## \mu~\to e~ \gamma ## decay width and neutrino propagator

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Discussion Overview

The discussion revolves around the decay process of ## \mu \to e~ \gamma ##, specifically focusing on the derivation and implications of the neutrino propagator as presented in Cheng & Li's book "Gauge Theory of Elementary Particles." Participants are examining the mathematical expressions related to the decay width and the role of the GIM cancellation mechanism.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant questions the derivation of the neutrino propagator and its representation in terms of a sum over neutrino flavors.
  • Another participant asserts that the sum should be over neutrino masses rather than flavors, emphasizing the lack of definite masses in flavor eigenstates.
  • There is a suggestion to expand the quotient for small ##m_i## to clarify the derivation.
  • Unitarity of the mixing matrix ##U## is cited as the reason for the leading term vanishing, specifically the element ##\sum_i U^{*}_{ei} U_{\mu i}## reflecting the GIM cancellation mechanism.
  • Participants express confusion about why the first term is ignored while the second term is considered, prompting requests for a Taylor expansion example.
  • Clarification is provided that the first term is independent of the index ##i## and can be factored out of the sum, while the second term is dependent on ##i##.

Areas of Agreement / Disagreement

Participants exhibit disagreement regarding the correct interpretation of the sum in the neutrino propagator, with differing views on whether it should be over flavors or masses. The discussion remains unresolved as participants seek further clarification on the implications of the GIM mechanism and the mathematical treatment of the terms involved.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about the summation indices and the implications of the GIM mechanism, which are not fully explored or resolved.

Safinaz
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Hi all,

I'm studying ## \mu \to e~ \gamma ## decay from cheng & Lie' book " gauge theory of elementary particles ". In Equation (13.84), he wrote the neutrino propagator
## \sum_i \Big ( \frac{U^{*}_{ei} U_{\mu i}}{(p+k)^2-m_i^2} \Big), ##
(where the sum taken over neutrinos flavors) in the form:

##\sum_i U^{*}_{ei} U_{\mu i} \Big ( \frac{1}{(p+k)^2} + \frac{m_i^2}{[(p+k)^2]^2} + ... \Big) ##
##= \sum_i \frac{U^{*}_{ei} U_{\mu i} m_i^2}{[(p+k)^2]^2} + ...##

Do anyone know how did he drive this ? Then he write that:

the leading term vanishes, ## \sum_i U^{*}_{ei} U_{\mu i}##, reflecting the GIM cancellation mechanism.

I can't get this statement .. Thanks,
 
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Safinaz said:
where the sum taken over neutrinos flavors
No, the sum should be taken over the neutrino masses. The flavour eigenstates do not have definite masses.

Safinaz said:
Do anyone know how did he drive this ?

Just expand the quotient for small ##m_i##.

Safinaz said:
Then he write that:

the leading term vanishes, ## \sum_i U^{*}_{ei} U_{\mu i}##, reflecting the GIM cancellation mechanism.

I can't get this statement ..,

It follows directly from the unitarity of ##U##. It is the ##\mu##-##e## element of ##U U^\dagger = 1##.
 
Hi, thanks for replying:

Orodruin said:
Just expand the quotient for small ##m_i##.

Can you please write the general form, like for instance taylor expansion, it seems I'm not so good in math !

Orodruin said:
It follows directly from the unitarity of U. It is the ##\mu-e## element of ##U U^\dagger = 1##.

Actually this still not clear for me , ##\sum_i U^{*}_{ei} U_{\mu i} ## is multiplied by the first term ## \frac{1}{(p+k)^2} ## as well as the second term ## \frac{m_i^2}{[(p+k)^2]^2} ##, so why the first one which has been ignored .. also what's GIM mechanism and he says due to this mechanism this first leading term vanishes ..
 
Safinaz said:
Can you please write the general form, like for instance taylor expansion, it seems I'm not so good in math !

$$
\frac{1}{1+x} = 1 - x + x^2 + \ldots
$$

Safinaz said:
Actually this still not clear for me , ##\sum_i U^{*}_{ei} U_{\mu i} ## is multiplied by the first term ## \frac{1}{(p+k)^2} ## as well as the second term ## \frac{m_i^2}{[(p+k)^2]^2} ##, so why the first one which has been ignored .. also what's GIM mechanism and he says due to this mechanism this first leading term vanishes ..

The first term ## \frac{1}{(p+k)^2} ## is independent of ##i## and can be taken out of the sum. The second term is not independent of ##i##.
 
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