Neutrino-neutrino to WW amplitude via Z-exchange

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Homework Help Overview

The discussion revolves around a problem in particle physics, specifically related to calculating the amplitude for neutrino-neutrino interactions via Z-exchange as presented in Chapter 6 of Quigg's Gauge Theories. The original poster is focused on understanding the S^{\mu}S^{\nu} term and its implications in the context of massless spinors.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to clarify how to derive the factors involving S^{\mu}S^{\nu} and expresses confusion about the interaction of these terms with the existing calculations. They seek explicit calculations or explanations to resolve their uncertainty.

Discussion Status

Some participants have engaged with the original poster's inquiry, with one asking for clarification on whether the focus is solely on the amplitude. The original poster later indicates they have resolved their confusion regarding the S^{\mu}S^{\nu} terms, noting that they lead to a zero contribution to the amplitude.

Contextual Notes

The original poster mentions fatigue as a factor in their earlier misunderstanding, suggesting that the discussion may involve complex calculations and concepts that require careful attention.

blankvin
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Homework Statement



I am working through an example in Chapter 6 of Quigg's Gauge Theories. I have it mostly figured out, with the exception of how to work out the S^{\mu}S^{\nu} term. All he writes is "...the term is impotent between massless spinors."

Homework Equations


I begin with:

nunu_WW_amplitude.png


What I want to know is how to obtain the factors that include S:

result.png


The Attempt at a Solution


I have all of the terms except those which include S. An explicit calculation or explanation would be extremely appreciated!

[Edit] I will show my work to point out where I am stuck.

I worked out the term involving g^{\mu\nu}. After the contraction of \gamma_\nu g^{\mu\nu}, the polarization vectors contract with the terms in square brackets to give:

\epsilon_+^{*\alpha}\epsilon_-^{*\beta}[...] = \epsilon_+^{*} \cdot \epsilon_-^{*} (k_- - k_+)_{\nu} + \epsilon_-^{*} \cdot k_+ \epsilon_{+\nu}^* - \epsilon_+^* \cdot k_- \epsilon_{-\nu}^* [1]

My understanding is that the S^{\mu}S^{\nu} will act on [1] above, but I do not see how to get the desired result. I thought that the contravariant S^{\nu} term would contract with the covariants, but instead somehow the k_+ and k_- in the second and third terms of [1] above are replaced by S. Either this is something I do not quite get, or I am being foolish.blankvin
 
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Are you just looking for the amplitude?
 
saybrook1 said:
Are you just looking for the amplitude?

I know what the amplitude is. It is how to deal with the S^{\mu}S^{\nu} that I do not know.blankvin
 
Yeah sorry, the first time I saw your post I was on mobile. I will check back on it when I have time if you haven't received a response yet.
 
I figured it out.

Working out the S^{\mu}S^{\nu} terms lead to zero contribution to the amplitude.

This blunder will be blamed on fatigue.blankvin
 

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