In group theory, Cayley's theorem, named in honour of Arthur Cayley, states that every group is isomorphic to a subgroup of a symmetric group. More specifically, is isomorphic to a subgroup of the symmetric group
\operatorname{Sym}(G)
g\inG
\ellg\colonG\toG
G\to\operatorname{Sym}(G)
\ellg
\operatorname{Sym}(G)
G\to\operatorname{Sym}(G)
When is finite,
\operatorname{Sym}(G)
Sn
Sm
m<n
G=S3
S6
S3
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".[4]
When is infinite,
\operatorname{Sym}(G)
While it seems elementary enough, at the time the modern definitions did not exist, and when Cayley introduced what are now called groups it was not immediately clear that this was equivalent to the previously known 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, in his original 1854 paper, showed that the correspondence in the theorem is one-to-one, but he failed to 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[5] and is attributed to Dyck in the first edition of Burnside's book.
A permutation of a set is a bijective function from to . The set of all permutations of forms a group under function composition, called the symmetric group on, and written as
\operatorname{Sym}(A)
\operatorname{Sym}(G)
If g is any element of a group G with operation ∗, consider the function, defined by . By the existence of inverses, this function has also an inverse,
f | |
g-1 |
The set is a subgroup of Sym(G) that is isomorphic to G. The fastest way to establish this is to consider the function with for every g in G. T is a group homomorphism because (using · to denote composition in Sym(G)):
(fg ⋅ fh)(x)=fg(fh(x))=fg(h*x)=g*(h*x)=(g*h)*x=fg*h(x),
T(g) ⋅ T(h)=fg ⋅ fh=fg*h=T(g*h).
Thus G is isomorphic to the image of T, which is the subgroup K.
T is sometimes called the regular representation of G.
An alternative setting uses the language of group actions. We consider the group
G
g ⋅ x=gx
\phi:G\toSym(G)
The representation is faithful if
\phi
\phi
g\in\ker\phi
g=ge=g ⋅ e=e
\ker\phi
Im\phi\congG
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.
Z2=\{0,1\}
Z3=\{0,1,2\}
Z4=\{0,1,2,3\}
The elements of Klein four-group 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 | e | a | b | c | d | f | e | |
a | a | e | d | f | b | c | (12)(35)(46) | |
b | b | f | e | d | c | a | (13)(26)(45) | |
c | c | d | f | e | a | b | (14)(25)(36) | |
d | d | c | a | b | f | e | (156)(243) | |
f | f | b | c | a | e | d | (165)(234) |
Theorem: Let be a group, and let be a subgroup.Let
G/H
G/N
\operatorname{Sym}(G/H)
The special case
H=1