PPT-Two non-equilibrium problems in heavy-ion collisions:

Author : jane-oiler | Published Date : 2016-08-08

Critical dynamics amp Sphaleron transitions Raju Venugopalan BNLHeidelberg Hirschegg 2016 January 1722 2016 Outline N onequilibrium dynamics of two situations of

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Two non-equilibrium problems in heavy-ion collisions:: Transcript


Critical dynamics amp Sphaleron transitions Raju Venugopalan BNLHeidelberg Hirschegg 2016 January 1722 2016 Outline N onequilibrium dynamics of two situations of interest in heavyion collisions. Satisfiability. and Constraint Satisfaction Problems. by Carla P. Gomes, Bart Selman, . Nuno. . Crato. and . henry. . Kautz. Presented by . Yunho. Kim. Provable Software Lab, KAIST. Contents. Heavy-Tailed Phenomena in . interesting ?. Interaction of heavy quarks with the plasma. . - . our model (elastic and inelastic collisions, LPM). . - comparison with data. . - how far we are with our understanding. . P. é. ter. Petreczky. . . Bielefeld, July 2013. Study of the strongly interacting matter and its new . “phases”. Past: . AGS, SPS, . E. cm. =(1-17) . Rainer Fries. Texas A&M University & RIKEN BNL. Workshop on RHIC Paradigms. UT Austin, April 14, 2010. Austin: RHIC Paradigms. 2. Rainer Fries. Overview. Introduction Recombination. Satisfiability. and Constraint Satisfaction Problems. by Carla P. Gomes, Bart Selman, . Nuno. . Crato. and . henry. . Kautz. Presented by . Yunho. Kim. Provable Software Lab, KAIST. Contents. Heavy-Tailed Phenomena in . He came from traditional nuclear physics, and is one of the few I know who made the transition to high energy heavy ion physics with a modern perspective.. People fall into three categories:. Those who make things happen.. . AGS. . -- . Heavy . Ion . P. rograms. Hideki Hamagaki. (. hamagaki_hideki@pilot.nias.ac.jp. ). Institute for Innovative Science and Technology. Nagasaki Institute of Applied Science. Contents. Introduction. PlasMA. Nonequilibrium. Dynamics. in Astrophysics and Material Science. YITP, Kyoto, Japan, Oct. 31-Nov. 3, 2011. Tetsufumi. Hirano. Sophia Univ./. the Univ. of Tokyo. Outline. Introduction. Physics of the quark gluon plasma. The Haber process proceeds as follows:. . 2NH. 3 (g). + 92KJ ↔ N. 2 (g). + 3H. 2 (g) . . If the equilibrium concentrations are:. [NH. 3. ] = 3.1x10. -2. M. [N. 2. ] = 8.5x10. -1. M. [H. 2. W. A. Horowitz. The Ohio State University. February 23, 2010. 16-Nov-10. 1. UCT Seminar. With many thanks to Brian Cole, . Miklos. . Gyulassy. , Ulrich Heinz, and Yuri . Kovchegov. Introduction. What is a heavy ion collision?. Collisions. @ LHC ++. 1. One. central ALICE event for . Pb+Pb @ 2.76 . TeV.A. => E(. kin_total. )= 574 GeV . 0-5% central: . 25000 . particles. Relativistic. AA . and. . eA. . Collisions. 2. “versus” AdS/CFT. Perils, Pitfalls, Progress, Prospects. W.A. . Zajc. Physics Department. Columbia University, New York, NY. . ( . this talk available . at . http://. www.phenix.bnl.gov/phenix/WWW/publish/zajc/sp/presentations/Durham. with heavy-ions. Hou. . Keong. (Tim) Lou,. Simon . Knapen. , . Tongyan. Lin and Tom Melia. PhysRevLett.118.171801. a. Pb. Light Dark Matter 2017. *Disclaimer: Not Dark Matter! Sorry!. “Light”? “Dark”? . Bedanga. Mohanty. NISER. (For STAR Collaboration). Based on STAR: . arXiv. : 1701.07065 . 01/20. Goals of Heavy-Ion Collision. Find out the phase structure of QCD phase . d. iagram . e. xperimentally.

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