Particle identification in detectors

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SUMMARY

Particle identification in detectors can be achieved without magnetic fields through various methods. Key techniques include measuring Cerenkov light, utilizing time-of-flight measurements, and analyzing electromagnetic interactions in calorimeters. Electrons and muons produce distinct Cerenkov light patterns and energy loss profiles in lead-scintillator calorimeters, allowing for differentiation. Additionally, varying gas pressure in Cerenkov detectors and employing electric fields in Wien filters can further assist in identifying particle velocities.

PREREQUISITES
  • Understanding of Cerenkov radiation and its applications in particle physics.
  • Familiarity with lead-scintillator calorimeters and their energy loss characteristics.
  • Knowledge of time-of-flight measurement techniques in particle detection.
  • Basic principles of electric fields and their use in Wien filters for particle velocity detection.
NEXT STEPS
  • Research the principles of Cerenkov radiation and its role in particle identification.
  • Explore the design and functionality of lead-scintillator calorimeters in high-energy physics experiments.
  • Learn about advanced time-of-flight techniques and their applications in distinguishing particle types.
  • Investigate the use of Wien filters and their effectiveness in measuring particle velocities.
USEFUL FOR

Particle physicists, experimental researchers, and anyone involved in the design and analysis of particle detectors will benefit from this discussion.

ghery
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Hello:

Can anyone please tell me how do they identify the particles in the detectors?+, for instance, how do you know if an electron is an electron and not a muon or some other negative charged particle in a detector (without using magnetic fields)?
 
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ghery said:
for instance, how do you know if an electron is an electron and not a muon or some other negative charged particle in a detector (without using magnetic fields)?
I do not know why you would like not to use a magnetic field : it is very convenient to measure the ratio charge/momentum. Anyway, muons and electrons will give different Cerenkov light (you will need to choose the medium optical index in advance, according to the range in momentum you are interested in). If your muon is slow enough you may be able to measure the time of flight accurately enough to distinguish with an electron. Also, they produce different electromagnetic interactions in heavy material at a given incident energy (the showering process for muons in calorimeters requires much more energy than for electrons).
 
Hi ghery-
A high energy electron going into a 20-radiation-length lead-scintillator calorimeter sandwich would lose all its energy and stop. A muon of the same energy would lose only about 2 MeV per gram per cm-squared of material (Bethe-Bloch de/dx). Many years ago, I used time of flight (with 1-ns time resolution) to separate muons and pions in a low-momentum beam.
Bob S
 
ghery said:
...(without using magnetic fields)?

Two fast charged particles of the same velocity make the same ionisation traces so using some magnetic filed and other things to distinguish the particle masses and charges is important.
 
Last edited:
When I wrote "without using magnetic fields" what I really meant was if there was any other way to distinguish for example the velocity of a charged particle besides the use of magnetic fields?
 
Hi ghery-
Lead-scintillator detectors can discriminate between electrons (electromagnetic showers) muons (minimum ionizing track) and mesons and hadrons (hadronic showers). Energy can be estimated for electromagnetic and hadronic showers.
Cerenkov counters (mentioned above) can measure the Cerenkov light angle (Cerenkov ring detectors) to select the particle velocity. Varying the pressure in high-pressure gas Cerenkov detectors has been used to identify particles by varying the threshold particle velocity.
Electric fields, often in Wien filters, have been used as velocity detectors. See
http://en.wikipedia.org/wiki/Wien_filter
Particle time-of-flight (mentioned above) between two plastic scintillators or Cerenkov radiators on photomultiplier tubes has been used to select particle velocities.
Bob S
 

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