Math 202C: Lecture 4

*** Problems in this lecture due April 12 at 23:59 ***

Let S_n=\mathrm{Aut}\{1,\dots,n\} be the symmetric group on \{1,\dots,n\}. Our convention is that permutations are multiplied left-to-right, \rho\sigma := \sigma \circ \rho. We identify $lates S_n$ with its Cayley graph \mathrm{Cay}(S_n,T_n) as generated by the conjugacy class of transpositions,

T_n=\{\tau=(s t) \colon 1 \leq s <t \leq n\}.

Thus, two permutations \rho,\sigma \in S_n are adjacent if and only if \sigma=\rho\tau for \tau \in T_n. Under this identification, S_n decomposes into a disjoint union of n independent sets, the levels

L_r=\{\pi \in S_n \colon |\pi|=r\} = \{\pi \in S_n \colon n-\mathsf{cyc}(\pi)=r\}, \quad 0 \leq r \leq n-1.

The cardinalities of these levels make up the nth row in the number triangle whose entries are the Stirling numbers of the first kind. Each level further decomposes as a disjoint union of conjugacy classes: we have

L_r = \bigsqcup\limits_{\substack{\alpha \in \Lambda \\ \ell(\alpha)=n-r}} C_\alpha,

where \Lambda is the set of partitions of n, and \ell(\alpha) is the number of terms in the partition \alpha. We can encode this decomposition algebraically in \mathcal{C}(S_n) as

|L_r\rangle = \sum\limits_{\substack{\alpha \in \Lambda \\ \ell(\alpha)=n-r}} |C_\alpha\rangle.

Note that, because S_n is an ambivalent group, each class indicator |C_\alpha\rangle is a selfadjoint element in the convolution algebra \mathcal{C}(S_n). In the regular representation, the above becomes an identity in \mathrm{End}\mathcal{C}(S_n), namely

L_r = \sum\limits_{\substack{\alpha \in \Lambda \\ \ell(\alpha)=n-r}} C_\alpha,

and we have used this already to give a simple proof of the fact that the metric level set operators L_1,\dots,L_{n-1} on S_n=\mathrm{Cay}(S_n,T_n) commute. In particular, these selfadjoint operators are simultaneously diagonalizable. In this Lecture, we will obtain a different combinatorial decomposition of L_r which opens the door to actually diagonalizing L_1,\dots,L_{n-1}.

In Lecture 1, we defined an edge-labeling of S_n by marking each edge corresponding to the transposition (s\ t) with t, the larger of the two elements it transposes. We defined a walk on S_n to be strictly monotone if the labels of the edges it traverses form a strictly increasing sequence. It is clear that the length of any such walk is at most n-1, which is the diameter of S_n. The following remarkable result holds.

Theorem 4.1. There exists a unique strictly monotone walk between every pair of permutations, and this walk is a geodesic.

Theorem 4.1 gives a second description of L_r as the set of all strictly monotone r-step walks on S_n emanating from the identity permutation, \iota. The figure below illustrates this for n=4, with \text{blue}=2, \text{purple}=3, \text{black}=4.

The Jucys-Murphy spanning tree of S_4.

Definition 4.2. The Jucys-Murphy subsets of S_n are defined by

J_1=\emptyset

J_2 = \{(1 2)\}

J_3=\{(1 3),(2 3)\}

\vdots

J_n=\{(1 n),(2 n),\dots,(n-1 n).\}

Thus,

J_t = \{(s t) \colon 1 \leq s <t\}

is the set of all transpositions which swap a given number t with smaller numbers s. The set J_1 = \emptyset is included only for notational convenience, as a sequence with initial index 2 may be unsettling. It is clear that the JM-subsets of S_n are pairwise disjoint, and that their union is T_n=L_1. More generally, the set of all r-step strictly monotone walks on S_n emanating from the identity permutation \iota is in bijection with

\bigsqcup\limits_{1 \leq t_1 < \dots < t_r \leq n} J_{t_1} \times J_{t_2} \times \dots \times J_{t_r},

and hence we have a bijection.

L_r \simeq \bigsqcup\limits_{1 \leq t_1 < \dots < t_r \leq n} J_{t_1} \times J_{t_2} \times \dots \times J_{t_r},

We will now encode this correspondence algebraically in \mathcal{C}(S_n).

Definition 4.3. The Jucys-Murphy elements in \mathcal{C}(S_n) are

|J_t\rangle = \sum\limits_{1 \leq s<t} |s t\rangle, \quad 1 \leq t \leq n.

The JM-elements are selfadjoint elements satisfying \langle J_t | J_t \rangle = t-1 and

|T_n\rangle = \sum\limits_{t=1}^n |J_t\rangle.

Thus, J_1,\dots,J_n \in \mathrm{End}\mathcal{C}(S_n) are selfadjoint operators satisfying

T_n = \sum\limits_{t=1}^n J_t,

where T_n is the adjacency operator on \mathrm{Cay}(S_n,T_n).

Problem 4.2. Prove that the operator norm of J_t is \|J_t\|=t-1.

At this point, we can write down the algebraic identity

|L_r\rangle = \sum\limits_{1 \leq t_1 < \dots < t_r \leq n}|J_{t_1}\rangle \dots |J_{t_n}\rangle.

This is equivalent to the combinatorial decomposition of L_r in terms of JM-subsets, but at the same time it has many advantages. To see these we first the need the following fact.

Theorem 4.3. The JM-elements |J_1\rangle,\dots,|J_n\rangle pairwise commute in \mathcal{C}(S_n).

One way to verify this would be to check directly that the products

|J_k\rangle|J_l\rangle = \sum\limits_{i<k}\sum\limits_{j<l}|ik\rangle|jl\rangle \quad\text{and}\quad |J_k\rangle|J_l\rangle = \sum\limits_{i<k}\sum\limits_{j<l}|jl\rangle|ik\rangle

are indeed the same. We will instead construct a manifestly commutative subalgebra \mathcal{J}_n of \mathcal{C}(S_n) which contains \{|J_1\rangle,\dots,|J_n\rangle\}.

The key to this construction is the fact that the symmetric groups S_1,S_2,\dots,S_n form an inductive chain

S_1 \subset S_2 \subset \dots \subset S_n,

where we identity S_k=\mathrm{Aut}\{1,\dots,k\} with the subgroup of S_n consisting of permutations which fix the numbers k+1,k+2,\dots,n. This gives an inductive chain of algebras,

\mathcal{C}(S_1) \subset \mathcal{C}(S_2) \subset \dots \subset \mathcal{C}(S_n),

each of which has its own center, giving us a collection

Z\mathcal{C}(S_1),\ Z\mathcal{C}(S_2),\ \dots,\ Z\mathcal{C}(S_n)

of commutative subalgebras of \mathcal{C}(S_n). However, it is not true that these commutative subalgebras form an inductive chain. In fact, they are as disjoint as subalgebras can be.

Problem 4.3. Prove that Z\mathcal{C}(S_k) \cap Z\mathcal{C}(S_l)=\mathbb{C}|\iota\rangle for k<l.

What is true is that each element of Z\mathcal{C}(S_k) commutes with every element of Z\mathcal{C}(S_l). Indeed, assuming k<l, the center Z\mathcal{C}(S_l) consists of all elements commuting with every element of \mathcal{C}(S_l), and

Z\mathcal{C}(S_k) \subset \mathcal{C}(S_k) \subset \mathcal{C}(S_l).

Definition 4.4. The Jucys-Murphy subalgebra \mathcal{J}_n of \mathcal{C}(S_n) is the commutative subalgebra generated by Z\mathcal{C}(S_1) \cup Z\mathcal{C}(S_2) \cup \dots \cup Z\mathcal{C}(S_n).

Problem 4.4. Prove that \dim \mathcal{J}_n \geq \sum_{k=1}^n p(k)-(n-1), where p(k) is the number of partitions of k.

The commutativity of the JM-elements follows from the fact that they belong to the JM-subalgebra.

Theorem 4.4. We have |J_1\rangle,|J_2\rangle,\dots,|J_n\rangle \in \mathcal{J}_n.

Proof: For each 1 \leq k \leq n, let

|T_k\rangle = \sum\limits_{1 \leq s < t \leq k} |st\rangle

be the sum of all transpositions in S_k. This is an element of \mathcal{C}(S_k), and indeed an element of Z\mathcal{C}(S_k). Now observe that

|J_k\rangle = |T_k\rangle - |T_{k-1}\rangle,

which expresses |J_k\rangle as a difference of elements in \mathcal{J}_n. \square

2 Comments

  1. a r n o says:

    Is there a typo? In its current form, theorem 4.4 is a bit of a letdown…

    1. Fixed, thanks.

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