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 | | Spinors are in a representation of its covering group $SL(2,C)$ (see~\cite{pct,bogoliubov}), but are not in general in a representation of the full Lorentz group, covered by what one call the $Pin(1,3)$ group~\cite{cdewitt} (and $Pin(3,1)$ for $O(3,1)$). |
 | | A Majorana spinor is its own charge conjugated particle, which necessarily constrains this kind of particle to be neutral, and it must therefore obey the relation $\psi^c = \alpha \psi$ ($\alpha$ being a possible phase). |
 | | The existence of a Majorana representation (which depends only on the metric signature), only implies the possible existence of Majorana spinors.}, $C_-$ is proportional to the identity (and thus $C_-$ can always be written in the form $C_-= \sqrt{{\bf c_-}} S^*S^{-1}$ where $S$ is any $4\times 4$ invertible matrix). |
| perso.orange.fr /eric.chopin/latex/9805203b.txt (7177 words) |
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