Spinor bundle

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Short description: Geometric structure

In differential geometry, given a spin structure on an n-dimensional orientable Riemannian manifold (M,g), one defines the spinor bundle to be the complex vector bundle π𝐒:𝐒M associated to the corresponding principal bundle π𝐏:𝐏M of spin frames over M and the spin representation of its structure group Spin(n) on the space of spinors Δn.

A section of the spinor bundle 𝐒 is called a spinor field.

Formal definition

Let (𝐏,F𝐏) be a spin structure on a Riemannian manifold (M,g),that is, an equivariant lift of the oriented orthonormal frame bundle FSO(M)M with respect to the double covering ρ:Spin(n)SO(n) of the special orthogonal group by the spin group.

The spinor bundle 𝐒 is defined [1] to be the complex vector bundle 𝐒=𝐏×κΔn associated to the spin structure 𝐏 via the spin representation κ:Spin(n)U(Δn), where U(𝐖) denotes the group of unitary operators acting on a Hilbert space 𝐖. It is worth noting that the spin representation κ is a faithful and unitary representation of the group Spin(n).[2]

See also

Notes

  1. Friedrich, Thomas (2000), Dirac Operators in Riemannian Geometry, American Mathematical Society, ISBN 978-0-8218-2055-1  page 53
  2. Friedrich, Thomas (2000), Dirac Operators in Riemannian Geometry, American Mathematical Society, ISBN 978-0-8218-2055-1  pages 20 and 24

Further reading

  • Lawson, H. Blaine; Michelsohn, Marie-Louise (1989). Spin Geometry. Princeton University Press. ISBN 978-0-691-08542-5. 
  • Friedrich, Thomas (2000), Dirac Operators in Riemannian Geometry, American Mathematical Society, ISBN 978-0-8218-2055-1 

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