2024-05-05
Algebra-I
00

Contents

§ 5 Cycle Notation
§ 5.1 Cycles
§ 5.2 Disjoint Cycles
§ 5.3 Cycle Notation
§ 5.4 Conjugacy Classes in $S_n$
§ 5.5 The Alternating Group
1. Kernel of the Sign Homomorphism
2. Conjugation Preserves the Parity of a Permutation
3. The Index of $An$ in $Sn$

§ 5 Cycle Notation

Definition 5.1 Suppose we have a group action

GAutsetG \to \mathrm{Aut}_{\text{set}}

on a set XX. Fix gGg \in G. We call the action

gGAutset\langle g \rangle \to G \to \mathrm{Aut}_{\text{set}}

the action of gg on XX.

Here gG\langle g \rangle \to G is a group homomorphism because the inclusion map of a subgroup is a group homomorphism. The map gAutset\langle g \rangle \to \mathrm{Aut}_{\text{set}} is a group homomorphism because the composition of two group homomorphisms is again a group homomorphism.

Essentially, the action of gg on XX can be expressed using cycle notation by decomposing gg into cycles, where each cycle corresponds to an orbit of the action of gg on XX.

§ 5.1 Cycles

Definition 5.2 If σSn\sigma \in S_n, and the action of σ\sigma on n\underline{n} has at most one orbit of size 2\geqslant 2, then σ\sigma is called a cycle.

Example 5.1

  • σ=1Sn\sigma=1_{S_n} has only orbits of size 11, so 1Sn1_{S_n} is a cycle.

  • Let τ:44\tau:\underline{4}\to\underline{4} be defined by

12213443\begin{aligned} 1 &\mapsto 2\\ 2 &\mapsto 1\\ 3 &\mapsto 4\\ 4 &\mapsto 3 \end{aligned}

which we may draw as

This is not a cycle because it has two orbits of size 2\geqslant2: 1,2{1,2} and 3,4{3,4}.

  • Let τ:55\tau:\underline{5}\to\underline{5} be defined by
1122354354\begin{aligned} 1 &\mapsto 1\\ 2 &\mapsto 2\\ 3 &\mapsto 5\\ 4 &\mapsto 3\\ 5 &\mapsto 4 \end{aligned}

which may be drawn as

This is a cycle.

Definition 5.3 If σSn\sigma\in S_n is a cycle, we use σn\underline{\sigma}\subset\underline{n} to denote the orbit of size 2\geqslant2. For σ=1G\sigma=1_G, we define

1G:=.\underline{1_G}:=\varnothing.

§ 5.2 Disjoint Cycles

Example 5.2

σ\underline{\sigma} is a subset, so the order of its elements does not matter. In particular, it is not a set together with a choice of ordering.

Definition 5.4 If σ,τSn\sigma,\tau\in S_n are cycles, we say that σ\sigma and τ\tau are disjoint cycles if and only if σ\underline{\sigma} and τ\underline{\tau} are disjoint.

Example 5.3

  • 1G1_G is disjoint from every cycle.

  • cycle and cycle are not disjoint because 1,2{1,2} and 2,3{2,3} intersect.

  • cycle and cycle are disjoint.

Proposition 5.1 Disjoint cycles in SnS_n commute.

Proof: Let σ\sigma and τ\tau be disjoint cycles and take kn=1,2,,nk\in\underline{n}={1,2,\ldots,n}. Then

(στ)(k)={σ(k)if kττ(k)if kτ={σ(k)if kσkif kσ,ττ(k)if kτ.\begin{aligned} (\sigma \circ \tau)(k) &= \begin{cases} \sigma(k) & \text{if } k \notin \underline{\tau}\\ \tau(k) & \text{if } k \in \underline{\tau} \end{cases}\\ &= \begin{cases} \sigma(k) & \text{if } k \in \underline{\sigma}\\ k & \text{if } k \notin \underline{\sigma}, \underline{\tau}\\ \tau(k) & \text{if } k \in \underline{\tau} \end{cases}. \end{aligned}

This follows because

kττ(k)=kσ(τ(k))=σ(k),kττ(k)ττ(k)σσ(τ(k))=τ(k).\begin{align*} k \notin \underline{\tau} &\Rightarrow \tau(k)=k\\ &\Rightarrow \sigma(\tau(k))=\sigma(k),\\ k \in \underline{\tau} &\Rightarrow \tau(k)\in\underline{\tau} \tag*{definition of an orbit}\\ &\Rightarrow \tau(k)\notin\underline{\sigma} \tag*{definition of disjointness}\\ &\Rightarrow \sigma(\tau(k))=\tau(k). \end{align*}

On the other hand,

(τσ)(k)={τ(k)if kσσ(k)if kσ={τ(k)if kτkif kσ,τσ(k)if kσ.\begin{aligned} (\tau \circ \sigma)(k) &= \begin{cases} \tau(k) & \text{if } k \notin \underline{\sigma}\\ \sigma(k) & \text{if } k \in \underline{\sigma} \end{cases}\\ &= \begin{cases} \tau(k) & \text{if } k \in \underline{\tau}\\ k & \text{if } k \notin \underline{\sigma}, \underline{\tau}\\ \sigma(k) & \text{if } k \in \underline{\sigma}. \end{cases} \end{aligned}

Therefore,

στ=τσ.\sigma\circ\tau=\tau\circ\sigma.
 ~\tag*{$\square$}

§ 5.3 Cycle Notation

Definition 5.5 Let σ\sigma be a cycle. The cycle notation of σ\sigma is an expression

(a σ(a) σ2(a)  σσ1(a))(a~\sigma(a)~\sigma^{2}(a)~\cdots~ \sigma^{|\sigma|-1}(a))

where aσa\in\underline{\sigma}.

Example 5.4 If σS5\sigma\in S_5 is as shown below:

then all of the following are cycle notations for σ\sigma:

(1 2 3 5),(2 3 5 1),(5 1 2 3),(3 5 1 2).a=1a=2a=5a=3\begin{array}{cccc} (1~2~3~5), & (2~3~5~1), & (5~1~2~3), & (3~5~1~2). \\ a=1 & a=2 & a=5 & a=3 \end{array}

Example 5.5 If τS5\tau\in S_5 is as shown below:

then

τ=σ,\underline{\tau}=\underline{\sigma},

but no cycle notation of τ\tau is a cycle notation of σ\sigma:

(1 2 5 3),(2 5 3 1),(5 3 1 2),(3 1 2 5).(1~2~5~3),\quad (2~5~3~1),\quad (5~3~1~2),\quad (3~1~2~5).

Implicitly, we identify the various cycle notations representing the same σ\sigma.

Theorem 5.2 Every element

σSn\sigma\in S_n

can be written as a product of disjoint cycles, uniquely up to order.

Proof: For σSn\sigma\in S_n, let Oa{\mathcal{O}_a} be the set of orbits of the action of σ\sigma on n\underline{n}.

For each

Oan/σ,\mathcal{O}_a\in\underline{n}/\langle\sigma\rangle,

choose aOaa\in\mathcal{O}_a and define

σa=(a σ(a)  σOa1(a))\sigma_a = (a~\sigma(a)~\cdots~ \sigma^{|\mathcal{O}_a|-1}(a))

as a cycle.

Then, by definition,

σ=Oaσa\sigma = \prod_{\mathcal{O}_a}\sigma_a

because

Oaσa(k)=σ(k).\prod_{\mathcal{O}_a}\sigma_a(k)=\sigma(k).

Moreover, when we write

Oaσa=σaσbσz\prod_{\mathcal{O}_a}\sigma_a = \sigma_a\cdot\sigma_b\cdots\sigma_z

without specifying an order, this is justified because every pair σa,σb\sigma_a,\sigma_b is disjoint, since distinct orbits are disjoint. Therefore these cycles commute, and the order does not matter.

For uniqueness, suppose someone else writes

σ=τi=τ1τ2τk\sigma = \prod\tau_i = \tau_1\cdot\tau_2\cdots\tau_k

where τi{\tau_i} is a collection of disjoint cycles.

Notice that

{τi}=n/σ.\{\tau_i\} = \underline{n}/\langle\sigma\rangle.

Thus, for each ii, there exists a unique σa\sigma_a such that

σa=τi.\underline{\sigma_a} = \underline{\tau_i}.

Write

τi=(b0 b1  bτi1).\tau_i = (b_0~b_1~\cdots~b_{|\tau_i|-1}).

Then

σ(bi)=bi+1,\sigma(b_i)=b_{i+1},

which proves the result.

 ~\tag*{$\square$}

Example 5.6 Let σS8\sigma\in S_8 be defined as follows:

Then

σ=(7 8 4)(1 2 6)(3 5)=(1 2 6)(7 8 4)(3 5)=(1 2 6)(3 5)(7 8 4)etc.\begin{aligned} \sigma &= (7~8~4)\circ(1~2~6)\circ(3~5)\\ &= (1~2~6)(7~8~4)(3~5)\\ &= (1~2~6)(3~5)(7~8~4) \quad\text{etc.} \end{aligned}

We may regard (1 2 6)(1~2~6) both as a cycle in S8S_8 and as its cycle notation. The element (1 2 6)S8(1~2~6)\in S_8 is represented by

In the second equality, we omit the composition symbol “\circ” for brevity.

Definition 5.6 For σSn\sigma\in S_n, a cycle notation for σ\sigma is an expression

σ=σ1σk\sigma=\sigma_1\cdots\sigma_k

where each σi\sigma_i is a cycle, and every pair σi,σj\sigma_i,\sigma_j with iji\neq j is disjoint.

Example 5.7 If σS5\sigma\in S_5 is as shown below:

then the following are cycle notations for σ\sigma:

(1 2 4)(3 5)(3 5)(1 2 4)(1 2 4)(5 3)(5 3)(1 2 4)(4 1 2)(3 5)(3 5)(4 1 2)(4 1 2)(5 3)(5 3)(4 1 2)(2 4 1)(3 5)(3 5)(2 4 1)(2 4 1)(5 3)(5 3)(2 4 1)\begin{array}{cc} (1~2~4)(3~5) & (3~5)(1~2~4) \\ (1~2~4)(5~3) & (5~3)(1~2~4) \\ (4~1~2)(3~5) & (3~5)(4~1~2) \\ (4~1~2)(5~3) & (5~3)(4~1~2) \\ (2~4~1)(3~5) & (3~5)(2~4~1) \\ (2~4~1)(5~3) & (5~3)(2~4~1) \end{array}

All of these represent the same σ\sigma.

Example 5.8 Let

σ=(1 2)(3 4),τ=(1 2 3).\begin{aligned} \sigma&=(1~2)(3~4),\\ \tau&=(1~2~3). \end{aligned}

The inverse of a cycle is obtained by reading the cycle backwards:

τ1=(3 2 1),σ1=(2 1)(4 3)=σ.\begin{aligned} \tau^{-1}&=(3~2~1),\\ \sigma^{-1}&=(2~1)(4~3)=\sigma. \end{aligned}

We can compute

τστ1=(1 2 3)(1 2)(3 4)(3 2 1)=(1 4)(2 3),στσ1=(1 2)(3 4)(1 2 3)(1 2)(3 4)=(3)(4 2 1)=(4 2 1).\begin{aligned} \tau\sigma\tau^{-1} &= (1~2~3)\circ(1~2)(3~4)\circ(3~2~1)\\ &=(1~4)(2~3),\\ \sigma\tau\sigma^{-1} &= (1~2)(3~4)\circ(1~2~3)\circ(1~2)(3~4)\\ &=(3)(4~2~1)\\ &=(4~2~1). \end{aligned}

Notice that

(some element)σ(some element)1(\text{some element})\sigma(\text{some element})^{-1}

has the same cycle shape as σ\sigma. This will help us classify the conjugacy classes of SnS_n.

§ 5.4 Conjugacy Classes in SnS_n

Cycle notation gives us some beautiful results.

Proposition 5.3

(1) Suppose σSn\sigma\in S_n is a cycle, so

σ=(a1  ak),\sigma=(a_1~\cdots~a_k),

where

ai+1=σ(ai).a_{i+1}=\sigma(a_i).

Then

σ1=(ak  a1).\sigma^{-1} = (a_k~\cdots~a_1).

That is,

σ1=(b1  bk),\sigma^{-1} = (b_1~\cdots~b_k),

where bi=σ(bi+1)b_i=\sigma(b_{i+1}) and bk=a1b_k=a_1.

(2) More generally, if

σ=σ1σ2σk\sigma = \sigma_1\sigma_2\cdots\sigma_k

where the σi\sigma_i are disjoint cycles, then

σ1=σ11σk1.\sigma^{-1} = \sigma_1^{-1}\cdots\sigma_k^{-1}.

(3) Let σ,τSn\sigma,\tau\in S_n and a,bna,b\in\underline{n}. If

σ(a)=b,\sigma(a)=b,

then τστ1\tau\sigma\tau^{-1} maps τ(a)\tau(a) to τ(b)\tau(b).

Proof:

(1) We need to prove that for every bnb\in\underline{n},

(ak  a1)(a1  ak):bb(a_k~\cdots~a_1) \circ (a_1~\cdots~a_k): b\mapsto b

and

(a1  ak)(ak  a1):bb.(a_1~\cdots~a_k) \circ (a_k~\cdots~a_1): b\mapsto b.

We prove the first composition; the second is similar.

  • If ba1,,akb\notin{a_1,\ldots,a_k}, then bb is fixed by σ\sigma and therefore also fixed by (ak  a1)(a_k~\cdots~a_1). Hence
(ak  a1)σ(b)=b.(a_k~\cdots~a_1)\circ\sigma(b)=b.\textcolor{red}{\checkmark}
  • If ba1,,akb\in{a_1,\ldots,a_k}, then b=aib=a_i for some i1,,ki\in{1,\ldots,k}. Thus
σ(b)=ai+1\sigma(b)=a_{i+1}

by the definition of cycle notation. Hence (ak  a1)(a_k~\cdots~a_1) maps σ(b)\sigma(b) back to bb. \textcolor{red}{\checkmark}

(2) In general, if g1,,glGg_1,\ldots,g_l\in G, then

(g1gl)1=gl1g11.(g_1\cdots g_l)^{-1} = g_l^{-1}\cdots g_1^{-1}.

Indeed,

(g1gl)(gl1g11)=g1gl1glgl1cancelgl11g11=g1gl1gl11cancelg11=g1g11=1G.\begin{aligned} (g_1\cdots g_l)(g_l^{-1}\cdots g_1^{-1}) &= g_1\cdots g_{l-1} \underbrace{g_lg_l^{-1}}_{\text{cancel}} g_{l-1}^{-1}\cdots g_1^{-1}\\ &= g_1\cdots \underbrace{g_{l-1}g_{l-1}^{-1}}_{\text{cancel}} \cdots g_1^{-1}\\ &\quad\vdots\\ &=g_1g_1^{-1}\\ &=1_G. \end{aligned}

Therefore,

(σ1σl)1=σl1σ11.(\sigma_1\cdots\sigma_l)^{-1} = \sigma_l^{-1}\cdots\sigma_1^{-1}.

But disjoint cycles commute, so

σl1σ11=σ11σl1.\sigma_l^{-1}\cdots\sigma_1^{-1} = \sigma_1^{-1}\cdots\sigma_l^{-1}.

(3)

τστ1(τ(a))=τστ1τ(a)=τσ(a)=τ(b).\begin{aligned} \tau\sigma\tau^{-1}(\tau(a)) &= \tau\sigma\tau^{-1}\circ\tau(a)\\ &= \tau\sigma(a)\\ &= \tau(b). \end{aligned}
 ~\tag*{$\square$}

Remark Conjugation is analogous to a change of basis. If v1,,vkv_1,\ldots,v_k is a basis of Rk\mathbb{R}^k, then there exists an invertible matrix TT whose iith column is viv_i.

If a linear transformation AA sends a\vec a to b\vec b, then

TAT1TAT^{-1}

sends TaT\vec a to TbT\vec b.

Thus the permutation τ\tau above may be regarded as a kind of “new basis” for n\underline{n}.

Corollary 5.4 Let σ,σSn\sigma,\sigma'\in S_n. If there exists τSn\tau\in S_n such that

σ=τστ1,\sigma' = \tau\sigma\tau^{-1},

then we can construct a cycle notation for σ\sigma' from a cycle notation for σ\sigma and from τ\tau.

Proof: If σ\sigma is a cycle,

σ=(a1  al),\sigma=(a_1~\cdots~a_l),

then

τστ1=(τ(a1)  τ(al)).\tau\sigma\tau^{-1} = (\tau(a_1)~\cdots~\tau(a_l)).

Part (3) of the proposition tells us that τ(ai)\tau(a_i) is mapped by τστ1\tau\sigma\tau^{-1} to τ(ai+1)\tau(a_{i+1}).

It also tells us that if σ(a)=a\sigma(a)=a, then τστ1\tau\sigma\tau^{-1} fixes τ(a)\tau(a). Therefore, τστ1\tau\sigma\tau^{-1} is another cycle whose nontrivial orbit is given by τ(ai){\tau(a_i)}.

If σ\sigma is a product of disjoint cycles,

σ=σ1σl,\sigma = \sigma_1\cdots\sigma_l,

then

τστ1=(τσ1τ1)(τσ2τ1)(τσlτ1)\tau\sigma\tau^{-1} = (\tau\sigma_1\tau^{-1}) (\tau\sigma_2\tau^{-1}) \cdots (\tau\sigma_l\tau^{-1})

because conjugation is a group homomorphism.

Thus, if

σ=(a1  ak1)(ak1+1  ak1+k2)(ak1++kl1+1  ak1++kl)\sigma = (a_1~\cdots~a_{k_1}) (a_{k_1+1}~\cdots~a_{k_1+k_2}) \cdots (a_{k_1+\cdots+k_{l-1}+1} ~\cdots~ a_{k_1+\cdots+k_l})

is a cycle notation for σ\sigma, then

τστ1=(τ(a1)  τ(ak1))(τ(ak1+1)  τ(ak1+k2))(τ(ak1++kl1+1)  τ(ak1++kl))\tau\sigma\tau^{-1} = (\tau(a_1)~\cdots~\tau(a_{k_1})) (\tau(a_{k_1+1})~\cdots~\tau(a_{k_1+k_2})) \cdots (\tau(a_{k_1+\cdots+k_{l-1}+1}) ~\cdots~ \tau(a_{k_1+\cdots+k_l}))

is a cycle notation for τστ1\tau\sigma\tau^{-1}.

 ~\tag*{$\square$}

Let σSn\sigma\in S_n.

Write σ\sigma as a product of disjoint cycles

σ=σ1σk\sigma = \sigma_1\cdots\sigma_k

and consider

σi,i.|\sigma_i|, \qquad \forall i.

These are the sizes of the orbits associated with the cycles σi\sigma_i. In this way we obtain a collection of numbers. Since the σi\sigma_i can be reordered, it is most convenient to regard this collection as unordered.

Example 5.9 Let

σ=(1 2 3)(6 9)S9.\sigma = (1~2~3)(6~9)\in S_9.

Notice that, for brevity, we do not write (8)(8). Then the numbers associated with σ\sigma are

3, 2, 3.3,\ 2,\ 3.

Definition 5.7 We call these numbers ai{a_i} the cycle shape of σ\sigma.

Example 5.10 Let

σ=(3 4 5)(8 7 9)(2 6).\sigma' = (3~4~5)(8~7~9)(2~6).

Then σ\sigma' has the associated numbers

3, 3, 2.3,\ 3,\ 2.

Up to order, this is the same collection as the one associated with σ\sigma. We say that σ\sigma and σ\sigma' have the same cycle shape.

Proposition 5.5 Two elements σ,σSn\sigma,\sigma'\in S_n are conjugate, meaning that there exists τ\tau such that

σ=τστ1,\sigma = \tau\sigma'\tau^{-1},

if and only if they have the same cycle shape.

Proof: Suppose σ\sigma and σ\sigma' have the same cycle shape. Then we may reorder any cycle notations for σ\sigma and σ\sigma' so that

σ=σ1σk,σ=σ1σkare both products of disjoint cycles,\begin{aligned} \sigma &= \sigma_1\circ\cdots\circ\sigma_k,\\ \sigma' &= \sigma_1'\circ\cdots\circ\sigma_k' \end{aligned} \quad \text{are both products of disjoint cycles,}

with

σi=σi|\sigma_i| = |\sigma_i'|

for every ii.

Choose any ii and a number aa appearing in the cycle notation of σi\sigma_i:

σi=( a ).\sigma_i = (\cdots~a~\cdots).

Choose any number aa' appearing in σi\sigma_i':

σi=( a ).\sigma_i' = (\cdots~a'~\cdots).

Define a bijection by

τ:aibi,σj(ai)(σ)j(bi).\begin{aligned} \tau:a_i&\mapsto b_i,\\ \sigma^j(a_i) &\mapsto (\sigma')^j(b_i). \end{aligned}

Then

τστ1(b)=τστ1((σ)j(bi))=τσ(σj(ai))=τ(σj+1(ai))=(σ)j+1(bi)=σ(b).\begin{aligned} \tau\sigma\tau^{-1}(b) &= \tau\sigma\tau^{-1} ((\sigma')^j(b_i))\\ &= \tau\sigma(\sigma^j(a_i))\\ &= \tau(\sigma^{j+1}(a_i))\\ &= (\sigma')^{j+1}(b_i)\\ &= \sigma'(b). \end{aligned}

Hence

τστ1=σ.\tau\sigma\tau^{-1} = \sigma'.

The converse follows from the corollary above.

 ~\tag*{$\square$}

Example 5.11

(1 2 3)(6 9)=σ,(4 5)(3 6 1)=σS9\begin{aligned} (1~2~3)(6~9)&=\sigma,\\ (4~5)(3~6~1)&=\sigma' \end{aligned} \in S_9

have the same cycle shape.

Likewise,

σ=(1 2)(3 4)(5 6 7),σ=(7 8)(5 9)(1 4 2)S9.\begin{aligned} \sigma &= (1~2)(3~4)(5~6~7),\\ \sigma' &= (7~8)(5~9)(1~4~2) \end{aligned} \in S_9.

Remark The cycle shape of σ\sigma simply says that the action of σ\sigma divides n\underline{n} into ll orbits, with the iith orbit having size kik_i.

If σ\sigma' also divides n\underline{n} into ll orbits, and its orbit sizes kik_i' can be matched with the kik_i of σ\sigma, then σ\sigma and σ\sigma' have the same cycle shape.

Example 5.12 How do we find τ\tau?

Let

σ=(1 2 3)(4 6)(7 8 5),σ=(1 5 7)(9 3)(6 8 4).\begin{aligned} \sigma &= (1~2~3)(4~6)(7~8~5),\\ \sigma' &= (1~5~7)(9~3)(6~8~4). \end{aligned}

If

τστ1=σ,\tau\sigma\tau^{-1} = \sigma',

then we know that a cycle

(b1  bk)(b_1~\cdots~b_k)

in the cycle notation of σ\sigma' must be equal to

(τ(a1)  τ(ak))(\tau(a_1)~\cdots~\tau(a_k))

for some cycle (a1  ak)(a_1~\cdots~a_k) in the cycle decomposition of σ\sigma.

This is not unique, but here is one way to find such a τ\tau.

Choose a cycle and an element appearing in it. Arbitrarily, choose

4(4 6).4\in(4~6).

In the cycle notation of σ\sigma', choose a cycle of the same length as (4 6)(4~6). In this case the only possible choice is (9 3)(9~3), although in general there may be several choices.

Choose an element appearing in that cycle, say 99.

So write

Next, look at how the cycle σi\sigma_i acts on 99. In this case, it does not: 99 is a fixed point of σ\sigma.

So choose any fixed point of σ\sigma'. Here our only choice is 22.

Now find the cycle σi\sigma_i containing 22. In the corresponding cycle σi\sigma_i', find the matching element. In this case the corresponding element is 55.

So the fourth step gives

5\textcircled{\small 5} After seeing that (4925)(4925) is a cycle of τ\tau, choose any element that has not yet been written. Arbitrarily choose 11.

6\textcircled{\small 6} Likewise, choose 33.

We do not write cycles of length 11.

§ 5.5 The Alternating Group

Definition 5.8 The alternating group AnA_n is defined as the kernel of the map

SnGLn(R)detR×σBσ\begin{aligned} S_n &\to GL_n(\mathbb{R}) \xrightarrow{\det} \mathbb{R}^{\times}\\ \sigma &\mapsto B_\sigma \end{aligned}

where

Bσ(ei)=eσ(i).B_\sigma(e_i)=e_{\sigma(i)}.

That is, AnA_n is the set of all σ\sigma such that

detBσ=1.\det B_\sigma=1.

Proposition 5.6 AnA_n is a subgroup of SnS_n consisting of all even permutations, i.e. permutations that can be written as a product of an even number of transpositions, where a transposition exchanges two elements.

Therefore,

An=n!2.|A_n| = \dfrac{n!}{2}.

Proposition 5.7 AnA_n is a normal subgroup of SnS_n.

There are three ways to prove this.

1. Kernel of the Sign Homomorphism

Proof: Define a map

sgn:Sn{1,1}\mathrm{sgn}:S_n\to\{1,-1\}

by

  • if σ\sigma is an even permutation,
sgn(σ)=1;\mathrm{sgn}(\sigma)=1;
  • if σ\sigma is an odd permutation,
sgn(σ)=1.\mathrm{sgn}(\sigma)=-1.

This is a group homomorphism because

sgn(στ)=sgn(σ)sgn(τ).\mathrm{sgn}(\sigma\tau) = \mathrm{sgn}(\sigma)\cdot\mathrm{sgn}(\tau).

We call this the sign homomorphism.

The kernel of a homomorphism is the set of elements that map to the identity element of the codomain. For sgn\mathrm{sgn}, the identity element is 11. Therefore,

ker(sgn)=An.\ker(\mathrm{sgn})=A_n.

The kernel of a group homomorphism is always a normal subgroup of the domain group. Therefore,

AnSn.A_n\triangleleft S_n.
 ~\tag*{$\square$}

2. Conjugation Preserves the Parity of a Permutation

Proof: For any σ,τSn\sigma,\tau\in S_n, conjugation preserves the cycle structure and the parity of a permutation.

If σ\sigma is even, then its conjugate

τστ1\tau\sigma\tau^{-1}

is also even.

A subgroup NN is normal if it is invariant under conjugation by elements of the group:

τNτ1=Nfor all τSn.\tau N\tau^{-1} = N \quad \text{for all }\tau\in S_n.

Since the conjugate of an even permutation is again even,

AnSn.A_n\triangleleft S_n.
 ~\tag*{$\square$}

3. The Index of AnA_n in SnS_n

Proof: The index of AnA_n in SnS_n is

[Sn:An]=SnAn=n!n!/2=2.[S_n:A_n] = \dfrac{|S_n|}{|A_n|} = \dfrac{n!}{n!/2} = 2.

Since every subgroup of index 22 in a group is normal,

AnSn.A_n\triangleleft S_n.
 ~\tag*{$\square$}