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M. Joos, PH/ESE 1 A simple Muon-Detector Scintillator Photomultiplier Light guide HV (2000 V) Discriminator Coincidence Counter NIM electronics Discriminator V t M u on tr ac e

A simple Muon -Detector

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A simple Muon -Detector. Muon trace. t. V. Scintillator. Light guide. HV (2000 V). Discriminator. Discriminator. Coincidence. Counter. Photomultiplier. NIM electronics. Scintillators in LHC experiments Example: ATLAS Tile calorimeter. Light guides. Photomultipliers. - PowerPoint PPT Presentation

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Page 1: A simple  Muon -Detector

1M. Joos, PH/ESE

A simple Muon-Detector

Scintillator

Photomultiplier

Light guideH

V (2

000

V)

Dis

crim

inat

or

Coin

cide

nce

Coun

ter

NIM electronics

Dis

crim

inat

or

V

t

Muo

n tr

ace

Page 2: A simple  Muon -Detector

2M. Joos, PH/ESE

Scintillators in LHC experimentsExample: ATLAS Tile calorimeter

Page 3: A simple  Muon -Detector

3M. Joos, PH/ESE

Light guides

Page 4: A simple  Muon -Detector

4M. Joos, PH/ESE

Photomultipliers

Reasons for noise:• Thermal electrons (dark current)• Light leaks

Page 5: A simple  Muon -Detector

5M. Joos, PH/ESE

Computing the number of photonscreated by the muon in the scintillator

Step1: Compute the number of electrons given by the PMTU = R * IQ = I * tResistance: 50 Ω1 Coulomb = 1 As = 6.24150965×1018 electrons

Therefore: Q = U * t / RFor a triangle: Q = U * t / 2 * R

Step 2: Properties of the PMTAdditional parameters:Electron amplification of the PMT: VE = ~106 Efficiency of the Photo-Cathode: EP = 0.1

Number of photons generated by a muon crossing the scintillator:

Nphoton = (U * t * 6.24 * 1018) / (2 * R * VE * EP)Nphoton = (U * t * 3.12 * 1014) / R

V

t

Sensitivity of the human eye: http://en.wikipedia.org/wiki/Rod_cell

Literature: 20.000 photons / cm

Page 6: A simple  Muon -Detector

6M. Joos, PH/ESE

A bit of mathematics (without formulas)

Random Coincidences

Discriminator 1

Discriminator 2

Coincidence module

Noise signals Muons or noise?

Muon? Muon?

• How likely is the overlapping of noise pulses on the two channels?• What parameters does the formula depend on?• How does the formula look like?

• How can we measure the rate of random coincidences with our set-up?

Page 7: A simple  Muon -Detector

7M. Joos, PH/ESE

What can be measured with our detector?

• Muon rate• Are there less muons inside of a building (due to shielding) than outside?• Does the muon flux depend on the time of day?

• Angular distribution of the muons• Muon life time (would require third PMT or a bigger scintillator)

• A muon that decays produces a signal with a higher amplitude than that of a muon that just crosses the scintillator

• Muon velocity (would required precise clock)• Other sources of radiation (e.g. beta decay)

Page 8: A simple  Muon -Detector

8M. Joos, PH/ESE

Application: Volcano-Tomography