Muon lifetime measurement experiment

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SUMMARY

The forum discussion centers on the measurement of muon lifetime using a coincidence detection setup with plastic scintillators. The primary concern raised is the impact of time resolution on systematic errors in the results. The participants discuss methods for addressing this issue, including the use of the standard deviation (σ) from a Gaussian fit and the importance of Monte Carlo (MC) simulations for stability checks. The experiment utilizes three organic scintillators to detect muon events, with specific attention to the timing of signals from the decay of muons.

PREREQUISITES
  • Understanding of muon decay processes and detection methods.
  • Familiarity with coincidence measurement techniques using plastic scintillators.
  • Knowledge of Gaussian distribution and statistical analysis in experimental physics.
  • Experience with Monte Carlo simulations for data analysis.
NEXT STEPS
  • Investigate the impact of time resolution on systematic errors in particle physics experiments.
  • Learn about advanced statistical methods for analyzing Gaussian distributions in experimental data.
  • Explore Monte Carlo simulation techniques for stability checks in experimental setups.
  • Research different scintillator materials and their properties for muon detection.
USEFUL FOR

Physics students, experimental physicists, and researchers involved in particle detection and analysis, particularly those focusing on muon lifetime measurements and related systematic uncertainties.

Aleolomorfo
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How to treat time resolution as a systematic in a muon lifetime measurement?
Hello everybody!

I have a question regarding my physics laboratory at the university. I am performing the measure of muon lifetime. The setup is quite standard (coincidence measurement with plastic scintillators).
My question is about the time resolution. I have tried to see if the time resolution could affect as a systematic my result. To prove this, I have acquired only coinciding events and I measure the difference in time of such signals. Theoretically, it should be zero, but due to many factors this time intervals follow a gaussian distribution. My question is about the way in which I can take into consideration this systematic. Should I take the ##\sigma## of the gaussian fit or should I repeat the measure many times and take as systematic position drift of the coincidence peak?
 
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The best approach would be to fold the exponential function with your resolution function and then use that in the fit (plus all the other stuff needed). In practice this shouldn't matter unless your time resolution is a large fraction of the muon lifetime.
 
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Aleolomorfo said:
Summary: How to treat time resolution as a systematic in a muon lifetime measurement?

Hello everybody!

I have a question regarding my physics laboratory at the university. I am performing the measure of muon lifetime. The setup is quite standard (coincidence measurement with plastic scintillators).
My question is about the time resolution. I have tried to see if the time resolution could affect as a systematic my result. To prove this, I have acquired only coinciding events and I measure the difference in time of such signals. Theoretically, it should be zero, but due to many factors this time intervals follow a gaussian distribution. My question is about the way in which I can take into consideration this systematic. Should I take the ##\sigma## of the gaussian fit or should I repeat the measure many times and take as systematic position drift of the coincidence peak?

Hi Aleolomorfo.
Muon detection is of great interest to me as well. Would you please describe the scintillator paddle dimensions, spacing and thickness, and mention which coincidence detection scheme is being used? i.e. NIM or student built such as Dr H. Matis' design.

Thanks

George Dowell
 
geoelectronics said:
Hi Aleolomorfo.
Muon detection is of great interest to me as well. Would you please describe the scintillator paddle dimensions, spacing and thickness, and mention which coincidence detection scheme is being used? i.e. NIM or student built such as Dr H. Matis' design.

Thanks

George Dowell

Hello George Dowell,

I have attached the final report where you can find the information you need.

One thing to notice: last year the particle physics laboratory had too many students, so we were chosen to perform the measurement of the muon lifetime with electronic modules and scintillators found quickly around the university. Consequently, they were not the best ones and we had many problems... our job was not so strightforward. But you can extract the main idea behind the experiment.

If you have any question, ask freely!
 

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Thank you, nice report, well written. The first effort I've seen to capture Cosmic "Ray" muons.

As a hardware person, the difficulties with scintillators and NIM support units is well appreciated.
I liked the part about an impromptu delay line made "of many LEMO cables".

The one I'm working on now is a single 3" X 3" BGO scintillator inside an 800 pound lead shield.

George Dowell
 
Did you do the stability checks with MC? Doing it with the main dataset is problematic - if you change the analysis based on what looks better you can get some biases. It is interesting to see what looks like a systematic trend for muon lifetime as function of bins.
 
mfb said:
Did you do the stability checks with MC? Doing it with the main dataset is problematic - if you change the analysis based on what looks better you can get some biases. It is interesting to see what looks like a systematic trend for muon lifetime as function of bins.

No, we did not. We only used the dataset but I see your point, we should have used MC.
 
Aleolomorfo said:
Hello George Dowell,

I have attached the final report where you can find the information you need.

One thing to notice: last year the particle physics laboratory had too many students, so we were chosen to perform the measurement of the muon lifetime with electronic modules and scintillators found quickly around the university. Consequently, they were not the best ones and we had many problems... our job was not so strightforward. But you can extract the main idea behind the experiment.

If you have any question, ask freely!
Again thanks for the report. I have spent considerable time reading it and several others and also consulted with a moderator to get a better understanding of the aims and the procedure.
From what I see in your paper, you are using multiple organic scintillators at the same time, correct? And recording their coincidences.
In your experiment are the original pulse and the secondary pulse detected in the same scintillator or on two or more? The reason I ask is there are two approaches to working with muons using organic scintillators and I want to understand more.

Thank you.

George Dowell
 
Hello George!

geoelectronics said:
From what I see in your paper, you are using multiple organic scintillators at the same time, correct? And recording their coincidences.

Yes, we use three scintillators at the same time, one over the other. We record a start signal from the passage of a muon in the first and the second scintillator (the events we are interested in are the ones in which the muon stops in the middle scintillator). So the start signal is a coincidence between the upper and the middle scintillator. Then we expect a signal from the decay of the muon. The muon decay mainly in electron/positron and neutrino/antineutrino. We expect a signal (the charged lepton) in the upper or the lower scintillator in a gate of 10 ##\mu s##. This is the main idea.

geoelectronics said:
In your experiment are the original pulse and the secondary pulse detected in the same scintillator or on two or more?

We have always used the same three scintillator
 

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