Spinor field
In differential geometry, given a spin structure on a n-dimensional Riemannian manifold (M, g) a section of the spinor bundle S is called a spinor field. The complex vector bundle
is associated to the corresponding principal bundle
of spin frames over M via the spin representation of its structure group Spin(n) on the space of spinors Δn.
In particle physics particles with spin s are described by 2s-dimensional spinor field, where s is a integer or a half-integer. Fermions are described by spinor field, while bosons by tensor field.
Contents
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 with respect to the double covering
One usually defines the spinor bundle[1] to be the complex vector bundle
associated to the spin structure P via the spin representation where U(W) denotes the group of unitary operators acting on a Hilbert space W.
A spinor field is defined to be a section of the spinor bundle S, i.e., a smooth mapping such that is the identity mapping idM of M.
See also
Notes
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Books
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