A). Introduction b). Quenched calculations c). Calculations with 2 light dynamical quarks d). (2+1) QCD LATTICE QCD SIMULATIONS, SOME RECENT RESULTS (END.
1 Electroweak Physics Lecture 4. 2 Physics Menu for Today Top quark and W boson properties at the Tevatron.
I’ll not discuss about Bayesian or Frequentist foundation (discussed by previous speakers) I’ll try to discuss some facts and my point of view. I think.
Robert Edwards Jefferson Lab Creutz-Fest 2014 TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AAAAAAAAAAAAAAA 1983 HADRONS.
K. Goulianos The Rockefeller University Pomeron Intercept and Slope: the QCD connection 12 th Blois Workshop, DESY, Hamburg, Germany 21-25 May2007 intercept.
Heavy Ion Theory Review Raju Venugopalan Brookhaven National Laboratory LHC week in Split, October 1-6, 2012.
RHIC Phenomenology: Quantum Chromo-Dynamics with relativistic heavy ions D. Kharzeev BNL School on Heavy Ion Phenomenology, Bielefeld, September 2005.
The Physics of GlueX Curtis A. Meyer Carnegie Mellon University.
QCD – from the vacuum to high temperature an analytical approach an analytical approach.
Structure of NLO corrections in 1/N C J. J. Sanz Cillero - Hadrons & Strings, Trento, July 21 st 2006 Structure of next-to-leading order corrections in.
IMFP2006 - Day 3 April 5, 2006 Rick Field – Florida/CDF/CMSPage 1 XXXIV International Meeting on Fundamental Physics Rick Field University of Florida (for.
Universality in ultra-cold fermionic atom gases. with S. Diehl, H.Gies, J.Pawlowski S. Diehl, H.Gies, J.Pawlowski.