PPT-Weak Structure of the Nucleon

Author : stefany-barnette | Published Date : 2017-09-14

Doron Gazit Institute for Nuclear Theory University of Washington Seattle From a few body physicists perspective Motivation Interaction of weak probes with nuclei

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Weak Structure of the Nucleon: Transcript

Doron Gazit Institute for Nuclear Theory University of Washington Seattle From a few body physicists perspective Motivation Interaction of weak probes with nuclei Part I Weak structure of the nucleon. Dingjue Ji, Yaojin Sun. Department of Bioinformatics and Biostatistics, School of Life Science, Shanghai Jiaotong University. 800 Dongchuan RD, Shanghai, China. Outline. Introduction. Methods. Results. Eli Piasetzky. Tel Aviv University, Israel . The EMC effect is 30 years old. Deep Inelastic Scattering (DIS) . . E. E`. (. ,. q. ). nucleon. Final state Hadrons . W. 2. Incident lepton. E, E’ 5-500 GeV. Gerhard . Mallot. Plan. Lecture I. Introduction. DIS and structure functions, sum rules. Why contribute the quark spin so little? . Principle of measurements, experiments. G. Mallot/CERN. Obergurgl, October 2007. Stryer. Short Course. Chapter 2. Water. Polarity. Medium for Brownian motion. Solvent. Intermolecular Forces. Electrostatic: Ionic. Permanent dipole. H-bonding. Van der Walls. Not true categories…. Salpeter. . approach and lepton-, hadron-deuteron . scattering. V.V.Burov. S.G.Bondarenko. , . E.P.Rogochaya. , . M.V.Rzjanin. , G.I Smirnov– JINR, . Dubna. . A.A.Goy. , . V.N.Dostovalov. , . K.Yu.Kazakov. And symmetries. the simplest nuclei. LHC Particle Accelerator @ CERN. Agenda. Nature of NN forces from gross nuclear properties. Reality check: Properties of the deuteron demand . sophistication (tensor & exchange forces. Stryer. Short Course. Chapter 2. Water. Polarity. Medium for Brownian motion. Solvent. Intermolecular Forces. Electrostatic: Ionic. Permanent dipole. H-bonding. Van der Walls. Not true categories…. 4 fundamental forces in nature. The familiar force of . gravity. pulls you down into your seat, toward the Earth's center. You feel it as your weight.. . Why don't you fall through your seat?. Well, another force, . Inclusive measurements at large . x. ; . quark models tests and Lattice QCD tests. Exclusive measurements in the valence region (imaging): . DVCS + DVMP + Lattice to create an image.. Semi-inclusive measurements . Craig Roberts. Physics Division. . Getting real. KITPC: From nucleon structure ... - 46pgs. Craig Roberts: The Issue of Substance in Hadron Physics (83). 2. Charting the Interaction. Interaction in QCD is not momentum-independent. Extending the reach of “ab initio” nuclear many-body methods. Thomas DUGUET. CEA/. SPhN. , Saclay, France. IKS, KU Leuven, . Belgium. NSCL, . Michigan State . University. , . USA. Collaborators: . Robert Edwards . Jefferson Lab. N. *. @ high . Q. 2. , 2011. TexPoint. fonts used in EMF. . Read the TexPoint manual before you delete this box.: . A. A. A. A. A. A. A. A. A. A. A. A. A. A. A. Collaborators:. Xiangdong Ji. University of Maryland. Why is the proton mass interesting?. How to communicate the lofty goals of nuclear physics to general public?. Long-range plan: . One of the purposes of modern nuclear physics is to understand the origin of the masse of the visible matter. . Craig Roberts, Physics Division. . Collaborators: 2012-Present. Rocio. BERMUDEZ (U . Michoácan. ). ;. Shi CHAO. (. Nanjing U. ) ;. Ming-. hui. DING (. PKU. );. Fei. GAO (. PKU. ) ;. S. HERNÁNDEZ.

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