γλώσσες
Σελίδες
Νομικός
Explore all categories to find your favorite topic
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…
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…
Jet evolution in a dense QCD medium Edmond Iancu IPhT Saclay CNRS based on work with J-P Blaizot P Caucal F Dominguez Y Mehtar-Tani A H Mueller and G Soyez 2013-18 June 19…
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+…
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…
Studies of the hadronic decays of Z bosons at LEP Alessandro De Angelis University of Udine and INFN Trieste ICHEP 2000 Osaka July 2000 105 OPAL: Charge multiplicities in…
Pacific Journal of Mathematics DISTRIBUTIVITY IN BOOLEAN ALGEBRAS RICHARD SCOTT PIERCE Vol. 7, No. 1 January 1957 DISTRIBUTIVITY IN BOOLEAN ALGEBRAS R. S. PIERCE 1. Introduction.…
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…
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…