Spinor bundle

In differential geometry, given a spin structure on a n-dimensional Riemannian manifold (M,g),\, one defines the spinor bundle to be the complex vector bundle \pi _{\mathbf {S} }\colon {\mathbf {S} }\to M\, associated to the corresponding principal bundle \pi _{\mathbf {P} }\colon {\mathbf {P} }\to M\, of spin frames over M and the spin representation of its structure group {\mathrm {Spin} }(n)\, on the space of spinors \Delta _{n}.\,.

A section of the spinor bundle {\mathbf {S} }\, is called a spinor field.

Formal definition

Let ({\mathbf {P} },F_{\mathbf {P} }) be a spin structure on a Riemannian manifold (M,g),\, that is, an equivariant lift of the oriented orthonormal frame bundle \mathrm {F} _{SO}(M)\to M with respect to the double covering \rho \colon {\mathrm {Spin} }(n)\to {\mathrm {SO} }(n).\,

The spinor bundle {\mathbf {S} }\, is defined [1] to be the complex vector bundle

{\mathbf {S} }={\mathbf {P} }\times _{\kappa }\Delta _{n}\,

associated to the spin structure {\mathbf {P} } via the spin representation \kappa \colon {\mathrm {Spin} }(n)\to {\mathrm {U} }(\Delta _{n}),\, where {\mathrm {U} }({\mathbf {W} })\, denotes the group of unitary operators acting on a Hilbert space {\mathbf {W} }.\, It is worth noting that the spin representation \kappa is a faithful and unitary representation of the group {\mathrm {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


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