String group explained
In topology, a branch of mathematics, a string group is an infinite-dimensional group
introduced by as a
-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 → {\displaystyleK(Z,2)} → \operatorname{String}(n) → \operatorname{Spin}(n) → 0
where
is an
Eilenberg–MacLane space and
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:
… → \operatorname{Fivebrane}(n)\to\operatorname{String}(n) → \operatorname{Spin}(n) → \operatorname{SO}(n) → \operatorname{O}(n)
It is obtained by killing the
homotopy group for
, in the same way that
is obtained from
by killing
. The resulting manifold cannot be any finite-dimensional
Lie group, since all finite-dimensional compact Lie groups have a non-vanishing
. The fivebrane group follows, by killing
.
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).
Intuition for the string group
The relevance of the Eilenberg-Maclane space
lies in the fact that there are the homotopy equivalences
for the
classifying space
, and the fact
. Notice that because the complex spin group is a group extension
0\toK(Z,1)\to\operatorname{Spin}C(n)\to\operatorname{Spin}(n)\to0
the String group can be thought of as a "higher" complex spin group extension, in the sense of
higher group theory since the space
is an example of a higher group. It can be thought of the topological realization of the
groupoid
whose object is a single point and whose morphisms are the group
. Note that the homotopical degree of
is
, meaning its homotopy is concentrated in degree
, because it comes from the
homotopy fiber of the map
\operatorname{String}(n)\to\operatorname{Spin}(n)
from the Whitehead tower whose homotopy cokernel is
. This is because the homotopy fiber lowers the degree by
.
Understanding the geometry
The geometry of String bundles requires the understanding of multiple constructions in homotopy theory,[1] but they essentially boil down to understanding what
-bundles are, and how these higher group extensions behave. Namely,
-bundles on a space
are represented geometrically as
bundle gerbes since any
-bundle can be realized as the homotopy fiber of a map giving a homotopy square
\begin{matrix}
P&\to&*\\
\downarrow&&\downarrow\\
M&\xrightarrow{}&K(Z,3)
\end{matrix}
where
. Then, a string bundle
must map to a spin bundle
which is
-equivariant, analogously to how spin bundles map equivariantly to the frame bundle.
Fivebrane group and higher groups
The fivebrane group can similarly be understood[2] by killing the
\pi7(\operatorname{Spin}(n))\cong\pi7(\operatorname{O}(n))
group of the string group
using the Whitehead tower. It can then be understood again using an exact sequence of
higher groups0\toK(Z,6)\to\operatorname{Fivebrane}(n)\to\operatorname{String}(n)\to0
giving a presentation of
\operatorname{Fivebrane}(n)
it terms of an iterated extension, i.e. an extension by
by
. Note map on the right is from the Whitehead tower, and the map on the left is the homotopy fiber.
See also
External links
- From Loop Groups to 2-groups - gives a characterization of String(n) as a 2-group
Notes and References
- Jurco. Branislav. August 2011. Crossed Module Bundle Gerbes; Classification, String Group and Differential Geometry. International Journal of Geometric Methods in Modern Physics. 08. 5. 1079–1095. 10.1142/S0219887811005555. 0219-8878. math/0510078. 2011IJGMM..08.1079J . 1347840.
- Sati. Hisham. Schreiber. Urs. Stasheff. Jim. November 2009. Fivebrane Structures. Reviews in Mathematical Physics. 21. 10. 1197–1240. 10.1142/S0129055X09003840. 0805.0564. 2009RvMaP..21.1197S . 13307997. 0129-055X.