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Cayley's theorem

Representation of groups by permutations

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Through Group (mathematics), Permutation and Bijection

  • for each g∈G, the left-multiplication-by-g map ℓg:G→G sending each element x to gx is a permutation of G, and
  • the map G→Sym⁡(G) sending each element g to ℓg is an injective homomorphism, so it defines an isomorphism from G onto a subgroup of Sym⁡(G).

The homomorphism G→Sym⁡(G) can also be understood as arising from the left translation action of G on the underlying set G.

When G is finite, 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 Sn. But G might also be isomorphic to a subgroup of a smaller symmetric group, Sm for some m<n; for instance, the order 6 group G=S3 is not only isomorphic to a subgroup of S6, but also (trivially) isomorphic to a subgroup of S3. 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, 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.

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