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Fierz identity : ウィキペディア英語版
Fierz identity
In theoretical physics, a Fierz identity is an identity that allows one to rewrite ''bilinears of the product'' of two spinors as a linear combination of ''products of the bilinears'' of the individual spinors. It is named after Swiss physicist Markus Fierz.
There is a version of the Fierz identities for Dirac spinors and there is another version for Weyl spinors. And there are versions for other dimensions besides 3+1 dimensions.
Spinor bilinears can be thought of as elements of a Clifford Algebra. Then the Fierz identity is the concrete realization of the relation to the exterior algebra.
The identities for a generic scalar written as the contraction of two Dirac bilinears of the same type can be written with coefficients according to the following table.
For example, the V × V product can be expanded as,
:
\left(\bar\chi\gamma^\mu\psi\right)\left(\bar\psi\gamma_\mu \chi\right)=
\left(\bar\chi\chi\right)\left(\bar\psi\psi\right)-
\frac\left(\bar\chi\gamma^\mu\chi\right)\left(\bar\psi\gamma_\mu\psi\right)-
\frac\left(\bar\chi\gamma^\mu\gamma_5\chi\right)\left(\bar\psi\gamma_\mu\gamma_5\psi\right)
-\left(\bar\chi\gamma_5\chi\right)\left(\bar\psi\gamma_5\psi\right).
Simplifications arise when the considered spinors are chiral or Majorana spinors as some term in the expansion can be vanishing.
==References==
A derivation of identities for rewriting any scalar contraction of Dirac bilinears can be found in 29.3.4 of
See also appendix B.1.2 in


抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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