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Cayley's theorem
Representation of groups by permutations
Representation of groups by permutations
In the mathematical discipline of group theory, Cayley's theorem, named in honour of Arthur Cayley, states that every group G is isomorphic to a subgroup of a symmetric group. More specifically, G is isomorphic to a subgroup of the symmetric group \operatorname{Sym}(G) whose elements are the permutations of the underlying set of G. Explicitly,
- for each g \in G, the left-multiplication-by-g map \ell_g \colon G \to G sending each element x to gx is a permutation of G, and
- the map G \to \operatorname{Sym}(G) sending each element g to \ell_g is an injective homomorphism, so it defines an isomorphism from G onto a subgroup of \operatorname{Sym}(G). The homomorphism G \to \operatorname{Sym}(G) can also be understood as arising from the left translation action of G on the underlying set G.
When G is finite, \operatorname{Sym}(G) is finite too. The proof of Cayley's theorem in this case shows that if G is a finite group of order n, then G is isomorphic to a subgroup of the standard symmetric group S_n. But G might also be isomorphic to a subgroup of a smaller symmetric group, S_m for some m; for instance, the order 6 group G=S_3 is not only isomorphic to a subgroup of S_6, but also (trivially) isomorphic to a subgroup of S_3. The problem of finding the minimal-order symmetric group into which a given group G embeds is rather difficult.
Alperin and Bell note that "in general the fact that finite groups are imbedded in symmetric groups has not influenced the methods used to study finite groups".
When G is infinite, \operatorname{Sym}(G) is infinite, but Cayley's theorem still applies.
History
When Cayley (1854) introduced what are now called groups, the modern definitions did not exist, and it was not immediately clear that this was equivalent to what were then called groups, which are now called permutation groups. Cayley's theorem unifies the two.
Although Burnside attributes the theorem to Jordan, Eric Nummela nonetheless argues that the standard name—"Cayley's Theorem"—is in fact appropriate. Cayley's original 1854 paper, showed that the correspondence in the theorem is one-to-one, but he did not explicitly show it was a homomorphism (and thus an embedding). However, Nummela notes that Cayley made this result known to the mathematical community at the time, thus predating Jordan by 16 years or so.
The theorem was later published by Walther Dyck in 1882 and is attributed to Dyck in the first edition of Burnside's book.
Background
A permutation of a set A is a bijective function from A to A. The set of all permutations of A forms a group under function composition, called the symmetric group on A, and written as \operatorname{Sym}(A). In particular, taking A to be the underlying set of a group G produces a symmetric group denoted \operatorname{Sym}(G).
Proof of the theorem
If g is any element of a group G with operation ∗, consider the function f**g : G → G, defined by . By the existence of inverses, this function has also an inverse, f_{g^{-1}}. So multiplication by g acts as a bijective function. Thus, f**g is a permutation of G, and so is a member of Sym(G).
The set is a subgroup of Sym(G) that is isomorphic to G. The fastest way to establish this is to consider the function T : G → Sym(G) with for every g in G. T is a group homomorphism because (using · to denote composition in Sym(G)):
: (f_g \cdot f_h)(x) = f_g(f_h(x)) = f_g(hx) = g(hx) = (gh)x = f_{gh}(x) , for all x in G, and hence: : T(g) \cdot T(h) = f_g \cdot f_h = f_{gh} = T(gh) . The homomorphism T is injective since (the identity element of Sym(G)) implies that for all x in G, and taking x to be the identity element e of G yields , i.e. the kernel is trivial. Alternatively, T is also injective since implies that (because every group is cancellative).
Thus G is isomorphic to the image of T, which is the subgroup K.
T is sometimes called the regular representation of G.
Alternative setting of proof
An alternative setting uses the language of group actions. We consider the group G as acting on itself by left multiplication, i.e. g \cdot x = gx, which has a permutation representation, say \phi : G \to \mathrm{Sym}(G).
The representation is faithful if \phi is injective, that is, if the kernel of \phi is trivial. Suppose g\in\ker\phi. Then, g = ge = g\cdot e = e. Thus, \ker\phi is trivial. The result follows by use of the first isomorphism theorem, from which we get \mathrm{Im}, \phi \cong G.
Remarks on the regular group representation
The identity element of the group corresponds to the identity permutation. All other group elements correspond to derangements: permutations that do not leave any element unchanged. Since this also applies for powers of a group element, lower than the order of that element, each element corresponds to a permutation that consists of cycles all of the same length: this length is the order of that element. The elements in each cycle form a right coset of the subgroup generated by the element.
Examples of the regular group representation
\mathbb Z_2 = {0,1} with addition modulo 2; group element 0 corresponds to the identity permutation e, group element 1 to permutation (12) (see cycle notation). E.g. 0 +1 = 1 and 1+1 = 0, so 1\mapsto0 and 0\mapsto1, as they would under a permutation.
\mathbb Z_3 = {0,1,2} with addition modulo 3; group element 0 corresponds to the identity permutation e, group element 1 to permutation (123), and group element 2 to permutation (132). E.g. 1 + 1 = 2 corresponds to (123)(123) = (132).
\mathbb Z_4 = {0,1,2,3} with addition modulo 4; the elements correspond to e, (1234), (13)(24), (1432).
The elements of Klein four-group {e, a, b, c} correspond to e, (12)(34), (13)(24), and (14)(23).
S3 (dihedral group of order 6) is the group of all permutations of 3 objects, but also a permutation group of the 6 group elements, and the latter is how it is realized by its regular representation.
| * | e | a | b | c | d | f | permutation | e | a | b | c | d | f |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| e | a | b | c | d | f | e | |||||||
| a | e | d | f | b | c | (12)(35)(46) | |||||||
| b | f | e | d | c | a | (13)(26)(45) | |||||||
| c | d | f | e | a | b | (14)(25)(36) | |||||||
| d | c | a | b | f | e | (156)(243) | |||||||
| f | b | c | a | e | d | (165)(234) |
More general statement
Theorem: Let G be a group, and let H be a subgroup. Let G/H be the set of left cosets of H in G. Let N be the normal core of H in G, defined to be the intersection of the conjugates of H in G. Then the quotient group G/N is isomorphic to a subgroup of \operatorname{Sym}(G/H).
The special case H=1 is Cayley's original theorem.
Notes
References
- .
References
- {{harvtxt. Jacobson. 2009
- {{harvtxt. Jacobson. 2009
- Peter J. Cameron. (2008). "Introduction to Algebra, Second Edition". Oxford University Press.
- (1971). "Minimal Permutation Representations of Finite Groups". American Journal of Mathematics.
- (2003). "On Minimal Permutation Representations of Classical Simple Groups". Siberian Mathematical Journal.
- (1995). "Groups and representations". Springer.
- Burnside, William. (1911). "Theory of Groups of Finite Order".
- Jordan, Camille. (1870). "Traite des substitutions et des equations algebriques". Gauther-Villars.
- Nummela, Eric. (1980). "Cayley's Theorem for Topological Groups". Mathematical Association of America.
- Cayley, Arthur. (1854). "On the theory of groups as depending on the symbolic equation θn=1". Philosophical Magazine.
- von Dyck, Walther. (1882). "Gruppentheoretische Studien". [[Mathematische Annalen]].
- Burnside, William. (1897). "Theory of Groups of Finite Order".
- {{harvtxt. Jacobson. 2009
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