Cluster decomposition of the S-matrix

acipsen
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Hi,

I am reading through Weinberg's "Quantum Theory of Fields" (vol. 1)
and I am somewhat confused about the signs in the cluster decomposition
of the S-matrix. Specifically, referring to eq. 4.3.2, let's say the term
coming from the partition
\alpha \to \alpha_1\alpha_2,\beta \to \beta_1\beta_2
would be
+S^C_{\beta_1,\alpha_1}S^C_{\beta_2,\alpha_2}.
Lets now assume that permuting \alpha_1,\alpha_2 gives a sign, while permuting \beta_1,\beta_2 doesn't,
then the equivalent partition
\alpha \to \alpha_2\alpha_1,\beta \to \beta_2\beta_1
would give rise to the term
-S^C_{\beta_2,\alpha_2}S^C_{\beta_1,\alpha_1},
i.e. minus what I had before. This clearly cannot be right, but I'm not sure where
the flaw in my reasoning is. Does it have something to do with conservation
of (-1)^F, where F is the number of Fermions?

I would be grateful for any hints. And no, this is not homework :smile:, the course I'm
following is using Peskin & Schroeder.

Regards,
Asger
 
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Welcome to PF!

Hi Asger! Welcome to PF! :smile:

(have an alpha: α and a beta: β and try using the X2 tag just above the Reply box :wink:)

Since αi and βi together form a separate experiment, for each i, the number of fermions in αi will be odd only if the number in βi is.

So swapping two experiments will give the same number of fermion interchanges for α as for β. :wink:
 
Hi Tim!

Thanks for the answer. I'm sure Weinberg thought that it too obvious to mention.

Regards,
Asger
 
acipsen said:
Hi Tim!

Thanks for the answer. I'm sure Weinberg thought that it too obvious to mention.

Regards,
Asger

That is Weinberg's style :) If it is too simple, he does not mention it ;)
 
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