Simplifying an expression given (on-shell & off-shell) conditions

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Discussion Overview

The discussion revolves around simplifying an expression related to unpolarized cross-sections in quantum field theory, specifically under on-shell and off-shell conditions. Participants explore the steps involved in simplifying a complex expression and clarify the notation used in scalar products of four-vectors.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents an expression for simplification and outlines their steps, noting discrepancies with a provided solution.
  • Another participant points out potential confusion in the notation used for scalar products and suggests clearer representation of vector contractions.
  • Further clarification is provided regarding the use of dot notation for scalar products, with emphasis on its importance for avoiding ambiguity.
  • A participant revisits the expression using dot notation and begins to work through the calculations again, seeking validation of their approach.
  • One participant expresses approval of the revised notation and approach, indicating progress in the discussion.

Areas of Agreement / Disagreement

Participants generally agree on the need for clearer notation in the expression, particularly regarding scalar products. However, the simplification of the expression itself remains unresolved, with differing interpretations of the calculations presented.

Contextual Notes

There is an emphasis on the importance of notation in mathematical expressions, particularly in the context of quantum field theory. The discussion highlights the potential for misinterpretation when scalar products are not clearly indicated.

Who May Find This Useful

This discussion may be useful for students and practitioners of quantum field theory, particularly those interested in the mathematical aspects of cross-section calculations and the importance of notation in vector operations.

JD_PM
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TL;DR
I want to understand how to get Eq. 8.71a in Mandl & Shaw
I was studying how to compute an unpolarized cross-section (QFT Mandl & Shaw, second edition,https://ia800108.us.archive.org/32/items/FranzMandlGrahamShawQuantumFieldTheoryWiley2010/Franz%20Mandl%2C%20Graham%20Shaw-Quantum%20Field%20Theory-Wiley%20%282010%29.pdf) and came across the following expression

$$Z:=16 \{ 2(f_1p)(f_1p') -f_1^2(pp')+m^2[-4(pf_1)+4f_1^2]+m^2 [(pp')-4(f_1 p')] +4m^4 \} \tag 1$$

Where:

$$f_1:=p+k \tag 2$$

We're also given the on-shell and off-shell conditions:

$$p^2 = p'^2=m^2, \ k^2=k'^2=0, \ pk=p'k', \ pk'=p'k \tag 3$$

Plugging ##(2)## into ##(1)## I get (I include all steps so that we can find the mistake)

$$Z=16\{2(p+k)p(p+k)p'-(p+k)^2(pp')+m^2[-4p(p+k)+4(p+k)^2]+m^2[(pp')-4(p+k)p']+4m^4\} \tag 4$$

Expanding out ##(4)## I get

$$Z=16\{ 2p^3p'+2kpkp'+2p^2kp'+2kp^2p'-p^3p'-2pkpp'-k^2pp'-4m^2p^2-4m^2pk+4m^2p^2+8m^2pk+4m^2k^2+m^2pp'-4m^2pp'-4m^2kp'+4m^4\} \tag 5$$

Now it is about simplifying ##(5)##. I'll go step by step.

I first used ##k^2=k'^2=0##, ##p^2 = p'^2=m^2## conditions to get

$$Z=16\{ 2p^3p'+2kpkp'+2p^2kp'+2kp^2p'-p^3p'-2pkpp'-4m^2pk+8m^2pk+m^2pp'-4m^2pp'-4m^2kp'+4m^4\} \tag 6$$

Then I simplified ##Xm^2kp'##, ##Ym^2pp'## terms and got

$$Z=16\{ +4m^2(pk) -2m^2pp'+4m^4+2kpkp'-2pkpp'\} \tag 6$$

Mmm but this is not the provided solution

$$Z=32\{m^4+m^2(pk)+(pk)(pk')\}$$

At least I got ##m^4## and ##m^2(pk)## right but I got the extra term ##-2m^2pp'## and did not get ##(pk)(pk')##. Actually, if the term ##-p^3p'## in ##(5)## were to be positive, ##Xm^2kp'## would cancel out but it is not the case.

Where did I get wrong then?

Any help is appreciated.

Thank you.

PS: I asked it https://math.stackexchange.com/questions/3702158/simplifying-an-expression-given-certain-on-shell-off-shell-conditions but got no answer.
 
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I don't have the time to go through all of this, but note that it is very confusing (possibly also to yourself) that you do not make clear which vectors are multiplied in a scalar product and which scalar products are then just multiplied as numbers. For example, your fourth term in (4), ##kp^2p^\prime##, if I identified it correctly, should read ##(k\cdot p)(p\cdot p^\prime)##, which is not equal to ##k(p^2)p^\prime = m^2 (k\cdot p^\prime)##. I suggest to go through the calculation again making sure to mark scalar product between vectors and products between numbers separately.
 
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Dr.AbeNikIanEdL said:
I don't have the time to go through all of this, but note that it is very confusing (possibly also to yourself) that you do not make clear which vectors are multiplied in a scalar product and which scalar products are then just multiplied as numbers. For example, your fourth term in (4), ##kp^2p^\prime##, if I identified it correctly, should read ##(k\cdot p)(p\cdot p^\prime)##, which is not equal to ##k(p^2)p^\prime = m^2 (k\cdot p^\prime)##. I suggest to go through the calculation again making sure to mark scalar product between vectors and products between numbers separately.
Dr AbeNikIanEdl is absolutely right. I had the same reaction when reading your post. One must indicate which four-vectors are contracted and the most used convention is to use a dot symbol. Otherwise something like ##pkpk'## is ambiguous. But I notice that Mandl and Shaw do not use a dot, which is probably why you started writing things this way. However, note that Mandl and Shaw still indicate clearly what four vectors are contracted, although it might be easy to miss. Note that whenever two four-vectors are contracted, they are placed inside a parenthesis. For example they might write ##(pk)(pk')##. So they still show clearly which ones are contracted, but the dot notation is more widely used now.
 
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nrqed said:
Dr AbeNikIanEdl is absolutely right. I had the same reaction when reading your post. One must indicate which four-vectors are contracted and the most used convention is to use a dot symbol. Otherwise something like ##pkpk'## is ambiguous. But I notice that Mandl and Shaw do not use a dot, which is probably why you started writing things this way. However, note that Mandl and Shaw still indicate clearly what four vectors are contracted, although it might be easy to miss. Note that whenever two four-vectors are contracted, they are placed inside a parenthesis. For example they might write ##(pk)(pk')##. So they still show clearly which ones are contracted, but the dot notation is more widely used now.

Oh I did not know that the dot notation was more widely used, thanks for informing.

So let's go step by step

Using the dot notation on ##(1)## we get

$$Z:=16 \{ 2(f_1 \cdot p)(f_1 \cdot p') -(f_1 \cdot f_1)(p \cdot p')+m^2[-4(p \cdot f_1)+4(f_1 \cdot f_1)]+m^2 [(p \cdot p')-4(f_1 \cdot p')] +4m^4 \} \tag 1$$

Now let's work out the term ##(f_1 \cdot p)(f_1 \cdot p')## as an example; I get

$$(f_1 \cdot p)(f_1 \cdot p')=\Big((p+k)\cdot p\Big)\Big((p+k)\cdot p'\Big)=\Big(m^2+p\cdot k\Big)\Big(p\cdot p' + p'\cdot k\Big)$$ $$=m^2(p\cdot p')+(p\cdot k)(p'\cdot k)+m^2(p'\cdot k)+(p\cdot k)(p\cdot p')$$

Is this the way to go then?
 
Looks good to me now.
 
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