PPT-Transverse Single Spin Asymmetries in PHENIX
Author : kittie-lecroy | Published Date : 2016-09-10
K Oleg Eyser 29 th Workshop on Nuclear Dynamics Squaw Valley CA Feb 310 2013 The Proton Spin Structure What is the connection to orbital angular momentum Transversity
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Transverse Single Spin Asymmetries in PHENIX: Transcript
K Oleg Eyser 29 th Workshop on Nuclear Dynamics Squaw Valley CA Feb 310 2013 The Proton Spin Structure What is the connection to orbital angular momentum Transversity tensor charge . Elastic Electron Scattering. Andrei Afanasev. Hampton University/JLAB. PAVI 2009. Bar Harbor, Maine, June 25, 2009. Plan of talk. Elastic electron-proton scattering beyond the leading order in QED. Models for two-photon exchange. Time Meeting, . 3/09/2010. Stefan Bathe. 03/09/2010. Stefan Bathe for PHENIX, Time Meeting. 1. Past Week History. 03/09/2010. Stefan Bathe for PHENIX, Time Meeting. 2. Had to swap HV mainframe for DC E Wednesday night: lost 10 h of beam. Aharonov. -Bohm, and . Color . Entanglement in Quantum Chromodynamics. Christine A. Aidala. University of Michigan. Jefferson Lab. January 30, 2015. left. right. C. Aidala, JLab, January 30, 2015. Theory of . XIII WORKSHOP ON HIGH ENERGY SPIN PHYSICS . Dubna, Russia . September 1 - 5, 2009. . AZIMUTHAL ASYMMETRIES IN SEMI-INCLUSIVE PRODUCTION OF HADRONS ON THE LONGITUDINALLY POLARIZED DEUTERIUM TARGET. Alexander Burin. Motivation: . to study cooperative dynamics of interacting spins. 2. of . 21. Three alternative models. Classical model of resonant window . E. 0. for electronic spins . due to. . nuclear spins: . 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. Douglas Fields. (University of New Mexico). For the PHENIX Collaboration. 4/9/2008. 1. Douglas Fields for. Motivation for Spin. The proton has a rather complicated structure.. Spin is a useful handle to dissect the proton.. on Neutron . Single . Target . Spin Asymmetries from Transversely . polarized . 3. He . target at . Jlab. Nilanga Liyanage . , . University of Virginia. . Recent SSA . Results from . JLab. Hall A with a Transversely Polarized . George . Igo. for STAR Collaboration. DIFFRACTION . 2012. Puerto del . Carmen,Lanzarote. Sept 10-15. Solenoidal Magnet – 0.5 Tesla field. Beam Pipe. Time Projection Chamber (TPC). Barrel Electromagnetic Calorimeter - BEMC. (an overview, but mainly . D. G). Abhay Deshpande. Stony Brook University. RIKEN BNL Research Center. PANIC’11 at MIT. July 28, 2011. Outline. Introduction. Relativistic Heavy Ion Collide as a polarized . Akio Ogawa . for the STAR collaboration. Brookhaven National Laboratory. 2017 Feb. 8 . QM2017 @ Chicago. Contents. 2. Introduction - Gluon saturation and RHIC . pA. STAR Forward Calorimeter. Results - Single Spin Asymmetry at . Juliette . Mammei. University of Massachusetts, Amherst. G0 finished data-taking in 2007. Published forward and backward angle PV asymmetry results → strange quark contribution to the nucleon. Also measured parity-conserving asymmetry at both forward and backward angles. Norbert Novitzky for PHENIX . collaboration. Stony Brook University. 1. 4. th. International Conference on New Frontiers in Physics, ICNFP 2015. PHENIX detector. 2. Central Arm, |. h. | < 0.35:. Tracking:. 11/21/13. Interference Fragmentation. . –. thrust method. 2. e. +. e. -. . . (. p. +. p. -. ). jet1. (. p. +. p. -. ). jet2. X. Find pion pairs in opposite hemispheres. Observe angles . j. 1.
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