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6.2: Symmetric Groups

  • Page ID
    84821
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    Definition: Symmetric Group

    When \(A=\{1,2,\ldots, n\}\) (\(n\in \mathbb{Z}^+\)), we call \(S_A\) the symmetric group on \(n\) letters and denote it by \(S_n\text{.}\)

    (We can, in fact, define \(S_0\text{,}\) the set of all permutations on the empty set. One can show, using the fact that a function is a relation on a Cartesian product of sets, that \(S_0\) is the trivial group. However, this will not be relevant in this text.)

    Remark

    Throughout this course, if we are discussing a group \(S_n\text{,}\) you should assume \(n\in \mathbb{Z}^+\text{.}\)

    It is important for us to be able to easily describe specific elements of \(S_n\text{.}\) It would be cumbersome to describe, for instance, an element of \(S_3\) by saying it swaps \(1\) and \(2\) and fixes \(3\text{;}\) imagine how much more cumbersome it could be to describe an element of, say, \(S_{100}\text{!}\) One can somewhat concisely describe a permutation \(\sigma\) of \(S_n\) by listing out the elements \(1,2,\ldots,n\) and writing the element \(\sigma(i)\) below each \(i\) for \(i=1,2,\ldots, n\text{.}\) For instance, if \(\sigma\) sends \(1\) to \(2\text{,}\) we'd write the number \(2\) below the number \(1\text{.}\) The convention is to enclose these two rows of numbers in a single set of parentheses, as in the following example.

    Example \(\PageIndex{1}\)

    We can denote the element \(\sigma\) of \(S_3\) that swaps \(1\) and \(2\) and fixes \(3\) by

    \begin{equation*} \sigma = \begin{pmatrix}1& 2& 3\\ 2& 1& 3 \end{pmatrix}, \end{equation*}

    and the element \(\tau\) of \(S_3\) that sends \(1\) to \(3\text{,}\) \(2\) to \(1\text{,}\) and \(3\) to \(2\) by

    \begin{equation*} \tau =\begin{pmatrix}1& 2&3\\ 3& 1& 2 \end{pmatrix}. \end{equation*}

    Then

    \begin{equation*} \sigma\tau = \begin{pmatrix}1& 2& 3\\ 3& 2&1 \end{pmatrix} \end{equation*}

    and

    \begin{equation*} \tau\sigma = \begin{pmatrix}1& 2& 3\\ 1& 3& 2 \end{pmatrix}. \end{equation*}

     

    But even this notation is unnecessarily cumbersome. Instead, we use cycle notation.

    Definition: Cycle, Cycle Notation, and Transposition

    A permutation \(\sigma\) in \(S_n\) is called a \(k\)-cycle or a cycle of length \(k\) (or, less specifically, a cycle) if there exist distinct elements \(a_1, a_2,\ldots, a_k\) in \(\{1,2,\ldots,n\}\) such that

    • \(\sigma(a_i)=a_{i+1}\) for each \(i=1,2,\ldots, k-1\text{;}\)

    • \(\sigma(a_k)=a_1\text{;}\)

    • \(\sigma(x)=x\) for every other element of \(\{1,2,\ldots, n\}\text{.}\)

    We use the cycle notation \(\sigma = (a_1 a_2 \cdots a_k)\) to describe such a cycle. A \(2\)-cycle is often called a transposition.

    Example \(\PageIndex{2}\)

    The permutation \(\tau\) in \(S_3\) that sends \(1\) to \(3\text{,}\) \(2\) to \(1\text{,}\) and \(3\) to \(2\) is a cycle. It can be denoted by \(\tau =(132)\text{.}\) Similarly, the cycle \(\rho\) in \(S_3\) swapping \(1\) and \(3\) can be denoted by \(\rho=(13)\text{.}\) On the other hand, the permutation in \(S_4\) that swaps \(1\) with \(2\) and \(3\) with \(4\) is not a cycle.

    Remark

    Given a \(k\)-cycle \(\sigma=(a_1 a_2\cdots a_k)\text{,}\) there are \(k\) different expressions for \(\sigma\text{.}\) Indeed, we have

    \begin{equation*} \sigma=(a_1 a_2\cdots a_k)=(a_2 a_3 \cdots a_k a_1)=(a_3 a_4 \cdots a_k a_1 a_2)=\cdots = (a_k a_1 \cdots a_{k-1}). \end{equation*}

    Example \(\PageIndex{3}\)

    The permutation \(\tau\) described in Example \(6.2.2\) can also be written as \((321)\) and as \((213)\text{.}\)

    However, by convention, we usually “start” a cycle \(\sigma\) with the smallest of the numbers that \(\sigma\) doesn't fix: e.g., we'd write \(\sigma=(213)\) as \((132)\text{.}\)

    Definition: Disjoint and Mutual Disjointness

    Two cycles \(\sigma=(a_1 a_2 \cdots a_k)\) and \(\tau=(b_1 b_2 \cdots b_m)\) are said to be disjoint if \(a_i \neq b_j\) for all \(i\) and \(j\text{.}\) Cycles \(\sigma_1\text{,}\) \(\sigma_2\text{,}\) \(\ldots\text{,}\) \(\sigma_m\) are disjoint if \(\sigma_i\) and \(\sigma_j\) are disjoint for each \(i \neq j\text{.}\) (Notice: this version of disjointness is what we usually refer to as mutual disjointness.)

    Remark

    Note that if cycles \(\sigma\) and \(\tau\) are disjoint, then \(\sigma\) and \(\tau\) commute; that is, \(\sigma \tau=\tau \sigma\text{.}\)

    Note

    If cycles \(\sigma\) and \(\tau\) are not disjoint then they may not commute. For instance, see Example 6.2.3, where \(\sigma\tau \neq \tau \sigma\text{.}\)

    Note that any permutation of \(S_n\) is a product of disjoint cycles (where by “product” we mean the permutation resulting from permutation multiplication).

    Definition: (Disjoint) Cycle Notation

    Writing a permutation in (disjoint) cycle notation means writing it as a product of disjoint cycles, where each cycle is written in cycle notation.

    Remark

    Note that if \(\sigma\) in \(S_n\) is written in cycle notation and the number \(a\in \{1,2,\ldots, n\}\) appears nowhere in \(\sigma\)'s representation, this means that \(\sigma\) fixes \(a\text{.}\) The only permutation that we cannot really write in cycle notation is the identity element of \(S_n\text{,}\) which we henceforth denote by \(e\text{.}\)

    Example \(\PageIndex{4}\)

    The permutation

    \begin{equation*} \sigma =\begin{pmatrix}1& 2& 3& 4& 5& 6\\ 3& 1& 2&6& 5& 4 \end{pmatrix} \end{equation*}

     

    is the product of disjoint cycles \((132)\) and \((46)\text{,}\) so in cycle notation we have

    \begin{equation*} \sigma=(132)(46). \end{equation*}

    Note that we could also write \(\sigma\) as \((321)(46)\text{,}\) \((213)(64)\text{,}\) \((64)(132)\text{,}\) etc.

    While it is true that we also have \(\sigma=(13)(23)(46)\text{,}\) this is not a disjoint cycle representation of \(\sigma\) since both \((13)\) and \((23)\) “move” the element \(3\text{.}\)

    Example \(\PageIndex{5}\)

    In \(S_4\text{,}\) let \(\sigma=(243)\) and \(\tau=(13)(24)\text{.}\) Then \(\sigma \tau=(123)\) and \(\tau \sigma = (134).\)

    Example \(\PageIndex{6}\)

    In \(S_9\text{,}\) let \(\sigma=(134)\text{,}\) \(\tau=(26)(17)\text{,}\) and \(\rho=(358)(12)\text{.}\) Find the following, writing your answers using disjoint cycle notation.

    1. \(\sigma^{-1}\)
    2. \(\sigma^{-1}\tau\sigma\)
    3. \(\sigma^2\)
    4. \(\sigma^3\)
    5. \(\rho^2\)
    6. \(\rho^{-2}\)
    7. \(\sigma \tau\)
    8. \(\sigma \rho\)

    Example \(\PageIndex{7}\)

    Explicitly express all the elements of \(S_4\) in disjoint cycle notation.

    Theorem \(\PageIndex{1}\)

    Any \(k\)-cycle has order \(k\) in \(S_n\text{.}\) More generally, if permutation \(\sigma\) can be written in disjoint cycle notation as \(\sigma=\sigma_1 \sigma_2 \cdots \sigma_m\text{,}\) then

    \begin{align*} o(\sigma)& =\text{lcm}(o(\sigma_1), o(\sigma_2),\ldots, o(\sigma_m))\\ & =\text{lcm}(\mathrm{length}(\sigma_1),\mathrm{length}(\sigma_2),\ldots,\mathrm{length}(\sigma_m)), \end{align*}

    where \(\text{lcm}\) denotes the least common multiple.

    Example \(\PageIndex{8}\)

    1. Find the orders of each of the elements in Example \(6.2.6\), including \(\sigma\text{,}\) \(\tau\text{,}\) and \(\rho\) themselves.

    2. Explicitly list the elements of \(\langle \sigma\rangle\text{,}\) \(\langle \tau\rangle\text{,}\) and \(\langle \rho\rangle\text{.}\) 


    This page titled 6.2: Symmetric Groups is shared under a GNU Free Documentation License 1.3 license and was authored, remixed, and/or curated by Jessica K. Sklar via source content that was edited to the style and standards of the LibreTexts platform; a detailed edit history is available upon request.