Design and performance tests of the CDF time-of-flight system

Ch. Paus,C. Grozis,R. Kephart,R. Stanek, B. Kim, D.H. Kim, S.B. Kim,Y. Oh, I. Yu,W. Carithers,Y.K. Kim,K. Anikeev,G. Bauer, I.K. Furić, A. Korn,I. Kravchenko, M. Mulhearn,S. Pavlon, K. Sumorok,S. Cabrera, T. Rodrigo,A. Ruiz,I. Vila,C. Chen,M. Jones,W. Kononenko, J. Kroll,G.M. Mayers,F.M. Newcomer,D. Usynin,R. VanBerg, G. Bellettini,C. Cerri, A. Menzione,D. Depedis, C. Dionisi,S. Giagu, M. Rescigno, L. Zanello,A. Kazama, S.H. Kim, H. Matsunaga,S. Motohashi,K. Sato,K. Takikawa,F. Ukegawa

NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT(2001)

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摘要
The CDF II detector contains a time-of-flight detector consisting of 216 scintillator bars of 279cm length and 4 x 4 cm(2) cross-section located at a radius of 138 cm from the beam asis. The bars are installed on the inner surface of the CDF solenoid, which produces all axial field of 1.4 T. Nineteen-stage fine-mesh photomultiplier tubes are attached at both ends of the scintillator bars. Photostatistics limit the time-of-flight resolution, which is expected to be 100 ps. The primary physics motivation is K+/- identification for improved neutral B meson flavor determination. (C) 2001 Elsevier Science B.V. All rights reserved.
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time of flight,cross section
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