Spinc structure

In spin geometry, a spinc structure (or complex spin 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 spinc structures also exist under weakened conditions, which might not allow spin structures, they provide a suitable alternative for such situations. Orientable manifolds with a spinc structure are called spinc manifolds. C stands for the complex numbers, which are denoted ℂ and appear in the definition of the underlying spinc group.

In four dimensions, a spinc structure defines two complex plane bundles, which can be used to describe negative and positive chirality of spinors, for example in the Dirac equation of relativistic quantum field theory. Another central application is Seiberg–Witten theory, which uses them to study 4-manifolds.

Definition

Let M be a n-dimensional orientable manifold. Its tangent bundle TM is described by a classifying map M→BSO⁡(n) into the classifying space BSO⁡(n) of the special orthogonal group SO⁡(n). It can factor over the map BSpinc(n)→BSO⁡(n) induced by the canonical projection Spinc(n)↠SO⁡(n) on classifying spaces. In this case, the classifying map lifts to a continuous map M→BSpinc(n) into the classifying space BSpinc(n) of the spinc group Spinc(n). Its homotopy class is called spinc structure.

Assume M has a spinc structure. Let then Spinc(M) denote the set of spinc structures on M. The first unitary group U⁡(1) is the second factor of the spinc group and using its classifying space BU⁡(1)≅BSO⁡(2), which is the infinite complex projective space ℂP∞ and a model of the Eilenberg–MacLane space K(ℤ,2), there is a bijection:

Spinc(M)≅[M,BU⁡(1)]≅[M,ℂP∞]≅[M,K(ℤ,2)]≅H2(M,ℤ).

The former isomorphism follows from the Puppe sequence for the fibration ℂP∞↪BSpinc(n)↠BSO⁡(n) (when applying [M,−]).

Due to the canonical projection BSpinc(n)→U⁡(1)/ℤ2≅U⁡(1), every spinc structure induces a principal U⁡(1)-bundle or equivalently a complex line bundle.

Properties

The following properties hold more generally for the lift on the Lie group Spink(n):=(Spin⁡(n)×Spin⁡(k))/ℤ2, with the particular case k=2 giving:

Cohomology of infinite classifying space

The cohomology ring of the infinite classifying space BSpinc:=limn→∞BSpinc(n) with coefficients in ℤ2 can be expressed using Steenrod squares and Wu classes:

H∗(BSpinc,ℤ2)≅H∗(BSO⁡,ℤ2)/(Sq1ν2r,r≥1).

See also

Literature

References

  1. ↑ Lawson & Michelson 90, Definition D.3
  2. ↑ Albanese & Milivojević 2021, Definition 3.1
  3. ↑ Stable complex and Spinc-structures, Definition D.28
  4. ↑ Mellor 1995, Theorem 5
  5. ↑ Albanese & Milivojević 2021, p. 6
  6. ↑ Mellor 1995, Theorem 2
  7. 1 2 3 Nicolaescu, Example 1.3.16
  8. ↑ Lawson & Michelson 90, Theorem D.2 und Corollary D.4
  9. ↑ Stable complex and Spinc-structures, Proposition D.31
  10. ↑ Mellor 1995, Theorem 3
  11. ↑ Lawson & Michelson 90, Corollary D.16
  12. 1 2 Albanese & Milivojević 2021, Proposition 3.6.
  13. ↑ Albanese & Milivojević 2021, Proposition 3.7.
  14. ↑ Albanese & Milivojević 2021, Proposition 3.2.
  15. ↑ Lawson 2023, p. 8
  16. ↑ Hu 2023, Rem. 4.30