PPT-Scintillator Calorimetry for PHENIX Detector Upgrade
Author : olivia-moreira | Published Date : 2016-07-08
Ohio University Athens OH USA Uniplast Ltd Co Vladimir Russia PHENIX Calorimetery Workshop 12142010 BNL Main Idea We have done some preliminary calculationsconsiderations
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Scintillator Calorimetry for PHENIX Detector Upgrade: Transcript
Ohio University Athens OH USA Uniplast Ltd Co Vladimir Russia PHENIX Calorimetery Workshop 12142010 BNL Main Idea We have done some preliminary calculationsconsiderations for the basic parameters of a few more conventional options . Douglas Fields . PHENIX Run-15 Run Coordinator. University of New Mexico. Status of Preparations. PHENIX is still pushing hard to be ready for Run 15 start on January 27, 2015.. Pink sheeting is complete.. of Plastic Scintillator. Oct. 2, 2009. IP-BSM Group. 1. Schematic . Drawing . of. new Gamma Detector. 2. sandwich type calorimeter. SUS and plastic scintillation plate. wavelength-shifting fiber (WLSF) for light transmission. Fall, 2010 Indirect Calorimetry 1 Indirect Calorimetry Indirect Calorimetry CALORIMETRY The science that quantifies the heat release from metabolism is termed calorimetry . Figure 4.5 CALORIMETRY D IBL – . Insertable. B-Layer. Tobias Flick. University Wuppertal. 17.09.2009, VERTEX 2009 . Putten. , Netherlands. Preliminary. Overview. Current ATLAS pixel detector. What is the IBL and why do we need it?. 37. K. . Erin France. Motivation. To test the Standard Model via the correlation parameters. Measure the beta asymmetry, and compare it to the Standard Model . prediction. Beta asymmetry: the magnitude of the tendency for a beta to be emitted (anti)parallel to the nuclear spin. SuperKEKB. and Belle II Upgrades. Tom Browder. University of Hawaii . B Mesons: . “. Laboratory Rats of the Weak Interaction. ”. Exotic bound state of matter and antimatter. (hydrogen-like). b quark mass . Mickey Chiu,. f. or the PHENIX Operations Crew. Chronology of Events on 5/27. On Friday, May 27, 2016 at 02:19, all power to the PHENIX experiment was crashed. The chronology of events leading up to this has been reconstructed from the alarm logs: . Eyser. ECT* Workshop on . Drell. Yan Physics. and the Structure of Hadrons . May 21-25, 2012, Trento, Italy. RHIC as Polarized Proton Collider. AGS. LINAC. BOOSTER. Polarized Source. Spin Rotators. for the PHENIX Experiment at RHIC. Douglas Fields. University of New Mexico. Feb. 12, 2011. Douglas Fields, WWND11, Feb 12th 2011. Douglas Fields, WWND11, Feb 12th 2011. 2. . Quick PHENIX overview. Norbert Novitzky for PHENIX . collaboration. Stony Brook University. 1. 4. th. International Conference on New Frontiers in Physics, ICNFP 2015. PHENIX detector. 2. Central Arm, |. h. | < 0.35:. Tracking:. FCC week Washington. 23. -27 March . 2015. W. . Riegler. D. . Denisov. , H. . ten. Kate, L. . Lienssen. , F. . Lanni. , M. . Abbrescia. , R. Richter, Y. . Onel. , W. Smith, S. . C. hekanov. Exploration + Higgs as a tool for . Varchaswi K S Kashyap*. On behalf of NISER group. Facilities at NISER. Gas mixing system:. 5 channel gas mixing system (Freon, . iso. -butane, SF. 6. , . Ar. and CO. 2. ). Supply gas to 8 detectors simultaneously with a maximum flow rate of 50 . J. Huston. Michigan State University. Reminder. The MBTS counters were somewhat of an afterthought, with thinking/plans not started until ~2004. The idea was that it was very useful/critical to have a trigger signal for the early running of ATLAS, such that we would know which crossings had interactions (at very low luminosity). (from a module 15x15 already available ). - 15x15 cm scintillator. - read out: pair of SiPM (Advansid). - directly coupled to the scintillator without fiber. Scientific purposes:. . - long-term measurements of.
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