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Preliminary Results of the Test Run at SLAC. Petra Hüntemeyer. This analysis based on. two weeks of data taking or 707 runs each with between 2500 to 5000 recorded ‘events’ or ï¾ 2 million recorded ‘events’ gas fillings: air, nitrogen, air-nitrogen mixtures, ethylene
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Preliminary Results of the Test Run at SLAC Petra Hüntemeyer
This analysis based on ... • two weeks of data taking • or 707 runs each with between 2500 to 5000 recorded ‘events’ • or 2 million recorded ‘events’ • gas fillings: air, nitrogen, air-nitrogen mixtures, ethylene • pressures between 3 and 760 torr • readout from one of two PMTs
Analysis variables are... • gas type/mixture • pressure • gas flow bit • beam charge • signal in the signal tubes • signal in the blind tubes • HV applied to the PMT
First Pass Data • Signal PMT
First Pass Data • Signal PMT
First Pass Data • Signal PMT
First Pass Data • Signal PMT
Corrected Signal • Scorr = Sraw - Pave - f eth S blind • S raw : raw signal • Pave : average pedestal • S blind : blind tube signal • f eth : factor from Sraw / Sblind ethylene runs
Linear Region • Definition of a range where signal vs beam charge behavior is linear
Yield Calculation Y = Scorrfconv / bc acc / sen • Scorr : corrected signal [ADC counts] • fconv : conversion factor, ADC counts to pC • bc : beam charge [ e-] • acc : geometrical acceptance • sen : sensitivity from calibration folded with Bunner • spectrum
How does this compare with earlier measurements? • Kakimoto et.al, • Nucl. Inst. And • Meth. A372 527 • (1996) • Preliminary result • from this test run • @ 28.5 GeV: • 5-6 photons • per m per e-
Analysis Conclusions • promising preliminary results from a first look at the data • a large amount of data collected during test run remains to be analyzed and more detailed systematic studies have to be performed • insights from test run and analysis serve as input for the preparation of the anticipated experiment at SLAC
Conclusions • purpose of T461: test run for a more sophisticated experiment proposed at SLAC • we observed PMT signals in coincidence with the beam whose features are consistent with fluorescence • the enhancement of the pure nitrogen signal over that in air is consistent with what we expect from earlier fluorescence measurements • we observed a non-linear behavior of the fluorescence signal versus beam charge in the excess of 2 109 e- • we also observed a linear behavior below 109 e- • a study of the blind tubes indicates that the beam halo related backgrounds are relatively small