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Noise Simulation on RPCs

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Noise Simulation on RPCs. Andrés Leonardo Cabrera Mora High Energy Physics Group Universidad de los Andes. ¿ What we are simulating ?. Resistive Plate Chambers. Geometry. First Aproximation. Polyethylene (0.2 mm) Graphite (0.2 mm) Bakelite (2 mm) Gas C 2 H 2 F 4 (2 mm) - PowerPoint PPT Presentation
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Noise Simulation on RPCs Andrés Leonardo Cabrera Mora High Energy Physics Group Universidad de los Andes
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Page 1: Noise Simulation on RPCs

Noise Simulation on RPCs

Andrés Leonardo Cabrera MoraHigh Energy Physics GroupUniversidad de los Andes

Page 2: Noise Simulation on RPCs

¿What we are simulating?

Resistive Plate Chambers

Page 3: Noise Simulation on RPCs

Geometry

• Polyethylene (0.2 mm)• Graphite (0.2 mm)• Bakelite (2 mm)• Gas C2H2F4 (2 mm)• Aluminum (strips)(0.04

mm)• Air• Localized Electric Field

(4.5 kV/mm)

FIRST APROXIMATION

Page 4: Noise Simulation on RPCs

Implementation

• Particles: photons, electrons, positrons, muons and antimuons.

• Processes: Compton Scattering, Photo Electric Effect, Gamma Conversion, Multiple Scattering, Ionization, Bremsstrahlung, Positron Annihilation and Pair Production.

• Results: Histograms, Scatter Plots, Angles Distribution and Distance Distribution.

Page 5: Noise Simulation on RPCs

Conditions on the Simulation

• Incidence of ten millions of muons through a Double RPC (perpendicular, fixed point)

• Localized field in the region of the gas-4.5 kV/mm in the z axis (negative)

• The results show electrons that come from photons in the gas region

Page 6: Noise Simulation on RPCs

RESULTS

Page 7: Noise Simulation on RPCs

Counts

Distance Distribution X (cm)

Electron Distance Distribution

Page 8: Noise Simulation on RPCs

Counts

Energy Distribution (MeV)

Electron Energy Distribution

Page 9: Noise Simulation on RPCs

Angular Distribution

Z (positive)

Cos (Ѳ) = 1 Cos (Ѳ) = -1

Page 10: Noise Simulation on RPCs

Counts

Cos (Ѳ) Distribution

Electron Cos (Ѳ) Distribution

Page 11: Noise Simulation on RPCs

Counts

Φ Distribution (Deg)

Electron Φ Angular Distribution

Page 12: Noise Simulation on RPCs

X (mm)

Y (mm)

Scatter Plot Y vs X

Page 13: Noise Simulation on RPCs

OTHER RESULTS

Page 14: Noise Simulation on RPCs

Positive Electric Field

(4.5 kV/mm en la dirección positiva del eje z)

Page 15: Noise Simulation on RPCs
Page 16: Noise Simulation on RPCs

Negative Electric Field

(4.5 kV/mm en la dirección negativa del eje z)

Page 17: Noise Simulation on RPCs
Page 18: Noise Simulation on RPCs

RPC with Iron

Page 19: Noise Simulation on RPCs

RPC with aluminium

Page 20: Noise Simulation on RPCs

Change in the incidence of particles

• Distribution of energies • Incidence from different angles and points.

Page 21: Noise Simulation on RPCs

Manage of Information• Twiki in english/spanish

http://twiki.org/cgi-bin/view/Sandbox/AndresCabreraSandbox

Page 22: Noise Simulation on RPCs

Conclusions• The incidence of ten millions of muons

produce a 0.09% (9242) of electrons that come from photons.

• Only 0.09% (9) of electrons are produced to more than 10 cm of the point of incidence.

Page 23: Noise Simulation on RPCs

Conclusions

• Only 2.7% (257) electrons are produced to more than 2.4 cm (1.2 cm) of the point of incidence.

Page 24: Noise Simulation on RPCs

Counts

Distance Distribution X (cm)

Electron Distance Distribution


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