Slide 1Hypernuclei: A very quick introduction Electroproduction of hypernuclei The experimental Program at Jefferson Lab Update on the analysis of O and Be targets Update…
Slide 1Javier Junquera Advanced Computing Starting-up: How to setup the initial conditions for a Molecular Dynamic Simulation Slide 2 The initial configuration In molecular…
Slide 1 Top Mass Measurement at the Tevatron HEP2005 Europhysics Conference Lisboa, Portugal, June 22, 2005 Koji Sato (Univ. of Tsukuba) for CDF and D0 Collaborations Slide…
Diapositiva 1 The angular dependence of the 16O(e,e’K+)16LN and H(e,e’K+)L F. Garibaldi – Jlab December 12-2012 The WATERFALL target: reactions on 16O and 1H nuclei…
CHAPTER 14 Systems of Particles The effective force of a particle is defined as the product of it mass and acceleration. It will be shown that the system of external forces…
Neutrino states in oscillation experiments – are they pure or mixd? Pheno 07, May, 07-09, 2007, Madison , Wisconsin Marek Zralek, Univ. of Silesia 1. INTRODUCTION P D Common…
eScience and Particle Physics Roger Barlow eScience showcase May 1st 2007 Particle physics yesterday Particle physics has pushed the computing envelope ever since the early…
Top Mass Measurement at the Tevatron HEP2005 Europhysics Conference Lisboa, Portugal, June 22, 2005 Koji Sato (Univ. of Tsukuba) for CDF and D0 Collaborations Top Quark Mass…
US participation in Heavy Ion Physics with Compact Muon Solenoid at LHC M. Ballintijn,K Barish,R Betts, BE Bonner, W.Busza, D.Cebra, G.Eppley, E.Garcia, F.Geurts, C.Halliwell,…