A question about trace technology

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Discussion Overview

The discussion revolves around understanding the trace technology in quantum field theory, specifically related to the unpolarized cross section of the process e^- e^+ → μ^- μ^+. Participants are trying to clarify the derivation of a specific trace expression involving gamma matrices and the associated indices.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant expresses confusion over the derivation of the trace relation in equation 5.4 from Peskin-Schroeder, specifically regarding the indices involved.
  • Another participant suggests that understanding traces with gamma matrices is essential and offers to provide useful relations.
  • A participant shares their initial experience of calculating traces "brute force" and emphasizes the importance of understanding the method rather than just the result.
  • Some participants mention that knowing trace identities is crucial for simplifying calculations, with one noting that the example can be calculated concisely if all identities are known.
  • There are inquiries about the application of trace formulas and how to transition from the left-hand side of the equation to the right-hand side, with suggestions to refer to specific equations in the text.
  • One participant asks for clarification on why certain terms can be commuted out of the trace, leading to a discussion about the nature of four-vectors and gamma matrices.
  • Another participant raises a question about the origin of the trace in a specific matrix product, prompting an explanation about the summation over indices in matrix multiplication.

Areas of Agreement / Disagreement

Participants generally agree on the need for a solid understanding of gamma matrix traces and the importance of trace identities. However, there is no consensus on the specific methods or approaches to derive the expressions discussed, indicating that multiple viewpoints and techniques are being explored.

Contextual Notes

Some participants express uncertainty about their familiarity with gamma matrices and trace operations, suggesting that their understanding may depend on prior knowledge of these concepts. There are also references to specific equations and identities that may not be universally known among all participants.

Vereinsamt
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Hi everybody!

While reading Peskin-Schroeder, i stuck in the in equation 5.4 about the unpolarized cross section of the e^- e^+ \rightarrow \mu^- \mu^+ annihilation. i didn't understand how this relationof the electron trace came to be, and where the indices came from?

\operatorname{tr}[(p\!\!/^\prime-m_e) \gamma^\mu (p\!\!/ + m_e) \gamma^\nu] = 4[p^{\prime \mu} p^\nu +p'^\nu p^\mu - g^{\mu \nu} (p \cdot p' + m^2_e)]


thanx in advanced!
 
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what have you tried? Do you know how traces with gamma matrices works at all?

if not, then I can give some relations that are useful
 
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Hi,

I remember when I first encountered with those... very confused I was. First time, I did it "brute force". Calculated all the components on one side, check they were the same on the other. Of course it is stupid, and not the right way to do it. But by doing so, I understood how to work it out neatly.

Everybody has his own methods...
 
This example can be calculated on 1/2 page, if one does all calculations. But one have to know all trace identies and so on.

\text{Tr}(\gamma ^{\alpha}\gamma ^{\beta}) = g^{\alpha \beta}
 
Vereinsamt said:
Hi everybody!

While reading Peskin-Schroeder, i stuck in the in equation 5.4 about the unpolarized cross section of the e^- e^+ \rightarrow \mu^- \mu^+ annihilation. i didn't understand how this relationof the electron trace came to be, and where the indices came from?

\operatorname{tr}[(p\!\!/^\prime-m_e) \gamma^\mu (p\!\!/ + m_e) \gamma^\nu] = 4[p^{\prime \mu} p^\nu +p'^\nu p^\mu - g^{\mu \nu} (p \cdot p' + m^2_e)]


thanx in advanced!

Are you asking about how to get from the trace (on the left) to the final result or are you asking how one gets from a Feynman amplitude to a trace expression (in other words how the left hand side comes from)?

To get from the left side to the right side is a simple application of trace formula. Look up the equations 5.5, 5.8, 5.9 etc. Or are you asking how where those trace formula come from? (using the cyclicity of the trace operation and using identities for the product of gamma matrices does the trick)
 
yes, i just want to know how to get from the left hand side to the right hand side. the problem mabye is thas i am not familiar with traces of gamma matrices. i'll try to learn it then come with a more concrete question..
but if anybody can give some hints that helps i'll be grateful.
 
Vereinsamt said:
yes, i just want to know how to get from the left hand side to the right hand side. the problem mabye is thas i am not familiar with traces of gamma matrices. i'll try to learn it then come with a more concrete question..
but if anybody can give some hints that helps i'll be grateful.

But then it's just a matter of applying the trace formula given in equation 5.5. Just expand the expression you gave in your first post (keeping in mind that that masses simplys multiply identity matrices) and use directly the formula of 5.5. That's all there is to it.
 
Then if you want a lot of rules and properties of gamma matrices and dirac-slash notation, you can find it on many places on the internet. And their derivation. Do you know how the minkowski metric tensor works?

I am actually trying to make my own collection of formulas, and a collection of proofs. Just to have it all collected in a nice reference and TeX - practicing. If you are interessted you can send me a PM.
 
ok tell me please how to trace this thing \operatorname{tr}(\gamma^\nu\gamma^\mu p'_\mu\gamma^\mu\gamma^\nu p_\nu)? why it can't show \operatorname{tr}(\gamma^\nu\gamma^\mu p'_\mu\gamma^\mu\gamma^\nu p_\nu)? the last is what i want to ask
 
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  • #10
Vereinsamt said:
ok tell me please how to trace this thing \operatorname{tr}(\gamma^\nu\gamma^\mu p'_\mu\gamma^\mu\gamma^\nu p_\nu)? why it can't show \operatorname{tr}(\gamma^\nu\gamma^\mu p'_\mu\gamma^\mu\gamma^\nu p_\nu)? the last is what i want to ask

how did you get the same indicies on two of them? you must as general as possible, i.e:

\operatorname{tr}[(p\!\!/^\prime-m_e) \gamma^\mu (p\!\!/ + m_e) \gamma^\nu] = \operatorname{tr}[(p'_{\alpha}\gamma^{\alpha}-m_e) \gamma^\mu (p_{\beta}\gamma^{\beta}+ m_e) \gamma^\nu]

Then use the trace formula for 4 gamma matrices which I mailed you a link to.
 
  • #11
\operatorname{tr}(8p'^\nu p^\mu) - \operatorname{tr}(2mp'^\mu \gamma^\nu) + \operatorname{tr}(2m\gamma^\mu p^\nu) + \operatorname{tr}(2m^2g^{\mu\nu})
am i on the right way?
 
  • #12
no, let's take this one for instance:

\text{Tr}(p'_{\alpha}\gamma^{\alpha}\gamma^\mu p_{\beta}\gamma^{\beta} \gamma^\nu) = \text{Tr}(p'_{\alpha}p_{\beta}\gamma^{\alpha}\gamma^\mu \gamma^{\beta} \gamma^\nu) = 4p'_{\alpha}p_{\beta}(g^{\alpha\mu}g^{\beta \nu} - g^{\alpha\beta}g^{\mu\nu}+g^{\alpha\nu}g^{\mu\beta}) = ...
 
  • #13
i didn't know that we can commute p with gamma and put it out of the trace! would you tell me why we can do this?
 
  • #14
p_a is just a number, an element in a 4-vector.

p_a\gamma ^a = p_0\gamma ^0 + p_1\gamma ^1 + p_2\gamma ^2 +p_3\gamma ^3

p_0 = E

p_1 = p_x etc.
 
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  • #15
thanx for help Glenn! i'll give it another shot
 
  • #16
Vereinsamt said:
thanx for help Glenn! i'll give it another shot

np, just knock yourself out hehe, cheers
 
  • #17
ok, i have another question that should have came earlier
(p&#039;\!\!\!\!\!/ \ -m)_{da}\gamma^\mu_{ab}(p\!\!\!\!\!/ \ +m)_{bc}\gamma^\nu_{cd} <br /> =\operatorname{Tr}[(p&#039;\!\!\!\!\!/ \ -m)\gamma^\mu(p\!\!\!\!\!/ \<br /> +m)\gamma^\nu]
where the trace came from here?
 
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  • #18
Vereinsamt said:
ok, i have another question that should have came earlier
(p&#039;\!\!\!\!\!/ \ -m)_{da}\gamma^\mu_{ab}(p\!\!\!\!\!/ \ +m)_{bc}\gamma^\nu_{cd} <br /> =\operatorname{Tr}[(p&#039;\!\!\!\!\!/ \ -m)\gamma^\mu(p\!\!\!\!\!/ \<br /> +m)\gamma^\nu]
where the trace came from here?



Let's say you have three matrices A, B and C. If you are calculating the following sum:

A_{cd} B_{de} C_{ec}

this is the same as

tr(ABC)

The fact that the last index of the third matrix is the same as the first index of the first matrix means that if you work with the actual matrices, you have to multiply tham and trace the product. That's all there is to it.
 
  • #19
i'll try to prove it to make sure i got it..
thanks nrqed!
 
  • #20
http://en.wikipedia.org/wiki/Trace_(linear_algebra )
 
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