Muon decay in flight - distribution of distance

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Homework Help Overview

The discussion revolves around the decay of muons in flight, specifically analyzing the average lifetime of muons at rest versus their measured lifetime in a laboratory frame. Participants are tasked with graphing the distribution of distances traveled by these muons based on their decay characteristics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the time-distribution of muon decays in both the rest frame and laboratory frame, questioning the assumptions about energy distribution and the effects of time dilation on decay rates. There are discussions about expressing decay in terms of distance and the implications of using different frames of reference.

Discussion Status

The discussion is active, with participants providing hints and guidance on how to approach the problem. There is a focus on ensuring that the exponential decay function accounts for time dilation and the correct interpretation of average distances in the laboratory frame. Multiple interpretations of the decay distribution are being explored.

Contextual Notes

Some participants note the need for clarity regarding the energy distribution of the muons, which is not specified in the problem statement. There is also a recognition of the importance of correctly applying gamma factors in the calculations related to the average distance traveled by the muons.

Vrbic
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Homework Statement


The average lifetime of muons at rest is τμ0 = 2.2 μs. A laboratory measurement on the decay in flight of muons in a beam emerging from a particle accelerator yields an average lifetime of τμ = 6.6 μs, as measured in the lab frame Σ.
(g)
[3 points] Given a large ensemble of these muons, some of the muons will travel farther than others in the laboratory frame Σ. The average distance traveled is the number you found in part (f). Graph the distribution of the distances traveled in the laboratory frame Σ by this ensemble of muons. Carefully label your axes, and show both horizontal and vertical scales.

Homework Equations


Δx = βcτμ = 1881 m for average distance part (f)

The Attempt at a Solution


I'm missing some point what is happening in such ensemble. Please give me some hint. Thank you.
 
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What is the time-distribution of decays in the muon rest frame? It is the same for all radioactive decays.

Unrelated:
The problem statement should specify that all muons have the same energy, or give some information about the energy distribution if you are supposed to take the distribution into account.
 
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mfb said:
What is the time-distribution of decays in the muon rest frame? It is the same for all radioactive decays.

Unrelated:
The problem statement should specify that all muons have the same energy, or give some information about the energy distribution if you are supposed to take the distribution into account.
Oh, yes, I looked at that by no-particle eyes. There occur standard particle decay. And it is governed by decay formula. Where probability of decay is $$ f(t)=\lambda e^{-\lambda t} $$ Where ## \lambda= 1/\tau_\mu ##. But I want to express it in lenghts. So I use my formula from (f) above. So than I have
$$ f(x)=\frac{1}{\beta c \tau_\mu}e^{-\frac{x}{\tau_\mu}} $$.
Do you agree?
Because first of all I expected Gauss distribution with mean value at ## \Delta x ## and parameter ## \frac{1}{\beta c \tau_\mu} ## . But this is probably something other.
 
It is an exponential distribution. You forgot time dilation, however.
 
mfb said:
It is an exponential distribution. You forgot time dilation, however.
Heh, ok :) So, if I substitute ##t->\gamma \tau## and then result of (f) will be it alright?
$$ f(x)=\frac{1}{\gamma \tau_\mu} e^{-\frac{\tau}{\tau_\mu}}=\frac{\beta c}{\gamma \Delta x} e^{-\frac{x}{\Delta x}}$$
 
As it is a distribution, you need ##\int_0^\infty f(x) = 1##. Does that work out?

The exponential term should take time dilation into account - it needs a gamma factor somewhere.
 
mfb said:
As it is a distribution, you need ##\int_0^\infty f(x) = 1##. Does that work out?

The exponential term should take time dilation into account - it needs a gamma factor somewhere.
I did it properly, and my results is
$$f(x)= \frac{1}{\Delta x}e^{-\frac{x}{\Delta x}} $$
but important is: ##\Delta x## and ##x## is average length in laboratory frame and length in laboratory frame. ##\gamma## doesn't appear in exponent because anything is expressed in same frame.
The integral which you mentioned is 1 for this distribution.
What do you mean now?
 
Your ##\Delta x## should include a gamma-factor, as the average length in the laboratory frame depends on it.
 
mfb said:
Your ##\Delta x## should include a gamma-factor, as the average length in the laboratory frame depends on it.
Hmmm ok I'm something missing.
$$ f(t)=\frac{1}{\tau_0}e^{-\frac{t}{\tau_0}}$$ is general formula for decay (let's say in rest frame it means what see flying particlee). Where ##\tau_0 ## is mean lifetime. Also $$ f(t)=\frac{1}{\tau'_0}e^{-\frac{t'}{\tau'_0}}$$ is same formula but expressed in moving frame with respect to particle (laboratory frame). Do you agree?
If I want to express second formula (in laboratory frame) in terms of rest frame I use ##t=t'/\gamma ## (x=0) and transform also ##\tau=\tau'/\gamma## and gamma-factors are deleted each other.
Please let me now what I'm missing or what is wrong.
Thank you.
 
  • #10
The left side didn't change, therefore the right side should be identical in both expressions. It is not.
 
  • #11
mfb said:
The left side didn't change, therefore the right side should be identical in both expressions. It is not.
The second equation has wrong left side there should be ##f(t')##. Now is it right?
 
Last edited:
  • #12
Then you just changed the variable, but that is possible.

I think it is way easier to just work in the lab frame. Calculate the mean lifetime in the lab, calculate the mean length, then write down the exponential decay with this mean length, done.
 
  • #13
mfb said:
Then you just changed the variable, but that is possible.

I think it is way easier to just work in the lab frame. Calculate the mean lifetime in the lab, calculate the mean length, then write down the exponential decay with this mean length, done.
Ok. One again. ##\tau_\mu=\gamma \tau_{\mu0} ##, where ##\tau_{\mu0} ## is lifetime at rest. ##\Delta x=\beta c \tau_\mu ## is path which travel in lab frame. ## x,t## is distance and time measured in lab frame. Then
$$ f(t)=\frac{1}{\tau_{\mu} }e^{-\frac{t}{\tau_{\mu}}}dt=\frac{1}{\gamma\tau_{\mu0} }e^{-\frac{t}{\gamma\tau_{\mu0}}}dt$$
$$ f(x)=\frac{\beta c}{\Delta x}e^{-\frac{x \beta c}{\Delta x}}dx$$ Is it now ok?
 
  • #14
Correct. You can simplify it and remove new variables by plugging in your equation for ##\Delta x## and then for ##\tau_\mu##
 
  • #15
mfb said:
Correct. You can simplify it and remove new variables by plugging in your equation for ##\Delta x## and then for ##\tau_\mu##
Do you mean only this?
$$f(x)=\frac{\beta c}{\Delta x}e^{-\frac{x \beta c}{\Delta x}} dx= \frac{1}{ \tau_{\mu}}e^{-\frac{x }{\tau_{\mu}}} dx$$
 
  • #16
Something is wrong with units now (edit: also in the post before). An additional factor ##\beta c## which should not be there.
One more step and you have the muon lifetime (in its rest frame) in it instead of the effective lifetime in the lab.
 
  • #17
mfb said:
Something is wrong with units now (edit: also in the post before). An additional factor ##\beta c## which should not be there.
One more step and you have the muon lifetime (in its rest frame) in it instead of the effective lifetime in the lab.
Ok I should use ##x=\beta c t ## for ##t##. So finally? :) And thank you for patience :)
$$f(x)=\frac{1}{\beta c\gamma\tau_{\mu 0}}e^{-\frac{x}{\beta c \gamma\tau_{\mu 0}}} dx$$
 
  • #18
Looks right.
 
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