PPT-Introduction to Hadronic

Final State Reconstruction in Collider Experiments Part VII amp VIII Peter Loch University of Arizona Tucson Arizona USA Validity of Jet Algorithms Need to be valid to any order of perturbative. Introduction:Introduction: Introduction:Introduction:A hard concept to sellA hard concept to sell Making sure the combat doesn Baryon Number Fluctuations. in Heavy Ion Collisions. Masakiyo. Kitazawa. (Osaka U.). MK, M. . Asakawa. , arXiv:1107.2755[. nucl-th. ]. Energy Scan Program @ RHIC. . T. 0. Hadrons. Color SC. m. high. Physics. Report from the Town Meeting October 25. Sebastian Kuhn, Old Dominion University. Agenda. Town Meeting “. Hadronic. Physics”. * 7:00 Medium Energy Physics Overview - Roy Holt. * 7:40 The future of hadron physics - Craig Roberts. 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). remnants. and . molecular. . clouds. Armand Fiasson. LAPP - . Annecy-le-vieux. Where. . CRs. . originate. ?. The . usual. suspects up to the . knee. are . s. upernova . remnants. (. SNRs. ). Diffusive . dilepton. production in semi-QGP. Shu. Lin. RIKEN BNL Research Center. RBRC, Aug 22, 2014. Collaborators:. Photon/. dilepton. . rate: Hidaka, SL, . Satow. , . Skokov. , . Pisarski. Collinear . photon rate: . Discrete Hadronic Symmetries. Christopher Crawford. , University of Kentucky. Symmetry Tests In Nuclei And . Atoms. KITP, U.C. Santa Barbara 2016-09-22. Madison. Spencer. Outline. Hadronic Parity Violation. Hadronic. Final State Reconstruction in Collider Experiments. (Supplement to Part IV: . The ATLAS Calorimeter System). Peter Loch. University of Arizona. Tucson, Arizona. USA. ATLAS: A General Purpose Detector For LHC. . Hadronic. Tensor . . INT Workshop on Flavor Structure of Nucleon Sea, Oct. 2 - 13, 2017. Path-integral Formulation of . Hadronic. . Tensor in . DIS. Parton Degrees of Freedom . . Short Distance Taylor expansion (OPE). muon. . g-. 2. Brendan Casey. PIC. . 2014. September 17. , . 2014. Sept. 11, . 2014 . muon. g-2 experimental hall. Outline. What is g and how do we predict its value. How we measure it for . muons. molecular. . clouds. Armand Fiasson. LAPP - . Annecy-le-vieux. Where. . CRs. . originate. ?. The . usual. suspects up to the . knee. are . s. upernova . remnants. (. SNRs. ). Diffusive . shock. Why study the anomalous magnetic moment of the muon?. Because, is one of the most precisely measured quantities in particle physics.. It put severe limits in deviations from the Standard Model and opens a window . Variability of . Blazars. Markus . B. öttcher. North-West University. Potchefstroom. South Africa. 0. Blazars. Class of AGN consisting of . BL. Lac objects and gamma-ray bright qu. asars. . Rapidly (often intra-day) variable. Markus . B. öttcher. North-West University. Potchefstroom, South . Africa. 0. Most of this work done by:. Haocheng. Zhang. . (Ohio University & Los Alamos). Leptonic. . Blazar. . Model. Relativistic jet outflow with .