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Description of the HADES RICH OEM Measurement Single Photon Response N 0 Calculation Summary. Photon Detection Efficiency in the CsI-based HADES RICH. The RICH Detector. C + C @1 AGeV. Lepton Rings. Photon Detector : CH 4 MWPC CsI cathode 28.600 pads 10 m s readout. - PowerPoint PPT Presentation
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RICH 2002 L. Fabbietti (TU-München)
Photon Detection Efficiency in the Photon Detection Efficiency in the CsI-based HADES RICHCsI-based HADES RICH
• Description of the HADES RICH
• OEM Measurement • Single Photon Response
• N0 Calculation
• Summary
RICH 2002 L. Fabbietti (TU-München)
The RICH DetectorThe RICH Detector
Photon Detector :• CH4 MWPC• CsI cathode• 28.600 pads• 10 s readout
C + C @1 AGeV
Lepton Rings
Single Photon Response is CRUCIAL
RICH 2002 L. Fabbietti (TU-München)
pad plane
tank
window
mirror
tank shell
target
radiator gas
detector gas
beam
field plane
photon detector
Efficiency CalibrationEfficiency Calibration(Online Efficiency Measurement (OEM))(Online Efficiency Measurement (OEM))
Photons produced by 600 AMeV 12C beam particles passing two
different solid radiators
beam
Calibrated light source !
n() -> C()
1
0.8
0.6
0.4
0.2
0.0 120 140 160 180 200 220
SiO2
MgF2Tra
nsm
issi
on
[nm]
RICH 2002 L. Fabbietti (TU-München)
OEM RadiatorOEM Radiator
2cm
beam
beam line
RICH 2002 L. Fabbietti (TU-München)
single 12C hit
beam pipe shadow
Single Particle ResponseSingle Particle Response
Nph ~ N0 * Z2100 evt accumulated
MgF2
SiO2
RICH 2002 L. Fabbietti (TU-München)
Single Photon
Pattern
Single Photon Response of Single Photon Response of MWPCMWPC
Pad X Coordinate
Pad
Y C
oord
inat
e
Pul
se H
eigh
t
–Photon Candidates : Local Maxima in an isolated 3X3 Pattern
–Single Pads below Threshold (4 and Charge Particle are cleaned
1 Event
Q Mean = 7 * 10 4 e-
SE ~ 90%
wires
6 mm
6 m
m
RICH 2002 L. Fabbietti (TU-München)
Coupling to Neighbouring PadsCoupling to Neighbouring Pads
Along the wire
photon impact resolution ~ 0.5 mm
Perpendicular to wire
RICH 2002 L. Fabbietti (TU-München)
Charge Distribution of Single Charge Distribution of Single PhotonsPhotons
Simulation
Experiment
single photon response
well understood
RICH 2002 L. Fabbietti (TU-München)
OEM Analysis OEM Analysis
Experimental Data Simulation Input (HGeant)(HGeant)
– Optical parameters (all independently measured)
– Simulation of single photon response
– Electronic noise
N0=102100 Events
Beam pipe shadow
C@600 AMeV
RICH 2002 L. Fabbietti (TU-München)
–150 nm
205
nm
205
nm
145
nm
163
nm
Wave Length Resolved Efficiency Wave Length Resolved Efficiency
MgF2
Radiator
Simulation
ExperimentSector 2
SIO2
Radiator
MgF2 SiO2
RICH 2002 L. Fabbietti (TU-München)
NN00 Calculation Calculation
4 .
( ) ( ) ( ) ( )
R ( ) ( )
i Gas CsI Windowi
Mirror CH Se
T QE T
T
2
04 10
1
2. ( ) ( ) ( )Exp SimC F i
i
dN const T R
Translation to HADES C4F10 Radiator
RICH 2002 L. Fabbietti (TU-München)
NN0 0 ResultsResults
Sector 1
MgF2 SiO2
Sector 2
MgF2 SiO2
Sector 3 MgF2 SiO2
Sector 6
MgF2 SiO2
102 102 102 102 102 102 102 102
82 114 97 102 94 122 102150
??
Experimental Results extracted from the April 2002 data: C @ 600 AMeV
RICH 2002 L. Fabbietti (TU-München)
• We have developed a powerful online efficiency measurement for the HADES Rich detector.
• The analysis of the single photon response has allowed to develop an heuristic model for the simulations.
• The quantitative comparison between experimental and simulated data enables an estimation of the figure of merit N0 for each sector of the HADES RICH detector.
• The OEM measurement is going to be repeated during the next experiment, to monitor the time evolution of the detector efficiency.
Conclusions and OutlookConclusions and Outlook
Munich RICH group :T.Christ, T.Eberl, L.Fabbietti, J.Friese, R. Gernhaeuser, L.Maier, B.Sailer and S.Winkler.