In topology, a branch of mathematics, a string group is an infinite-dimensional group String ( n ) {\displaystyle \operatorname {String} (n)} introduced by Stolz (1996) as a 3 {\displaystyle 3} -connected cover of a spin group. A string manifold is a manifold with a lifting of its frame bundle to a string group bundle. This means that in addition to being able to define holonomy along paths, one can also define holonomies for surfaces going between strings. There is a short exact sequence of topological groups
0 → K ( Z , 2 ) → String ( n ) → Spin ( n ) → 0 {\displaystyle 0\rightarrow {\displaystyle K(\mathbb {Z} ,2)}\rightarrow \operatorname {String} (n)\rightarrow \operatorname {Spin} (n)\rightarrow 0}
where K ( Z , 2 ) {\displaystyle K(\mathbb {Z} ,2)} is an Eilenberg–MacLane space and Spin ( n ) {\displaystyle \operatorname {Spin} (n)} is a spin group. The string group is an entry in the Whitehead tower (dual to the notion of Postnikov tower) for the orthogonal group:
⋯ → Fivebrane ( n ) → String ( n ) → Spin ( n ) → SO ( n ) → O ( n ) {\displaystyle \cdots \rightarrow \operatorname {Fivebrane} (n)\to \operatorname {String} (n)\rightarrow \operatorname {Spin} (n)\rightarrow \operatorname {SO} (n)\rightarrow \operatorname {O} (n)}
It is obtained by killing the π 3 {\displaystyle \pi _{3}} homotopy group for Spin ( n ) {\displaystyle \operatorname {Spin} (n)} , in the same way that Spin ( n ) {\displaystyle \operatorname {Spin} (n)} is obtained from SO ( n ) {\displaystyle \operatorname {SO} (n)} by killing π 1 {\displaystyle \pi _{1}} . The resulting manifold cannot be any finite-dimensional Lie group, since all finite-dimensional compact Lie groups have a non-vanishing π 3 {\displaystyle \pi _{3}} . The fivebrane group follows, by killing π 7 {\displaystyle \pi _{7}} .
More generally, the construction of the Postnikov tower via short exact sequences starting with Eilenberg–MacLane spaces can be applied to any Lie group G, giving the string group String(G).