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The Schur-Weyl mutual centralizer theorem on tensor powers
Statement
Let be a finite-dimensional complex vector space, let , and let carry the left place action of (Commuting symmetric-group and linear actions on a tensor power). Let be the image of the algebra homomorphism extending the place action, and let be the linear span of the diagonal operators . Then:
- (Mutual centralizers.) and .
- (Uniqueness of the identification.) is a unital -subalgebra of and equals the image of the diagonal action of the universal enveloping algebra , that is the unital subalgebra generated by the operators , (Diagonal tensor operators span the symmetric centralizer).
All statements include , where .
Facts & Assumptions
Given: a finite-dimensional complex vector space , an integer , with its left -action, the algebra and the space of the Statement.
The left place action of on and the diagonal action of commute, and is linear in (Commuting symmetric-group and linear actions on a tensor power). It is a Lie algebra homomorphism: operators in distinct tensor positions commute, and in each position the commutator is , so .
The map is a linear isomorphism, equivariant for the place action and conjugation, and where is the centralizer of the place action and is the unital subalgebra generated by the , which is the image of the diagonal action of (Diagonal tensor operators span the symmetric centralizer).
Every finite-dimensional -module is completely reducible (Maschke's theorem for finite groups over fields whose characteristic does not divide ).
The modules form a complete irredundant list of the finite-dimensional irreducible complex -representations (Specht modules classify the complex irreducibles of ).
A nonzero intertwiner between irreducible representations is an isomorphism, and every endomorphism of an irreducible representation over an algebraically closed field is scalar (Schur's lemma for irreducible representations: a nonzero intertwiner is an isomorphism, and is a division ring, Over an algebraically closed field, every endomorphism of an irreducible representation is scalar).
For a finite-dimensional completely reducible representation of a group the isotypic decomposition into the sums of copies of the distinct irreducible subrepresentations is unique; and for an irreducible and an -isotypical module , evaluation , , is an isomorphism under which every -map is uniquely of the form for a linear , with -spaces carrying the trivial action and composition preserved (The isotypic decomposition of a completely reducible representation is unique, Isotypical evaluation and multiplicity subspaces).
for positive integers , and the simple left modules over such a product are the column modules , one isomorphism class per factor, each supported on exactly one factor (If is algebraically closed and , then , Simple modules over a product of matrix rings over division rings).
Under the correspondence between -linear -actions and compatible left -module structures, the subrepresentations of a representation are exactly the -submodules and is irreducible if and only if it is simple as a -module; -equivariant maps are exactly the -module homomorphisms (For a commutative ring , -linear -actions are exactly the compatible left -module structures, Under the dictionary, subrepresentations are exactly submodules and irreducible representations are exactly simple modules).
Proof
[construct] Recall that is a unital subalgebra of , because it is the image of a unital algebra homomorphism, and that is a unital subalgebra, because for ; both contain (for take , and for note for every and is nonempty).
By [F3] the -module is completely reducible, so by [F4] and the uniqueness of the isotypic decomposition in [F6] there are subspaces for in the finite set with , each is -isotypical, and the evaluation maps of [F6] give -isomorphisms with carrying the trivial action; consequently the action of on corresponds to , where is the action on the irreducible .
The simple left -modules are, by [F7], the column modules of the factors of a decomposition , one class per factor and each supported on one factor; by [F8] the irreducible complex representations of the group are exactly the simple left -modules, so by [F4] the isomorphism classes of simple left -modules are exactly the classes , . Hence the factors are indexed by the partitions of , with for the factor attached to , and .
An endomorphism of a tensor product, finite-dimensional over with , commuting with for all is of the form for a unique : choose bases of and of (both finite, with ), write with well-defined linear maps ; for each let be given on the basis by and for ; then , so on all basis vectors, and conversely every commutes with the operators .
The first displayed identity of claim 1 holds: a map commutes with every exactly when it commutes with for every , because is the linear span of the place operators ; hence the centralizer of is , which equals by [F2]. The same fact of [F2] identifies with the image of the diagonal action of , so claim 2 holds; in particular is a subalgebra, in agreement with step 1.1.
The canonical algebra homomorphism , , is an isomorphism. It is injective: if acts as on every , then under the product decomposition of step 1.3 the element has a component in each factor which annihilates that factor's own column module, and so is , so ; here [F8] identifies the column module of the factor attached to with the simple module , on which acts as by definition of . It is then bijective because, by step 1.3 and , source and target have the same finite dimension .
The algebra is : an -endomorphism of maps each isotypic component into itself, since the image of a copy of is or a copy of by [F5] and [F4]; on it is, by [F6] and step 1.2, exactly the operator induced by a unique on the second tensor factor; maps between distinct components are zero by [F5] and [F4] because and are non-isomorphic for ; and the identifications preserve composition, so this is an algebra isomorphism under which corresponds to the operator on . In particular, by step 2.1, is exactly the set of operators with .
Under the isomorphism of step 2.2 and the isomorphisms of step 1.2, the action of on is , the factors with acting on no summand; hence the image of this action map is exactly the direct sum of the indicated block subalgebras indexed by : indeed the projection is surjective and is an isomorphism.
Claim 1's second identity holds. Let commute with every element of ; decompose as a block matrix with using the decomposition of step 1.2. Commuting with the operator on the -block and on the -block gives . If , use , (available in by step 3.1 and ), obtaining . Thus every off-diagonal block vanishes. For each , the diagonal block commutes with for every , since contains the operators supported on that single block by step 3.1.
By steps 4.1 and 1.4 the centralizer of consists exactly of the elements with , which is exactly by step 3.2; this proves the second identity of claim 1, and claim 2 was proved in step 2.1.
Boundary and choice audit. For one has , and both centralizers equal the whole of , in agreement with claims 1 and 2; the case is covered by the argument with when . For and one has , so by [F2] and all assertions hold; here , the products over are the zero algebra, and steps 4.1 and 1.4 are vacuous. For and , every has by definition, so step 1.4 applies with . All bases and decompositions used are attached to finite-dimensional spaces and to the finitely many partitions of ; the decomposition of and the factors of are canonical, and no choice principle is invoked.
Remarks
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Two halves, two mechanisms. The identity is the polarization lemma (Diagonal tensor operators span the symmetric centralizer), a direct computation with symmetric tensors. The reverse identity goes through the semisimple structure of : the isotypic decomposition of makes both centralizers products of full matrix algebras, and the two products are exchanged by the evaluation isomorphism (Isotypical evaluation and multiplicity subspaces).
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No Lie machinery is imported. The only Lie-theoretic input is the identification of with the image of the diagonal -action, which is proved inside Diagonal tensor operators span the symmetric centralizer by Newton identities; no classification or highest-weight theory is used here.
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What the theorem does not say. Nothing is asserted about the multiplicity spaces beyond their occurrence: their irreducibility, pairwise inequivalence and highest weights are proved via the length cutoff and the local highest-weight computation later on this page.
Depends on
- Diagonal tensor operators span the symmetric centralizer
- Maschke's theorem for finite groups over fields whose characteristic does not divide $|G|$
- Specht modules classify the complex irreducibles of $S_n$
- Commuting symmetric-group and linear actions on a tensor power
- If $k$ is algebraically closed and $\operatorname{char} k \nmid |G|$, then $k[G]\cong\prod_{i=1}^r M_{n_i}(k)$
- Simple modules over a product of matrix rings over division rings
- Schur's lemma for irreducible representations: a nonzero intertwiner is an isomorphism, and $\operatorname{End}_G(V)$ is a division ring
- Over an algebraically closed field, every endomorphism of an irreducible representation is scalar
- The isotypic decomposition of a completely reducible representation is unique
- Isotypical evaluation and multiplicity subspaces
- For a commutative ring $R$, $R$-linear $G$-actions are exactly the compatible left $R[G]$-module structures
- Under the dictionary, subrepresentations are exactly submodules and irreducible representations are exactly simple modules
Used by
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Sources
- Pavel Etingof et al., Introduction to Representation Theory, MIT 18.712 Chapter 4, Theorems 4.54-4.57, PDF pp. 18-20 (standard reference, not scraped)
- Hsueh-Yung Lin, Modern Algebra I, Section 27, printed pp. 71-74 (standard reference, not scraped)