PPT-Transverse Spin Asymmetries in

Elastic Electron Scattering Andrei Afanasev Hampton UniversityJLAB PAVI 2009 Bar Harbor Maine June 25 2009 Plan of talk Elastic electronproton scattering beyond the leading order in QED Models for twophoton exchange. RESONANCE. . RAJAN PANDYA & MOHIT GANGULY. Magnetic Resonance Imaging. Provide high resolution anatomic structure (as with X-ray CT). Provide . high contrast between different soft tissues (X-ray CT cannot). isospin. correlated matter. Masayasu. Harada . (Nagoya Univ.). at Mini workshop on . . . “Structure and production of charmed baryons II”. . (J-PARC, August 7, 2014). Based on. ・ . D.Suenaga, B.-. 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: . 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.. 10-8. Complex . multiplets. sometimes occur when there is a relatively small difference in . δ. between two absorptions.. The N+1 rule may not apply in a direct way if several neighboring hydrogens having fairly different coupling constants are coupled to the resonating nucleus.. (♯). K. Oleg . Eyser. 29. th. Workshop on. Nuclear Dynamics. Squaw Valley, CA, Feb. 3-10, 2013. The Proton Spin Structure. What is the connection to orbital angular momentum?. Transversity. ↔ tensor charge . 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. . Alain . Magnon. CEA-IRFU/. SPhN. & COMPASS . DIS2009 – Madrid 29 April, 2009 . . CO. MMON. M. UON. . and. P. ROTON. A. PPARATUS. . for. S. . RAJAN PANDYA & MOHIT GANGULY. Magnetic Resonance Imaging. Provide high resolution anatomic structure (as with X-ray CT). Provide . high contrast between different soft tissues (X-ray CT cannot). EMN Meeting: Quantum Comm. & Quantum Imaging, Berlin, Aug 2016. John S. Colton. Physics Department. Brigham Young . University, Provo, Utah. Student researchers: . Ken Clark. Daniel Craft. Jane Cutler. 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 . hh. 10/8/2015. FCC-hh RF and Transverse Feedback System / W. Hofle 08 October 2015. 1. As presented at the FCC Week. With some additional remarks. Wolfgang Hofle. BE-RF-FB. Start with where we stand . R. Apsimon. Lancaster University / Cockcroft Institute. Motivation. Currently bunch length and energy spread measurements done with separate diagnostics. Can’t reconstruct the longitudinal phase space. Maureen A. Mealy, RN, BSN, Daniel Becker MD, Scott D. Newsome, DO,. John . N. Ratchford, MD, Michael Levy, MD, PhD, Carlos A. Pardo, MD. The Johns Hopkins Transverse Myelitis Center performed a retrospective analysis .