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The Branching Rule and the Young Graph

1 · Prerequisites

2 · Summary

This page develops the branching rule for the symmetric group, its bookkeeping by the Young graph, Young's rule for permutation modules, and the Schur–Weyl decomposition of a tensor power. It uses the tabloid and permutation-module conventions of young-diagrams-tableaux-and-permutation-modules, the complex Specht modules and their classification from specht-modules-and-the-irreducibles-of-the-symmetric-group, the induction adjunction of induced-representations-and-frobenius-reciprocity, and the tensor constructions of tensor-products-of-modules.

The Specht module construction is developed over arbitrary commutative rings; the restriction filtration itself is proved over every field. Integral and field-valued Specht modules defines the tabloid modules, the antisymmetrizers and the Specht modules over a ring, and Integral Garnir straightening and the field-uniform standard basis proves the integral Garnir relation together with the standard-polytabloid basis that survives reduction to every field, including characteristic two. The corner order on removable rows and the associated deletion maps are recorded in Ordered removable corners and tabloid deletion maps; they build the nested Sn−1-stable subspaces of The corner-filtration subspaces of a Specht module are S_(n-1)-invariant, whose successive quotients are computed in Deletion identifies each Specht branching quotient. Assembling these gives the field-uniform filtration of Specht restriction has a removable-corner filtration over every field. Over C Maschke's theorem splits the filtration, and The complex Specht restriction branching rule identifies the restriction as the direct sum over the removable corners, each shape occurring once. Frobenius reciprocity converts that statement into the induction rule of Multiplicity-free complex Specht induction.

The combinatorial shadow of the two rules is the Young graph of The Young graph of partitions, whose vertices are partitions and whose edges add one box. Paths from the empty partition encode standard tableaux, as proved in Young-graph paths correspond to standard tableaux, so the branching multiplicities are path counts.

Young's rule computes the multiplicity of a Specht module in a permutation module as a Kostka number. The linear maps attached to semistandard tableaux are constructed in Semistandard fillings construct Specht-to-permutation homomorphisms; their triangular independence is Semistandard maps are independent and respect dominance and the spanning argument that avoids a separate RSK input is Semistandard maps span the Hom space in characteristic zero. Together they identify the dimension of the homomorphism space with the number of semistandard tableaux, and Young's rule for complex permutation modules states the resulting decomposition.

The final part concerns the tensor power V⊗n with its commuting actions. Commuting symmetric-group and linear actions on a tensor power fixes the left place action of Sn, the diagonal action of GL⁡(V) and the place-sum operators; Diagonal tensor operators span the symmetric centralizer shows that the unital algebra generated by those operators is the centralizer of the symmetric-group action. The double-centralizer theorem The Schur-Weyl mutual centralizer theorem on tensor powers identifies the two commutants, and Column antisymmetrization gives the exact Schur–Weyl length cutoff determines exactly which shapes occur for finite-dimensional V. The row-labelled polytabloid map has highest weight lambda computes the highest weight and its uniqueness, and Schur-Weyl decomposition and highest weights assembles the decomposition V⊗n≅⨁ℓ(λ)≤dim⁡VSλ⊗Mλ, the irreducibility of the multiplicity factors, and their pairwise inequivalence for the nonzero factors; the zero factors are exactly those of length exceeding dim⁡V.

Restriction is taken along the subgroup of permutations fixing n, and the left place action is normalized with the inverse permutation on positions so that it commutes with the diagonal action. The modular filtration is stated without any splitting assertion; the companion page shows that the splitting genuinely fails in positive characteristic.

3 · Logical flowchart

4 · Definitions, theorems and proofs

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6.1-sol)audited 2026-10-02Open item page →

Integral and field-valued Specht modules

Definition

Throughout, R is a commutative ring, n≥0, and λ⊢n with Young diagram [λ]. Tabloids, the left action σ⋅{t}:={σ⋅t} of Sn on the finite set Ωλ of λ-tabloids, and the complex tabloid module Mλ=C(Ωλ) are as in Young subgroups, tabloids, and permutation modules: rows are labelled and the order of entries inside a row is forgotten.

The tabloid module over R. Put MRλ:=R(Ωλ), the free left R-module with the tabloids as R-basis, and let Sn act on MRλ by R-linear extension of σ⋅{t}:={σ⋅t} on basis elements. The row-set computation of Young subgroups, tabloids, and permutation modules shows that this rule is well defined on tabloids, and because the action on tableaux is a left action, id⋅{t}={t} and σ⋅(τ⋅{t})=(στ)⋅{t}; hence MRλ is a left module over Sn and over the group ring R[Sn].

Antisymmetrizers, polytabloids, and Specht modules. Let t be a λ-tableau with column stabilizer Ct (Row and column stabilizers), and let sgn⁡:Sn→{+1,−1} be the sign homomorphism (The sign is a homomorphism Sn→{+1,−1}, surjective exactly when n≥2); its values are read in R through the unique unital ring homomorphism Z→R. Define κt:=∑γ∈Ctsgn⁡(γ) γ ∈R[Sn],et:=κt⋅{t}=∑γ∈Ctsgn⁡(γ) {γ⋅t} ∈MRλ, and let SRλ:=span⁡R{ et: t is a λ-tableau } ⊆MRλ. All sums here are finite sums over the finite group Ct, so κt, et and SRλ are well defined for every commutative ring R. For the empty partition the empty tableau is the unique one and has Ct={1}, so κt=1, et={∅} and SR∅=R. For every tableau t one has Ct∩Rt={1}: a permutation preserving every row set and every column set must fix the entry in each row-column intersection, since each intersection contains a single box. Hence the tabloids γ⋅{t}, γ∈Ct, are distinct and the coefficient of {t} in et is 1. Thus et≠0 whenever R is nonzero; if R is the zero ring, then MRλ=SRλ=0 and et=0.

Covariance of the construction over R. For every λ-tableau t and every σ∈Sn, κσ⋅t=σκtσ−1andeσ⋅t=σ⋅et, and for every γ∈Ct one has γ⋅et=sgn⁡(γ)et. Consequently SRλ is an R[Sn]-submodule of MRλ, and for any single λ-tableau t the orbit of et spans SRλ. These identities are the ones published for R=C in Polytabloid covariance and the column sign rule; because the argument there consists only of reindexing the finite sums over Ct and over Cσ⋅t, it is valid verbatim over an arbitrary commutative ring. The two reindexings are written out in the remarks below.

Agreement with the complex Specht module. For R=C the module MCλ, the element κt, the polytabloid et and the space SCλ coincide with Mλ, κt, et and Sλ of Column antisymmetrizers, polytabloids, and Specht modules: the tabloid set and the left action are the same, the permutation sign used there is the sign of The sign is a homomorphism Sn→{+1,−1}, surjective exactly when n≥2 transported along the order-preserving relabelling described in that item, and the defining formulas are identical. In particular every published statement about κt,et,Sλ applies to SCλ.

Remarks

  • The two reindexings. First, Cσ⋅t=σCtσ−1: a permutation γ preserves each column set σ(Bj) of σ⋅t exactly when σ−1γσ preserves each column set Bj of t. Reindexing the finite sum defining κσ⋅t by γ=σcσ−1 and using sgn⁡(σcσ−1)=sgn⁡(c), which follows from multiplicativity of the sign and sgn⁡(σ−1)=sgn⁡(σ)−1=sgn⁡(σ) in {+1,−1}, gives κσ⋅t=σκtσ−1. Applying both sides to {σ⋅t} and using σ−1⋅{σ⋅t}={t} gives eσ⋅t=σ⋅et. Second, reindexing the sum defining κt by c↦γc for γ∈Ct and using multiplicativity of the sign gives γκt=sgn⁡(γ)κt, hence γ⋅et=sgn⁡(γ)et.

  • Reasons for stating the construction over a commutative ring. The restriction of a Specht module to Sn−1 has a removable-corner filtration over every field, and in positive characteristic that filtration need not split; the filtration and its modular failure are stated below on this page in terms of SFλ for a general field F. The case R=Z records the integral lattice spanned by the polytabloids.

  • No choice is used. The sums are over the finite group Ct, and the scalar extension Z→R is unique, so no selection principle enters the definition.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passjudge pass (gpt-6.1-sol)audited 2026-10-02Open item page →

Integral Garnir straightening and the field-uniform standard basis

Statement

Let n≥0 and let λ⊢n. Write MRλ for the free R-module on the λ-tabloids and SRλ for the R-span of the polytabloids over a commutative ring R (Integral and field-valued Specht modules). Then:

  1. (Integral Garnir relation.) Let t be a λ-tableau, let j,j+1 be adjacent columns, let X be a set of entries of column j and Y a set of entries of column j+1, with ∣X∣+∣Y∣>λj′. Let GX,Y:=∑g∈Tsgn⁡(g)g, where T is any set of representatives containing 1 for the left cosets of H:=SX×SY in SX∪Y (the transpositions in SX and SY act on the corresponding labels and fix all other labels). Then GX,Y et=0in MZλ; the same identity holds after base change in MFλ for every field F, for the same transversal T.
  2. (Straightening over Z.) For every λ-tableau t, the polytabloid et is a finite Z-linear combination of standard λ-polytabloids.
  3. (Integral and field-uniform basis.) The standard polytabloids {et:t standard} are a Z-basis of SZλ; for every field F, their images under coefficient reduction are an F-basis of SFλ. In particular dim⁡FSFλ=fλ for every field F, including F of characteristic 2.

Facts & Assumptions

Given: n≥0, λ⊢n, a λ-tableau t, adjacent columns j,j+1, subsets X,Y of their entry sets with ∣X∣+∣Y∣>λj′, and a left-coset transversal T for SX∪Y/H containing 1, where H=SX×SY.

[F1]

MRλ is free with the λ-tabloids as R-basis, and es=κs⋅{s}=∑γ∈Cssgn⁡(γ){γ⋅s} for every tableau s; for γ∈Cs, γ⋅es=sgn⁡(γ)es; moreover eσ⋅s=σ⋅es for every σ∈Sn, and SRλ is the R-span of all es (Integral and field-valued Specht modules).

[F3]

Cs and Rs are the subgroups of Sn preserving each column set and each row set of s; they act by permuting labels within columns and within rows respectively (Row and column stabilizers).

[F4]

Column j of [λ] has λj′ nodes and λj+1′≤λj′ (Partitions, English diagrams, and conjugation).

[F5]

A λ-tableau is a bijection [λ]→{1,…,n}; it is standard when entries strictly increase along rows and down columns, and it is column-standard when entries strictly increase down columns (Tableaux and standard tableaux, Tabloid and column orders for Specht straightening).

[F6]

The tabloids carry a finite strict total order, and the column-standard tableaux carry a finite strict total order ≺ in which s≺u means that the largest label lying in different columns in s and u is farther left in s (Tabloid and column orders for Specht straightening).

[F7]

If s is column-standard, then the coefficient of {s} in es is 1 and every other tabloid occurring in es is strictly below {s} in the tabloid order of [F6]; moreover distinct standard tableaux have distinct tabloids (Leading tabloid of a column-standard polytabloid).

Proof

technique · constructive straightening
1.1givenF1F2F3constructalgebra

[construct] Put Z:=X∪Y and AH:=∑h∈Hsgn⁡(h)h; then GX∪Y:=∑g∈SZsgn⁡(g)g satisfies GX∪Y=GX,YAH, because SZ is the disjoint union of the left cosets gH, g∈T, and sgn⁡(gh)=sgn⁡(g)sgn⁡(h) by [F2]. Since H permutes labels inside the two columns j and j+1 and fixes all other labels, H⊆Ct by [F3]; hence [F1] gives AHet=∑h∈Hsgn⁡(h)h⋅et=∑h∈Het=∣H∣et, a multiplication in MZλ by the positive integer ∣H∣=∣X∣! ∣Y∣!.

1.2givenF3F4F5algebra

Let h∈Ct and consider the tabloid {h⋅t} of the tableau h⋅t. The labels of X occupy, in the tableau h⋅t, the positions h−1(x) for x∈X; these lie in column j, because h preserves each column set by [F3], and they are pairwise distinct positions of that column, hence lie in pairwise distinct rows. Likewise the labels of Y lie in pairwise distinct rows, all of them rows ≤λj+1′≤λj′ by [F4], while the labels of X lie in rows ≤λj′. All ∣X∣+∣Y∣>λj′ labels of Z therefore lie in the first λj′ rows of the tabloid, and within this set two labels of X never share a row and two labels of Y never share a row; hence some row of {h⋅t} contains a label x∈X and a label y∈Y.

1.3givenF1F3F5constructalgebra

[construct] Let s be any λ-tableau. Sorting the entries of each column of s increasingly gives the unique column-standard λ-tableau scol with the same column sets as s, and the rule π(s(i,j))=scol(i,j) defines a unique π∈Cs with π⋅s=scol. By [F1] and [F5], escol=π⋅es=sgn⁡(π)es, so es=sgn⁡(π)escol: it suffices to straighten column-standard polytabloids over Z.

1.4F6F7algebra

The standard polytabloids are linearly independent over Z and over every field F. Indeed, let ∑scses=0 be a finite linear relation with coefficients in Z or in a field, not all zero, and let s be a standard tableau whose leading tabloid {s} is greatest, in the finite tabloid order of [F6], among the tabloids {s′} attached to the tableaux s′ with cs′≠0. By [F7] the coefficient of {s} in es′ is 0 for every such s′≠s (its leading tabloid is {s′}≠{s}, and all its other tabloids are strictly below {s′}, hence strictly below {s}), while the coefficient of {s} in es is 1; the coefficient of {s} in the relation is therefore cs≠0, a contradiction.

2.1givenF1F2F3step 1.2algebra

For h∈Ct let x∈X, y∈Y be labels in one row of {h⋅t}, as provided by step 1.2. Then (xy)⋅{h⋅t}={h⋅t} because a transposition of two labels in one row preserves the row sets. Choose representatives k for the right cosets k⟨(xy)⟩ in SZ. Since sgn⁡((xy))=−1 by [F2], GX∪Y=∑ksgn⁡(k)k(1−(xy)), so GX∪Y⋅{h⋅t}=0.

2.2givenF4F5step 1.3algebra

Because s is column-standard but not standard, some row contains adjacent entries with s(q,j)>s(q,j+1); fix such a descent, put h0:=λj′, and set xr:=s(r,j) for q≤r≤h0 and ya:=s(a,j+1) for 1≤a≤q. Column-standardness gives xq<xq+1<⋯<xh0 and y1<⋯<yq, while xq>yq; hence every element of X:={xq,…,xh0} is larger than every element of Y:={y1,…,yq}. Since the box (q,j+1) lies in [λ], we have q≤λj+1′, and ∣X∣+∣Y∣=(h0−q+1)+q=λj′+1>λj′.

3.1givenF1step 1.1step 2.1algebra

Summing step 2.1 over h∈Ct with coefficients sgn⁡(h) gives GX∪Yet=∑h∈Ctsgn⁡(h)GX∪Y{h⋅t}=0 by [F1]. By step 1.1 this is GX,YAHet=∣H∣GX,Yet=0 in MZλ. Expanding GX,Yet=∑TaT{T} in the tabloid basis, uniqueness of coefficients in the free module [F1] gives ∣H∣aT=0 in Z for every tabloid T, hence aT=0 since ∣H∣>0; therefore GX,Yet=0 in MZλ, which is claim 1 for integral scalars, and its image under Z→F gives the same identity in MFλ for every field F.

4.1givenF1step 2.2step 3.1constructalgebra

[construct] Fix a column-standard tableau s and the descent data X, Y of step 2.2, with p:=∣X∣ and Z=X∪Y. For each p-element subset A⊆Z write X∖A={a1<⋯<ar} and A∖X={b1<⋯<br} and put gA:=(a1 b1)⋯(ar br), the empty product being the identity; then gA(X)=A, the gA are pairwise distinct, and as A runs over the p-element subsets of Z they form a left-coset transversal for H in SZ with gX=1, because H is exactly the setwise stabiliser of X in SZ and the left cosets gH are distinguished by g(X). Applying step 3.1 to this transversal and using the covariance identity g⋅es=eg⋅s of [F1] yields, by isolating the identity term, es=−∑A≠Xsgn⁡(gA) egA⋅s with integer coefficients.

5.1givenF1F5F6step 2.2step 4.1algebra

For A≠X let xA be the greatest element of X∖A; then gA(xA)∈Y⊆ column j+1 of s, and every element of X∖A other than xA is smaller than xA, while every element of Y is smaller than every element of X by step 2.2. Under the left action gA⋅s, the changed labels are exactly the elements of (X∖A)∪(A∖X)⊆Z, and xA is the greatest of them, moving from column j in s to column j+1 in gA⋅s; all labels greater than xA are fixed by gA and stay in their columns. Sorting the columns of gA⋅s increasingly gives a column-standard tableau uA with the same column sets, so xA stays in column j+1, and by step 1.3 and [F5] we have egA⋅s=±euA; since the largest label in different columns of s and uA is xA, with cs(xA)=j<j+1=cuA(xA), the order of [F6] gives s≺uA.

6.1givenF6step 1.3step 4.1step 5.1algebra

There are finitely many column-standard λ-tableaux, ordered by ≺ in [F6]; list them as s1≺s2≺⋯≺sN. For the greatest element sN, if it were not standard then step 4.1 would produce tableaux uA with sN≺uA by step 5.1, contradicting maximality, so sN is standard. Now let k<N and suppose every esl with l>k is a finite Z-linear combination of standard polytabloids. If sk is standard there is nothing to prove; otherwise steps 4.1 and 5.1 express esk as a finite Z-linear combination of elements euA=±esl with l>k, which are of the required form by the supposition. Finite downward induction on k therefore proves claim 2 for column-standard tableaux, and step 1.3 removes the column-standard hypothesis: every polytabloid over Z is a finite Z-linear combination of standard polytabloids.

7.1givenF1F5step 1.4step 3.1step 6.1discharge-construct∎

By claim 2 every element of SZλ, which is spanned by the polytabloids by [F1], lies in the Z-span of the standard polytabloids, and step 1.4 shows that this family is Z-linearly independent; hence it is a Z-basis of SZλ. Reducing coefficients along Z→F, the images span SFλ because the reduction of every et is an F-linear combination of the images of standard polytabloids, and they are F-linearly independent by step 1.4 read in F; hence they form an F-basis of SFλ, so dim⁡FSFλ=fλ by [F5]. Claim 1 for fields is step 3.1, and the empty shape is included since SR∅=R with its single standard polytabloid. This proves all three claims.

Remarks

  • No division by factorials. The integral argument never divides by ∣H∣=∣X∣! ∣Y∣!: the proof of the Garnir relation first produces the identity ∣H∣GX,Yet=0 and then cancels the integer ∣H∣ inside the free, hence torsion-free, module MZλ. This is why the result survives in characteristic 2 and is not available from the complex-only Garnir relation (Adjacent-column Garnir relation over C) by base change.

  • Unitriangularity. The induction of step 6.1 straightens strictly upward in the column order ≺ of [F6], and each step has coefficients ±1; combined with the leading-tabioid unitriangularity of [F7] this gives the standard basis without the hook-length formula or RSK.

  • Consistency with the complex basis. For F=C the field case of claim 3 recovers the published Standard polytabloids form a basis of a complex Specht module without citing it; the two proofs use the same column order and the same Garnir mechanism, so they agree.

  • No choice. The transversals in claims 1 and 2 are given by explicit finite rules (a supplied transversal in claim 1, the swapping products gA in step 4.1), and the induction of step 6.1 runs over a finite ordered set; no selection principle is used.

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-10-02Open item page →

Ordered removable corners and tabloid deletion maps

Definition

Let R be a commutative ring, let n≥1, and let λ⊢n with Young diagram [λ] (Partitions, English diagrams, and conjugation). Tabloids, the tabloid module MRλ with its tabloid basis, and the left Sn-action σ⋅{t}={σ⋅t} are as in Integral and field-valued Specht modules.

The ordered removable corners. A removable node of λ is a node whose deletion leaves a Young diagram (Removable and addable nodes); by the row criterion there, the removable nodes are exactly the nodes (i,λi) with λi>λi+1, where λk+1:=0 for a partition λ=(λ1,…,λk). For n≥1 there is at least one: the node (k,λk) of the last row satisfies λk>λk+1=0. List the removable rows from top to bottom, r1<r2<⋯<rm,m≥1, so that the removable nodes are the corners xi:=(ri,λri), and for each i let [λ(i)]:=[λ]∖{xi}. This is the diagram of a partition of n−1 by the definition of a removable node. In the parts list, shorten row ri by one; if its length becomes zero, omit that last row. Indeed, λri−1≥λri+1 by the removability criterion, and if λri=1, that criterion forces ri to be the last row. Thus the remaining row lengths are weakly decreasing and [λ(i)]=[λ]∖{xi} (Removable and addable nodes).

The deletion maps. For 1≤i≤m define a map on tabloids by θi({t}):={{ the tabloid obtained from {t} by deleting n },n lies in row ri of {t},0,n does not lie in row ri of {t}, and extend R-linearly; this is the unique R-linear map θi:MRλ→MRλ(i) with the displayed values on the tabloid basis. It is well defined: whether n lies in row ri is a property of the tabloid, and if it does, deleting n from that row set leaves a set partition of {1,…,n−1} whose block sizes are the λj(i), so the result is a tabloid of shape λ(i), which is a basis element of MRλ(i). In tabloid notation, θi({t})={t with n removed} when n is in row ri of the row sets of t, and θi({t})=0 otherwise.

Elementary properties of θi. For every σ∈Sn−1 and every λ-tabloid {t}, the permutation σ fixes n and preserves the row of n, and deleting n commutes with relabelling the other entries, so θi(σ⋅{t})=σ⋅θi({t}); hence θi is Sn−1-linear: the source MRλ is restricted along Sn−1⊆Sn, while the target MRλ(i) has its natural Sn−1-action on the labels 1,…,n−1 (Integral and field-valued Specht modules). Moreover θi is surjective: given any λ(i)-tabloid, insert the label n into its row ri; this produces a λ-tabloid that θi sends back to it. So the image of θi is all of MRλ(i), and its kernel consists exactly of the elements of MRλ whose expansion in the tabloid basis involves only tabloids with n outside row ri.

Remarks

  • Why n≥1. For n=0 there are no removable nodes and no map to define; the restriction problem considered below is only nontrivial for n≥1. For n=1 one has λ=(1), m=1, r1=1, λ(1)=∅, and θ1 is the augmentation-like map sending the unique tabloid to the unique empty tabloid.

  • Order is part of the definition. The list r1<⋯<rm gives the corners from the top row to the bottom row; this fixed order is what the filtration 0=V0⊆V1⊆⋯⊆Vm=SFλ and the quotients Vi/Vi−1≅SFλ(i) below refer to. Nothing here permits replacing this top-to-bottom order by an arbitrary order.

  • Relation to the tabloid order. The maps θi are not the same as the tabloid ordering used in Tabloid and column orders for Specht straightening; they are Sn−1-equivariant deletions and are used only to compare submodules of SFλ with Specht modules of the shapes λ(i).

  • No choice. The list of corners is a finite ordered list determined by λ, and the maps are defined by an explicit rule on a finite basis; no selection principle is used.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-10-02Open item page →

The corner-filtration subspaces of a Specht module are S_(n-1)-invariant

Statement

Let n≥1, let λ⊢n, let F be any field, and let r1<r2<⋯<rm be the rows of the removable corners of λ, as in Ordered removable corners and tabloid deletion maps. For 1≤i≤m let Vi:=span⁡F{ et: t a standard λ-tableau whose entry n lies in one of the rows r1,…,ri } inside SFλ, and put V0:=0. Then each Vi is stable under the action of Sn−1 on SFλ obtained by restriction from Sn, that is σ⋅Vi⊆Vi for every σ∈Sn−1; moreover V0⊆V1⊆⋯⊆Vm=SFλ.

Facts & Assumptions

Given: an integer n≥1, a partition λ⊢n, a field F, the removable rows r1<⋯<rm of λ, and the subspaces Vi of the Statement.

[F1]

MFλ is free with the λ-tabloids as basis, et=κt⋅{t} for a λ-tableau t, and SFλ is the F-span of all et; moreover eσ⋅t=σ⋅et and γ⋅et=sgn⁡(γ)et for γ in the column stabilizer Ct, so SFλ is an Sn-submodule and is generated by any one et (Integral and field-valued Specht modules, Polytabloid covariance and the column sign rule).

[F2]

The standard polytabloids {et:t standard} are an F-basis of SFλ, and every polytabloid is an F-linear (indeed Z-linear) combination of standard polytabloids (Integral Garnir straightening and the field-uniform standard basis, claims 2 and 3).

[F3]

A λ-tableau is column-standard when its entries strictly increase down every column; for a column-standard tableau u, writing cu(a) for the column of the label a, the largest label on which two distinct column-standard tableaux differ has comparable column numbers, and the resulting relation s≺u  ⟺  cs(x)<cu(x) for the largest label x with cs(x)≠cu(x) is a finite strict total order on the column-standard λ-tableaux (Tabloid and column orders for Specht straightening).

[F4]

The removable nodes of λ are exactly the nodes (i,λi) with λi>λi+1 (with λk+1:=0), and deleting a removable node leaves the diagram of a partition of n−1; for a removable node (r,λr) the column λr has boxes in exactly the rows 1,…,r, so (r,λr) is the bottom box of that column and column j of [λ] has height λj′ with λ1′≥λ2′≥⋯ (Removable and addable nodes, Partitions, English diagrams, and conjugation).

[F5]

Cu is the subgroup of permutations preserving each column set of u; sorting the entries of every column of any tableau u increasingly gives a column-standard tableau ucol, and eucol=sgn⁡(π)eu for the permutation π∈Cu with π⋅u=ucol (Row and column stabilizers, [F1]).

[F6]

If t is a standard λ-tableau, then the box of t containing n is removable, and deleting it leaves a standard tableau of size n−1 (The largest standard entry lies in a removable box).

[F8]

(Garnir.) Let t be a λ-tableau, j,j+1 adjacent columns, X a set of entries of column j of t and Y a set of entries of column j+1 of t with ∣X∣+∣Y∣>λj′, and let T be any left-coset transversal containing 1 for SX∪Y/(SX×SY), where the transpositions in SX and SY act on the corresponding labels and fix all other labels. Then ∑g∈Tsgn⁡(g) g⋅et=0 in MFλ (Integral Garnir straightening and the field-uniform standard basis, claim 1).

Proof

technique · constructive
1.1F1F5F7constructalgebra

[construct] We fix notation for the invariance argument. For a tableau u let c(u) be the column containing the label n; since n is the largest label, n is the bottom entry of its column in every column-standard tableau, and if n already lies at the bottom of its column in u then the sorting permutation π∈Cu with π⋅u=ucol fixes the column of n and leaves n in its box, so n occupies the same box in u and in ucol; in this situation we write ρ(u) for the row of the box containing n, and then ρ(ucol)=ρ(u) and eu=sgn⁡(π)−1eucol=±eucol by [F5] and [F7].

1.2constructalgebra

For σ∈Sn−1 and any tableau u the tableau σ⋅u has the same entry n in the same box as u, because σ fixes the label n; so if u has n at the bottom of its column, then so does σ⋅u, with ρ(σ⋅u)=ρ(u) and c(σ⋅u)=c(u).

1.3F1F4F5F6constructalgebra

Thus it suffices to prove the straightening statement (S): if u is a tableau in which n lies at the bottom of its column, then eu is an F-linear combination of standard polytabloids et′ with ρ(t′)≤ρ(u). Indeed, for a standard λ-tableau t with n in row rl and σ∈Sn−1, the tableau u:=σ⋅t has n in the same box as t, and that box is removable and hence the bottom box of its column by [F6] and [F4]; so u satisfies the hypothesis of (S), and eσ⋅t∈Vl follows from (S) together with the fact that a standard t′ with ρ(t′)≤rl has ρ(t′) equal to some removable row rl′ with l′≤l, by [F6] and [F4].

1.4F3F4constructalgebra

(Garnir setup.) Let s be column-standard and not standard. Since the entries strictly increase down each column but some row fails to weakly increase, there are a row q and a column index j with s(q,j)>s(q,j+1). Put hj:=λj′ and let X be the set of labels in the boxes (r,j) for q≤r≤hj and Y the set of labels in the boxes (r,j+1) for 1≤r≤q; these are label sets of the two adjacent columns j,j+1 of s, and ∣X∣+∣Y∣=(hj−q+1)+q=hj+1>λj′. Column-standardness gives s(q,j)<s(q+1,j)<⋯<s(hj,j), so every label in X is ≥s(q,j), and gives s(1,j+1)<⋯<s(q,j+1), so every label in Y is ≤s(q,j+1); since s(q,j)>s(q,j+1), every label of X is strictly larger than every label of Y.

2.1F1F7F8step 1.4constructalgebra

(The transversal.) Put Z:=X∪Y, p:=∣X∣, and for every p-element subset A⊆Z write X∖A={a1<⋯<ar} and A∖X={b1<⋯<br} and put gA:=(a1 b1)⋯(ar br), the empty product for A=X giving gX=1. Then gA(X)=A, the gA are pairwise distinct, and they form a left-coset transversal for H:=SX×SY in SZ containing 1: indeed H is exactly the setwise stabilizer of X in SZ, so the left coset gH is determined by g(X), and gA(X)=A realizes every possible value A. Hence the Garnir relation [F8] applies to s, X, Y and this transversal and gives ∑Asgn⁡(gA) gA⋅es=0 in MFλ, so es=−∑A≠Xsgn⁡(gA) egA⋅s by [F1] and [F7]; here gA acts on es through the action on tabloids, that is gA⋅es=egA⋅s by [F1].

3.1F3F5step 1.4step 2.1algebra

(The move and the order.) Let s and X,Y be as in step 1.4 and let A≠X, and let uA:=(gA⋅s)col be the column-sorted tableau of gA⋅s. Then s≺uA in the order of [F3]. Indeed, gA fixes every label outside Z and moves the labels ai∈X∖A into the boxes previously holding bi∈A∖X⊆Y and conversely, so the labels that change column are exactly the elements of (X∖A)∪(A∖X), those in X∖A moving from column j to column j+1 and those in A∖X moving from column j+1 to column j; the largest of them is xA:=max⁡(X∖A), since every element of X∖A exceeds every element of Y by step 1.4; every label larger than xA therefore stays in its column; column sorting preserves the column of each label, so in uA the label xA lies in column j+1 while in s it lies in column j, and xA is the largest label on which s and uA differ, whence s≺uA.

4.1F4step 1.4step 2.1step 3.1algebra

(The move does not raise ρ.) With s, X, Y and A≠X as in step 3.1 one has ρ(uA)≤ρ(s). Let c:=c(s) be the column containing n in s; since s is column-standard, n is the bottom entry of column c, so ρ(s)=λc′ by [F4]. If c∉{j,j+1}, then the labels moved by gA lie in columns j and j+1, so n is fixed and stays at the bottom of column c, giving ρ(uA)=ρ(s). If c=j, then n∈X because n is the bottom entry of column j with row hj≥q; if n∉A, then n=max⁡(X∖A)=xA is moved to column j+1 and after column sorting lies at the bottom of column j+1, so ρ(uA)=λj+1′≤λj′=ρ(s) by [F4]; while if n∈A, then n is neither among the ai nor among the bi, hence is fixed and stays at the bottom of column j, so ρ(uA)=ρ(s). Finally, if c=j+1, then n∉Y: otherwise n would be smaller than every element of X by step 1.4, contradicting the maximality of n because X≠∅; so n∉X∪Y, n is fixed, and again ρ(uA)=ρ(s).

5.1F1F3step 1.1step 2.1step 3.1step 4.1constructalgebra

(Row-controlled straightening.) Every column-standard s satisfies: es is an F-linear combination of standard polytabloids et′ with ρ(t′)≤ρ(s). List the finitely many column-standard tableaux as s1≺s2≺⋯≺sN using the finite strict total order of [F3] and prove the assertion for sk by downward induction on k. If sk is standard there is nothing to prove. If sk is not standard, then steps 1.4, 2.1 and 3.1 produce, for each A≠X, a column-standard tableau uA≻sk, so uA=sl with l>k, and esk=∑A≠X±euA by steps 2.1 and 1.1; by the induction hypothesis each euA is a combination of standard polytabloids with ρ≤ρ(uA), and ρ(uA)≤ρ(sk) by step 4.1, so esk is such a combination as well. This also shows that sN is standard, since otherwise it would satisfy sN≺uA for some A, contradicting maximality; hence the induction covers k=N.

6.1F5step 1.1step 1.3step 5.1algebra

This proves (S) of step 1.3: if u has n at the bottom of its column, then eu=±eucol with ρ(ucol)=ρ(u) and ucol column-standard by step 1.1, and step 5.1 expands eucol in standard polytabloids with ρ≤ρ(u), the sign being absorbed into the coefficients over F.

7.1F1F4F6step 1.2step 6.1algebra

(Invariance.) Let σ∈Sn−1 and let t be a standard tableau whose entry n lies in row rl. The box of n in t is removable by [F6] and is the bottom box of its column by [F4]; σ fixes the label n, so u:=σ⋅t has n in the same box by step 1.2, and by step 6.1 eu is an F-linear combination of standard polytabloids et′ with ρ(t′)≤rl. Each such t′ is standard, so by [F6] and [F4] the row ρ(t′) of n in t′ is one of the removable rows r1<⋯<rm, and ρ(t′)≤rl then gives ρ(t′)=rl′ with l′≤l; hence et′∈Vl. Since eu=eσ⋅t=σ⋅et by [F1], we get σ⋅et∈Vl⊆Vi whenever l≤i. As the polytabloids et with n in rows r1,…,ri span Vi, this proves σ⋅Vi⊆Vi for every σ∈Sn−1, that is, Vi is Sn−1-stable.

8.1F1F2F4F6step 7.1algebra

(The chain and the top term.) V0=0⊆V1 is the definition, and Vi⊆Vi+1 for 1≤i<m holds because the set of tableaux whose entry n lies in rows r1,…,ri is contained in the corresponding set for i+1. For Vm=SFλ: the inclusion Vm⊆SFλ is clear, and conversely the standard polytabloids span SFλ by [F2]; if t is standard then the box of n is removable by [F6], so its row is one of r1,…,rm by [F4], whence et∈Vm. This proves the chain 0=V0⊆V1⊆⋯⊆Vm=SFλ.

9.1F2step 1.4step 2.1step 7.1step 8.1discharge-construct∎

For n=1 we have λ=(1), m=1, r1=1, the only standard tableau is the single box with entry 1, the group Sn−1=S0 is trivial, and V1=SFλ is stable; the argument above covers this case, as it does every n≥1. The field F is arbitrary: no division and no characteristic hypothesis is used, the straightening being the integral algorithm of [F2]. The only choices are the finite descent (q,j) of step 1.4 and the finitely many transversal elements gA of step 2.1, both given by explicit rules on finite data, so no choice principle is invoked. This proves the Sn−1-stability of every Vi, the chain 0=V0⊆⋯⊆Vm=SFλ, and completes the proof.

Remarks

  • What is proved where. Steps 1.3--6.1 give the straightening argument with a controlled label: n starts at the bottom of its column and never moves down. Step 3.1 shows that each Garnir move advances in the column order, so the finite induction in step 5.1 terminates. Step 4.1 controls the row: a move either fixes n or carries it to the bottom of the adjacent column, whose height λj+1′ is at most the height λj′ it came from.

  • Why the deleted corner stays put. After stripping the labels 1,…,n−1 the surviving entries of each standard term lie in rows r1,…,rl with l≤i, which is exactly the input to the successive quotient computation (Deletion identifies each Specht branching quotient).

  • No splitting is claimed here. The subspaces Vi are only shown to be nested Sn−1-stable subspaces; that the successive quotients are Specht modules, and in characteristic zero that the filtration splits, are separate statements of this page.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-10-02Open item page →

Deletion identifies each Specht branching quotient

Statement

Let n≥1, let λ⊢n, let F be any field, and let r1<r2<⋯<rm be the rows of the removable corners of λ, so that λ(i) and the deletion map θi:MFλ→MFλ(i) are as in Ordered removable corners and tabloid deletion maps. Let 0=V0⊆V1⊆⋯⊆Vm=SFλ be the Sn−1-stable subspaces of SFλ of The corner-filtration subspaces of a Specht module are S_(n-1)-invariant, so that Vi is spanned by the standard polytabloids et whose tableau t carries the entry n in one of the rows r1,…,ri. For a standard λ-tableau t whose entry n lies in row ri, let tˉ denote the tableau of shape λ(i) obtained from t by deleting the box of n (all other entries unchanged), which is again standard. Then for every 1≤i≤m:

  1. (Values on the standard basis.) One has θi(et)=etˉ for every standard λ-tableau t with n in row ri, and θi(et)=0 for every standard λ-tableau t whose entry n lies in a row rl with l<i.
  2. (Image and kernel.) θi restricts to a surjection θi∣Vi:Vi→SFλ(i) with kernel Vi−1.
  3. (The quotient.) θi∣Vi induces an isomorphism of Sn−1-modules Vi/Vi−1≅SFλ(i), where SFλ(i) carries its natural Sn−1-action on the labels 1,…,n−1.

Facts & Assumptions

Given: an integer n≥1, a partition λ⊢n, a field F, the removable rows r1<⋯<rm of λ, the partitions λ(i) and maps θi, the subspaces Vi of the Statement, and the standard polytabloids of the various shapes.

[F1]

MFλ is free with the λ-tabloids as basis, the left action satisfies σ⋅{t}={σ⋅t}, et=κt⋅{t}=∑γ∈Ctsgn⁡(γ) {γ⋅t}, SFλ is the F-span of all polytabloids, Ct∩Rt={1}, et≠0, γ⋅et=sgn⁡(γ)et for γ∈Ct, and eσ⋅t=σ⋅et, so that SFλ is an Sn-submodule generated by any one et; the sign is read in F through ±1 (Integral and field-valued Specht modules, Polytabloid covariance and the column sign rule).

[F2]

For every field F the standard polytabloids {et:t standard} are an F-basis of SFλ; consequently they are linearly independent and dim⁡FSFλ=fλ, the number of standard λ-tableaux (Integral Garnir straightening and the field-uniform standard basis, claim 3).

[F3]

θi:MFλ→MFλ(i) is F-linear and Sn−1-linear; on a tabloid {u} it equals the tabloid obtained by deleting the label n when n lies in row ri of {u}, and equals 0 otherwise; in particular θi(γ⋅{u})=γ⋅θi({u}) for γ∈Sn−1 (Ordered removable corners and tabloid deletion maps).

[F4]

Vi=span⁡F{et:t standard, n lies in one of the rows r1,…,ri}, V0=0, V0⊆V1⊆⋯⊆Vm=SFλ, and each Vi is stable under the action of Sn−1 (The corner-filtration subspaces of a Specht module are S_(n-1)-invariant).

[F5]

The box occupied by n in a standard λ-tableau is removable, and deleting it leaves a standard tableau of size n−1 (The largest standard entry lies in a removable box).

[F6]

The removable nodes of λ are exactly the nodes (j,λj) with λj>λj+1 (where λk+1:=0), the removable rows are r1<⋯<rm, and λ(i) is λ with the corner xi=(ri,λri) deleted; a node (j,ℓ) belongs to the diagram of λ if and only if ℓ≤λj, equivalently j≤λℓ′, and column ℓ has height λℓ′; also ℓ(λ)=λ1′≥λ2′≥⋯ (Removable and addable nodes, Ordered removable corners and tabloid deletion maps, Partitions, English diagrams, and conjugation).

[F7]

A λ-tableau is a bijection from the boxes of the diagram of λ to {1,…,n}, standard when its entries strictly increase along rows and down columns, and the left action is (σ⋅t)(i,j)=σ(t(i,j)); the row stabilizer Rt and column stabilizer Ct=∏jS(Bj) are built from the row sets Ai and the column sets Bj={t(i,j):1≤i≤λj′} (Tableaux and standard tableaux, Row and column stabilizers).

[F8]

sgn⁡ is a homomorphism, and for a permutation of {1,…,n−1} extended to {1,…,n} by fixing n, the inversion pairs are the same in both groups, so its sign is unchanged (The sign is a homomorphism Sn→{+1,−1}, surjective exactly when n≥2, Inversions, inversion number, the sign sgn⁡(σ)=(−1)inv⁡(σ), and even and odd permutations).

[F9]

A linear map T:U→W induces a linear isomorphism U/ker⁡T→im⁡T (First isomorphism theorem for vector spaces: V/ker⁡T is isomorphic to im⁡T).

Proof

technique · constructive
1.1givenF1F3F4construct

[construct] For a λ-tableau u let ρ(u) be the row of the entry n in u, so that by [F3] θi({u})≠0 if and only if ρ(u)=ri, in which case θi({u}) is {u} with n deleted. Put Wi:=span⁡F{et:t standard, ρ(t)=ri}⊆Vi, so that Vi=Vi−1+Wi by [F4]; and for a standard t with ρ(t)=ri let tˉ be the tableau of shape λ(i) obtained from t by deleting the box of n.

1.2F5F6F7givenalgebra

Let t be standard with ρ(t)=rl, and let c be the column of n in t. Since n is the largest entry of t, it is the last entry of its row and the bottom entry of its column, so n occupies the box (rl,λrl) and c=λrl; by [F5] and [F6] this box is removable, so λrl>λrl+1, and column c has boxes in exactly the rows 1,…,rl. Indeed λc′ counts the rows j with λj≥c=λrl, and by weak decrease and λrl>λrl+1 these are exactly j≤rl. In particular λc′=rl and the column set Bc={t(1,c),…,t(rl,c)} has n as its largest element.

2.1F2F4F5F6step 1.1algebra

For every standard λ-tableau t the row ρ(t) is one of the removable rows r1,…,rm: the box of n is removable by [F5], and the removable nodes are the corners (j,λj) by [F6]. Hence Vi=span⁡F{et:t standard, ρ(t)∈{r1,…,ri}}, the polytabloids et with ρ(t)=ri are linearly independent and form an F-basis of Wi, and the sets {t:ρ(t)=rl, l≤i−1} and {t:ρ(t)=ri} are disjoint.

2.2F3F6F7step 1.2algebra

Let t be standard with ρ(t)=rl and column c of n, and let γ∈Ct. Since γ preserves every column set by [F7], γ−1(n)∈Bc; and the row of n in the tabloid γ⋅{t}={γ⋅t} is the row of γ−1(n) in t, so by [F3] θi(γ⋅{t})≠0 if and only if γ−1(n)∈Ari∩Bc, where Ari is the entry set of row ri of t. Now Ari∩Bc is the set of entries in the box (ri,c), which by [F6] is a single label when ri≤λc′ and is empty otherwise. If l=i then ri=rl=λc′ by step 1.2, the box (ri,c) exists and contains n, so Ari∩Bc={n}; if l<i then ri>rl=λc′, the box (ri,c) does not exist, and Ari∩Bc=∅.

2.3F5F6F7step 1.1step 1.2constructalgebra

For each i the assignment t↦tˉ is a bijection from the set of standard λ-tableaux with ρ(t)=ri onto the set of standard λ(i)-tableaux. It is well defined: by step 1.2 such a t carries n in the removable box xi=(ri,λri), and deleting that box leaves a standard tableau of shape λ(i) by [F5] and [F6]. Conversely, given a standard λ(i)-tableau u, insert the label n into the box xi; since xi is the last box of row ri and the bottom box of its column in the diagram of λ (the column height is λλri′=ri, as the argument of step 1.2 shows for the corner), appending the largest label n preserves both monotonicities of [F7], so the result is a standard λ-tableau with ρ(t)=ri, and the two constructions are inverse to each other.

3.1F1F3F7F8step 1.1step 1.2step 2.2algebra

Let t be standard with ρ(t)=ri. By step 2.2 the only γ∈Ct with θi(γ⋅{t})≠0 are those with γ−1(n)=n, that is γ∈Ct∩Sn−1; for such γ one has θi(γ⋅{t})=γ⋅θi({t})=γ⋅{tˉ} by the Sn−1-linearity of θi in [F3]. Hence θi(et)=∑γ∈Ct∩Sn−1sgn⁡(γ) γ⋅{tˉ}. Now Ct∩Sn−1=Ctˉ: by [F7] Ct=∏jS(Bj) for the column sets Bj of t, so its elements fixing n are the products of permutations of the Bj with j≠c and of a permutation of Bc∖{n}, and Bc∖{n} is the column set of tˉ in column c because the deleted box is the bottom box of column c in t (step 1.2), the other column sets being unchanged. By [F8] the sign of such a γ is the same computed in Sn−1, so θi(et)=∑γ∈Ctˉsgn⁡(γ) γ⋅{tˉ}=κtˉ⋅{tˉ}=etˉ in MFλ(i), which is the first assertion of claim 1.

3.2F1F3step 2.2algebra

Let t be standard with ρ(t)=rl and l<i. By step 2.2 every γ∈Ct satisfies θi(γ⋅{t})=0, so all terms of θi(et)=∑γ∈Ctsgn⁡(γ)θi(γ⋅{t}) vanish and θi(et)=0, which is the second assertion of claim 1.

4.1F2step 1.1step 3.1step 3.2step 2.3algebra

By steps 3.1, 3.2 and 2.3, θi annihilates Vi−1 and sends the basis {et:ρ(t)=ri} of Wi onto the set of standard polytabloids eu of shape λ(i), which by [F2] is an F-basis of SFλ(i); hence θi(Wi)=SFλ(i). Since Vi=Vi−1+Wi (step 1.1) and θi(Vi−1)=0 by step 3.2, also θi(Vi)=SFλ(i): the restriction θi∣Vi is surjective.

4.2F2step 2.1step 3.1step 2.3algebra

The map θi∣Wi:Wi→SFλ(i) carries the F-basis {et:ρ(t)=ri} of Wi (step 2.1) onto the F-basis {eu:u standard of shape λ(i)} of SFλ(i) (steps 3.1 and 2.3 and [F2]), so it is an isomorphism of F-vector spaces; in particular Wi∩ker⁡θi=0.

5.1step 1.1step 3.2step 4.1step 4.2algebra

Let v∈Vi with θi(v)=0. By step 1.1 write v=v′+w with v′∈Vi−1 and w∈Wi. Since θi(v′)=0 by step 3.2, linearity gives θi(w)=0, so w=0 by step 4.2 and v=v′∈Vi−1. Conversely Vi−1⊆ker⁡θi∣Vi by step 3.2, so the kernel is exactly Vi−1; with the surjectivity of step 4.1 this proves claim 2.

6.1F3F4F9step 5.1algebra

The restriction θi∣Vi:Vi→SFλ(i) is a linear map with kernel Vi−1 and image SFλ(i) (claim 2), so by [F9] it induces an F-linear isomorphism Vi/Vi−1→SFλ(i). This isomorphism is Sn−1-equivariant: θi is Sn−1-linear by [F3], and Vi, Vi−1 are Sn−1-stable by [F4], so the induced map on the quotient intertwines the quotient action with the natural Sn−1-action on SFλ(i). This proves claim 3.

7.1F2F3F4F6step 2.3step 4.1step 5.1discharge-construct∎

Boundary and choice audit. For n≥1 there is at least one removable row by [F6], so m≥1 and the list r1<⋯<rm is a finite nonempty list; for n=1 one has λ=(1), m=1, r1=1, λ(1)=∅, the unique standard tableau t has n=1 in row r1 and Ct=Ctˉ={1}, and claim 1 reads θ1(et)=etˉ, the standard basis vector etˉ=1 of SF∅=F, so that V1=SF(1)→F is an isomorphism with kernel V0=0, in agreement with claims 2 and 3. The argument is uniform in the field: it uses the standard basis on both sides, available over any F by [F2] with no division and no characteristic hypothesis (in particular it covers F of characteristic 2), together with the finite groups Ct and the explicit deletion and insertion of the largest label, so no choice principle is invoked. This proves claims 1, 2 and 3.

Remarks

  • Where the corner condition is used. Both values in claim 1 come from the single observation of step 2.2: a column permutation can move a label into the box of n only from the same column, and the corner column of a standard tableau has height equal to the row of n, so the box of n is met only by the label n itself when n sits in row ri, and by no label at all from row ri when n sits in an earlier removable row rl with l<i.

  • No splitting is claimed. The lemma identifies the successive quotients Vi/Vi−1 of the restricted module SFλ; it does not assert that the filtration splits, and this is exactly the point that fails in characteristic p≤n for some shapes (see the companion examples page).

  • Field-uniformity. Both bases used are the standard-polytabloid bases of Integral Garnir straightening and the field-uniform standard basis, so the statement holds over every field, including characteristic 2; no RSK correspondence or dimension count over C is used.

TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-10-02Open item page →

Specht restriction has a removable-corner filtration over every field

Statement

Let n≥1, let λ⊢n, let F be any field, and let r1<⋯<rm be the rows of the removable corners of λ, so that m≥1, the corners xi=(ri,λri) are listed from top to bottom, and the partitions λ(i) of n−1 are obtained by deleting xi (Ordered removable corners and tabloid deletion maps, Removable and addable nodes). Let Vi:=span⁡F{et:t a standard λ-tableau whose entry n lies in one of the rows r1,…,ri} for 1≤i≤m and V0:=0, inside the Specht module SFλ (Integral and field-valued Specht modules). Then the restriction Res⁡Sn−1SnSFλ of SFλ to the subgroup Sn−1≤Sn of permutations fixing n (The sign representation of Sn and the restriction Res⁡HG(V) of a representation to a subgroup) has a filtration by Sn−1-submodules 0=V0⊊V1⊊⋯⊊Vm=SFλ whose successive quotients are Vi/Vi−1≅SFλ(i)(1≤i≤m) as Sn−1-modules. Equivalently, the restriction of SFλ has a filtration whose successive quotients are SFλ(1),…,SFλ(m), one for each removable corner of λ, taken from top to bottom. No splitting of this filtration is asserted.

Facts & Assumptions

Given: an integer n≥1, a partition λ⊢n, a field F, the removable rows r1<⋯<rm with corners xi and partitions λ(i), the Specht module SFλ, and its subspaces Vi defined in the Statement.

[F1]

Each Vi is stable under the action of Sn−1 on SFλ by restriction, and V0⊆V1⊆⋯⊆Vm=SFλ (The corner-filtration subspaces of a Specht module are S_(n-1)-invariant).

[F2]

For every 1≤i≤m the deletion map θi restricts to a surjection Vi→SFλ(i) with kernel Vi−1, hence induces an isomorphism of Sn−1-modules Vi/Vi−1≅SFλ(i) (Deletion identifies each Specht branching quotient).

[F3]

For every partition ν of n−1 the Specht module SFν is nonzero: for ν=∅ one has SF∅=F, and for ν≠∅ the polytabloid et of any ν-tableau t has coefficient 1 at the tabloid {t}, whence et≠0 (Integral and field-valued Specht modules).

[F4]

A subspace of a representation stable under the action of a subgroup is a subrepresentation of the restricted representation (Subrepresentations, direct sums of representations, and irreducibility, The sign representation of Sn and the restriction Res⁡HG(V) of a representation to a subgroup).

[F5]

For n≥1 a partition of n has at least one removable corner, so m≥1 and the list r1<⋯<rm is finite and nonempty (Ordered removable corners and tabloid deletion maps, Removable and addable nodes).

Proof

technique · constructive
1.1F1F4construct

[construct] By [F1] the subspaces Vi are stable under the action of Sn−1 and satisfy 0=V0⊆V1⊆⋯⊆Vm=SFλ; by [F4] each Vi is therefore an Sn−1-submodule of Res⁡Sn−1SnSFλ.

1.2F2algebra

By [F2], for every 1≤i≤m the quotient Vi/Vi−1 is isomorphic to SFλ(i) as an Sn−1-module; in particular the successive quotients of the chain are the Specht modules of the deletion shapes, in the order i=1,…,m of the corners from top to bottom.

2.1F2F3step 1.1step 1.2algebra

The inclusions are strict: by [F3] the quotient SFλ(i) is nonzero, so Vi/Vi−1≠0 and Vi−1≠Vi for every i. Hence 0=V0⊊V1⊊⋯⊊Vm=SFλ is a filtration of the Sn−1-module SFλ with successive quotients SFλ(1),…,SFλ(m). This proves the displayed filtration and the identification of its quotients.

3.1F3F5givenstep 2.1discharge-construct∎

Boundary, field and choice audit. For n=1 one has λ=(1), m=1, r1=1, λ(1)=∅ and SF(1)=F et with a single standard tableau t, so the filtration reads 0⊊V1=SF(1) with quotient SF∅=F, in agreement with the statement. More generally the list of corners is finite and nonempty by [F5], and every removable corner of λ occurs exactly once, as the corner xi for the unique i with ri its row. The argument is uniform in F: the two quoted lemmas use the standard-polytabloid bases and the field-uniform deletion maps of [F2], with no division and no characteristic hypothesis, and [F3] gives nonzero quotients over every field, including char⁡F=2. Nothing here asserts that the filtration splits or that the quotients are simple or irreducible, and in positive characteristic the restriction need not be semisimple; only the existence of the filtration with the stated quotients is claimed. The subspaces Vi are explicitly defined spans of finite standard-polytabloid sets determined by λ, and the corner list is determined by λ, so no choice principle is invoked. This proves the theorem.

Remarks

  • Why the order matters. The standard-polytabloid filtration uses the top-to-bottom corner order of Ordered removable corners and tabloid deletion maps; arbitrary reordering can destroy invariance. For λ=(2,1), putting the bottom corner first gives the line spanned by v={12∣3}−{23∣1}. But (12)v={12∣3}−{13∣2} lies outside that line, by independence of the three tabloids. The specified order is the one used in Deletion identifies each Specht branching quotient.

  • What is not claimed. No direct sum decomposition Res⁡Sn−1SnSFλ≅⨁iSFλ(i) is asserted; over C such a splitting does follow from complete reducibility, which is the content of the complex branching rule proved later on this page, but in positive characteristic the filtration genuinely need not split.

  • Provenance caveat. The statement of the filtration is classical (Chan Theorem 4.16, printed pp. 18-19; Wildon Section 6, printed pp. 26-33); the proof above is assembled from the two preceding lemmas, whose arguments are field-uniform and avoid the Robinson-Schensted-Knuth correspondence.

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The complex Specht restriction branching rule

Statement

Let n≥1, let λ⊢n with Young diagram [λ], and let x1,…,xm be the removable corners of [λ], listed from top to bottom, so that λ(i)=λ−xi⊢n−1 is the partition obtained by deleting xi (Ordered removable corners and tabloid deletion maps). Then there is an isomorphism of CSn−1-modules Res⁡Sn−1SnSCλ≅SCλ(1)⊕⋯⊕SCλ(m), the restriction being along the subgroup Sn−1≤Sn of permutations fixing n (The sign representation of Sn and the restriction Res⁡HG(V) of a representation to a subgroup). Equivalently, for every μ⊢n−1 the multiplicity of SCμ as a summand of Res⁡Sn−1SnSCλ equals the number of removable corners x of [λ] with λ−x=μ, so it is 0 or 1; in particular each SCλ(i) occurs exactly once.

Facts & Assumptions

Given: an integer n≥1, a partition λ⊢n, its removable corners x1,…,xm from top to bottom with λ(i)=λ−xi, and the restricted complex Specht module Res⁡Sn−1SnSCλ.

[F1]

There is a filtration by Sn−1-submodules 0=V0⊊V1⊊⋯⊊Vm=SCλ with Vi/Vi−1≅SCλ(i) for every 1≤i≤m; this holds over every field and in particular over C (Specht restriction has a removable-corner filtration over every field, Ordered removable corners and tabloid deletion maps).

[F2]

The complex Specht modules SCμ, μ⊢n−1, form a complete irredundant list of the finite-dimensional irreducible complex Sn−1-representations (Specht modules classify the complex irreducibles of Sn).

[F3]

Maschke's theorem: if G is a finite group, k a field with char⁡k∤∣G∣, and W≤V a subrepresentation of a finite-dimensional representation of G over k, then there is a subrepresentation U≤V with V=W⊕U; consequently every finite-dimensional representation of such a group is completely reducible (Maschke's theorem for finite groups over fields whose characteristic does not divide ∣G∣, If char⁡k∤∣G∣, every finite-dimensional representation of G is completely reducible).

[F4]

The partition λ(i)=λ−xi is obtained by deleting a distinct corner for each i, so λ(i)=λ(j) happens only for i=j; consequently the multiplicities in a direct sum of the SCλ(i) are 0 or 1 (Ordered removable corners and tabloid deletion maps).

[F5]

If V=W⊕U and both are finite-dimensional, the projection V→V/W restricts to an isomorphism U→V/W (First isomorphism theorem for vector spaces: V/ker⁡T is isomorphic to im⁡T).

Proof

technique · constructive
1.1F1F3construct

[construct] By [F1] there is a chain of Sn−1-submodules 0=V0⊊V1⊊⋯⊊Vm=SCλ whose successive quotients are Vi/Vi−1≅SCλ(i). Since char⁡C=0 does not divide ∣Sn−1∣=(n−1)!, [F3] applies to each subrepresentation Vi−1≤Vi: there is an Sn−1-submodule Ui≤Vi with Vi=Vi−1⊕Ui.

2.1F5step 1.1algebra

By [F5] the projection Vi→Vi/Vi−1 restricts to an Sn−1-isomorphism Ui→Vi/Vi−1; composing with the isomorphism of step 1.1 gives an Sn−1-isomorphism Ui≅SCλ(i).

2.2F1step 1.1algebra

Since V0=0 we have V1=U1, and Vi=Vi−1⊕Ui for every i by step 1.1, so SCλ=Vm=U1⊕U2⊕⋯⊕Um; in particular dim⁡CSCλ=∑i=1mdim⁡CUi.

3.1F2F4step 2.1step 2.2algebra

Combining steps 2.1 and 2.2 gives the asserted CSn−1-isomorphism Res⁡Sn−1SnSCλ≅SCλ(1)⊕⋯⊕SCλ(m). By [F2] the irreducible summands of a decomposition into Specht modules are classified up to isomorphism by their shapes, and by [F4] the shapes λ(i) are pairwise distinct, so each SCλ(i) occurs exactly once and, for μ⊢n−1, the multiplicity of SCμ is the number of corners x with λ−x=μ. This proves the Statement.

4.1F1F3F4givenstep 3.1discharge-construct∎

Boundary and choice audit. For n=1 one has λ=(1), m=1, x1 the unique box, λ(1)=∅ and SC∅=C, so the isomorphism reads Res⁡S0S1SC(1)≅SC∅, both sides being the one-dimensional trivial representation of the trivial group; the filtration has length one and no splitting choice is needed beyond U1=V1. If λ is a row or a column there is exactly one removable corner and the restriction is irreducible; in general m is the finite number of removable corners of λ. The complement Ui furnished by [F3] is produced by averaging over the finite group Sn−1 and involves no choice principle, and by step 3.1 the isomorphism type of the resulting direct sum does not depend on those complements. This proves the corollary.

Remarks

  • Over other fields the splitting can fail. The corollary uses characteristic zero through Maschke's theorem for Sn−1; over a field F of positive characteristic the filtration of Specht restriction has a removable-corner filtration over every field need not split, and the restriction of a Specht module can be a nonsplit extension of its removable-corner factors.

  • Two extreme shapes. The one-row diagram (n) has the single removable corner (1,n) and the one-column diagram (1n) has the single removable corner (n,1), so the corollary gives Res⁡SC(n)≅SC(n−1) and Res⁡SC(1n)≅SC(1n−1): each of the two extremes restricts to the corresponding extreme shape with exactly one summand.

TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passjudge pass (gpt-6.1-sol)audited 2026-10-02Open item page →

Multiplicity-free complex Specht induction

Statement

Let n≥0 and λ⊢n, let Sn≤Sn+1 be the subgroup of permutations of {1,…,n+1} fixing n+1 (The symmetric group Sym⁡(X): the bijections of a set X under composition), and let Ind⁡SnSn+1SCλ be the induced CSn+1-module of the complex Specht module SCλ (The induced R-linear G-module Ind⁡HGW as H-covariant functions on G, Column antisymmetrizers, polytabloids, and Specht modules). Then Ind⁡SnSn+1SCλ≅⨁y∈Add⁡(λ)SCλ+y, where Add⁡(λ) is the set of addable nodes of the Young diagram [λ] and λ+y is the unique partition with [λ+y]=[λ]∪{y} (Removable and addable nodes). Each summand occurs exactly once; equivalently, for every ν⊢n+1 the multiplicity of SCν in Ind⁡SnSn+1SCλ is 1 when ν=λ+y for some addable node y of [λ], and 0 otherwise. In particular, for n=0 this reads Ind⁡S0S1SC∅≅SC(1).

Facts & Assumptions

Given: an integer n≥0, a partition λ⊢n, the finite groups H:=Sn≤G:=Sn+1 with H acting as the permutations of {1,…,n} extended by n+1↦n+1, and the complex Specht modules SCμ for μ⊢n and SCν for ν⊢n+1.

[F1]

For a commutative ring R, a finite group G, a subgroup H≤G and an R-linear H-module W, the induced module is Ind⁡HGW={f:G→W:f(gh)=h−1⋅f(g) for all g∈G,h∈H} with (x⋅f)(g)=f(x−1g); it is an R-linear G-module, and when G is finite and W is finite-dimensional over R it is finite-dimensional over R (The induced R-linear G-module Ind⁡HGW as H-covariant functions on G).

[F2]

For a finite group G, a subgroup H≤G, an H-module W and a G-module V there is a natural isomorphism Hom⁡G(Ind⁡HGW,V)≅Hom⁡H(W,Res⁡HGV) (Induction is left adjoint to restriction for finite-group modules over a commutative ring).

[F3]

For m≥1, ν⊢m and the subgroup Sm−1≤Sm of permutations fixing m, there is an isomorphism of CSm−1-modules Res⁡Sm−1SmSCν≅⨁x∈Rem⁡(ν)SCν−x, each summand occurring once (The complex Specht restriction branching rule, Removable and addable nodes).

[F4]

For every m≥0 the modules {SCμ:μ⊢m} form a complete irredundant list, up to isomorphism, of the finite-dimensional irreducible complex Sm-representations (Specht modules classify the complex irreducibles of Sn).

[F5]

A nonzero intertwiner between irreducible representations is an isomorphism, and over the algebraically closed field C every endomorphism of an irreducible representation is a scalar; hence for partitions ρ,τ⊢m the space Hom⁡Sm(SCρ,SCτ) is C id when ρ=τ and is 0 otherwise (Schur's lemma for irreducible representations: a nonzero intertwiner is an isomorphism, and End⁡G(V) is a division ring, Over an algebraically closed field, every endomorphism of an irreducible representation is scalar).

[F6]

Every finite-dimensional complex representation of a finite group is completely reducible, so it is a direct sum of finitely many irreducible subrepresentations; this is Maschke's theorem in characteristic 0 (Maschke's theorem for finite groups over fields whose characteristic does not divide ∣G∣, If char⁡k∤∣G∣, every finite-dimensional representation of G is completely reducible, A completely reducible representation as a finite direct sum of irreducible subrepresentations).

[F7]

For a completely reducible representation, the isotypic component V(S) is the sum of all irreducible subrepresentations equivalent to S, only the equivalence class of S matters, and V is the direct sum of its isotypic components, a decomposition that is independent of the chosen decomposition of V into irreducibles (The isotypic component of a completely reducible representation, The isotypic decomposition of a completely reducible representation is unique).

[F8]

A node x∈[ν] is removable when [ν]∖{x}=[ν−x] for a partition ν−x of m−1, which is then unique, and a point y∉[λ] is addable for λ when [λ]∪{y}=[λ+y] for a partition λ+y of n+1, which is then unique (Removable and addable nodes).

[F9]

For μ⊢k the complex Specht module SCμ is the span of the polytabloids inside the tabloid module MCμ, which has finitely many tabloids of shape μ as a basis; hence SCμ is a finite-dimensional complex Sk-module (Column antisymmetrizers, polytabloids, and Specht modules, Young subgroups, tabloids, and permutation modules).

No form of the Axiom of Choice is used: G is finite, all direct sums are finite, and the corresponding statements of [F3] and [F4] are themselves choice-free.

Proof

technique · constructive
1.1givenF1F9

Put m:=n+1≥1, G:=Sn+1, H:=Sn and W:=SCλ; by [F1] the induced module Ind⁡HGW is a finite-dimensional complex G-module, and by [F9] for every ν⊢m the modules SCν and, for every x, SCν−x are finite-dimensional complex representations of G and of H respectively.

1.2F4F8

The right-hand module ⨁y∈Add⁡(λ)SCλ+y is a finite direct sum of irreducible G-modules with multiplicity exactly 1 at those ν of the form ν=λ+y and multiplicity 0 at all other ν: the addable nodes y of [λ] give pairwise distinct partitions λ+y and hence pairwise non-isomorphic summands by [F4] and [F8].

2.1F2step 1.1

For every ν⊢m, the adjunction [F2] with R=C gives a C-linear isomorphism Hom⁡G(Ind⁡HGW,SCν)≅Hom⁡H(W,Res⁡HGSCν).

2.2F3step 1.1

For every ν⊢m the restriction rule [F3] applies with its parameter equal to m≥1, so Res⁡HGSCν≅⨁x∈Rem⁡(ν)SCν−x; composing with this isomorphism and splitting a homomorphism into a direct sum into its finitely many components gives Hom⁡H(W,Res⁡HGSCν)≅⨁x∈Rem⁡(ν)Hom⁡Sn(SCλ,SCν−x).

2.3F4F5step 1.1

For each x∈Rem⁡(ν) the summand Hom⁡Sn(SCλ,SCν−x) is one-dimensional when ν−x=λ and is zero otherwise: both arguments are irreducible complex Sn-modules and the partitions λ and ν−x of n are either equal or distinct, so [F5] applies.

2.4F4F5F6step 1.1

By [F6] the module Ind⁡HGW is completely reducible, so it is isomorphic to a finite direct sum ⨁ν⊢m(SCν)⊕mν for nonnegative integers mν; [F4] makes the indexing complete and irredundant, and [F5] together with additivity of Hom⁡ in each argument gives mν=dim⁡CHom⁡G(SCν,Ind⁡HGW)=dim⁡CHom⁡G(Ind⁡HGW,SCν).

3.1step 2.1step 2.2step 2.3algebra

Steps 2.1, 2.2 and 2.3 combine to dim⁡CHom⁡G(Ind⁡HGW,SCν)=#{x∈Rem⁡(ν):ν−x=λ}.

4.1F8step 3.1constructalgebra

The set {x∈Rem⁡(ν):ν−x=λ} is in bijection with {y∈Add⁡(λ):λ+y=ν} by the identity map on nodes: if x is removable with [ν]∖{x}=[λ], then y:=x is a point outside [λ] with [λ]∪{y}=[ν] a Young diagram, so y is addable for λ and λ+y=ν; conversely if y is addable with [λ]∪{y}=[ν], then x:=y lies in [ν] with [ν]∖{x}=[λ] a Young diagram, so x is removable for ν and ν−x=λ. Hence by step 3.1 the dimension dim⁡CHom⁡G(Ind⁡HGW,SCν) equals 1 if ν=λ+y for some addable node y of [λ], and equals 0 otherwise.

5.1F6F7step 4.1step 2.4step 1.2

By step 2.4 and step 4.1 the multiplicities of Ind⁡HGW are 1 exactly at the partitions ν=λ+y with y addable for λ and 0 at all other ν⊢m; by step 1.2 the module ⨁ySCλ+y has the same multiplicities, and both modules are completely reducible by [F6]. Grouping each module into its isotypic components, which by [F7] are determined by the multiplicities alone, gives the asserted isomorphism Ind⁡SnSn+1SCλ≅⨁y∈Add⁡(λ)SCλ+y with each summand occurring once.

6.1F8step 5.1givenalgebradischarge-construct∎

Boundary and consistency check. For n=0 one has λ=∅, H=S0={1} and m=1; the single partition ν=(1) has the single removable node x=(1,1) with ν−x=∅=λ, while Add⁡(∅)={(1,1)} by [F8], so step 5.1 gives Ind⁡S0S1SC∅≅SC(1); every partition λ⊢n with n≥1 has at least the addable node opening a new row, so the displayed direct sum is never empty in that case, and the theorem uses the finite groups Sn, Sn+1 and finitely many partitions throughout, invoking no choice principle. This proves the Statement.

Remarks

  • Consistency of dimensions. For λ=(2,1)⊢3 the theorem reads Ind⁡S3S4SC(2,1)≅SC(3,1)⊕SC(2,2)⊕SC(2,1,1), and the standard tableaux counts f(3,1)=3, f(2,2)=2, f(2,1,1)=3 give 3+2+3=8=4⋅2=[S4:S3] f(2,1), as they must. Similarly Ind⁡S3S4SC(3)≅SC(4)⊕SC(3,1) with 1+3=4=4⋅1.

  • Where semisimplicity enters. Both the complete reducibility of the induced module (step 2.4) and the splitting of the restriction filtration used in [F3] require Maschke's theorem over C; the multiplicity-free statement above is therefore a characteristic-zero result. The corresponding statement over fields of positive characteristic is a different theorem, and the two directions of the rule are mirror images of one another along the add/remove-one-node correspondence of step 4.1.

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-10-02Open item page →

The Young graph of partitions

Definition

Diagrams are English Young diagrams and addable nodes are those of Removable and addable nodes; [λ] denotes the diagram of a partition λ (Partitions, English diagrams, and conjugation).

The Young graph is the directed graph whose

  • vertices are all partitions λ, including λ=∅ and including partitions of every size n≥0; and
  • directed edges are the pairs (λ,ν) for which ν is a partition and there is an addable node y of λ with [ν]=[λ]∪{y}, the edge pointing from λ to ν.

An edge λ→ν therefore always joins a partition of some n to a partition of n+1: inserting a node raises the size by one. The rank, or size, of a vertex λ is ∣λ∣. We say that λ→ν adds the unique node [ν]∖[λ]. A path in the Young graph is a finite sequence λ(0)→λ(1)→⋯→λ(k) of edges; its endpoints are λ(0) and λ(k), and its length is k. Paths of length 0 are the single vertices.

The edge relation is well defined as a set of ordered pairs: by Removable and addable nodes, for an addable node y the partition ν with [ν]=[λ]∪{y} is unique, and conversely the node [ν]∖[λ] determines ν from λ; hence distinct addable nodes of λ give distinct edges out of λ, and there are no multiple edges. The empty partition has Add⁡(∅)={(1,1)}, so its unique edge points to (1), while Rem⁡(∅)=∅, so no edge points into ∅.

Remarks

  • Layering and acyclicity. Since every edge raises the size by one, every directed path from λ to μ has length exactly ∣μ∣−∣λ∣; in particular λ→ν and ν→λ can never both occur, no directed cycle exists, and the vertices of a fixed size form an independent layer. Paths of length k from λ end at partitions of size ∣λ∣+k.

  • Locally finite, globally infinite. A partition λ has at most ℓ(λ)+1 addable nodes, because an addable node lies at a row end (i,λi+1) with i=1 or λi−1>λi, or is the node (k+1,1) opening one new row; a finitely supported region of the plane can be added to a fixed diagram in only finitely many ways, so λ has finitely many outgoing edges. Likewise, each ν has finitely many incoming edges, since a partition of n+1 has finitely many removable nodes. The vertex set is countably infinite, with a finite layer for each n: every partition of n≥1 is a list of at most n entries in {1,…,n}, and rank 0 consists only of ∅. There is at least one vertex at every rank.

  • Row endpoints that are not addable give no edge. In λ=(2,2) the row end (2,3), a third box in the second row, is not addable: addability of (i,λi+1) requires i=1 or λi−1>λi, and here λ1=λ2=2. No partition of 5 contains (2,2) and (2,3) without containing (1,3), so the attempt to add (2,3) produces no vertex and no edge. The actual edges out of (2,2) are the edge to (3,2), adding the addable node (1,3), and the edge to (2,2,1), adding the addable node (3,1) that opens the third row. For partitions λ and ν with ∣ν∣=∣λ∣+1, containment [λ]⊆[ν] is equivalent to an edge λ→ν: their unique difference node is addable because the enlarged diagram is already a Young diagram.

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Young-graph paths correspond to standard tableaux

Statement

For every λ⊢n with n≥0, the paths in the Young graph from the empty partition ∅ to λ (The Young graph of partitions) are in bijection with the standard λ-tableaux (Tableaux and standard tableaux). In particular the number of such paths is fλ, the number of standard λ-tableaux.

Facts & Assumptions

Given: a partition λ⊢n with n≥0.

[F1]

An edge α→β of the Young graph adds a unique node, so [β]=[α]∪{y} for an addable node y of α, and ∣β∣=∣α∣+1; paths are finite sequences of edges, and the unique path of length 0 from λ to λ is the single vertex (The Young graph of partitions).

[F2]

A λ-tableau is a bijection t:[λ]→{1,…,n}; it is standard when its entries strictly increase along rows and down columns, and fλ denotes the number of standard λ-tableaux; the empty tableau is the unique standard tableau of shape ∅ (Tableaux and standard tableaux).

[F3]

[λ]={(i,j):1≤i≤k, 1≤j≤λi} where k is the number of parts, so [λ] is closed to the left and upwards: (i,j)∈[λ] with j≥2 implies (i,j−1)∈[λ], and (i,j)∈[λ] with i≥2 implies (i−1,j)∈[λ] (Partitions, English diagrams, and conjugation).

[F4]

A node (i,λi) is removable exactly when λi>λi+1; deleting it leaves the Young diagram of a partition of n−1 (Removable and addable nodes).

[F5]

For n≥1 the box occupied by n in a standard λ-tableau is removable, and deleting it leaves a standard tableau of size n−1 (The largest standard entry lies in a removable box).

Proof

technique · constructive
1.1F1F2constructalgebra

[construct] Let ∅=λ(0)→λ(1)→⋯→λ(n)=λ be a path from ∅ to λ; by [F1] each step k adds one node yk to [λ(k−1)] to produce [λ(k)], and ∣λ(k)∣=k. Define t:[λ]→{1,…,n} by t(x):=k where x is the node added at step k. The nodes y1,…,yn are pairwise distinct and their union is [λ], because each yk is the unique element of [λ(k)]∖[λ(k−1)] and [λ]=⋃k[λ(k)]; hence t is a well-defined bijection, that is, a λ-tableau.

1.2F1F4F5constructalgebra

[construct] Conversely, let t be a standard λ-tableau. If n=0 take the path of length 0 at ∅; otherwise set λ(n):=λ and tn:=t, and for k=n,n−1,…,1 let tk−1 be the standard tableau of size k−1 obtained from tk by deleting the box containing k, which by [F5] is removable and leaves a standard tableau; let λ(k−1) be its shape, a partition of k−1 by [F4]. Then [λ(k−1)]⊆[λ(k)] with exactly one node removed, that node being removable in λ(k) and addable in λ(k−1), so λ(k−1)→λ(k) is an edge of the Young graph and we obtain a path from ∅ to λ.

2.1F2F3step 1.1algebra

The tableau t of step 1.1 is standard. Let (i,j),(i,j+1)∈[λ]. Both lie in [λ(m)] for m:=t(i,j+1), because t(i,j+1)=m means (i,j+1)∈[λ(m)], and then (i,j)∈[λ(m)] by left-closure of the Young diagram [λ(m)], [F3]. Since [λ(m)]=⋃l≤m[λ(l)] and the yl are distinct, (i,j) was added at a step t(i,j)≤m=t(i,j+1); the two boxes are distinct, so t(i,j)≠t(i,j+1) and therefore t(i,j)<t(i,j+1). The same argument with up-closure in place of left-closure gives t(i,j)<t(i+1,j) whenever both boxes lie in [λ]. Hence t is standard.

2.2F2step 1.2algebra

The path of step 1.2 has the property that λ(k) is the diagram of the boxes of t carrying labels ≤k. Indeed λ(n)=[λ] is all boxes, and at each step the box deleted from λ(k) is the box of the largest label k, which is present in λ(k) because deleting the boxes of the largest labels n,n−1,…,k+1 leaves all boxes with labels ≤k; hence by downward induction on k the diagram [λ(k)] is exactly the set of boxes with labels in {1,…,k} and has size k.

3.1step 1.1step 1.2step 2.2algebra

The two constructions are mutually inverse. Starting from a path and forming t by step 1.1, step 2.2 shows that the path recovered from t by the deletion procedure of step 1.2 has λ(k) equal to the set of boxes with labels ≤k, which is exactly the diagram of the k-th vertex of the original path by definition of t; so the recovered path is the original one. Starting from a standard t and forming the path by step 1.2, the tableau produced from that path by step 1.1 assigns to each box the index k at which it was deleted in the construction of step 1.2, which is its label; so the recovered tableau is t. Hence the two assignments are inverse bijections between the set of paths from ∅ to λ and the set of standard λ-tableaux.

4.1F1F2step 3.1discharge-construct∎

Applying the bijection of step 3.1, the number of paths from ∅ to λ equals the number of standard λ-tableaux, which is fλ by [F2]. For λ=∅ both sets consist of one element: the unique path of length 0 by [F1] and the empty tableau by [F2]. This proves the corollary.

Remarks

  • Consequence for branching counts. The corollary turns the multiplicity bookkeeping of restriction and induction over C into a count of standard tableaux: the number of chains of removable nodes from λ down to the empty partition is fλ, matching the dimension of the complex Specht module Sλ (Standard polytabloids form a basis of a complex Specht module).

  • The first few sizes. The paths from ∅ through size 0,1,2,3,4 give f(1)=1, f(2)=f(1,1)=1, and f(3)=1, f(2,1)=2, f(1,1,1)=1; also f(4)=1, f(3,1)=3, f(2,2)=2, f(2,1,1)=3, f(14)=1. The example on the companion page enumerates these paths.

  • No choice. Both constructions are given by explicit finite recursions on the finitely many boxes of [λ]; no selection principle is used.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passjudge pass (gpt-6.1-sol)audited 2026-10-02Open item page →

Semistandard fillings construct Specht-to-permutation homomorphisms

Statement

Let λ,μ⊢n, and fix a λ-tableau t. Let Tλ,μ be the set of fillings of the boxes of [λ] by positive integers with content μ (Semistandard tableaux and Kostka numbers). Identifying μ-tabloids with the elements of Tλ,μ by recording, at the box that t labels x, the row of x in the tabloid, one obtains an Sn-module isomorphism C(Ωμ)≅CTλ,μ for the transported left action (σ⋅f)(x)=f(x′),t(x′)=σ−1(t(x)). For u∈Tλ,μ let Rt⋅u⊆Tλ,μ be its orbit under this restricted action and put θu({t}):=∑v∈Rt⋅uv ∈ CTλ,μ, extended to a map θu:Mλ→Mμ by θu(σ⋅{t}):=σ⋅θu({t}). Then θu is a well-defined Sn-module homomorphism, and for every semistandard λ-tableau T of content μ the restriction θT∣Sλ:Sλ→Mμ is a homomorphism of Sn-modules. No assertion is made here that this restriction is nonzero.

Facts & Assumptions

Given: partitions λ,μ⊢n, a fixed λ-tableau t, and a filling u of [λ] with content μ.

[F1]

A μ-tabloid is a row-equivalence class {s} of μ-tableaux; the tabloids form a basis of Mμ, and Sn acts on Mμ by σ⋅{s}={σ⋅s}, where (σ⋅s)(i,j)=σ(s(i,j)) (Young subgroups, tabloids, and permutation modules).

[F2]

The stabilizer in Sn of the tabloid {t} is the row stabilizer Rt (Young subgroups, tabloids, and permutation modules).

[F3]

Every λ-tabloid is σ⋅{t} for some σ∈Sn, because the action on tabloids is transitive (Young subgroups, tabloids, and permutation modules).

[F4]

Rt={ρ∈Sn:ρ(Ai)=Ai for every row i} where Ai={t(i,j)}, and Rt is the direct product of the symmetric groups on the pairwise disjoint sets A1,…,Ak (Row and column stabilizers).

[F5]

A λ-tableau is a bijection [λ]→{1,…,n}, and σ⋅t is characterised by (σ⋅t)(i,j)=σ(t(i,j)) (Tableaux and standard tableaux, Row and column stabilizers).

[F6]

A semistandard λ-tableau of content μ is a filling satisfying weak row increase, strict column increase and content μ (Semistandard tableaux and Kostka numbers).

[F7]

Sλ⊆Mλ is the complex span of the polytabloids es=κs⋅{s} (Column antisymmetrizers, polytabloids, and Specht modules), and it is an Sn-submodule of Mλ (Polytabloid covariance and the column sign rule).

Proof

technique · constructive
1.1F1F5constructalgebra

[construct] For a μ-tabloid {s} write B1,…,Bk for its row sets, so ∣Bi∣=μi; define φ({s})∈Tλ,μ to be the filling f with f(x):=i whenever t(x)∈Bi, which has content μ because t is a bijection, and conversely for f∈Tλ,μ put Bi:={t(x):f(x)=i}, so that the pairwise disjoint sets Bi cover {1,…,n} with ∣Bi∣=μi and are the rows of a μ-tabloid {s} with φ({s})=f; the two rules are inverse and φ:Ωμ→Tλ,μ is a bijection.

2.1F1step 1.1algebra

The left action on the tabloid basis transports along φ to the left action (σ⋅f)(x)=f(x′) with t(x′)=σ−1(t(x)), because the row of the label t(x) in σ⋅{s}={σ⋅s} is the row of σ−1(t(x)) in {s} by [F1]; hence the display in the Statement is a left action of Sn on Tλ,μ and φ is an isomorphism of Sn-modules, so we may compute with fillings and translate back along φ−1 at the end.

3.1F4F5step 2.1algebra

Let ρ∈Rt and f∈Tλ,μ. By [F5], ρ−1(t(x))=t(x′′) for the box x′′ in the same row i of [λ], since ρ preserves the row sets Ai of t by [F4], so (ρ⋅f)(x)=f(x′′): the entries of f are permuted within each row of [λ] and none leaves its row; conversely each permutation of the entries within the rows of f arises this way, because Rt is the full direct product of the symmetric groups on the disjoint sets A1,…,Ak by [F4] and the boxes of row i correspond bijectively to Ai via t by [F5]. Hence Rt⋅f is exactly the finite nonempty set of fillings obtained from f by permuting entries within rows.

4.1step 2.1step 3.1algebra

Let θu({t}):=∑v∈Rt⋅uv as in the Statement, a finite sum over the orbit of step 3.1; for every ρ∈Rt one has ρ⋅(Rt⋅u)=Rt⋅u because Rt is a subgroup acting on Tλ,μ by step 2.1, so ρ⋅θu({t})=θu({t}) and the orbit sum is Rt-invariant.

5.1F1F2F3step 4.1algebra

Define θu(σ⋅{t}):=σ⋅θu({t}) for σ∈Sn. This is well defined: if σ⋅{t}=τ⋅{t}, then τ−1σ∈Rt by [F2], so by step 4.1 and the left action axioms σ⋅θu({t})=τ⋅((τ−1σ)⋅θu({t}))=τ⋅θu({t}); since every tabloid is σ⋅{t} by [F3] and the tabloids form a basis of Mλ by [F1], the formula defines a unique C-linear map θu:Mλ→Mμ.

6.1step 5.1algebra

The map θu is Sn-linear: for γ,σ∈Sn, the left action axioms and step 5.1 give θu(γ⋅(σ⋅{t}))=θu((γσ)⋅{t})=(γσ)⋅θu({t})=γ⋅(σ⋅θu({t}))=γ⋅θu(σ⋅{t}), and the elements σ⋅{t} span Mλ.

7.1F6F7step 4.1step 6.1discharge-construct∎

Restricting along the inclusion Sλ⊆Mλ of the Sn-submodule [F7] gives a linear map θu∣Sλ:Sλ→Mμ with θu(γ⋅e)=γ⋅θu(e) for e∈Sλ and γ∈Sn by step 6.1, that is, a homomorphism of Sn-modules; if u=T is semistandard of content μ by [F6], this is the map θT of the Statement, whose value on {t} is the row-orbit sum ∑v∈Rt⋅Tv of step 4.1, and no nonvanishing of θT∣Sλ is asserted.

Remarks

  • The map depends only on the row class. If u′=ρ⋅u for some ρ∈Rt, then Rt⋅u′=Rt⋅u, so θu′=θu by step 4.1. The construction therefore attaches a homomorphism to each Rt-orbit of fillings of content μ, in agreement with the source's "sum of all members row equivalent to s" (Row and column stabilizers).

  • Dependence on the reference tableau. A different reference tableau t′=π⋅t produces the conjugate orbit sum and the same θ up to the identification Mμ→Mμ it induces; the homomorphisms relevant below are attached to semistandard fillings of a fixed reference tableau, which is all that is used.

  • The empty and singleton cases. For n=0 we have λ=μ=∅, the only filling is empty, Rt={1}, and θ is the identity C→C. For n=1, λ=μ=(1), again Rt={1} and θ is the identity.

  • No choice. The orbit sum is a finite sum over the finite group Rt, and the linear extension uses the tabloid basis of [F1]; no selection principle is used.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passjudge pass (gpt-6.1-sol)audited 2026-10-02Open item page →

Semistandard maps are independent and respect dominance

Statement

Let λ,μ⊢n and let t0 be the standard λ-tableau that carries the labels λ1+⋯+λi−1+1,…,λ1+⋯+λi in row i. Write Tλ,μ for the set of fillings of [λ] by positive integers with content μ (Semistandard tableaux and Kostka numbers), and for u∈Tλ,μ let θu:Mλ→Mμ be the Sn-module homomorphism of Semistandard fillings construct Specht-to-permutation homomorphisms constructed from the reference tableau t0. Then:

  1. (Nonvanishing and independence.) For every semistandard T∈Tλ,μ the restriction θT∣Sλ:Sλ→Mμ is nonzero; and if T1,…,Tr are pairwise distinct semistandard fillings of content μ, then θT1∣Sλ,…,θTr∣Sλ are linearly independent. In particular dim⁡CHom⁡Sn(Sλ,Mμ)≥Kλ,μ.
  2. (Dominance.) If there exists a semistandard λ-tableau of content μ, that is, if Kλ,μ≠0, then λ⊵μ in the dominance order (Dominance order on partitions).
  3. (Diagonal case.) Kλ,λ=1: there is exactly one semistandard λ-tableau of content λ, the filling whose i-th row consists entirely of the entry i.

Facts & Assumptions

Given: partitions λ,μ⊢n, the standard reference tableau t0, and the homomorphisms θu for u∈Tλ,μ.

[F1]

The rule {s}↦f, where f(x) is the row of t0(x) in the μ-tabloid {s}, is a bijection from the μ-tabloids onto Tλ,μ, and the transported left action on fillings satisfies (σ⋅f)(x)=f(x′) whenever t0(x′)=σ−1(t0(x)); the μ-tabloids form a basis of Mμ, and θu is the Sn-linear map determined by θu({t0})=∑v∈Rt0⋅uv (Semistandard fillings construct Specht-to-permutation homomorphisms).

[F2]

A filling T of [λ] has content μ when the entry i occurs in exactly μi boxes; it is semistandard when its entries weakly increase along every row and strictly increase down every column, and Kλ,μ is the number of such fillings (Semistandard tableaux and Kostka numbers).

[F3]

et=κt⋅{t} and κt=∑γ∈Ctsgn⁡(γ)γ; the stabilizer subgroups Ct,Rt preserve every column set and every row set of t; Ct0 is the direct product of the symmetric groups on the label sets of the columns of t0 (Column antisymmetrizers, polytabloids, and Specht modules, Row and column stabilizers).

[F4]

eσ⋅t=σ⋅et for every σ∈Sn and γ⋅et=sgn⁡(γ)et for γ∈Ct; Sλ is the C-span of the polytabloids et and is an Sn-submodule of Mλ (Polytabloid covariance and the column sign rule).

[F5]

A λ-tableau is a bijection [λ]→{1,…,n}; it is standard when its entries strictly increase along rows and down columns, and the tabloid {t} records the row sets of t (Tableaux and standard tableaux, Young subgroups, tabloids, and permutation modules).

[F6]

[λ]={(r,c):1≤r≤k, 1≤c≤λr} is a Young diagram, so it is closed to the left and upwards (Partitions, English diagrams, and conjugation).

Proof

technique · constructive
1.1F5F6construct

[construct] The rule t0(r,c):=λ1+⋯+λr−1+c defines a bijection [λ]→{1,…,n}, because the row blocks Br={λ1+⋯+λr−1+1,…,λ1+⋯+λr} are disjoint intervals of sizes λr covering {1,…,n} and increase along each row, and t0(r,c)=λ1+⋯+λr−1+c<t0(r+1,c)=λ1+⋯+λr+c, so the entries strictly increase down every column. Hence t0 is a standard λ-tableau.

1.2F1F3F5algebra

The stabilizer Rt0 of {t0} consists of the permutations that preserve each row set of t0, and such a ρ acts on a filling f by (ρ⋅f)(x)=f(x′′) with t0(x′′)=ρ−1(t0(x)) by [F1]; since t0 carries the labels λ1+⋯+λr−1+1,…,λ1+⋯+λr in row r, the box x′′ lies in the same row of [λ] as x. So the row orbit Rt0⋅f consists exactly of the fillings obtained from f by permuting the entries within each row of [λ], and two fillings in the same row orbit have the same multiset of entries in every row.

1.3F2F6constructalgebra

For f∈Tλ,μ define Nf(i,j):=#{(r,c):c≤j, f(r,c)≤i} for 1≤i≤μ1′ and 1≤j≤λ1, and set Nf(0,j)=Nf(i,0)=0 on the boundary. Because the number of entries equal to i in column c is (Nf(i,c)−Nf(i−1,c))−(Nf(i,c−1)−Nf(i−1,c−1)), the vector Nf determines, and is determined by, the ordered tuple of the multisets of entries in the columns of [λ]; thus Nf=Ng holds exactly when every column of g is a rearrangement of the corresponding column of f, and the relation f⪯g defined by Nf(i,j)≤Ng(i,j) for all i,j is a preorder on the finite set Tλ,μ.

1.4F2F6algebra

Let T be a semistandard λ-tableau of content μ and let i≥1. The set Di:={(r,c)∈[λ]:T(r,c)≤i} of boxes with entries ≤i is closed to the left and upwards: if (r,c)∈Di and c≥2 then T(r,c−1)≤T(r,c)≤i by weak increase along rows, and if r≥2 then T(r−1,c)<T(r,c)≤i by strict increase down columns; hence Di is a Young diagram inside [λ] by [F6]. Moreover (r,c)∈Di implies r≤i, since the entries strictly increase down a column, so 1≤T(1,c)<⋯<T(r,c)≤i gives r≤T(r,c)≤i. So Di lies in the first i rows and has μ1+⋯+μi boxes by the content condition [F2], whence μ1+⋯+μi≤λ1+⋯+λi for all i≥1 (both prefixes equal n for i at least the number of parts of μ), that is λ⊵μ: this proves claim 2. If moreover μ=λ, then ∣Di∣=λ1+⋯+λi is the number of boxes in the first i rows of [λ]; a left- and upward-closed subdiagram with the same number of boxes as its ambient diagram equals it, so Di is exactly those first i rows, a box in row r carries an entry ≤r but not ≤r−1, namely r, and T is the filling whose r-th row is constant with entry r; conversely that filling is semistandard of shape and content λ, so Kλ,λ=1, proving claim 3.

2.1F1F3step 1.1step 1.3algebra

For γ∈Ct0 the box x′ with t0(x′)=γ−1(t0(x)) lies in the same column of [λ] as x by step 1.1, since γ preserves the column sets of t0 by [F3]; hence γ acts on fillings by permuting the entries within each column of [λ], and conversely every such columnwise permutation of labels lies in Ct0. Therefore Nγ⋅f=Nf for all γ∈Ct0 and f∈Tλ,μ by step 1.3, and if Ng=Nf then g=γ⋅f for some γ∈Ct0.

2.2F2step 1.2step 1.3algebra

Let T∈Tλ,μ be semistandard and let f be a filling obtained from T by permuting the entries within rows. Fix i: in each row r of T the entries ≤i form an initial segment, since T(r,1)≤T(r,2)≤⋯, so the number of entries ≤i in the first j columns of row r of T is min⁡(j,mr(i)) with mr(i):=#{c:T(r,c)≤i}, while the same count for f is at most min⁡(j,mr(i)), because f has the same entries in row r as T by step 1.2. Summing over rows gives Nf(i,j)≤NT(i,j) for all i,j, that is f⪯T. If moreover Nf=NT, then for each row r and all i,j we have #{c≤j:f(r,c)≤i}=min⁡(j,mr(i)), and induction on j gives f(r,j)=T(r,j): assuming f(r,c)=T(r,c) for c<j, the difference of the identities for j and j−1 yields [f(r,j)≤i]=min⁡(j,m(i))−min⁡(j−1,m(i))=[m(i)≥j]=[T(r,j)≤i] for every i, and a value is determined by the thresholds that dominate it. As r was arbitrary, f=T; so among the fillings of the row orbit Rt0⋅T the filling T is the unique one with Nf=NT.

2.3F2step 1.3algebra

Two distinct semistandard fillings T,T′ of content μ satisfy NT≠NT′: if NT=NT′ then by step 1.3 each column of T′ is a rearrangement of the corresponding column of T, and each column of a semistandard filling is strictly increasing, hence determined by its multiset, so T=T′.

2.4F1F2F3F4step 1.2algebra

For any finite C-linear combination F=∑TaTθT of the maps attached to semistandard fillings, Sn-linearity of the θT, the identity et0=κt0⋅{t0} of [F3] and the defining value of θT in [F1] give the identity F(et0)=κt0⋅(∑TaT∑f∈Rt0⋅Tf)=∑TaT∑f∈Rt0⋅Tκt0⋅f in Mμ, the outer sums being finite because Tλ,μ is finite by [F2].

3.1F2F7step 2.1algebra

For f∈Tλ,μ the expansion of κt0⋅f=∑γ∈Ct0sgn⁡(γ) γ⋅f in the filling basis involves, by step 2.1, only fillings g with Ng=Nf; so the coefficient of a filling g in κt0⋅f is zero unless Ng=Nf, and the coefficient of f itself is ∑γ⋅f=fsgn⁡(γ). The latter is 1 when f=T is semistandard: a nontrivial γ∈Ct0 permutes two entries of some column of T, whereas T has distinct entries in every column, so only γ=1 fixes T and sgn⁡(1)=1 by [F7].

4.1F2step 1.3step 2.2step 2.3step 2.4step 3.1constructalgebra

Suppose that ∑TaTθT=0 with not all aT=0, and among the semistandard T with aT≠0 choose T∗ whose vector NT∗ is maximal in the preorder of step 1.3: whenever NT∗(i,j)≤NT(i,j) for all i,j and aT≠0, then NT=NT∗; such T∗ exists because the semistandard fillings of content μ form a finite set by [F2]. In the filling-basis expansion of F(et0)=∑TaT∑f∈Rt0⋅Tκt0⋅f from step 2.4, the coefficient of T∗ is exactly aT∗≠0: a term κt0⋅f with f∈Rt0⋅T can contribute only if Nf=NT∗ by step 3.1, while Nf⪯NT by step 2.2, so maximality gives NT=NT∗ and then T=T∗ by step 2.3; within the orbit Rt0⋅T∗ the condition Nf=NT∗ forces f=T∗ by step 2.2, and the coefficient of T∗ in κt0⋅T∗ is 1 by step 3.1.

5.1F2F4step 1.4step 2.4step 4.1discharge-construct

Hence every nonzero combination F=∑TaTθT satisfies F(et0)≠0 by steps 2.4 and 4.1, so the restrictions θT∣Sλ for distinct semistandard T are linearly independent; taking a combination with a single nonzero coefficient shows that each θT∣Sλ is nonzero. Since these restrictions lie in Hom⁡Sn(Sλ,Mμ) by [F4], that space has dimension at least the number of semistandard fillings, which is Kλ,μ by [F2]. This proves claim 1, and claims 2 and 3 are step 1.4.

6.1step 1.3step 1.4step 5.1discharge-construct∎

Claims 1, 2 and 3 are steps 5.1 and 1.4. No division and no choice principle is used: the order of step 1.3 compares finitely many integer vectors attached to the finitely many fillings of content μ, and T∗ is a maximal element of a finite set.

Remarks

  • What the order does. The vector Nf is the dominance criterion applied to the multiset of entries of each column: increasing Nf(i,j) means moving smaller entries to the left, the move generating the column-word order used in the source proof. Step 4.1 shows that the matrix of coefficients of the maps θT against the filling basis is triangular with diagonal entries 1 when the semistandard fillings are listed compatibly with ⪯, which is the triangularity behind the independence statement. Step 2.2 is the quantitative form of the source observation that a row permutation of a semistandard tableau produces a strictly smaller column word (Semistandard fillings construct Specht-to-permutation homomorphisms).

  • Linearity over other rings. Steps 1.1--5.1 never divide by an integer and never use a sign cancellation of the form c=−c, so the independence statement holds verbatim after base change to any commutative ring over which the maps θT are defined, and in particular over any field. The counting statements 2 and 3 are ring-independent. The characteristic-zero hypothesis is used only later, when these maps are upgraded to a spanning set and to multiplicities of Specht modules.

  • Dominance is not an input to independence. The choice of T∗ in step 4.1 uses only maximality in a finite preorder; the dominance statement 2 is proved separately in step 1.4 and is not used in steps 1.1--5.1. In particular no circular use of Young's rule occurs here.

  • Boundary cases. For n=0 we have λ=μ=∅, the unique filling is empty and semistandard, K∅,∅=1, and θ is the identity of the one-dimensional space C; all claims hold. For n≥1 and λ=(n) there is exactly one semistandard filling of content μ for each partition μ of n, namely the single row filled with the entries of μ in weakly increasing order, in agreement with K(n),μ=1.

  • No choice. All sets of fillings are finite, the order is a componentwise integer comparison, and the maximal element T∗ is selected from a finite set; no selection principle is used.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-10-02Open item page →

Semistandard maps span the Hom space in characteristic zero

Statement

Let n≥0, let λ,μ⊢n, and work over C. Fix the standard reference λ-tableau t0 with t0(r,c)=λ1+⋯+λr−1+c (Semistandard maps are independent and respect dominance), write Tλ,μ for the finitely many fillings of [λ] with content μ (Semistandard tableaux and Kostka numbers), and for u∈Tλ,μ let θu:Mλ→Mμ be the Sn-module homomorphism with θu({t0})=∑v∈Rt0⋅uv (Semistandard fillings construct Specht-to-permutation homomorphisms). Then the restrictions θT∣Sλ:Sλ→Mμ of the semistandard fillings T∈Tλ,μ span Hom⁡Sn(Sλ,Mμ) over C.

Facts & Assumptions

Given: partitions λ,μ⊢n, the standard reference tableau t0, and the maps θu for u∈Tλ,μ.

[F1]

The rule {s}↦f, where f(x) is the row of t0(x) in the μ-tabloid {s}, is a bijection from the μ-tabloids onto Tλ,μ; the transported left action satisfies (σ⋅f)(x)=f(x′) whenever t0(x′)=σ−1(t0(x)), so a transposition of two labels a≠b exchanges the entries in the boxes labelled a and b and fixes all other entries, and the μ-tabloids, equivalently the fillings Tλ,μ, form a basis of Mμ; the maps θu are the well-defined Sn-linear maps with θu({t0})=∑v∈Rt0⋅uv and θu(σ⋅{t0})=σ⋅θu({t0}) (Semistandard fillings construct Specht-to-permutation homomorphisms).

[F2]

Tλ,μ is finite; a filling is semistandard when its entries weakly increase along every row and strictly increase down every column, and Kλ,μ counts the semistandard members (Semistandard tableaux and Kostka numbers).

[F3]

et=κt⋅{t} and κt=∑γ∈Ctsgn⁡(γ)γ; for γ∈Ct one has γ⋅et=sgn⁡(γ)et; for every σ∈Sn one has eσ⋅t=σ⋅et; and Sλ is generated as an Sn-module by et for any single λ-tableau t (Column antisymmetrizers, polytabloids, and Specht modules, Polytabloid covariance and the column sign rule).

[F4]

For f∈Tλ,μ put Nf(i,j):=#{(r,c):c≤j, f(r,c)≤i} for i≥1, j≥1. Then Nf=Ng holds exactly when every column of g is a rearrangement of the corresponding column of f; if T is semistandard and f lies in the row orbit Rt0⋅T, then Nf(i,j)≤NT(i,j) for all i,j with equality exactly for f=T; and if T is semistandard then the coefficient of T in κt0⋅f is 0 unless Nf=NT, while the coefficient of T in κt0⋅T equals 1 (Semistandard maps are independent and respect dominance, established in the course of that proof).

[F5]

(Garnir.) Let j,j+1 be adjacent columns of [λ], let X be a set of entries of column j of t0 and Y a set of entries of column j+1 of t0 with ∣X∣+∣Y∣>λj′, and let T be any set of representatives containing 1 for the left cosets of H:=SX×SY in SX∪Y. Then ∑g∈Tsgn⁡(g) g⋅et0=0 (Integral Garnir straightening and the field-uniform standard basis, claim 1).

[F6]

Ct0 preserves every column set of t0 and is the direct product of the symmetric groups on the label sets of the columns; acting on fillings, its elements permute the entries within each column (Row and column stabilizers, [F1]).

[F7]

sgn⁡ is a homomorphism and sgn⁡((a b))=−1 for a transposition, and C has characteristic 0 so 2≠0 (The sign is a homomorphism Sn→{+1,−1}, surjective exactly when n≥2).

Proof

technique · constructive
1.1F1F2F3constructalgebra

[construct] Fix f∈Hom⁡Sn(Sλ,Mμ) and expand f(et0)=∑T∈Tλ,μcT T in the filling basis of [F1]; the sum is finite by [F2]. Since et0 generates Sλ as an Sn-module by [F3], the map f is determined by f(et0): if f(et0)=0 then f(σ⋅et0)=σ⋅f(et0)=0 for every σ∈Sn, and these elements span Sλ. It therefore suffices to express f(et0) as a C-linear combination of the vectors θT(et0) with T semistandard: if f(et0)=∑TaTθT(et0) then the Sn-linear maps f and ∑TaTθT agree on the generator et0, hence are equal.

1.2F1F3F7algebra

For τ∈Ct0 and every filling T one has cτ⋅T=sgn⁡(τ)cT: by [F3] and Sn-linearity of f, τ⋅f(et0)=f(τ⋅et0)=sgn⁡(τ)f(et0), while expanding the left side in the filling basis gives τ⋅f(et0)=∑TcT (τ⋅T), so comparing coefficients of the basis element τ⋅T yields cT=sgn⁡(τ)cτ⋅T and hence cτ⋅T=sgn⁡(τ)cT by [F7].

1.3F1F4algebra

(Cross swaps increase N.) Let x be a box in a column j, let y be a box in the column j+1, let f be a filling with f(x)>f(y), and let τ:=(t0(x) t0(y)), so that τ⋅f is obtained from f by exchanging the values at x and y by [F1]. Then Nτ⋅f(i,k)≥Nf(i,k) for all i,k, with strict inequality for i=f(y), k=j: for k<j or k≥j+1 the swap changes no count of entries in the first k columns, while for k=j the two counts differ by [f(y)≤i]−[f(x)≤i], which is 0 or 1 because f(y)<f(x), namely 1 exactly when f(y)≤i<f(x).

1.4F5constructalgebra

(A transverse transversal.) Let X,Y be disjoint nonempty label sets carried by a set of boxes of column j and column j+1 respectively, put Z:=X∪Y and p:=∣X∣, and for every p-element subset A⊆Z write X∖A={a1<⋯<ar} and A∖X={b1<⋯<br}, with r:=∣X∖A∣=∣A∖X∣, and put gA:=(a1 b1)⋯(ar br), the empty product for A=X giving gX=1. Then gA(X)=A and gA maps each element of X∖A to an element of Y and conversely, so gA−1=(ar br)⋯(a1 b1) is a product of r transpositions each exchanging an element of X with an element of Y; and {gA:∣A∣=p} is a set of representatives for the left cosets of H=SX×SY in SZ containing 1, because H is exactly the setwise stabilizer of X in SZ so the coset gH is determined by g(X)∈{A:∣A∣=p} and gA(X)=A realizes each value; consequently this is a transversal of the kind required in [F5].

1.5F2constructalgebra

(Finite descending induction.) Since Tλ,μ is finite by [F2], the set N:={NT:T∈Tλ,μ} is finite, and we fix a total order ⪯ on N extending the componentwise order in the sense that N⊑N′ implies N⪯N′; such an order exists because a finite partial order is listed by repeatedly removing a maximal element. For a nonzero v∈Mμ let m(v) be the ⪯-greatest element of {NT:the coefficient of T in v is nonzero}. Claim: if v=f(et0) for some f∈Hom⁡Sn(Sλ,Mμ) and v≠0, then there is a semistandard S such that v−cSθS(et0)=0 or m(v−cSθS(et0))≺m(v), where cS is the coefficient of S in v.

2.1F1F6F7step 1.2algebra

If a filling T has two boxes x≠y of the same column carrying the same entry, then cT=0. Indeed, let a:=t0(x)≠b:=t0(y) be the labels of those boxes and let τ:=(a b); then τ∈Ct0 by [F6] and, by [F1], τ exchanges the entries in the boxes labelled a and b, so τ⋅T=T; step 1.2 gives cT=cτ⋅T=sgn⁡(τ)cT=−cT by [F7], hence 2cT=0 and cT=0 in C. Thus every filling with cT≠0 has pairwise distinct entries in each of its columns.

2.2F2F3F4step 1.1algebra

(Expansion of a semistandard θS.) Let S∈Tλ,μ be semistandard and write θS(et0)=∑gdg g in the filling basis. Then dg=0 unless Ng⊑NS componentwise, and for every g with Ng=NS there is a unique τg∈Ct0 with τg⋅S=g, and dg=sgn⁡(τg). Indeed θS(et0)=∑u∈Rt0⋅Sκt0⋅u, and the coefficient of g in κt0⋅u vanishes unless Ng=Nu by [F4], while Nu⊑NS for u in the row orbit; so dg=0 unless Ng=Nu for some such u, whence Ng⊑NS, and if Ng=NS then Nu=NS forces u=S by [F4], so dg is the coefficient of g in κt0⋅S, namely ∑γ∈Ct0:γ⋅S=gsgn⁡(γ); the column-sorted semistandard S has distinct entries in each column by [F2], so γ⋅S=S only for γ=1 and there is exactly one γ∈Ct0 with γ⋅S=g, giving dg=sgn⁡(γ) for that unique γ, which we call τg.

3.1F4step 1.2step 1.5step 2.1constructalgebra

Let us record the standing choice of a maximal level. For the fixed f of step 1.1 with support {T:cT≠0} nonempty put v:=f(et0) and choose T1 in the support with NT1=m(v), the ⪯-greatest support level of step 1.5; then every support filling T satisfies NT⪯NT1, and no support filling has NT strictly above NT1 componentwise, because NT⊐NT1 would imply NT≻NT1 in the total order by the extension property of ⪯. Replace T1 by the unique filling obtained from it by sorting each column increasingly; NT1=m(v) is unchanged by [F4] because column sorting only rearranges entries within columns, the coefficient still satisfies cT1≠0 (it is multiplied by a sign by step 1.2), the entries of T1 are pairwise distinct in each column by step 2.1, and the columns of T1 are strictly increasing by construction. So we may assume: cT1≠0, the columns of T1 strictly increase, NT1=m(v), and no filling T with cT≠0 has NT strictly above NT1 in the componentwise order.

4.1F2F4step 3.1algebra

(Descent contradicts maximality.) Suppose the filling T1 of step 3.1 is not semistandard. Since its columns are strictly increasing and it is not semistandard, some row q of T1 descends between adjacent columns j,j+1: with a:=T1(q,j) and b:=T1(q,j+1) one has a>b. Let X be the set of labels of the boxes (r,j) with q≤r≤λj′ and Y the set of labels of the boxes (r,j+1) with 1≤r≤q; these are label sets of column j and column j+1 of t0, and ∣X∣+∣Y∣=(λj′−q+1)+q=λj′+1>λj′. Because the columns of T1 strictly increase, T1(x)≥a for every box x∈X and T1(y)≤b for every box y∈Y, and a>b, so T1(x)>T1(y) for all such boxes.

5.1F1F5step 1.1step 1.4algebra

With X,Y,Z as in step 4.1 and the transversal {gA} of step 1.4, the Garnir relation [F5] gives ∑Asgn⁡(gA) gA⋅et0=0 in Mλ, where A ranges over the p-element subsets of Z. Applying the Sn-linear map f and expanding yields the identity 0=∑AcgA−1T1sgn⁡(gA) in C: the coefficient of the basis element T1 in ∑Asgn⁡(gA) gA⋅f(et0) is ∑Asgn⁡(gA)cgA−1⋅T1, because within the A-th summand exactly the filling gA−1⋅T1 is transported to T1 by gA.

6.1F4step 2.1step 1.3step 1.4step 3.1step 4.1algebra

In the identity of step 5.1, every term with A≠X vanishes. Indeed, for A≠X the permutation gA−1 is a product of r=∣X∖A∣≥1 transpositions (ai bi) with ai∈X and bi∈Y by step 1.4, and these act on disjoint pairs of boxes labelled by elements of Z; applying them one after another to T1, each step exchanges the value at the box labelled ai, which is still T1's value there and is >b, with the value at the box labelled bi, which is still ≤b, and hence, by step 1.3 and T1(x)>T1(y) for all boxes x∈X, y∈Y from step 4.1, strictly increases the count vector N at each step. So NgA−1T1(i,k)≥NT1(i,k) for all i,k with strict inequality somewhere, and cgA−1T1=0 by the maximality of NT1 in step 3.1.

7.1F1step 3.1step 5.1step 6.1algebra

Therefore the identity of step 5.1 reduces to cT1sgn⁡(gX)=cT1=0, contradicting cT1≠0 from step 3.1. Hence the filling T1 is semistandard.

8.1F4step 1.2step 1.5step 2.2step 3.1step 7.1algebra

(Subtraction kills a whole level.) Keep T1 semistandard with cT1≠0 and NT1=m(v) from step 7.1 and step 3.1 and put v′:=f(et0)−cT1 θT1(et0), with coefficients cg′=cg−cT1dg in the filling basis. If Ng=NT1 then g is a column rearrangement of T1 by [F4], so g=τg⋅T1 for the unique τg∈Ct0 of step 2.2; step 1.2 gives cg=sgn⁡(τg)cT1 and step 2.2 gives dg=sgn⁡(τg), so cg′=sgn⁡(τg)cT1−sgn⁡(τg)cT1=0. Every g with cg′≠0 satisfies Ng⪯NT1: if cg≠0 then this is the maximality of NT1=m(v) among the support levels in the total order of step 1.5, and if dg≠0 then Ng⊑NT1 by step 2.2, hence again Ng⪯NT1. Since no such g has Ng=NT1, every nonzero coefficient of v′ sits at a level strictly below NT1 in the total order.

9.1step 1.5step 3.1step 7.1step 8.1algebra

This proves the claim of step 1.5: take S:=T1, which is semistandard by step 7.1. Step 8.1 says that the residual v′:=v−cSθS(et0) either is zero or has every support level strictly below m(v), so in the nonzero case m(v′)≺m(v).

10.1F1F3step 1.1step 1.5step 9.1constructalgebra

Set f0:=f and v0:=f(et0). Whenever vk≠0, apply step 9.1 to vk=fk(et0), choose the resulting semistandard Sk and its coefficient ak in vk, and put fk+1:=fk−akθSk∣Sλ and vk+1:=fk+1(et0). Each fk+1 is Sn-linear by [F1]. Either vk+1=0 and we stop, or m(vk+1)≺m(vk). The nonzero residuals thus have strictly decreasing levels in the finite set N, so after at most ∣N∣ subtractions we reach vk=0. Then f(et0)=∑j<kajθSj(et0), and the Sn-linear maps agree on a module generator, hence f=∑j<kajθSj∣Sλ by step 1.1. If v0=0, the same conclusion holds with the empty sum.

11.1F2F7step 1.1step 7.1step 10.1discharge-construct∎

The remaining cases are the empty ones: for n=0 one has λ=μ=∅, the set T∅,∅ consists of the single empty filling, which is semistandard because its row and column conditions are vacuous, and θ∅ is the identity of M∅=C, so Hom⁡(S∅,M∅)=C is spanned by that restriction; here step 1.1 applies with et0 generating S∅, and the argument of the descent and subtraction steps is either vacuous or terminates at once, since the support of f(et0) is empty or consists of the semistandard empty filling. No division is used anywhere, only the fact that 2≠0 in C in step 2.1, and all choices made are selections of a maximal element or a unique column-sorted filling from finite explicitly given sets, so no choice principle is invoked.

Remarks

  • Route. Step 1.1 reduces the spanning claim to the vectors θT(et0); for any nonzero f(et0) the covariance and descent steps produce a semistandard filling at the greatest count vector in the total order of step 1.5 by comparing the integral Garnir relation with the count vector N, and the subtraction and induction steps remove those semistandard maps one whole level at a time. This is the direct characteristic-zero proof, using no RSK bijection and no dimension count; the independent semistandard maps give the reverse inequality, so together they yield dim⁡Hom⁡Sn(Sλ,Mμ)=Kλ,μ on the next page (Young's rule for complex permutation modules).

  • Characteristic zero. Step 2.1 divides by 2 implicitly when it cancels 2cT=0; over a field of characteristic 2 the semistandard maps need not span, and the spanning statement is a characteristic-zero phenomenon. The last stages use only finite well-ordering, not division.

  • No choice. The only selections are from the finite sets Tλ,μ and N and the finite gallery of subsets A of Z; the total order ⪯ of step 1.5 is produced by finitely many maximal-element removals.

TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-10-02Open item page →

Young's rule for complex permutation modules

Statement

Let n≥0, let λ,μ⊢n, let Mμ be the complex Young permutation module of shape μ with its tabloid basis (Young subgroups, tabloids, and permutation modules), and let Sλ⊆Mλ be the complex Specht module (Column antisymmetrizers, polytabloids, and Specht modules). Write Kλ,μ for the Kostka number (Semistandard tableaux and Kostka numbers) and, for an integer r≥0, let (Sλ)⊕r denote a direct sum of r copies of Sλ, the zero module when r=0. Then:

  1. (Isomorphism type.) Mμ is completely reducible and there is an isomorphism of CSn-modules Mμ≅⨁λ⊢n(Sλ)⊕Kλ,μ, the sum being over the finitely many partitions of n.
  2. (Multiplicity.) In every decomposition of Mμ as a direct sum of irreducible subrepresentations the number of summands isomorphic to Sλ equals Kλ,μ; that is, the multiplicity [Mμ:Sλ] is well defined and equal to the Kostka number Kλ,μ, independently of the decomposition.

Facts & Assumptions

Given: an integer n≥0, partitions λ,μ⊢n, the complex Young permutation module Mμ with its tabloid basis, the Specht module Sλ⊆Mλ, the standard reference λ-tableau t0 and the homomorphisms θu:Mλ→Mμ attached to the fillings u of [λ] with content μ.

[F1]

The tabloids of shape μ form a basis of Mμ, on which Sn acts by σ⋅{t}={σ⋅t}; the finite set Ωμ of tabloids is nonempty, so Mμ≠0, and Mμ is a finite-dimensional complex representation of Sn. For n=0 one has μ=∅, M∅=C with basis the empty tabloid and trivial S0-action, and S∅=C (Young subgroups, tabloids, and permutation modules, Column antisymmetrizers, polytabloids, and Specht modules).

[F2]

For every filling u of [λ] with content μ the rule θu({t0})=∑v∈Rt0⋅uv, extended Sn-equivariantly, defines an Sn-module homomorphism θu:Mλ→Mμ, and its restriction θT∣Sλ:Sλ→Mμ to the Specht module is again Sn-linear, for every semistandard T of content μ (Semistandard fillings construct Specht-to-permutation homomorphisms, Semistandard tableaux and Kostka numbers).

[F3]

If T1,…,Tr are pairwise distinct semistandard λ-tableaux of content μ, then θT1∣Sλ,…,θTr∣Sλ are linearly independent over C, so dim⁡CHom⁡Sn(Sλ,Mμ)≥Kλ,μ; moreover Kλ,λ=1, and Kλ,μ≠0 implies λ⊵μ in the dominance order (Semistandard maps are independent and respect dominance).

[F4]

The restrictions θT∣Sλ of the semistandard λ-tableaux T of content μ span Hom⁡Sn(Sλ,Mμ) over C (Semistandard maps span the Hom space in characteristic zero).

[F5]

Kλ,μ is the number of semistandard λ-tableaux of content μ; the set of fillings of [λ] with content μ is finite; every entry of such a filling lies between 1 and the number l(μ) of parts of μ; and K∅,∅=1 (Semistandard tableaux and Kostka numbers).

[F6]

Every finite-dimensional complex representation of Sn is completely reducible, that is, a direct sum of finitely many irreducible subrepresentations (with the empty sum allowed for the zero representation); this is Maschke's theorem for the finite group Sn in characteristic 0, where char⁡C=0 does not divide ∣Sn∣=n! (If char⁡k∤∣G∣, every finite-dimensional representation of G is completely reducible, Maschke's theorem for finite groups over fields whose characteristic does not divide ∣G∣, A completely reducible representation as a finite direct sum of irreducible subrepresentations).

[F7]

The modules {Sλ:λ⊢n} form a complete irredundant list of the finite-dimensional irreducible complex Sn-representations: each Sλ is irreducible, every finite-dimensional irreducible complex Sn-representation is isomorphic to some Sλ, and Sλ≅Sσ if and only if λ=σ (Specht modules classify the complex irreducibles of Sn).

[F8]

A nonzero intertwiner between irreducible representations over any field is an isomorphism, so Hom⁡Sn(Sλ,Sσ)=0 for non-isomorphic irreducibles; and over the algebraically closed field C every endomorphism of an irreducible representation is a scalar, so End⁡Sn(Sλ)=C idSλ (Schur's lemma for irreducible representations: a nonzero intertwiner is an isomorphism, and End⁡G(V) is a division ring, Over an algebraically closed field, every endomorphism of an irreducible representation is scalar).

Proof

technique · constructive
1.1F2F3F4F5constructalgebra

[construct] The restrictions θT∣Sλ:Sλ→Mμ of the semistandard fillings T of content μ form a basis of the complex vector space Hom⁡Sn(Sλ,Mμ): they span by [F4], they are linearly independent by [F3], and by [F5] there are exactly Kλ,μ of them. Hence dim⁡CHom⁡Sn(Sλ,Mμ)=Kλ,μ, and in particular a nonzero intertwiner Sλ→Mμ exists exactly when Kλ,μ≠0.

1.2F1F6F7construct

By [F6] the finite-dimensional complex representation Mμ is completely reducible, so there are irreducible subrepresentations U1,…,Ur with Mμ=U1⊕⋯⊕Ur; here r≥1 because the tabloid basis of [F1] is nonempty. By [F7] each Ui is isomorphic to Sσ(i) for exactly one partition σ(i)⊢n, and Sλ≅Sσ holds only for σ=λ.

1.3constructalgebra

Let W be a CSn-module and let M=U1⊕⋯⊕Ur be a direct sum of subrepresentations with projections πi:M→Ui along the other summands. Then πi is Sn-linear, so the rule f↦(π1f,…,πrf) maps Hom⁡Sn(W,M) into Hom⁡Sn(W,U1)⊕⋯⊕Hom⁡Sn(W,Ur); this map is C-linear, it is injective because f(w)=∑ifi(w) is determined by its components fi=πif, and it is surjective because a tuple of intertwiners (f1,…,fr) defines the intertwiner w↦∑ifi(w) of which it is the tuple of components. Hence Hom⁡Sn(W,U1⊕⋯⊕Ur)≅⨁i=1rHom⁡Sn(W,Ui).

1.4F7F8algebra

For irreducible Sλ and Sσ one has dim⁡CHom⁡Sn(Sλ,Sσ)=1 when σ=λ and 0 otherwise. If σ≠λ, then Sλ and Sσ are non-isomorphic by the irredundancy in [F7], so every intertwiner between them is zero by [F8]. If σ=λ, the same fact of [F8] makes every endomorphism of the irreducible Sλ a scalar multiple of idSλ, so End⁡Sn(Sλ)=C idSλ has dimension one.

2.1step 1.2step 1.3step 1.4algebra

Applying step 1.3 with W=Sλ to the decomposition of step 1.2 gives Hom⁡Sn(Sλ,Mμ)≅⨁i=1rHom⁡Sn(Sλ,Ui), and substituting the isomorphism Ui≅Sσ(i) of step 1.2 into step 1.4 gives dim⁡CHom⁡Sn(Sλ,Ui)=1 when σ(i)=λ and 0 otherwise. Hence dim⁡CHom⁡Sn(Sλ,Mμ) equals the number #{i:σ(i)=λ} of summands of this decomposition isomorphic to Sλ.

3.1step 1.1step 1.2step 2.1algebra

By step 1.1 the dimension in step 2.1 is Kλ,μ, so the decomposition of step 1.2 contains exactly Kλ,μ summands isomorphic to Sλ. Steps 1.2 and 2.1 apply verbatim to every decomposition of Mμ into irreducible subrepresentations, and the quantity they compute, dim⁡CHom⁡Sn(Sλ,Mμ), depends only on Mμ and λ; hence every such decomposition contains exactly Kλ,μ summands isomorphic to Sλ and the multiplicity [Mμ:Sλ] is well defined and equal to Kλ,μ. Grouping the summands of step 1.2 by their isomorphism classes gives the asserted isomorphism Mμ≅⨁λ⊢n(Sλ)⊕Kλ,μ.

4.1F1F3F5F6F7givenstep 3.1discharge-construct∎

Boundary, degenerate, characteristic and choice audit. For n=0 the only partition is ∅, and M∅=C, S∅=C, K∅,∅=1 by [F1] and [F5], so claim 1 reads M∅≅S∅ and steps 1.2 and 2.1 give r=1 with σ(1)=∅. If Kλ,μ=0, the summand (Sλ)⊕0=0 is omitted and claim 2 says that Sλ does not occur in Mμ; this happens for instance when l(λ)>l(μ), since every entry of a semistandard filling of content μ lies in {1,…,l(μ)} by [F5] while the first column of [λ] has l(λ) boxes carrying strictly increasing entries, and also for μ=(n) with λ≠(n), where all entries of a filling of content (n) are equal to 1 and a column of length at least two cannot strictly increase. If Kλ,μ=1, the summand is a single copy of Sλ: by [F3] this happens for λ=μ, so every Mλ contains exactly one copy of Sλ; and it happens for the one-row shape λ=(n) for every μ⊢n, since a semistandard filling of the single-row diagram (n) with content μ is exactly the weakly increasing word 1μ12μ2⋯ of content μ, which exists and is unique. The argument is particular to C: [F6] uses that char⁡C=0 does not divide ∣Sn∣=n! and [F8] uses that C is algebraically closed, and no analogue over a field of positive characteristic is asserted. The only selection made is the decomposition of the finite-dimensional module Mμ into finitely many irreducible summands, whose existence is supplied by [F6]; step 3.1 shows the multiplicities do not depend on this selection, and no choice principle is invoked. This proves claims 1 and 2.

Remarks

  • The two computations of one number. Young's rule is the equality of two counts of dim⁡CHom⁡Sn(Sλ,Mμ): the semistandard construction of Semistandard maps are independent and respect dominance and Semistandard maps span the Hom space in characteristic zero exhibits a basis indexed by the semistandard tableaux, while complete reducibility of Mμ and Schur's lemma compute the same dimension as the multiplicity of Sλ. Equivalently, for complex representations [Mμ:Sλ]=dim⁡CHom⁡Sn(Sλ,Mμ).

  • No Robinson-Schensted-Knuth input. The count Kλ,μ of semistandard tableaux enters only through its definition (Semistandard tableaux and Kostka numbers); the spanning argument behind the basis of the Hom space is the Garnir straightening computation of Integral Garnir straightening and the field-uniform standard basis, not the Robinson-Schensted-Knuth correspondence used in Craven's dimension count (Craven Theorem 2.16, printed pp. 28-31).

  • Dominance. Combining claims 1 and 2 with the dominance part of [F3] shows that the sum in claim 1 is supported on the shapes λ⊵μ: the permutation module Mμ is a direct sum of Specht modules of shapes dominating μ, with Sμ itself occurring exactly once, in agreement with Semistandard maps are independent and respect dominance.

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-10-02Open item page →

Commuting symmetric-group and linear actions on a tensor power

Definition

Let V be a finite-dimensional complex vector space and let n≥0. Write End⁡(V) for the C-vector space of all linear maps V→V, and GL⁡(V)⊆End⁡(V) for the invertible ones (A finite-dimensional representation ρ:G→GL⁡(V) over a field, and its degree). All tensor products below are over C.

The tensor power. For n≥1 fix the parenthesization En  :=  V⊗n  :=  V⊗C⋯⊗CV⏟n factors,V⊗0  :=  C, and write v1⊗⋯⊗vn for the elementary tensor of (v1,…,vn)∈Vn; for n=0 the unique elementary tensor is 1∈C. By Finite iterated tensor products represent multilinear maps independently of parenthesization the assignment (v1,…,vn)↦v1⊗⋯⊗vn is C-multilinear and every element of En is a finite C-linear combination of elementary tensors; for n=0 this means c=c⋅1 for c∈C. If e1,…,ed is a C-basis of V, then by iterating The elementary tensors of two bases form the product basis of the tensor product the dn tensors ei1⊗⋯⊗ein form a C-basis of En, so En is finite-dimensional.

Place permutations: the left Sn-action. Let Sn be the symmetric group of the set {1,…,n} (The symmetric group Sym⁡(X): the bijections of a set X under composition). For σ∈Sn define, on elementary tensors, σ⋅(v1⊗⋯⊗vn)  :=  vσ−1(1)⊗⋯⊗vσ−1(n). The right-hand side depends C-multilinearly on (v1,…,vn), so by the universal property in Finite iterated tensor products represent multilinear maps independently of parenthesization there is a unique C-linear map En→En with this value on every elementary tensor. Uniqueness is what makes the rule well defined on all of En, since the elementary tensors span. The identity permutation acts trivially, and for σ,τ∈Sn and every elementary tensor, (στ)⋅(v1⊗⋯⊗vn)=v(στ)−1(1)⊗⋯⊗v(στ)−1(n)=vτ−1(σ−1(1))⊗⋯⊗vτ−1(σ−1(n)), while τ⋅(v1⊗⋯⊗vn)=vτ−1(1)⊗⋯⊗vτ−1(n) and hence σ⋅(τ⋅(v1⊗⋯⊗vn))=vτ−1(σ−1(1))⊗⋯⊗vτ−1(σ−1(n)). The two agree, so the assignments constitute a left action of the group Sn on En; equivalently En is a left module over Sn (A finite-dimensional representation ρ:G→GL⁡(V) over a field, and its degree). For n=0 the group S0 is trivial and acts on E0=C by the identity.

Diagonal linear action. For g∈GL⁡(V) define, on elementary tensors, g⊗n⋅(v1⊗⋯⊗vn)  :=  gv1⊗⋯⊗gvn, again first on elementary tensors by multilinearity and then uniquely on En. Since g and h are linear, the two assignments compose in the expected way: on elementary tensors, (gh)⊗n⋅(v1⊗⋯⊗vn)=g(hv1)⊗⋯⊗g(hvn)=g⊗n⋅(h⊗n⋅(v1⊗⋯⊗vn)), and (idV)⊗n is the identity. In particular (g−1)⊗n is the inverse of g⊗n. For n=0 every diagonal operator is the identity on C. Thus g↦g⊗n is a group homomorphism GL⁡(V)→GL⁡(En), that is, a finite-dimensional representation of the group GL⁡(V) on En.

The two actions commute. For σ∈Sn, g∈GL⁡(V) and an elementary tensor, σ⋅(g⊗n⋅(v1⊗⋯⊗vn))=gvσ−1(1)⊗⋯⊗gvσ−1(n)=g⊗n⋅(σ⋅(v1⊗⋯⊗vn)), so the two linear maps σ⋅(−) and g⊗n⋅(−) commute; equivalently, every g⊗n is an Sn-equivariant endomorphism of En (Intertwiners, the spaces Hom⁡G(V,W) and End⁡G(V), equivalent representations, and faithful representations).

The diagonal infinitesimal operator. For T∈End⁡(V) put Δ(T)  :=  ∑i=1n1⊗(i−1)⊗T⊗1⊗(n−i) ∈ End⁡(En), where 1=idV and the sum is 0 for n=0. Each summand lies in End⁡(En), and Δ:End⁡(V)→End⁡(En) is C-linear. It is the first coefficient of the diagonal action along the line t↦1+tT. In this polynomial calculation, (1+tT)⊗n is the tensor power of the endomorphism 1+tT; it agrees with the GL⁡(V) action whenever that endomorphism is invertible. For every t∈C one computes, on elementary tensors, (1+tT)⊗n⋅(v1⊗⋯⊗vn)=∑k=0ntk∑1≤i1<⋯<ik≤nwi1,…,ik,(wi1,…,ik)j={Tvj,j∈{i1,…,ik},vj,otherwise the coefficient of t being Δ(T)⋅(v1⊗⋯⊗vn) (zero when n=0); both sides are polynomials in t with values in the finite-dimensional space En described on a spanning set. Finally let An  :=  the unital C-subalgebra of End⁡(En) generated by {Δ(T):T∈End⁡(V)}; this is the image of the diagonal action of the universal enveloping algebra U(gl(V)) on En, defined here as that generated algebra, with no Lie-theoretic input.

Remarks

  • Why the inverse is in the place action. Using vσ(1)⊗⋯⊗vσ(n) would give a right action, (στ)⋅x=τ⋅(σ⋅x), because then the permutation acts on the positions by i↦σ(i). The convention above is arranged so that Sn acts on the left, which is the direction needed for the permutation-module and Specht-module conventions of this library.

  • Degenerate cases. For n=0, E0=C is the trivial representation of the trivial group S0 and of GL⁡(V), Δ(T)=0 is the empty sum, and A0=C idC is one-dimensional. For n=1, E1=V, the group S1 is trivial, g⊗1=g, and Δ(T)=T; thus A1=End⁡(V). If V=0 then En=0 for n≥1 and E0=C, and all statements below about these spaces remain true with the zero space.

  • Δ is not multiplicative. In general Δ(TT′)≠Δ(T)Δ(T′) for dim⁡V>1: the product expands to include cross terms 1⊗(a−1)⊗T⊗1⊗(b−a−1)⊗T′⊗1⊗(n−b) with a<b, and the commutator relation is [Δ(T),Δ(T′)]=Δ([T,T′]), which is not used below. What is used is that An contains Δ(T) for every T, hence every polynomial in these operators; the centralizer statement that uses this algebra is proved later on this page.

  • No choice. All sums are finite sums over n places and over the finite group Sn, and the multilinear universal property produces the maps directly; no selection principle is used.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-10-02Open item page →

Diagonal tensor operators span the symmetric centralizer

Statement

Let V be a finite-dimensional complex vector space, let n≥0, and let E:=V⊗n carry the left place action of Sn (Commuting symmetric-group and linear actions on a tensor power). Write W:=End⁡(V) and let End⁡Sn(E):={F∈End⁡(E):σF=Fσ for all σ∈Sn} be the centralizer of the action. Then:

  1. (Canonical identification.) The linear map Ψ:W⊗n→End⁡(E) with Ψ(T1⊗⋯⊗Tn)(v1⊗⋯⊗vn)=T1v1⊗⋯⊗Tnvn on elementary tensors is a linear isomorphism, and it is equivariant for the place action of Sn on W⊗n and conjugation F↦σFσ−1 on End⁡(E). Hence Ψ restricts to an isomorphism from the invariant tensors, that is from the image of the symmetrization operator 1n!∑σ∈Snσ on W⊗n (the n-th symmetric tensor power of W), onto End⁡Sn(E).
  2. (Spans.) The subspaces span⁡{T⊗n:T∈W} and span⁡{g⊗n:g∈GL⁡(V)} of W⊗n are both equal to the invariant tensors; equivalently, with Δ(T)=∑i=1n1⊗(i−1)⊗T⊗1⊗(n−i) and An the unital C-subalgebra of End⁡(E) generated by all Δ(T) (the image of the diagonal action of U(gl(V)) as defined there, Commuting symmetric-group and linear actions on a tensor power), End⁡Sn(E)=Ψ(span⁡{T⊗n:T∈W})=Ψ(span⁡{g⊗n:g∈GL⁡(V)})=An.

All statements include n=0, where W⊗0=C and E=C, and the case V=0.

Facts & Assumptions

Given: A finite-dimensional complex vector space V, an integer n≥0, E=V⊗n with its left Sn-action, and W=End⁡(V).

[F1]

σ⋅(v1⊗⋯⊗vn)=vσ−1(1)⊗⋯⊗vσ−1(n) defines a left Sn-action on E by linear maps, E=C for n=0; the diagonal operators Δ(T) and the algebra An are as displayed, with Δ linear in T (Commuting symmetric-group and linear actions on a tensor power).

[F2]

If e1,…,ed is a basis of V, the elementary tensors ea1⊗⋯⊗ean form a basis of E, and for n=0 the single element 1 is a basis of E=C (The elementary tensors of two bases form the product basis of the tensor product, Basis of a vector space: a linearly independent spanning subset; and ordered basis: an injective finite list whose image is a basis).

[F3]

The assignment (v1,…,vn)↦v1⊗⋯⊗vn is multilinear, so linear maps out of E are the same as multilinear maps on Vn (Finite iterated tensor products represent multilinear maps independently of parenthesization).

[F4]

For finite-dimensional V one has dim⁡CEnd⁡(V)=d2 with d=dim⁡CV, and matrix representation relative to bases is a vector-space isomorphism (dim⁡FMm×n(F)=mn and dim⁡FL(V,W)=(dim⁡FV)(dim⁡FW) for finite-dimensional V,W, T↦[T]BC is a vector-space isomorphism L(V,W)≅Mm×n(F)).

[F5]

Every nonzero polynomial over an integral domain of degree m has at most m distinct roots. The characteristic polynomial of −T is χ−T(t)=det⁡(t 1V+T), a monic polynomial of degree d=dim⁡CV; an operator is invertible if and only if its determinant is nonzero (A nonzero polynomial of degree n over an integral domain has at most n distinct roots, The basis-independent characteristic polynomial χT of an endomorphism of a finite-dimensional space, including χT=1 in dimension zero, A finite-dimensional linear operator over a field is invertible if and only if its determinant is nonzero).

[F6]

C is an infinite field.

[F7]

In n variables the elementary symmetric polynomial en is x1⋯xn, with e0=1 for n=0; if n! 1R is a unit in a commutative ring R, then en is a polynomial in the power sums ∑ixik with coefficients in R (The elementary symmetric polynomials e0,e1,…,en, If n! is invertible, then p1,…,pn freely generate the symmetric-polynomial ring).

[F8]

A unital ring homomorphism from a polynomial ring on generators x1,…,xm over a commutative ring R into a commutative R-algebra S exists uniquely with prescribed images of the xi (Universal property of a polynomial ring on an arbitrary family of indeterminates).

Proof

technique · constructive
1.1F1F3constructalgebra

[construct] Fix T1,…,Tn∈W. For fixed (v1,…,vn)∈Vn the assignment Ti↦Tivi is linear in each variable, so (T1,…,Tn)↦T1v1⊗⋯⊗Tnvn is multilinear in the Ti and its values in E are linear in (v1,…,vn) separately in each vi; hence there is a unique linear map Φ(T1,…,Tn)∈End⁡(E) with the displayed value on every elementary tensor by [F3], and Φ is multilinear in the Ti because both sides of every identity are checked on the spanning elementary tensors by [F3]. By the representing property of the tensor product [F3] there is a unique linear Ψ:W⊗n→End⁡(E) with Ψ(T1⊗⋯⊗Tn)=Φ(T1,…,Tn), which is the map of the Statement; in particular Ψ is linear and is given on elementary tensors as displayed. For n=0 one has W⊗0=C and Ψ(1)=idC by the same universal property.

1.2F1algebraconstruct

Let p:=1n!∑σ∈Snσ∈End⁡(W⊗n), a well-defined operator because n!≠0 in C; then p2=p, since each group element occurs n! times in the product sum, and p commutes with the action, since left multiplication permutes the summands. Its image is exactly the invariant subspace (W⊗n)Sn: pX is invariant for every X, and pX=X whenever X is invariant. Thus the invariant tensors are the image of the symmetrization operator. Pure tensors span W⊗n, so their symmetrizations span the image of p. For T1,…,Tn∈W, inclusion-exclusion gives ∑σ∈SnTσ(1)⊗⋯⊗Tσ(n)=∑J⊆{1,…,n}(−1)n−∣J∣(∑j∈JTj)⊗n. Indeed, after expanding the right side, an ordered tensor survives exactly when every index 1,…,n occurs, which in a tensor with n factors means each occurs once. Hence each symmetrized pure tensor is a linear combination of powers T⊗n, and (W⊗n)Sn=span⁡{T⊗n:T∈W}. For n=0 this equality is immediate in W⊗0=C.

1.3F5F6algebra

The two spans of the Statement are equal. One inclusion is clear, since GL⁡(V)⊆W. For the reverse let T∈W and consider the W⊗n-valued polynomial t↦(T+t 1V)⊗n; expanding the tensor power of a sum gives (T+t 1V)⊗n=∑k=0ntkck with c0=T⊗n, so it is a polynomial of degree at most n in t. The function t↦det⁡(t 1V+T) is a monic polynomial of degree d=dim⁡CV by [F5], hence nonzero with at most d roots by [F5], so by [F6] there exist n+1 distinct scalars t1,…,tn+1 with T+ti1V invertible for all i by [F5] (if d=0 then W={0} and T=0 is invertible, so any distinct scalars work). For the Lagrange polynomials Li(t):=∏j≠i(t−tj)/(ti−tj) one has tk=∑itikLi(t) for every t and every 0≤k≤n, because it holds at the n+1 distinct points and both sides have degree at most n; multiplying by ck and summing gives T⊗n=c0=∑iLi(0) (T+ti1V)⊗n∈span⁡{g⊗n:g∈GL⁡(V)}. Hence the two spans are equal.

2.1F2F4step 1.1constructalgebra

The matrix units of W with respect to a basis e1,…,ed of V form a basis of W: define Eab∈W by Eabec:=δbcea; every S∈W satisfies S=∑a,bsabEab with sab the coefficients in S(eb)=∑asabea, because the two sides agree on each basis vector of V, and a relation ∑a,bλabEab=0 evaluated at eb gives ∑aλabea=0, so all λab=0. Likewise the endomorphisms fab of E defined by fab(ec1⊗⋯⊗ecn):=δb1c1⋯δbncn ea1⊗⋯⊗ean for words a,b∈[d]n form a basis of End⁡(E), indexed by the finite set [d]n×[d]n; for n=0 this is the single endomorphism idC of the one-dimensional space C, and for d=0 and n≥1 all these sets of words are empty and both spaces are zero. By [F2] and [F3] the d2n tensors Ea1b1⊗⋯⊗Eanbn form a basis of W⊗n, and Ψ sends such a tensor to fab by the formula of step 1.1; a linear map that carries a basis bijectively onto a basis is an isomorphism, so Ψ is a linear isomorphism.

2.2F1F2step 1.1algebra

Ψ is Sn-equivariant for the place action on W⊗n and conjugation on End⁡(E): for σ∈Sn and T1,…,Tn∈W the place action gives σ⋅(T1⊗⋯⊗Tn)=Tσ−1(1)⊗⋯⊗Tσ−1(n) by [F1], so by step 1.1 both Ψ(σ⋅(T1⊗⋯⊗Tn)) and σΨ(T1⊗⋯⊗Tn)σ−1 map v1⊗⋯⊗vn to Tσ−1(1)v1⊗⋯⊗Tσ−1(n)vn; two linear maps agreeing on the spanning elementary tensors agree, so the identity Ψ(σ⋅X)=σΨ(X)σ−1 holds for all X∈W⊗n by linearity.

2.3F1F7F8step 1.1algebra

For T∈W one has Ψ(T⊗n)∈An. For n=0 this is idC∈A0, since A0 is unital. Assume n≥1 and put Ti:=1⊗(i−1)⊗T⊗1⊗(n−i)∈End⁡(E) for 1≤i≤n; these operators commute pairwise and Ψ(T⊗n)=T1T2⋯Tn, while ∑i=1nTik=Δ(Tk) for every k≥1, all by the tensor formula of step 1.1 and [F1]. By [F7] with R=C (where n! is a unit) there is a polynomial Q in n variables over C with en(x1,…,xn)=Q(p1,…,pn) in C[x1,…,xn], where pk=∑ixik. The operators T1,…,Tn commute, so the C-subalgebra they generate is commutative, and the universal property of the polynomial ring [F8] gives a C-algebra homomorphism sending xi↦Ti; it sends en(x1,…,xn) to T1⋯Tn by [F7] and pk to Δ(Tk), so T1⋯Tn=Q(Δ(T),…,Δ(Tn))∈An, since each Δ(Tk) lies in the generating algebra An and Q has coefficients in C.

3.1F1step 1.1step 2.2algebra

For T∈W put dT:=∑i=1n1⊗(i−1)⊗T⊗1⊗(n−i)∈W⊗n (the empty sum for n=0, giving dT=0∈C). Then Ψ(dT)=Δ(T) by step 1.1, and dT is invariant under the place action: a permutation sends the i-th summand, which has T in position i, to the same kind of summand with T in position σ(i) by [F1], and σ permutes the index set, so σ⋅dT=dT. By the equivariance of step 2.2, Δ(T)=Ψ(dT) is fixed by conjugation by every σ∈Sn, that is Δ(T)∈End⁡Sn(E); since End⁡Sn(E) is closed under addition and composition and An is generated by the Δ(T), this gives An⊆End⁡Sn(E).

4.1F1step 2.1step 2.2step 1.2step 3.1step 1.3step 2.3discharge-construct∎

Combining steps: Ψ induces a bijection from (W⊗n)Sn onto End⁡Sn(E) by step 2.2 and step 2.1, the invariant subspace is span⁡{T⊗n}=span⁡{g⊗n} by steps 1.2 and 1.3, and Ψ(span⁡{T⊗n})⊆An⊆End⁡Sn(E) by steps 3.1 and 2.3, so all four subspaces of the Statement coincide. For n=0: W⊗0=E=C, Ψ is the identity, S0 is trivial, T⊗0=1 for every T, Δ(T)=0 and A0=C idC, and the displayed chain reads C=C=C=C. For V=0 and n≥1: W=0, E=0, both sides of the identity are the zero space, and An=0. This proves both claims.

Remarks

  • What is used where. The basis argument of step 2.1 identifies End⁡(V⊗n) with W⊗n; steps 1.2 and 1.3 are the polarization step, expressing an arbitrary invariant tensor through the powers T⊗n and then through powers of invertible operators; step 2.3 is the Newton-identity argument identifying the algebra generated by the place operators Δ(T) with those powers. The interpolation in step 1.3 is where the field C is used as an infinite field of characteristic zero; the statement is false in characteristic p≤n, where n! is not invertible.

  • The zero and empty cases. For n=0 the symmetric tensor power is the ground field and the whole claim degenerates to C=C; for V=0 and n≥1 both E and W⊗n are the zero space, so End⁡Sn(E)=An=0. These are the only cases in which the basis argument of step 2.1 has no words a,b.

  • Relation to the double centralizer. The equality End⁡Sn(E)=An identifies the commutant of the C[Sn]-image with the image of the diagonal gl(V)-action. The converse commutant equality is the other half of the double-centralizer statement proved on this page (Commuting symmetric-group and linear actions on a tensor power).

  • No choice. All bases, matrix units and the finitely many scalars t1,…,tn+1 are chosen from explicit finite or countable ranges; the multilinear universal property of [F3] produces the maps without any selection, and no selection principle is used.

TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-10-02Open item page →

The Schur-Weyl mutual centralizer theorem on tensor powers

Statement

Let V be a finite-dimensional complex vector space, let n≥0, and let E:=V⊗n carry the left place action of Sn (Commuting symmetric-group and linear actions on a tensor power). Let A be the image of the algebra homomorphism C[Sn]→End⁡(E) extending the place action, and let B:=span⁡C{g⊗n:g∈GL⁡(V)} be the linear span of the diagonal operators g⊗n(v1⊗⋯⊗vn)=gv1⊗⋯⊗gvn. Then:

  1. (Mutual centralizers.) B={F∈End⁡(E):Fa=aF for all a∈A} and A={F∈End⁡(E):Fb=bF for all b∈B}.
  2. (Uniqueness of the identification.) B is a unital C-subalgebra of End⁡(E) and equals the image of the diagonal action of the universal enveloping algebra U(gl(V)), that is the unital subalgebra generated by the operators Δ(T)=∑i=1n1⊗(i−1)⊗T⊗1⊗(n−i), T∈End⁡(V) (Diagonal tensor operators span the symmetric centralizer).

All statements include n=0, where E=C.

Facts & Assumptions

Given: a finite-dimensional complex vector space V, an integer n≥0, E=V⊗n with its left Sn-action, the algebra A and the space B of the Statement.

[F1]

The left place action of Sn on E and the diagonal action of g∈GL⁡(V) commute, and Δ(T)=∑i=1n1⊗(i−1)⊗T⊗1⊗(n−i) is linear in T (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 [T,U]=TU−UT, so [Δ(T),Δ(U)]=Δ([T,U]).

[F2]

The map Ψ:(End⁡V)⊗n→End⁡(E) is a linear isomorphism, equivariant for the place action and conjugation, and End⁡Sn(E)=Ψ(span⁡{T⊗n:T∈End⁡(V)})=Ψ(span⁡{g⊗n:g∈GL⁡(V)})=An, where End⁡Sn(E) is the centralizer of the place action and An is the unital subalgebra generated by the Δ(T), which is the image of the diagonal action of U(gl(V)) (Diagonal tensor operators span the symmetric centralizer).

[F3]

Every finite-dimensional C[Sn]-module is completely reducible (Maschke's theorem for finite groups over fields whose characteristic does not divide ∣G∣).

[F4]

The modules {Sλ:λ⊢n} form a complete irredundant list of the finite-dimensional irreducible complex Sn-representations (Specht modules classify the complex irreducibles of Sn).

[F5]

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 End⁡G(V) is a division ring, Over an algebraically closed field, every endomorphism of an irreducible representation is scalar).

[F6]

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 S and an S-isotypical module U, evaluation S⊗Hom⁡Sn(S,U)→U, s⊗f↦f(s), is an isomorphism under which every Sn-map U→U′ is uniquely of the form EU′(1S⊗a)EU−1 for a linear a:Hom⁡Sn(S,U)→Hom⁡Sn(S,U′), with Hom⁡-spaces carrying the trivial action and composition preserved (The isotypic decomposition of a completely reducible representation is unique, Isotypical evaluation and multiplicity subspaces).

[F7]

C[Sn]≅∏i=1rMni(C) for positive integers ni, and the simple left modules over such a product are the column modules Cni, one isomorphism class per factor, each supported on exactly one factor (If k is algebraically closed and char⁡k∤∣G∣, then k[G]≅∏i=1rMni(k), Simple modules over a product of matrix rings over division rings).

[F8]

Under the correspondence between k-linear G-actions and compatible left k[G]-module structures, the subrepresentations of a representation V are exactly the k[G]-submodules and V is irreducible if and only if it is simple as a k[G]-module; G-equivariant maps are exactly the k[G]-module homomorphisms (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).

Proof

technique · direct
1.1F1givenconstructalgebra

[construct] Recall that A is a unital subalgebra of End⁡(E), because it is the image of a unital algebra homomorphism, and that B is a unital subalgebra, because g⊗nh⊗n=(gh)⊗n for g,h∈GL⁡(V); both contain 1E (for B take g=1V, and for n=0 note g⊗0=idC for every g and GL⁡(V) is nonempty).

1.2F3F4F6constructalgebra

By [F3] the C[Sn]-module E is completely reducible, so by [F4] and the uniqueness of the isotypic decomposition in [F6] there are subspaces Eλ for λ in the finite set Λ:={λ⊢n:Hom⁡Sn(Sλ,E)≠0} with E=⨁λ∈ΛEλ, each Eλ is λ-isotypical, and the evaluation maps of [F6] give Sn-isomorphisms Eλ≅Sλ⊗Mλ with Mλ:=Hom⁡Sn(Sλ,E) carrying the trivial action; consequently the action of σ∈Sn on Eλ corresponds to ρλ(σ)⊗1Mλ, where ρλ is the action on the irreducible Sλ.

1.3F4F7F8algebra

The simple left C[Sn]-modules are, by [F7], the column modules of the factors of a decomposition C[Sn]≅∏i=1rMni(C), one class per factor and each supported on one factor; by [F8] the irreducible complex representations of the group Sn are exactly the simple left C[Sn]-modules, so by [F4] the isomorphism classes of simple left C[Sn]-modules are exactly the classes [Sλ], λ⊢n. Hence the factors are indexed by the partitions of n, with ni=dim⁡CSλ for the factor attached to λ, and dim⁡CC[Sn]=∑λ⊢n(dim⁡CSλ)2.

1.4constructalgebra

An endomorphism T∈End⁡(S⊗M) of a tensor product, S,M finite-dimensional over C with M≠0, commuting with 1S⊗b for all b∈End⁡(M) is of the form T=x⊗1M for a unique x∈End⁡(S): choose bases s1,…,sp of S and m1,…,mq of M (both finite, with q≥1), write T(s⊗m1)=∑j=1qxj(s)⊗mj with well-defined linear maps xj:S→S; for each j let bj∈End⁡(M) be given on the basis by bj(m1)=mj and bj(mi)=0 for i≥2; then T(s⊗mj)=T((1⊗bj)(s⊗m1))=(1⊗bj)T(s⊗m1)=x1(s)⊗mj, so T=x1⊗1M on all basis vectors, and conversely every x⊗1M commutes with the operators 1⊗b.

2.1F2step 1.1algebra

The first displayed identity of claim 1 holds: a map F∈End⁡(E) commutes with every a∈A exactly when it commutes with σ for every σ∈Sn, because A is the linear span of the place operators σ; hence the centralizer of A is End⁡Sn(E), which equals B by [F2]. The same fact of [F2] identifies B with the image of the diagonal action of U(gl(V)), so claim 2 holds; in particular B is a subalgebra, in agreement with step 1.1.

2.2F7F8step 1.3constructalgebra

The canonical algebra homomorphism Φ:C[Sn]→∏λ⊢nEnd⁡(Sλ), Φ(x)=(ρλ(x))λ, is an isomorphism. It is injective: if x acts as 0 on every Sλ, then under the product decomposition of step 1.3 the element x has a component in each factor which annihilates that factor's own column module, and so is 0, so x=0; here [F8] identifies the column module of the factor attached to λ with the simple module Sλ, on which x acts as ρλ(x) by definition of Φ. It is then bijective because, by step 1.3 and dim⁡CEnd⁡(Sλ)=(dim⁡CSλ)2, source and target have the same finite dimension ∑λ⊢n(dim⁡CSλ)2.

3.1F4F5F6step 2.1step 1.2algebra

The algebra End⁡Sn(E) is ∏λ∈ΛEnd⁡(Mλ): an Sn-endomorphism of E maps each isotypic component Eλ into itself, since the image of a copy of Sλ is 0 or a copy of Sλ by [F5] and [F4]; on Eλ it is, by [F6] and step 1.2, exactly the operator induced by a unique aλ∈End⁡(Mλ) on the second tensor factor; maps between distinct components Eλ→Eμ are zero by [F5] and [F4] because Sλ and Sμ are non-isomorphic for λ≠μ; and the identifications preserve composition, so this is an algebra isomorphism under which aλ corresponds to the operator 1Sλ⊗aλ on Eλ. In particular, by step 2.1, B is exactly the set of operators ⨁λ∈Λ(1Sλ⊗bλ) with bλ∈End⁡(Mλ).

3.2step 1.2step 2.2algebra

Under the isomorphism Φ of step 2.2 and the isomorphisms Eλ≅Sλ⊗Mλ of step 1.2, the action of x∈C[Sn] on E=⨁λ∈ΛEλ is ⨁λ∈Λ(ρλ(x)⊗1Mλ), the factors with λ∉Λ acting on no summand; hence the image A of this action map is exactly A=⨁λ∈Λ(End⁡(Sλ)⊗1Mλ)⊆End⁡(E), the direct sum of the indicated block subalgebras indexed by Λ: indeed the projection ∏λ⊢nEnd⁡(Sλ)→∏λ∈ΛEnd⁡(Sλ) is surjective and Φ is an isomorphism.

4.1F6step 1.2step 3.1algebra

Claim 1's second identity holds. Let F∈End⁡(E) commute with every element of B; decompose F as a block matrix (Fμλ)μ,λ∈Λ with Fμλ∈Hom⁡(Sλ⊗Mλ,Sμ⊗Mμ) using the decomposition of step 1.2. Commuting with the operator 1Sλ⊗bλ on the λ-block and 1Sμ⊗bμ on the μ-block gives Fμλ(1Sλ⊗bλ)=(1Sμ⊗bμ)Fμλ. If μ≠λ, use bλ=1Mλ, bμ=0 (available in B by step 3.1 and λ,μ∈Λ), obtaining Fμλ=0. Thus every off-diagonal block vanishes. For each λ, the diagonal block Fλλ commutes with 1Sλ⊗b for every b∈End⁡(Mλ), since B contains the operators supported on that single block by step 3.1.

5.1step 3.2step 4.1step 1.4algebra

By steps 4.1 and 1.4 the centralizer of B consists exactly of the elements ⨁λ∈Λ(xλ⊗1Mλ) with xλ∈End⁡(Sλ), which is exactly A by step 3.2; this proves the second identity of claim 1, and claim 2 was proved in step 2.1.

6.1F2F6step 1.2step 4.1step 1.4given∎

Boundary and choice audit. For n=0 one has E=V⊗0=C, A=B=C idC=End⁡(E) and both centralizers equal the whole of End⁡(E), in agreement with claims 1 and 2; the case is covered by the argument with Λ={(∅)} when Hom⁡S0(S∅,C)=C. For V=0 and n≥1 one has E=0, so End⁡(E)=0=A=B by [F2] and all assertions hold; here Λ=∅, the products over Λ are the zero algebra, and steps 4.1 and 1.4 are vacuous. For V≠0 and n≥1, every λ∈Λ has Mλ≠0 by definition, so step 1.4 applies with M=Mλ. All bases and decompositions used are attached to finite-dimensional spaces and to the finitely many partitions of n; the decomposition of E and the factors of C[Sn] are canonical, and no choice principle is invoked.

Remarks

  • Two halves, two mechanisms. The identity End⁡A(E)=B is the polarization lemma (Diagonal tensor operators span the symmetric centralizer), a direct computation with symmetric tensors. The reverse identity End⁡B(E)=A goes through the semisimple structure of C[Sn]: the isotypic decomposition of E makes both centralizers products of full matrix algebras, and the two products are exchanged by the evaluation isomorphism (Isotypical evaluation and multiplicity subspaces).

  • No Lie machinery is imported. The only Lie-theoretic input is the identification of B with the image of the diagonal U(gl(V))-action, which is proved inside Diagonal tensor operators span the symmetric centralizer by Newton identities; no classification or highest-weight theory is used here.

  • What the theorem does not say. Nothing is asserted about the multiplicity spaces Mλ 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.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-10-02Open item page →

Column antisymmetrization gives the exact Schur–Weyl length cutoff

Statement

Let V be a finite-dimensional complex vector space of dimension d, let n≥0, and let E:=V⊗n with the left place action of Sn of Commuting symmetric-group and linear actions on a tensor power. For every λ⊢n, Hom⁡Sn(Sλ,E)≠0⟺ℓ(λ)≤d, where ℓ(λ) is the number of nonzero rows of λ and Sλ⊆Mλ is the complex Specht module (Column antisymmetrizers, polytabloids, and Specht modules). Equivalently, the complex irreducible Sn-module Sλ occurs in V⊗n exactly for the partitions of n with at most d rows.

Facts & Assumptions

Given: a finite-dimensional complex vector space V of dimension d, an integer n≥0, a partition λ⊢n, and the module E=V⊗n with its left Sn-action.

[F1]

σ⋅(v1⊗⋯⊗vn)=vσ−1(1)⊗⋯⊗vσ−1(n) defines a left Sn-action on E with E=V⊗n finite-dimensional and E=C for n=0 (Commuting symmetric-group and linear actions on a tensor power).

[F2]

Mλ is free with the λ-tabloids as basis, et=κt⋅{t} with κt=∑γ∈Ctsgn⁡(γ)γ, Sλ is the span of the polytabloids, Ct∩Rt={1}, and eσ⋅t=σ⋅et, γ⋅et=sgn⁡(γ)et for γ∈Ct (Column antisymmetrizers, polytabloids, and Specht modules, Polytabloid covariance and the column sign rule).

[F3]

Sλ is a nonzero irreducible C[Sn]-module, and Sλ is generated by et for any single λ-tableau t (Complex Specht modules are irreducible, Polytabloid covariance and the column sign rule).

[F4]

Rt and Ct preserve each row set and each column set of t respectively, and the row stabilizer of the tabloid {t} is Rt; every λ-tabloid is σ⋅{t} for some σ∈Sn, and Ct=∏jSBj over the disjoint column label sets Bj (Row and column stabilizers, Young subgroups, tabloids, and permutation modules).

[F5]

If e1,…,ed is a basis of V, the elementary tensors ea1⊗⋯⊗ean form a basis of E, so distinct such tensors are linearly independent; ℓ(λ)=λ1′ is the height of the first column of [λ] (The elementary tensors of two bases form the product basis of the tensor product, Basis of a vector space: a linearly independent spanning subset; and ordered basis: an injective finite list whose image is a basis, Partitions, English diagrams, and conjugation).

[F6]

sgn⁡ is multiplicative and sgn⁡((ab))=−1 for a transposition (The sign is a homomorphism Sn→{+1,−1}, surjective exactly when n≥2).

Proof

technique · constructive
1.1givenF1F4F5constructalgebra

[construct] Assume ℓ(λ)≤d and fix a λ-tableau t and a basis e1,…,ed of V. Let wt∈E be the tensor with factor ei in every place labelled by an entry of row i of t, that is, the place carrying label a holds er(a), where r(a) is the row of the box of t containing a; define Φ(σ⋅{t}):=σ⋅wt for σ∈Sn and extend linearly. If ρ∈Rt, then ρ permutes only the places inside each row of t, all of which carry the same basis vector, so ρ⋅wt=wt; hence, since the stabilizer of {t} is Rt and every tabloid is σ⋅{t} by [F4], Φ is a well-defined C-linear map Mλ→E, and it is Sn-linear by construction.

1.2givenF4F5F6algebra

Conversely, assume ℓ(λ)>d, and let Z be the set of labels in the first column of a λ-tableau t, so ∣Z∣=λ1′=ℓ(λ)>d by [F4, F5]. Let AZ:=∑z∈SZsgn⁡(z)z, acting on E through place permutations. Then AZ annihilates E: it suffices by linearity and [F5] to check this on a basis tensor w=ea1⊗⋯⊗ean, where the place carrying label a holds eaa for basis indices aa∈{1,…,d}. Since ∣Z∣>d, two labels a≠b of Z carry the same basis vector, so the transposition τ=(ab) fixes w. Choose representatives k for the right cosets k⟨τ⟩ in SZ. By [F6], AZ=∑ksgn⁡(k)k(1−τ), and therefore AZw=0.

2.1givenF2F4F5step 1.1algebra

For γ∈Ct, the tensor γ⋅wt has at the place carrying label a the factor er(γ−1(a)), so γ⋅wt=wt holds exactly when γ−1 maps every row set of t to itself, that is, exactly when γ∈Rt; since Ct∩Rt={1} by [F2], the tensors γ⋅wt, γ∈Ct, are pairwise distinct, and the coefficient of wt in κt⋅wt=∑γ∈Ctsgn⁡(γ) γ⋅wt is the coefficient of the single term γ=1, namely 1. By [F5] and [F2], Φ(et)=Φ(κt⋅{t})=κt⋅wt≠0.

2.2givenF2F3F4F6step 1.2algebra

Write B1,…,Br for the column label sets of t. By [F4], Ct=∏jSBj is the direct product over disjoint supports, so with ABj:=∑z∈SBjsgn⁡(z)z the multiplicativity of the sign [F6] gives κt=AB1AB2⋯ABr in C[Sn]; here B1=Z. Since AB1 annihilates E by step 1.2 and the operators commute, κt acts as the zero operator on E. Also κt⋅et=∑γ∈Ctsgn⁡(γ) γ⋅et=∑γ∈Ctet=∣Ct∣et by [F2], so et=∣Ct∣−1κt⋅et with ∣Ct∣≠0 in C. If f:Sλ→E is Sn-linear, then f(et)=∣Ct∣−1f(κt⋅et)=∣Ct∣−1κt⋅f(et)=0; since et generates Sλ by [F3], f=0. Hence Hom⁡Sn(Sλ,E)=0 when ℓ(λ)>d.

3.1givenF2F3step 1.1step 2.1algebra

The restriction Φ∣Sλ:Sλ→E is a map of Sn-modules, because Sλ⊆Mλ is an Sn-submodule and Φ is Sn-linear by step 1.1; it is nonzero at et by step 2.1. Its kernel is a proper Sn-submodule of Sλ, hence zero because Sλ is irreducible by [F3]; therefore Φ∣Sλ is injective and Hom⁡Sn(Sλ,E)≠0 when ℓ(λ)≤d.

4.1givenF1F3step 2.2step 3.1discharge-construct∎

Steps 3.1 and 2.2 prove the equivalence for n≥1; for n=0 we have λ=∅, ℓ(λ)=0≤d, S∅=C=E and Hom⁡(C,C)≠0, in agreement. If d=0 and n≥1 then E=0, so every homomorphism into E is zero, and indeed ℓ(λ)≥1>0=d; if d=0 and n=0 the previous case applies. This proves the claimed equivalence in all cases.

Remarks

  • Where irreducibility and nonvanishing are used. The forward direction uses irreducibility of Sλ only to convert a nonzero map into an injection, and uses the nonvanishing of κtwt to produce that map; the reverse direction uses ∣Ct∣≠0 in C, so it does not survive in characteristic p≤n, where the corresponding multiplicity question is a modular branching question treated elsewhere.

  • Interpretation. For λ=(n) and λ=(1n) the cutoff requires 1≤d and n≤d; the corresponding multiplicity factors below are the symmetric and exterior powers of V, of dimensions (n+d−1n) and (dn), and the second vanishes exactly when n>d.

  • No choice. The basis of V, the tableau t and the tensor wt are fixed explicitly, and Z is a finite set; no selection principle is used.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-10-02Open item page →

The row-labelled polytabloid map has highest weight lambda

Statement

Let V be a finite-dimensional complex vector space of dimension d≥0 with a fixed basis e1,…,ed, let n≥0, and let λ⊢n with ℓ(λ)≤d. For 1≤i,j≤d let Eij∈End⁡(V) be the matrix unit with Eijej=ei and Eijek=0 for k≠j. Fix a λ-tableau t and endow V⊗n with the left place action of Sn and the diagonal action of GL⁡(V) of Commuting symmetric-group and linear actions on a tensor power, so that Δ(X)=∑a=1n1⊗(a−1)⊗X⊗1⊗(n−a) for X∈End⁡(V). Put Mλ:=Hom⁡Sn(Sλ,V⊗n), on which GL⁡(V) acts by (g⋅ψ)(s):=g⊗nψ(s) and the algebra B:=span⁡C{g⊗n:g∈GL⁡(V)} acts by postcomposition b⋅ψ:=b∘ψ.

Let wt∈V⊗n be the elementary tensor whose place labelled a carries er(a), where r(a) is the row of the box of t containing a, and let Φ:Mλ→V⊗n be the row-labelled map Φ(σ⋅{t}):=σ⋅wt of Column antisymmetrization gives the exact Schur–Weyl length cutoff. Then φ:=Φ∣Sλ∈Mλ is nonzero, and, writing λi:=0 for i>ℓ(λ), the following hold.

  1. (Weight λ.) For every diagonal g=diag⁡(x1,…,xd)∈GL⁡(V) one has g⊗n∘φ=xλφ, where xλ:=x1λ1⋯xdλd; equivalently Δ(Eii)∘φ=λiφ for every i. Thus φ is a vector of weight (λ1,…,λd) in the multiplicity space Mλ.
  2. (Highest weight vector.) Δ(Eij)∘φ=0 for all 1≤i<j≤d: the map φ is killed by every upper-triangular raising matrix unit.
  3. (Uniqueness.) If Mλ is irreducible as a module over B by postcomposition, then every nonzero ψ∈Mλ with Δ(Eij)∘ψ=0 for all i<j and Δ(Eii)∘ψ=μiψ for all i, for some scalars μ1,…,μd, satisfies μi=λi for every i and lies in Cφ; that is, λ is then the unique highest weight of Mλ, and its highest weight vector is unique up to a scalar.

Facts & Assumptions

Given: a finite-dimensional complex vector space V with basis e1,…,ed (d=dim⁡CV≥0), an integer n≥0, a partition λ⊢n with ℓ(λ)≤d, a λ-tableau t, the matrix units Eij, the permutation module Mλ with its Specht submodule Sλ, and V⊗n with its place and diagonal actions.

[F1]

The rule σ⋅(v1⊗⋯⊗vn)=vσ−1(1)⊗⋯⊗vσ−1(n) defines a left action of Sn on V⊗n by linear maps, g⊗n(v1⊗⋯⊗vn)=gv1⊗⋯⊗gvn defines a representation of GL⁡(V), the operators g⊗n commute with every place permutation, Δ(X)=∑a=1n1⊗(a−1)⊗X⊗1⊗(n−a) is C-linear in X and equals 0 when n=0, and V⊗0=C (Commuting symmetric-group and linear actions on a tensor power).

[F2]

The dn elementary tensors ea1⊗⋯⊗ean with a1,…,an∈{1,…,d} form a basis of V⊗n; in particular distinct elementary tensors are linearly independent (The elementary tensors of two bases form the product basis of the tensor product, Basis of a vector space: a linearly independent spanning subset; and ordered basis: an injective finite list whose image is a basis).

[F3]

The λ-tabloids form a basis of Mλ, et=κt{t} with κt=∑γ∈Ctsgn⁡(γ)γ, Sλ is the span of the polytabloids, Ct∩Rt={1}, et≠0, γ⋅et=sgn⁡(γ)et for γ∈Ct, and eσ⋅t=σ⋅et (Column antisymmetrizers, polytabloids, and Specht modules, Polytabloid covariance and the column sign rule).

[F4]

Sλ is a nonzero irreducible C[Sn]-module and is generated by et, that is, Sλ=span⁡C{σ⋅et:σ∈Sn} (Complex Specht modules are irreducible, Polytabloid covariance and the column sign rule).

[F5]

Every λ-tabloid is σ⋅{t} for some σ∈Sn, and the stabilizer of {t} in Sn is the row stabilizer Rt (Young subgroups, tabloids, and permutation modules).

[F6]

With Bt:={t(i,j):1≤i≤λj′} the column set of column j, one has Ct=S(B1)×⋯×S(Bλ1) and Rt=S(A1)×⋯×S(Ak) for the row sets Ai; the boxes of column j of the diagram of λ are exactly the pairs (i,j) with i≤λj′, and ℓ(λ)=λ1′ (Row and column stabilizers, Partitions, English diagrams, and conjugation, Tableaux and standard tableaux).

[F7]

B=span⁡C{g⊗n:g∈GL⁡(V)} is a unital C-subalgebra of End⁡(V⊗n), it equals the centralizer End⁡Sn(V⊗n)={F:Fa=aF for all a in the image A of C[Sn]} of the place action, and it equals the unital subalgebra generated by {Δ(X):X∈End⁡(V)} (The Schur-Weyl mutual centralizer theorem on tensor powers).

[F8]

Eigenvectors of an endomorphism belonging to pairwise distinct eigenvalues are linearly independent (Eigenvectors belonging to pairwise distinct eigenvalues are linearly independent).

[F9]

The sign sgn⁡ is multiplicative and sgn⁡((ab))=−1 for every transposition (ab) (The sign is a homomorphism Sn→{+1,−1}, surjective exactly when n≥2).

Proof

technique · constructive
1.1givenF1F3F5construct

[construct] Let wt:=er(1)⊗⋯⊗er(n)∈V⊗n be the elementary tensor whose place labelled a carries er(a), and define Φ(σ⋅{t}):=σ⋅wt for σ∈Sn, extended linearly. This is well defined: if σ⋅{t}=σ′⋅{t}, then σ′=σρ with ρ∈Rt, and ρ⋅wt=wt because ρ permutes only the places inside each row of t, all carrying the same factor ei in row i; hence σ′⋅wt=σ⋅wt. As the tabloids form a basis of Mλ and every tabloid is σ⋅{t}, Φ is a well-defined C-linear map, and it is Sn-linear because τ⋅(σ⋅{t})=(τσ)⋅{t} and the place action on V⊗n is a left action.

1.2givenF1constructalgebra

For X∈End⁡(V) and a∈{1,…,n} put Xa:=1⊗(a−1)⊗X⊗1⊗(n−a), so that Δ(X)=∑aXa. For σ∈Sn one has σXaσ−1=Xσ(a): both sides act as X on the place σ(a) and as the identity on the other places. Since a↦σ(a) is a bijection, σΔ(X)σ−1=Δ(X), so Δ(X) commutes with the place action of every element of C[Sn], in particular with κt. Moreover [Δ(X),Δ(Y)]=Δ([X,Y]) for all X,Y∈End⁡(V): summands on distinct places commute, [Xa,Ya]=[X,Y]a, so [Δ(X),Δ(Y)]=∑a[Xa,Ya]=Δ([X,Y]). Finally [Eij,Ekℓ]=δjkEiℓ−δℓiEkj: both sides send em to δℓmδkjei−δjmδiℓek.

1.3givenF1F2F7algebra

Every X∈End⁡(V) has an expansion X=∑i,jcijEij: define cij by Xej=∑icijei, so that the two sides agree on each basis vector. By C-linearity of Δ, every product Δ(X1)⋯Δ(Xm) of diagonal operators is therefore a finite C-linear combination of products of matrix-unit operators Δ(Eij), and by [F7] every element of B is such a combination; so it suffices to run all bookkeeping below on matrix-unit words.

2.1givenF1F2F3F4step 1.1algebra

The tensors γ⋅wt for γ∈Ct are pairwise distinct: γ⋅wt carries er(γ−1(a)) in the place labelled a, so γ⋅wt=wt exactly when γ−1, equivalently γ, preserves every row set of t, that is, exactly when γ∈Rt; and if γ⋅wt=γ′⋅wt, then γ′−1γ∈Ct∩Rt={1}, so γ=γ′. Distinct elementary tensors are linearly independent, and in κt⋅wt=∑γ∈Ctsgn⁡(γ) γ⋅wt the tensor wt occurs only as the term γ=1, with coefficient sgn⁡(1)=1; hence κt⋅wt≠0. Therefore φ(et)=Φ(κt⋅{t})=κt⋅Φ({t})=κt⋅wt≠0, so φ=Φ∣Sλ is a nonzero element of Mλ.

2.2givenF1step 1.1algebra

The place labelled a of wt carries er(a), and Esser(a) equals es if r(a)=s and 0 otherwise; hence Δ(Ess)⋅wt=λswt, because exactly the λs places of row s of t contribute a copy of wt. Likewise, for diagonal g=diag⁡(x1,…,xd), one has g⊗n⋅wt=(∏a=1nxr(a))wt=x1λ1⋯xdλdwt=xλwt, the product collecting one factor xs from each of the λs places of row s and λs=0 for s>ℓ(λ).

2.3givenF3F6F9step 1.1step 1.2algebra

Fix i<j and let Sj:={a:r(a)=j} be the set of places of row j of t. Then Δ(Eij)wt=∑a∈Sjwt(a), where wt(a) is wt with the factor at place a replaced by ei: the operator Eij sends ej to ei and kills every other basis vector. For a∈Sj, let m be its column in t, so that a occupies the box (j,m) with j≤λm′; since i<j≤λm′, the box (i,m) also belongs to the diagram of λ and contains a label b in the same column set Bm as a, so the transposition τ=(ab) lies in Ct, and τ⋅wt(a)=wt(a) because wt(a) carries ei in both places a and b and τ exchanges only these two places. Consequently κtτ=∑γ∈Ctsgn⁡(γ)γτ=∑δ∈Ctsgn⁡(δτ−1)δ=sgn⁡(τ)κt=−κt by [F9] after the reindexing δ=γτ, so κt⋅wt(a)=κtτ⋅wt(a)=−κt⋅wt(a); as 2κt⋅wt(a)=0 over C, we get κt⋅wt(a)=0.

2.4givenF1step 1.2constructalgebra

Every product Δ(Y1)⋯Δ(Yp) of matrix-unit operators Yk=Eikjk with ik≥jk for all k is a product V of non-raising factors; we show that an arbitrary product Δ(Y1)⋯Δ(Yp) of matrix-unit operators is a finite sum ∑cVcRc with every Vc a product of Δ(Eij) with i≥j and every Rc a product of Δ(Eij) with i<j, products of either kind possibly empty. [construct: induction on p, and for fixed p on the number of pairs u<v with Yu raising and Yv non-raising]. If such a pair exists, choose one with v−u minimal; then v=u+1, for if v>u+1 then either Yv−1 is non-raising and (u,v−1) is an earlier pair, or Yv−1 is raising and (v−1,v) is such a pair. Replace the adjacent pair by Δ(Yu)Δ(Yv)=Δ(Yv)Δ(Yu)+Δ([Yu,Yv]) using step 1.2; the first term has the same number p of factors and one fewer pair, while [Yu,Yv]=δjkEiℓ−δℓiEkj by step 1.2 is a linear combination of at most two matrix units. By linearity of Δ, expand the commutator term accordingly; each nonzero resulting word has p−1 factors, so the induction hypothesis on p applies to each, and zero terms are dropped. If no such pair exists, every raising factor already lies to the right of every non-raising factor, so the product is already of the required form V⋅R.

2.5givenstep 1.2constructalgebra

Let x∈Mλ satisfy Δ(Eij)x=0 for all i<j and Δ(Ess)x=νsx for all s, and let V=Δ(Y1)⋯Δ(Yp) be a product of matrix-unit operators with Yk=Eikjk and ik≥jk for all k. Then Vx is either 0 or a weight vector with Δ(Ess)Vx=(ν−α)sVx for all s, where α:=∑k=1p(ejk−eik) is a nonnegative integer combination of the simple vectors e1−e2,…,ed−1−ed. [construct: induction on p]. For p=0 the empty product is the identity and Vx=x has weight ν, with α=0. For p≥1, put W:=Δ(Y2)⋯Δ(Yp)x, which is 0 or a weight vector of weight ν−α′ with α′ nonnegative, by the induction hypothesis; if W=0 then Vx=0, and otherwise, for every s, Δ(Ess)Δ(Y1)W=Δ(Y1)Δ(Ess)W+Δ([Ess,Y1])W by step 1.2, and [Ess,Eij]=δsiEij−δsjEij, so Δ(Ess)Vx=(ν−α′)sVx+(δsi−δsj)Vx=(ν−α)sVx with α=α′+(ej−ei); here i≥j, so ej−ei is 0 or a sum of simple vectors with nonnegative coefficients.

3.1givenF3F4step 1.1step 2.1step 1.2step 2.2algebra

Hence Δ(Ess)∘φ=λsφ for every s, and g⊗n∘φ=xλφ for every diagonal g: both Δ(Ess)∘φ and g⊗n∘φ are Sn-linear (steps 1.1 and 1.2 and [F1]), and at et they take the values Δ(Ess)φ(et)=κtΔ(Ess)wt=λsκtwt=λsφ(et) and g⊗nφ(et)=κtg⊗nwt=xλκtwt=xλφ(et), by steps 1.2 and 2.2 and φ(et)=κtwt; since et generates Sλ [F4], the two Sn-linear maps agree on all of Sλ. This proves claim 1.

3.2givenF4step 1.1step 2.1step 1.2step 2.3algebra

For every i<j one then has Δ(Eij)φ(et)=Δ(Eij)κtwt=κtΔ(Eij)wt=∑a∈Sjκtwt(a)=0, by steps 1.2 and 2.3 and φ(et)=κtwt. If j>ℓ(λ) then Sj=∅ and the same computation gives 0; if j≤ℓ(λ) the sum is over the λj places of row j and step 2.3 applies to each. Since Δ(Eij)φ is Sn-linear (step 1.2) and et generates Sλ [F4], Δ(Eij)∘φ=0. This proves claim 2.

3.3givenstep 2.5algebra

In the situation of step 2.5, let ws:=d+1−s, put H:=Δ(diag⁡(w1,…,wd))=∑swsΔ(Ess), and let ht⁡(α):=∑k=1p(ik−jk). If Vx≠0, then HVx=(⟨w,ν⟩−ht⁡(α))Vx with ⟨w,ν⟩:=∑swsνs; moreover ht⁡(α)≥0, and ht⁡(α)=0 if and only if α=0, if and only if every Yk is diagonal, in which case Vx=ν1m1⋯νdmdx∈Cx, where ms is the number of indices k with Yk=Ess. Indeed wj−wi=i−j for all i,j, so ⟨w,α⟩=∑k(wjk−wik)=ht⁡(α), and ht⁡(α)=0 with ik≥jk forces ik=jk for every k; a product of diagonal factors Δ(Ess) then acts on x by the scalar νs, once per factor.

4.1givenF7step 1.3step 2.4step 2.5step 3.3algebra

In the situation of step 2.5 and for arbitrary b∈B, the element y:=b⋅x can be written as a finite sum y=∑e≥0ye indexed by integers e, where each ye is 0 or an eigenvector of H with Hye=(⟨w,ν⟩−e)ye, and y0∈Cx. Indeed, by steps 1.3 and 2.4 the element y is a finite sum ∑cVcRcx with each Vc a non-raising and each Rc a raising product of matrix-unit operators; if Rc is nonempty then its rightmost factor is some Δ(Eij) with i<j, so Rcx=0; hence y=∑c: Rc emptyVcx, and grouping the finitely many remaining terms by the value e=ht⁡(αc)≥0 from step 3.3 gives the ye, the e=0 part lying in Cx by step 3.3.

5.1givenF8step 4.1algebra

In the situation of step 4.1, suppose in addition that y≠0 is an eigenvector of H with Hy=Ey. Then E=⟨w,ν⟩−e for some e≥0 with ye≠0; in particular ⟨w,ν⟩−E∈Z≥0, and if E=⟨w,ν⟩ then y∈Cx. Indeed the set Z:={e:ye≠0} is finite and nonempty; if E∉{⟨w,ν⟩−e:e∈Z}, then the nonzero members of {y}∪{ye:e∈Z} are eigenvectors of H with pairwise distinct eigenvalues while y−∑e∈Zye=0 is a nontrivial vanishing linear combination, contradicting [F8]; so E=⟨w,ν⟩−e0 for some e0∈Z and ⟨w,ν⟩−E∈Z≥0. If E=⟨w,ν⟩, then e0=0, every nonzero member of {y−y0}∪{ye:e∈Z, e≠0} is an eigenvector of H with eigenvalue ⟨w,ν⟩ or ⟨w,ν⟩−e≠⟨w,ν⟩, these eigenvalues are pairwise distinct, and (y−y0)−∑e∈Z, e≠0ye=0 vanishes, so [F8] forces every member to be 0 and y=y0∈Cx.

6.1givenF7step 2.1step 3.1step 3.2step 5.1algebra

Assume that Mλ is irreducible over B. Since φ≠0 by step 2.1, the space Bφ is a nonzero B-stable subspace of Mλ, hence Bφ=Mλ; likewise Bψ=Mλ for the nonzero ψ, so ψ∈Bφ and φ∈Bψ. Applying step 5.1 with x:=φ, ν:=λ (claim 1 proved in step 3.1) and y:=ψ (an eigenvector of H with eigenvalue ⟨w,μ⟩, since Δ(Ess)ψ=μsψ) gives ⟨w,λ⟩−⟨w,μ⟩∈Z≥0; applying step 5.1 with x:=ψ, ν:=μ and y:=φ gives ⟨w,μ⟩−⟨w,λ⟩∈Z≥0. These two nonnegative integers sum to zero, so ⟨w,λ⟩=⟨w,μ⟩, and the equality case of the first application gives ψ∈Cφ: write ψ=cφ with c≠0. Then for every s, μsψ=Δ(Ess)ψ=cΔ(Ess)φ=cλsφ=λsψ, so μs=λs and μ=λ. Thus λ is the unique highest weight of Mλ and the highest weight vector is unique up to a scalar, which proves claim 3.

7.1givenF1F7step 1.1step 2.1step 3.1step 3.2step 6.1discharge-construct∎

Boundary and choice audit. If n=0 then λ=∅, V⊗0=C, w∅=1, κ∅=1, Φ=φ=idC≠0, and Δ(X)=0 for all X by [F1]; claims 1 and 2 are then immediate (λi=0 and Δ(Eij)=0), and in claim 3 the space M∅=Hom⁡S0(C,C)=C id is one-dimensional and irreducible over B=C id, every nonzero ψ is a scalar multiple of φ, and its weight is μ=(0,…,0)=λ. If d=0 then ℓ(λ)≤0 forces n=0, no indices i<j exist, and the same discussion applies with V=0. In the remaining case n≥1, d≥1 the sets Sj of steps 2.3 and 2.5 are finite (possibly empty) sets of places of the fixed tableau t, and the arguments of steps 1.1, 2.1, 1.2, 1.3, 2.2, 3.1, 2.3, 3.2, 2.4, 2.5, 3.3, 4.1, 5.1 and 6.1 use only the fixed basis, the fixed tableau, the explicit matrix units and finite sums, so no choice principle is invoked; this completes the proof of all three claims.

Remarks

  • Concrete highest weight vectors. For λ=(n) the module S(n) is trivial and M(n)=Sym⁡nV, and φ is the map 1↦e1n of weight (n,0,…,0); for λ=(1n) with n≤d, S(1n) is the sign representation and φ is the antisymmetrization map whose image is spanned by ∑σ∈Snsgn⁡(σ) eσ(1)⊗⋯⊗eσ(n)≠0, of weight (1,…,1,0,…,0). These are the usual highest weight vectors of the symmetric and exterior powers.

  • No Lie theory is imported. The proof uses matrix units, diagonal operators and finite sums only. The bracket relation [Δ(X),Δ(Y)]=Δ([X,Y]) and the place-commutation of Δ(X) are proved directly in step 1.2, and the uniqueness argument reduces to the elementary independence of eigenvectors for distinct eigenvalues; no root system, PBW theorem or classification of irreducible gl(V)-modules is used.

  • Characteristic. The cancellation κt⋅wt(a)=−κt⋅wt(a) in step 2.3 uses that 2 is invertible, and the argument is carried out over C.

  • Dependence on the choices. The map φ depends on the tableau t and on the basis e1,…,ed. When Mλ is irreducible, claim 3 says that every nonzero highest weight vector is a scalar multiple of φ, so the weight λ is an invariant of Mλ and does not depend on those choices.

  • Use in the Schur–Weyl decomposition. Together with the double centralizer theorem, which makes the multiplicity spaces Mλ irreducible whenever they are nonzero, this lemma identifies Mλ as the irreducible module of highest weight λ in the decomposition of V⊗n proved later on this page.

TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-10-02Open item page →

Schur-Weyl decomposition and highest weights

Statement

Let V be a finite-dimensional complex vector space of dimension d≥0, let n≥0, and let E:=V⊗n carry the commuting left place action of Sn and diagonal action of GL⁡(V) (Commuting symmetric-group and linear actions on a tensor power). Let B:=span⁡C{g⊗n:g∈GL⁡(V)}, and for λ⊢n put Mλ:=Hom⁡Sn(Sλ,E), on which GL⁡(V) acts by postcomposition (g⋅ψ)(s):=g⊗nψ(s) and B acts by b⋅ψ:=b∘ψ. Then:

  1. (Decomposition.) There is an isomorphism of (Sn×GL⁡(V))-modules E≅⨁λ⊢n, ℓ(λ)≤dSλ⊗Mλ, where Sn acts on the first factor and trivially on Mλ and GL⁡(V) acts on Mλ by postcomposition and trivially on Sλ. The sum runs over exactly the partitions λ⊢n with at most d rows.
  2. (Nonzero irreducible factors.) For every λ⊢n with ℓ(λ)≤d the space Mλ is nonzero and irreducible as a module over B by postcomposition, hence also irreducible as a GL⁡(V)-module and as a gl(V)-module under x↦Δ(x) (Irreducible, completely reducible, and faithful representations); for ℓ(λ)>d one has Mλ=0.
  3. (Pairwise inequivalence of the nonzero factors.) If λ≠μ are partitions of n with ℓ(λ)≤d and ℓ(μ)≤d, then Mλ and Mμ are non-isomorphic as B-modules, as GL⁡(V)-modules and as gl(V)-modules. Thus the nonzero factors in the decomposition of claim 1 are pairwise inequivalent, and a nonzero Mλ is not isomorphic to a zero Mμ with ℓ(μ)>d because their dimensions differ; no assertion is made about two zero factors.
  4. (Highest weight λ.) For every λ⊢n with ℓ(λ)≤d, writing λi:=0 for i>ℓ(λ), the module Mλ has highest weight λ with respect to the Borel of upper triangular matrices: it contains a nonzero vector φ with Δ(Eii)∘φ=λiφ for all i and Δ(Eij)∘φ=0 for all i<j, and every nonzero ψ∈Mλ killed by all raising operators Δ(Eij), i<j, and satisfying Δ(Eii)∘ψ=μiψ for scalars μ1,…,μd satisfies μ=λ and lies in Cφ.
  5. (Homogeneous polynomial module of degree n.) Fix a basis e1,…,ed of V and write gej=∑igijei for the matrix entries of g∈GL⁡(V). For every λ⊢n with ℓ(λ)≤d and every basis of Mλ, each matrix coefficient g↦⟨ψ∗,g⋅ψ⟩ of the action on Mλ is a homogeneous polynomial of degree n in the entries gij.

All statements are over C.

Facts & Assumptions

Given: a finite-dimensional complex vector space V of dimension d, an integer n≥0, the module E=V⊗n with its place Sn-action and diagonal GL⁡(V)-action, the algebra B=span⁡C{g⊗n}, and the spaces Mλ=Hom⁡Sn(Sλ,E) with the postcomposition actions.

[F1]

The place action σ⋅(v1⊗⋯⊗vn)=vσ−1(1)⊗⋯⊗vσ−1(n) and the diagonal action g⊗n(v1⊗⋯⊗vn)=gv1⊗⋯⊗gvn are well-defined linear actions that commute with each other, E=C for n=0, the assignment Δ(X)=∑a=1n1⊗(a−1)⊗X⊗1⊗(n−a) is linear in X, and if e1,…,ed is a basis of V then the assignment (v1,…,vn)↦v1⊗⋯⊗vn is multilinear, so g⊗n is computed on basis tensors by expanding each factor (Commuting symmetric-group and linear actions on a tensor power, Finite iterated tensor products represent multilinear maps independently of parenthesization).

[F2]

The dn elementary tensors ea1⊗⋯⊗ean form a basis of E (The elementary tensors of two bases form the product basis of the tensor product).

[F4]

The modules {Sλ:λ⊢n} form a complete irredundant list of the finite-dimensional irreducible complex Sn-representations (Specht modules classify the complex irreducibles of Sn, Column antisymmetrizers, polytabloids, and Specht modules).

[F5]

For a finite-dimensional completely reducible representation U of Sn the isotypic components U(λ), the sums of all irreducible subrepresentations isomorphic to Sλ, are defined and satisfy U=⨁λ⊢nU(λ) with the decomposition independent of choices; each U(λ) is a direct sum of copies of Sλ (The isotypic component of a completely reducible representation, The isotypic decomposition of a completely reducible representation is unique).

[F6]

If U is a finite-dimensional Sλ-isotypical Sn-module and Nλ=Hom⁡Sn(Sλ,U), then evaluation EU:Sλ⊗Nλ→U, s⊗f↦f(s), is an Sn-isomorphism; if U,U′ are such modules, every Sn-map U→U′ is uniquely EU′(1⊗a)EU−1 for a linear a:Nλ→Nλ′, and these identifications preserve composition (Isotypical evaluation and multiplicity subspaces).

[F7]

A nonzero Sn-intertwiner between irreducible complex Sn-representations is an isomorphism, and every endomorphism of an irreducible complex representation is a scalar (Schur's lemma for irreducible representations: a nonzero intertwiner is an isomorphism, and End⁡G(V) is a division ring, Over an algebraically closed field, every endomorphism of an irreducible representation is scalar).

[F8]

B is a unital C-subalgebra of End⁡(E) equal to the centralizer End⁡Sn(E) of the place action, and B is also the unital subalgebra generated by {Δ(T):T∈End⁡(V)} (The Schur-Weyl mutual centralizer theorem on tensor powers).

[F9]

For every λ⊢n one has Hom⁡Sn(Sλ,E)≠0 if and only if ℓ(λ)≤d (Column antisymmetrization gives the exact Schur–Weyl length cutoff).

[F10]

Assume ℓ(λ)≤d and let t be a λ-tableau. The row-labelled map Φ:Mλ→E, Φ(σ⋅{t})=σ⋅wt with wt carrying er(a) in the place labelled a, restricts to a nonzero φ=Φ∣Sλ∈Mλ with Δ(Eii)∘φ=λiφ for all i (where λi:=0 for i>ℓ(λ)) and Δ(Eij)∘φ=0 for all i<j; and if Mλ is irreducible over B by postcomposition, then every nonzero ψ∈Mλ with Δ(Eij)∘ψ=0 for all i<j and Δ(Eii)∘ψ=μiψ for scalars μi satisfies μ=λ and ψ∈Cφ (The row-labelled polytabloid map has highest weight lambda).

[F11]

Let r≥1, let every mi≥1 and let every Di be a division ring. Every simple left module over R=∏i=1rMmi(Di) is supported on exactly one factor and is isomorphic to that factor's column module Dimi, these column modules representing all simple left R-module isomorphism classes, one per factor (Simple modules over a product of matrix rings over division rings).

[F12]

A subspace of a gl(V)-module is a submodule when it is stable under Δ(x) for every x∈gl(V); the module is irreducible when it is nonzero and has no proper nonzero submodule (Irreducible, completely reducible, and faithful representations).

Proof

technique · constructive
1.1F3F4F5F6constructalgebra

[construct] By [F3] the Sn-module E is completely reducible, so by [F5] and [F4] its isotypic decomposition E=⨁λ⊢nEλ over the classes Sλ is defined and unique, with Eλ a (possibly zero) direct sum of copies of Sλ. If ψ:Sλ→E is Sn-linear, then ker⁡ψ is a submodule of the irreducible Sλ, so ψ=0 or ψ is injective with image isomorphic to Sλ, hence contained in Eλ; therefore Hom⁡Sn(Sλ,E)=Hom⁡Sn(Sλ,Eλ)=Mλ. Applying [F6] to the isotypical module Eλ gives an Sn-isomorphism Sλ⊗Mλ→Eλ, s⊗ψ↦ψ(s), so dim⁡CEλ=dim⁡CSλ⋅dim⁡CMλ and Eλ=0 if and only if Mλ=0.

1.2givenF1constructalgebra

Fix a basis s1,…,sk of Sλ and consider the evaluation map ev:Mλ→Ek, ψ↦(ψ(s1),…,ψ(sk)). It is C-linear and injective, because an Sn-linear map is determined by its values on a basis; and it intertwines the postcomposition action on Mλ with the componentwise diagonal action on Ek, since (g⋅ψ)(sl)=g⊗nψ(sl) for every l.

1.3F1F2algebra

Fix the basis e1,…,ed of V and write gej=∑igijei. By the multilinearity of the tensor product in [F1], for all b1,…,bn∈{1,…,d} one has g⊗n(eb1⊗⋯⊗ebn)=(geb1)⊗⋯⊗(gebn)=∑a1,…,an(∏l=1ngalbl)ea1⊗⋯⊗ean; hence each matrix entry of g⊗n in the elementary tensor basis [F2] is either 0 or a monomial ∏l=1ngalbl of degree n in the entries gij.

2.1givenF1F6step 1.1algebra

The evaluation isomorphism of step 1.1 intertwines the postcomposition action of GL⁡(V) on Mλ with the diagonal action on Eλ: for g∈GL⁡(V), s∈Sλ and ψ∈Mλ one has Eλ(s⊗g⋅ψ)=(g⋅ψ)(s)=g⊗nψ(s)=g⊗nEλ(s⊗ψ). It also intertwines the action of Sn, which is ρλ⊗id because Eλ(σs⊗ψ)=ψ(σs)=σψ(s)=σEλ(s⊗ψ); equivalently the conjugation action σ⋅ψ=σψσ−1 is trivial on Mλ, since ψ is Sn-linear. Hence Eλ≅Sλ⊗Mλ as (Sn×GL⁡(V))-modules.

2.2F2step 1.2step 1.3constructalgebra

Let ψ∈Mλ and ψ∗∈Mλ∗. Since ev of step 1.2 is injective, it has a linear retraction: choosing a basis of the image ev(Mλ) and extending it to a basis of the finite-dimensional space Ek, define r:Ek→Mλ on the basis by r(v)=ev−1(v) for v in that basis of the image and r=0 on the added vectors, so that r∘ev=id. Then g⋅ψ=r(ev(g⋅ψ)) and the matrix coefficient is ψ∗(g⋅ψ)=(ψ∗∘r)(g⊗nψ(s1),…,g⊗nψ(sk)). The vectors ψ(sl)∈E are fixed, so their coordinates in the elementary tensor basis [F2] are constants, and by step 1.3 the numbers ψ∗(g⋅ψ) are constant-coefficient linear combinations of monomials of degree n in the entries gij: they are homogeneous polynomials of degree n. This holds for the matrix coefficients of the action with respect to any basis of Mλ, so Mλ is a homogeneous polynomial GL⁡(V)-module of degree n. This proves claim 5.

3.1F9step 1.1step 2.1algebra

By [F9], Mλ≠0 exactly when ℓ(λ)≤d; combined with step 1.1 and step 2.1 this gives the (Sn×GL⁡(V))-isomorphism E=⨁ℓ(λ)≤dEλ≅⨁ℓ(λ)≤dSλ⊗Mλ, the omitted components being exactly the zero ones, and proves claim 1.

4.1F5F6F8step 1.1step 3.1algebra

An Sn-endomorphism F∈End⁡Sn(E) maps each isotypic component Eλ into itself: Eλ is a sum of copies of Sλ by [F5], and the image under F of such a copy is either 0 or, by irreducibility of Sλ, a copy of Sλ, hence lies in Eλ. Restriction gives an isomorphism of C-algebras End⁡Sn(E)→∏λ⊢nEnd⁡Sn(Eλ) (injective, since F is determined on the direct sum, and blockwise surjective, with componentwise composition). For each λ with Mλ≠0, [F6] identifies End⁡Sn(Eλ) with End⁡(Mλ): every Fλ∈End⁡Sn(Eλ) is uniquely Eλ(1⊗aλ)Eλ−1 with aλ∈End⁡(Mλ) and the identification preserves composition. Therefore, by [F8], B=End⁡Sn(E)≅∏ℓ(λ)≤dEnd⁡(Mλ) as C-algebras, the product being over the λ with Mλ≠0 (and B=0 when there are none).

5.1F9F11step 4.1algebra

Under the identification of step 4.1, an element b∈B acts on Eλ as Eλ(1⊗aλ)Eλ−1, where aλ is its λ-component in ∏End⁡(Mλ); hence for ψ∈Mλ one has (b⋅ψ)(s)=b(ψ(s))=Eλ(s⊗aλψ)=(aλψ)(s), that is, b acts on Mλ by aλ. Since Mλ≠0 for ℓ(λ)≤d by [F9], End⁡(Mλ) is the full matrix algebra Mmλ(C) with mλ=dim⁡CMλ≥1, so B≅∏ℓ(λ)≤dMmλ(C) is a product of full matrix algebras over the field C; by [F11] every simple left B-module is supported on exactly one factor and is isomorphic to that factor's column module, and distinct factors have non-isomorphic column modules. The postcomposition module Mλ is the column module of the λ-th factor End⁡(Mλ) (the other factors acting as zero, as step 4.1 shows the action factors through the λ-component), so Mλ is a simple B-module and Mλ≅Mμ as B-modules implies λ=μ.

6.1F8F9F12step 5.1algebra

Because B is spanned by the operators g⊗n, a GL⁡(V)-stable subspace of Mλ is stable under every b∈B; because B is the unital subalgebra generated by the operators Δ(T), T∈End⁡(V), a subspace stable under all Δ(T) (that is, a gl(V)-submodule, [F12]) is also B-stable. By step 5.1 the space Mλ is a simple B-module and nonzero, so it has no proper nonzero subspace of either kind: it is irreducible as a GL⁡(V)-module and as a gl(V)-module. This proves claim 2, the case ℓ(λ)>d being [F9].

6.2F8F9step 5.1algebra

Let λ,μ⊢n satisfy ℓ(λ)≤d and ℓ(μ)≤d, so that Mλ≠0 and Mμ≠0 by [F9], and let T:Mλ→Mμ be an isomorphism of GL⁡(V)-modules. For b=∑gcgg⊗n∈B and ψ∈Mλ one has T(b⋅ψ)=∑gcgT(g⊗nψ)=∑gcgg⊗nT(ψ)=b⋅T(ψ), so T is a B-module isomorphism and, both modules being nonzero, step 5.1 forces λ=μ. Likewise an isomorphism of gl(V)-modules intertwines every Δ(T), and since finite sums and products of such operators span B by [F8], it is a B-module isomorphism and again forces λ=μ. If exactly one of ℓ(λ),ℓ(μ) is at most d, then exactly one of Mλ,Mμ is zero by [F9], so the two are not isomorphic even as vector spaces. This proves claim 3.

6.3F10F9step 5.1algebra

Assume ℓ(λ)≤d, so Mλ≠0 by [F9] and Mλ is irreducible over B by step 5.1. The highest weight lemma [F10] then supplies a nonzero φ∈Mλ with Δ(Eii)∘φ=λiφ (with λi=0 for i>ℓ(λ)) and Δ(Eij)∘φ=0 for i<j, and shows that every nonzero ψ∈Mλ killed by all raising operators and of weight μ satisfies μ=λ and ψ∈Cφ. This proves claim 4.

7.1F1F3F9step 3.1step 6.1step 6.2step 6.3step 2.2discharge-construct∎

Boundary and choice audit. For n=0 one has E=C, the only partition is ∅ with ℓ(∅)=0≤d, M∅=Hom⁡(C,C)=C, and claim 1 reads E≅S∅⊗M∅; B=C id, M∅ is a one-dimensional simple B-module, claim 4 holds with λ=(0,…,0) and claim 5 with degree 0 polynomials, the constants. For d=0 and n≥1 one has V=0, E=0 and no partition of n satisfies ℓ(λ)≤0, so the sum in claim 1 is empty and E=0, the assertions of claims 2, 3, 4 and 5 are vacuous since all Mλ=0, and B=End⁡Sn(0)=0 consistently. For d≥1 and n≥1 there are finitely many partitions of n and all spaces are finite-dimensional. The argument uses that C has characteristic 0 not dividing n! ([F3]), that C is algebraically closed ([F6], [F7]), and the fixed basis of V, the fixed basis of Sλ, the fixed tableau t and the finite-dimensional retraction r of step 2.2; finite sums over the partitions of n and over the coordinate index sets occur throughout, and no choice principle is invoked. This proves claims 1, 2, 3, 4 and 5.

Remarks

  • Two actions, two refinements. The Schur-Weyl decomposition refines the isotypic decomposition of E as an Sn-module by the action of the centralizer B=End⁡Sn(E): the double centralizer theorem (The Schur-Weyl mutual centralizer theorem on tensor powers) turns B into a product of full matrix algebras, one factor on each nonzero multiplicity space, which is both why each nonzero Mλ is irreducible and why the distinct nonzero λ-factors are inequivalent. The length cutoff comes from Column antisymmetrization gives the exact Schur–Weyl length cutoff and the weight from The row-labelled polytabloid map has highest weight lambda; no root system, PBW theorem or classification of gl(V)-modules is used.

  • Symmetric and exterior powers. For λ=(n) the factor M(n) is isomorphic to the n-th symmetric power of V, and for λ=(1n), which appears exactly when n≤d, the factor M(1n) is isomorphic to the n-th exterior power; the highest weight vectors of claim 4 are the usual ones, as computed in the remarks of The row-labelled polytabloid map has highest weight lambda.

  • Polynomial degree. The degree n in claim 5 records the polynomiality of g↦g⊗n: the matrix coefficients are homogeneous of degree n because they are combinations of n-fold products of the entries of g. This is the precise content of the phrase that each multiplicity space Mλ is a homogeneous polynomial module of degree n.

5 · Examples, counterexamples and false statements

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