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A bijection between all Shi regions and core partitions

Matt Davis

Department of Mathematics and Computer Science
Muskingum University, 10 College Dr., New Concord, OH, 43762
[email protected]

1 Introduction

The mm-Shi arrangement is a hyperplane arrangement related to a number of areas of study in combinatorics and representation theory, including parking functions and nn-core partitions. There are multiple bijections between the set of all regions of the arrangement and parking functions ([4], [22]), and the Athanasiadis-Linusson bijection in particular is interesting in part because the natural symmetric group action on parking functions reflects the geometry of the Shi arrangment.

In [11] (resp. [12]), Fishel and Vazirani showed a bijection between the dominant (resp. bounded dominant) chambers of the mm-Shi arrangement and partitions which are simultaneously nn-core and (mn+1)(mn+1)-core (resp. (mn1)(mn-1)-core). However, this bijection does not extend outside the dominant chamber. The goal of this paper is to extend the results of Fishel-Vazirani by giving a bijection between the set of all chambers of the mm-Shi arrangement and a certain subset of nn-core partitions. Moreover, like the original, it adapts in a natural way to a bijection on the bounded chambers of the arrangement. In addition, it has the same SnS_{n}-structure as parking functions in the Athanasiadis-Linusson bijection. Thus we close the loop from the Fishel-Vazirani result to the more classical indexings of Shi regions, and bring the SnS_{n} action to the partition picture. As part of the proof, we will establish an independently interesting characterization of the minimal chambers that occur in the SnS_{n}-orbit of a minimal chamber of the mm-Shi arrangement.

2 The Affine Symmetric Group and Alcoves

We being with a brief survey of known results on the relationship between the mm-Shi arrangement, nn-core partitions, and the affine symmetric group. Our notation in this section closely models that of [11], which contains several results which will be important in what follows.

2.1 The affine symmetric group

The affine symmetric group S~n\widetilde{S}_{n} is defined to be the set of all permutations ϕ\phi of \mathbb{Z} satisfying the condition that, for any integer mm,

ϕ(m+n)=ϕ(m)+n, and i=0n1ϕ(i)=i=0n1i.\phi(m+n)=\phi(m)+n\textrm{, and }\sum_{i=0}^{n-1}\phi(i)=\sum_{i=0}^{n-1}i.

To define an element ϕS~n\phi\in\widetilde{S}_{n}, it is sufficient to specify ϕ(0),ϕ(1),ϕ(n1)\phi(0),\phi(1),\cdots\phi(n-1), a set of numbers that form a transversal of the congruence classes of \mathbb{Z} mod nn, and sum to (n2)\binom{n}{2}. We will refer to such an nn-tuple (ϕ(0),ϕ(1),ϕ(n1))(\phi(0),\phi(1),\ldots\phi(n-1)) as the nn-window of ϕ\phi.

This group is generated by the elements s0,s1,sn1s_{0},s_{1},\cdots s_{n-1}, where s0s_{0} has the nn-window (1,1,2,,n2,n)(-1,1,2,\ldots,n-2,n), and for 1in11\leq i\leq n-1, sis_{i} has nn-window (0,1,i2,i,i1,i+1,n1)(0,1,\ldots i-2,i,i-1,i+1,\ldots n-1). With these generators, S~n\widetilde{S}_{n} for n>2n>2 has presentation:

si2=es_{i}^{2}=e
sisj=sjsi if ji±1 mod ns_{i}s_{j}=s_{j}s_{i}\textrm{ if }j\neq i\pm 1\textrm{ mod }n
sisjsi=sjsisj if j=i±1 mod n.s_{i}s_{j}s_{i}=s_{j}s_{i}s_{j}\textrm{ if }j=i\pm 1\textrm{ mod }n.

We will always assume that n>2n>2 in what follows.

We also note that G=s1,sn1G=\langle s_{1},\ldots s_{n-1}\rangle is a subgroup of S~n\widetilde{S}_{n} isomorphic to the finite symmetric group SnS_{n}. There is a homomorphism fn:S~nGf_{n}:\widetilde{S}_{n}\rightarrow G given by sending s0s_{0} to sθ=s1s2sn2sn1sn2s2s1s_{\theta}=s_{1}s_{2}\ldots s_{n-2}s_{n-1}s_{n-2}\ldots s_{2}s_{1} and fixing each other sis_{i}. We will use GG and fnf_{n} in this paper only to mean this specific group and homomorphism.

2.2 Root data

We will need to understand the root data associated to the affine symmetric group S~n\widetilde{S}_{n}. We let ϵ1,ϵn\epsilon_{1},\ldots\epsilon_{n} be the standard basis for n\mathbb{R}^{n}, and let |\langle\cdot|\cdot\rangle be the usual inner product. Let V={a1ϵ1++anϵn|a1++an=0}V=\{a_{1}\epsilon_{1}+\ldots+a_{n}\epsilon_{n}\,|\,a_{1}+\ldots+a_{n}=0\}, and let αi=ϵiϵi+1\alpha_{i}=\epsilon_{i}-\epsilon_{i+1}. Then Π={αi| 1in1}\Pi=\{\alpha_{i}\,|\,1\leq i\leq n-1\} is a basis for VV, and Π\Pi is the set of simple roots of the type An1A_{n-1} root system. We identify Q=in1αiQ=\bigoplus_{i}^{n-1}\mathbb{Z}\alpha_{i} with the root lattice of this system. The set of all roots is Δ={ϵiϵj,| 1i,j,n,ij}\Delta=\{\epsilon_{i}-\epsilon_{j},\,|\,1\leq i,j,\leq n,\,i\neq j\}, and θ=α1++αn=ϵ1ϵn\theta=\alpha_{1}+\ldots+\alpha_{n}=\epsilon_{1}-\epsilon_{n} is the highest root. The set Δ+\Delta^{+} of positive roots consists of those roots ϵiϵj\epsilon_{i}-\epsilon_{j} where i<ji<j. We let Δ=Δ+\Delta^{-}=-\Delta^{+} and write α>0\alpha>0 (resp. α<0\alpha<0) if αΔ+\alpha\in\Delta^{+} (resp. αΔ\alpha\in\Delta^{-}). As usual, for any root αΔ+\alpha\in\Delta^{+} we will use sαs_{\alpha} to denote the reflection associated to α\alpha in the Weyl group SnS_{n}, with si=sαis_{i}=s_{\alpha_{i}} and sθ=s1s2sn1s1s_{\theta}=s_{1}s_{2}\ldots s_{n-1}\ldots s_{1} as above.

We must also consider the affine root system A~n1\widetilde{A}_{n-1}, built by including the “imaginary” root δ\delta in the root system of type An1A_{n-1}. We let Δ~={kδ+α|αΔ,k}\widetilde{\Delta}=\{k\delta+\alpha\,|\,\alpha\in\Delta,k\in\mathbb{Z}\} with Δ~+={kδ+α|k0,αΔ+ OR k>0,αΔ}\widetilde{\Delta}^{+}=\{k\delta+\alpha\,|\,k\in\mathbb{Z}_{\geq 0},\alpha\in\Delta^{+}\textrm{ OR }k\in\mathbb{Z}>0,\alpha\in\Delta^{-}\}, and Δ~=Δ~+\widetilde{\Delta}^{-}=-\widetilde{\Delta}^{+}. We let α0=δθ\alpha_{0}=\delta-\theta, and the simple roots in A~n1\widetilde{A}_{n-1} are Π~=Π{α0}\widetilde{\Pi}=\Pi\cup\{\alpha_{0}\}. We again write α>0\alpha>0 (resp. α<0\alpha<0) to mean αΔ~+\alpha\in\widetilde{\Delta}^{+} (resp. αΔ~\alpha\in\widetilde{\Delta}^{-}.)

For any αΔ\alpha\in\Delta and kk\in\mathbb{Z}, we define the hyperplane

Hα,k={vV|v|α=k}.H_{\alpha,k}=\{v\in V\,|\,\langle v|\alpha\rangle=k\}.

Note that Hα,k=Hα,kH_{-\alpha,-k}=H_{\alpha,k}. For any hyperplane Hα,kH_{\alpha,k}, we consider the (closed) half spaces Hα,k+={vV|v|αk}H_{\alpha,k}^{+}=\{v\in V\,|\,\langle v|\alpha\rangle\geq k\} and Hα,k={vV|v|αk}H_{\alpha,k}^{-}=\{v\in V\,|\,\langle v|\alpha\rangle\leq k\}.

2.3 Hyperplane Arrangements

We will be mainly interested in two particular hyperplane arrangements: the Coxeter arrangement 𝒜n\mathcal{A}_{n}, consisting of all the hyperplanes {Hα,k|αΔ+,k}\{H_{\alpha,k}\,|\,\alpha\in\Delta^{+},k\in\mathbb{Z}\}, and the mm-Shi arrangement 𝒮n,m\mathcal{S}_{n,m}, consisting of the hyperplanes {Hα,k|αΔ+ and m<km}\{H_{\alpha,k}\,|\,\alpha\in\Delta^{+}\textrm{ and }-m<k\leq m\}. For a hyperplane arrangement \mathcal{H}, we are interested in the connected components of VHHV\setminus\bigcup_{H\in\mathcal{H}}H, the complement of the hyperplanes in \mathcal{H}. Each such connected component is called a region of the hyperplane arrangement, and can be written as the intersection of a collection of half-planes of hyperplanes in \mathcal{H}. A region is said to be dominant if it is a subset of i=1nHαi,0+\bigcap_{i=1}^{n}H_{\alpha_{i},0}^{+}. We call i=1nHαi,0+\bigcap_{i=1}^{n}H_{\alpha_{i},0}^{+} the dominant chamber, and the elements of its GG-orbit are called chambers or Weyl chambers.

The regions of 𝒜n\mathcal{A}_{n} are referred to as alcoves, and A0=(αΠ+Hα,0+)Hθ,1A_{0}=\left(\bigcap_{\alpha\in\Pi^{+}}H_{\alpha,0}^{+}\right)\cap H_{\theta,1}^{-} is the fundamental alcove. Note that since 𝒮n,m𝒜n\mathcal{S}_{n,m}\subseteq\mathcal{A}_{n}, the regions of 𝒮n,m\mathcal{S}_{n,m} are (up to a measure 0 set) unions of alcoves. As such, the geometry of 𝒜n\mathcal{A}_{n} is fundamental to understanding 𝒮n,m\mathcal{S}_{n,m}. In turn, the affine symmetric group is intimately tied to the set of alcoves of 𝒜n\mathcal{A}_{n}; we summarize the relationship here.

We let S~n\widetilde{S}_{n} act on VV via:

si(a1,,an)=(a1,,ai1,ai+1,ai,ai+2,,an) for i0s_{i}\cdot(a_{1},\ldots,a_{n})=(a_{1},\ldots,a_{i-1},a_{i+1},a_{i},a_{i+2},\ldots,a_{n})\textrm{ for }i\neq 0
s0(a1,,an)=(an+1,a2,an1,a11).s_{0}\cdot(a_{1},\ldots,a_{n})=(a_{n}+1,a_{2},\ldots a_{n-1},a_{1}-1).

Then for i0i\neq 0, sis_{i} acts as reflection through Hαi,0H_{\alpha_{i},0}, and s0s_{0} reflects through Hθ,1H_{\theta,1}. This action preserves the lattice QQ and acts freely and transitively on the set of alcoves. Thus we can identify each element wS~nw\in\widetilde{S}_{n} with the alcove wA0w\cdot A_{0}, and this correspondence is a bijection.

Note that GG preserves |\langle|\rangle on VV (although S~n\widetilde{S}_{n} does not). Let wS~nw\in\widetilde{S}_{n}. Then if yy is a minimal-length representative of the coset GwGw, then either y=ey=e or any reduced word for yy must have s0s_{0} as its leftmost letter. We note here (see [18], for example) that if wS~nw\in\widetilde{S}_{n} and yy is a minimal-length coset representative of GwGw, then the window for y1y^{-1} is sorted in ascending order, and yA0yA_{0} is in the dominant chamber. We will abuse notation slightly and use S~n/G\widetilde{S}_{n}/G to denote the set of minimal-length right coset representatives of GG in S~n\widetilde{S}_{n}.

The combinatorics of the alcoves of 𝒜n\mathcal{A}_{n} and S~n\widetilde{S}_{n} are closely related, but here we will only point out the fact that the length of an element wS~nw\in\widetilde{S}_{n} is exactly the number of distinct hyperplanes in 𝒜n\mathcal{A}_{n} separating wA0wA_{0} from the origin.

The boundary of any alcove of AnA_{n} is a union of subsets of various hyperplanes Hα,kH_{\alpha,k}, which we call facets. Each facet of an alcove is in the S~n\widetilde{S}_{n}-orbit of exactly one facet of A0A_{0} ([20]). If Hα,kH_{\alpha,k} is the hyperplane containing a facet of an alcove, we call it a wall of the alcove. Since the walls of A0A_{0} are Hαi,0H_{\alpha_{i},0} for 1in11\leq i\leq n-1 or Hθ,1H_{\theta,1}, we can label each of these facets with the corresponding ii or 0 for Hθ,1H_{\theta,1}. Applying the same label to each facet in the orbit of the facets of A0A_{0} applies a label to each facet of each alcove of AnA_{n}.

Shi proved ([20]) that each region of S~n,m\widetilde{S}_{n,m} contains a unique alcove wA0wA_{0} such that (w)\ell(w) is minimal. We call such an alcove mm-minimal, and note that studying the regions of 𝒮n,m\mathcal{S}_{n,m} is in many ways equivalent to studying the mm-minimal alcoves. Moreover, any bounded region of 𝒮n,m\mathcal{S}_{n,m} has a unique alcove wA0wA_{0} such that (w)\ell(w) is maximal, which we call an mm-maximal region.

Fishel-Vazirani gave the following characterization of the walls of an alcove.

Lemma 1.

([11], Proposition 4.1) For wS~mw\in\widetilde{S}_{m} and 0in10\leq i\leq n-1, wA0Hα,k+wA_{0}\subseteq H_{\alpha,k}^{+} and wsiA0Hα,kws_{i}A_{0}\subseteq H_{\alpha,k}^{-} if and only if w(αi)=αkδw(\alpha_{i})=\alpha-k\delta.

The first condition here says that the alcove wA0wA_{0} has Hα,kH_{\alpha,k} as one of its walls, with label sis_{i}, and the alcove wsiA0ws_{i}A_{0} on the other side of the wall is on the negative side of Hα,kH_{\alpha,k}. Note that [11] only proves the forward implication, but the reverse is implicit. If w(αi)=αkδw(\alpha_{i})=\alpha-k\delta, then we note that w𝒜0w\mathcal{A}_{0} always has some facet with label ii, so wsi𝒜0ws_{i}\mathcal{A}_{0} shares a facet with it. Then if wA0Hα,k+wA_{0}\subseteq H_{\alpha^{\prime},k^{\prime}}^{+} and wsiA0Hα,kws_{i}A_{0}\subseteq H_{\alpha^{\prime},k^{\prime}}^{-} (possibly for α<0\alpha^{\prime}<0), we must have w(αi)=αkδw(\alpha_{i})=\alpha^{\prime}-k^{\prime}\delta, so k=kk^{\prime}=k and α=α\alpha^{\prime}=\alpha.

A floor of an alcove is a wall of that alcove that does not go through the origin, but separates the alcove from the origin. A ceiling of an alcove is a wall of that alcove so that the alcove and origin are on the same side of the wall.

3 n-cores and abaci

We now summarize some standard facts about partitions - see [17] for example, for details. A partition λ\lambda of a positive integer nn is an infinite sequence (λ1,λ2,)(\lambda_{1},\lambda_{2},\cdots) of non-negative integers, written in non-increasing order, that sum to nn. For example, (5,4,2,1,0,0,)(5,4,2,1,0,0,\cdots) and (10,1,1,0,0,)(10,1,1,0,0,\cdots) are partitions of 12. We will usually write a partition as a finite list consisting only of the non-zero entries of λ\lambda. We will also typically identify a partition with its Young diagram - a configuration of boxes arranged in a grid, where the first row has λ1\lambda_{1} boxes, the second has λ2\lambda_{2} boxes, etc.

\ytableausetup

centertableaux {ytableau} 0 & 1 2 3 4
-1 0 1
-2
-3

Figure 1: The partition (5,3,1,1)(5,3,1,1), with contents

The boxes in λ\lambda will be referred to by their coordinates, so that box (i,j)(i,j) is in the jjth row and iith column, counting from the top and left sides of the diagram. We say that a box bb in a Young diagram λ\lambda is removable for λ\lambda if it is in λ\lambda, but removing it from λ\lambda still yields a valid Young diagram. We say that a box bb is addable for λ\lambda if it is not in λ\lambda, but adding it to λ\lambda would still yield a valid Young diagram. Each box in the grid is assigned a content. Specifically, the box in row jj and column ii has content iji-j.

Each box in a Young diagram also has associated to it a hook length, defined as the the number of boxes directly to the right of the box in its row plus the number of boxes directly below the box in its column, plus 1.

\ytableausetup

centertableaux {ytableau} 8 & 5 4 2 1
5 2 1
2
1

Figure 2: The hook lengths for (5,3,1,1)(5,3,1,1)

If a given box bb has hook length ss, then there will be a connected chain of boxes along the lower-right edge of the Young diagram, starting at the end of the row containing bb, and ending at the bottom of the column containing bb, that has exactly ss boxes.

\ytableausetup

centertableaux {ytableau}   & 5 *(red) *(red) *(red)
  *(red) *(red)

Figure 3: The rim hook for box (2,1)(2,1)

This chain of boxes is the rim hook associated to bb. Removing the rim hook associated to a given box will yield a valid Young diagram. If we repeatedly remove rim hooks of length nn from a Young diagram λ\lambda until none remain, the result will be independent of the order in which the rim hooks are removed. In this case, we call the resulting partition λ\lambda^{\prime} the nn-core of λ\lambda. If a Young diagram λ\lambda has no hook lengths equal to nn, we say that λ\lambda is nn-core, since the nn-core of λ\lambda is λ\lambda itself. A partition λ\lambda is nn-core if and only if none of its hook lengths are divisible by nn. We say that a partition λ\lambda is (n,t)(n,t)-core if it is simultaneously nn-core and tt-core.

In [18], Lascoux described a way for S~n\widetilde{S}_{n} to act on Young diagrams of nn-core partitions by adding or removing boxes of a given content. Specifically, if λ\lambda is a partition, then it cannot have both addable and removable boxes with content congruent to ii mod nn. (Due to the importance of this action, in our treatment of nn-cores, we will always reduce the contents of boxes mod nn.) Then sis_{i} acts on λ\lambda by

si1λ={λ{All addable boxes of content i mod n} If λ has such addable boxesλ{All removable boxes of content i mod n} If λ has such removable boxesλ Otherwise .s_{i}\cdot_{1}\lambda=\begin{cases}\lambda\cup\{\textrm{All addable boxes of content $i$ mod $n$}\}&\textrm{ If $\lambda$ has such addable boxes}\\ \lambda\setminus\{\textrm{All removable boxes of content $i$ mod $n$}\}&\textrm{ If $\lambda$ has such removable boxes}\\ \lambda&\textrm{ Otherwise }\end{cases}.

This is the description of this action originally given in [18], although [11] has more of the details worked out. We will refer to this as the level 1 action, to contrast the level tt action below.

There are a number of combinatorial indexings of nn-core partitions that we will move between often in this paper. We will begin by introducing all of these indexings and a description of the necessary actions of S~n\widetilde{S}_{n} on each one.

Balanced nn-abaci The first combinatorial indexing of partitions which is particularly useful for nn-cores is the notion of an nn-abacus ([17] is a standard reference). Imagine the integers arranged in an infinite grid containing nn columns, marked with the numbers 0,1,2,n10,1,2,\cdots n-1. We label the rows by integers, so that row 0 contains 0,1,2,n10,1,2,\cdots n-1, row 1 contains n,n+1,2n1n,n+1,\ldots 2n-1, row -1 contains n,n+1,1-n,-n+1,\ldots-1, etc. An abacus diagram is merely a set of integers whose complement is bounded below, which we draw on the infinite grid by circling each number in the set. The columns of this diagram are called the runners of the abacus, and the circled numbers are called beads.

From a partition λ\lambda, we can obtain a particular abacus diagram which we will call the positive nn-abacus of λ\lambda. The positive nn-abacus of a partition λ\lambda is the diagram obtained from this grid by circling each number which is the hook length of a box in the first column of the Young diagram of λ\lambda, as well as all the negative integers. Then a partition is nn-core if and only its positive nn-abacus has no positive beads on the 0 runner, and for each ii from 11 to n1n-1, if runner ii has any positive beads, they are in positions i,i+n,i+2n,i+kni,i+n,i+2n,\ldots i+kn for some nonnegative integer kk. In other words, the beads on the abacus must be pushed as far up the runners as possible, with no positive beads on the 0 runner.

We say that two abacus diagrams are equivalent to each other if one can be obtained from the other by adding a constant to each bead in the diagram. Any abacus diagram that is equivalent to the positive nn-abacus of λ\lambda will be referred to as an nn-abacus for λ\lambda.

Refer to caption
Figure 4: The positive 3-abacus diagram for (5,3,1,1)(5,3,1,1)

We define the balance number of an abacus diagram for an nn-core λ\lambda to be the sum over the runners of the diagram of the row number of the first non-circled number on that runner, and say that a diagram is balanced if its balance number is 0.

Refer to caption
Figure 5: The balanced 3-abacus diagram for (5,3,1,1)(5,3,1,1)

Then every nn-core partition has an abacus diagram equivalent to a unique balanced abacus diagram, which we call the balanced nn-abacus of λ\lambda. This correspondence gives a bijection between balanced nn-abacus diagrams meeting the “flushness” property described above and nn-core partitions. (Note the positive part of the 0 runner may no longer be empty in the balanced abacus.) The balanced nn-abacus is particularly useful because the action of S~n\widetilde{S}_{n} on the set of balanced nn-abaci is easily described. Given a balanced nn-abacus XX for λ\lambda, we define wiXw_{i}\cdot X to be XX with runners i1i-1 and ii swapped if 1in11\leq i\leq n-1, and w0Xw_{0}\cdot X to be the diagram obtained from XX by swapping runners 0 and n1n-1, and then adding one bead to runner 0 and removing the last bead from runner n1n-1. The result will be the balanced abacus of an nn-core partition, and [5] shows that this action is equivalent to the action on nn-core partitions described above.

nn-vectors Because of the “flushness” condition, the balanced nn-abacus of an nn-core partition is completely determined by the row number of the first non-circled bead on each runner. We can encode this as a vector with nn components, the iith entry of which is the row number of the first non-circled number on that runner. This is the ‘nn-vector’ construction of Garvan, Kim, and Stanton ([14]). Since the abacus diagram is balanced, the entries of the resulting vector will sum to 0. Thus this correspondence gives a bijection between nn-core partitions and nn-dimensional vectors with integer entries that sum to zero. In [5] it is shown that this is an S~n\widetilde{S}_{n}-equivariant bijection between nn-core partitions and QQ.

Moreover, [11] shows that this map induces a bijection between the set of partitions which are (n,mn+1)(n,mn+1)-core and the dominant mm-minimal alcoves. Specifically, if λ\lambda is an (n,mn+1)(n,mn+1)-core partition equal to w1w^{-1}\cdot\emptyset, where wS~n/Gw\in\widetilde{S}_{n}/G, then wA0wA_{0} is an mm-minimal alcove.

nn-sets and nn-windows Consider the nn-vector v=(a1,,an)v=(a_{1},\ldots,a_{n}) of an nn-core partition λ\lambda, and let S(λ)={na1,na2+1,,nan+n1}S(\lambda)=\{na_{1},na_{2}+1,\ldots,na_{n}+n-1\}. Since vv encodes the rows of the first non-circled beads on each runner of the abacus, the (unique) element of S(λ)S(\lambda) that is congruent to ii mod nn is the label of the first non-circled bead on runner ii. Also, since ai=0\sum a_{i}=0, we notice that the sum of the elements of S(λ)S(\lambda) is (n2)\binom{n}{2}. The tuple S(λ)S(\lambda) is called the nn-set of λ\lambda, and the resulting correspondence is a bijection between transversals of /n\mathbb{Z}/n\mathbb{Z} with sum equal to (n2)\binom{n}{2} and nn-core partitions. Since S~n\widetilde{S}_{n} acts on \mathbb{Z}, it also acts on nn-sets by acting on each element of the set. It is routine to check that the action on the nn-set of a partition corresponds to the action on its abacus.

We will use S(λ)iS(\lambda)_{i} to denote the element of S(λ)S(\lambda) which is congruent to ii mod nn. Finally, we let X(λ)X(\lambda) be the nn-tuple consisting of the elements of S(λ)S(\lambda) sorted in increasing order, which we call the nn-window for λ\lambda. Similarly to above, we will use X(λ)iX(\lambda)_{i} to denote the iith entry of X(λ)X(\lambda), i.e. the iith smallest entry in S(λ)S(\lambda). Then if λ=w1\lambda=w^{-1}\emptyset where wS~n/Gw\in\widetilde{S}_{n}/G, we have that X(λ)X(\lambda) is the nn-window of w1w^{-1}. We note that nn-windows give yet another parametrization for nn-cores.

4 The level t action and n-cores

We turn now to Fayers’ “level tt” action of S~n\widetilde{S}_{n} on \mathbb{Z}. Specifically, in [9] and [10], for any tt relatively prime to nn (which we assume throughout), Fayers defined an action which we denote as t\ast_{t}:

sitj={j+t if j(i1)tnt mod njt if jitnt mod nj otherwise ,s_{i}\ast_{t}j=\begin{cases}j+t&\textrm{ if }j\equiv(i-1)t-n\circ t\textrm{ mod }n\\ j-t&\textrm{ if }j\equiv it-n\circ t\textrm{ mod }n\\ j&\textrm{ otherwise }\end{cases},

where nt=12(n1)(t1)n\circ t=\frac{1}{2}(n-1)(t-1). We will not use this precise action, but we restate it here to point out why Fayers’ results still apply in our case. Instead, we focus on two variants of this action which are specific to the case t±1t\equiv\pm 1 mod nn, denoted t\cdot_{t}. First, if t=mn+1t=mn+1, we define:

sitj={j+t if j(i1) mod njt if ji mod nj otherwise .s_{i}\cdot_{t}j=\begin{cases}j+t&\textrm{ if }j\equiv(i-1)\textrm{ mod }n\\ j-t&\textrm{ if }j\equiv i\textrm{ mod }n\\ j&\textrm{ otherwise }\end{cases}.

Secondly, if t=mn1t=mn-1, then we define:

sitj={jt if j(i1) mod nj+t if ji mod nj otherwise .s_{i}\cdot_{t}j=\begin{cases}j-t&\textrm{ if }j\equiv(i-1)\textrm{ mod }n\\ j+t&\textrm{ if }j\equiv i\textrm{ mod }n\\ j&\textrm{ otherwise }\end{cases}.

We use these particular definitions because in either case, the level tt action of sis_{i} will swap the i1i-1 and ii congruence classes setwise, by shifting by tt in the appropriate direction. A similar definition could be given done for any value of tt relatively prime to nn, but the choice of which congruence classes to swap may start to matter, and it is unclear if such an action has a direct application. However, in our case, tailoring the level mn+1mn+1 and mn1mn-1 actions in this way will let us give a consistent description of both of our bijections. (Note that we also have the nice property that the level 1 action is the usual action of S~n\widetilde{S}_{n}, which we will denote as 1\cdot_{1} from now on. )

Now, for t=mn+1t=mn+1, the actions t\ast_{t} and t\cdot_{t} differ only by an index shift by ntn\circ t, an automorphism of S~n\widetilde{S}_{n}. Similarly, for t=mn1t=mn-1, the actions differ by shifting the index by ntn\circ t and negating (mod nn). Thus, the orbit of any integer or set of integers will be the same under either t\ast_{t} or t\cdot_{t}, meaning several important results from [9] still hold. (We will refer to simply “the orbit of the level tt action”, since it is the same regardless of whether we look at t\cdot_{t} or t\ast_{t}. For results specific to t=mn±1t=mn\pm 1, we will specify the value of tt.) The proofs of the other results we need from [9] are virtually unchanged, and we summarize all those results here.

The level tt action is important for us in the way that it acts on nn-windows, nn-cores, and their nn-sets. In [9], Fayers described t\ast_{t} acting on nn-cores, which operates in terms of adding or removing rim hooks of legnth tt with a particular pattern of contents - a direct generalization of Lascoux’s S~n\widetilde{S}_{n} action. On the level of nn-sets, the level tt action on \mathbb{Z} can be applied directly to sets of integers as well. Fayers ([9]) shows that if λ\lambda is an nn-core, then for any wS~nw\in\widetilde{S}_{n}, wtS(λ)w\ast_{t}S(\lambda) is the nn-set of another nn-core partition. Now, as in [10] we let CnC_{n} be the set of all nn-cores, and define Cn(N)C_{n}^{(N)} to be the set of all nn-cores λ\lambda satisfying |xy|<nN|x-y|<nN for all x,yS(λ)x,y\in S(\lambda). Fayers ([10], Lemma 3.16) shows that each (s,t)(s,t) core is an element of Cn(t)C_{n}^{(t)}. We also give an equivalence relation N\equiv_{N} on nn-cores where λ1Nλ2\lambda_{1}\equiv_{N}\lambda_{2} if there is a bijection ϕ:S(λ1)S(λ2)\phi:S(\lambda_{1})\rightarrow S(\lambda_{2}) with ϕ(x)x\phi(x)\equiv x mod nNnN for all xS(λ1)x\in S(\lambda_{1}).

We should note here that Cn(mn+1)C_{n}^{(mn+1)} has essentially already appeared as an indexing set for chambers of the Shi arrangement. The group n+1n\mathbb{Z}^{n}_{n+1} of nn-tuples of integers mod n+1n+1 has a subgroup HH of order n+1n+1 generated by (1,1,,1)(1,1,\ldots,1), so the quotient n+1n/H\mathbb{Z}^{n}_{n+1}/H has (n+1)n1(n+1)^{n-1} elements. (This set appears in [2], [4], and [23], among many others.) But each coset has a unique representative with a 0 in the first entry, and (0,a1,an1)(0,a_{1},\ldots a_{n-1}) can be associated to the positive abacus with aia_{i} (flush) beads on the runner labeled ii. If all the aia_{i} are less than n+1n+1, then that abacus represents a partition in Cn(n+1)C_{n}^{(n+1)}. These cosets also each contain a single representative that describes a parking function, and the Athanasiadis-Linusson bijection (though not the Pak-Stanley) from regions to parking functions is SnS_{n}-equivariant with the normal permutation action on n+1n/H\mathbb{Z}^{n}_{n+1}/H. Interestingly, while the partition indexing of dominant Shi regions feels very natural because of the affine symmetric group action, the abaci associated to the partitions do not match up well to the obvious SnS_{n} action on n+1n/H\mathbb{Z}^{n}_{n+1}/H. As we will see, our level tt action on Cn(mn+1)C_{n}^{(mn+1)} is an appropriate substitute.

For the level tt action, we have:

Lemma 2.

(cf. [10], Lemma 3.12) |Cn(t)|=tn1|C_{n}^{(t)}|=t^{n-1}

Lemma 3.

(cf. [10], Proposition 3.13) Each equivalence class in CnC_{n} under t\equiv_{t} contains a unique element of Cn(t)C_{n}^{(t)}.

Lemma 4.

(cf. [10], Proposition 3.14) The equivalence relation t\equiv_{t} is preserved by the level tt action of S~n\widetilde{S}_{n}

These lemmata together mean in particular that the level mn±1mn\pm 1 actions are well-defined on the sets Cn(mn±1)C_{n}^{(mn\pm 1)}, which have size (mn±1)n1(mn\pm 1)^{n-1}. These are precisely the number of regions and bounded regions in the mm-Shi arrangement. Our next goal is to understand the orbits of this action.

Lemma 5.

The level mn±1mn\pm 1 action of S~n\widetilde{S}_{n} on Cn(t)C_{n}^{(t)} is generated by the action of GG.

Proof. We claim that s0s_{0} acts on Cn(t)C_{n}^{(t)} in the same way as sθs_{\theta} does. Since the action of S~n\widetilde{S}_{n} on \mathbb{Z} is completely determined by its action on a set of congruence class representatives mod nn, we look at the set Y={0,t,2t,(n1)t}Y=\{0,t,2t,\ldots(n-1)t\} if t=mn+1t=mn+1 and Y={0,t,2t,(n1)t}Y=\{0,-t,-2t,\ldots-(n-1)t\} for t=mn1t=mn-1. Then for 1in11\leq i\leq n-1, the action of sis_{i} switches the entries of YY congruent to i1i-1 and ii mod nn, and leaves the other elements of YY fixed, so that the action of sθs_{\theta} on YY switches the elements congruent to 0 and (n1)(n-1) mod nn, and leaves the other elements fixed. But by the same token, for t=mn+1t=mn+1, s0t0=t(n1)ts_{0}\cdot_{t}0=-t\equiv(n-1)t mod ntnt, and s0t(n1)t=nt0s_{0}\cdot_{t}(n-1)t=nt\equiv 0 mod ntnt, while s0s_{0} fixes the other elements of YY. Similar statements hold for t=mn1t=mn-1, so that, mod ntnt, s0s_{0} and sθs_{\theta} have the same level tt action on \mathbb{Z}, so they act the same way on the equivalence classes under nt\sim_{nt}. \square

As a result of this lemma, from this point on, we can focus on the level tt action of GG on Cn(t)C_{n}^{(t)}. To make notation easier, we let wi=siw_{i}=s_{i} for 1in11\leq i\leq n-1, and let w0=sθw_{0}=s_{\theta}. Now, following the proof of ([10], Lemma 3.10), we describe the stabilizer of the GG-action on Cn(mn+1)C_{n}^{(mn+1)}.

Lemma 6.

Let λ\lambda be an (n,t)(n,t)-core partition where t=mn±1t=mn\pm 1. Then the GG-stabilizer of λ\lambda in Cn(t)C_{n}^{(t)} is generated by the wiw_{i} for ii such that S(λ)iS(λ)i1=tS(\lambda)_{i}-S(\lambda)_{i-1}=\mp t.

Proof. We prove the case t=mn+1t=mn+1 - the other case is similar. If S(λ)iS(λ)i1=tS(\lambda)_{i}-S(\lambda)_{i-1}=t, then witS(λ)i=S(λ)i1w_{i}\cdot_{t}S(\lambda)_{i}=S(\lambda)_{i-1} and witS(λ)i1=S(λ)iw_{i}\cdot_{t}S(\lambda)_{i-1}=S(\lambda)_{i}, but wiw_{i} fixes the other elements of S(λ)S(\lambda), so that witλ=λw_{i}\cdot_{t}\lambda=\lambda.

Now, let wGw\in G and assume that wtλ=λw\cdot_{t}\lambda=\lambda. Since λ\lambda is a tt-core, if the abacus for λ\lambda contains circled beads at aa and a+kta+kt for some positive kk, then the beads a+t,a+2t,,a+(k1)ta+t,a+2t,\ldots,a+(k-1)t are also circled. The same must be true of the balanced abacus for λ\lambda, so that if aa and a+kta+kt are elements of S(λ)S(\lambda), then so are a+t,a+2t,,a+(k1)ta+t,a+2t,\ldots,a+(k-1)t. Since t1t\equiv 1 mod nn, we may assume the elements of S(λ)S(\lambda) lying in a single mod tt congruence class are exactly S(λ)i=aS(\lambda)_{i}=a through S(λ)i+k=a+(k1)tS(\lambda)_{i+k}=a+(k-1)t. To fix S(λ)S(\lambda) setwise, the level tt action of ww must permute the set {S(λ)i,S(λ)i+1,,S(λ)i+k}\{S(\lambda)_{i},S(\lambda)_{i+1},\ldots,S(\lambda)_{i+k}\}. But the permutations of this set are generated by wi+1,wi+2,,wi+kw_{i+1},w_{i+2},\ldots,w_{i+k}. Since the different mod tt congruence classes correspond to disjoint cycles in SnS_{n}, the result follows.

Of course, the orbit of an (s,t)(s,t)-core λ\lambda in Cn(mn±1)C_{n}^{(mn\pm 1)} is in bijection with the cosets of its stablizer. This (along with Lemma 9 below) completes the information we need about the partition side of our main bijection.

5 Alcoves

While nn-sets contain all the information we need about nn-core partitions, nn-windows corresponding to alcoves will also be important for us since the ordering of the elements of the window captures the data about the labels of the floors and ceilings of an alcove, as well as the actual hyperplanes that contain those floors and ceilings. For a minimal length coset representative ww, the permutation σ=fn(w)\sigma=f_{n}(w) contains the necessary information that links all this data.

To understand the significance of σ\sigma, let λ=w1\lambda=w^{-1}\emptyset. We let σ\sigma act on X(λ)X(\lambda) by letting each wiw_{i} swap the positions of the entries of the tuple that are congruent to i1i-1 and ii mod nn, which, reduced mod nn, is the same as the level one action of sis_{i}. Since w11(0,1,,n1)=X(λ)w^{-1}\cdot_{1}(0,1,\ldots,n-1)=X(\lambda), the action of σ\sigma sorts X(λ)X(\lambda) back in congruence class order (0,1,2,)(0,1,2,\ldots). As a result, X(λ)σ(i)=S(λ)i1.X(\lambda)_{\sigma(i)}=S(\lambda)_{i-1}. (The index shifts by 1 since the “first” element of S(λ)S(\lambda) is S(λ)0S(\lambda)_{0}.)

Lemma 7.

Let wS~nw\in\widetilde{S}_{n} and let αi\alpha_{i} be a simple root. Then if w(αi)=α+kδw(\alpha_{i})=\alpha+k\delta, (fn(w))(αi)=α(f_{n}(w))(\alpha_{i})=\alpha.

Proof. For 1in11\leq i\leq n-1, sis_{i} acts linearly on QQ and fixes δ\delta. For s0s_{0}, we note that for any α\alpha^{\prime}, s0(α+kδ)=α+kδα+kδ,α0α0=αα,θ(θ)+jδs_{0}(\alpha^{\prime}+k\delta)=\alpha^{\prime}+k\delta-\langle\alpha^{\prime}+k\delta,\alpha_{0}\rangle\alpha_{0}=\alpha^{\prime}-\langle\alpha^{\prime},-\theta\rangle(-\theta)+j\delta, for some jj, while sθ(α)=αα,θθs_{\theta}(\alpha^{\prime})=\alpha^{\prime}-\langle\alpha^{\prime},\theta\rangle\theta. Thus the real parts of the actions match.

Most importantly, though, σ\sigma links the labels and the walls of an alcove of AnA_{n}.

Lemma 8.

Let wA0wA_{0} be a dominant alcove, with σ=fn(w)\sigma=f_{n}(w). Let Hα,kH_{\alpha,k} be a wall of wA0wA_{0}. Then σsiσ1=sα\sigma s_{i}\sigma^{-1}=s_{\alpha} iff Hα,kH_{\alpha,k} has label ii.

Proof. By Lemma 1, if Hα,kH_{\alpha,k} is a floor of wA0wA_{0} with label ii, then w(αi)=αkδw(\alpha_{i})=\alpha-k\delta, so that σ(αi)=α\sigma(\alpha_{i})=\alpha. If Hα,kH_{\alpha,k} is a ceiling of wA0wA_{0}, then wsi(αi)=αkδws_{i}(\alpha_{i})=\alpha-k\delta, so that σ(αi)=α\sigma(-\alpha_{i})=\alpha. Either way, (σsiσ1)α=α(\sigma s_{i}\sigma^{-1})\cdot\alpha=-\alpha, so it is a reflection that inverts α\alpha, and must equal sαs_{\alpha}.

So we see that σ\sigma links nn-sets with nn-windows, but also walls of alcoves with their labels. Combining these observations, we have the following lemma about how the partition associated to an mm-minimal dominant alcove encodes its floors.

Lemma 9.

Let wA0wA_{0} be a dominant alcove that is a subset of Hα,k+Hα,k+1H_{\alpha,k}^{+}\cap H_{\alpha,k+1}^{-}, where α=ϵiϵj\alpha=\epsilon_{i}-\epsilon_{j} and i<ji<j. We let XX be the nn-window of w1w^{-1} and let λ\lambda be the partition w1w^{-1}\emptyset so that S(λ)S(\lambda) is its nn-set. Then:

  1. i.

    nk<XjXi<n(k+1)nk<X_{j}-X_{i}<n(k+1).

  2. ii.

    XjXi=nk+1X_{j}-X_{i}=nk+1 iff Hα,kH_{\alpha,k} is a wall of wA0wA_{0}.

  3. iii.

    XjXi=n(k+1)1X_{j}-X_{i}=n(k+1)-1 iff Hα,k+1H_{\alpha,k+1} is a wall of wA0wA_{0}.

  4. iv.

    |S(λ)j1S(λ)i1|=Xσ(j)Xσ(i)|S(\lambda)_{j-1}-S(\lambda)_{i-1}|=X_{\sigma(j)}-X_{\sigma(i)}.

Proof. Part i is intrinsic in [13]. In their notation, the alcove wA0wA_{0} has kα=kk_{\alpha}=k. The numbers pip_{i} constructed in section 2.7 of [13] are the nn-window for w1w^{-1}, shifted by a constant. Thus the difference between entries remain the same and so XjXin=k\lfloor\frac{X_{j}-X_{i}}{n}\rfloor=k. XjXiX_{j}-X_{i} cannot equal knkn since XiX_{i} and XjX_{j} are not congruent mod nn.

For the other parts, we note that if Hα,kH_{\alpha,k} is a wall of wA0wA_{0} with label rr, then for σ=fn(w)\sigma=f_{n}(w), we have σsrσ1=sα\sigma s_{r}\sigma^{-1}=s_{\alpha}. This means σ\sigma sends rr and r+1r+1 to ii and jj in some order. Thus XjX_{j} and XiX_{i} are equal to S(λ)r1S(\lambda)_{r-1} and S(λ)rS(\lambda)_{r} in some order. But these differ by 11 mod nn so that XjXi=nk+1X_{j}-X_{i}=nk+1 or n(k+1)1n(k+1)-1. But if Hα,kH_{\alpha,k} is a wall of wA0wA_{0}, then wsrA0ws_{r}A_{0} is on the other side of Hα,kH_{\alpha,k}, which can only happen if (srX)j(srX)i<kn(s_{r}X)_{j}-(s_{r}X)_{i}<kn. But since srs_{r} only changes the elements of XX by a total of 2, this must mean that XjXi=kn+1X_{j}-X_{i}=kn+1 and (srX)j(srX)i=kn1(s_{r}X)_{j}-(s_{r}X)_{i}=kn-1. A similar argument proves iii.

The conditions ii. and iii. essentially identify floors and ceilings of wA0wA_{0}, although not exactly. Hyperplanes of the form Hα,0H_{\alpha,0} are the only exception since they are technically never floors or ceilings. And condition iv. completes Lemma 6, showing that it is the labels of the walls of an alcove that index its stabilizer. (Note that it has occurred before that the labels on floors of an alcove index the stabilizer of an object indexing the regions of 𝒮n,m\mathcal{S}_{n,m}. See, for example, Lemma 4.1 in [3].)

In what follows, we will want SnS_{n} to act on nn-windows of nn-core partitions, but with the goal of swapping the congruence classes in certain positions of the window. To swap, say, positions ii and i+1i+1 of an nn-window, we must “twist” the action of wiw_{i} by exactly σ\sigma. More precisely, we have the following:

Lemma 10.

Fix wS~n/Gw\in\widetilde{S}_{n}/G, and XX, the nn-window of w1w^{-1}. Let σ=fn(w)\sigma=f_{n}(w). Then for any 1in11\leq i\leq n-1, ((σwiσ1)mn±1X)\left((\sigma w_{i}\sigma^{-1})\cdot_{mn\pm 1}X\right) modulo nn is exactly XX modulo nn but with the iith and i+1i+1st entries swapped.

Proof. Note that the congruence classes of the iith and i+1i+1st entries of XX are σ(i)\sigma(i) and σ(i+1)\sigma(i+1). But (σwiσ1)tσ(i)(\sigma w_{i}\sigma^{-1})\cdot_{t}\sigma(i) is in the congruence class of σ(i+1)\sigma(i+1) and vice versa.

Notice that, for different choices of wS~n/Gw\in\widetilde{S}_{n}/G, corresponding to different (n,mn±1)(n,mn\pm 1)-core partitions, the twisting may act differently. So this action is not globally consistent in some sense, but it is well-defined within each orbit of the level tt action of GG on Cn(t)C_{n}^{(t)}.

6 The Bijections

We are finally in a position to state our main results.

Theorem 11.

Let w=gwyww=g_{w}y_{w} where gwGg_{w}\in G and ywS~n/Gy_{w}\in\widetilde{S}_{n}/G. Write σ=f(yw1)Sn\sigma=f(y_{w}^{-1})\in S_{n} and let XX be the nn-window of yw1y_{w}^{-1}. The partition associated to ww is the partition in Cn(mn+1)C_{n}^{(mn+1)} with nn-set equivalent to σgwσ1mn+1X\sigma g_{w}\sigma^{-1}\cdot_{mn+1}X (considered as a set).

This restricts to a bijection between mm-minimal alcoves wA0wA_{0} and Cn(mn+1)C_{n}^{(mn+1)}.

Theorem 12.

Let w=gwyww=g_{w}y_{w} where gwGg_{w}\in G and ywS~n/Gy_{w}\in\widetilde{S}_{n}/G. Write σ=f(yw1)Sn\sigma=f(y_{w}^{-1})\in S_{n} and let XX be the nn-window of yw1y_{w}^{-1}. The partition associated to ww is the partition in Cn(mn1)C_{n}^{(mn-1)} with nn-set equivalent to σgwσ1mn1X\sigma g_{w}\sigma^{-1}\cdot_{mn-1}X (considered as a set).

This restricts to a bijection between mm-maximal alcoves wA0wA_{0} and Cn(mn1)C_{n}^{(mn-1)}.

Notice if we assume gw=eg_{w}=e, then these are precisely the correspondences described in [11] and [12]. The key result of this paper is that this extends the Fishel-Vazirani results to give a bijection between Cn(mn+1)C_{n}^{(mn+1)} and the set of all mm-minimal alcoves in the mm-Shi arrangement and then a bijection between Cn(mn1)C_{n}^{(mn-1)} and the mm-maximal alcoves. The proofs are virtually the same for both results, merely swapping minimal for maximal, ceilings for floors, and t=mn+1t=mn+1 for t=mn1t=mn-1. For clarity, the exposition in what follows will discuss the minimal case only, but the results will be spelled out for both cases.

A broad perspective on the bijection as a whole might shed some light on the “twist” by σ\sigma in this action. We start with the correspondence between dominant regions and nn-sets of (n,mn+1)(n,mn+1)-core partitions. The mm-minimal alcoves can be divided into subsets based on which of them are in the SnS_{n}-orbit of one another. (The SnS_{n} action restricted to only minimal alcoves is not well-defined, but as we shall see, a relationship like the orbit-stabilizer theorem does exist.) The level tt action does the same with the orbits Cn(mn+1)C_{n}^{(mn+1)}, a set of the same size as the number of mm-minimal alcoves. We hope for a bijection between these sets, which we will obtain by way of cosets of certain subgroups on either side of the correspondence. On the partition side, we have the tools in place - the stabilizer (and thus the orbit) under the level tt action of GG is controlled by the labels on the floors of the corresponding alcove. On the alcove side, the group is built from the walls of the dominant mm-minimal alcove. The twisting as described above creates the link between the label of a facet and the root indexing the corresponding wall which will bridge the gap between the two subgroups. Lemma 8 above merely describes how that link directly relates to the orientation of wA0wA_{0} as related to A0A_{0}. The added relation that comes from substituting w0w_{0} for s0s_{0} is a reflection of the fact that s0A0s_{0}A_{0} and w0A0w_{0}A_{0} have the same orientation.

Refer to caption

Figure 6: The Shi arrangement 𝒮2,1\mathcal{S}_{2,1}. The shaded area is the dominant chamber.

We also give an example illustrating the twist. First we examine the alcove A marked in Figure 6 by w=s0s1w=s_{0}s_{1}. The 3-window of w1w^{-1} is X=(1,0,4)X=(-1,0,4), so that σ=s2s1\sigma=s_{2}s_{1}. Notice that the alcoves s1As_{1}A and s2s1As_{2}s_{1}A are also minimal alcoves, and σs1σ1=s2s1s2\sigma s_{1}\sigma^{-1}=s_{2}s_{1}s_{2}, while σs2s1σ1=s2s1\sigma s_{2}s_{1}\sigma^{-1}=s_{2}s_{1}. Then s1s2s1t{0,4,1}t{3,4,4}s_{1}s_{2}s_{1}\cdot_{t}\{0,4,-1\}\equiv_{t}\{3,4,-4\}, while s2s1t{0,4,1}={0,7,4}s_{2}s_{1}\cdot_{t}\{0,4,-1\}=\{0,7,-4\} - these 33-sets are the only other elements of the orbit of {0,4,1}\{0,4,-1\} in C3(4)C_{3}^{(4)}.

Now, notice that these last calculations could perhaps have been reached more easily - s1s_{1} could act in a way that mimics the level tt action of S~n\widetilde{S}_{n} on (0,1,2)(0,1,2) - adding 4 to the first entry, subtracting 4 from the second, and swapping the resulting numbers. Applying this to {1,0,4}\{-1,0,4\} (in that order) yields {4,3,4}\{-4,3,4\}, and then carrying out a similar process on the second and third numbers (mimicing the action of s2s_{2}) gives {4,0,7}\{-4,0,7\}. However, if we let AA be the alcove marked s0s_{0}, it has nn-window (1,1,3)(-1,1,3), and the alcoves s1As_{1}A and s2As_{2}A are also minimal. Now, if s1s_{1} were to shift the first two entries by 4 and then swap them as before, this would yield (3,3,3)(-3,3,3), which is no-longer a 3-window! To “properly” shift and swap 1 and -1, we must use σ=s1s2s1\sigma=s_{1}s_{2}s_{1} and note that σs1σ1=s2\sigma s_{1}\sigma^{-1}=s_{2}. So we apply the level tt action of s2s_{2} to {1,1,3}\{-1,1,3\} so that the action adds 4 to 1 and subtracts from -1, properly swapping the mod 3 congruence classes and giving {5,5,3}\{-5,5,3\}.

In short, when we write w=gwyww=g_{w}y_{w}, we let yw1y_{w}^{-1} act via the level 11 action on congruence classes in the nn-window, and then let gwg_{w} act via the level tt action on positions in the nn-window. The resulting window indexes the desired partition.

To work toward proving our main result, we first need to show that for every mm-minimal alcove wA0wA_{0}, once we write w=gwyww=g_{w}y_{w} as above, ywA0y_{w}A_{0} is an mm-minimal alcove.

Lemma 13.

Let wA0wA_{0} be an mm-minimal alcove of 𝒮n,m\mathcal{S}_{n,m}, and let πSn\pi\in S_{n} be the unique element so πwA0\pi wA_{0} is dominant. Then πwA0\pi wA_{0} is mm-minimal.

Proof. The action of SnS_{n} permutes the hyperplanes Hα,kH_{\alpha,k} for fixed kk because the sis_{i} for i>0i>0 are isometries that fix the origin. Note that if πwA0\pi wA_{0} were not mm-minimal, there would be a hyperplane Hα,kH_{\alpha,k} with k>mk>m that is a floor of πwA0\pi wA_{0}, but where that hyperplane is a ceiling of some chamber πwsiA0\pi ws_{i}A_{0}. But then π1(Hα,k)\pi^{-1}(H_{\alpha,k}) is a floor of wA0wA_{0}, a contradiction since k>mk>m.

This lemma also holds for maximal alcoves - the proof is the same, simply swapping the roles of floors and ceilings.

Lemma 14.

Let wA0wA_{0} be an mm-maximal alcove of 𝒮n,m\mathcal{S}_{n,m}, and let πSn\pi\in S_{n} be the unique element so πwA0\pi wA_{0} is dominant. Then πwA0\pi wA_{0} is mm-maximal.

We would like to make an observation about which alcoves in the SnS_{n}-orbit of a dominant mm-minimal alcove can themselves be mm-minimal. Specifically, we want to show that these alcoves are also in bijection with the cosets of a certain subgroup of SnS_{n} built from the dominant alcove. If these subgroups (and thus sets of cosets) correspond to the level tt stabilizers of the corresponding partition, then our results are proven.

We recall that for I{1,2,,n1}I\subseteq\{1,2,\ldots,n-1\}, the parabolic subgroup GIG_{I} of SnS_{n} is the group generated by {(i,i+1)|iI}\{(i,i+1)\,|\,i\in I\}. There is a nice characterization of GIG_{I}’s cosets - specifically, the elements of GG that do not have any (i,i+1)(i,i+1) for iIi\in I as a right descent form a set of minimal length left coset representatives for GIG_{I}. ([6], section 2.4) We wish to generalize this result to groups generated by any set of transpositions in SnS_{n}. First, we note that if XX is a set of transpositions in SnS_{n}, then the group GXG_{X} it generates is a direct product of symmetric groups. Specifically, we define a set partition on {1,2,,n}\{1,2,\ldots,n\} by choosing the finest set partition so that jj and kk are in the same set for each (j,k)X(j,k)\in X. Then GXG_{X} is the product of the symmetric groups on each set in this partition.

Lemma 15.

Let XX be a set of transpositions in SnS_{n}. Then the subgroup GXG_{X} generated by XX has a unique set of minimal length left coset reprsentatives in SnS_{n}.

Proof. Let wGw\in G and consider the one-line notation for ww, a1a2ana_{1}a_{2}\ldots a_{n} with ai=w(i)a_{i}=w(i) for all ii. Then if (j,k)(j,k) is a transposition, the one-line word for w(j,k)w\cdot(j,k) is the same word but with the positions of jj and kk swapped. Then since GXG_{X} is a product of full symmetric groups on some sets XiX_{i}, we can rearrange each such set XiX_{i} by swapping elements of XiX_{i} within the one-line word, and the resulting word will correspond to another element in the same coset wGXwG_{X}. However, there is a unique such word that has each set XiX_{i} sorted in increasing order, which will srictly minimize the number of inversions. Thus, that one-line word is the unique minimal length coset representative for wGI.wG_{I}.\qed

Now, we need a characterization of these minimal coset representatives for GXG_{X}. Unfortunately, in general, it is not sufficient to find the elements ww so that (wx)>(w)\ell(wx)>\ell(w) for all xXx\in X. (This is the usual condition for coset representatives of parabolic subgroups. [6]) Say, for example, that n=4n=4 and X={(3,4),(1,4)}={w3,w0}X=\{(3,4),(1,4)\}=\{w_{3},w_{0}\}. Then the unique minimal set of left coset representatives for GXG_{X} is {e,w1,w2,w3w2}\{e,w_{1},w_{2},w_{3}w_{2}\}. However, the classical definition does not identify these coset representatives in this case. For example, w=w1w2w1w=w_{1}w_{2}w_{1} (3214 in one-line notation) has the classical property: right-multiplying by either (3,4)(3,4) or (1,4)(1,4) will increase the number of inversions. We must multiply by (1,3)X(1,3)\notin X to get to the minimal coset representative ee. In some sense, 3214 is a local minimum of the length function within its coset, but not a global minimum. Even though GXG_{X} is conjugate to a parabolic subgroup of S4S_{4}, the classical coset characterization fails. (It seems that in general, the minimal coset representatives of GXG_{X} must be described as the ww so that (wy)>(w)\ell(wy)>\ell(w) for all yGXy\in G_{X}, so that non-minimal coset representatives come equipped with a weaker property.)

The issue arose here because 1,3, and 4 can be permuted freely, but only using the transpositions (1,4)(1,4) and (3,4)(3,4), which are somewhat out of order - this problem would not arise if X={(1,3),(3,4)}X=\{(1,3),(3,4)\}. Luckily for us, the particular groups GXG_{X} that arise from the Shi arrangement avoid this obstruction and do follow the classical characterization of minimal coset reprsentatives, which we show now. Consider an mm-minimal dominant alcove wA0wA_{0}. It will have floors of the form Hα,kH_{\alpha,k} for some positive roots α\alpha and kmk\leq m. For each α\alpha so that Hα,mH_{\alpha,m} is a floor of the alcove, we consider the element sαs_{\alpha} of GG, considered as the Weyl group of type AnA_{n}. Specifically, if α=ϵiϵj\alpha=\epsilon_{i}-\epsilon_{j} for i<ji<j, then sαs_{\alpha} is the transposition (i,j)(i,j). We let XX be the set of such sαs_{\alpha} and we will soon show that GXG_{X} determines which alcoves in the GG-orbit of wA0wA_{0} are again mm-minimal. First though, we characterize the minimal coset representatives of these groups.

Lemma 16.

Let wA0wA_{0} be a dominant mm-minimal alcove of Sn,mS_{n,m}.

  1. 1.

    If Hϵiϵj,mH_{\epsilon_{i}-\epsilon_{j},m} is a floor of wA0wA_{0} for some i<ji<j, then there is no other k<jk<j so that Hϵkϵj,mH_{\epsilon_{k}-\epsilon_{j},m} is a floor of wA0wA_{0}.

  2. 2.

    If Hθ,mH_{\theta,m} is a floor of wA0wA_{0}, then it is the only floor of the form Hα,mH_{\alpha,m}.

  3. 3.

    If Hϵiϵj,mH_{\epsilon_{i}-\epsilon_{j},m} is a ceiling of wA0wA_{0} for some i<ji<j, then there is no other k<jk<j so that Hϵkϵj,mH_{\epsilon_{k}-\epsilon_{j},m} is a ceiling of wA0wA_{0}.

  4. 4.

    If Hθ,mH_{\theta,m} is a ceiling of wA0wA_{0}, then it is the only ceiling of the form Hα,mH_{\alpha,m}.

Proof. Let XX be the nn-window of w1w^{-1}. First, if Hϵiϵj,mH_{\epsilon_{i}-\epsilon_{j},m} is a floor of wA0wA_{0}, then the iith and jjth entries of XX differ by exactly mn+1mn+1. But the entries of XX are strictly increasing, so if another entry of XX differed from the jjth by mn+1mn+1, it would come after the jjth entry.

Then if Hθ,mH_{\theta,m} is a floor of wA0wA_{0}, the first and last entries of XX differ by exactly mn+1mn+1. But since XX is sorted in ascending order, no other pair of entries can differ by exactly mm. The last two results again simply swap ceilings for floors and mn1mn-1 for mn+1mn+1.

This lemma ensures that the set XX cannot be “out of order” in the way that caused the problem in our example above if it comes from floors or ceilings of the form Hα,mH_{\alpha,m} for a particular alcove.

Proposition 17.

Let wA0wA_{0} be a dominant mm-minimal alcove of Sn,mS_{n,m}. Let XX be a set of transpositions which has the property that if sϵiϵjXs_{\epsilon_{i}-\epsilon_{j}}\in X for i<ji<j, then for k<jk<j, kik\neq i, the reflection sϵkϵjXs_{\epsilon_{k}-\epsilon_{j}}\notin X. Define GX={wSn|(wx)>(w) for all xX}G^{X}=\{w\in S_{n}\,|\,\ell(wx)>\ell(w)\textrm{ for all }x\in X\}. Then GXG^{X} is the set of minimal coset representatives for GXG_{X}.

Proof. First, it is clear that any minimal coset representative for GXG_{X} has the property that (wx)>(w)\ell(wx)>\ell(w) for all xXx\in X. We must merely show that, for any wSnw\in S_{n}, if there is some yGXy\in G_{X} with (wy)<(w)\ell(wy)<\ell(w), then in fact there is an xXx\in X with (wx)<(w)\ell(wx)<\ell(w) so that wGXw\notin G^{X}.

As before, we consider a1a2ana_{1}a_{2}\ldots a_{n}, the word for ww in one-line notation. If (wy)<(w)\ell(wy)<\ell(w) for some yGXy\in G_{X}, then choose some inversion ai>aja_{i}>a_{j} with i<ji<j so that aia_{i} occurs after aja_{j} in the word for wywy. This means that the set partition of {1,2,,n}\{1,2,\ldots,n\} associated to XX contains some set BB that contains both aia_{i} and aja_{j}. Write B=(b1,b2,bk)B=(b_{1},b_{2},\ldots b_{k}) in increasing order. Then by the previous lemma, XX must contain the transpositions (b1,b2)(b_{1},b_{2}), (b2,b3),,(bk1,bk)(b_{2},b_{3}),\ldots,(b_{k-1},b_{k}). If aia_{i} and aja_{j} appear consecutively in BB, then (ai,aj)X(a_{i},a_{j})\in X, and (w(ai,aj))<(w)\ell(w\cdot(a_{i},a_{j}))<\ell(w), as desired. Otherwise, we proceed inductively.

If they are not consecutive in BB, choose some ara_{r} with aj<ar<aia_{j}<a_{r}<a_{i}. If r<jr<j, then ara_{r} and aja_{j} are an inversion in ww. If r>jr>j, then r>ir>i, so that ara_{r} and aia_{i} are an inversion in ww. Either way, we have found another pair of elements of BB which form an inversion in ww and whose entries in BB are closer together than aia_{i} and aja_{j}. Repeating this, we eventually find consecutive elements of BB that are inverted in ww.

This characterization of the groups GXG_{X} finally lets us show that the mm-minimal alcoves in the SnS_{n} orbit of an mm-minimal alcove are in bijection with GXG^{X}.

Theorem 18.

Let wS~nw\in\widetilde{S}_{n} such that wA0wA_{0} is dominant and mm-minimal. Let XX be the set of transpositions sαs_{\alpha} so that Hα,mH_{\alpha,m} is a floor of the alcove wA0wA_{0}. Let ρSn\rho\in S_{n}. Then ρwA0\rho wA_{0} is mm-minimal if and only if ρGX\rho\in G^{X}.

Proof. First, note that the action of GG permutes the hyperplanes Hα,kH_{\alpha,k} for fixed kk. Thus the only way that ρwA0\rho wA_{0} can fail to be mm-minimal is if ρ\rho sends a hyperplane Hα,mH_{\alpha,m} that is a floor of wA0wA_{0} to a hyperplane Hα,mH_{\alpha^{\prime},m} which is a floor of ρwA0\rho wA_{0}, where α<0\alpha^{\prime}<0. By Lemma 1, if Hα,mH_{\alpha,m} is a floor of wA0wA_{0} with label jj, then w(αj)=αmδw(\alpha_{j})=\alpha-m\delta. But then ρw(αj)=ρ(α)mδ\rho w(\alpha_{j})=\rho(\alpha)-m\delta. So we let α=ρ(α)\alpha^{\prime}=\rho(\alpha) and note that if α<0\alpha^{\prime}<0, then α\alpha is an inversion of ρ\rho, so that (ρsα)<(ρ)\ell(\rho s_{\alpha})<\ell(\rho). This cannot occur if ρGX\rho\in G^{X}.

Conversely, though, if ρGX\rho\notin G^{X}, there must be some sαXs_{\alpha}\in X so that (ρsα)<(ρ)\ell(\rho s_{\alpha})<\ell(\rho). Assume that the facet of wA0wA_{0} contained in Hα,mH_{\alpha,m} has label jj. Then w(αj)=αmδw(\alpha_{j})=\alpha-m\delta, and by assumption ρw(αj)=αmδ\rho w(\alpha_{j})=\alpha^{\prime}-m\delta where α<0\alpha^{\prime}<0. This implies that Hα,mH_{\alpha^{\prime},m} is a floor of ρwA0\rho wA_{0}, which is thus not mm-minimal.

This proof needs very few adjustments to establish the following.

Theorem 19.

Let wS~nw\in\widetilde{S}_{n} such that wA0wA_{0} is dominant and mm-maximal. Let XX be the set of transpositions sαs_{\alpha} so that Hα,mH_{\alpha,m} is a ceiling of the alcove wA0wA_{0}. Let ρSn\rho\in S_{n}. Then ρwA0\rho wA_{0} is mm-minimal if and only if ρGX\rho\in G^{X}.

Proof. Now, the only way that ρwA0\rho wA_{0} can fail to be mm-maximal is if ρ\rho sends a hyperplane Hα,mH_{\alpha,m} that is a ceilng of wA0wA_{0} to a hyperplane Hα,mH_{\alpha^{\prime},m} which is a ceiling of ρwA0\rho wA_{0}, where α<0\alpha^{\prime}<0. By Lemma 1, if Hα,mH_{\alpha,m} is a ceiling of wA0wA_{0} with label jj, then w(αj)=mδαw(\alpha_{j})=m\delta-\alpha. But then ρw(αj)=mδρ(α)\rho w(\alpha_{j})=m\delta-\rho(\alpha). So we let α=ρ(α)\alpha^{\prime}=\rho(\alpha) and note that if α<0\alpha^{\prime}<0, then α\alpha is an inversion of ρ\rho, so that (ρsα)<(ρ)\ell(\rho s_{\alpha})<\ell(\rho). This cannot occur if ρGX\rho\in G^{X}.

Conversely, though, if ρGX\rho\notin G^{X}, there must be some sαXs_{\alpha}\in X so that (ρsα)<(ρ)\ell(\rho s_{\alpha})<\ell(\rho). Assume that the facet of wA0wA_{0} contained in Hα,mH_{\alpha,m} has label jj. Then w(αj)=mδαw(\alpha_{j})=m\delta-\alpha, and by assumption ρw(αj)=mδα\rho w(\alpha_{j})=m\delta-\alpha^{\prime} where α<0\alpha^{\prime}<0. This implies that Hα,mH_{\alpha^{\prime},m} is a ceiling of ρwA0\rho wA_{0}, which is thus not mm-maximal.

We now understand the alcove side of the bijection, which essentially completes the proof of our two main results.

Proof of Theorem 11 and 12. The mm-minimal alcoves of 𝒮n,m\mathcal{S}_{n,m} are in bijection with pairs consisting of a dominant mm-minimal alcove wA0wA_{0} and a minimal coset representative of GXG_{X} as defined in Theorem 18. For any such pair, by Lemmas 8 and 6, GXG_{X} is conjugate to HH, the GG-stabilizer of the partition w1w^{-1}\emptyset in Cn(mn+1)C_{n}^{(mn+1)} under the level tt action. Thus the cosets of GXG_{X} and HH are in bijection.

Similarly, the mm-maximal alcoves of 𝒮n,m\mathcal{S}_{n,m} are in bijection with pairs consisting of a dominant mm-maximal alcove wA0wA_{0} and a minimal coset representative of GXG_{X} as defined in Theorem 19. For any such pair, by Lemmas 8 and 6, GXG_{X} is conjugate to HH, the GG-stabilizer of the partition w1w^{-1}\emptyset in Cn(mn1)C_{n}^{(mn-1)} under the level tt action. Thus the cosets of GXG_{X} and HH are in bijection.

Before we close, we want to show one relationship between our results and other combinatorial indexings of Shi regions. Specifically, [4] assigns an mm-parking function to each region of 𝒮n,m\mathcal{S}_{n,m}. We show that our bijection reflects the structure of these parking functions - specifically, their stabilizers. (Note this argument is essentially in [3], but we include it here for completeness.)

Proposition 20.

Let wA0wA_{0} be a dominant mm-minimal alcove, with XX the transpositions associated to floors of wA0wA_{0} as defined as in Theorem 18. Let ff be the mm-parking function associated to wA0wA_{0} in [4]. Then if xXx\in X, xf=fx\cdot f=f when acting via permutation.

Proof. The Athanasiadis-Linusson bijection is as follows. Make a list consisting of terms of the form xi+kx_{i}+k for 0km10\leq k\leq m-1. Arrange the list in the unique permutation {yi}\{y_{i}\} so that for points in wA0wA_{0}, y1>y2>>ymny_{1}>y_{2}>\ldots>y_{mn} holds. We then connect each xi+kx_{i}+k for k>0k>0 to xi+k1x_{i}+k-1 with an arc. In addition, we connect xix_{i} to xj+m1x_{j}+m-1 with an arc whenever wA0Hϵiϵj,m+wA_{0}\subseteq H_{\epsilon_{i}-\epsilon_{j},m}^{+}. Finally we remove each arc containing another and define f(i)f(i) to be the position of the leftmost term in the chain containing xix_{i}.

So, assume sϵiϵjXs_{\epsilon_{i}-\epsilon_{j}}\in X for i<ji<j, so that the construction for the parking functions connects xix_{i} to xj+m1x_{j}+m-1. Thus, as long as this arc is not deleted in the construction, f(i)=f(j)f(i)=f(j). However, this arc would only be deleted if another arc were contained in it. So assume xi>xr+k>xs+>xj+m1x_{i}>x_{r}+k>x_{s}+\ell>x_{j}+m-1 is a sublist in the construction with xr+kx_{r}+k connected to xs+x_{s}+\ell.

For the first case, this configuration could occur if r=sr=s and =k1\ell=k-1. Note that xi>xr>xsx_{i}>x_{r}>x_{s}, so i>r>si>r>s by dominance. But then xixr>kx_{i}-x_{r}>k, and xrxj>mkx_{r}-x_{j}>m-k. If Hϵiϵj,mH_{\epsilon_{i}-\epsilon_{j},m} were a floor of the region, then there would be an alcove of 𝒜𝓃\mathcal{A_{n}} sharing that facet with wA0wA_{0}. However, xixr>kx_{i}-x_{r}>k, and xrxj>mkx_{r}-x_{j}>m-k would still hold on that region, contradicting the fact that xixj<mx_{i}-x_{j}<m.

For the second case, it could occur that k=0k=0 while =m1\ell=m-1. However, this would mean that xi>xr>xs>xjx_{i}>x_{r}>x_{s}>x_{j}, so that i>r>s>ji>r>s>j by dominance. However, we then have xixr>0x_{i}-x_{r}>0, xrxs>mx_{r}-x_{s}>m, and xsxj>0x_{s}-x_{j}>0. Again, it is impossible for Hϵiϵj,mH_{\epsilon_{i}-\epsilon_{j},m} to be a floor of this region by the same argument.

So, XX is a subset of the stabilizer of ff. However, the index of the stabilizer of ff is the same as the index of GXG_{X} by Theorem 11, so GXG_{X} has the same number of elements as the stabilizer of ff and they must be equal.

7 Conclusion

Our two main results provide a unified extension of the results of [11] and [12]. It is worth noting that these bijections reflect other combinatorial indexings of Shi regions. In essence, Proposition 20 shows that the level tt action translates the SnS_{n}-action inherent in the Athanasiadis-Linusson bijection (along with the corresponding stabilizer and orbits) and translates them into the partition context of Fishel-Vazirani. The labelled Dyck paths of Garsia and Haiman ([15]) are similar - each valid Dyck path corresponds to a dominant mm-minimal alcove, and the labels are permutations which represent the different Weyl chambers with a minimal alcove in the SnS_{n} orbit of the dominant one. Whether Cn(mn+1)C_{n}^{(mn+1)} is the exact right indexing set to use is somewhat questionable - the GG-orbits of the (n,mn+1)(n,mn+1) cores (ignoring the equivalence mn+1\equiv_{mn+1}) would work just as well to index the minimal alcoves, but a description of that set of partitions is somewhat elusive. A better understanding of how the level tt action acts directly on abaci might be helpful in understanding it. Another area of interest might be understanding how to turn a partition in Cn(mn+1)C_{n}^{(mn+1)} directly into a parking function. For (n,n+1)(n,n+1)-core partitions, the process is relatively straightforward. We can take the positive abacus corresponding to λ\lambda and read it as a Dyck path as in [1] - the area above that path forms a partition λ\lambda^{\prime} that fits in the “staircase” partition (n1,n2,,1)(n-1,n-2,\ldots,1). Then the removable boxes in λ\lambda^{\prime} encode roots as described in [13]. The Athanasiadis-Linusson diagram corresponding to the same region as λ\lambda is 12n12\ldots n, with an arc connecting ii and jj exactly if the box corresponding to the root ϵiϵj\epsilon_{i}-\epsilon_{j} is removable in λ\lambda^{\prime}. A similar process to go directly from Cn(mn+1)C_{n}^{(mn+1)} to an mm-parking function would be greatly desirable.

It is also worth noting that near the completion of this paper, the author became aware of [8], which takes a vastly different approach to characterizing the mm-minimal alcoves than Theorem 18. A better understanding of how these characterizations interact would be greatly desirable - in particular determining the extent to which any of our results can be generalized out of type A seems like an important next step.

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