Menu
Home Explore People Places Arts History Plants & Animals Science Life & Culture Technology
On this page
Spinor bundle
Geometric structure

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

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

We don't have any images related to Spinor bundle yet.
We don't have any YouTube videos related to Spinor bundle yet.
We don't have any PDF documents related to Spinor bundle yet.
We don't have any Books related to Spinor bundle yet.
We don't have any archived web articles related to Spinor bundle yet.

Formal definition

Let ( P , F P ) {\displaystyle ({\mathbf {P} },F_{\mathbf {P} })} be a spin structure on a Riemannian manifold ( M , g ) , {\displaystyle (M,g),\,} that is, an equivariant lift of the oriented orthonormal frame bundle F S O ( M ) → M {\displaystyle \mathrm {F} _{SO}(M)\to M} with respect to the double covering ρ : S p i n ( n ) → S O ( n ) {\displaystyle \rho \colon {\mathrm {Spin} }(n)\to {\mathrm {SO} }(n)} of the special orthogonal group by the spin group.

The spinor bundle S {\displaystyle {\mathbf {S} }\,} is defined 1 to be the complex vector bundle S = P × κ Δ n {\displaystyle {\mathbf {S} }={\mathbf {P} }\times _{\kappa }\Delta _{n}\,} associated to the spin structure P {\displaystyle {\mathbf {P} }} via the spin representation κ : S p i n ( n ) → U ( Δ n ) , {\displaystyle \kappa \colon {\mathrm {Spin} }(n)\to {\mathrm {U} }(\Delta _{n}),\,} where U ( W ) {\displaystyle {\mathrm {U} }({\mathbf {W} })\,} denotes the group of unitary operators acting on a Hilbert space W . {\displaystyle {\mathbf {W} }.\,} The spin representation κ {\displaystyle \kappa } is a faithful and unitary representation of the group S p i n ( n ) . {\displaystyle {\mathrm {Spin} }(n).} 2

See also

Notes

Further reading

|

References

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

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