2000
DOI: 10.1007/bf02759066
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CsI(Tl)-calorimeter calibration with positive-kaon decay products

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Cited by 4 publications
(2 citation statements)
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“…The photon detector covers a solid angle of 3π steradians, with openings for the beam entry and exit and 12 holes for charged particles to pass into the magnet gaps. The photon energy was obtained by summing the cluster energy distributed among several crystals surrounding a central 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 11 11 11 11 11 11 11 11 11 11 11 11 000000 000000 000000 000000 000000 000000 000000 were obtained in the experiment [6,9]. The study of the K e3 decay required a trigger condition different from that of the main experiment.…”
Section: Methodsmentioning
confidence: 99%
“…The photon detector covers a solid angle of 3π steradians, with openings for the beam entry and exit and 12 holes for charged particles to pass into the magnet gaps. The photon energy was obtained by summing the cluster energy distributed among several crystals surrounding a central 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 00 11 11 11 11 11 11 11 11 11 11 11 11 000000 000000 000000 000000 000000 000000 000000 were obtained in the experiment [6,9]. The study of the K e3 decay required a trigger condition different from that of the main experiment.…”
Section: Methodsmentioning
confidence: 99%
“…The events in which no energy was detected in the neighboring crystals were selected to obtain the individual gains of CsI modules. The kaon decay vertex was reconstructed from µ + tracking and muon energy losses in the target were corrected using the target fiber ADC information [11]. Using individual CsI calibration coefficients the decay K + → π + π 0 is reconstructed.…”
Section: In-beam Calibrationmentioning
confidence: 99%