In mathematics, a group extension is a general means of describing a group in terms of a particular normal subgroup and quotient group. If
Q
N
G
Q
N
1\toN \overset{\iota}{\to} G \overset{\pi}{\to} Q\to1.
If
G
Q
N
G
\iota(N)
G
G/\iota(N)
Q
Q
N
G
G
N
Q
G
N
G/N
An extension is called a central extension if the subgroup
N
G
One extension, the direct product, is immediately obvious. If one requires
G
Q
Q
N
1 | |
\operatorname{Ext} | |
Z |
(Q,N);
cf. the Ext functor. Several other general classes of extensions are known but no theory exists that treats all the possible extensions at one time. Group extension is usually described as a hard problem; it is termed the extension problem.
To consider some examples, if, then
G
H
K
G
K
H
G=K\rtimesH
G
H
K
The question of what groups
G
H
N
\{Ai\}
\{Ai+1\}
\{Ai\}
Solving the extension problem amounts to classifying all extensions of H by K; or more practically, by expressing all such extensions in terms of mathematical objects that are easier to understand and compute. In general, this problem is very hard, and all the most useful results classify extensions that satisfy some additional condition.
It is important to know when two extensions are equivalent or congruent. We say that the extensions
1\toK\stackrel{i}{{}\to{}}G\stackrel{\pi}{{}\to{}}H\to1
1\toK\stackrel{i'}{{}\to{}}G'\stackrel{\pi'}{{}\to{}}H\to1
T:G\toG'
T
It may happen that the extensions
1\toK\toG\toH\to1
1\toK\toG\prime\toH\to1
8
Z/2Z
8
2
A trivial extension is an extension
1\toK\toG\toH\to1
that is equivalent to the extension
1\toK\toK x H\toH\to1
where the left and right arrows are respectively the inclusion and the projection of each factor of
K x H
A split extension is an extension
1\toK\toG\toH\to1
s\colonH\toG
\pi\circs=idH
Split extensions are very easy to classify, because an extension is split if and only if the group G is a semidirect product of K and H. Semidirect products themselves are easy to classify, because they are in one-to-one correspondence with homomorphisms from
H\to\operatorname{Aut}(K)
In general in mathematics, an extension of a structure K is usually regarded as a structure L of which K is a substructure. See for example field extension. However, in group theory the opposite terminology has crept in, partly because of the notation
\operatorname{Ext}(Q,N)
A paper of Ronald Brown and Timothy Porter on Otto Schreier's theory of nonabelian extensions uses the terminology that an extension of K gives a larger structure.[3]
A central extension of a group G is a short exact sequence of groups
1\toA\toE\toG\to1
Z(E)
H2(G,A)
Examples of central extensions can be constructed by taking any group G and any abelian group A, and setting E to be
A x G
H2(G,A)
A\rtimesG
In the case of finite perfect groups, there is a universal perfect central extension.
ak{g}
0 → ak{a} → ak{e} → ak{g} → 0
ak{a}
ak{e}
There is a general theory of central extensions in Maltsev varieties.[4]
There is a similar classification of all extensions of G by A in terms of homomorphisms from
G\to\operatorname{Out}(A)
In Lie group theory, central extensions arise in connection with algebraic topology. Roughly speaking, central extensions of Lie groups by discrete groups are the same as covering groups. More precisely, a connected covering space of a connected Lie group is naturally a central extension of, in such a way that the projection
\pi\colonG*\toG
is a group homomorphism, and surjective. (The group structure on depends on the choice of an identity element mapping to the identity in .) For example, when is the universal cover of, the kernel of π is the fundamental group of, which is known to be abelian (see H-space). Conversely, given a Lie group and a discrete central subgroup, the quotient is a Lie group and is a covering space of it.
More generally, when the groups, and occurring in a central extension are Lie groups, and the maps between them are homomorphisms of Lie groups, then if the Lie algebra of is, that of is, and that of is, then is a central Lie algebra extension of by . In the terminology of theoretical physics, generators of are called central charges. These generators are in the center of ; by Noether's theorem, generators of symmetry groups correspond to conserved quantities, referred to as charges.
The basic examples of central extensions as covering groups are:
The case of involves a fundamental group that is infinite cyclic. Here the central extension involved is well known in modular form theory, in the case of forms of weight . A projective representation that corresponds is the Weil representation, constructed from the Fourier transform, in this case on the real line. Metaplectic groups also occur in quantum mechanics.