What Is the Momentum of an Electron in Muon Decay?

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Homework Help Overview

The discussion revolves around the momentum of an electron produced in the decay of a muon, which has a rest energy of 105.7 MeV and is moving at a speed of 0.994c. Participants explore the implications of conservation of momentum and energy in this context, particularly focusing on the interactions between the electron and a photon produced during the decay.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the conservation of momentum and energy, with some attempting to relate the energies and momenta of the electron and photon. There are questions about the use of four-vectors and the implications of treating the muon at rest. Some participants express uncertainty about how to apply certain equations and whether the energy is split evenly between the electron and photon.

Discussion Status

The discussion is ongoing, with participants offering guidance on relevant equations and concepts. There is a recognition of the complexity involved in the problem, and various interpretations of the energy distribution between the electron and photon are being explored.

Contextual Notes

Some participants note a lack of familiarity with four-vectors, which may be impacting their ability to engage fully with the problem. There is also mention of the need to clarify assumptions regarding the energy distribution in the decay process.

tib
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Homework Statement



Unstable, subatomic particles called muons have a rest energy of 105.7 MeV and a speed of 0.994c. If a muon were to decay and produce an electron and a photon, what would be the momentum of the electron as measured by an observer in the muon's frame? HINT: assume that the electro goes in the +x direction, the photon goes in the -x direction, and the muon is at rest in its own frame.


Homework Equations



E = mc^2 + K; p = gamma*m*v; numerous other forms of relativistic energy equations

The Attempt at a Solution



By the hint, (muon is at rest) we can assume that the initial momentum is zero. By conservation of momentum, initial momentum = final momentum thus, momentum of the electron = momentum of the photon.

This is as far as I can get. The posted answer is 52.8 MeV/c.
 
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You need to conserve total energy as well.

Do you know how to use four-vectors?
 
i do not know how to use four-vectors
 
OK, no problem. So far you have

0 = pe-pγ

What equation do you get from conservation of energy?

EDIT: Some advice: write it in terms of Ee, Eγ, and any relevant masses.

Also, the subscript γ is meant to label the energy and momentum of the photon; it's not the gamma that shows up in the relativity equations.
 
Last edited:
if we treat the muon at rest, Ei=Emuon=Eo=105.7 MeV

Ef=Ee+Eγ

I know Eγ=hf, but I feel like that's going in the wrong direction for the problem; also I know Ee=γmec2, but without the Eγ, I feel that's a deadend as well.
 
tib said:
if we treat the muon at rest, Ei=Emuon=Eo=105.7 MeV
Right. I'd just write it as Ei=mμc2. It's easier to plug the numbers in at the end.
Ef=Ee+Eγ

I know Eγ=hf, but I feel like that's going in the wrong direction for the problem; also I know Ee=γmec2, but without the Eγ, I feel that's a deadend as well.
Yeah, generally, you want to solve for energies and momenta directly. Throwing in things like gamma, velocity, and frequency just complicate the algebra.

One of the most useful relations you have for these types of problems is

(mc^2)^2 = E^2 - (pc)^2

So the idea is to rearrange the terms in the equations slightly, then square both equations, subtract one from the other, and use this relation to simplify the result.
 
I can see where I (think) I should go, by the equation you gave and by knowing the actual answer, I can see I find p=E/2c. If this is correct, we know by conservation of momentum that pe=pgamma; how do we know that the energy of the muon is split equally between the electron and photon?

Additionally, I still don't see the math to get to p=E/2c; using (mc2)2=E2-(pc)2 for the Ei; the result is 0=-(pc)2, because E=Eo=mc2 -- which does make sense, but isn't useful

And for Ef, photons are massless, but have momentum, so I don't see how to apply that equation to Ef.
 
The energy isn't split evenly between the electron and photon.

The relation (mc2)2=E2-(pc)2 is good for each particle, so for the electron, you'd have (mec2)2=Ee2-(pec)2. The photon has no rest mass, so the relation reduces to 0=Eγ2-(pγc)2, or Eγ=|pγ|c.
 
tib said:
i do not know how to use four-vectors

It is easy to learn.

Also, note that the energy is split approximately evenly between the photon and electron, as a result of the electron being extremely relativistic.
 

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