What Are Symmetric Groups and Their Mathematical Significance?

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SUMMARY

The symmetric group S(n), also known as Sym(n), encompasses all permutations of n symbols and has an order of n!. Its index-2 subgroup, the alternating group A(n) or Alt(n), consists of even permutations and has an order of n!/2, being simple for n ≥ 5. The representation theory of S(n) reveals elegant structures, with irreducible representations (irreps) categorized by cycle lengths. Notably, every finite group can be represented as a subgroup of a symmetric group, highlighting the foundational significance of symmetric groups in group theory.

PREREQUISITES
  • Understanding of group theory concepts, specifically symmetric and alternating groups.
  • Familiarity with permutations and cyclic permutations.
  • Knowledge of representation theory and irreducible representations.
  • Basic understanding of conjugacy classes and their properties.
NEXT STEPS
  • Explore the properties of symmetric groups in detail, focusing on S(n) and A(n).
  • Study the representation theory of groups, particularly the character tables of symmetric and alternating groups.
  • Investigate the implications of duality in the context of irreducible representations.
  • Learn about the applications of symmetric groups in various fields of mathematics, including combinatorics and algebra.
USEFUL FOR

Mathematicians, particularly those specializing in group theory, algebraists, and students seeking to deepen their understanding of symmetric and alternating groups.

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Definition/Summary

The symmetric group S(n) or Sym(n) is the group of all possible permutations of n symbols. It has order n!.

It has an index-2 subgroup, the alternating group A(n) or Alt(n), the group of all possible even permutations of n symbols. That group has order n!/2. For n >= 5, the alternating group is simple.

Equations



Extended explanation

First, some details about permutations. Every finite-length permutation can be broken up into cyclic permutations, where a cyclic permutation has the form
a1 -> a2, a2 -> a3, a3 -> a4, ..., a(n) -> a1

where n is the length of the cycle.

The conjugacy classes of S(n) are all elements that share some set of lengths of cycles. For S(3), the elements are 123 -> 123, 132, 213, 231, 312, 321. Its conjugacy classes are
13: {123}
1*2: {132, 213, 321}
3: {231, 312}

The elements of A(n) are all even permutations, those with an even number of even-length cycles. Thus, A(3) has elements 123, 231, 312. Some of the S(n) conjugacy classes get split in two, those with all odd cycle lengths that do not get repeated. Thus, the 3 splits into {231} and {312}.

The remaining coset of A(n) in S(n) is the odd permutations, those with an odd number of even-length cycles. The group (even permutations, odd permutations) is, of course, Z(2).

The representation theory of the symmetric group is very elegant, with the irreducible representations or irreps being labeled with sets of cycle lengths, just like the classes. The character values are all integers.

Going from a symmetric group to its alternating group, the irreps with length sets that are dual to each other get merged, while the irreps with self-dual length sets get split. Duality of the length sets is defined as follows:

Order the lengths from largest to smallest, then make (length) boxes for each one in a 2D pattern. Find out how many boxes there are in the other direction, and that gives the dual. Example:

The length set 3,2,1,1 gives
***
**
*
*
Its dual is 4,2,1

For even permutations, duality leaves the character value's sign unchanged, while for odd permutations, duality reverses the sign. In the self-dual case, odd permutations get zero character.

The irrep (n) for S(n) is the identity irrep, while the irrep (1n) is the parity irrep; it is 1 for even permutations and -1 for odd permutations.

For S(3), the 13 and 3 irreps are a dual set, while the 1*2 irrep is self-dual. Its character table is
\begin{matrix} & 3 & 1 \cdot 2 & 1^3 \\ 1^3 & 1 & 2 & 1 \\ 1 \cdot 2 & 1 & 0 & -1 \\ 3 & 1 & -1 & 1 \end{matrix}
Rows: classes, columns: irreps

For A(3), we get the character table
\begin{matrix} &amp; (3,1^3) &amp; (1 \cdot 2)_1 &amp; (1 \cdot 2)_2 \\<br /> 1^3 &amp; 1 &amp; 1 &amp; 1 \\ 3_1 &amp; 1 &amp; \frac12(-1 + \sqrt{-3}) &amp; \frac12(-1 - \sqrt{-3}) \\ 3_2 &amp; 1 &amp; \frac12(-1 - \sqrt{-3}) &amp; \frac12(-1 + \sqrt{-3}) \end{matrix}
The sqrt(-3) is typical of splitting.

* This entry is from our old Library feature. If you know who wrote it, please let us know so we can attribute a writer. Thanks!
 
Physics news on Phys.org
The importance of symmetric groups lies in the fact, that every finite group can be considered a subgroup of a symmetric group: Given a finite group ##G=\{\,a_1,\ldots,a_n\,\}## then the functions ##L_i\, : \,a_j \longmapsto a_ia_j## are permutations of ##\{\,1,\ldots,n\,\}##.
 

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