Loop group explained

In mathematics, a loop group (not to be confused with a loop) is a group of loops in a topological group G with multiplication defined pointwise.

Definition

In its most general form a loop group is a group of continuous mappings from a manifold to a topological group .

More specifically, let, the circle in the complex plane, and let denote the space of continuous maps, i.e.

LG=\{\gamma:S1\toG|\gamma\inC(S1,G)\},

equipped with the compact-open topology. An element of is called a loop in . Pointwise multiplication of such loops gives the structure of a topological group. Parametrize with,

\gamma:\theta\inS1\mapsto\gamma(\theta)\inG,

and define multiplication in by

(\gamma1\gamma2)(\theta)\equiv\gamma1(\theta)\gamma2(\theta).

Associativity follows from associativity in . The inverse is given by

\gamma-1:\gamma-1(\theta)\equiv\gamma(\theta)-1,

and the identity by

e:\theta\mapstoe\inG.

The space is called the free loop group on . A loop group is any subgroup of the free loop group .

Examples

An important example of a loop group is the group

\OmegaG

of based loops on . It is defined to be the kernel of the evaluation map

e1:LG\toG,\gamma\mapsto\gamma(1)

,

and hence is a closed normal subgroup of . (Here, is the map that sends a loop to its value at

1\to\OmegaG\toLG\toG\to1

.

The space splits as a semi-direct product,

LG=\OmegaG\rtimesG

.

We may also think of as the loop space on . From this point of view, is an H-space with respect to concatenation of loops. On the face of it, this seems to provide with two very different product maps. However, it can be shown that concatenation and pointwise multiplication are homotopic. Thus, in terms of the homotopy theory of, these maps are interchangeable.

Loop groups were used to explain the phenomenon of Bäcklund transforms in soliton equations by Chuu-Lian Terng and Karen Uhlenbeck.[1]

References

See also

Notes and References

  1. https://www.ams.org/notices/200001/fea-terng.pdf Geometry of Solitons