The Role of Propagators in Determining Decay Rates

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Discussion Overview

The discussion revolves around the role of propagators in determining decay rates in particle physics, particularly in the context of electromagnetic interactions and specific decay processes like those of pions. Participants explore the mathematical representations of decay amplitudes and the implications of propagators in these calculations.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions why the propagator \(\frac{1}{q^{2}}\) is not considered when determining decay rates, suggesting that decay rates are simply proportional to the fine structure constant raised to the number of vertices.
  • Another participant clarifies that in electromagnetic interactions, the coupling constant \(g\) is equivalent to the fine structure constant.
  • There is a discussion about the integration over momentum space and the need to account for particle functions, indicating that the transition amplitude is not solely represented by the propagator function.
  • One participant mentions that the factor associated with the propagator is indeed taken into account, depending on the energy scale of the problem.
  • Concerns are raised regarding the claim that there is "no propagator" in the decay of the neutral pion, with one participant asserting that a propagator for a virtual quark exists in the diagram.
  • Another participant emphasizes that decay rates must maintain consistent dimensions across different processes, challenging the validity of certain claims made in the discussion.
  • There is a query about the role of virtual quarks in mediating processes, questioning their classification as gauge bosons.

Areas of Agreement / Disagreement

Participants express differing views on the role and presence of propagators in decay processes, particularly regarding the neutral pion decay. The discussion remains unresolved with multiple competing perspectives on the implications of propagators and decay rates.

Contextual Notes

Participants note that the discussion involves assumptions about the dimensional consistency of decay rates and the specific roles of virtual particles in decay processes, which may not be fully addressed.

vertices
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i was thinking about propagators, and I've got bit of a silly question.

The amplitude for any given decay takes the form:

f(q^{2})=\frac{g^{2}}{q^{2}+M_{X}^{2}c^{2}}.

for EMAG decays, the Mx=0 (as we're dealing with photons), so the amplitude is just:

f(q^{2})=\frac{g^{2}}{q^{2}},

Why do we not consider the propagator: \frac{1}{q^{2}} when determining decay rates (we just say its proportional to the fine structure constant to power of the number of vertices)?
 
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Hello.
In the case of EM interactions,
g IS the fine structure constant.. where's your problem ?
 
Atakor said:
Hello.
In the case of EM interactions,
g IS the fine structure constant.. where's your problem ?

thanks Atakor.

I understand that. However, the gauge boson (the carrier of the electromagnetic force), in this case a massless photon, transfers a momenmtum q. Why is the propagor 1/q^2, ignored when calculating the transition amplitude?
 
Hello vertices!
In feynman language:

to each vertex we associate the couplig constant : -ig
for each _internal_ line we associate the function you dubbed f(q)

but f(q) is not the amplitude of the transition..
we have to integrate over all momentum space (q) (with conservation of energy-momentum)
after taking into account the functions of the particles (spin 1/2 ->spinors ...)

I hope this will help you.
 
vertices said:
i was thinking about propagators, and I've got bit of a silly question.

The amplitude for any given decay takes the form:

f(q^{2})=\frac{g^{2}}{q^{2}+M_{X}^{2}c^{2}}.

for EMAG decays, the Mx=0 (as we're dealing with photons), so the amplitude is just:

f(q^{2})=\frac{g^{2}}{q^{2}},

Why do we not consider the propagator: \frac{1}{q^{2}} when determining decay rates (we just say its proportional to the fine structure constant to power of the number of vertices)?


We do take that factor into account! Do you have any specific example to discuss? That factor will be there with q having the value of some energy scale in the problem (of order the mass of the decaying particle).
 
nrqed said:
We do take that factor into account! Do you have any specific example to discuss? That factor will be there with q having the value of some energy scale in the problem (of order the mass of the decaying particle).

Yes, as it happens I do. Please look at the attached files which consider the decays of the pi and pi- mesons. The bit I have highlighted bit in the file "Propagator 2", basically says that, in the case of the neutral pion, which decays electromagnetically, "there is no propagator". I don't get this!
 

Attachments

A propagator is used when a virtual particle propagates from one vertex to another. In the decay of the pi0, there are no virtual photons, so there are no photon propagators. In decays where you do have a virtual photon, e.g. J/\psi \rightarrow \mu^+ \mu^-, you have a photon propagator.
 
Vanadium 50 said:
A propagator is used when a virtual particle propagates from one vertex to another. In the decay of the pi0, there are no virtual photons, so there are no photon propagators. In decays where you do have a virtual photon, e.g. J/\psi \rightarrow \mu^+ \mu^-, you have a photon propagator.

i see. thanks for your reply Vanadium:)
 
vertices said:
Yes, as it happens I do. Please look at the attached files which consider the decays of the pi and pi- mesons. The bit I have highlighted bit in the file "Propagator 2", basically says that, in the case of the neutral pion, which decays electromagnetically, "there is no propagator". I don't get this!

If you look at the Feynman diagram, you will see that there is no gauge boson propagator (no photon propagator or W or Z boson propagator) involved in the neutral pion decay.

However, this is not the end of the story. And the excerpts you provided don't make much sense. You see right away that what they say does not make sense because a decay rate must always have the same dimensions no matter what process is computed. They seem to say that in one case the decay rate goes like 1/M^4 and in the other case it is dimensionless. This is clearly nonsense.

two things are missing to the discussion. First, in the charged pion decay there will be spinor factors coming from the outgoing fermions taht are being produced. These will provide additional dimensionful factors that must be taken into account. These will produce an additional factor with dimension of energy.

Also, in the neutral pion decay there is a propagator in the diagram: it's the propagator of the virtual quark between the two photon vertices! This must be taken into account as well. This wil produce a factor of dimension E^{-1}. This way the two diagrams will have the same dimensions (I am setting aside the factors coming from the initial quarks which are presumably of the same order in both diagrams so if we are taking a ratio of the two diagrams we don't have to think about those).

What is the source of those excerpts you provided. I hope it's not the book by D McMahon!
 
  • #10
nrqed said:
However, this is not the end of the story. And the excerpts you provided don't make much sense. You see right away that what they say does not make sense because a decay rate must always have the same dimensions no matter what process is computed. They seem to say that in one case the decay rate goes like 1/M^4 and in the other case it is dimensionless. This is clearly nonsense.

Yes indeed it is, thanks for pointing that out!

Also, in the neutral pion decay there is a propagator in the diagram: it's the propagator of the virtual quark between the two photon vertices! This must be taken into account as well. This wil produce a factor of dimension E^{-1}. This way the two diagrams will have the same dimensions (I am setting aside the factors coming from the initial quarks which are presumably of the same order in both diagrams so if we are taking a ratio of the two diagrams we don't have to think about those).

aahhh. didn't think of that. here comes a really stupid question - a virtual quark isn't a gauge boson, so how does it/why can it mediate the process in question?

What is the source of those excerpts you provided. I hope it's not the book by D McMahon!

Its "Nuclear and Particle Physics" by Brian Martin. I can overlook its complacency/lack of rigour because it does explain concepts quite well:)
 

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