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Galois fixed points recover finite-dimensional scalar extensions
Statement
Let be finite Galois with group , and let be a finite-dimensional semilinear -space. Then is an -linear isomorphism. If is an -algebra and the action is by semilinear algebra automorphisms, this is an algebra isomorphism. For a finite-dimensional -space with the canonical action on , Here is injective, so is a copy of . Consequently , respecting algebra multiplication and units when is an -algebra.
Facts & Assumptions
Semilinear actions and canonical tensor actions have the formulas in Semilinear Galois actions, twists, and split central idempotents.
Finite Galois implies and : Equivalent characterizations of a finite Galois extension.
The trace pairing of a finite separable extension is nondegenerate: The trace form of a finite extension is nondegenerate exactly when the extension is separable.
For a separable extension, trace is the sum of the distinct embeddings: Norm and trace from embeddings, with the inseparable exponent in the norm formula. Here normality makes those embeddings precisely .
Distinct multiplicative characters of a group are linearly independent over the target field: Dedekind's linear independence theorem for distinct characters.
Tensor products of free modules have the product basis, including empty bases: The elementary tensors of two bases form the product basis of the tensor product.
Proof
Given: , , and as stated. All bases and sums used below are finite.
Put , choose an -basis of , and form its trace Gram matrix . Separability and nondegeneracy make invertible. Set . Then . The invertible coefficient matrix also shows that is a basis.
Any finite -independent list in is -independent. Indeed, if a relation exists, select one with the least positive number of nonzero coefficients and normalize one of those coefficients to . Applying and subtracting produces a relation with that coefficient zero; minimality forces every other coefficient to be fixed by every . They all lie in , contradicting -independence. A one-term relation is already impossible since a nonzero scalar cannot annihilate a nonzero vector.
For the canonical action, choose a finite -basis of . Each tensor has a unique expression : the product -basis in F6, regrouped by the , proves existence and uniqueness of its coefficients in . Such a tensor is fixed exactly when for every , equivalently each . It then equals . Conversely every is fixed. This also proves that is injective, including the empty-basis case.
Let and . A relation among the rows of vanishes on the , hence by -linearity on every ; restricting to and using independence of the distinct automorphisms as multiplicative characters makes every coefficient zero. Thus is invertible. The trace formula gives , so . Its row at yields .
Any tensor in the kernel is a finite sum . By eliminating dependent members of the finite list , rewrite it as with the -independent and invariant. Its image is , so step 1.2 forces every . Hence the tensor is zero and is injective. For the domain and codomain are zero and the same argument uses the empty list.
For define . For , semilinearity gives , since permutes the finite group. Moreover . Thus , and is onto. The formula is -balanced and -linear.
If is an algebra, its fixed space is an -subalgebra containing . For invariant and , and . Distributing over finite sums proves multiplicativity on all tensors. Together with bijectivity, this proves both algebra assertions. If , and the map is the usual multiplication ; the proof divides by no group order in any characteristic. [F1, step 3.1, step 2.2, step 1.3, algebra] QED
Remarks
The local trace-dual formula refines the evaluation-matrix proof in Zheng, Theorem 3.8.1, pp.132–133. Its injectivity argument uses finite lists, so no choice of an infinite invariant basis is needed.
Depends on
Semilinear Galois actions, twists, and split central idempotents
Equivalent characterizations of a finite Galois extension
The trace form of a finite extension is nondegenerate exactly when the extension is separable
Norm and trace from embeddings, with the inseparable exponent in the norm formula
Dedekind's linear independence theorem for distinct characters
The elementary tensors of two bases form the product basis of the tensor product