Covariant Bilinears: Fierz Expansion of Dirac gamma matrices products

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Homework Help Overview

The discussion revolves around the Fierz identities in quantum field theory, specifically focusing on the expansion of products of Dirac gamma matrices. The original poster attempts to explore an alternative method to the trace method for expressing the product of gamma matrices.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the expression of \(\gamma_5\gamma^{\alpha}\gamma^{\mu}\) using a method that involves ensuring the same number of indices on both sides and utilizing base matrices. Questions arise about the correctness of the proposed expansion and the determination of coefficients in the expression.

Discussion Status

Some participants suggest that there should be a pseudotensor term in the expansion, while others question the completeness of the initial expression. The conversation indicates that additional terms may be necessary for a complete representation, and there is acknowledgment of the need to refine the expression further.

Contextual Notes

There is mention of specific mathematical identities and properties, such as the anticommutation relations and the Levi-Civita symbol, which are relevant to the discussion but not fully resolved within the thread.

PLuz
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Homework Statement



So my question is related somehow to the Fierz Identities.

I'm taking a course on QFT. My teacher explained in class that instead of using the traces method one could use another, more intuitive, method. He said that we could use the fact that if we garante that we have the same number os indexes at each side of the expression and only use the base matrices (scalar, vector, pseudoscalar, tensor and axial) one would get the same results as using the traces method.

He then gave an example and advised for us to try with some other example.

I then tried to write \gamma_5\gamma^{\alpha}\gamma^{\mu} using that method.

Homework Equations



\sigma^{\alpha\mu}=\frac{i}{2}[\gamma^{\alpha},\gamma^{\mu}]
\eta^{\alpha \mu} is the minkowski metric and I_{4} is the identity matrix in 4-spacetime.

The Attempt at a Solution



The attempt of a solution goes as:
\gamma_{5}\gamma^{\alpha}\gamma^{\mu}=<br /> a*\eta^{\alpha\mu}I_{4}+b*\eta^{\alpha\mu}\gamma_{5}<br /> +c*\sigma^{\alpha\mu}

Is this correct?

If I contract \gamma_5\gamma^\alpha\gamma^\mu with \eta_{\alpha \mu} I get a=0 and b=1. But if the above expression is correct, how can I get c?

Please, somebody help me.
 
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From the definition of \sigma^{\alpha\mu} and the anticommutation relations, you can see that there must be a term \gamma_5\sigma^{\alpha\mu} in the expansion of \gamma_5\gamma^\alpha\gamma^\mu. I guess we'd call this a pseudotensor term.
 
Thanks for the prompt reply,

I thought so, but I have read that such term would not be independent of the other 16 matrices.

\sigma^{\alpha \mu}\gamma_{5}=\frac{i}{2}\epsilon^{\alpha \mu \nu \beta}\sigma_{\nu \beta}

,where \epsilon^{\alpha \mu \nu \beta} is the Levi-Civita symbol

So the above expression for \gamma_{5}\gamma^{\alpha} \gamma^{\mu} is incomplete and I should add a extra term
d* \epsilon^{\alpha \mu \nu \beta}\sigma_{\nu \beta} ?
 
Last edited:
I got it now.

One as to add such term and then get the correct answer. For other readers with a similar doubt I got:

\gamma_{5}\gamma^{\alpha}\gamma^{\mu}=\eta^{\alpha\mu}I_{4}+\frac{1}{2}\epsilon^{\alpha\mu\nu\beta}σ_{\nu\beta}

Which I believe, it's the correct answer.
 

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