Subgroup

Given a group G under an operation *, we say that some subset H of G is a subgroup if H is a group under the restriction of * thereto. (The same definition applies more generally when G is an arbitrary semigroup, but this article will only deal with subgroups of groups.)

It is easily shown that H is a subgroup of the group G if and only if it is nonempty and closed to products and inverses. Furthermore, H's identity element is equal to G's identity element, and the inverse of an element of H is the same as the inverse of that element in G.

The subgroups of any given group form a complete lattice under inclusion. There is a minimal subgroup, the trivial group {e} (e being Gs identity element), and a maximal subgroup, the group G itself.

If S is a subset of G, then there exists a minimal subgroup containing S; it is denoted by <S> and is said to be generated by S. The elements of <S> are all finite products of elements of S and their inverses. Groups generated by a single element are called cyclic and are isomorphic to either (Z, +), where Z denotes the integers, or to (Zn, +), where Zn denotes the integers modulo n for some positive integer n (see modular arithmetic).

Order of an element of a group: Given an element x of G, the order of the cyclic subgroup <x> is called the order of x; it is the smallest positive integer n such that xn = e.

Given a subgroup H and some g in G, we define the left coset g*H = {g*h : h in H}. Because g is invertible, the set g*H has just as many elements as H. Furthermore, every element of G is contained in precisely one left coset of H; the left cosets are the equivalence classes corresponding to the equivalence relation g1 ~ g2 iff g1-1 * g2 is in H. The number of left cosets of H is called the index of H in G and is denoted by [G : H]. Lagrange's theorem states that

[G : H] |H| = |G|
where |G| and |H| denote the cardinalities of G and H, respectively. In particular, if G is finite, then the cardinality of every subgroup of G (and the order of every element of G) must be a divisor of |G|.

Right cosets are defined analogously: H*g = {h*g : h in H}. They are also the equivalence classes for a suitable equivalence relation and their number is equal to [G : H]. If g*H = H*g for every g in G, then H is said to be a normal subgroup. In that case we can define a multiplication on cosets by

   (g1*H)*(g2*H) := (g1*g2)*H

This turns the set of cosets in a group called the quotient group G/H. There is a natural homomorphism f : G -> G/H given by f(g)=g*H. The image f(H) consists only of the identity element of G/H, the coset e*H.

In general, a group homomorphism f: G -> K sends subgroups of G to subgroups of K. Also, the preimage of any subgroup of K is a subgroup of G. We call the preimage of the trivial group {e} in K the kernel of the homomorphism and denote it by ker(f). As it turns out, the kernel is always normal and the image f(G) of G is always isomorphic to G/ker(f).

The normal subgroups of any group G form a lattice under inclusion. The minimal and maximal elements are {e} and G, the greatest lower bound of two subgroup is their intersection and their least upper bound is a product group[?].

Common misspelling and questions (FAQ)

ubgroup  sbgroup  sugroup  subroup  subgoup  subgrup  subgrop  subgrou  usbgroup  sbugroup  sugbroup  subrgoup  subgorup  subgruop  subgropu  subgrou  ssubgroup  suubgroup  subbgroup  subggroup  subgrroup  subgrooup  subgrouup  subgroupp  wubgroup  aubgroup  zubgroup  eubgroup  xubgroup  eubgroup  dubgroup  xubgroup  s7bgroup  sybgroup  shbgroup  s8bgroup  sjbgroup  s8bgroup  sibgroup  sjbgroup  suggroup  suvgroup  suhgroup  suhgroup  sungroup  subtroup  subfroup  subvroup  subyroup  subbroup  subyroup  subhroup  subbroup  subg4oup  subgeoup  subgdoup  subg5oup  subgfoup  subg5oup  subgtoup  subgfoup  subgr9up  subgriup  subgrkup  subgr0up  subgrlup  subgr0up  subgrpup  subgrlup  subgro7p  subgroyp  subgrohp  subgro8p  subgrojp  subgro8p  subgroip  subgrojp  subgrou0  subgrouo  subgroul  subgrou-  subgrou;  subgrou-  subgrou[  subgrou;  subgroups 


au-dehors. Quelques gens timores s'effrayaient un peu a l'idee d'un demandait quel canon pourrait jamais transmettre une vitesse initiale seance du Comite devait repondre victorieusement a ces questions. Le lendemain soir, les quatre membres du Gun-Club s'attablaient devant de the. La discussion reprit aussitot son cours, et, cette fois, sans l'engin a construire, de sa longueur, de sa forme, de sa composition dimensions gigantesques; mais si grandes que soient les difficultes, m'ecouter, et ne m'epargnez pas les objections a bout portant. Je ne a conduits hier; le probleme se presente maintenant sous cette forme: obus de cent huit pouces de diametre et d'un poids de vingt mille l'espace, que se passe-t-il? Il est sollicite par trois forces force d'impulsion dont il est anime. Examinons ces trois forces. La importante. En effet, l'atmosphere terrestre n'a que quarante milles le projectile l'aura traversee en cinq secondes, et ce temps est assez insignifiante. Passons alors a l'attraction de la Terre, c'est-a-dire en raison inverse du carre des distances; en effet, voici ce que la surface de la Terre, sa chute est de quinze pieds [Soit 4 metres 90 .

getting around

home

adv.search

site map



Current spider themes

news archive

 

Licence of article: GNU FDL.
Original source @ wikipedia.