PPT-Two-Particle Correlation in e + e - Collisions at 91.2 GeV with

TwoParticle Correlation in e e Collisions at 912 GeV with ALEPH Archived Data 1 TwoParticle Correlation in ee with ALEPH archived data Anthony Badea Austin Baty YenJie Lee . Assuming all the particles started out above the 711oor theyd all have to stay there for the rest of the simulation How could we go about implementing this Clearly there are two problems We need to detect when particles are near the 711oor and when introduction. Erik . Adli. , University . of . Oslo, . . August 2015, . Erik.Adli. @cern.ch. . , . v2.11. Video: the LHC accelerator. youtube: the LHC Accelerator. 3. 25 ns. Event rate in ATLAS : . Exercise. : . Nuclear Modification Factor. Outline. ALICE. goals of the new exercise. physics objective. geometry of Pb-Pb collisions. nuclear modification factor: R. AA. (R. CP. ). new exercise. step 1: visual analysis of pp and Pb-Pb collisions. geometric . fluctuations of the . Glauber. model make specific predictions for . a dipole and triangle terms in the observed azimuthal distribution of particles. Preliminary . results on . the v. 1. Limin Fan (. 樊利敏. ). Central. . China. . Normal. . University. (CCNU). 1. Outline. Introduction.. Model and calculation.. Results and discussion.. Summary and outlook.. 2. 3. Pre-equilibrium. arXiv:1408.3108 [hep-. ph. ]. Gin. és. MARTINEZ-GARCIA. Subatech. (CNRS/IN2P3 - . École. des Mines de Nantes – . Université. de Nantes). Oral presentation in the 10th International Workshop on High . Cross Sections and Collision Geometry. The . cross . section: Experimental Meaning. Scattering Experiment. Monoenergetic. particle beam. Beam impinges on a target. Particles are scattered by target. to unravel . nature’s secrets. B.Satyanarayana. Department of High Energy Physics. bsn@tifr.res.in, www.tifr.res.in/~bsn. Science and engineering. Science.  . . is a systematic enterprise that builds and organizes knowledge in the form of . Valeriy Tenishev, . Dmitriy. . Borovikov. , Nicolas . Fougere. , . Yuni. Lee, . Michael R. . Combi. , . Tamas. . Gombosi. , Martin Rubin. New component of SWMF. SWMF Control & Infrastructure. Eruption. Distinguishing Between Soft- . and . Hard-Component . by . Multiplicity Correlation. Na Li. Huazhong. University of Science and Technology. 7th International Workshop on . CPOD. , . 7 . - 11 November 2011. Outline. February 9, 2008. Quark Matter 2008. 2. Results. dN/dy. Stopping. Summary. and discussion. Experiment and motivation. Motivation: . reference to understand baryon transport. February 9, 2008. Law of Conservation of Momentum. With no external force, momentum doesn’t change. It’s the opposite of the impulse momentum relationship!. Ft = Δmv. Example. Consider a gun being fired.. A gun recoils when it is fired. . 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. Erik . Adli, University of Oslo,. . September 2017, . Erik.Adli. @cern.ch. . , v2.30. Particle accelerator physics. Particle detectors. Data analysis. The study of relativistic charged particle beams in electromagnetic fields.