Spinh structure


In spin geometry, a spinh structure is a generalization of a spin structure. In mathematics, these are used to describe spinor bundles and spinors, which in physics are used to describe spin, an intrinsic angular momentum of particles after which they have been named. Since spinh structures also exist under weakened conditions, which might not allow spin structures, they provide a suitable alternative for such situations. Orientable manifolds with spinh structures are called spinh manifolds. H stands for the quaternions, which are denoted and appear in the definition of the underlying spinh group.

Definition

Let be a -dimensional orientable manifold. Its tangent bundle is described by a classifying map into the classifying space of the special orthogonal group. It can factor over the map induced by the canonical projection on classifying spaces. In this case, the classifying map lifts to a continuous map into the classifying space of the spinh group. Its homotopy class is called spinh structure.
Assume has a spinh structure. Let then denote the set of spinh structures on. The first symplectic group [Principal U(1)-bundle|] is the second factor of the spinh group and using its classifying space [Principal U(1)-bundle|], which is the infinite quaternionic projective space [Principal U(1)-bundle|]and through its Postnikov tower projects onto the Eilenberg–MacLane space, there is a map:
The former isomorphism follows from the Puppe sequence for the fibration . Although this map is not a bijection in general, it is in special cases, for example for a 4-manifold.
Due to the canonical projection, every spinh structure induces a principal -bundle or equivalently a orientable real vector bundle of third rank.

Properties

The following properties hold more generally for the lift on the Lie group, with the particular case giving:
  • If is a spinh manifold, then and are spinh manifolds.
  • If is a spin manifold, then is a spinh manifold iff is a spinh manifold.
  • If and are spinh manifolds of same dimension, then their connected sum is a spinh manifold.
  • The following conditions are equivalent:
  • * is a spinh manifold.
  • * There is a real vector bundle of third rank, so that has a spin structure or equivalently.
  • * can be immersed in a spin manifold with three dimensions more.
  • * can be embedded in a spin manifold with three dimensions more.

Cohomology of infinite classifying space

The cohomology ring of the infinite classifying space with coefficients in can be expressed using Steenrod squares and Wu classes:

Literature

*