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Slide 1 Description of α-decay of heavy and superheavy nuclei A. Sobiczewski and A. Parkhomenko Sołtan Institute for Nuclear Studies, Warsaw XII Nuclear Physics Workshop…

Status of facility design Activities of the IPNS Nuclear/Particle Physics group Basic information for the working sessions Activities of Nuclear and Particle Physics Group…

Nuclear Matrix Elements for Fundamental Symmetries Javier Menéndez JSPS Fellow The University of Tokyo 3rd European Nuclear Physics Conference Groningen 3rd September 2015…

Prezentacja programu PowerPoint Two photon physics with forward detectors Beata Krupa , Leszek Zawiejski Institute of Nuclear Physics Polish Academy of Sciences 22nd FCAL…

On bound states of hadrons in nuclei J. Mareš Nuclear Physics Institute, Řež + D. Gazda, A. Cieplý, N.V. Shevchenko Řež E. Friedman, A. Gal Jerusalem Physics…

Alexander Karpov, JINR, Dubna NUCLEUS-2015, Peterhof, 03.06.15 • What is “Knowledge base” • Fusion-Fission-Evaporation analysis http://nrv.jinr.ru Web knowledge base…

1 1 Dec 2005, Lecture 11 Nuclear Physics Lectures, Dr. Armin Reichold 1 Lectures 11 Particle Detectors 1 Dec 2005, Lecture 11 Nuclear Physics Lectures, Dr. Armin Reichold…

Modern Physicsww w. me ga le ct ur e. co m www.fahadsacademy.com www.youtube.com/megalecture Page 1 of 33 The results of the α-particle scattering experiment &

John On Fifty Remarkable Years of Research at Argonne John P Schiffer BUT ROBERT me robert Me again Me JohnMe Checking a setup in GAMMASPHERE ! John I-Yang LeeMe John SD…

1• If Δm = Mout-Min < 0, then we can get Eout > Ein outoutinin MEME +→+ edba +→+ reactants products 22 ,, 2 1 2 Ex) d-t fusion reaction +→+

Lecture Notes For PHYS 415 Introduction to Nuclear and Particle Physics To Accompany the Text Introduction to Nuclear and Particle Physics, 2nd Ed. A. Das and T. Ferbel World…

Slide 1QCD Constituent quark masses as SM parameters S.I. Sukhoruchkin Petersburg Nuclear Physics Institute 188300 Gatchina Russia Slide 2 Introduction Nonstrange pion and…

FNSN 2 - Introduction A.A. 2016 - 2017 Paolo Bagnaia last mod. 13-May-17 Contents Paolo Bagnaia - FNSN2 - 00 2 1. The static quark model 2. Hadron structure 3. Heavy flavors…

Το άρθρο αυτό μπορεί να έχει 75-125 λέξεις Η επιλογή εικόνων ή γραφικών είναι ένας σημαντικός τρόπος…

Slide 1Anna Kaczmarska Przegląd IFJ PAN, 6.02.09 Kraków Tau leptons as an exciting probe for New Physics in ATLAS Anna Kaczmarska NZ14, Institute of Nuclear Physics PAN,…

University of Turin DEPARTMENT OF PHYSICS Master’s Degree in Nuclear and Subnuclear Physics Measurement of the relative phase between EM and strong amplitudes in ψ2s→…

QCD @ LHC 2016 22-26August 2016 Zurich Burkhard Schmidt CERN on behalf of the LHCb collaboration LHCb results and perspectives on heavy-ion physics  Introduction  LHCb…

PRECISION MEASUREMENT AND FUNDAMENTAL PHYSICS XXXXX 2012 LHC - “ ” “ ” ... ... What is “SIZE” Coulomb interaction Distribution of charge density y r2E = ∫ d3r…

Praha- Dubna SPIN2013 Helical magnets Siberian snakes I.Koop, A.Otboyev, P.Shatunov Yu.Shatunov Budker Institute for Nuclear Physics Novosibirsk Helical magnet yoke cm cm…