Indices which have hats are called Dirac indices, and are the set of dotted and undotted, or chiral and anti-chiral, indices. For example, if : \alpha = 1,2\,,\dot{\alpha} = \dot{1},\dot{2} then a spinor in the chiral basis is represented as :\Sigma_\hat{\alpha} = \begin{pmatrix} \psi_{\alpha}\\ \bar{\chi}^{\dot{\alpha}}\\ \end{pmatrix} where : \hat{\alpha}= (\alpha,\dot{\alpha}) = 1,2,\dot{1},\dot{2} In this notation the
Dirac adjoint (also called the
Dirac conjugate) is :\Sigma^\hat{\alpha} = \begin{pmatrix} \chi^{\alpha} & \bar{\psi}_{\dot{\alpha}} \end{pmatrix} ==See also==