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288 November 7, 2013<br />

where S, p µ , q µ and P are real, and T µν is real and antisymmetric. The requirement<br />

is now that N ≡ Π 2 − Π vanish, and so its trace with any Clifford<br />

element must also vanish. We can immediately find<br />

2Tr ( γ 5 /pN ) = (p · q)S , 2Tr ( (γ 5 /q − /p)N ) = (p 2 + q 2 )S . (10.155)<br />

There are now several possibilities, the first of which is the regular case : it is<br />

the case where S ≠ 0 and p 2 ≠ 0. We see that it implies that q 2 = −p 2 and<br />

p · q = 0, so that p and q are linearly independent and one of them must be<br />

timelike. In that case we may form a Vierbein by finding two additional vectors<br />

e 1,2 µ with<br />

p · e 1,2 = q · e 1,2 = e 1 · e 2 = 0 , e 1,2 2 = −1 , (10.156)<br />

so that the tensor T can be decomposed 24 as follows:<br />

T αβ = c pq p [α q β] + c 12 e [α 1 e β] 2 + ∑ (<br />

) c pj p [α e β] j + c qj q [α β]<br />

e j , (10.157)<br />

j=1,2<br />

where the coefficients are all real and the square brackets indicate antisymmetrization<br />

over the indices. We can now find two more conditions:<br />

1<br />

p 2 S Tr ((c p1p µ e ν 1 − c q2 q µ e ν 2 )σ µν N) = c 2 p1 + c 2 q2 ,<br />

1<br />

p 2 S Tr ((c p2p µ e ν 2 − c q1 q µ e ν 1 )σ µν N) = c 2 p2 + c 2 q1 , (10.158)<br />

which tells us that c p1 = c p2 = c q1 = c q2 = 0. The tensorial part can therefore<br />

only consist of /p/q and /pγ 5 /q, and we may write<br />

Π = 1 4<br />

(<br />

(2 − S) + /p + γ 5 /q + iP γ 5 + ia/p/q + b/pγ 5 /q ) (10.159)<br />

with a and b real. Then, the results<br />

− 2 p 2 Tr (/pN) = S − p2 b , 2iTr ( γ 5 N ) = SP + p 4 ab (10.160)<br />

fix the values of a = −P/p 2 and b = S/p 2 . Continuing, we evaluate<br />

− 1 p 2 ɛ αβµνp α q β Tr (σ µν N) = S 2 + P 2 − p 2 , (10.161)<br />

which proves that p µ must actually be the timelike vector, and fixes |P |. Using<br />

all the relations obtained, we finally have<br />

Tr (N) = S 2 − 1 , (10.162)<br />

which tells us that if S ≠ 0 we can take S = 1 (without loss of generality since<br />

both Π and 1 − Π satisfy Eq.(10.151)), and we must have p 2 ≥ 1. The generic<br />

24 No matter that the vectors e 1,2 are not unambiguous : the point is that a decompisition<br />

is possible.

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