07.05.16 · representation-theory / symmetric

Wreath products and the representations of the hyperoctahedral group

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Anchor (Master): Specht 1932 Eine Verallgemeinerung der symmetrischen Gruppe; James-Kerber The Representation Theory of the Symmetric Group (1981) Ch. 4; Macdonald Symmetric Functions and Hall Polynomials (2nd ed.) Ch. I App. B

Intuition Beginner

Take a group and make copies of it, one sitting in each of slots. An element of this big group is just a list: one element of for each slot. Now bring in the permutations of , the group that reshuffles the slots. A wreath product lets you do both at once: first permute the slots, then drop a copy of into each slot. The notation is , read " wreath ".

The cleanest example replaces by the two-element group of signs, plus and minus. Each slot now carries a sign, and on top of that you may shuffle the slots. The result is the group of signed permutations: rearrange items and flip the sign of any of them. This is the hyperoctahedral group , and it is exactly the set of symmetries of an -dimensional cube.

Visual Beginner

Picture a square in the plane with corners labelled. Its symmetries either rotate the square or reflect it. Each symmetry permutes the two coordinate axes and may flip the direction of either axis. That is a signed permutation of two slots, so the square's symmetry group is .

Swapping the two axes is the part; flipping the arrow on an axis is the sign part. Combine all swaps with all sign choices and you get every symmetry of the square: there are of them.

Worked example Beginner

Let us count the hyperoctahedral group , the symmetries of an ordinary cube, slot by slot.

Step 1. There are 3 slots, the three coordinate axes. The number of ways to permute 3 slots is .

Step 2. Each slot independently carries a sign, plus or minus, so there are sign patterns.

Step 3. A signed permutation is a choice of slot-shuffle together with a choice of sign pattern, so the total count is .

That matches the known number of symmetries of a cube: 48. The general formula is . For this is , and for it is .

A single element of might send the first axis to the third axis with a flipped sign, keep the second axis in place, and send the third axis to the first axis. Writing a minus where a sign flips, this is the signed permutation that takes to .

Check your understanding Beginner

Formal definition Intermediate+

Let be a finite group and let be the symmetric group on . The symmetric group acts on the direct power by permuting coordinates: for and ,

Definition (wreath product). The wreath product is the semidirect product with respect to this action. Its underlying set is , and multiplication is

The subgroup is the base group, normal in , and the subgroup is a complement isomorphic to . The order is .

Definition (hyperoctahedral group). Taking gives the hyperoctahedral group

An element is a signed permutation: a permutation together with a sign attached to each . Concretely is the group of matrices with exactly one nonzero entry in each row and column, every such entry being or ; it is the symmetry group of the hypercube .

Conjugacy classes. Let have conjugacy classes . Each together with the cycle structure of produces, for each cycle of , a cycle product in (the ordered product of the base entries around the cycle), well defined up to conjugacy. A conjugacy class of is recorded by a function assigning to each class of a partition , where the parts of are the lengths of the cycles whose cycle product lies in , subject to . These are the -coloured partitions of .

Counterexamples to common slips

  • Order of the factors. is not . The base group is the power ; the symmetric group acts on it. Reversing the symbols changes the group.
  • Cycle products, not entries. Two base vectors paired with the same are conjugate exactly when their cycle products match up to conjugacy in , not when the individual entries match. Conjugating by an element of the base group slides entries around a cycle and changes them individually while preserving the ordered product.
  • Signs versus a single global sign. In each slot carries its own sign. The diagonal copy of (all signs equal) is a proper subgroup; the full base group has elements, not 2.

Key theorem with proof Intermediate+

The irreducibles of are built by the little-group method, the Wigner-Mackey construction for a semidirect product with abelian-or-not base, applied through the induced representation 07.01.07 and controlled by Frobenius reciprocity 07.01.08.

Theorem (classification of irreducibles of ). Let be the irreducible representations of . The irreducible representations of are indexed by -tuples of partitions with . Writing , the irreducible attached to is

where is the canonical extension of the outer tensor power of the base to , and is the Specht module of pulled back to .

Proof. The base group is normal in , so Clifford theory applies. An irreducible of restricts to as a direct sum of an -orbit of irreducibles of . The irreducibles of are the outer tensor products , indexed by functions . The quotient permutes these functions by permuting their arguments, so an -orbit is a function recorded up to relabelling of slots: equivalently a multiset assigning to each a number of slots, with .

Fix such an orbit, with representative (the first slots carry , the next carry , and so on). Its stabiliser in is the Young subgroup , so the inertia subgroup is . By Clifford theory the irreducibles of lying over the orbit of are obtained by inducing from the irreducibles of that restrict on the base to .

It remains to extend to and to list the irreducibles of over it. For each block the outer power extends canonically to a representation of : the base acts diagonally through and a slot-permutation acts by the operator that permutes the tensor factors of . One checks the cocycle identity, so this is an honest representation extending on that block. Given one extension, the irreducibles of over are , and the irreducibles of are the Specht modules , (the symmetric-group theory of 07.05.01). Taking the outer tensor product over the blocks and inducing to yields . Distinct give inequivalent irreducibles, and counting over -tuples summing to matches the number of -coloured partitions, hence the number of conjugacy classes. This exhausts .

Bridge. This classification builds toward the character theory of the hyperoctahedral group and appears again in the symmetric-function description below, where the induction is repackaged as a product of Frobenius characteristics. The foundational reason the little-group method works is that the base group is normal, so Clifford theory forces every irreducible to live over a single -orbit of base-characters; this is exactly the orbit-and-stabiliser bookkeeping that induced representations 07.01.07 and Frobenius reciprocity 07.01.08 were built to handle. The construction generalises the bijection {partitions of } {irreducibles of } of 07.05.01: taking to be the one-element group collapses and recovers the symmetric-group case, so the pattern that organises -representations is dual to the pattern here, now indexed by tuples of diagrams. Putting these together, the central insight is that the representation theory of factors into the representation theory of (which colours the slots) and the representation theory of (which fills each colour-block with a Young diagram).

Exercises Intermediate+

Advanced results Master

Theorem 1 (signed cycle type and conjugacy in ). A signed permutation decomposes into signed cycles. Each cycle has a sign equal to the product of the signs of its entries, splitting cycles into positive and negative; the conjugacy class of is recorded by a pair of partitions , where lists the lengths of the positive cycles and the lengths of the negative cycles, with . The number of conjugacy classes is therefore , equal to the number of irreducibles indexed by pairs .

This is the specialisation of the -coloured-partition description: the two conjugacy classes of produce the two partitions (cycle product ) and (cycle product ).

Theorem 2 (wreath Frobenius characteristic). Let denote the ring of symmetric functions and let carry one copy per irreducible of . There is an isometric isomorphism $$ \mathrm{ch}: \bigoplus_{n \geq 0} R(G \wr S_n) ;\xrightarrow{\ \sim\ }; \Lambda^{\otimes r}, \qquad W^{\boldsymbol{\lambda}} \longmapsto \prod_k s_{\lambda^{(k)}}\big[ X^{(k)} \big], $$ where is the representation ring, is a Schur function, and is the alphabet attached to . Induction of representations corresponds to multiplication of symmetric functions, and the inner product matching characters corresponds to the Hall inner product on each tensor factor. This is the wreath-product analogue of the Frobenius characteristic for and underlies the plethystic substitution that converts power sums of into power sums on the alphabets.

Theorem 3 (Murnaghan-Nakayama for ). The irreducible character of , evaluated on an element of signed cycle type , satisfies a border-strip recursion that removes a positive cycle of length from either or (with a sign from the border-strip height), and removes a negative cycle of length from minus the same removal from (with the type- sign convention). This refines the symmetric-group rule of 07.05.10: setting and recovers the recursion on .

Theorem 4 ( as a Weyl group). The hyperoctahedral group is the Weyl group of the root systems of type and . It acts on by permuting and sign-changing the standard coordinates, with simple reflections the adjacent transpositions for together with the sign change . The Coxeter presentation has braid relations of among and the single order-4 relation . The longest element is , and the order equals the product of the degrees of the fundamental invariants.

Theorem 5 (random walk on the cube via and the Ehrenfest connection). The simple random walk driven by single sign-flips on the base of is the Ehrenfest urn walk on the hypercube; its eigenvalues are for , the Krawtchouk spectrum, and the upper bound lemma for the abelian group gives the mixing threshold. Walks that also shuffle slots live on the full and require the pair-of-partitions character theory above to diagonalise. Diaconis uses exactly this for signed-rank statistics, where data carry a sign and a rank.

Synthesis. The wreath-product construction is the foundational reason that the representation theory of signed permutations parallels that of ordinary permutations one level up. The central insight is that a normal base group forces Clifford theory, and the little-group method then factors every irreducible into a colouring of slots by irreducibles of and a Young diagram filling each colour-block, which is exactly the bijection {tuples of partitions} {irreducibles of }. Putting these together with the Frobenius characteristic, the entire character theory becomes symmetric-function algebra on alphabets, and the Murnaghan-Nakayama recursion of 07.05.10 generalises verbatim to border strips removed from a pair of diagrams. The bridge is that is simultaneously the symmetry group of the hypercube, the Weyl group of type , and the natural home for signed statistical data, so the same pair-of-partitions index governs cube geometry, root-system combinatorics, and the hyperoctahedral random walks; this construction generalises the theory of 07.05.01 and is dual, through the characteristic map, to the plethystic structure of symmetric functions.

Full proof set Master

Proposition 1 (order of the wreath product). For a finite group , , and in particular .

Proof. As a set , a Cartesian product, so its cardinality is . The semidirect-product multiplication does not change the underlying set, only the group law. For this gives .

Proposition 2 (the base power extends to ). Let be a representation of on a space . Define an action of on by $$ \big((g_1, \dots, g_n); \sigma\big)\cdot (u_1 \otimes \cdots \otimes u_n) = g_1 u_{\sigma^{-1}(1)} \otimes \cdots \otimes g_n u_{\sigma^{-1}(n)}. $$ This is a representation of extending the outer power of the base.

Proof. Restricting to the base () gives , which is . To verify the homomorphism property, apply then to a pure tensor and compare with the action of their product . Reindexing the tensor slots shows both routes send to . The two agree because the slot-permutations compose as and the group elements multiply within each slot in the order dictated by the wreath law. Hence the assignment is a representation.

Proposition 3 (irreducible count equals conjugacy-class count for ). The number of irreducibles of equals the number of conjugacy classes, both equal to .

Proof. By Theorem 1 a conjugacy class is a pair of partitions with , and the count of such pairs is on splitting by . By the classification theorem the irreducibles are indexed by pairs with , the same count. Both equal the number of conjugacy classes by the general theorem that a finite group over has as many irreducibles as conjugacy classes, so the two indexings are matched in cardinality.

Connections Master

  • Induced representation 07.01.07. The little-group construction of the irreducibles of is induction from the inertia subgroup up to the full wreath product. Without the induced representation there is no way to assemble an irreducible of the large group from data living on a stabiliser of a base-orbit.

  • Frobenius reciprocity 07.01.08. The proof that distinct tuples give inequivalent irreducibles, and that the induced modules are themselves irreducible, runs through Frobenius reciprocity: the multiplicity of an induced module in another is computed as a restriction multiplicity on the inertia subgroup, where the orbit-stabiliser structure makes it a single Specht-module pairing.

  • Symmetric group representation 07.05.01. The wreath product theory contains the symmetric-group theory as the special case , : tuples of partitions collapse to a single partition, and is the Specht module . The slots-and-fillings picture here is the colour-graded generalisation of the partition indexing of -irreducibles.

  • Murnaghan-Nakayama rule 07.05.10. The border-strip character recursion for in Theorem 3 specialises to the symmetric-group Murnaghan-Nakayama rule when all signs are positive, so the unsigned recursion of 07.05.10 is the , corner of the signed one.

Historical & philosophical context Master

Wilhelm Specht introduced the representation theory of what he called the generalised symmetric groups in his 1932 paper Eine Verallgemeinerung der symmetrischen Gruppe [Specht 1932], extending the partition-indexed theory of that Frobenius and Young had built. The systematic treatment of arbitrary wreath products , the -coloured-partition description of conjugacy classes, and the little-group classification of irreducibles were consolidated by James and Kerber in their 1981 monograph [James-Kerber 1981], which remains the standard reference. Macdonald gave the symmetric-function formulation, with the wreath Frobenius characteristic and its plethystic substitution, in Appendix B to Chapter I of Symmetric Functions and Hall Polynomials [Macdonald 1995].

The hyperoctahedral group predates this representation theory as a geometric object: it is the symmetry group of the -cube and the cross-polytope, and it reappears as the Weyl group of the type- root systems in the Cartan-Killing classification. Persi Diaconis brought the wreath-product machinery into probability and statistics, using for signed-rank statistics and for random walks on the cube, where the pair-of-partitions characters diagonalise the relevant Markov chains [Diaconis 1988].

Bibliography Master

@article{Specht1932,
  author = {Specht, Wilhelm},
  title = {Eine Verallgemeinerung der symmetrischen Gruppe},
  journal = {Schriften des Mathematischen Seminars der Universit\"at Berlin},
  volume = {1},
  year = {1932},
  pages = {1--32},
}

@book{JamesKerber1981,
  author = {James, Gordon and Kerber, Adalbert},
  title = {The Representation Theory of the Symmetric Group},
  publisher = {Addison-Wesley},
  year = {1981},
  series = {Encyclopedia of Mathematics and its Applications},
  volume = {16},
}

@book{Macdonald1995,
  author = {Macdonald, Ian G.},
  title = {Symmetric Functions and Hall Polynomials},
  edition = {2nd},
  publisher = {Oxford University Press},
  year = {1995},
  series = {Oxford Mathematical Monographs},
}

@book{Serre1977,
  author = {Serre, Jean-Pierre},
  title = {Linear Representations of Finite Groups},
  publisher = {Springer},
  year = {1977},
  series = {Graduate Texts in Mathematics},
  volume = {42},
}

@book{Diaconis1988wreath,
  author = {Diaconis, Persi},
  title = {Group Representations in Probability and Statistics},
  publisher = {Institute of Mathematical Statistics},
  year = {1988},
  series = {IMS Lecture Notes--Monograph Series},
  volume = {11},
}