nLab
spin group

Context

-Lie theory

∞-Lie theory

Background

Smooth structure

Higher groupoids

Lie theory

∞-Lie groupoids

∞-Lie algebroids

Formal Lie groupoids

Cohomology

Homotopy

Examples

-Lie groupoids

-Lie groups

-Lie algebroids

-Lie algebras

Contents

Idea

The spin group Spin(n) is the universal covering space of the special orthogonal group SO(n). By the usual arguments it inherits a group structure for which the operations are smooth and so is a Lie group like SO(n).

Properties

General

By definition the spin group sits in a short exact sequence of groups

2SpinSO.\mathbb{Z}_2 \to Spin \to SO \,.

Homotopy theory

The spin group is one element in the Whitehead tower of O(n), which starts out like

Fivebrane(n)String(n)Spin(n)SO(n)O(n).\cdots \to Fivebrane(n) \to String(n) \to Spin(n) \to SO(n) \to \mathrm{O}(n) \,.

The homotopy groups of O(n) are for k and for sufficiently large n

π 8k+0(O) = 2 π 8k+1(O) = 2 π 8k+2(O) =0 π 8k+3(O) = π 8k+4(O) =0 π 8k+5(O) =0 π 8k+6(O) =0 π 8k+7(O) =.\array{ \pi_{8k+0}(O) & = \mathbb{Z}_2 \\ \pi_{8k+1}(O) & = \mathbb{Z}_2 \\ \pi_{8k+2}(O) & = 0 \\ \pi_{8k+3}(O) & = \mathbb{Z} \\ \pi_{8k+4}(O) & = 0 \\ \pi_{8k+5}(O) & = 0 \\ \pi_{8k+6}(O) & = 0 \\ \pi_{8k+7}(O) & = \mathbb{Z} } \,.

By co-killing these groups step by step one gets

cokillthis toget π 0(O) = 2 SO π 1(O) = 2 Spin π 2(O) =0 π 3(O) = String π 4(O) =0 π 5(O) =0 π 6(O) =0 π 7(O) = Fivebrane.\array{ cokill this &&&& to get \\ \\ \pi_{0}(O) & = \mathbb{Z}_2 &&& SO \\ \pi_{1}(O) & = \mathbb{Z}_2 &&& Spin \\ \pi_{2}(O) & = 0 \\ \pi_{3}(O) & = \mathbb{Z} &&& String \\ \pi_{4}(O) & = 0 \\ \pi_{5}(O) & = 0 \\ \pi_{6}(O) & = 0 \\ \pi_{7}(O) & = \mathbb{Z} &&& Fivebrane } \,.

Exceptional isomorphisms

In low dimensions the spin group happens to be isomorphic to various other classical group (among them the general linear group GL(p,V) for V the real numbers , the complex numbers and the quaternions , the orthogonal group O(p,q), the unitary group U(p,q) and the symplectic group Sp(p,q)).

We have

  • in Riemannian signature

    • Spin(1)O(1)

    • Spin(2)U(1)SO(2)

    • Spin(3)Sp(1)SU(2)

    • Spin(4)Sp(1)×Sp(1)

    • Spin(5)Sp(2)

    • Spin(6)SU(4)

  • in Lorentzian signature

    • Spin(1,1)GL(1,)

    • Spin(2,1)SL(2,)

    • Spin(3,1)SL(2,)

    • Spin(4,1)Sp(1,1)

    • Spin(5,1)SL(2,)

  • in anti de Sitter signature

    • Spin(2,2)SL(2,)×SL(2,)

    • Spin(3,2)Sp(4,)

    • Spin(4,2)SU(2,2)

Beyond these dimensions there are still some interesting identifications, but the situation becomes much more involved.

Applications

Spin geometry

See spin geometry

In physics

The name arises due to the requirement that the structure group of the tangent bundle of spacetime lifts to Spin(n) so as to ‘define particles with spin’… (Someone more awake and focused please put this into proper words!)

See spin structure.

The Whitehead tower of the orthogonal group looks like

fivebrane group string group spin group special orthogonal group orthogonal group.

Another extension of SO is the spin^c group.

groupsymboluniversal coversymbolhigher coversymbol
orthogonal groupO(n)Pin groupPin(n)Tring groupTring(n)
special orthogonal groupSO(n)Spin groupSpin(n)String groupString(n)
Lorentz groupO(n,1)Spin(n,1)
anti de Sitter groupO(n,2)Spin(n,2)
Poincaré groupISO(n,1)
super Poincaré groupsISO(n,1)

References

A standard textbook reference is

  • H.B. Lawson and M.-L. Michelson, Spin Geometry , Princeton University Press, Princeton, NJ, (1989)

See also