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Quark masses and the strong CP problem Michael Creutz Brookhaven Lab Michael Creutz BNL 1 Conventional picture • quark mass matrix can have a phase M = M eiΘ • U1 anomaly…
11 CKM quark-mixing matrix 1 11 THE CKM QUARK-MIXING MATRIX Written January 2006 by A Ceccucci CERN Z Ligeti LBNL and Y Sakai KEK 111 Introduction The masses and mixings…
Determination of the light quark masses The mu and md quark masses from η → 3π decay Martin Zdráhal Institute of Particle and Nuclear Physics Faculty of Mathematics…
1 Roberto Casalbuoni Dipartimento di Fisica e Astronomia, Sezione INFN Istituto G. Galilei per la Fisica Teorica GGI, Terza Cultura Firenze 201718 - [email protected]…
Measurements of the top quark mass with the ATLAS detector p p t b b-jet W+ ν� �+ t b b-jet W− �− ν� GeVrecolbm 40 60 80 100 120 140 160 E ve nt s 2 G eV 0…
Paul Hoyer Jlab 24 May 2007 1 Paul Hoyer University of Helsinki Exclusive Reactions at High Momentum Transfer Jefferson Lab 21 - 24 May 2007 Inclusive Perspectives Paul Hoyer…
Where does the proton spin come from? • Quark and glue spins -- status • Gauge field tensor operator • Momentum and angular momentum sum rules and renormalization •…
Letter of Intent for Experiments at 50 GeV PS of the JPARC Measurement of the K0L → π0νν Branching Ratio Y. B. Hsiung Fermi National Accelerator Laboratory, USA National…
Train Wreck of the Mundane?Train Wreck of the Mundane? The The NuTeVNuTeV Anomaly:Anomaly: A hint of New Physics? orA hint of New Physics? or Kevin McFarlandKevin McFarland…
Nucleon form factors and N-Δ transitions in a hypercentral constituent quark model D. Y. Chen, Y. B. Dong, Institute of High Energy Physics, Beijing 10049, P. R. China M.…
Nucleon form factors and N-Δ transitions in a hypercentral constituent quark model D. Y. Chen, Y. B. Dong, Institute of High Energy Physics, Beijing 10049, P. R. China M.…
Quark Correlations and Single Spin Asymmetry G. Musulmanbekov JINR, Dubna, Russia e-mail:[email protected] Contents Introduction Strongly Correlated Quark Model (SCQM) Spin in…
Quark Imaging at JLab 12 GeV and beyond (1) Tanja Horn Jefferson Lab HUGS, Newport News, VA 9 June 2009 1Tanja Horn, CUA ColloquiumTanja Horn, Quark Imaging at JLab 12 GeV…
Single Spin Asymmetry in Correlated Quark Model G. Musulmanbekov JINR, Dubna e-mail:[email protected] Contents Introduction Strongly Correlated Quark Model (SCQM) Single Spin…
Slide 1 The speed of sound in a magnetized hot Quark-Gluon-Plasma Based on: 0905.2097 Neda Sadooghi Department of Physics Sharif University of Technology Tehran-Iran MIDEAST…
Quark-Gluon Plasma Sijbo-Jan Holtman Overview Introduction Phases of nuclear matter Thermodynamics Experiments Conclusion Introduction Research of quark-gluon plasma important…
Slide 1QCD Constituent quark masses as SM parameters S.I. Sukhoruchkin Petersburg Nuclear Physics Institute 188300 Gatchina Russia Slide 2 Introduction Nonstrange pion and…
Inclusive b-quark and upsilon production in DØ Horst D. Wahl Florida State University DIS 2005, Madison Outline l Tevatron and DØ detector Bottomonium ϒ(1S) production…
Poster Session XXVI International Conference on Ultrarelativistic Nucleus-Nucleus Collisions February 5-11 2017 Chicago IL 1 Location Title Presenter A01 Production of Σ±1385…
• Accoppiamenti del W • correnti cariche e correnti neutre • Le interazioni nel Modello Standard • Angolo di Weinberg A i i d ll i f i i• Accoppiamenti dello…