The Known Knowns and the Known Unknowns 20 Years of Tevatron Collider Physics.
Automation of fast NLO QCD calculations for PDF fits
Martín Schvellinger Instituto de Física de La Plata - CONICET Departamento de Física - UNLP The gauge/gravity duality and Non-Relativistic Quantum Field.
Low-x and PDF studies at LHC Sept 2008 A M Cooper-Sarkar, Oxford At the LHC high precision (SM and BSM) cross section predictions require precision Parton.
1 Generators at the LHC concerns for the startup Albert De Roeck CERN MC4BSM Workshop Thanks to: P. Bartalini, I. Hinchlife, J. Huston, B. Kersevan, F.
Bonn 23 rd Feb1 Simulations of BSM Signals Peter Richardson IPPP, Durham University.
ACFI-FRIBM. Horoi CMU Double-beta decay and BSM physics: shell model nuclear matrix elements for competing mechanisms Mihai Horoi Department of Physics,
K. Zuber, University of Sussex Neutrinoless double beta decay SUSSP 61, St. Andrews, 9-23 Aug. 2006.
Les Houches SM and NLO multi-leg group: experimental introduction and charge G. Heinrich, J. Huston, J. Maestre, D. Maitre, R. Pittau, G. Soyez (jet liason)
Cosmology Basics Coherent story of the evolution of the Universe that successfully explains a wide variety of observations This story injects 4-5 pieces.
B. Lee Roberts, DPF09- Wayne State University – 29 July 2009 - p. 1/36 Low Energy Searches for BSM Physics: The other path to the summit B. Lee Roberts.
Contents Lecture 1 General introduction What is measured in DBD ? Neutrino oscillations and DBD Other BSM physics and DBD Nuclear matrix elements Lecture.