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Jucys–Murphy Elements and Seminormal Forms

1 · Prerequisites

2 · Summary

This page develops the Jucys–Murphy elements Xk=∑j<k(j k) of the symmetric group algebra and the representation theory they generate. The elements are introduced over an arbitrary commutative ring, are shown to commute pairwise, and satisfy the local relations siXj=Xjsi for j∉{i,i+1} and siXi+1=Xi+1si, which give the local H(2) relations on consecutive pairs. The Gelfand–Tsetlin algebra of the chain S1⊂⋯⊂Sn is introduced from the centres of the subalgebras, and the diagonal-algebra theorem identifies it with the algebra of the Young basis, so that over C the Jucys–Murphy elements act diagonally in that basis.

An independent polytabloid coefficient calculation shows that the transposition class sum acts by the total node content. Taking successive differences along the branching chain gives the spectral weights. The central structural result is the computation of the joint spectrum: the eigenvalue vector of the Young line of a standard tableau T is its content vector Cont⁡(T)=(cT(1),…,cT(n)), and the vectors satisfying the three classical conditions are exactly the content vectors of standard tableaux. From this the primitive tableau idempotents are reconstructed by Lagrange interpolation in the eigenvalues of Xn, proving that the Gelfand–Tsetlin algebra is exactly the algebra generated by X1,…,Xn over C, and the symmetric polynomial evaluations of the Jucys–Murphy elements are identified with the centre of the group algebra.

The final part obtains Young's explicit forms. The Young vectors are normalized by applying the primitive idempotents to the images of the canonical tableau, and the Coxeter generators act by the seminormal two-by-two blocks with structure constants r−1 and 1−r−2, where r is the axial distance cT(i+1)−cT(i). Rescaling to unit vectors for the positive-definite invariant form on the Specht module produces the symmetric orthogonal blocks with off-diagonal entry 1−r−2, i.e. Young's orthogonal form. The relative centralizer of C[Sn−1] in C[Sn] is identified with the algebra of functions on the Young-graph edges and shown to be generated by the previous centre together with the single element Xn.

3 · Logical flowchart

4 · Definitions, theorems and proofs

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

The content of a node and the content vector of a standard tableau

Definition

Let λ⊢n with Young diagram [λ] (Partitions, English diagrams, and conjugation), so that the nodes of [λ] are the pairs (r,c) with r,c≥1 and c≤λr (rows numbered downward, columns rightward).

The content of a node (r,c)∈[λ] is c(r,c):=c−r, the column index minus the row index. The node (r,c) therefore has content t exactly when it lies on the diagonal c−r=t; the content of (1,1) is 0, contents increase by 1 along a row and decrease by 1 down a column.

Now let T be a standard tableau of shape λ (Tableaux and standard tableaux). For 1≤k≤n let (rk,ck) be the node of [λ] carrying the entry k, so that T(rk,ck)=k. The content vector of T is Cont⁡(T):=(cT(1),…,cT(n))∈Zn,cT(k):=c(rk,ck)=ck−rk, the list of contents of the nodes read in the order of the entries 1,2,…,n. For the empty tableau of shape ∅ the content vector is the empty vector, the unique element of Z0.

Remarks

  • Well-definedness. A tableau T of shape λ is a bijection [λ]→{1,…,n}, so each k∈{1,…,n} occupies exactly one node (rk,ck) and the integers cT(k)=ck−rk are determined by T. The map T↦Cont⁡(T) uses the fixed row and column coordinates and the labels of T: it depends only on which entry stands in which node.

  • The entries of the content vector are the contents of the shape. Since T is a bijection onto the n nodes of [λ], the multiset of entries of Cont⁡(T) equals the multiset of node contents {c(x):x∈[λ]}, independent of T. In particular two standard tableaux of the same shape have content vectors that differ by a permutation of their entries, and the multiset of contents of a tableau is an invariant of its shape.

  • Two extreme examples. The row tableau of shape (n) carries k in (1,k), so its content vector is (0,1,2,…,n−1); the column tableau of shape (1n) carries k in (k,1), so its content vector is (0,−1,−2,…,−(n−1)).

  • First entries. The entry 1 always occupies the node (1,1), because every other node has a node weakly to its left and weakly above it, whose entry would be smaller. Hence cT(1)=0 for every nonempty standard tableau T. Similarly, cT(k) need not be monotone in k: for the tableau 123 of shape (2,1) one has Cont⁡=(0,1,−1).

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

The Gelfand-Tsetlin algebra of the symmetric group chain

Definition

For n≥1 and 1≤m≤n let Z(C[Sm]) be the centre of the complex group algebra C[Sm] (The center Z(k[G]) of the group algebra, The group ring R[G] of finitely supported formal R-linear combinations of group elements). We use the standard chain of symmetric groups S1⊂S2⊂⋯⊂Sn,Sm=Sym⁡({1,…,m}), in which Sm is the subgroup of Sn fixing every element of {m+1,…,n} pointwise; thus C[Sm] is the subalgebra of C[Sn] spanned by Sm, and Z(C[S1])=C⋅1. Each centre Z(C[Sm]) is thereby regarded as a subalgebra of C[Sn].

The Gelfand-Tsetlin algebra of the chain is GZ(n):=⟨Z(C[S1]),Z(C[S2]),…,Z(C[Sn])⟩⊆C[Sn], the unital subalgebra of C[Sn] generated by all these centres.

Remarks

  • Well-definedness. Each Z(C[Sm]) is a C-subalgebra of C[Sm], hence, via the inclusion C[Sm]⊆C[Sn], a subset of C[Sn] closed under addition, multiplication and scalar multiplication; the generated subalgebra is therefore a unital subalgebra of C[Sn]. It is finite-dimensional because C[Sn] is: each C[Sm] is a finite-dimensional semisimple algebra (If char⁡k∤∣G∣, then k[G] is a semisimple ring), so its centre is finite-dimensional as well.

  • Commutativity. Every element of Z(C[Sm]) is central in C[Sm]. If m≤k and z∈Z(C[Sm]), w∈Z(C[Sk]), then C[Sm]⊆C[Sk] and w commutes with every element of C[Sk], in particular with z; hence zw=wz. Thus all the generating centres commute with one another, and GZ(n) is a commutative subalgebra of C[Sn]. Only this centrality, not semisimplicity, is used.

  • The top centre is included. The term m=n shows Z(C[Sn])⊆GZ(n); in fact the centre of C[Sn] is the algebra generated by its class sums, and the other centres are generated by the class sums of the subgroups, so GZ(n) is generated by class sums of the chain together with C[S1]=C.

  • The algebra used below. GZ(n) is the diagonal algebra of the Young basis: The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis identifies it with ⨁TCPT over the standard tableaux T of size n, and The Jucys-Murphy elements generate the Gelfand-Tsetlin algebra shows that it is also the algebra generated by the Jucys-Murphy elements.

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

The Jucys-Murphy elements of the symmetric group algebra

Definition

Let n≥1 and let R be a commutative ring. In the group ring R[Sn] of the symmetric group on {1,…,n} (Partitions, English diagrams, and conjugation, The symmetric group Sym⁡(X): the bijections of a set X under composition, The group ring R[G] of finitely supported formal R-linear combinations of group elements), where (j k) denotes the transposition of the distinct entries j,k∈{1,…,n} (The symmetric group Sym⁡(X): the bijections of a set X under composition), the Jucys-Murphy elements are X1:=0,Xk:=∑j=1k−1(j k)∈R[Sn](2≤k≤n). Each Xk is a finite sum of group elements with coefficient 1, so the formula already defines an element of the integral group ring Z[Sn], and its image under the base change Z[Sn]→R[Sn] is the displayed element (Restriction of scalars and extension of scalars S⊗RM along a ring homomorphism R→S); for 1≤k≤m≤n the element Xk of R[Sm], computed in the subgroup Sm=Sym⁡({1,…,m})⊆Sn of permutations fixing m+1,…,n, maps to Xk under the inclusion Sm↪Sn. Equivalently Xk=Tk−Tk−1, where Tk=∑1≤i<j≤k(i j) is the sum of all transpositions in Sk.

Remarks

  • Well-definedness. The sum defining Xk has the k−1 terms (1 k),…,(k−1 k), each of which is an element of the subgroup Sk⊆Sn, hence a basis element of the free R-module R[Sn]; a finite sum of basis elements is an element of R[Sn] independent of any ordering of the summands. The formula uses only the labels 1,…,k, so it is preserved by the inclusion Sm↪Sn for k≤m≤n and by the base change Z[Sn]→R[Sn]. The group-ring multiplication is bilinear and sends basis elements g,h to gh (The group ring R[G] is a unital R-algebra with basis G, and each g∈G is a unit of R[G]). Thus the subgroup inclusions and the coefficient map ∑gagg↦∑g(ag1R)g preserve products and the identity.

  • The identity Xk=Tk−Tk−1. The transpositions of Sk are (i j) with 1≤i<j≤k; those with j<k are exactly the transpositions of Sk−1, and the remaining ones are (i k) with i<k. Hence Tk−Tk−1=∑j=1k−1(j k)=Xk. For k=2 this reads X2=(1 2)=T2−T1, where T1=0. Since each Tk is a sum of all transpositions of the subgroup Sk, it is a sum of full conjugacy classes of Sk.

  • Integral normalization. Every coefficient in Xk is 1, not ±1 or a fraction; no characteristic is inverted, so Xk is defined over Z and over every commutative ring. This is the normalization used throughout this page; the spectral statements below specialize the coefficient ring to C, but no integral identity of this page uses division.

  • Centrality. The elements Xk need not be central in R[Sn]. The element X1=0 is always central, and for n=2 the algebra R[S2] is commutative, so X2 is central as well. For n≥3 and R≠0, conjugation by (2 3) sends X2=(1 2) to (1 3)≠X2: these are distinct basis elements and 1R≠0. Thus X2 is not central in this case. Pairwise commutativity of the Xk is proved in The Jucys-Murphy elements commute pairwise.

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

Every element of Sn is inverted by an involution of Sn−1

Statement

Let n≥1, let Sn−1≤Sn be the stabilizer of n, and let g∈Sn. There is h∈Sn−1 with h2=1 (the identity is allowed) and hgh−1=g−1; here such a self-inverse permutation is called an involution. In particular every element of Sn is conjugate to its inverse by an element of Sn−1.

Facts & Assumptions

Given: An integer n≥1 and a permutation g∈Sn, where Sn=Sym⁡({1,…,n}) (Partitions, English diagrams, and conjugation).

[F1]

Every permutation of a finite set is a product of pairwise disjoint cycles, uniquely up to reordering the factors and cyclically rotating the entries within each cycle; the identity has the empty such product (Every permutation of a finite set is a product of pairwise disjoint cycles, uniquely up to reordering and cyclic rotation).

[F2]

A cycle (a0 a1 … ak−1) has support {a0,…,ak−1}, sends ai to ai+1 for i<k−1 and ak−1 to a0, and fixes every point outside its support; cycles with disjoint supports are disjoint, and a cycle may be written starting at any of its entries (Support, fixed points, disjoint cycles, cycle length, disjoint-cycle decompositions, and cycle type, The symmetric group Sym⁡(X): the bijections of a set X under composition).

[F3]

For every g∈Sn and every cycle c=(a1 a2 … ak) one has gcg−1=(g(a1) g(a2) … g(ak)) (Conjugating a cycle relabels each entry: g(a1 … ak)g−1=(g(a1) … g(ak))).

[F4]

Cycles with disjoint supports commute (Cycles with disjoint supports commute).

Proof

technique · explicit construction
1.1F1F2

By [F1] write g=c1c2⋯cr with the ci pairwise disjoint cycles of length at least 2. If g(n)≠n, exactly one factor meets {n}, say cs; its support is the orbit of n under g, and by [F2] we may write cs=(n a1 … ak−1) with k≥2 and distinct a1,…,ak−1∈{1,…,n−1}. If g(n)=n, no factor meets {n}; in that case put k=1, leave the list a1,…,ak−1 empty and drop the discussion of cs.

2.1step 1.1F1F2construct

Define h∈Sym⁡({1,…,n}) by the following rules on the pairwise disjoint sets listed so far: h(n):=n; h(ai):=ak−i for 1≤i≤k−1 when cs exists; and for each remaining factor ci=(b1 … bm) of the decomposition, h(bj):=bm+1−j for 1≤j≤m; every element of {1,…,n} not yet mentioned is fixed by h. The listed points are distinct, so h is a well-defined bijection: each rule pairs the listed points in pairs, possibly fixing a middle point, and in every case applying the rule twice returns the point. Hence h is an involution; it fixes n and every point outside {1,…,n−1}, so h∈Sn−1 and h−1=h.

3.1step 2.1F2F3algebra

Conjugation by h acts on each factor by [F3]: for cs=(n a1 … ak−1) we get hcsh−1=(h(n) h(a1) … h(ak−1))=(n ak−1 … a1), the cycle sending n to ak−1, sending ai to ai−1 and sending a1 to n, which is exactly cs−1; for every other factor ci=(b1 … bm) we get hcih−1=(h(b1) … h(bm))=(bm … b1)=ci−1.

4.1step 3.1F4algebra∎

Inserting h−1h=1 between consecutive factors gives hgh−1=(hc1h−1)⋯(hcrh−1)=c1−1⋯cr−1 by step 3.1. Reversing a product inverts it, so c1−1⋯cr−1=(cr⋯c1)−1; by [F4] the pairwise disjoint factors commute, hence cr⋯c1=c1⋯cr=g. Therefore hgh−1=g−1 with h∈Sn−1 an involution, which is the statement.

Remarks

  • The source's shorter argument is incomplete as printed. The cited source proves the fact by deleting the letter n from g and choosing an element h∈Sn−1 that conjugates the deletion g′ to g′−1; it then asserts that such an h realizes g−1=hgh−1. That step is not correct for an arbitrary such h: for g=(1 2 3 4) and h=(2 3) one has h (1 2 3) h−1=(1 3 2)=(1 2 3)−1, while hgh−1=(1 3 2 4)≠g−1=(1 4 3 2). The construction above chooses the explicit cycle-reversing involution, which does satisfy hgh−1=g−1; only that corrected construction is used later, in The centralizer of C[Sn−1] in C[Sn] is commutative.

  • No choice. For each g the involution h is given by explicit formulas on the finitely many cycles of g, so the statement is proved without any selection principle, and the argument is integral and characteristic-free: it uses only the group structure of Sn.

CorollaryStatement: Literature-sourcedProof: AI-adaptedprecheck passjudge pass (gpt-6.1-sol)Open item page →

The Jucys-Murphy elements commute pairwise

Statement

For all 1≤i,j≤n one has XiXj=XjXi in Z[Sn], hence in R[Sn] for every commutative ring R; that is, the Jucys-Murphy elements commute pairwise, and the subalgebra they generate is commutative.

Facts & Assumptions

Given: An integer n≥1, the Jucys-Murphy elements X1,…,Xn∈Z[Sn], and for each k the transposition sum Tk=∑1≤i<j≤k(i j) (The Jucys-Murphy elements of the symmetric group algebra).

[F1]

X1=0, Xk=Tk−Tk−1 for 2≤k≤n, and therefore ∑k=2nXk=Tn−T1=Tn; for m≤n the element Xk of Z[Sm] maps to Xk under the inclusion Z[Sm]↪Z[Sn], and the identity Z[Sn]→R[Sn] of the base change is a unital ring homomorphism sending Xk to Xk (The Jucys-Murphy elements of the symmetric group algebra).

[F2]

For h∈Sn and distinct i,j∈{1,…,n} one has h (i j) h−1=(h(i) h(j)) (Conjugating a cycle relabels each entry: g(a1 … ak)g−1=(g(a1) … g(ak))).

Proof

technique · induction on $n$
1.1givenbase

Base case. For n=1 the only element is X1=0; for n=2 the elements are X1=0 and X2=(1 2). In both cases every pair among X1,…,Xn consists of two commuting elements, namely 0 or the single element X2.

1.2givenihF1

Induction hypothesis. Let n≥3 and assume that X2,…,Xn−1 commute pairwise in Z[Sn−1]. By [F1] the inclusion of group rings is a unital ring homomorphism carrying these elements to the corresponding elements of Z[Sn], so X2,…,Xn−1 commute pairwise in Z[Sn] as well.

1.3F2givenalgebra

The element Tn=∑1≤i<j≤n(i j) is central in Z[Sn]. Indeed, for h∈Sn, [F2] gives h (i j) h−1=(h(i) h(j)) for every pair i<j, so hTnh−1=∑i<j(h(i) h(j))=∑i<j(i j)=Tn, because {i,j}↦{h(i),h(j)} is a bijection of the set of 2-element subsets of {1,…,n}. Thus hTn=Tnh for every h∈Sn, and extending by linearity over the basis Sn gives zTn=Tnz for every z∈Z[Sn].

2.1step 1.2step 1.3F1algebra

For 2≤j≤n−1 compare the two expansions of XjTn. On the one hand XjTn=TnXj by step 1.3; on the other hand, using [F1] and the induction hypothesis of step 1.2, XjTn=Xj(∑k=2n−1Xk+Xn)=∑k=2n−1XjXk+XjXn=∑k=2n−1XkXj+XjXn, while TnXj=(∑k=2n−1Xk+Xn)Xj=∑k=2n−1XkXj+XnXj. Subtracting the common term ∑k=2n−1XkXj gives XjXn=XnXj. Together with the induction hypothesis and the base case this covers every pair, so all of X1,…,Xn commute pairwise in Z[Sn].

3.1step 2.1F1discharge-induction: step 1.1∎

Finally let R be a commutative ring. The base change Z[Sn]→R[Sn] is a unital ring homomorphism and carries Xk to Xk for every k by [F1]; applying it to the identity XiXj=XjXi of step 2.1 gives XiXj=XjXi in R[Sn]. Hence the subalgebra generated by the Xk is commutative over any commutative ring.

Remarks

  • Integrality and no choice. The argument takes place entirely in Z[Sn] and uses only bilinear expansion in the group basis and the bijection {i,j}↦{h(i),h(j)} on two-element subsets. No characteristic is inverted, no module is selected and no choice principle is used; the base-change sentence is the only place a general ring appears.

  • The centrality of Tk in the subgroup. The same computation with n replaced by k shows that each Tk is central in Z[Sk], since conjugation by Sk permutes the transpositions of Sk. This is the only property of Tn used above.

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

A partition is determined by the multiset of its node contents

Statement

Let λ,μ⊢n. If the multiset of contents {c(x):x∈[λ]} equals the multiset {c(y):y∈[μ]}, then λ=μ.

Facts & Assumptions

Given: Partitions λ,μ⊢n; for a partition ν⊢n we write [ν] for its Young diagram, ν′ for its conjugate, and νj′=#{i:νi≥j} for the height of column j (Partitions, English diagrams, and conjugation).

[F1]

A node of [ν] is a pair (r,c) with r,c≥1 and c≤νr; its content is c(r,c)=c−r; the rows of [ν] are weakly decreasing (Partitions, English diagrams, and conjugation).

[F2]

The content of a node and the content vector are as defined in The content of a node and the content vector of a standard tableau; in particular the content map is c(r,c)=c−r on nodes.

Proof

technique · direct
1.1F1F2algebra

For a partition ν⊢n and an integer t≥0 put nt(ν):=#{x∈[ν]:c(x)=t}. A node of content t has the form (i,i+t) with i≥1, and it lies in [ν] exactly when i+t≤νi, that is νi−i≥t; hence nt(ν)=#{i≥1:νi−i≥t} for every t≥0, the count being finite and equal to 0 for t>n.

1.2F1F2algebra

Similarly, for an integer s≥0 put n−s(ν):=#{x∈[ν]:c(x)=−s}. A node of content −s is (j+s,j) with j≥1; it lies in [ν] exactly when j+s≤νj′, that is νj′−j≥s. Hence n−s(ν)=#{j≥1:νj′−j≥s} for every s≥0.

1.3F1F2algebra

The partition ν is recovered from the pair of strictly decreasing sequences a1>a2>⋯>ad and b1>b2>⋯>bd by the formula νr=(ar+1)⋅[r≤d]+#{c:1≤c<r, bc≥r−c} for every row index r. Indeed, for each diagonal node (i,i)∈[ν] with i≤d let Ai:={(i,c):i≤c≤νi} be its arm and Li:={(r,i):i≤r≤νi′} its leg; arms and legs have sizes ai+1 and bi+1, and the d hooks Ai∪Li partition [ν], because a node (r,c) with c≥r lies in the arm Ar and a node (r,c) with c<r lies in the leg Lc. Counting row r therefore gives νr=∣Ar∣+#{c<r:(r,c)∈Lc}=(ar+1)⋅[r≤d]+#{c<r:bc≥r−c}, since (r,c)∈Lc means c≤r≤νc′=c+bc.

2.1step 1.1step 1.2F1algebra

For each row index i put ai:=νi−i, and for each column index j put bj:=νj′−j. The row lengths are weakly decreasing, so ai+1<ai for all i; the column heights are weakly decreasing as well, so bj+1<bj for all j. Moreover ai≥0 exactly for the diagonal rows i with (i,i)∈[ν], and bj≥0 exactly for the diagonal columns j with (j,j)∈[ν], so the two multisets A(ν):={ai:ai≥0} and B(ν):={bj:bj≥0} have a common cardinality d(ν), the number of diagonal nodes. By steps 1.1 and 1.2 the numbers nt(ν), t≥0, determine the multiplicity of every value t≥0 among the ai, namely nt(ν)−nt+1(ν), and hence determine the multiset A(ν) together with d(ν); likewise the numbers n−s(ν), s≥0, determine B(ν).

3.1step 2.1step 1.3given∎

Assume now that the multiset of contents of [λ] equals that of [μ]. Then nt(λ)=nt(μ) for every integer t; by steps 1.1 and 1.2 this forces A(λ)=A(μ) and B(λ)=B(μ), including the common cardinality d. Writing both multisets as strictly decreasing sequences a1>⋯>ad and b1>⋯>bd, step 1.3 computes the row lengths of λ and μ by the same formula from the same data, so all row lengths agree and λ=μ.

Remarks

  • Why the diagonal data are Frobenius coordinates. The numbers a1>⋯>ad and b1>⋯>bd are the arm and leg lengths of the diagonal nodes, the Frobenius coordinates of ν; the formula of step 1.3 is the usual reconstruction of a partition from them. The lemma says that the content multiset, which records the ai and bj through the diagonal counts of steps 1.1 and 1.2, is equivalent to that data.

  • Sharper statement. The proof shows the two multisets A(ν) and B(ν) separately, not merely their union; both are needed, since the nonnegative and negative contents determine the arms and the legs respectively.

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

Distinct addable nodes of a partition have distinct contents

Statement

Let λ be a partition. If x≠y are addable nodes of [λ], then c(x)≠c(y); equivalently the content map is injective on the set Add⁡(λ) of addable nodes.

Facts & Assumptions

Given: A partition λ=(λ1,…,λk) with Young diagram [λ] and set of addable nodes Add⁡(λ) (Removable and addable nodes).

[F1]

A node (i,λi+1) with 1≤i≤k is addable if and only if i=1 or λi−1>λi; the node (k+1,1) is always addable; and these are all addable nodes. With the conventions λ0:=+∞ and λk+1:=0, the addable nodes of [λ] are exactly the nodes (i,λi+1) for the indices 1≤i≤k+1 satisfying λi−1>λi (Removable and addable nodes).

[F2]

The content of a node is c(r,c)=c−r; in particular c(i,λi+1)=λi+1−i (The content of a node and the content vector of a standard tableau).

Proof

technique · direct
1.1F1given

By [F1] every addable node has the form (i,λi+1) for a unique index i∈I:={1≤i≤k+1:λi−1>λi}, where we use λ0=+∞ and λk+1=0; indeed for i≤k the condition is exactly the addability criterion, and i=k+1 is the new-row node (k+1,1)=(k+1,λk+1+1) with λk>λk+1=0.

1.2F2given

For such an index i the content of the addable node is c(i,λi+1)=λi+1−i by [F2], and the partition is weakly decreasing, so λi≥λi+1≥⋯≥0.

2.1step 1.2algebra

Let i<i′ be two indices in I. By weak monotonicity λi≥λi′, and since i<i′ we get λi−i>λi′−i′, that is λi+1−i>λi′+1−i′.

3.1step 1.1step 2.1∎

Combined with step 1.1, distinct addable nodes (i,λi+1) and (i′,λi′+1) with i≠i′ have contents differing by the strict inequality of step 2.1; hence c is injective on Add⁡(λ).

Remarks

  • The content is the addable-node coordinate. For an addable node (i,λi+1) the content λi+1−i is the integer at which the interpolation factors of the projector recursion of Primitive tableau idempotents by Jucys-Murphy interpolation are evaluated; the lemma is what makes all their denominators nonzero.

  • Empty partition. For λ=∅ the only addable node is (1,1), of content 0, so injectivity is vacuous there; the argument above applies with k=0 and I={1}.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passOpen item page →

Local relations between the Jucys-Murphy elements and adjacent transpositions

Statement

Let n≥2 and put si:=(i i+1) for 1≤i≤n−1, the Coxeter generators of Sn. Then in Z[Sn], hence in R[Sn] for every commutative ring R: (a) siXj=Xjsi whenever j∉{i,i+1}; (b) siXi+1=Xi+1si; equivalently siXisi+si=Xi+1 and siXi+1=Xisi+1. In particular the subalgebra generated by si,Xi,Xi+1 satisfies the local H(2) relations si2=1, XiXi+1=Xi+1Xi, siXi+1=Xi+1si.

Facts & Assumptions

Given: An integer n≥2, an index 1≤i≤n−1, the adjacent transposition si=(i i+1), the transposition sums Tk=∑1≤p<q≤k(p q), and the Jucys-Murphy elements Xk=∑j<k(j k)=Tk−Tk−1 (The Jucys-Murphy elements of the symmetric group algebra).

[F1]

For 1≤k≤m≤n the element Xk of Z[Sm] maps to Xk under the inclusion Z[Sm]↪Z[Sn], and each base change Z[Sn]→R[Sn] is a unital ring homomorphism carrying Xk to Xk for 1≤k≤n: the coefficient map ∑gagg↦∑g(ag1R)g preserves the group-basis product and the identity (The Jucys-Murphy elements of the symmetric group algebra).

[F2]

The elements s1,…,sn−1 generate Sn subject to the Coxeter relations; in particular si2=1 and si−1=si (The symmetric group has the Coxeter presentation).

[F3]

For h∈Sn and distinct a,b∈{1,…,n} one has h (a b) h−1=(h(a) h(b)) (Conjugating a cycle relabels each entry: g(a1 … ak)g−1=(g(a1) … g(ak))).

Proof

technique · direct computation in the group basis
1.1F1F2F3algebra

Case j<i of (a). For such j one has Xj=∑l<j(l j) with l<j<i, and si fixes both letters l and j; [F3] and [F2] give si(l j)si=(si(l) si(j))=(l j), hence si(l j)=(l j)si. Summing over l<j gives siXj=Xjsi.

1.2F1F2F3algebra

Case j>i+1 of (a). Here si fixes j, and [F3] gives siXjsi=∑l<j(si(l) si(j))=∑l<j(si(l) j). The map l↦si(l) is a bijection of {1,…,j−1} onto itself, because it interchanges the two elements i,i+1 of that set and fixes all others; hence ∑l<j(si(l) j)=∑l<j(l j)=Xj and siXj=Xjsi.

1.3F1F2algebra

Part (b). For j<i the two permutations (i i+1)(j i) and (j i+1)(i i+1) agree on j, on i and on i+1 and fix every other letter, hence are equal; and Xi+1=∑j<i(j i+1)+(i i+1). Using Xi=∑j<i(j i) and si=(i i+1) we therefore get siXi=∑j<i(i i+1)(j i)=∑j<i(j i+1)(i i+1)=(∑j<i(j i+1))si=(Xi+1−si)si=Xi+1si−si2=Xi+1si−1 by [F2]. Hence siXi+1=Xi+1si.

1.4F1F3algebra

The product XiXi+1. The element Tk is central in Z[Sk] for every k: by [F3] conjugation by h∈Sk sends each transposition (p q) to the transposition (h(p) h(q)), and {p,q}↦{h(p),h(q)} is a bijection of the two-element subsets of {1,…,k}, so hTkh−1=Tk. Since Ti+1=Ti+Xi+1 and Xi∈Z[Si], centrality of Ti+1∈Z[Si+1] and of Ti∈Z[Si] gives XiXi+1=Xi(Ti+1−Ti)=XiTi+1−XiTi=Ti+1Xi−TiXi=(Ti+1−Ti)Xi=Xi+1Xi.

2.1step 1.3F2algebra

Equivalent forms. Multiplying siXi+1=Xi+1si on the right by si and using si2=1 from [F2] gives siXisi+si=Xi+1; multiplying that identity on the left by si gives Xisi+1=siXi+1. Thus all three displayed forms of (b) hold.

3.1step 1.1step 1.2step 1.3step 2.1step 1.4F1F2∎

Collecting steps 1.1 and 1.2 covers every j∉{i,i+1}, since j<i and j>i+1 are the only possibilities for 1≤j≤n; step 1.3 and step 2.1 give the three listed forms of (b); step 1.4 and [F2] give XiXi+1=Xi+1Xi and si2=1. All these identities are equalities in Z[Sn], and by [F1] the base change Z[Sn]→R[Sn] carries them to the corresponding identities in R[Sn]. Hence (a) and (b) hold, and the subalgebra generated by si,Xi,Xi+1 satisfies the three listed H(2) relations.

Remarks

  • Local meaning of the relations. The identity (b) says that Xi+1 is obtained from Xi by conjugating with si and adding si, so the pair Xi,Xi+1 together with si generates a local subalgebra satisfying the H(2) relations: on a joint eigenline of the Xk on which Xi acts by a and si by ±1, the relation forces Xi+1 to act by a±1. This is the computation behind the weight-transposition analysis of The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors.

  • What is not claimed. The statement records that the three listed relations hold in the subalgebra generated by si,Xi,Xi+1; no claim is made that this subalgebra has a presentation with exactly these generators and relations, and no dimension count for it is used on this page.

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The centralizer of C[Sn−1] in C[Sn] is commutative

Statement

Let Z(C[Sn],C[Sn−1])={z∈C[Sn]:zh=hz for every h∈Sn−1} be the centralizer of the subalgebra C[Sn−1] in C[Sn]. Then Z(C[Sn],C[Sn−1]) is a commutative subalgebra of C[Sn].

Facts & Assumptions

Given: An integer n≥1, the group Sn=Sym⁡({1,…,n}) with its subgroup Sn−1=Sym⁡({1,…,n−1}) of permutations fixing n, and the group algebra C[Sn] with basis {[g]:g∈Sn} and multiplication [g][h]=[gh] (Partitions, English diagrams, and conjugation, The symmetric group Sym⁡(X): the bijections of a set X under composition, The group ring R[G] is a unital R-algebra with basis G, and each g∈G is a unit of R[G]).

[F1]

For every g∈Sn there is an involution hg∈Sn−1 with hgghg−1=g−1; the proof of the cited lemma exhibits hg by explicit formulas on the cycles of g (Every element of Sn is inverted by an involution of Sn−1).

[F2]

C[Sn] has the group elements as a C-basis, every element has a unique expansion ∑gcg[g] with finitely many nonzero coefficients, and [g][h]=[gh]; coefficients of equal basis elements are equal. The inverse in Sn reverses products: (gh)−1=h−1g−1 (The group ring R[G] is a unital R-algebra with basis G, and each g∈G is a unit of R[G], The symmetric group Sym⁡(X): the bijections of a set X under composition).

Proof

technique · inversion anti-automorphism
1.1F2givenalgebra

The centralizer C:=Z(C[Sn],C[Sn−1]) is a C-subalgebra of C[Sn]: it contains 1, is closed under addition and scalar multiplication because equality with each h∈Sn−1 is preserved by these operations, and is closed under multiplication because yz h=y hz=h yz for all h∈Sn−1 whenever y,z∈C; closure under multiplication is also checked on the basis expansions using [F2].

1.2F2givenalgebra

Define σ:C[Sn]→C[Sn] on the basis by σ([g]):=[g−1] and extend C-linearly: σ(∑gcg[g])=∑gcg[g−1]. Then σ is an involution, since (g−1)−1=g, and it is an anti-automorphism: σ([g][h])=σ([gh])=[(gh)−1]=[h−1g−1]=[h−1][g−1]=σ([h])σ([g]) by [F2], and the identity extends to all elements by bilinearity.

2.1step 1.2F1F2algebra

The anti-automorphism σ fixes every element of C. Let z=∑gcg[g]∈C, and fix one g∈Sn. By [F1] there is hg∈Sn−1 with hgghg−1=g−1. Since z=hgzhg−1, comparison of the coefficient of [g−1] on the two sides gives cg−1=cg; conjugation is a bijection, so exactly the summand indexed by g contributes on the right. This equality holds for every g, and therefore σ(z)=z by [F2]. The argument compares each coefficient separately and requires no common conjugator.

3.1step 1.1step 2.1algebra∎

For y,z∈C we have yz=σ(yz)=σ(z)σ(y)=zy: the first equality is step 2.1, the second holds because σ is an anti-automorphism by step 1.2, and the third is step 2.1 applied to y and to z. Hence C is a commutative subalgebra of C[Sn] by step 1.1.

Remarks

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Elementary symmetric Jucys-Murphy evaluations are cycle-count class sums

Statement

For n≥1 and 0≤s≤n, es(X2,X3,…,Xn)=∑ρ⊢nℓ(ρ)=n−sCρ(n), where the right-hand side is the sum of all permutations of Sn with exactly n−s cycles (fixed points counted), grouped into conjugacy classes; it is zero for s>n−1. In particular e0=1, e1 is the sum of all transpositions, and en−1 is the sum of all n-cycles.

Facts & Assumptions

Given: An integer n≥1 and the Jucys-Murphy elements Xk=∑j<k(j k)∈Z[Sn] (The Jucys-Murphy elements of the symmetric group algebra).

[F1]

For m≤n the element Xk of Z[Sm] maps to Xk under the inclusion Z[Sm]↪Z[Sn]; in particular Xn=∑j<n(j n) (The Jucys-Murphy elements of the symmetric group algebra).

[F2]

For 0≤k≤m the k-th elementary symmetric polynomial is ek(x1,…,xm)=∑1≤i1<⋯<ik≤mxi1⋯xik, with e0=1 and ek=0 for k>m (The elementary symmetric polynomials e0,e1,…,en).

[F3]

The cycle type of a permutation of a finite n-element set is the family c1,…,cn in which ck is the number of k-element orbits, fixed points being recorded as 1-cycles; thus the cycle lengths form a partition ρ⊢n and the number of parts ℓ(ρ) is the total number of cycles, fixed points included. Cycles are written (a0 a1 … ak−1) and a k-cycle fixes every point outside its support (Support, fixed points, disjoint cycles, cycle length, disjoint-cycle decompositions, and cycle type, The symmetric group Sym⁡(X): the bijections of a set X under composition).

[F4]

Every permutation of a finite set is a product of pairwise disjoint cycles, uniquely up to reordering the factors and cyclically rotating the entries inside each factor; the identity is the empty product (Every permutation of a finite set is a product of pairwise disjoint cycles, uniquely up to reordering and cyclic rotation).

[F5]

The Jucys-Murphy elements commute pairwise, so polynomial substitution and the commutative recursion apply. (The Jucys-Murphy elements commute pairwise)

Proof

technique · induction on $n$
1.1givenbaseF2F3

Base case. For n=1 the list X2,…,Xn is empty, so e0=1 by [F2], and the right-hand side for s=0 is the single class sum C(1)(1) of the identity of S1, whose cycle type (1) has ℓ=1=n−0; for s≥1 the left-hand side is es of no variables, hence 0 by [F2], and no partition ρ⊢1 has ℓ(ρ)=1−s≤0. Thus the identity holds for n=1 and all s.

1.2givenih

Induction hypothesis. Let n≥2 and assume that for all 0≤s≤n−1 one has es(X2,…,Xn−1)=∑ρ⊢n−1, ℓ(ρ)=n−1−sCρ(n−1) in Z[Sn−1], the sum being 0 when no such partition exists.

1.3F2algebra

Recursion for elementary symmetric polynomials. For m≥1 and 0≤s≤m, splitting the s-element subsets of {1,…,m} into those not containing m and those containing m gives es(x1,…,xm)=es(x1,…,xm−1)+xmes−1(x1,…,xm−1) in any commutative ring, with the convention e−1=0; the identity is trivial for s=0 as well.

2.1step 1.2step 1.3F1F3F5algebra

First summand. For 0≤s≤n−1, take m=n−1 and xi=Xi+1 in step 1.3, using [F5] and use [F1] to identify Xk in Z[Sn−1] with Xk in Z[Sn]: es(X2,…,Xn−1)=∑ρ⊢n−1, ℓ(ρ)=n−1−sCρ(n−1) by step 1.2. Each class sum Cρ(n−1) is the sum of the permutations σ∈Sn−1 of cycle type ρ; regarded in Sn such a σ fixes n and has one further cycle, namely (n), so its cycle type in Sn has ℓ(ρ)+1=n−s cycles; conversely every τ∈Sn with τ(n)=n and n−s cycles restricts to a permutation of Sn−1 with cycle type ρ and ℓ(ρ)=n−1−s. Hence this summand equals the sum of all τ∈Sn with τ(n)=n and exactly n−s cycles.

2.2step 1.2F1F3F4algebra

Second summand. For s=0 this summand is zero by e−1=0. For 1≤s≤n−1, with the same substitution, Xnes−1(X2,…,Xn−1)=(∑j<n(j n))es−1(X2,…,Xn−1)=∑j<n∑σ(j n)σ, where σ runs over the permutations of Sn−1 with exactly n−s cycles and the second identity uses step 1.2 for s−1 and [F1]. For such a σ and j, use [F4] to write σ as a product of pairwise disjoint cycles and insert the fixed point j as a 1-cycle if necessary; if (j c1 … cb) is the cycle of j, then evaluating on the letters j,c1,…,cb,n shows (j n)σ replaces that factor by the single cycle (n j c1 … cb) and keep all other factors, so (j n)σ moves n and has the same number n−s of cycles as σ. The map (σ,j)↦τ:=(j n)σ is a bijection from these pairs onto the permutations τ∈Sn with τ(n)≠n and n−s cycles, with inverse τ↦((τ(n) n)τ, τ(n)): indeed j:=τ(n) lies in {1,…,n−1}, the product (j n)τ fixes n and hence lies in Sn−1, and the two constructions invert one another because (j n)2=1. Hence this summand is the sum of all τ∈Sn with τ(n)≠n and exactly n−s cycles, each occurring once.

3.1step 1.3step 2.1step 2.2F2F3discharge-induction: step 1.1∎

Adding the two summands via step 1.3, every τ∈Sn with exactly n−s cycles is counted exactly once, according to whether τ(n)=n or τ(n)≠n; grouping by cycle type and using [F3] gives es(X2,…,Xn)=∑ρ⊢n, ℓ(ρ)=n−sCρ(n). For s=0 this reads 1=C(1n)(n); for s=1 it sums the permutations with n−1 cycles, exactly the transpositions when n≥2; when n=1 both the transposition sum and e1 vanish; for s=n−1 it sums the permutations with a single cycle, the n-cycles. For s>n−1 the left-hand side is es in the n−1 variables X2,…,Xn, hence 0 by [F2], and the right-hand side is an empty sum.

Remarks

  • The identity is integral. Both sides lie in Z[Sn], and the proof uses only the compatibility of the Xk with the subgroup chain and the elementary symmetric recursion; no representation theory, no characteristic-zero hypothesis, and no choice are used.

  • A check of the normalization. For n=1 the sum for s=0 is the class of the identity, and for n=2 and s=1 it is the sum of the single transposition C(2)(2)=X2; both match the asserted evaluations.

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The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis

Statement

For m≥1 and λ⊢m let eλ(m)∈Z(C[Sm]) be the central idempotent of the Wedderburn factor End⁡(SCλ) of C[Sm], so that 1=∑λ⊢meλ(m) with pairwise orthogonal central idempotents and eλ(m) acts as the identity on SCλ and as 0 on SCμ for μ≠λ. For a path T=(λ(1),…,λ(n)) in the Young graph (a standard tableau of size n) put PT:=eλ(1)(1)eλ(2)(2)⋯eλ(n)(n), the factors commuting pairwise. Then:

(i) every PT is a nonzero idempotent of rank one; (ii) PTPT′=0 for T≠T′ and ∑TPT=1; (iii) GZ(n)=⨁TC PT, the algebra diagonal in the basis of the lines CvT:=im⁡PT (the Young basis); (iv) the elements X1,…,Xn act diagonally in the Young basis, and GZ(n) is a maximal commutative subalgebra of C[Sn].

Facts & Assumptions

Given: The chain S1⊂⋯⊂Sn and the Gelfand-Tsetlin algebra GZ(n)=⟨Z(C[S1]),…,Z(C[Sn])⟩ (The Gelfand-Tsetlin algebra of the symmetric group chain); for each m≥1 the complex Specht modules Vλ:=SCλ, λ⊢m, which are the irreducible C[Sm]-modules up to isomorphism, pairwise inequivalent for distinct λ (Specht modules classify the complex irreducibles of Sn).

[F1]

For every m≥1 the group algebra is a product of matrix algebras indexed by its simple modules; by the classification this reads C[Sm]≅∏λ⊢mEnd⁡(Vλ), and the identity of the factor End⁡(Vλ) is a central idempotent eλ(m) in C[Sm] such that 1=∑λ⊢meλ(m), eλ(m)eμ(m)=δλμeλ(m) for all λ,μ⊢m, and for every C[Sm]-module W the element eλ(m) acts as the projection onto the sum of the irreducible summands of W isomorphic to Vλ; in particular eλ(m) acts as the identity on Vλ and as 0 on Vμ for μ≠λ (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, If char⁡k∤∣G∣, then k[G] is a semisimple ring).

[F2]

For m≥2 and λ⊢m the restriction of Vλ to Sm−1 is Res⁡Sm−1SmVλ≅⨁x∈Rem⁡(λ)Vλ−x, the summands being irreducible with pairwise distinct shapes and each occurring exactly once; for m=1 one has V(1)=C with S0 acting trivially (The complex Specht restriction branching rule).

Proof

technique · direct
1.1F1given

The idempotents eλ(m) of [F1] are central in C[Sm], pairwise orthogonal, sum to 1, and project each C[Sm]-module onto its λ-isotypic part.

1.2F1givenalgebra

The idempotents attached to different levels commute: if m≤k, then C[Sm]⊆C[Sk] and eμ(k) is central in C[Sk], hence commutes with every element of C[Sm], in particular with eλ(m).

2.1step 1.1F2algebra

Let m≥2 and λ⊢m. The restriction of Vλ to Sm−1 is the direct sum of the distinct irreducible modules Vλ−x over the removable nodes x∈Rem⁡(λ); consequently eμ(m−1) acts on Vλ as the projection onto the summand Vμ when μ=λ−x for some x∈Rem⁡(λ), and as 0 otherwise.

2.2step 1.1step 1.2F1algebra

For every standard tableau T of size n the product PT=eλ(1)(1)⋯eλ(n)(n) is an idempotent, and PTPT′=0 whenever T≠T′: distinct standard tableaux of size n differ at some level m≤n, where their entries are distinct partitions, and the corresponding factors are orthogonal by [F1] after all factors are commuted past one another using step 1.2.

2.3step 1.1F1algebra

Every central element of C[Sm] is a linear combination of the eλ(m): under the isomorphism C[Sm]≅∏λEnd⁡(Vλ) of [F1] the centre corresponds to the product of the centres of the factors, and the centre of the matrix algebra End⁡(Vλ) consists of the scalars, that is, of Ceλ(m). Hence z=∑λ⊢mωλ(z)eλ(m) for every z∈Z(C[Sm]), where ωλ(z) is the scalar by which z acts on Vλ.

3.1step 1.1step 2.1F1F2algebra

Rank one and the sum over paths, by induction on m: for every μ⊢m and every path T of length m ending at μ, the product ET:=eλ(1)(1)⋯eμ(m) acts on Vμ as a rank-one idempotent with image a line LT≠0, kills every Vν with ν⊢m, ν≠μ, and ∑T ending at μET acts as the identity on Vμ, that is, ∑T ending at μET=eμ(m) in C[Sm]. For m=1 the unique path gives E=e(1)(1)=1 acting as the identity on V(1)=C by [F2], which is the rank-one projection onto the whole line. For the induction step write T′=T↓[m−1] and μ=λ(m−1)+x; by [F2] and step 2.1 the operator eλ(m−1)(m−1) projects Vμ onto the summand Vλ(m−1), on which ET′ acts as the rank-one projection onto LT′ by the induction hypothesis, while the remaining summands of the restriction are killed; multiplying by eμ(m), which is the identity on Vμ and kills the other Vν, gives the claim for ET. Summing over all paths ending at μ and using the induction hypothesis at level m−1 together with [F1] gives ∑T ending at μET=∑ν⊢m−1∑T′ ending at νET′eμ(m)=(∑ν⊢m−1eν(m−1))eμ(m)=eμ(m). Distinct paths give distinct lines: if two paths end at μ through different removable nodes their lines lie in different summands of the restriction, and if they end through the same node the induction hypothesis separates their prefixes.

4.1step 2.2step 2.3step 3.1algebra

The algebra GZ(n) equals ⨁TCPT. For the inclusion ⊇: each factor eλ(m)(m) of PT lies in Z(C[Sm]), so PT∈GZ(n). For the inclusion ⊆: step 2.3 writes every element of every generating centre as ∑λωλeλ(m), and step 3.1 writes eλ(m)=∑T ending at λET; substituting gives a linear combination of the PT=eλ(1)(1)⋯eλ(n)(n) for paths of length n, so every generating element lies in the span, and the span is a subalgebra because PTPT′=δTT′PT by step 2.2; hence GZ(n)⊆⨁TCPT. The PT are linearly independent because they are nonzero and pairwise orthogonal, so the sum is direct and GZ(n) is commutative.

4.2step 3.1F1algebra

The idempotents add up to 1: summing the identity of step 3.1 over all λ⊢n and using [F1] gives ∑TPT=∑λ⊢neλ(n)=1.

5.1step 4.1givenalgebra

The Jucys-Murphy elements lie in GZ(n) and act diagonally. For k≥2 one has Xk=Tk−Tk−1, where Tm=∑1≤i<j≤m(i j) is the sum of the transpositions of Sm (The Jucys-Murphy elements of the symmetric group algebra); any two transpositions are conjugate, since for transpositions (a b) and (c d) a permutation g with g(a)=c, g(b)=d satisfies g(a b)g−1=(c d) by Conjugating a cycle relabels each entry: g(a1 … ak)g−1=(g(a1) … g(ak)), so Tm is a class sum and hence central in C[Sm] by For a finite group, the class sums form a basis of Z(k[G]) for m≥2, while T1=0. Thus each Tm lies in Z(C[Sm])⊆GZ(n) and each Xk lies in GZ(n); also X1=0. By step 4.1 we may write Xk=∑TcT,kPT, and then Xk acts on the line CvT=im⁡PT by the scalar cT,k, because PT is the identity on its own image. Hence X1,…,Xn act diagonally in the Young basis.

6.1step 4.1step 5.1F1algebra∎

Maximal commutativity. Under the isomorphism C[Sn]≅∏λ⊢nEnd⁡(Vλ) of [F1], step 3.1 shows that PT corresponds to the tuple whose entry in the factor End⁡(Vλ), λ=λ(n), is the rank-one projection pT onto the line LT⊆Vλ, and whose other entries are 0; since the lines LT for T of shape λ are independent and number dim⁡CVλ, they form a basis of Vλ. Therefore GZ(n)=⨁TCPT corresponds to the tuples (aλ) with aλ in the algebra Dλ of all operators on Vλ diagonal in that basis. An element b=(bλ) commutes with every PT if and only if each bλ commutes with the full diagonal algebra Dλ; and the commutant of Dλ in End⁡(Vλ) is Dλ itself, because a matrix commuting with every diagonal matrix is diagonal. Hence the commutant of GZ(n) in C[Sn] is GZ(n), and if B⊆C[Sn] is any commutative subalgebra containing GZ(n), then B commutes with GZ(n), so B⊆GZ(n) and B=GZ(n). Thus GZ(n) is a maximal commutative subalgebra, and with steps 4.1-5.1 all four assertions are proved.

Remarks

  • The Young basis. The lines CvT=im⁡PT are the simultaneous eigenspaces of the Gelfand-Tsetlin algebra; choosing a nonzero vector vT in each gives the Young basis. The eigenvalues of the Jucys-Murphy elements in this basis are computed in The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors, and the idempotents PT are reproduced by interpolation in Primitive tableau idempotents by Jucys-Murphy interpolation.

  • Where the hypotheses are used. The argument uses characteristic zero only through the semisimplicity and the classification of the complex irreducibles; the branching rule and the centre are used to build and count the PT. Nothing here uses the Axiom of Choice: all sums and products are finite and the idempotents are constructed from the fixed chain.

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The transposition class sum acts on a complex Specht module by total content

Statement

Let m≥0, let ν⊢m, and let SCν be the complex Specht module. Put Tm=∑1≤a<b≤m(a b),n(ν)=∑i(i−1)νi. Then Tm is central in C[Sm] and acts on SCν as the scalar zν=∑i(νi2)−∑j(νj′2)=∑(r,c)∈[ν](c−r)=n(ν′)−n(ν). If m≥2, dν=dim⁡CSCν and χν is its character, then χν((1 2))=dνzν(m2). For m=0,1, Tm=0 and zν=0; no transposition character value is asserted.

Facts & Assumptions

Given: m,ν, the complex Specht module, and the displayed transposition sum.

[F1]

Row and column stabilizers preserve the individual row and column sets. The tabloid stabilizer is the row stabilizer. The Specht module lies in the finite-dimensional tabloid permutation module and contains et=∑γ∈Ctsgn⁡(γ)γ{t}, whose coefficient at {t} is 1 because Rt∩Ct={1}. (Row and column stabilizers, Young subgroups, tabloids, and permutation modules, Column antisymmetrizers, polytabloids, and Specht modules)

[F2]

Complex Specht modules are nonzero irreducible representations. An endomorphism of a finite-dimensional irreducible representation over an algebraically closed field is scalar. (Complex Specht modules are irreducible, Over an algebraically closed field, every endomorphism of an irreducible representation is scalar)

[F3]

A partition's conjugate records its column heights; its diagram consists of the nodes (r,c) with 1≤c≤νr. Characters are traces, and trace is linear. (Partitions, English diagrams, and conjugation, The character χV(g)=tr⁡(ρV(g)) of a finite-dimensional complex representation, Trace is a linear functional on Mn(F))

Proof

1.1F1F2givenconstruct

Conjugation by any permutation sends (a b) to the transposition of its two images, hence permutes the summands of Tm. Thus Tm is central, so its action on the nonzero finite-dimensional irreducible Specht module is an intertwiner and equals zid⁡ for some z∈C by [F2]. Choose the row-filled tableau t of shape ν, and use its nonzero polytabloid et. Taking the coefficient of {t} in Tmet=zet recovers z, since that coefficient in et is 1 by [F1].

2.1F1step 1.1algebra

A summand indexed by a transposition τ=(a b) and γ∈Ct contributes to this coefficient precisely when τγ∈Rt. Put r=τγ, so τ=rγ−1. If x∉{a,b}, then rγ−1(x)=x. The entry γ−1(x) has the column of x, and since r preserves each row it also has the row of x. Their row-column intersection consists of x alone, so γ−1(x)=x and r(x)=x. Thus both r and γ fix the complement of {a,b}; each is either the identity or τ. Their product is τ exactly when one is τ and the other is the identity. Therefore the contributing pairs are exactly: γ=1, τ∈Rt, of sign +1; and γ=τ, τ∈Ct, of sign −1. These cases cannot overlap, since two distinct entries cannot share both row and column.

3.1F3step 1.1step 2.1algebra

There are ∑i(νi2) transpositions within rows and ∑j(νj′2) within columns. By steps 1.1 and 2.1 their difference is z. Summing c−1 within every row gives the first count, and summing r−1 within every column gives the second; hence their difference is ∑(r,c)∈[ν](c−r). Also n(ν)=∑(r,c)∈[ν](r−1) and n(ν′)=∑(r,c)∈[ν](c−1), proving every formula for zν. This includes m=0,1: there are no row or column pairs and the transposition sum is zero.

4.1F3step 3.1algebra∎

For m≥2, all (m2) transpositions are conjugate, so their representing matrices are similar and have character value χν((1 2)). Taking traces of the scalar action in step 3.1 gives (m2)χν((1 2))=dνzν by [F3]. Dividing by the nonzero integer (m2) proves the stated character formula. The construction and coefficient count are finite and use no choice of an arbitrary family or seminormal-basis input.

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The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors

Statement

Let n≥1. (a) The elements X1,…,Xn act diagonally in the Young basis of the previous item: for every standard tableau T of size n and every k, XkvT=cT(k)vT, and the joint eigenspaces are one-dimensional, indexed by the standard tableaux. (b) A vector α=(a1,…,an)∈Zn occurs as the joint eigenvalue vector of a vT, equivalently α=Cont⁡(T) for a standard tableau T, if and only if: (1) a1=0; (2) for every q>1 at least one of aq−1,aq+1 occurs among a1,…,aq−1; (3) if ap=aq with p<q, then both ap−1 and ap+1 occur among ap+1,…,aq−1. The association T↦Cont⁡(T) is a bijection from the standard tableaux of size n onto this set.

Facts & Assumptions

Given: The chain S1⊂⋯⊂Sn, the Gelfand-Tsetlin algebra GZ(n), the Young lines CvT=im⁡PT for the standard tableaux T of size n, and the Jucys-Murphy elements Xk=∑j<k(j k) (The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis, The Jucys-Murphy elements of the symmetric group algebra). The Young lines are considered in each irreducible SCλ and, collectively, in the multiplicity-free sum ⨁λ⊢nSCλ, as in the preceding diagonal-algebra construction.

[F1]

The transposition class sum Tm acts on the complex Specht module of shape ν⊢m by zν=n(ν′)−n(ν)=∑(r,c)∈[ν](c−r). Its character value for m≥2 is dim⁡(SCν)zν/(m2); the denominator is not used for m=0,1. The scalar is proved independently by a polytabloid coefficient count, without seminormal forms. (The transposition class sum acts on a complex Specht module by total content)

[F2]

The complex Specht modules SCλ are a complete irredundant list of finite-dimensional irreducible complex Sm-modules; for λ⊢m the restriction Res⁡Sm−1SmSCλ≅⨁x∈Rem⁡(λ)SCλ−x (Specht modules classify the complex irreducibles of Sn, The complex Specht restriction branching rule).

[F3]

Contents, content vectors and the content c(x)=c−r of the node (r,c) are as defined in The content of a node and the content vector of a standard tableau; standard tableaux and shapes are as in Tableaux and standard tableaux; addable and removable nodes are as in Removable and addable nodes, and distinct addable nodes of a partition have distinct contents (Distinct addable nodes of a partition have distinct contents).

[F4]

The Young lines of each shape give a basis of the corresponding irreducible. Each Xk lies in GZ(n) and acts by a scalar on those lines; GZ(n) is maximal commutative (The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis).

Proof

1.1F1F2F3F4givenalgebra

For a standard tableau T, let λ(k) be the shape of its entries 1,…,k. The Young line LT lies in the corresponding irreducible summand at each level of the restriction chain by [F2] and the given diagonal-algebra construction. For k≥2, Tk and Tk−1 therefore act on this line by zλ(k) and zλ(k−1). Since Xk=Tk−Tk−1, [F1] gives its eigenvalue as their difference, the content of the one node added at step k. For k=1, X1=0 and entry 1 occupies (1,1), of content zero. Thus XkvT=cT(k)vT for all k.

1.2F3givenalgebra

Every tableau content vector satisfies (1) and (2): entry 1 lies in (1,1), and any later node has a left or upper neighbour of smaller entry and content respectively one less or one greater. Nodes of a fixed content lie on a northwest-to-southeast diagonal, and their entries strictly increase along it: the right neighbour of an earlier diagonal node lies before the next diagonal node. If entries p<q have equal content, their nodes are (r,c) and (r+d,c+d) for d≥1. The nodes (r,c+1) and (r+1,c) exist because the later node does, and their entries lie strictly between p and q by row/column increase along paths inside the diagram. Their contents are respectively c−r+1 and c−r−1, proving (3).

2.1F3step 1.2algebra

We prove the precise criterion needed to construct a tableau. Let a nonempty standard tableau have content vector β and shape λ. An integer t is an addable content exactly when (A) t−1 or t+1 occurs in β, and (B) after every occurrence of t, both neighbours t−1,t+1 occur later in β. First suppose the diagonal of content t is absent. Then t≠0. If t>0, absence means λ1≤t; content t+1 is also absent, and content t−1 occurs exactly when λ1≥t. Thus (A) says λ1=t, exactly when (1,t+1) is addable. If t<0, transpose the diagram: absence means the first column has height at most −t, and (A) says its height is exactly −t, exactly when the new bottom node of content t is addable. In these cases (B) is vacuous.

3.1F3step 1.2step 2.1algebra

Suppose instead that the last node of content t is x=(r,c), with c−r=t. Any addable node of that content must be (r+1,c+1): a diagram is closed under moving northwest, so all earlier nodes on the same diagonal already exist and a later one would require its immediate predecessor. This next node is addable exactly when both u=(r,c+1) and v=(r+1,c) exist. If they exist, each entry is larger than the entry of x and their contents are t+1,t−1, so (A) and (B) hold, since x has the largest entry among the content-t nodes. Conversely, if u is absent, every content-(t+1) node (a,a+t+1) has a<r: a node with a>r would force a content-t node in its own row beyond x, and a=r would be u. Its column is then at most c, so it is northwest of x and has smaller entry. If v is absent, every content-(t−1) node (a,a+t−1) has a≤r: a≥r+2 would force the content-t node (a−1,a+t−1) beyond x, while a=r+1 would be v. Such a node is again strictly northwest of x and has smaller entry. Thus in either absence case (B) fails at the entry of x. This proves the criterion completely.

4.1F3step 1.2step 2.1step 3.1givenconstruct

Given α satisfying (1)-(3), start with entry 1 at (1,1). Suppose its first q−1 entries have been placed in a standard tableau. Condition (2) at q is (A) of the criterion, and condition (3) applied to every earlier occurrence of aq is exactly (B). Steps 2.1 and 3.1 therefore give an addable node of content aq. It is unique by [F3]. Put entry q in that node; the shape remains a Young diagram and standardness holds because every previous entry is smaller. Induction constructs a tableau with content vector α. Any tableau with that vector has the same successive shapes and entries, by uniqueness of the addable node at each step, so it is the same tableau. Combined with step 1.2, this proves the asserted bijection.

5.1F4step 1.1step 1.2step 4.1algebra∎

The Young lines give a basis in each SCλ by [F4] and the given diagonal-algebra theorem; their union is a basis of the specified multiplicity-free sum. By step 1.1 their joint weights are precisely the tableau content vectors. Step 4.1 proves these vectors are distinct: across all shapes, each vector specifies exactly one tableau. In a basis of joint eigenvectors, the eigenspace for a fixed vector is the span of exactly those basis vectors with that weight, because comparing each coordinate coefficient in Xkv=akv forces any nonzero coefficient to have that weight for every k. Hence each such eigenspace is one-dimensional, and the eigenvalue vectors are exactly the integer vectors satisfying (1)-(3). This proves (a) and (b).

Remarks

The scalar input is the independent polytabloid calculation in [F1]. The character normalization is χν((1 2))=dim⁡(SCν)zν/(m2) for m≥2, not its reciprocal. The one-dimensional eigenspace assertion uses each irreducible Young basis, or their multiplicity-free sum. Repeated copies of an irreducible in another representation can enlarge these eigenspaces. All node placements are forced by distinct addable contents; the combinatorial construction requires no additional choice principle.

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Primitive tableau idempotents by Jucys-Murphy interpolation

Statement

Let T be a standard tableau of size n, let μ be the shape of the restriction of T to [n−1], and let A(μ) be the set of contents of the addable nodes of μ. Set P[1]:=1 and define recursively, for n≥2, PT:=PT↓[n−1]∏c∈A(μ)c≠cT(n)Xn−ccT(n)−c∈C[Sn]. Then all displayed denominators are nonzero, PT is the rank-one idempotent projecting onto the Young line CvT, each PT is a polynomial in X1,…,Xn with rational coefficients, and the PT over the standard tableaux of size n are pairwise orthogonal idempotents with ∑TPT=1.

Facts & Assumptions

Given: The chain S1⊂⋯⊂Sn, the Jucys-Murphy elements Xk, and, for every standard tableau T of size n, the Young line CvT=im⁡PT with the idempotents PT of the diagonal-algebra theorem (The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis, The Jucys-Murphy elements of the symmetric group algebra).

[F1]

GZ(n)=⨁TCPT over the standard tableaux T of size n; the PT are nonzero pairwise orthogonal idempotents with ∑TPT=1, and CvT=im⁡PT is one-dimensional (The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis).

[F2]

XkvT=cT(k)vT for every standard tableau T and every k, with cT(k) the content of the node carrying k (The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors, The content of a node and the content vector of a standard tableau).

[F3]

For a partition μ, the contents of distinct addable nodes are distinct, and the addable nodes of μ are the nodes (i,μi+1) with i=1 or μi−1>μi, together with the new-row node (Distinct addable nodes of a partition have distinct contents, Removable and addable nodes).

[F4]

The restriction of T to [n−1] is a standard tableau of shape μ that is obtained by deleting the node carrying n; conversely every standard tableau S of size n with S↓[n−1]=T↓[n−1] is obtained by placing n in an addable node of μ (Tableaux and standard tableaux, Removable and addable nodes).

Proof

technique · induction
1.1F1givenbase

Base case. For n=1 the only standard tableau is [1], the line is Cv[1]=C⋅1, and P[1]:=1 is the rank-one projection onto it with rational (indeed integer) coefficients.

1.2F1givenih

Induction hypothesis. For every standard tableau S of size n−1 the recursively defined element PS∈C[Sn−1] equals the idempotent PS of [F1], is the projection onto CvS, and is a polynomial in X1,…,Xn−1 with rational coefficients.

1.3F3F4givenalgebra

Let T be a standard tableau of size n and μ:=shape⁡(T↓[n−1]). The set A(μ) of contents of addable nodes is finite and cT(n)∈A(μ): the node carrying n is an addable node of μ by [F4]. By [F3] the denominators cT(n)−c, c∈A(μ), c≠cT(n), are nonzero integers, so the displayed product is a well-defined element of C[Sn].

2.1step 1.2F1algebra

If S is a standard tableau of size n−1 with S≠T↓[n−1], then the factor PT↓[n−1] acts as 0 on the line CvS by step 1.2; hence PT acts as 0 on every Young line of size n whose restriction to [n−1] differs from T↓[n−1].

2.2step 1.2F2F4algebra

Now let S be a standard tableau of size n with S↓[n−1]=T↓[n−1], and let x be the addable node of μ carrying n in S, so that cS(n)=c(x) by [F4] and [F2]. Then PT↓[n−1] acts as the identity on CvS by step 1.2, and the interpolation factor acts on CvS by the scalar ∏c∈A(μ)c≠cT(n)cS(n)−ccT(n)−c, because Xn acts on CvS by cS(n) by [F2].

2.3step 1.2step 1.3algebra

Polynomial form. By step 1.2 the factor PT↓[n−1] is a polynomial in X1,…,Xn−1 with rational coefficients; each factor (Xn−c)/(cT(n)−c) is a polynomial in Xn with rational coefficients because cT(n)−c∈Z∖{0} by step 1.3; hence PT is a polynomial in X1,…,Xn with rational coefficients.

3.1F3step 1.3step 2.2algebra

The scalar of step 2.2 equals 1 when S=T, and equals 0 when S≠T: if S=T then cS(n)=cT(n) and every factor is (cT(n)−c)/(cT(n)−c)=1; if S≠T then S places n in a different addable node of μ, so cS(n)≠cT(n) by [F3], and the factor with c=cS(n) has numerator 0 while the denominator is nonzero by step 1.3.

4.1step 2.1step 3.1F1algebra

Steps 2.1-2.3 show that PT acts as the identity on the line CvT and as 0 on every other Young line of size n. Since GZ(n)=⨁SCPS is the algebra of operators diagonal in the Young basis by [F1], the element PT equals the idempotent PT of [F1], namely the rank-one projection onto CvT. In particular PT2=PT and PT≠0.

5.1step 4.1F1

Orthogonality and the partition of unity are inherited from [F1]: for T≠T′ the idempotents PT,PT′ of [F1] multiply to 0, and ∑TPT=1 over the standard tableaux of size n.

6.1step 1.1step 4.1step 5.1step 2.3discharge-induction∎

Steps 1.1, 2.1-2.3, 3.1 and 4.1 are the base, the successor and the conclusions of an induction on n; therefore the recursive formula defines the tableau idempotents for every n, with all properties asserted.

Remarks

  • Interpolation at the spectrum. The factor is the Lagrange polynomial that takes the value 1 at the content cT(n) and vanishes at the other contents in A(μ); the contents in A(μ) are pairwise distinct by [F3], and they are the eigenvalues of Xn on the lines over T↓[n−1] by [F2]. This is Garsia's recursion for the seminormal units, stated here for the tableau idempotents of the diagonal algebra.

  • Integrality fails only at the denominators. Over Z the formula must be cleared of denominators; over C the rational coefficients are harmless. The first nontrivial denominator occurs for n=2: the addable contents of (1) are 1,−1, giving the projectors (1+X2)/2 and (1−X2)/2.

  • Choice. The recursion selects no object: the addable node carrying n in a given tableau is determined by that tableau, and the idempotents are built from the fixed chain.

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The relative centralizer is generated by the previous centre and the last Jucys-Murphy element

Statement

Let n≥2 and let Z(C[Sn],C[Sn−1])={z∈C[Sn]:zh=hz for every h∈Sn−1} be the centralizer of C[Sn−1] in C[Sn]. Then Z(C[Sn],C[Sn−1])=⟨Z(C[Sn−1]),Xn⟩, the subalgebra generated by the centre of C[Sn−1] and the element Xn. Consequently Z(C[Sn])⊆⟨Z(C[Sn−1]),Xn⟩, because the centre of C[Sn] is contained in the centralizer.

Facts & Assumptions

Given: The chain S1⊂⋯⊂Sn, the subalgebra C[Sn−1]⊆C[Sn], the centre Z(C[Sn−1]) (The center Z(k[G]) of the group algebra) and Xn=∑j<n(j n) (The Jucys-Murphy elements of the symmetric group algebra).

[F1]

For every finite-dimensional representation V of a finite group G over an algebraically closed field of characteristic zero the centre Z(C[G]) acts by a scalar on each irreducible constituent, the scalar being constant on isomorphic constituents; the algebra itself decomposes as ∏λ⊢mEnd⁡(Vλ) for G=Sm, and endomorphisms of an irreducible are scalars (If k is algebraically closed and char⁡k∤∣G∣, then k[G]≅∏i=1rMni(k), Over an algebraically closed field, every endomorphism of an irreducible representation is scalar).

[F2]

The complex Specht modules Vμ=SCμ, μ⊢m, are a complete list of pairwise inequivalent irreducible complex Sm-modules, and for λ⊢n the restriction Res⁡Sn−1SnVλ≅⨁x∈Rem⁡(λ)Vλ−x is multiplicity-free (Specht modules classify the complex irreducibles of Sn, The complex Specht restriction branching rule).

[F3]

siXn=Xnsi for 1≤i≤n−2, hence Xn commutes with every element of C[Sn−1] (Local relations between the Jucys-Murphy elements and adjacent transpositions).

[F4]

For a partition μ, distinct addable nodes have distinct contents, so the map sending λ=μ+x to the content c(x) is injective on the set of λ⊢n containing μ (Distinct addable nodes of a partition have distinct contents).

[F5]

XnvT=cT(n)vT for every standard tableau T of size n, the eigenvalue being the content of the node carrying n; the eigenvalue of Xn on the Sn−1-irreducible copy Vμ⊆Vμ+x is therefore the content c(x), independent of T (The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors).

Proof

technique · direct
1.1F3givenalgebra

By [F3] the element Xn commutes with C[Sn−1]; every z∈Z(C[Sn−1]) commutes with every element of C[Sn−1] by definition of the centre. Hence Xn and all of Z(C[Sn−1]) lie in Z(C[Sn],C[Sn−1]), and since that set is a subalgebra, ⟨Z(C[Sn−1]),Xn⟩⊆Z(C[Sn],C[Sn−1]).

1.2F2given

Write E for the set of pairs (μ,λ) with μ⊢n−1, λ⊢n and μ⊆λ; equivalently E={(μ,μ+x):x∈Add⁡(μ)}. For μ⊢n−1 let Wμ denote the μ-isotypic component of the multiplicity-free sum W:=⨁λ⊢nVλ restricted to Sn−1; by [F2] it is the direct sum of the copies Vμ⊆Vλ over the pairs (μ,λ)∈E.

2.1F1F2step 1.2algebra

Structure of the centralizer. By [F1] applied to Sn, an element z∈C[Sn] corresponds to a tuple (zλ)λ⊢n with zλ∈End⁡(Vλ), and z lies in Z(C[Sn],C[Sn−1]) exactly when each zλ commutes with the Sn−1-action on Vλ. By [F2] and [F1] the commutant of Sn−1 in End⁡(Vλ) is ∏x∈Rem⁡(λ)C idVλ−x: restriction is multiplicity-free; any nonzero map between two irreducible summands would be an isomorphism (its kernel and image are invariant), contrary to their distinct shapes, so off-diagonal maps vanish; by Schur's lemma an Sn−1-endomorphism of each irreducible summand Vλ−x is a scalar. Hence evaluation on the copies induces an algebra isomorphism Z(C[Sn],C[Sn−1])→CE, z↦(z(μ,λ))(μ,λ)∈E, where z(μ,λ) is the scalar by which z acts on the copy of Vμ inside Vλ; it is injective because zero scalars on every restriction summand make every operator zλ zero, and the Wedderburn product isomorphism in [F1] then gives z=0, and surjective by [F1] because the scalars on the finitely many copies may be prescribed independently.

3.1F5step 2.1algebra

The image A of ⟨Z(C[Sn−1]),Xn⟩ under the isomorphism of step 2.1 is the unital subalgebra of CE generated by the evaluations of the two generating pieces: an element z∈Z(C[Sn−1]) acts on every copy Vμ by the central character value ωμ(z) of the irreducible Vμ; and Xn acts on the copy (μ,λ)=(μ,μ+x) by the scalar c(x) by [F5].

4.1F1F2step 3.1algebra

Separation of edges with distinct predecessor. Let (μ,λ),(μ′,λ′)∈E with μ≠μ′. The central idempotent eμ∈Z(C[Sn−1]) of the Wedderburn factor End⁡(Vμ) acts as 1 on Vμ and as 0 on Vμ′, since μ≠μ′ and the irreducible modules are inequivalent; by step 3.1 the element eμ therefore separates the two edges.

4.2F4F5step 3.1algebra

Separation of edges with the same predecessor. Let (μ,λ),(μ,λ′)∈E with λ≠λ′; write λ=μ+x, λ′=μ+x′ with distinct addable nodes x≠x′ of μ. By [F4] their contents differ, c(x)≠c(x′), so by step 3.1 the element Xn assumes the distinct values c(x),c(x′) on the two edges and separates them.

5.1step 4.1step 4.2algebra

A unital subalgebra of CE that separates the points of the finite set E is all of CE: indeed, for each e∈E and each e′≠e separation gives ae′∈A with ae′(e)≠ae′(e′), and then be:=∏e′≠e(ae′−ae′(e′)⋅1) lies in A, satisfies be(e)≠0 and be(e′′)=0 for e′′≠e, and is therefore a nonzero multiple of the standard basis idempotent δe; hence every δe∈A and A=CE.

6.1step 5.1step 2.1algebra

By steps 4.1 and 4.2 the subalgebra A of step 3.1 separates every pair of distinct edges, so step 5.1 gives A=CE. Since the evaluation map of step 2.1 is an isomorphism, the preimage of CE is the whole centralizer; hence ⟨Z(C[Sn−1]),Xn⟩=Z(C[Sn],C[Sn−1]).

7.1step 6.1givenalgebra∎

Every central element of C[Sn] commutes with C[Sn−1], so Z(C[Sn])⊆Z(C[Sn],C[Sn−1])=⟨Z(C[Sn−1]),Xn⟩ by step 6.1.

Remarks

  • The dimension count. The isomorphism of step 2.1 gives dim⁡Z(C[Sn],C[Sn−1])=#E=∑μ⊢n−1#Add⁡(μ)=∑λ⊢n#Rem⁡(λ), the number of edges of the Young graph between levels n−1 and n. At n=3 this is 4, matching the direct commutant computation in C[S3].

  • Commutativity. The centralizer is the algebra of functions on the finite set E, hence commutative; this is the content of The centralizer of C[Sn−1] in C[Sn] is commutative, and the isomorphism of step 2.1 makes it transparent.

  • Generators and the top centre. The centres of the subgroup chain generate GZ(m) (The Gelfand-Tsetlin algebra of the symmetric group chain). The theorem identifies the relative centralizer with the algebra generated by the previous centre and Xn, and puts the top centre inside that algebra; the proof uses no symmetric-function input.

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Young's seminormal form from the Jucys-Murphy eigenlines

Statement

Let n≥1, λ⊢n, and Tλ be the standard row-filled tableau of shape λ. Fix 0≠v0∈LTλ, where LT is the Young line of T. Let σT be the unique permutation carrying Tλ to T, put ℓ(T):=inv⁡(σT), and define vT:=PTσTv0. These vectors are nonzero and form a basis of SCλ. For si=(i i+1) and r=cT(i+1)−cT(i), the same-row and same-column cases give sivT=vT and sivT=−vT, respectively. Otherwise T′=siT is standard and ∣r∣>1. When ℓ(T′)=ℓ(T)+1, sivT=vT′+r−1vT,sivT′=(1−r−2)vT−r−1vT′. When ℓ(T′)=ℓ(T)−1, the equivalent formulas in the original ordering are sivT=(1−r−2)vT′+r−1vT,sivT′=vT−r−1vT′. In particular the matrices of the Coxeter generators in this basis are rational.

Facts & Assumptions

Given: n,λ,Tλ, its nonzero Young vector v0, and the Young projections PT and lines LT in SCλ.

[F1]

The Young lines form a basis of each complex Specht module, and PTv=δTSv for v∈LS. (The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis)

[F2]

On LT, Xk acts by cT(k). The content vector uniquely determines a standard tableau, and these are exactly the joint weights in the multiplicity-free sum of complex Specht modules. (The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors, The content of a node and the content vector of a standard tableau)

[F3]

The local relations give Xisi=siXi+1−1, Xi+1si=siXi+1, and Xjsi=siXj for j∉{i,i+1}; also si2=1. (Local relations between the Jucys-Murphy elements and adjacent transpositions)

[F4]

Standard tableaux increase along rows and columns; the row-filled tableau orders the nodes row by row. Consecutive entries in a common row or column occupy adjacent nodes, with content difference +1 or −1. (Tableaux and standard tableaux, The content of a node and the content vector of a standard tableau, Partitions, English diagrams, and conjugation)

[F5]

The multiset of node contents determines a partition. (A partition is determined by the multiset of its node contents)

Proof

technique · local eigenvector calculation and reduced-chain normalization
1.1F4algebra

Swapping consecutive entries in different rows and columns preserves standardness: every neighbour other than the swapped entry is either smaller than both entries or larger than both. Such nodes must be incomparable in the northwest order, since comparable nodes in different rows and columns would have an intermediate node with entry strictly between i and i+1. Their row and column differences therefore have opposite signs, so ∣cT(i+1)−cT(i)∣≥2. In a common row or column the nodes are adjacent and the difference is +1 or −1 by [F4]. Thus the axial distance never vanishes.

2.1F1F2F3step 1.1algebra

For 0≠v∈LT, put a=cT(i), b=cT(i+1) and r=b−a. By [F3], u:=(si−r−1)v is a joint eigenvector with the weight of T having coordinates i,i+1 exchanged: Xiu=bu, Xi+1u=au, and the other eigenvalues are unchanged. If the nodes are in different rows and columns, [F2] identifies this weight with T′=siT. Moreover u≠0, since u=0 would imply siv=r−1v and then v=si2v=r−2v, contrary to ∣r∣>1. Hence siLT⊆LT⊕LT′, and its component in LT′ is nonzero.

2.2F4step 1.1algebra

A reduced admissible chain joins Tλ to each T. To construct it in reverse, let the last node in row order carry k in T. Swap k with k+1, then k+1 with k+2, through n. Every value larger than the current value in that node is in a different row and column: entries in its own row or column are smaller by standardness. The swaps are therefore admissible by step 1.1. In the row-reading word each swap moves the larger of two consecutive values from an earlier position to the final position, decreasing its inversion count by exactly one; all other inversion comparisons are unchanged. Remove the final node and entry n and repeat. The process reaches Tλ after exactly ℓ(T) swaps, since the row-reading word is the one-line notation of σT and the final word has no inversions. Reversing this chain gives the asserted reduced chain.

3.1F2F4F5step 2.1algebra

In the same-row or same-column case, the exchanged weight is not a tableau weight. Indeed, uniqueness of reconstruction from contents fixes the prefix through i−1, while equality of the content multisets through i+1 fixes that prefix shape by [F5]. Thus the two new nodes must be the original nodes of i,i+1, with their entries exchanged. The node originally carrying i+1 cannot be added first, because its immediate left or upper neighbour is the still-absent node of i. This violates standardness. By [F2] the vector u of step 2.1 is zero, giving siv=r−1v, hence +v in the row case and −v in the column case.

4.1F1step 2.1step 3.1step 2.2algebra

Expand σTv0 along such a reduced chain of length L=ℓ(T) using [F1] and steps 2.1 and 3.1. At each factor a vector in a Young line either stays in that line or passes to its admissible neighbour; every neighbour changes the inversion count by one, and the component passing to it is nonzero by step 2.1. To reach a line of inversion count L after L factors, every factor must pass to the neighbour and increase the count. This unique sequence is the reduced chain to T, and its product of nonzero coefficients is nonzero. All other resulting lines have length less than L. Therefore vT=PTσTv0≠0 and σTv0−vT is a linear combination of lines LR with ℓ(R)<ℓ(T). The permutation σT is uniquely determined by the fillings, so this definition does not depend on a reduced expression.

5.1F1F3step 2.1step 3.1step 4.1algebra

Suppose T′=siT is standard and ℓ(T′)=ℓ(T)+1. The unique permutations obey σT′=siσT. By step 4.1, write σTv0=vT+w, with w supported on lines of length strictly less than ℓ(T). Steps 2.1 and 3.1 show that siw is supported on lines of length at most ℓ(T), so PT′siw=0. Hence vT′=PT′siσTv0=PT′sivT. Together with step 2.1 this gives sivT=vT′+r−1vT. Applying si once more and using si2=1 yields sivT′=(1−r−2)vT−r−1vT′.

6.1F1step 3.1step 4.1step 5.1algebra∎

If T′ is shorter, apply step 5.1 to the pair (T′,T) with axial distance −r. It gives sivT′=vT−r−1vT′ and sivT=(1−r−2)vT′+r−1vT, as stated. The vectors vT form a basis by [F1] and step 4.1. Steps 3.1, 5.1 and this reverse reading give rational matrices for every generator, with no zero denominator. They are matrices of the actual group action, so satisfy all Coxeter relations and define a rational representation whose complexification is the given Specht module. The chain construction and projections are finite; no arbitrary-index choice is used.

Remarks

The normalization uses the unique label permutation σT, not a choice of reduced word. The length condition specifies which off-diagonal coefficient equals 1. The reduced-chain expansion in steps 4.1-5.1 supplies the compatibility needed for all adjacent pairs simultaneously; compare Okounkov–Vershik, Lemma 5.4 and Remark 5.6, printed pp. 20–21, and equations (6.1)–(6.4), printed pp. 22–23.

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The Jucys-Murphy elements generate the Gelfand-Tsetlin algebra

Statement

Let n≥1. Then GZ(n)=C[X1,…,Xn], the unital subalgebra generated by the Jucys-Murphy elements; this algebra is the diagonal algebra in the Young basis and is a maximal commutative subalgebra of C[Sn].

Facts & Assumptions

Given: The Gelfand-Tsetlin algebra GZ(n)=⟨Z(C[S1]),…,Z(C[Sn])⟩ and the Jucys-Murphy elements X1=0, Xk=∑j<k(j k) for 2≤k≤n (The Gelfand-Tsetlin algebra of the symmetric group chain, The Jucys-Murphy elements of the symmetric group algebra, The center Z(k[G]) of the group algebra).

[F1]

GZ(n)=⨁TCPT over the standard tableaux T of size n, where the PT are nonzero pairwise orthogonal idempotents with ∑TPT=1 projecting onto the Young lines; GZ(n) is a maximal commutative subalgebra of C[Sn] and is the diagonal algebra in the Young basis (The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis).

[F2]

Every PT is a polynomial in X1,…,Xn with rational coefficients, by the interpolation recursion PT=PT↓[n−1]∏c∈A(μ), c≠cT(n)(Xn−c)/(cT(n)−c) (Primitive tableau idempotents by Jucys-Murphy interpolation).

[F3]

Xk=Tk−Tk−1 for 2≤k≤n, where Tm=∑1≤i<j≤m(i j) is the sum of all transpositions of Sm; Tm is a class sum, hence central in C[Sm], and T1=0 (The Jucys-Murphy elements of the symmetric group algebra, For a finite group, the class sums form a basis of Z(k[G])).

Proof

technique · direct
1.1F1F2algebra

Inclusion GZ(n)⊆C[X1,…,Xn]. By [F2] every PT lies in C[X1,…,Xn], and by [F1] the PT span GZ(n); hence every element of GZ(n) is a polynomial in the Xk.

1.2F1F3givenalgebra

Inclusion C[X1,…,Xn]⊆GZ(n). The element X1=0 lies in GZ(n); for k≥2, [F3] writes Xk=Tk−Tk−1 as the difference of a central element of C[Sk] and a central element of C[Sk−1], both of which lie in the generating centres of GZ(n). Since GZ(n) is a subalgebra, it contains every polynomial in the Xk.

2.1F1step 1.1step 1.2algebra∎

The two inclusions give GZ(n)=C[X1,…,Xn], the algebra generated by the Jucys-Murphy elements; by [F1] this algebra equals ⨁TCPT, the diagonal algebra in the Young basis, and is maximal commutative in C[Sn]. Finally C[X1,…,Xn] is reduced and finite-dimensional: it is the algebra of functions on the finitely many content vectors of the standard tableaux, of dimension the number of standard tableaux of size n.

Remarks

  • Where maximality comes from. The maximal-commutativity assertion is inherited from the diagonal-algebra theorem and not reproved here; the content of the theorem is the equality GZ(n)=C[X1,…,Xn], i.e. that the chain of centres and the commuting family of Jucys-Murphy elements generate the same algebra.

  • No centre-generation input. The inclusion ⊆ uses the interpolation formula for the path idempotents rather than the classical generation of the centre by one-cycle class sums; the inclusion ⊇ uses only Xk=Tk−Tk−1 and the centrality of the transposition sums. No symmetric-function input and no choice principle is used.

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Young's orthogonal form from the seminormal rescaling

Statement

Rescale each Young vector of the previous item to a unit vector for the positive-definite invariant inner product on the Specht module induced from the tabloid form, chosen with positive square roots. Then for T with T′=siT standard and i,i+1 in different rows and columns of T, in the phasing of the previous item in which T′ is the longer tableau, the matrix of si on the ordered basis (vT,vT′) is the orthogonal symmetric matrix (r−11−r−21−r−2−r−1),r=cT(i+1)−cT(i), while the same-row and same-column cases remain the scalars +1 and −1. In particular each si acts by a real orthogonal (hence unitary) involution on each complex Specht module with respect to this inner product, and the resulting matrices form Young's orthogonal representation of Sn.

Facts & Assumptions

Given: The Specht module SCλ=Vλ⊆Mλ inside the tabloid module over C (Column antisymmetrizers, polytabloids, and Specht modules), the Hermitian tabloid product, and the seminormal Young basis vectors vT of the previous item (Young's seminormal form from the Jucys-Murphy eigenlines).

[F1]

The tabloid product ⟨⋅,⋅⟩ is a Hermitian form on Mλ which is positive definite, so ⟨x,x⟩>0 for x≠0, and Sn-invariant, so each σ∈Sn acts unitarily and has adjoint σ−1 (Invariant Hermitian product on a tabloid module).

[F2]

Sλ∩(Sλ)⊥={0}: the restriction of the tabloid product to Sλ is nondegenerate, hence, being the restriction of a positive definite form, positive definite (Complex Specht modules have nondegenerate Hermitian self-pairing, Invariant Hermitian product on a tabloid module).

[F3]

In the seminormal normalization of the previous item, if T′=siT is standard with i,i+1 in different rows and columns of T and T′ the longer tableau, then r=cT(i+1)−cT(i)∉{0,±1} and sivT=vT′+r−1vT, sivT′=(1−r−2)vT−r−1vT′; if i,i+1 lie in the same row or column then sivT=±vT (Young's seminormal form from the Jucys-Murphy eigenlines).

[F4]

si2=1 in Sn; consequently a unitary involution is self-adjoint, si∗=si. [F1, given]

[F5]

Distinct Young lines have distinct joint content vectors, and Xk acts on each line by its real node content. (The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors, The content of a node and the content vector of a standard tableau)

Proof

technique · direct
1.1F1F2F3givenalgebra

Let T have T′=siT standard with i,i+1 in different rows and columns, in the phasing of [F3]. The vectors vT,vT′ are nonzero, so by [F2] their norms ∥vT∥=⟨vT,vT⟩ and ∥vT′∥ are positive real numbers; define uT:=vT/∥vT∥ and uT′:=vT′/∥vT′∥.

2.1F1F3F5step 1.1algebra

Matrix in the unit basis. Each Xk is self-adjoint by [F1], since it is a sum of transpositions, which are unitary involutions. Distinct Young lines have distinct joint content vectors by [F5], so some self-adjoint Xk has different eigenvalues on them; the identity ⟨Xkv,w⟩=⟨v,Xkw⟩ then makes them orthogonal. Thus all the unit vectors uT form an orthonormal basis. Write A for the matrix of si in (vT,vT′) and B for its matrix in (uT,uT′). Since uT=vT/∥vT∥, set D=diag⁡(∥vT∥−1,∥vT′∥−1); then B=D−1AD. By [F3], A=(r−11−r−21−r−1),B=(r−1(1−r−2)∥vT∥/∥vT′∥∥vT′∥/∥vT∥−r−1).

2.2F3step 1.1algebra

Same row and same column. If i,i+1 lie in the same row or column of a standard tableau, [F3] gives sivT=±vT with the sign +1 in the row case and −1 in the column case; rescaling by a positive norm does not change these scalars.

3.1F1F4step 2.1algebra

Symmetry. By [F4] and [F1] the operator si is a unitary involution, hence self-adjoint; in the orthonormal basis (uT,uT′) its matrix B therefore satisfies B=B∗, the conjugate transpose of B. Since B11=r−1 and B22=−r−1 are real, this forces B21=B12‾ and ∣B12∣=∣B21∣.

4.1F3step 2.1step 3.1algebra

The off-diagonal entries are positive and equal. By step 2.1, B21=∥vT′∥/∥vT∥>0, so self-adjointness in step 3.1 makes both off-diagonal entries the same positive real number c. The (1,1) entry of B2=I gives r−2+c2=1, hence c=1−r−2, with ∣r∣>1 by [F3]. In particular ∥vT′∥/∥vT∥=1−r−2, and B is the displayed symmetric orthogonal matrix.

5.1step 4.1F2algebra

Orthogonality. The matrices B of step 4.1 are real, symmetric and satisfy B2=I, hence are orthogonal with determinant −r−2−(1−r−2)=−1; the unit basis was chosen with positive square roots, and the common phase of the initial vector does not affect these matrices. In particular each si acts by a real orthogonal involution on each Vλ for the restricted inner product.

6.1step 2.2step 5.1F3givenalgebra∎

Representation. The matrices so obtained are the matrices of the actual elements si∈Sn in a basis of Vλ, so they satisfy the Coxeter relations si2=1 and sisi+1si=si+1sisi+1 and generate a representation equivalent to Vλ; this is Young's orthogonal representation.

Remarks

  • Positive rescaling. The off-diagonal entry is fixed by B21=∥vT′∥/∥vT∥>0 and self-adjointness; this gives the source's equation (6.5). A common phase of the initial vector remains harmless.

  • Positivity of the form. The argument uses positive definiteness of the restricted form, which follows from the published nondegeneracy statement; no appeal to complete reducibility or to a general averaging argument over C is made beyond the tabloid product itself.

  • Consistency with the seminormal block. For r=2 the matrix is (1/23/23/2−1/2), the block computed on the examples page for shape (2,1).

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Symmetric polynomials in the Jucys-Murphy elements give exactly the centre

Statement

Let n≥1 and let f∈C[y1,…,yn] be a symmetric polynomial. Then (i) f(X1,…,Xn)∈Z(C[Sn]); and (ii) conversely, for every central element z∈Z(C[Sn]) there is a symmetric polynomial f with z=f(X1,…,Xn). In other words, the symmetric polynomial evaluations of the Jucys-Murphy elements are exactly the central elements of the symmetric group algebra.

Facts & Assumptions

Given: The Jucys-Murphy elements X1,…,Xn, and for each standard tableau T of size n the Young line CvT with XkvT=cT(k)vT (The Jucys-Murphy elements of the symmetric group algebra, The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors).

[F1]

Hence for every polynomial f∈C[y1,…,yn] the element f(X1,…,Xn) acts on CvT by the scalar f(cT(1),…,cT(n)) (The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors).

[F2]

C[Sn]≅∏λ⊢nEnd⁡(Vλ), the factors being indexed by the irreducible modules Vλ, and an element is central if and only if it acts by a scalar on each irreducible; the central elements form the centre Z(C[Sn]) (If k is algebraically closed and char⁡k∤∣G∣, then k[G]≅∏i=1rMni(k), Over an algebraically closed field, every endomorphism of an irreducible representation is scalar, The center Z(k[G]) of the group algebra).

[F3]

The multiset of entries of Cont⁡(T) is the multiset of contents of the shape of T; if λ,μ⊢n have the same multiset of node contents, then λ=μ (The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors, A partition is determined by the multiset of its node contents).

[F4]

Over C the substitution Pk↦pk, k=1,…,n, is an isomorphism from the polynomial ring in n variables onto the symmetric polynomials, so every symmetric polynomial in the variables is a polynomial in the first n power sums; the power sums of a multiset are determined by its elementary symmetric polynomials through Newton's identities with k ek=∑i=1k(−1)i−1ek−ipi (If n! is invertible, then p1,…,pn freely generate the symmetric-polynomial ring, Newton's identities: kek=∑i=1k(−1)i−1ek−ipi, Power sums pk and complete homogeneous symmetric polynomials hk, Symmetric polynomials as the invariants of variable permutations).

Proof

technique · direct
1.1F1F2F3algebra

Part (i). Let f be symmetric and let T,T′ be standard tableaux of the same shape λ. By [F3] the vectors Cont⁡(T) and Cont⁡(T′) are permutations of the same multiset, so symmetry of f gives f(Cont⁡(T))=f(Cont⁡(T′)); by [F1] the element f(X) acts on every Young line of shape λ by the same scalar, hence on the whole irreducible Vλ by that scalar. By [F2] an element acting by scalars on every irreducible is central, so f(X1,…,Xn)∈Z(C[Sn]).

1.2F3F4algebra

Part (ii), coordinates and their distinctness. For a partition λ⊢n put qλ:=(p1(λ),…,pn(λ))∈Cn, where pk(λ):=∑x∈[λ]c(x)k is the k-th power sum of the multiset of node contents. If qλ=qμ, then pk(λ)=pk(μ) for k≤n, and Newton's identities of [F4] recursively express ek in terms of p1,…,pk over C, so ek(λ)=ek(μ) for k≤n; the monic polynomial ∏x∈[λ](t−c(x))=tn−e1(λ)tn−1+⋯+(−1)nen(λ) then equals ∏x∈[μ](t−c(x)), so the two content multisets coincide and λ=μ by [F3]. Hence the p(n) points qλ are pairwise distinct.

2.1step 1.2F2algebra

Lagrange interpolation. Let z∈Z(C[Sn]) act on Vλ by ζλ, as in [F2]. For each ordered pair λ≠μ, let j(λ,μ) be the least index with qλ,j≠qμ,j; it exists by step 1.2. Define F(y1,…,yn):=∑λ⊢nζλ∏μ≠λyj(λ,μ)−qμ,j(λ,μ)qλ,j(λ,μ)−qμ,j(λ,μ). Every denominator is nonzero by its selection. The product indexed by λ is 1 at qλ and 0 at every qν with ν≠λ, because its factor indexed by μ=ν vanishes there. Thus F(qλ)=ζλ for every partition, including n=1, when the product is empty.

3.1F1F3F4step 2.1algebra

Substitution. By [F4] the power sums p1,…,pn in the variables X1,…,Xn generate the symmetric polynomials; define f to be the symmetric polynomial F(p1,…,pn) obtained by substituting Pk↦pk in the polynomial F(P1,…,Pn). Then f is symmetric and f(X1,…,Xn) acts on CvT by F(p1(λ),…,pn(λ))=F(qλ)=ζλ, where λ=shape⁡(T) and pk(λ)=∑jcT(j)k by [F3].

4.1step 1.1step 3.1F2algebra∎

The difference f(X1,…,Xn)−z acts by ζλ−ζλ=0 on every Vλ, hence is zero by [F2]; therefore z=f(X1,…,Xn) with f symmetric. With step 1.1 this proves both directions.

Remarks

  • The finite coordinates. Only the p(n) points qλ of the partitions of n are used; the interpolation degree can be bounded by p(n)−1 in each variable, and the construction is the converse of Garsia's Theorem 5.1 in the form recorded by the source.

  • Where the content lemma enters. The distinctness of the points qλ uses that the content multiset determines the partition; this is the only place where the shape is recovered, and it fails for nothing: the lemma is exactly a partition-level statement.

  • Elementary symmetric coordinates. The same argument works with the elementary symmetric polynomials of the contents in place of the power sums, since the two coordinate systems determine each other over C; the power sums are used because the substitution theorem for them is recorded in the library.

5 · Examples, counterexamples and false statements

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