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                                 Abstract:Detailed measurements of Hamamatsu R5912 photomultiplier signals are presented, including the single photoelectron charge response, waveform shape, nonlinearity, saturation, overshoot, oscillation, prepulsing, and afterpulsing. The results were used to build a detailed model of the PMT signal characteristics over a wide range of light intensities. Including the PMT model in simulated Daya Bay particle interactions shows no significant systematic effects that are detrimental to the experimental sensitivity.
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                        References
	
			| [1] | GUO X et al. (Daya-Bay collaboration). arXiv:hep-ex/ 0701029[2] LIU D. PMT Evaluation for the Daya Bay Neutrino Experiment, Nuclear Science Symposium Conference Record, 2008. NSS '08. IEEE, 3133-3139[3] Dossi R, Ianni A, Ranucci G, Smirnov O Y. Nucl. Instrum. Methods A, 2000, 451: 623[4] Coates P B. J. Phys. D: Appl. Phys., 1973, 6: 153[5] Bellamy E H et al. (SDC collaboration). Nucl. Instrum. Methods A, 1994, 339: 468-476[6] Photomultiplier Tubes: Basics and Applications. Third Edition. Hamamatsu, 2006[7] Zbiri K. Simplified PMT Model. arXiv:0809.4210 [physics.ins-det][8] JIANG W, GU S, Joseph J, LIU D et al. Chin. Phys. C (HEP  NP), 2012, 36(3): 235 |  
 
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