PPT-PHENIX results on the anisotropic flow of thermal photons

Martin L Purschke BNL for the PHENIX Collaboration What youll hear Quick rehash of recent published results on direct photon yields New ingenious method to extend the former low p T. Yuan Li. Advisor: Greg Bryan. Department of Astronomy, Columbia . University. July 2011. The Cooling Flow Problem. In Cool-Core Clusters: . t. cool. . << Hubble Time. Steady state => Cooling flow. Time Meeting, 1/26/2010. Stefan Bathe. 01/26/2010. Stefan Bathe for PHENIX, Time Meeting. 1. Sampled Integrated Luminosity. 01/26/2010. Stefan Bathe for PHENIX, Time Meeting. 2. DAQ Performance. 01/26/2010. Tripp Winters . Anisotropy is a common feature in water laid sedimentary deposits (fluvial, . clastic. lake, deltaic and glacial outwash). . Water lain deposits may exhibit anisotropy on the horizontal plain (X,Y if looking down from above). Time Meeting, . 3/09/2010. Stefan Bathe. 03/09/2010. Stefan Bathe for PHENIX, Time Meeting. 1. Past Week History. 03/09/2010. Stefan Bathe for PHENIX, Time Meeting. 2. Had to swap HV mainframe for DC E Wednesday night: lost 10 h of beam. Chatterjee. Variable Energy Cyclotron . Centre, Kolkata. Elliptic Flow of Electromagnetic Radiation & . Thermalization. Time @ RHIC. Collision of heavy nuclei at relativistic energies leads to formation of Quark- Gluon Plasma (QGP). Takao . Sakaguchi. Brookhaven National Laboratory. Serious Preface. Discovery and quantification are both important and should go along. Mandatory condition as far as I think, in order to expand a field (and get budget). Status and Hungarian activities. M. Csanád for PHENIX/Hu & TOTEM/Hu. +. Heavy Ion Physics. Recreate conditions similar to those at the Big Bang. Explore quark matter. 2. The Relativistic Heavy Ion Collider. Current Status. Justin Frantz (for . T.Todoroki. ). Ohio University. WWND 15 Keystone, CO. 1. (Filling in For . Takahito. . Todoroki. , his suggestions + A. . Taranenko’s. slides). PHENIX . v. n. hadronic. phases in relativistic collisions of heavy nuclei. Dinesh. K. Srivastava. Variable Energy cyclotron Centre, Kolkata. In collaboration with . Rupa. . Chatterjee. In-medium photon self energy: . Photodiode sensitivity modelling. 2. Introduction. One . of the main working parts of any optical receiver is the photodetector (which converts optical power to an electric current). Either a PIN or APD (avalanche photodiode) photodetector can be used depending on the system . A. (1) symmetry restoration . at . RHIC and . LHC. . energies. T. . . Csörgő. . 1,2. 1. . Wigner R. CP. , . Budapest, Hungary. 2. . EKU KRC, Gyöngyös, Hungary. . Introduction. CERES: . dilepton. 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:. for Cardinal Newman Hall. Randall . Lessard. ET 494. Spring 2014. Instructor: Dr. . Cris. . Koutsougeras. Advisors: Dr. . Rana. . Mitra. . Mr. Byron Patterson. Originally:. The goal of . the . Centre, Kolkata. Elliptic Flow of Electromagnetic Radiation & . Thermalization. Time @ RHIC. Collision of heavy nuclei at relativistic energies leads to formation of Quark- Gluon Plasma (QGP). .