dextercioby said:
The electron is a quanta of the electron field:a Grassmann \left(\frac{1}{2},0\right)\oplus \left(0,\frac{1}{2}\right) irreductible representation of \mbox{SO(3,1)} to which certain conditions are imposed (see the solving of Dirac's equation for free field).
Daniel.
Yes and every good student should ask the question : WHY ?
Well, the answer is once again group theory.
When studying the Lorentz group (the group that arises when you 'add up' both rotations and Lorentz boosts) one can prove that the generators will obey certain commutation relations conform the SO(3,1)-algebra.
When studying this algebra we can prove that (by writing these generators in a 'certain' way : J+, J-) [J+,J-] = 0. This results tells us that the representations generated by these two operators are 'independent' of each other. More formally, the SO(3,1) breaks up into two SU(2)-algebra's. Why SU(2), well that's because of how J+ and J- are defined (which we won't discuss). Just imagine that the two operators obey the rules 'for belonging to this SU(2)-algebra'
Basically this means that once you know the SU(2)-representations, you also know the SO(3,1)-representations. The generators of these algebra's are the famous Pauli-matrices.
Each SU(2) representation is denoted by a number j which has values 0,1/2,1,3/2,...and it contains 2j+1 objects \phi _{m} (and m is equal to -j,-j-1,...,0,1,...,j) that transform into each other under such transformations generated by the Pauli-matrices.
For SO(3,1) we need two such j's : (j+,j-) and the representations are (0,0), (1/2,0), (0,1/2), (1,0),...
The (1/2,0) and (0,1/2) are the socalled spinor representations. If have explained what a spinor is, in my journal.As you can see, a spinor has two components (2*1/2+1) and can be represented by a 2*1-matrix (\phi_{1,2}, the component-notation of such a matrix). But Dirac proved (when quantizing the Dirac field of which the fluctuations are the electrons) that the 'correct' spinor (that describes an electron) needs 4 components. Why ? Well, because of parity conservation. The two representations that we are talking about are interchanged when parity is changed. Thus we work with BOTh representations at once : this is what dexter wrote in his post : (1/2,0) + (0,1/2). We basically put two (Weyl)spinors together to form a Dirac spinor.
regards
marlon