PPT-Towards computing the lepton and quark mass spectra and the
Author : ellena-manuel | Published Date : 2016-04-26
Jiří Hošek Department of Theoretical Physic s Nuclear Physics Institute R ez Prague Czech Republic arXiv 14017503
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Towards computing the lepton and quark mass spectra and the: Transcript
Jiří Hošek Department of Theoretical Physic s Nuclear Physics Institute R ez Prague Czech Republic arXiv 14017503 . (photoelectric effect), . light scattered . (Compton) . like particle →Photon . γ. Elecrodynamics. : field →. exchage. particle. . (mediator; . photon. ). 뉴트리노에. Lee. . . . . Quark . condensate and the . h. ’ mass. . . h. ‘ at finite temperature. 1. 1. . Quark condensate and the. . h. ’ meson. 2. Some introduction. Casher Banks formula. First Look at Samples. LCD WG6 Meeting, 13/03/2012. J.S. Marshall, University of Cambridge. HZ Recoil Analysis - Reminder. . s. = 500GeV. L. int. = 500fb. -1. m. H. . = 120GeV. No polarization. R. e. l. d. The. d. i. A. Yu. Smirnov. Max-Planck Institute. for Nuclear Physics,. Heidelberg, Germany . NOW 2014 . September 8– 13, 2014 . . The riddle of neutrino mass:. strongly suppresses . Philippe Doublet. Roman . Pöschl. , François Richard. + Thibault Frisson & Jérémy . Rouene. LCWS Granada, Sept. 2011. Philippe Doublet - LAL. Plan. Motivation. Measurement. . method. Efficiencies. Leptogenesis. University of Maryland. Department of Physics. Chang-Hun Lee. P.S. . Bhupal. Dev, C.-H. Lee, R.N. . Mohapatra. , . Phys.Rev. . D90 (2014) 9, . 095012. P.S. . Bhupal. Dev, C.-H. Lee, R.N. . . Lee . . . 1. Few words on a recent sum rule result. 2. A simple constituent quark model for D meson . 3. Consequences . 4. Summary. D meson in nuclear medium: a . consituent. Sergey L. Sheetlin. ,. Yuri A. Mirokhin, Dmitrii V. Tchekhovskoi, Xiaoyu Yang, Stephen E. Stein. NIST Mass Spectrometry Data Center, Biomolecular Measurement Division,. National Institute of Standards and Technology. ass: Facts and Fancy. Francesco Vissani. LNGS and GSSI. Introduction. Baryon and lepton numbers and their status in the standard model of particles and interactions. L. epton and baryon number. In all known transformations among particles,. Xiangdong Ji. University of Maryland. Why is the proton mass interesting?. How to communicate the lofty goals of nuclear physics to general public?. Long-range plan: . One of the purposes of modern nuclear physics is to understand the origin of the masse of the visible matter. . = 2.4 GeV measured . with HADES. . Dominique Dittert for the HADES Collaboration. Outline. Introduction. Differential Spectra. Azimuthal Anisotropy. Recent Ag+Ag Beamtime. Summary. Introduction. The HADES Physics Case. Jet suppression . Heavy flavor . Future . Non-zero v_2,3 in D0 production observed . light quark recombination effects? . D_s? ALICE data, smaller . coalescence effect? . How about J/Psi ? Upsilons? . . Higgs boson production in association with top quark pairs at CMS. Dr. . Ram Krishna . Dewanjee. Lab of High Energy and Computational Physics,. K.B.F.I, Tallinn . On behalf of the CMS collaboration. Sergey L. Sheetlin. ,. Yuri A. Mirokhin, Dmitrii V. Tchekhovskoi, Xiaoyu Yang, Stephen E. Stein. NIST Mass Spectrometry Data Center, Biomolecular Measurement Division,. National Institute of Standards and Technology.
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