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Jucys–Murphy Elements and Seminormal Forms
1 · Prerequisites
- Algebraic Closure, Embeddings, and Separability
- Algebraic Extensions, Extension Degree, and Finite Fields
- Binary Operations, Monoids, Groups and Subgroups
- Braided and Symmetric Monoidal Categories
- Chain Conditions, Semisimple Modules and the Wedderburn–Artin Theorem
- Characters and the Orthogonality Relations
- Composition Series, the Jordan–Hölder Theorem and Solvable Groups
- Congruences, the Integers Modulo n and the Chinese Remainder Theorem
- Conjugacy in Sₙ, Generation, and the Simplicity of Aₙ
- Construction of the Natural Numbers
- Construction of the Real Numbers via Cauchy Sequences
- Construction of the Real Numbers via Dedekind Cuts
- Continuity, IVT, EVT, and Uniform Continuity
- Cosets, Index and Lagrange's Theorem
- Countability and Uncountability
- Cyclic Groups and Direct Products
- Determinants of Matrices over a Commutative Ring
- Diagonalisation and the Minimal Polynomial
- Divisibility, Euclidean Domains, Principal Ideal Domains and Unique Factorisation
- Divisibility, Greatest Common Divisors and Bézout's Identity
- Dual Spaces, Bilinear and Quadratic Forms, and Sylvester's Law of Inertia
- Eigenvalues, Eigenvectors and the Characteristic Polynomial
- Finite Averaging and Character-Theory Prerequisites
- Finite Counting, Factorials and Binomial Coefficients
- Foundations of the Real Numbers for Analysis
- Free Groups and Presentations
- Free Modules, Exact Sequences, Projective and Injective Modules
- Group Actions, Orbits, Stabilisers and Cayley's Theorem
- Group Homomorphisms and the Isomorphism Theorems
- Hilbert Space Geometry and Riesz Representation
- Ideals, Quotient Rings and the Isomorphism Theorems for Rings
- Inner Product Spaces, Gram-Schmidt, Projections and Adjoints
- Limits of Real Functions
- Linear Independence, Bases and Dimension
- Linear Transformations, Rank-Nullity and Quotient Spaces
- Maschke's Theorem, Complete Reducibility and the Structure of k[G]
- Matrices, the Matrix of a Linear Map, and Change of Basis
- Metric Spaces
- Modules, Submodules, Quotient Modules and the Isomorphism Theorems
- Monotone Sequences, Bolzano-Weierstrass, and Cauchy Completeness
- Normal Subgroups and Quotient Groups
- Normed and Banach Spaces
- Order, Zorn's Lemma, and the Axiom of Choice
- Permutation Statistics, Inversions and Eulerian Numbers
- Polynomial Rings, the Division Algorithm and Roots
- Primes, Euclid's Lemma and the Fundamental Theorem of Arithmetic
- Relations, Functions, and Quotients
- Rings, Subrings, Integral Domains and Fields
- Rⁿ as a Normed Space; Vector-Valued Functions
- Roots, Rational Powers, and Classical Inequalities
- Sequences and Limits
- Simple Field Extensions and the Construction of the Complex Numbers
- Specht Modules and the Irreducibles of the Symmetric Group
- Splitting Fields
- Suprema and Infima
- Sylow's Theorems, p-Groups and Nilpotent Groups
- Symmetric Groups, Cycle Decomposition and the Sign Homomorphism
- Symmetric Polynomials and the Fundamental Theorem of Symmetric Functions
- Tensor Products of Modules
- The Branching Rule and the Young Graph
- The Determinant of a Linear Operator, Cofactors and Cramer's Rule
- The Fundamental Theorem of Algebra
- The Fundamental Theorem of Finite Abelian Groups
- The Galois Correspondence
- The Group Algebra and Representations of Finite Groups
- The ZFC Axioms and the Basic Set Constructions
- Topology of ℝ
- Triangularisation, Generalised Eigenspaces and Jordan Canonical Form
- Vector Spaces, Linear Subspaces, Span and Direct Sums
- Young Diagrams Tableaux and Permutation Modules
2 · Summary
This page develops the Jucys–Murphy elements 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 for and , which give the local relations on consecutive pairs. The Gelfand–Tsetlin algebra of the chain 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 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 is its content vector , 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 , proving that the Gelfand–Tsetlin algebra is exactly the algebra generated by over , 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 and , where is the axial distance . Rescaling to unit vectors for the positive-definite invariant form on the Specht module produces the symmetric orthogonal blocks with off-diagonal entry , i.e. Young's orthogonal form. The relative centralizer of in 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 .
3 · Logical flowchart
4 · Definitions, theorems and proofs
The content of a node and the content vector of a standard tableau
Definition
Let with Young diagram (Partitions, English diagrams, and conjugation), so that the nodes of are the pairs with and (rows numbered downward, columns rightward).
The content of a node is the column index minus the row index. The node therefore has content exactly when it lies on the diagonal ; the content of is , contents increase by along a row and decrease by down a column.
Now let be a standard tableau of shape (Tableaux and standard tableaux). For let be the node of carrying the entry , so that . The content vector of is the list of contents of the nodes read in the order of the entries . For the empty tableau of shape the content vector is the empty vector, the unique element of .
Remarks
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Well-definedness. A tableau of shape is a bijection , so each occupies exactly one node and the integers are determined by . The map uses the fixed row and column coordinates and the labels of : it depends only on which entry stands in which node.
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The entries of the content vector are the contents of the shape. Since is a bijection onto the nodes of , the multiset of entries of equals the multiset of node contents , independent of . 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.
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Two extreme examples. The row tableau of shape carries in , so its content vector is ; the column tableau of shape carries in , so its content vector is .
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First entries. The entry always occupies the node , because every other node has a node weakly to its left and weakly above it, whose entry would be smaller. Hence for every nonempty standard tableau . Similarly, need not be monotone in : for the tableau of shape one has .
The Gelfand-Tsetlin algebra of the symmetric group chain
Definition
For and let be the centre of the complex group algebra (The center of the group algebra, The group ring of finitely supported formal -linear combinations of group elements). We use the standard chain of symmetric groups in which is the subgroup of fixing every element of pointwise; thus is the subalgebra of spanned by , and . Each centre is thereby regarded as a subalgebra of .
The Gelfand-Tsetlin algebra of the chain is the unital subalgebra of generated by all these centres.
Remarks
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Well-definedness. Each is a -subalgebra of , hence, via the inclusion , a subset of closed under addition, multiplication and scalar multiplication; the generated subalgebra is therefore a unital subalgebra of . It is finite-dimensional because is: each is a finite-dimensional semisimple algebra (If , then is a semisimple ring), so its centre is finite-dimensional as well.
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Commutativity. Every element of is central in . If and , , then and commutes with every element of , in particular with ; hence . Thus all the generating centres commute with one another, and is a commutative subalgebra of . Only this centrality, not semisimplicity, is used.
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The top centre is included. The term shows ; in fact the centre of is the algebra generated by its class sums, and the other centres are generated by the class sums of the subgroups, so is generated by class sums of the chain together with .
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The algebra used below. is the diagonal algebra of the Young basis: The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis identifies it with over the standard tableaux of size , and The Jucys-Murphy elements generate the Gelfand-Tsetlin algebra shows that it is also the algebra generated by the Jucys-Murphy elements.
The Jucys-Murphy elements of the symmetric group algebra
Definition
Let and let be a commutative ring. In the group ring of the symmetric group on (Partitions, English diagrams, and conjugation, The symmetric group : the bijections of a set under composition, The group ring of finitely supported formal -linear combinations of group elements), where denotes the transposition of the distinct entries (The symmetric group : the bijections of a set under composition), the Jucys-Murphy elements are Each is a finite sum of group elements with coefficient , so the formula already defines an element of the integral group ring , and its image under the base change is the displayed element (Restriction of scalars and extension of scalars along a ring homomorphism ); for the element of , computed in the subgroup of permutations fixing , maps to under the inclusion . Equivalently , where is the sum of all transpositions in .
Remarks
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Well-definedness. The sum defining has the terms , each of which is an element of the subgroup , hence a basis element of the free -module ; a finite sum of basis elements is an element of independent of any ordering of the summands. The formula uses only the labels , so it is preserved by the inclusion for and by the base change . The group-ring multiplication is bilinear and sends basis elements to (The group ring is a unital -algebra with basis , and each is a unit of ). Thus the subgroup inclusions and the coefficient map preserve products and the identity.
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The identity . The transpositions of are with ; those with are exactly the transpositions of , and the remaining ones are with . Hence . For this reads , where . Since each is a sum of all transpositions of the subgroup , it is a sum of full conjugacy classes of .
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Integral normalization. Every coefficient in is , not or a fraction; no characteristic is inverted, so is defined over and over every commutative ring. This is the normalization used throughout this page; the spectral statements below specialize the coefficient ring to , but no integral identity of this page uses division.
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Centrality. The elements need not be central in . The element is always central, and for the algebra is commutative, so is central as well. For and , conjugation by sends to : these are distinct basis elements and . Thus is not central in this case. Pairwise commutativity of the is proved in The Jucys-Murphy elements commute pairwise.
Every element of is inverted by an involution of
Statement
Let , let be the stabilizer of , and let . There is with (the identity is allowed) and ; here such a self-inverse permutation is called an involution. In particular every element of is conjugate to its inverse by an element of .
Facts & Assumptions
Given: An integer and a permutation , where (Partitions, English diagrams, and conjugation).
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).
A cycle has support , sends to for and to , 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 : the bijections of a set under composition).
For every and every cycle one has (Conjugating a cycle relabels each entry: ).
Cycles with disjoint supports commute (Cycles with disjoint supports commute).
Proof
By [F1] write with the pairwise disjoint cycles of length at least . If , exactly one factor meets , say ; its support is the orbit of under , and by [F2] we may write with and distinct . If , no factor meets ; in that case put , leave the list empty and drop the discussion of .
Define by the following rules on the pairwise disjoint sets listed so far: ; for when exists; and for each remaining factor of the decomposition, for ; every element of not yet mentioned is fixed by . The listed points are distinct, so 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 is an involution; it fixes and every point outside , so and .
Conjugation by acts on each factor by [F3]: for we get , the cycle sending to , sending to and sending to , which is exactly ; for every other factor we get .
Inserting between consecutive factors gives by step 3.1. Reversing a product inverts it, so ; by [F4] the pairwise disjoint factors commute, hence . Therefore with an involution, which is the statement.
Remarks
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The source's shorter argument is incomplete as printed. The cited source proves the fact by deleting the letter from and choosing an element that conjugates the deletion to ; it then asserts that such an realizes . That step is not correct for an arbitrary such : for and one has , while . The construction above chooses the explicit cycle-reversing involution, which does satisfy ; only that corrected construction is used later, in The centralizer of in is commutative.
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No choice. For each the involution is given by explicit formulas on the finitely many cycles of , so the statement is proved without any selection principle, and the argument is integral and characteristic-free: it uses only the group structure of .
The Jucys-Murphy elements commute pairwise
Statement
For all one has in , hence in for every commutative ring ; that is, the Jucys-Murphy elements commute pairwise, and the subalgebra they generate is commutative.
Facts & Assumptions
Given: An integer , the Jucys-Murphy elements , and for each the transposition sum (The Jucys-Murphy elements of the symmetric group algebra).
, for , and therefore ; for the element of maps to under the inclusion , and the identity of the base change is a unital ring homomorphism sending to (The Jucys-Murphy elements of the symmetric group algebra).
For and distinct one has (Conjugating a cycle relabels each entry: ).
Proof
Base case. For the only element is ; for the elements are and . In both cases every pair among consists of two commuting elements, namely or the single element .
Induction hypothesis. Let and assume that commute pairwise in . By [F1] the inclusion of group rings is a unital ring homomorphism carrying these elements to the corresponding elements of , so commute pairwise in as well.
The element is central in . Indeed, for , [F2] gives for every pair , so , because is a bijection of the set of -element subsets of . Thus for every , and extending by linearity over the basis gives for every .
For compare the two expansions of . On the one hand by step 1.3; on the other hand, using [F1] and the induction hypothesis of step 1.2, , while . Subtracting the common term gives . Together with the induction hypothesis and the base case this covers every pair, so all of commute pairwise in .
Finally let be a commutative ring. The base change is a unital ring homomorphism and carries to for every by [F1]; applying it to the identity of step 2.1 gives in . Hence the subalgebra generated by the is commutative over any commutative ring.
Remarks
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Integrality and no choice. The argument takes place entirely in and uses only bilinear expansion in the group basis and the bijection 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.
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The centrality of in the subgroup. The same computation with replaced by shows that each is central in , since conjugation by permutes the transpositions of . This is the only property of used above.
A partition is determined by the multiset of its node contents
Statement
Let . If the multiset of contents equals the multiset , then .
Facts & Assumptions
Given: Partitions ; for a partition we write for its Young diagram, for its conjugate, and for the height of column (Partitions, English diagrams, and conjugation).
A node of is a pair with and ; its content is ; the rows of are weakly decreasing (Partitions, English diagrams, and conjugation).
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 on nodes.
Proof
For a partition and an integer put . A node of content has the form with , and it lies in exactly when , that is ; hence for every , the count being finite and equal to for .
Similarly, for an integer put . A node of content is with ; it lies in exactly when , that is . Hence for every .
The partition is recovered from the pair of strictly decreasing sequences and by the formula for every row index . Indeed, for each diagonal node with let be its arm and its leg; arms and legs have sizes and , and the hooks partition , because a node with lies in the arm and a node with lies in the leg . Counting row therefore gives , since means .
For each row index put , and for each column index put . The row lengths are weakly decreasing, so for all ; the column heights are weakly decreasing as well, so for all . Moreover exactly for the diagonal rows with , and exactly for the diagonal columns with , so the two multisets and have a common cardinality , the number of diagonal nodes. By steps 1.1 and 1.2 the numbers , , determine the multiplicity of every value among the , namely , and hence determine the multiset together with ; likewise the numbers , , determine .
Assume now that the multiset of contents of equals that of . Then for every integer ; by steps 1.1 and 1.2 this forces and , including the common cardinality . Writing both multisets as strictly decreasing sequences and , step 1.3 computes the row lengths of and by the same formula from the same data, so all row lengths agree and .
Remarks
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Why the diagonal data are Frobenius coordinates. The numbers and are the arm and leg lengths of the diagonal nodes, the Frobenius coordinates of ; 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 and through the diagonal counts of steps 1.1 and 1.2, is equivalent to that data.
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Sharper statement. The proof shows the two multisets and separately, not merely their union; both are needed, since the nonnegative and negative contents determine the arms and the legs respectively.
Distinct addable nodes of a partition have distinct contents
Statement
Let be a partition. If are addable nodes of , then ; equivalently the content map is injective on the set of addable nodes.
Facts & Assumptions
Given: A partition with Young diagram and set of addable nodes (Removable and addable nodes).
A node with is addable if and only if or ; the node is always addable; and these are all addable nodes. With the conventions and , the addable nodes of are exactly the nodes for the indices satisfying (Removable and addable nodes).
The content of a node is ; in particular (The content of a node and the content vector of a standard tableau).
Proof
By [F1] every addable node has the form for a unique index , where we use and ; indeed for the condition is exactly the addability criterion, and is the new-row node with .
For such an index the content of the addable node is by [F2], and the partition is weakly decreasing, so .
Let be two indices in . By weak monotonicity , and since we get , that is .
Combined with step 1.1, distinct addable nodes and with have contents differing by the strict inequality of step 2.1; hence is injective on .
Remarks
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The content is the addable-node coordinate. For an addable node the content 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.
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Empty partition. For the only addable node is , of content , so injectivity is vacuous there; the argument above applies with and .
Local relations between the Jucys-Murphy elements and adjacent transpositions
Statement
Let and put for , the Coxeter generators of . Then in , hence in for every commutative ring : (a) whenever ; (b) ; equivalently and . In particular the subalgebra generated by satisfies the local relations , , .
Facts & Assumptions
Given: An integer , an index , the adjacent transposition , the transposition sums , and the Jucys-Murphy elements (The Jucys-Murphy elements of the symmetric group algebra).
For the element of maps to under the inclusion , and each base change is a unital ring homomorphism carrying to for : the coefficient map preserves the group-basis product and the identity (The Jucys-Murphy elements of the symmetric group algebra).
The elements generate subject to the Coxeter relations; in particular and (The symmetric group has the Coxeter presentation).
For and distinct one has (Conjugating a cycle relabels each entry: ).
Proof
Case of (a). For such one has with , and fixes both letters and ; [F3] and [F2] give , hence . Summing over gives .
Case of (a). Here fixes , and [F3] gives . The map is a bijection of onto itself, because it interchanges the two elements of that set and fixes all others; hence and .
Part (b). For the two permutations and agree on , on and on and fix every other letter, hence are equal; and . Using and we therefore get by [F2]. Hence .
The product . The element is central in for every : by [F3] conjugation by sends each transposition to the transposition , and is a bijection of the two-element subsets of , so . Since and , centrality of and of gives .
Equivalent forms. Multiplying on the right by and using from [F2] gives ; multiplying that identity on the left by gives . Thus all three displayed forms of (b) hold.
Collecting steps 1.1 and 1.2 covers every , since and are the only possibilities for ; step 1.3 and step 2.1 give the three listed forms of (b); step 1.4 and [F2] give and . All these identities are equalities in , and by [F1] the base change carries them to the corresponding identities in . Hence (a) and (b) hold, and the subalgebra generated by satisfies the three listed relations.
Remarks
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Local meaning of the relations. The identity (b) says that is obtained from by conjugating with and adding , so the pair together with generates a local subalgebra satisfying the relations: on a joint eigenline of the on which acts by and by , the relation forces to act by . 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.
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What is not claimed. The statement records that the three listed relations hold in the subalgebra generated by ; 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.
The centralizer of in is commutative
Statement
Let be the centralizer of the subalgebra in . Then is a commutative subalgebra of .
Facts & Assumptions
Given: An integer , the group with its subgroup of permutations fixing , and the group algebra with basis and multiplication (Partitions, English diagrams, and conjugation, The symmetric group : the bijections of a set under composition, The group ring is a unital -algebra with basis , and each is a unit of ).
For every there is an involution with ; the proof of the cited lemma exhibits by explicit formulas on the cycles of (Every element of is inverted by an involution of ).
has the group elements as a -basis, every element has a unique expansion with finitely many nonzero coefficients, and ; coefficients of equal basis elements are equal. The inverse in reverses products: (The group ring is a unital -algebra with basis , and each is a unit of , The symmetric group : the bijections of a set under composition).
Proof
The centralizer is a -subalgebra of : it contains , is closed under addition and scalar multiplication because equality with each is preserved by these operations, and is closed under multiplication because for all whenever ; closure under multiplication is also checked on the basis expansions using [F2].
Define on the basis by and extend -linearly: . Then is an involution, since , and it is an anti-automorphism: by [F2], and the identity extends to all elements by bilinearity.
The anti-automorphism fixes every element of . Let , and fix one . By [F1] there is with . Since , comparison of the coefficient of on the two sides gives ; conjugation is a bijection, so exactly the summand indexed by contributes on the right. This equality holds for every , and therefore by [F2]. The argument compares each coefficient separately and requires no common conjugator.
For we have : the first equality is step 2.1, the second holds because is an anti-automorphism by step 1.2, and the third is step 2.1 applied to and to . Hence is a commutative subalgebra of by step 1.1.
Remarks
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Choice-free. The element is constructed in Every element of is inverted by an involution of by reversing the cycles of , so no selection principle is used; the argument also avoids Maschke's theorem and any semisimplicity input, and works verbatim with replaced by any commutative ring.
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What the centralizer contains. The centre and the element both lie in : elements of the centre commute with , and conjugating by gives , so conjugation permutes the summands of . The opposite inclusion, that is generated by these two pieces, is The relative centralizer is generated by the previous centre and the last Jucys-Murphy element.
Elementary symmetric Jucys-Murphy evaluations are cycle-count class sums
Statement
For and , where the right-hand side is the sum of all permutations of with exactly cycles (fixed points counted), grouped into conjugacy classes; it is zero for . In particular , is the sum of all transpositions, and is the sum of all -cycles.
Facts & Assumptions
Given: An integer and the Jucys-Murphy elements (The Jucys-Murphy elements of the symmetric group algebra).
For the element of maps to under the inclusion ; in particular (The Jucys-Murphy elements of the symmetric group algebra).
For the -th elementary symmetric polynomial is , with and for (The elementary symmetric polynomials ).
The cycle type of a permutation of a finite -element set is the family in which is the number of -element orbits, fixed points being recorded as -cycles; thus the cycle lengths form a partition and the number of parts is the total number of cycles, fixed points included. Cycles are written and a -cycle fixes every point outside its support (Support, fixed points, disjoint cycles, cycle length, disjoint-cycle decompositions, and cycle type, The symmetric group : the bijections of a set under composition).
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).
The Jucys-Murphy elements commute pairwise, so polynomial substitution and the commutative recursion apply. (The Jucys-Murphy elements commute pairwise)
Proof
Base case. For the list is empty, so by [F2], and the right-hand side for is the single class sum of the identity of , whose cycle type has ; for the left-hand side is of no variables, hence by [F2], and no partition has . Thus the identity holds for and all .
Induction hypothesis. Let and assume that for all one has in , the sum being when no such partition exists.
Recursion for elementary symmetric polynomials. For and , splitting the -element subsets of into those not containing and those containing gives in any commutative ring, with the convention ; the identity is trivial for as well.
First summand. For , take and in step 1.3, using [F5] and use [F1] to identify in with in : by step 1.2. Each class sum is the sum of the permutations of cycle type ; regarded in such a fixes and has one further cycle, namely , so its cycle type in has cycles; conversely every with and cycles restricts to a permutation of with cycle type and . Hence this summand equals the sum of all with and exactly cycles.
Second summand. For this summand is zero by . For , with the same substitution, , where runs over the permutations of with exactly cycles and the second identity uses step 1.2 for and [F1]. For such a and , use [F4] to write as a product of pairwise disjoint cycles and insert the fixed point as a -cycle if necessary; if is the cycle of , then evaluating on the letters shows replaces that factor by the single cycle and keep all other factors, so moves and has the same number of cycles as . The map is a bijection from these pairs onto the permutations with and cycles, with inverse : indeed lies in , the product fixes and hence lies in , and the two constructions invert one another because . Hence this summand is the sum of all with and exactly cycles, each occurring once.
Adding the two summands via step 1.3, every with exactly cycles is counted exactly once, according to whether or ; grouping by cycle type and using [F3] gives . For this reads ; for it sums the permutations with cycles, exactly the transpositions when ; when both the transposition sum and vanish; for it sums the permutations with a single cycle, the -cycles. For the left-hand side is in the variables , hence by [F2], and the right-hand side is an empty sum.
Remarks
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The identity is integral. Both sides lie in , and the proof uses only the compatibility of the with the subgroup chain and the elementary symmetric recursion; no representation theory, no characteristic-zero hypothesis, and no choice are used.
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A check of the normalization. For the sum for is the class of the identity, and for and it is the sum of the single transposition ; both match the asserted evaluations.
The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis
Statement
For and let be the central idempotent of the Wedderburn factor of , so that with pairwise orthogonal central idempotents and acts as the identity on and as on for . For a path in the Young graph (a standard tableau of size ) put the factors commuting pairwise. Then:
(i) every is a nonzero idempotent of rank one; (ii) for and ; (iii) , the algebra diagonal in the basis of the lines (the Young basis); (iv) the elements act diagonally in the Young basis, and is a maximal commutative subalgebra of .
Facts & Assumptions
Given: The chain and the Gelfand-Tsetlin algebra (The Gelfand-Tsetlin algebra of the symmetric group chain); for each the complex Specht modules , , which are the irreducible -modules up to isomorphism, pairwise inequivalent for distinct (Specht modules classify the complex irreducibles of ).
For every the group algebra is a product of matrix algebras indexed by its simple modules; by the classification this reads , and the identity of the factor is a central idempotent in such that , for all , and for every -module the element acts as the projection onto the sum of the irreducible summands of isomorphic to ; in particular acts as the identity on and as on for (If is algebraically closed and , then , Simple modules over a product of matrix rings over division rings, If , then is a semisimple ring).
For and the restriction of to is , the summands being irreducible with pairwise distinct shapes and each occurring exactly once; for one has with acting trivially (The complex Specht restriction branching rule).
Proof
The idempotents of [F1] are central in , pairwise orthogonal, sum to , and project each -module onto its -isotypic part.
The idempotents attached to different levels commute: if , then and is central in , hence commutes with every element of , in particular with .
Let and . The restriction of to is the direct sum of the distinct irreducible modules over the removable nodes ; consequently acts on as the projection onto the summand when for some , and as otherwise.
For every standard tableau of size the product is an idempotent, and whenever : distinct standard tableaux of size differ at some level , 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.
Every central element of is a linear combination of the : under the isomorphism of [F1] the centre corresponds to the product of the centres of the factors, and the centre of the matrix algebra consists of the scalars, that is, of . Hence for every , where is the scalar by which acts on .
Rank one and the sum over paths, by induction on : for every and every path of length ending at , the product acts on as a rank-one idempotent with image a line , kills every with , , and acts as the identity on , that is, in . For the unique path gives acting as the identity on by [F2], which is the rank-one projection onto the whole line. For the induction step write and ; by [F2] and step 2.1 the operator projects onto the summand , on which acts as the rank-one projection onto by the induction hypothesis, while the remaining summands of the restriction are killed; multiplying by , which is the identity on and kills the other , gives the claim for . Summing over all paths ending at and using the induction hypothesis at level together with [F1] gives . Distinct paths give distinct lines: if two paths end at 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.
The algebra equals . For the inclusion : each factor of lies in , so . For the inclusion : step 2.3 writes every element of every generating centre as , and step 3.1 writes ; substituting gives a linear combination of the for paths of length , so every generating element lies in the span, and the span is a subalgebra because by step 2.2; hence . The are linearly independent because they are nonzero and pairwise orthogonal, so the sum is direct and is commutative.
The idempotents add up to : summing the identity of step 3.1 over all and using [F1] gives .
The Jucys-Murphy elements lie in and act diagonally. For one has , where is the sum of the transpositions of (The Jucys-Murphy elements of the symmetric group algebra); any two transpositions are conjugate, since for transpositions and a permutation with , satisfies by Conjugating a cycle relabels each entry: , so is a class sum and hence central in by For a finite group, the class sums form a basis of for , while . Thus each lies in and each lies in ; also . By step 4.1 we may write , and then acts on the line by the scalar , because is the identity on its own image. Hence act diagonally in the Young basis.
Maximal commutativity. Under the isomorphism of [F1], step 3.1 shows that corresponds to the tuple whose entry in the factor , , is the rank-one projection onto the line , and whose other entries are ; since the lines for of shape are independent and number , they form a basis of . Therefore corresponds to the tuples with in the algebra of all operators on diagonal in that basis. An element commutes with every if and only if each commutes with the full diagonal algebra ; and the commutant of in is itself, because a matrix commuting with every diagonal matrix is diagonal. Hence the commutant of in is , and if is any commutative subalgebra containing , then commutes with , so and . Thus is a maximal commutative subalgebra, and with steps 4.1-5.1 all four assertions are proved.
Remarks
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The Young basis. The lines are the simultaneous eigenspaces of the Gelfand-Tsetlin algebra; choosing a nonzero vector 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 are reproduced by interpolation in Primitive tableau idempotents by Jucys-Murphy interpolation.
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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 . Nothing here uses the Axiom of Choice: all sums and products are finite and the idempotents are constructed from the fixed chain.
The transposition class sum acts on a complex Specht module by total content
Statement
Let , let , and let be the complex Specht module. Put Then is central in and acts on as the scalar If , and is its character, then For , and ; no transposition character value is asserted.
Facts & Assumptions
Given: , the complex Specht module, and the displayed transposition sum.
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 , whose coefficient at is because . (Row and column stabilizers, Young subgroups, tabloids, and permutation modules, Column antisymmetrizers, polytabloids, and Specht modules)
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)
A partition's conjugate records its column heights; its diagram consists of the nodes with . Characters are traces, and trace is linear. (Partitions, English diagrams, and conjugation, The character of a finite-dimensional complex representation, Trace is a linear functional on )
Proof
Conjugation by any permutation sends to the transposition of its two images, hence permutes the summands of . Thus is central, so its action on the nonzero finite-dimensional irreducible Specht module is an intertwiner and equals for some by [F2]. Choose the row-filled tableau of shape , and use its nonzero polytabloid . Taking the coefficient of in recovers , since that coefficient in is by [F1].
A summand indexed by a transposition and contributes to this coefficient precisely when . Put , so . If , then . The entry has the column of , and since preserves each row it also has the row of . Their row-column intersection consists of alone, so and . Thus both and fix the complement of ; each is either the identity or . Their product is exactly when one is and the other is the identity. Therefore the contributing pairs are exactly: , , of sign ; and , , of sign . These cases cannot overlap, since two distinct entries cannot share both row and column.
There are transpositions within rows and within columns. By steps 1.1 and 2.1 their difference is . Summing within every row gives the first count, and summing within every column gives the second; hence their difference is . Also and , proving every formula for . This includes : there are no row or column pairs and the transposition sum is zero.
For , all transpositions are conjugate, so their representing matrices are similar and have character value . Taking traces of the scalar action in step 3.1 gives by [F3]. Dividing by the nonzero integer proves the stated character formula. The construction and coefficient count are finite and use no choice of an arbitrary family or seminormal-basis input.
The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors
Statement
Let . (a) The elements act diagonally in the Young basis of the previous item: for every standard tableau of size and every , , and the joint eigenspaces are one-dimensional, indexed by the standard tableaux. (b) A vector occurs as the joint eigenvalue vector of a , equivalently for a standard tableau , if and only if: (1) ; (2) for every at least one of occurs among ; (3) if with , then both and occur among . The association is a bijection from the standard tableaux of size onto this set.
Facts & Assumptions
Given: The chain , the Gelfand-Tsetlin algebra , the Young lines for the standard tableaux of size , and the Jucys-Murphy elements (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 and, collectively, in the multiplicity-free sum , as in the preceding diagonal-algebra construction.
The transposition class sum acts on the complex Specht module of shape by . Its character value for is ; the denominator is not used for . 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)
The complex Specht modules are a complete irredundant list of finite-dimensional irreducible complex -modules; for the restriction (Specht modules classify the complex irreducibles of , The complex Specht restriction branching rule).
Contents, content vectors and the content of the node 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).
The Young lines of each shape give a basis of the corresponding irreducible. Each lies in and acts by a scalar on those lines; is maximal commutative (The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis).
Proof
For a standard tableau , let be the shape of its entries . The Young line lies in the corresponding irreducible summand at each level of the restriction chain by [F2] and the given diagonal-algebra construction. For , and therefore act on this line by and . Since , [F1] gives its eigenvalue as their difference, the content of the one node added at step . For , and entry occupies , of content zero. Thus for all .
Every tableau content vector satisfies (1) and (2): entry lies in , 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 have equal content, their nodes are and for . The nodes and exist because the later node does, and their entries lie strictly between and by row/column increase along paths inside the diagram. Their contents are respectively and , proving (3).
We prove the precise criterion needed to construct a tableau. Let a nonempty standard tableau have content vector and shape . An integer is an addable content exactly when (A) or occurs in , and (B) after every occurrence of , both neighbours occur later in . First suppose the diagonal of content is absent. Then . If , absence means ; content is also absent, and content occurs exactly when . Thus (A) says , exactly when is addable. If , transpose the diagram: absence means the first column has height at most , and (A) says its height is exactly , exactly when the new bottom node of content is addable. In these cases (B) is vacuous.
Suppose instead that the last node of content is , with . Any addable node of that content must be : 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 and exist. If they exist, each entry is larger than the entry of and their contents are , so (A) and (B) hold, since has the largest entry among the content- nodes. Conversely, if is absent, every content- node has : a node with would force a content- node in its own row beyond , and would be . Its column is then at most , so it is northwest of and has smaller entry. If is absent, every content- node has : would force the content- node beyond , while would be . Such a node is again strictly northwest of and has smaller entry. Thus in either absence case (B) fails at the entry of . This proves the criterion completely.
Given satisfying (1)-(3), start with entry at . Suppose its first entries have been placed in a standard tableau. Condition (2) at is (A) of the criterion, and condition (3) applied to every earlier occurrence of is exactly (B). Steps 2.1 and 3.1 therefore give an addable node of content . It is unique by [F3]. Put entry 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 . 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.
The Young lines give a basis in each 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 forces any nonzero coefficient to have that weight for every . 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 for , 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.
Primitive tableau idempotents by Jucys-Murphy interpolation
Statement
Let be a standard tableau of size , let be the shape of the restriction of to , and let be the set of contents of the addable nodes of . Set and define recursively, for , Then all displayed denominators are nonzero, is the rank-one idempotent projecting onto the Young line , each is a polynomial in with rational coefficients, and the over the standard tableaux of size are pairwise orthogonal idempotents with .
Facts & Assumptions
Given: The chain , the Jucys-Murphy elements , and, for every standard tableau of size , the Young line with the idempotents 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).
over the standard tableaux of size ; the are nonzero pairwise orthogonal idempotents with , and is one-dimensional (The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis).
for every standard tableau and every , with the content of the node carrying (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).
For a partition , the contents of distinct addable nodes are distinct, and the addable nodes of are the nodes with or , together with the new-row node (Distinct addable nodes of a partition have distinct contents, Removable and addable nodes).
The restriction of to is a standard tableau of shape that is obtained by deleting the node carrying ; conversely every standard tableau of size with is obtained by placing in an addable node of (Tableaux and standard tableaux, Removable and addable nodes).
Proof
Base case. For the only standard tableau is , the line is , and is the rank-one projection onto it with rational (indeed integer) coefficients.
Induction hypothesis. For every standard tableau of size the recursively defined element equals the idempotent of [F1], is the projection onto , and is a polynomial in with rational coefficients.
Let be a standard tableau of size and . The set of contents of addable nodes is finite and : the node carrying is an addable node of by [F4]. By [F3] the denominators , , , are nonzero integers, so the displayed product is a well-defined element of .
If is a standard tableau of size with , then the factor acts as on the line by step 1.2; hence acts as on every Young line of size whose restriction to differs from .
Now let be a standard tableau of size with , and let be the addable node of carrying in , so that by [F4] and [F2]. Then acts as the identity on by step 1.2, and the interpolation factor acts on by the scalar because acts on by by [F2].
Polynomial form. By step 1.2 the factor is a polynomial in with rational coefficients; each factor is a polynomial in with rational coefficients because by step 1.3; hence is a polynomial in with rational coefficients.
The scalar of step 2.2 equals when , and equals when : if then and every factor is ; if then places in a different addable node of , so by [F3], and the factor with has numerator while the denominator is nonzero by step 1.3.
Steps 2.1-2.3 show that acts as the identity on the line and as on every other Young line of size . Since is the algebra of operators diagonal in the Young basis by [F1], the element equals the idempotent of [F1], namely the rank-one projection onto . In particular and .
Orthogonality and the partition of unity are inherited from [F1]: for the idempotents of [F1] multiply to , and over the standard tableaux of size .
Steps 1.1, 2.1-2.3, 3.1 and 4.1 are the base, the successor and the conclusions of an induction on ; therefore the recursive formula defines the tableau idempotents for every , with all properties asserted.
Remarks
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Interpolation at the spectrum. The factor is the Lagrange polynomial that takes the value at the content and vanishes at the other contents in ; the contents in are pairwise distinct by [F3], and they are the eigenvalues of on the lines over by [F2]. This is Garsia's recursion for the seminormal units, stated here for the tableau idempotents of the diagonal algebra.
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Integrality fails only at the denominators. Over the formula must be cleared of denominators; over the rational coefficients are harmless. The first nontrivial denominator occurs for : the addable contents of are , giving the projectors and .
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Choice. The recursion selects no object: the addable node carrying in a given tableau is determined by that tableau, and the idempotents are built from the fixed chain.
The relative centralizer is generated by the previous centre and the last Jucys-Murphy element
Statement
Let and let be the centralizer of in . Then the subalgebra generated by the centre of and the element . Consequently , because the centre of is contained in the centralizer.
Facts & Assumptions
Given: The chain , the subalgebra , the centre (The center of the group algebra) and (The Jucys-Murphy elements of the symmetric group algebra).
For every finite-dimensional representation of a finite group over an algebraically closed field of characteristic zero the centre acts by a scalar on each irreducible constituent, the scalar being constant on isomorphic constituents; the algebra itself decomposes as for , and endomorphisms of an irreducible are scalars (If is algebraically closed and , then , Over an algebraically closed field, every endomorphism of an irreducible representation is scalar).
The complex Specht modules , , are a complete list of pairwise inequivalent irreducible complex -modules, and for the restriction is multiplicity-free (Specht modules classify the complex irreducibles of , The complex Specht restriction branching rule).
for , hence commutes with every element of (Local relations between the Jucys-Murphy elements and adjacent transpositions).
For a partition , distinct addable nodes have distinct contents, so the map sending to the content is injective on the set of containing (Distinct addable nodes of a partition have distinct contents).
for every standard tableau of size , the eigenvalue being the content of the node carrying ; the eigenvalue of on the -irreducible copy is therefore the content , independent of (The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors).
Proof
By [F3] the element commutes with ; every commutes with every element of by definition of the centre. Hence and all of lie in , and since that set is a subalgebra, .
Write for the set of pairs with , and ; equivalently . For let denote the -isotypic component of the multiplicity-free sum restricted to ; by [F2] it is the direct sum of the copies over the pairs .
Structure of the centralizer. By [F1] applied to , an element corresponds to a tuple with , and lies in exactly when each commutes with the -action on . By [F2] and [F1] the commutant of in is : 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 -endomorphism of each irreducible summand is a scalar. Hence evaluation on the copies induces an algebra isomorphism , , where is the scalar by which acts on the copy of inside ; it is injective because zero scalars on every restriction summand make every operator zero, and the Wedderburn product isomorphism in [F1] then gives , and surjective by [F1] because the scalars on the finitely many copies may be prescribed independently.
The image of under the isomorphism of step 2.1 is the unital subalgebra of generated by the evaluations of the two generating pieces: an element acts on every copy by the central character value of the irreducible ; and acts on the copy by the scalar by [F5].
Separation of edges with distinct predecessor. Let with . The central idempotent of the Wedderburn factor acts as on and as on , since and the irreducible modules are inequivalent; by step 3.1 the element therefore separates the two edges.
Separation of edges with the same predecessor. Let with ; write , with distinct addable nodes of . By [F4] their contents differ, , so by step 3.1 the element assumes the distinct values on the two edges and separates them.
A unital subalgebra of that separates the points of the finite set is all of : indeed, for each and each separation gives with , and then lies in , satisfies and for , and is therefore a nonzero multiple of the standard basis idempotent ; hence every and .
By steps 4.1 and 4.2 the subalgebra of step 3.1 separates every pair of distinct edges, so step 5.1 gives . Since the evaluation map of step 2.1 is an isomorphism, the preimage of is the whole centralizer; hence .
Every central element of commutes with , so by step 6.1.
Remarks
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The dimension count. The isomorphism of step 2.1 gives , the number of edges of the Young graph between levels and . At this is , matching the direct commutant computation in .
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Commutativity. The centralizer is the algebra of functions on the finite set , hence commutative; this is the content of The centralizer of in is commutative, and the isomorphism of step 2.1 makes it transparent.
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Generators and the top centre. The centres of the subgroup chain generate (The Gelfand-Tsetlin algebra of the symmetric group chain). The theorem identifies the relative centralizer with the algebra generated by the previous centre and , and puts the top centre inside that algebra; the proof uses no symmetric-function input.
Young's seminormal form from the Jucys-Murphy eigenlines
Statement
Let , , and be the standard row-filled tableau of shape . Fix , where is the Young line of . Let be the unique permutation carrying to , put , and define These vectors are nonzero and form a basis of . For and , the same-row and same-column cases give and , respectively. Otherwise is standard and . When , When , the equivalent formulas in the original ordering are In particular the matrices of the Coxeter generators in this basis are rational.
Facts & Assumptions
Given: , its nonzero Young vector , and the Young projections and lines in .
The Young lines form a basis of each complex Specht module, and for . (The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis)
On , acts by . 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)
The local relations give , , and for ; also . (Local relations between the Jucys-Murphy elements and adjacent transpositions)
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 or . (Tableaux and standard tableaux, The content of a node and the content vector of a standard tableau, Partitions, English diagrams, and conjugation)
The multiset of node contents determines a partition. (A partition is determined by the multiset of its node contents)
Proof
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 and . Their row and column differences therefore have opposite signs, so . In a common row or column the nodes are adjacent and the difference is or by [F4]. Thus the axial distance never vanishes.
For , put , and . By [F3], is a joint eigenvector with the weight of having coordinates exchanged: , , and the other eigenvalues are unchanged. If the nodes are in different rows and columns, [F2] identifies this weight with . Moreover , since would imply and then , contrary to . Hence , and its component in is nonzero.
A reduced admissible chain joins to each . To construct it in reverse, let the last node in row order carry in . Swap with , then with , through . 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 and repeat. The process reaches after exactly swaps, since the row-reading word is the one-line notation of and the final word has no inversions. Reversing this chain gives the asserted reduced chain.
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 , while equality of the content multisets through fixes that prefix shape by [F5]. Thus the two new nodes must be the original nodes of , with their entries exchanged. The node originally carrying cannot be added first, because its immediate left or upper neighbour is the still-absent node of . This violates standardness. By [F2] the vector of step 2.1 is zero, giving , hence in the row case and in the column case.
Expand along such a reduced chain of length 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 after factors, every factor must pass to the neighbour and increase the count. This unique sequence is the reduced chain to , and its product of nonzero coefficients is nonzero. All other resulting lines have length less than . Therefore and is a linear combination of lines with . The permutation is uniquely determined by the fillings, so this definition does not depend on a reduced expression.
Suppose is standard and . The unique permutations obey . By step 4.1, write , with supported on lines of length strictly less than . Steps 2.1 and 3.1 show that is supported on lines of length at most , so . Hence . Together with step 2.1 this gives . Applying once more and using yields .
If is shorter, apply step 5.1 to the pair with axial distance . It gives and , as stated. The vectors 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 , not a choice of reduced word. The length condition specifies which off-diagonal coefficient equals . 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.
The Jucys-Murphy elements generate the Gelfand-Tsetlin algebra
Statement
Let . Then 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 .
Facts & Assumptions
Given: The Gelfand-Tsetlin algebra and the Jucys-Murphy elements , for (The Gelfand-Tsetlin algebra of the symmetric group chain, The Jucys-Murphy elements of the symmetric group algebra, The center of the group algebra).
over the standard tableaux of size , where the are nonzero pairwise orthogonal idempotents with projecting onto the Young lines; is a maximal commutative subalgebra of and is the diagonal algebra in the Young basis (The Gelfand-Tsetlin algebra is the diagonal algebra of the Young basis).
Every is a polynomial in with rational coefficients, by the interpolation recursion (Primitive tableau idempotents by Jucys-Murphy interpolation).
for , where is the sum of all transpositions of ; is a class sum, hence central in , and (The Jucys-Murphy elements of the symmetric group algebra, For a finite group, the class sums form a basis of ).
Proof
Inclusion . By [F2] every lies in , and by [F1] the span ; hence every element of is a polynomial in the .
Inclusion . The element lies in ; for , [F3] writes as the difference of a central element of and a central element of , both of which lie in the generating centres of . Since is a subalgebra, it contains every polynomial in the .
The two inclusions give , the algebra generated by the Jucys-Murphy elements; by [F1] this algebra equals , the diagonal algebra in the Young basis, and is maximal commutative in . Finally 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 .
Remarks
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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 , i.e. that the chain of centres and the commuting family of Jucys-Murphy elements generate the same algebra.
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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 and the centrality of the transposition sums. No symmetric-function input and no choice principle is used.
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 with standard and in different rows and columns of , in the phasing of the previous item in which is the longer tableau, the matrix of on the ordered basis is the orthogonal symmetric matrix while the same-row and same-column cases remain the scalars and . In particular each 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 .
Facts & Assumptions
Given: The Specht module inside the tabloid module over (Column antisymmetrizers, polytabloids, and Specht modules), the Hermitian tabloid product, and the seminormal Young basis vectors of the previous item (Young's seminormal form from the Jucys-Murphy eigenlines).
The tabloid product is a Hermitian form on which is positive definite, so for , and -invariant, so each acts unitarily and has adjoint (Invariant Hermitian product on a tabloid module).
: the restriction of the tabloid product to 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).
In the seminormal normalization of the previous item, if is standard with in different rows and columns of and the longer tableau, then and , ; if lie in the same row or column then (Young's seminormal form from the Jucys-Murphy eigenlines).
in ; consequently a unitary involution is self-adjoint, . [F1, given]
Distinct Young lines have distinct joint content vectors, and 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
Let have standard with in different rows and columns, in the phasing of [F3]. The vectors are nonzero, so by [F2] their norms and are positive real numbers; define and .
Matrix in the unit basis. Each 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 has different eigenvalues on them; the identity then makes them orthogonal. Thus all the unit vectors form an orthonormal basis. Write for the matrix of in and for its matrix in . Since , set ; then . By [F3],
Same row and same column. If lie in the same row or column of a standard tableau, [F3] gives with the sign in the row case and in the column case; rescaling by a positive norm does not change these scalars.
Symmetry. By [F4] and [F1] the operator is a unitary involution, hence self-adjoint; in the orthonormal basis its matrix therefore satisfies , the conjugate transpose of . Since and are real, this forces and .
The off-diagonal entries are positive and equal. By step 2.1, , so self-adjointness in step 3.1 makes both off-diagonal entries the same positive real number . The entry of gives , hence , with by [F3]. In particular , and is the displayed symmetric orthogonal matrix.
Orthogonality. The matrices of step 4.1 are real, symmetric and satisfy , hence are orthogonal with determinant ; 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 acts by a real orthogonal involution on each for the restricted inner product.
Representation. The matrices so obtained are the matrices of the actual elements in a basis of , so they satisfy the Coxeter relations and and generate a representation equivalent to ; this is Young's orthogonal representation.
Remarks
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Positive rescaling. The off-diagonal entry is fixed by and self-adjointness; this gives the source's equation (6.5). A common phase of the initial vector remains harmless.
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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 is made beyond the tabloid product itself.
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Consistency with the seminormal block. For the matrix is , the block computed on the examples page for shape .
Symmetric polynomials in the Jucys-Murphy elements give exactly the centre
Statement
Let and let be a symmetric polynomial. Then (i) ; and (ii) conversely, for every central element there is a symmetric polynomial with . 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 , and for each standard tableau of size the Young line with (The Jucys-Murphy elements of the symmetric group algebra, The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors).
Hence for every polynomial the element acts on by the scalar (The joint spectrum of the Jucys-Murphy elements is the set of tableau content vectors).
, the factors being indexed by the irreducible modules , and an element is central if and only if it acts by a scalar on each irreducible; the central elements form the centre (If is algebraically closed and , then , Over an algebraically closed field, every endomorphism of an irreducible representation is scalar, The center of the group algebra).
The multiset of entries of is the multiset of contents of the shape of ; if have the same multiset of node contents, then (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).
Over the substitution , , is an isomorphism from the polynomial ring in variables onto the symmetric polynomials, so every symmetric polynomial in the variables is a polynomial in the first power sums; the power sums of a multiset are determined by its elementary symmetric polynomials through Newton's identities with (If is invertible, then freely generate the symmetric-polynomial ring, Newton's identities: , Power sums and complete homogeneous symmetric polynomials , Symmetric polynomials as the invariants of variable permutations).
Proof
Part (i). Let be symmetric and let be standard tableaux of the same shape . By [F3] the vectors and are permutations of the same multiset, so symmetry of gives ; by [F1] the element acts on every Young line of shape by the same scalar, hence on the whole irreducible by that scalar. By [F2] an element acting by scalars on every irreducible is central, so .
Part (ii), coordinates and their distinctness. For a partition put , where is the -th power sum of the multiset of node contents. If , then for , and Newton's identities of [F4] recursively express in terms of over , so for ; the monic polynomial then equals , so the two content multisets coincide and by [F3]. Hence the points are pairwise distinct.
Lagrange interpolation. Let act on by , as in [F2]. For each ordered pair , let be the least index with ; it exists by step 1.2. Define Every denominator is nonzero by its selection. The product indexed by is at and at every with , because its factor indexed by vanishes there. Thus for every partition, including , when the product is empty.
Substitution. By [F4] the power sums in the variables generate the symmetric polynomials; define to be the symmetric polynomial obtained by substituting in the polynomial . Then is symmetric and acts on by , where and by [F3].
The difference acts by on every , hence is zero by [F2]; therefore with symmetric. With step 1.1 this proves both directions.
Remarks
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The finite coordinates. Only the points of the partitions of are used; the interpolation degree can be bounded by in each variable, and the construction is the converse of Garsia's Theorem 5.1 in the form recorded by the source.
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Where the content lemma enters. The distinctness of the points 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.
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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 ; the power sums are used because the substitution theorem for them is recorded in the library.
5 · Examples, counterexamples and false statements
None yet.
Sources
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, section 5, printed pp. 17-22
- Garsia, Young Seminormal Representation, Murphy Elements and Content Evaluations, UCSD lecture notes (2003), section 3, printed pp. 18-25
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, sections 1-2, printed pp. 7-12
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, section 3, printed pp. 12-15
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, Lemma 2.2, printed p. 9; its deletion argument is replaced by the explicit cycle-reversal proof below
- K. Conrad, Conjugacy Classes (cycle conjugation), as cited by the published cycle-conjugation lemma
- Garsia, Young Seminormal Representation, Murphy Elements and Content Evaluations, UCSD lecture notes (2003), section 3, printed pp. 18-25, Theorem 3.1(a)
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, equation (2.1) and its following commutativity observation, printed p. 10
- Mathas-Soriano, Seminormal Forms and Gram Determinants for Cellular Algebras, J. reine angew. Math. 619 (2008) 141-173; arXiv:math/0604108, section 2, printed pp. 4-8
- Garsia, Young Seminormal Representation, Murphy Elements and Content Evaluations, UCSD lecture notes (2003), section 3, printed pp. 18-25, addable-cell notation
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, section 5, printed pp. 19-22
- Garsia, Young Seminormal Representation, Murphy Elements and Content Evaluations, UCSD lecture notes (2003), section 3, printed pp. 18-25, Theorem 3.1
- Michael Muger, Tensor Categories: A Selective Guided Tour, section 4 (Coxeter presentation of the symmetric group)
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, Theorem 2.1 and its complete coefficient-inversion proof, printed pp. 9-10
- Garsia, Young Seminormal Representation, Murphy Elements and Content Evaluations, UCSD lecture notes (2003), Theorem 5.10, printed pp. 51-52, and section 3, printed pp. 18-25
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, Proposition 1.1, Theorem 2.8 and section 3, printed pp. 7-16
- Garsia, Young Seminormal Representation, Murphy Elements and Content Evaluations, UCSD lecture notes (2003), section 2, printed pp. 12-18
- Garsia, Young Seminormal Representation, Murphy Elements and Content Evaluations, Theorem 3.2 and Remark 3.1, printed pp.19-21; coefficient argument reproduced using polytabloids instead of seminormal units
- Charlotte Chan, Representation Theory of Symmetric Groups, Definitions 3.8/3.12 and Theorem 4.4, printed pp.12-16
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, sections 1-7, printed pp. 7-25
- Garsia, Young Seminormal Representation, Murphy Elements and Content Evaluations, UCSD lecture notes (2003), Theorem 3.2, Remark 2.1 and sections 3-5, printed pp. 19-45
- Garsia, Young Seminormal Representation, Murphy Elements and Content Evaluations, UCSD lecture notes (2003), Theorems 3.4-3.5, printed pp. 22-24
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, sections 5-6, printed pp. 17-24
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, Theorem 2.8 and section 2, printed pp. 10-12
- Alexander Kleshchev, Essen Lectures: Representation Theory of Symmetric Groups, Proposition 1.2.2 (Olshanskii's lemma), case m=1, printed p. 12
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, sections 4-6, printed pp. 15-23
- Garsia, Young Seminormal Representation, Murphy Elements and Content Evaluations, UCSD lecture notes (2003), Theorems 4.2-4.4, printed pp. 26-32
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, Corollary 2.6 and Proposition 1.1, printed pp. 7-12
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, section 6, printed pp. 22-24
- James, The Representation Theory of the Symmetric Groups, Lecture Notes in Mathematics 682, Springer (1978), section 25 (Young's orthogonal form, 25.1-25.5 and Theorem 25.3), printed pp. 114-124
- Garsia, Young Seminormal Representation, Murphy Elements and Content Evaluations, UCSD lecture notes (2003), Theorem 5.1 with the converse discussion, printed pp. 32-36 and 51-52
- Okounkov-Vershik, A New Approach to the Representation Theory of the Symmetric Groups, Selecta Math. (N.S.) 2 (1996) 581-605; complete arXiv repost math/0503040, Corollary 2.6 and section 5, printed pp. 11 and 17-22