Slide 1The Role of the Pion in QCD/SM Model S.I. Sukhoruchkin Petersburg Nuclear Physics Institute 188300 Gatchina Russia Slide 2 Introduction Nonstrange pion and $\ro$-meson…

Baryon spectrum from Nf =2+1+1 Christos Kallidonis 4 April 2013 ETM Collaboration Meeting Nicosia, 3-6 April 2013 CaSToRC OUTLINE o  Simulation details o  Overview of…

Slide 1Structure of the Roper Resonance from Measurements of p(e,e’ p)  0 using Recoil Polarization Observables Spokespeople: Simon Sirca (U. of Ljubljana, Slovenia)…

Slide 1Probing QCD Phase Diagram with Fluctuations of conserved charges Krzysztof Redlich University of Wroclaw & EMMI/GSI QCD phase boundary and its O(4) „scaling”…

Slide 1Daniel Gómez Dumm IFLP (CONICET) – Dpto. de Física, Fac. de Ciencias Exactas Universidad de La Plata, Argentina Issues on nonlocal chiral quark models Slide 2…

Slide 1 The DWEF Model: Refractive Distortions of HBT John G. Cramer (with Gerald A. Miller) University of Washington Seattle, Washington, USA John G. Cramer (with Gerald…

Slide 1 Equation of state for distributed mass quark matter T.S.Bíró, P.Lévai, P.Ván, J.Zimányi KFKI RMKI, Budapest, Hungary Distributed mass partons in quark matter…

Slide 1 The GlueX Experiment Curtis A. Meyer Carnegie Mellon University The GlueX Collaboration 8/23/10 1 GlueX Experiment 12 GeV electrons 40% lin. Pol. Uncollimated Collimated…

Developing supercomputers and computational physics 1 Multi-nucleon bound states in Nf=2+1 lattice QCD T. Yamazaki1), K.-I. Ishikawa2), Y. Kuramashi3,4), A. Ukawa3) 1) Kobayashi-Maskawa…

DEK Varying fundamental constants - a key property and key problem of quintessence Fundamental “constants” are not constant Have coupling constants in the early Universe…