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Spinor bundle
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In differential geometry, given a on an n-dimensional orientable 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 \pi_{\mathbf P}\colon{\mathbf P}\to M\, of spin frames over M and the spin representation of its {\mathrm {Spin}}(n)\, on the space of \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 on a Riemannian manifold (M, g),\,that is, an 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) of the special orthogonal group by the .

The spinor bundle {\mathbf S}\, is defined page 53 to be the complex vector bundle {\mathbf S}={\mathbf P}\times_{\kappa}\Delta_n\, associated to the {\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 acting on a {\mathbf W}.\, The spin representation \kappa is a faithful and unitary representation of the group {\mathrm {Spin}}(n). pages 20 and 24


See also


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