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Heavy Quark Physics and CP Violation II Jeffrey D. RichmanJeffrey D. Richman University of California, Santa BarbaraUniversity of California, Santa Barbara XIII Mexican School…
Challenges of the Standard Model: studying the quark mass dependence Akaki Rusetsky, University of Bonn 7th Georgian-German School and Workshop in Basic Science, 29 August…
n1 ΚΕΙΜΕΝΟ 1 Μάθημα γαλλικών Δεν ήξερα πώς ν’ αρχίσω το μάθημα των γαλλικών. Σκέφτηκα πως το καλύτερο…
SPIN OF THE PROTON IN CORRELATED QUARK MODEL G. Musulmanbekov JINR, Dubna, Russia e-mail:[email protected] Contents Introduction Strongly Correlated Quark Model (SCQM) Spin in…
Triple-gluon and Triple-quark Elastic Scatterings and Early Thermalization Xiao-Ming Xu Shanghai University X.-M. Xu, Y. Sun, A.-Q. Chen, L. Zheng, Nucl. Phys. 744(2004)347…
QCD Matter: A Search for a Mixed Quark-Hadron Phase XXXIII INTERNATIONAL CONFERENCE ON HIGH ENERGY PHYSICS ICHEP'06 Moscow, 26.07- 02.08, 2006 A.N.Sissakian, A.S.Sorin,…
The quark-antiquark potential in N=4 Super Yang Mills The quark-antiquark potential in N=4 Super Yang Mills Juan Maldacena Based on: arXiv:1203.1913, arXiv:1203.1019, arXiv:1202.4455…
QCD Sum Rules: from Quark Masses to Hadronic Form FactorsQCD Sum Rules: from Quark Masses to Hadronic Form Factors Alexander Khodjamirian QCD sum rules (SVZ) [M.Shifman,
THE ROLE OF CONSTITUENT QUARK MASS IN THE STANDARD MODEL S.I.Sukhoruchkin Petersburg Nuclear Physics Institute, Gatchina, Russia Fig. 4, Top: Distribution of ΔEB in nuclei…
Quark-Hadron Duality Rolf Ent PAC-25 Mini-Workshop on Nucleon Excited States First observed ~1970 by Bloom and Gilman at SLAC by comparing resonance production data with…
Physics 661, Chapter 5 1 Lepton and Quark Scattering • e+ e- → µ+ µ- • e+ e- annihilation to hadrons ( e+ e- → QQ ) • Electron-muon scattering, e- µ+…
Dense hadronic and quark matter and its astrophysical applications 51 Krakow School of Theoretical Physics, Zakopane Motoi Tachibana Saga Uni., Japan Topics 1. QCD phase…
Quark Flavor Physics from Belle II Toru Iijima Kobayashi-Maskawa Institute Graduate School of Science Nagoya University 2014.3.7 Lattice QCD Meets Experiment 2014 @ Fermilab…
Quark-Gluon Plasma 200707 Martin Ries Gliederung ● Was ist eigentlich QGP Experimentelle Evidenzen: ● Jψ Unterdrückung an NA50 ● Jetquenching an PHENIX ● Ausblick…
Quark Compositeness Search with γ +Jet Final State at the LHC Satyaki Bhattacharya, Sushil S. Chauhan, Brajesh Choudhary, Debajyoti Choudhury Department of Physics &…
J/ψ Elliptic Flow and High pT Suppression Measurements in A+A Collisions by the PHENIX Experiment Ermias T. ATOMSSA SBU/LLR QUARK MATTER 2009 03/31/2009 E.T. Atomssa. QM2009,…
Lecture 9 Isospin The quark model There is one more “symmetry” that applies to strong interactions. isospin or isotopic spin It was useful in formulation of the quark…
FYS3500 – spring 2020 Ionut Arsene | UiO 3 Ionut Arsene | UiO 4 and 8 gluons (coloured!) ...difficult to calculate No analytical solutions (except 1+1) LQCD=ψi(i
η → 3π and quark masses Stefan Lanz Department of Astronomy and Theoretical Physics, Lund University International Workshop on Chiral Dynamics, August 6 – 10, 2012,…
HEAVY-QUARK FRAGMENTATION FUNCTIONS IN e � e � COLLISIONS Carlo Oleari Università di Milano-Bicocca, Milan DIS2006, Tzukuba 21 April 2006 � � Theoretical introduction…