)h. For a product of matrix rings, first decompose by its coordinate identities and apply this argument to each coordinate. It includes h=0.

F9algebra
1.3

For the finite-group specialization, let G,F,E satisfy the finite-group hypotheses, and fix k=F or k=E. The field inclusion makes k characteristic zero. Let V be a finite-dimensional k[G]-module and UV a submodule. F9 supplies a finite basis u1,,ur of U extended to a basis u1,,ur,vr+1,,vd of V. Define P(jrajuj+j>rajvj)=jrajuj. Coordinate uniqueness makes P linear, with image U and PU=id. This includes U=0 and U=V.

F9algebra
2.1

Separating a matrix into its nO columns gives AeOSOnO as left A-modules. Scalar extension yields BcO(EFSO)nO: the first identification sends eaeO to (ea)cO; it is onto and injective by regrouping the tensor basis along a basis of AeO. The direct-sum isomorphism is F6, and its coordinate formula commutes with the B-action. F7 similarly gives dimE(EFSO)=dimFSO.

F1F6F7step 1.1algebra
2.2

Since G contains its identity, N=G1. F10 gives N1k0, and F11 gives its inverse N1. In the additive commutative monoid of linear endomorphisms set Q=N1gGgPg1. This finite sum is defined by F12. Composition and evaluation distribute over it: for an empty list both sides are zero, and adjoining one term follows from binary distributivity; induction on the list length proves the finite identity. Thus Q is a linear map.

F10F11F12F14step 1.3algebra
3.1

Put M=EFSO. By step 1.2 it has a finite simple decomposition. The regular module BcO consists of exactly the split factors indexed by O, each with its nonzero column multiplicity. Comparing step 2.1 with these decompositions, F8 gives nO times the multiplicity of each class in M equal to its regular-block multiplicity. Since nO>0, precisely the classes in O occur in M, each positively; no other class occurs. The use of F8 is legitimate because ordering the summands of a finite simple direct sum gives a composition series.

F2F5F8step 2.1step 1.2algebra
3.2

For hG, distributing composition and reindexing by ghg gives hQh1=N1g(hg)P(hg)1=Q. Hence Q is G-equivariant and is a module map by F15. Since U is G-stable, each gPg1 maps into U and is identity on U. Therefore Q(V)U and Q(u)=N1Nu=u for uU.

F13F15step 1.3step 2.2algebra
4.1

The canonical map Tσ(es)=σ(e)s is an isomorphism σMM: for bB, Tσ(σB1(b)m)=bTσ(m), and its inverse is Tσ1. Twisting a direct-sum decomposition therefore permutes the simple types of M without changing their multiplicities, by F8. Any two classes in O are related by a twist, so all the positive multiplicities of step 3.1 equal one integer mSO. F8 also proves its uniqueness.

F1F8step 3.1algebra
4.2

For vV, the vector vQv lies in kerQ because QvU and Q fixes U. Thus v=Qv+(vQv) belongs to U+kerQ. If uUkerQ, then u=Qu=0, proving V=UkerQ. The kernel is a submodule since Q is a module map.

step 3.2algebra
5.1

The assignment [SO]O is independent of the displayed matrix decomposition: F2 defines the orbit intrinsically via central idempotents, and F3 gives its unique simple class downstairs. Step 3.1 shows different orbits have disjoint supports and that every simple B-class is in the support assigned to its orbit. Conversely that support recovers O from SO. This proves bijectivity in both directions. If E=F, all orbits are singletons and EFSS, so the multiplicity is 1.

F2F3step 3.1step 4.1algebra
5.2

Apply strong induction on d=dimkV to the assertion that every such V is a finite direct sum of simple submodules. For d=0 use the empty sum. For d>0, a simple V is already one summand. Otherwise the definition of simplicity supplies a nonzero proper submodule U. Step 4.2 splits it off; both U and kerQ are proper, the latter because Q is identity on the nonzero U. F9 gives dimensions strictly below d for both. The induction hypothesis decomposes each into finitely many simple submodules, whose combined direct sum is V. F14 proves the assertion for every d, and F17 identifies these modules as semisimple.

F9F14F17step 4.2algebra
6.1

The group ring has the finite group basis [g], with [g][h]=[gh]; its regular action is one of the actions in F15. Apply step 5.2 to V=k[G], whose dimension is N, and then F18 to obtain semisimplicity of k[G] for both k=F,E. The basis map EFF[G]E[G], e[g]e[g], is bijective by F7 and multiplicative by the group-basis product. For the trivial group this is just EFFE, and averaging above is Q=P.

F19F7F15F18step 5.2algebra
7.1

Apply F4 to the nonzero semisimple algebra E[G]. For a factor Mn(D), its column module W=Dn is simple by F5. To compute its endomorphisms without assuming splitting, let f commute with the factor action. Commuting with E11 forces f(e1)=e1d for some dD; commuting with Ej1 gives f(ej)=ejd, and commuting with diagonal left multiplications gives f(x)=xd for every column x. Conversely each right multiplication commutes with all matrices. Their compositions reverse multiplication in D, so End(W)Dop as an E-algebra. F15 identifies this endomorphism ring with EndG(W); by the given splitting-field condition F16 it is exactly the scalar field E. Taking the opposite ring leaves E unchanged, so every division factor is E as an E-algebra. Hence E[G] is split semisimple. The general classification in step 5.1 now applies to F[G] and the given finite Galois extension and prove the specialization. All selections in this argument concern finite-dimensional spaces or finite decompositions; no additional arbitrary-index choice assumption is used. [F4, F5, F15, F16, step 5.1, step 6.1, algebra] QED

Remarks

Zheng, Proposition 4.3.2, pp.145–146, gives scalar-extension multiplicities; Wiese, Lemma 2.2.9 and Corollary 2.2.12, pp.29–30, give their Galois-orbit behavior. The local proof obtains it from descended central idempotents. The specialization steps expand Zheng's averaging argument (Theorem 4.1.6, p.139) using finite basis extension and strict dimension induction. They provide the needed finite-group semisimplicity directly.

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