WikiJournal of Science/Affine symmetric group
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Joel Brewster Lewis (21 April 2021). "Affine symmetric group". WikiJournal of Science 4 (1): 3. doi:10.15347/WJS/2021.003. Wikidata Q100400684. ISSN 2470-6345. https://upload.wikimedia.org/wikiversity/en/7/7c/Affine_symmetric_group.pdf.
The affine symmetric group, , may be equivalently defined as an abstract group by generators and relations, or in terms of concrete geometric and combinatorial models.
In terms of generators and relations, is generated by a set
- (the generators are involutions),
- if j is not one of , and
In the relations above, indices are taken modulo n, so that the third relation includes as a particular case . (The second and third relation are sometimes called the braid relations.) When , the affine symmetric group is the infinite dihedral group generated by two elements subject only to the relations .
This definition endows with the structure of a Coxeter group, with the as Coxeter generating set. For , its Coxeter–Dynkin diagram is the n-cycle, while for it consists of two nodes joined by an edge labeled .
In the Euclidean space with coordinates , the set V of points that satisfy the equation forms a (hyper)plane (an (n − 1)-dimensional subspace). For every pair of distinct elements i and j of and every integer k, the set of points in V that satisfy forms a plane in V, and there is a unique reflection of V that fixes this plane. Then the affine symmetric group can be realized geometrically as the collection of all maps from V to itself that arise by composing several of these reflections.
Inside V, the type A root lattice Λ is the subset of points with integer coordinates, that is, it is the set of all the integer vectors such that . Each of the reflections preserves this lattice, and so the lattice is preserved by the whole group. In fact, one may define to be the group of rigid transformations of V that preserve the lattice Λ.
These reflecting planes divide the space V into congruent simplicies, called alcoves. The situation when is shown at right; in this case, the root lattice is a triangular lattice, and the reflecting lines divide the plane into equilateral triangular alcoves. (For larger n, the alcoves are not regular simplices.)
To translate between the geometric and algebraic definitions, fix an alcove and consider the n hyperplanes that form its boundary. For example, there is a unique alcove (the fundamental alcove) consisting of points such that , which is bounded by the hyperplanes , , ..., and . (This is illustrated in the case at right.) For , one may identify the reflection through with the Coxeter generator , and also identify the reflection through with the generator .
The affine symmetric group may be realized as a group of periodic permutations of the integers. In particular, say that a bijection is an affine permutation if for all integers x and . (It is a consequence of the first property that the numbers must all be distinct modulo n.) Such a function is uniquely determined by its window notation , and so affine permutations may also be identified with tuples of integers that contain one element from each congruence class modulo n and sum to .
To translate between the combinatorial and algebraic definitions, for one may identify the Coxeter generator with the affine permutation that has window notation , and also identify the generator with the affine permutation . More generally, every reflection (that is, a conjugate of one of the Coxeter generators) can be described uniquely as follows: for distinct integers i, j in and arbitrary integer k, it maps i to j − kn, maps j to i + kn, and fixes all inputs not congruent to i or j modulo n. (In terms of the geometric definition, this corresponds to the reflection across the plane . The correspondence between the geometric and combinatorial representations for other elements is discussed below.)
Representation as matrices
One may represent affine permutations as infinite periodic permutation matrices. If is an affine permutation, one places the entry 1 at position in the infinite grid for each integer i, and all other entries are equal to 0. Since u is a bijection, the resulting matrix contains exactly one 1 in every row and column. The periodicity condition on the map u ensures that the entry at position is equal to the entry at position for every pair of integers . For example, a portion of matrix for the affine permutation is shown below, with the conventions that 1s are replaced by •, 0s are omitted, rows numbers increase from top to bottom, column numbers increase from left to right, and the boundary of the box consisting of rows and columns 1, 2, 3 is drawn:
Relationship to the finite symmetric group
As a subgroup
There is a canonical way to choose a subgroup of that is isomorphic to the finite symmetric group . In terms of the algebraic definition, this is the subgroup of generated by (excluding the simple reflection ). Geometrically, this corresponds to the subgroup of transformations that fix the origin, while combinatorially it corresponds to the window notations for which (that is, in which the window notation is the one-line notation of a finite permutation).
If is the window notation of an element of this standard copy of , its action on the hyperplane V in is given by permutation of coordinates: . (In this article, the geometric action of permutations and affine permutations is on the right; thus, if u and v are two affine permutations, the action of uv on a point is given by first applying u, then applying v.)
There are also many nonstandard copies of contained in . A geometric construction is to pick any point a in Λ (that is, an integer vector whose coordinates sum to 0); the subgroup of of isometries that fix a is isomorphic to . The analogous combinatorial construction is to choose any subset A of that contains one element from each conjugacy class modulo n and whose elements sum to ; the subgroup of of affine permutations that stabilize A is isomorphic to .
As a quotient
There is a simple map (technically, a surjective group homomorphism) π from onto the finite symmetric group . In terms of the combinatorial definition, it is to reduce the window entries modulo n to elements of , leaving the one-line notation of a permutation. The image of an affine permutation u is called the underlying permutation of u.
The map π sends the Coxeter generator to the permutation whose one-line notation and cycle notation are and , respectively. In terms of the Coxeter generators of , this can be written as .
The kernel π is the set of affine permutations whose underlying permutation is the identity. The window notations of such affine permutations are of the form , where is an integer vector such that , that is, where . Geometrically, this kernel consists of the translations, that is, the isometries that shift the entire space V without rotating or reflecting it. In an abuse of notation, the symbol Λ is used in this article for all three of these sets (integer vectors in V, affine permutations with underlying permutation the identity, and translations); in all three settings, the natural group operation turns Λ into an abelian group, generated freely by the n − 1 vectors .
Connection between the geometric and combinatorial definitions
The subgroup Λ is a normal subgroup of , and one has an isomorphism
This point of view allows for a direct translation between the combinatorial and geometric definitions of : if one writes where and then the affine permutation u corresponds to the rigid motion of V defined by
Furthermore, as with every affine Coxeter group, the affine symmetric group acts transitively and freely on the set of alcoves. Hence, by making an arbitrary choice of alcove , one may place the group in one-to-one correspondence with the alcoves: the identity element corresponds to , and every other group element g corresponds to the alcove that is the image of under the action of g. This identification for is illustrated at right.
Example: n = 2
Algebraically, is the infinite dihedral group, generated by two generators subject to the relations . Every other element of the group can be written as an alternating product of copies of and .
Combinatorially, the affine permutation has window notation , corresponding to the bijection for every integer k. The affine permutation has window notation , corresponding to the bijection for every integer k. Other elements have the following window notations:
Geometrically, the space V is the line with equation in the Euclidean plane . The root lattice inside V consists of those pairs for integral a. The Coxeter generator acts on V by reflection across the line (that is, across the origin); the generator acts on V by reflection across the line (that is, across the point . It is natural to identify the line V with the real line , by sending the point to the real number 2x. With this identification, the root lattice consists of the even integers; the fundamental alcove is the interval [0, 1]; the element acts by translation by k for any integer k; and the reflection reflects across the point −k for any integer k.
Permutation statistics and permutation patterns
Many permutation statistics and other features of the combinatorics of finite permutations can be extended to the affine case.
Descents, length, and inversions
The length of an element g of a Coxeter group G is the smallest number k such that g can be written as a product of k Coxeter generators of G.
Geometrically, the length of an element g in is the number of reflecting hyperplanes that separate and , where is the fundamental alcove (the simplex bounded by the reflecting hyperplanes of the Coxeter generators ). (In fact, the same is true for any affine Coxeter group.)
Similarly, one may define an affine analogue of descents in permutations: say that an affine permutation u has a descent in position i if . (By periodicity, u has a descent in position i if and only if it has a descent in position for all integers k.)
Algebraically, the descents corresponds to the right descents in the sense of Coxeter groups; that is, i is a descent of u if and only if . The left descents (that is, those indices i such that are the descents of the inverse affine permutation ; equivalently, they are the values i such that i occurs before i − 1 in the sequence .
Geometrically, i is a descent of u if and only if the fixed hyperplane of separates the alcoves and .
Because there are only finitely many possibilities for the number of descents of an affine permutation, but infinitely many affine permutations, it is not possible to naively form a generating function for affine permutations by number of descents (an affine analogue of Eulerian polynomials). One possible resolution is to consider affine descents (equivalently, cyclic descents) in the finite symmetric group . Another is to consider simultaneously the length and number of descents of an affine permutation. The generating function for these statistics over simultaneously for all n is
Cycle type and reflection length
Any bijection partitions the integers into a (possibly infinite) list of (possibly infinite) cycles: for each integer i, the cycle containing i is the sequence where exponentiation represents functional composition. For example, the affine permutation in with window notation contains the two infinite cycles and as well as infinitely many finite cycles for each . Cycles of an affine permutation correspond to cycles of the underlying permutation in an obvious way: in the example above, with underlying permutation , the first infinite cycle corresponds to the cycle (1), the second corresponds to the cycle (45), and the finite cycles all correspond to the cycle (23).
The reflection length of an element u of is the smallest number k such that there exist reflections such that . (In the symmetric group, reflections are transpositions, and the reflection length of a permutation u is , where is the number of cycles of u.) In (Lewis et al. 2019), the following formula was proved for the reflection length of an affine permutation u: for each cycle of u, define the weight to be the integer k such that consecutive entries congruent modulo n differ by exactly kn. (For example, in the permutation above, the first infinite cycle has weight 1 and the second infinite cycle has weight −1; all finite cycles have weight 0.) Form a tuple of cycle weights of u (counting translates of the same cycle by multiples of n only once), and define the nullity to be the size of the smallest set partition of this tuple so that each part sums to 0. (In the example above, the tuple is and the nullity is 2, since one can take the partition .) Then the reflection length of u is
For every affine permutation u, there is a choice of subgroup W of such that , , and for the standard form implied by this semidirect product, one has .
Fully commutative elements and pattern avoidance
A reduced word for an element g of a Coxeter group is a tuple of Coxeter generators of minimum possible length such that . The element g is called fully commutative if one can transform any reduced word into any other by sequentially swapping pairs of factors that commute. For example, in the finite symmetric group , the element is fully commutative, since its two reduced words and can be connected by swapping commuting factors, but is not fully commutative because there is no way to reach the reduced word starting from the reduced word by commutations.
Billey, Jockusch & Stanley (1993) proved that in the finite symmetric group , a permutation is fully commutative if and only if it avoids the permutation pattern 321, that is, if and only if its one-line notation contains no three-term decreasing subsequence. In (Green 2002), this result was extended to affine permutations: an affine permutation u is fully commutative if and only if there do not exist integers such that .[a]
It has also been shown that the number of affine permutations avoiding a single pattern p is finite if and only if p avoids the pattern 321, so in particular there are infinitely many fully commutative affine permutations. These were enumerated by length in (Hanusa & Jones 2010).
Parabolic subgroups and other structures
The parabolic subgroups of and their coset representatives offer a rich combinatorial structure. Other aspects of the affine symmetric group, such as its Bruhat order and representation theory, may also be understood via combinatorial models.
Parabolic subgroups, coset representatives
A standard parabolic subgroup of a Coxeter group is a subgroup generated by a subset of its Coxeter generating set. The maximal parabolic subgroups are those that come from omitting a single Coxeter generator. In , all maximal parabolic subgroups are isomorphic to the finite symmetric group . The subgroup generated by the subset consists of those affine permutations that stabilize the interval , that is, that map every element of this interval to another element of the interval.
The non-maximal parabolic subgroups of are all isomorphic to parabolic subgroups of , that is, to a Young subgroup for some positive integers with sum n.
For a fixed element i of , let be the maximal proper subset of Coxeter generators omitting , and let denote the parabolic subgroup generated by J. Every coset has a unique element of minimum length. The collection of such representatives, denoted , consists of the following affine permutations:
In the particular case that , so that is the standard copy of inside , the elements of may naturally be represented by abacus diagrams: the integers are arranged in an infinite strip of width n, increasing sequentially along rows and then from top to bottom; integers are circled if they lie directly above one of the window entries of the minimal coset representative. For example, the minimal coset representative is represented by the abacus diagram at right. To compute the length of the representative from the abacus diagram, one adds up the number of uncircled numbers that are smaller than the last circled entry in each column. (In the example shown, this gives .)
Other combinatorial models of minimum-length coset representatives for can be given in terms of core partitions (integer partitions in which no hook length is divisible by n) or bounded partitions (integer partitions in which no part is larger than n − 1). Under these correspondences, it can be shown that the weak Bruhat order on is isomorphic to a certain subposet of Young's lattice.
The Bruhat order on has the following combinatorial realization. If u is an affine permutation and i and j are integers, define to be the number of integers a such that and . (For example, with , one has : the three relevant values are , which are respectively mapped by u to 1, 2, and 4.) Then for two affine permutations u, v, one has that in Bruhat order if and only if for all integers i, j.
Representation theory and an affine Robinson–Schensted correspondence
In the finite symmetric group, the Robinson–Schensted correspondence gives a bijection between the group and pairs of standard Young tableaux of the same shape. This bijection plays a central role in the combinatorics and the representation theory of the symmetric group. For example, in the language of Kazhdan–Lusztig theory, two permutations lie in the same left cell if and only if their images under Robinson–Schensted have the same tableau Q, and in the same right cell if and only if their images have the same tableau P. In (Shi 1986), J.-Y. Shi showed that left cells for are indexed instead by tabloids,[b] and in (Shi 1991) he gave an algorithm to compute the tabloid analogous to the tableau P for an affine permutation. In (Chmutov, Pylyavskyy & Yudovina 2018), the authors extended Shi's work to give a bijective map between and triples consisting of two tabloids of the same shape and an integer vector whose entries satisfy certain inequalities. Their procedure uses the matrix representation of affine permutations and generalizes the shadow construction of Viennot (1977).
In some situations, one may wish to consider the action of the affine symmetric group on or on alcoves that is inverse to the one given above.[c] We describe these alternate realizations now.
In the combinatorial action of on , the generator acts by switching the values i and i + 1. In the inverse action, it instead switches the entries in positions i and i + 1. Similarly, the action of a general reflection will be to switch the entries at positions j − kn and i + kn for each k, fixing all inputs at positions not congruent to i or j modulo n. (In the finite symmetric group , the analogous distinction is between the active and passive forms of a permutation.)
In the geometric action of , the generator acts on an alcove A by reflecting it across one of the bounding planes of the fundamental alcove A0. In the inverse action, it instead reflects A across one of its own bounding planes. From this perspective, a reduced word corresponds to an alcove walk on the tesselated space V.
Relationship to other mathematical objects
The affine symmetric group is closely related to a variety of other mathematical objects.
In (Ehrenborg & Readdy 1996), a correspondence is given between affine permutations and juggling patterns encoded in a version of siteswap notation. Here, a juggling pattern of period n is a sequence of nonnegative integers (with certain restrictions) that captures the behavior of balls thrown by a juggler, where the number indicates the length of time the ith throw spends in the air (equivalently, the height of the throw).[d] The number b of balls in the pattern is the average . The Ehrenborg–Readdy correspondence associates to each juggling pattern of period n the function defined by
For example, the juggling pattern 441 (illustrated at right) has and . Therefore, it corresponds to the affine permutation . The juggling pattern has four crossings, and the affine permutation has length .
Similar techniques can be used to derive the generating function for minimal coset representatives of by length.
Complex reflection groups
In a finite-dimensional real inner product space, a reflection is a linear transformation that fixes a linear hyperplane pointwise and negates the vector orthogonal to the plane. This notion may be extended to vector spaces over other fields. In particular, in a complex inner product space, a reflection is a unitary transformation T of finite order that fixes a hyperplane.[e] This implies that the vectors orthogonal to the hyperplane are eigenvectors of T, and the associated eigenvalue is a complex root of unity. A complex reflection group is a finite group of linear transformations on a complex vector space generated by reflections.
The complex reflection groups were fully classified by Shephard & Todd (1954): each complex reflection group is isomorphic to a product of irreducible complex reflection groups, and every irreducible either belongs to an infinite family (where m, p, and n are positive integers such that p divides m) or is one of 34 other (so-called "exceptional") examples. The group is the generalized symmetric group: algebraically, it is the wreath product of the cyclic group with the symmetric group . Concretely, the elements of the group may be represented by monomial matrices (matrices having one nonzero entry in every row and column) whose nonzero entries are all mth roots of unity. The groups are subgroups of , and in particular the group consists of those matrices in which the product of the nonzero entries is equal to 1.
In (Shi 2002), Shi showed that the affine symmetric group is a generic cover of the family , in the following sense: for every positive integer m, there is a surjection from to , and these maps are compatible with the natural surjections when that come from raising each entry to the m/pth power. Moreover, these projections respect the reflection group structure, in that the image of every reflection in under is a reflection in ; and similarly when the image of the standard Coxeter element in is a Coxeter element in .
Affine Lie algebras
Each affine Coxeter group is associated to an affine Lie algebra, a certain infinite-dimensional non-associative algebra with unusually nice representation-theoretic properties. In this association, the Coxeter group arises as a group of symmetries of the root space of the Lie algebra (the dual of the Cartan subalgebra). In the classification of affine Lie algebras, the one associated to is of (untwisted) type , with Cartan matrix for and
Like other Kac–Moody algebras, affine Lie algebras satisfy the Weyl–Kac character formula, which expresses the characters of the algebra in terms of their highest weights. In the case of affine Lie algebras, the resulting identities are equivalent to the Macdonald identities. In particular, for the affine Lie algebra of type , associated to the affine symmetric group , the corresponding Macdonald identity is equivalent to the Jacobi triple product.
Extended affine symmetric group
The affine symmetric group is a subgroup of the extended affine symmetric group. The extended group is isomorphic to the wreath product . Its elements are extended affine permutations: bijections such that for all integers x. Unlike the affine symmetric group, the extended affine symmetric group is not a Coxeter group. However, it has a natural generating set that extends the Coxeter generating set for : the shift operator whose window notation is generates the extended group with the simple reflections, subject to the additional relations .
Combinatorics of other affine Coxeter groups
The geometric action of the affine symmetric group places it naturally in the family of affine Coxeter groups, all of which have a similar geometric action. The combinatorial description of the may also be extended to many of these groups: in (Eriksson & Eriksson 1998), an axiomatic description is given of certain permutation groups acting on (the "George groups", in honor of George Lusztig), and it is shown that they are exactly the "classical" Coxeter groups of finite and affine types A, B, C, and D. Thus, the combinatorial interpretations of descents, inversions, etc., carry over in these cases. Abacus models of minimum-length coset representatives for parabolic quotients have also been extended to this context.
The author thanks the three referees for their many helpful comments, and Max Glick for his help with the less technical summary. The work of the author was supported in part by a Simons Collaboration Grant (634530).
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