Summary of Workshop on Spin of Nucleons from Low to High Energy Scales
|
|
- Dina Evans
- 5 years ago
- Views:
Transcription
1 Summary of Workshop on Spin of Nucleons from Low to High Energy Scales Jen-Chieh Peng University of Illinois at Urbana-Champaign EINN2015, Paphos, Cyprus, Nov. 1-7,
2 Three Sessions of the Spin Workshop High Energy Spin Structure Peng, Armstrong, Eyser, Steffens, Contalbrigo, Baltzel, Kubarovsky Low Energy Spin Structure Chen, Collicott, Correa, Sparveris, Pascalutsa, Krebs, Pauk, Kallidonis New Directions and Discussion Reimer, Dashpande, Voutier 2
3 Main topics of this summary Flavor structure of the nucleon sea Flavor asymmetry of the light-quark sea (new data from Fermilab and RHIC. New results from lattice) Gluon polarization and OAM in the nucleon Results from COMPASS, RHIC, and JLab Nucleon polarizability and spin sum rules Data from MAMI and JLab. Comparison with theories 3
4 Flavor Structure of the Nucleon Sea 4
5 There was a time when a simple flavor structure of nucleon sea was assumed u( x) d ( x) s( x) s( x) SU(3) symmetric sea From Frank Close s textbook (1980) Questions Is u ( x) d ( x)? Is s ( x) u ( x)? Is s ( x) s( x)? Actually, the nucleon sea is more subtle 5
6 Is u d in the Proton? Expect d u since sea quarks are produced in g qq = 6
7 Is u d in the Proton? The Gottfried Sum Rule I constructed this sum rule in the hope of destroying the quark model Gottfried, S [( F ( x) F ( x)) / x] dx G 0 p n ( u ( ) ( )) p x d p x 1 ( if u p d p) 3 dx New Muon Collaboration (NMC) obtains S G = ± ( Significantly lower than 1/3! ) d u? Need an independent check! 7
8 Complimentality between DIS and Drell-Yan DIS Drell-Yan Ann.Rev.Nucl. Part. Sci. 49 (1999) 217 Both DIS and Drell-Yan process are tools to probe the quark and antiquark structure in hadrons (factorization, universality) 88
9 d / u flavor asymmetry from Drell-Yan d dx dx 4 9sx x DY a e q ( x ) q ( x ) q ( x ) q ( x ) 2 a a 1 a 2 a 1 a 2 mass spectrum 800 GeV proton beam on hydrogen and deuterium pd pp 1 Dr ell-yan: / 2 (1 d ( x2) / u( x2) ) 2 9
10 Some Theoretical Models for d / u Asymmetry Meson Cloud Models Chiral-Quark Soliton Model Instantons nucleon = chiral soliton expand in 1/Nc Quark degrees of freedom in a pion mean-field Meson cloud has significant contributions to sea-quark distributions The meson cloud has various implications on Asymmetry between s( x) and s( x)? Asymmetry between u ( x) and d( x)? Orbital angular momentum carried by the mesons? 10
11 What happens to d ( x) / u ( x) at large x? SeaQuest Experiment ( Unpolarized Drell-Yan using 120 GeV proton beam) Main goals: 1) Measure d / u flavor asymmet ry up to x ) Measure EMC effect of antiquarks up to x 0.45 Talk of Paul Reimer 11
12 Sign change of d ( x) u( x) at x ~ 0.25? (or d ( x) / u( x) 1 at x ~ 0.25?) Why is it interestin g? Meson cloud model (no models can explain it yet!) Chiral-quark soliton model Statistical model 12
13 Preliminary result from 5% of anticipated data Talk by Paul Reimer 13
14 First lattice calculation of u( x) d ( x) First time the x dependence, rather than the moment of quark distribution is calculated on lattice Using an algorithm proposed by X. Ji (PRL 110 (2013) ) [ d( x) u ( x)] dx consistent with the experiment x H.W. Lin et al,
15 Lattice Calculation of Polarized PDFs Talk by Fernanda Steffens q( x) q( x) d ( x) u( x) u( x) d( x) Steffens confirms the result d ( x) u( x) The calculation also predicts d ( x) u ( x) x 15
16 u ( x) and d ( x) from W production at RHIC-spin Oleg Eyser and Bernd Surrow x u ( x) x d ( x) u d consistent with some models and lattice 16
17 Gluon polarization and orbital angular momentum in the nucleon 17
18 Where does the spin of the proton come from? EMC experiment in 1988/1989 q q "Spin Crisis" q 18
19 World-wide effort to measure g 1p, g 1 d Spin-dependent DIS CERN: EMC, SMC, COMPASS SLAC: E80, E142, E143, E154, E155 DESY: HERMES JLab: Hall A, B, and C world data on g 1 p (hep-ex/ ) 19
20 NLO fit to world DIS g 1p, g 1 d data (arxiv: ) x g( x) Q 3 GeV 2 2 integrals: G 0.5 x u V ( x) x d V ( x) x S( x) 0.82 U D S
21 NLO fit to world DIS g 1p, g 1 d data (arxiv: ) Q 3 GeV 2 2 integrals: G U D S 0.08 ~1/3 of the proton's spin is carried by quark/antiquark's spin 21
22 Lattice result on ΔΣ q for hyperons and charmed baryons Talk by C. Kallidonis 22
23 NLO fit to world DIS g 1p, g 1 d data (arxiv: ) Q 3 GeV 2 2 integrals: G U D S 0.08 ~1/3 of the proton's spin is carried by quark/antiquark 's spin G is only loosely contrained by polarized DIS 23
24 Di-hadron production in polarized DIS PLB 718 (2013) 922 Photon-gluon fusion Di-hadron production data suggest positive Δg/g 24
25 Δg from RHIC-spin 0 A jet from PHENIX from STAR LL A LL Talk by Oleg Eyser PRD 90 (2014) PRL 115 (2015) Sensitive to Δg due to the q + g q + g underlying process 25
26 Δg from RHIC Talk by Oleg Eyser with published RHIC data until
27 Δg from EIC Talk by A. Deshpande 27
28 Extraction of orbital angular momentum via Generalized Parton Distribution (GPD) 28
29 M. Contalbrigo 29
30 Nathan Baltzell 30
31 Transversity GPD from Deeply Pseudoscalar Meson Production at JLab Talk by V. Kubarovsky Flavor separation is possible from π 0 and η production data 31
32 DVCS kinematic coverage 32
33 Nucleon polarizability and spin sum rules 33
34 34
35 35
36 Talk by Cristina Collicott 36
37 Cristina Collicott 37
38 Cristina Collicott 38
39 New measurement of generalized polarizabilities Loup Correa 2 2 E( Q ) and M( Q ) 39
40 Other ongoing and proposed measurements for generalized polarizabilities Nikos Sparveris 40
41 Moments of spin structure functions Jian-Ping Chen 41
42 Jian-Ping Chen The LT puzzle neutron New data on proton target are being analyzed 42
43 V. Pascalutsa 43
44 V. Pascalutsa 44
45 Hermann Krebs 45
46 Whitney Armstrong 46
47 Extraction of Whitney Armstrong d 2 for protn and neutron 47
48 Lepton universality test in lepton-pair production Vladimir Pauk p e e p versus p p 48
49 Lepton universality test in lepton-pair production Vladimir Pauk p e e p versus p p Relevant to the proton radius puzzle 49
50 Talk by E. Voutier
51 Eric Voutier 51
52 End of the Workshop Summary Thanks to all speakers and organizers! 52
Nucleon Spin Structure: Overview
Nucleon Spin Structure: Overview Jen-Chieh Peng University of Illinois at Urbana-Champaign Workshop on Spin Structure of Nucleons and Nuclei from Low to High Energy Scales EINN2015, Paphos, Cyprus, Nov.
More informationHelicity: Experimental Status. Matthias Grosse Perdekamp, University of Illinois
Helicity: Experimental Status Matthias Grosse Perdekamp, University of Illinois Content o The Experimental Effort o Quark and Sea Quark Helicity è DIS, SIDIS, pp è new FFs for global analysis è results
More informationFlavor Asymmetry of the Nucleon Sea and W-Boson Production*
Flavor Asymmetry of the Nucleon Sea and W-Boson Production* Department of Physics University of Illinois 7 December 2012 *R. Yang, J.C. Peng, M. Grosse-Perdekamp, Phys. Lett. B 680 (2009) 231-234 What
More informationNucleon Spin Structure from Confinement to Asymptotic Freedom
21 September 2009 QNP09 Beijing Nucleon Spin Structure from Confinement to Asymptotic Freedom K. Griffioen College of William & Mary griff@physics.wm.edu 5th International Conference on Quarks in Nuclear
More informationSpin Structure of the Nucleon: quark spin dependence
Spin Structure of the Nucleon: quark spin dependence R. De Vita Istituto Nazionale di Fisica Nucleare Electromagnetic Interactions with Nucleons and Nuclei EINN005 Milos September, 005 The discovery of
More informationQuarkonium Production at J-PARC
Quarkonium Production at J-PARC Jen-Chieh Peng University of Illinois at Urbana-Champaign J-PARC Meeting for Spin and Hadron Physics RIKEN, April 7-8, 008 Outline Quarkonium Production at J-PARC with Unpolarized
More informationSpin Structure with JLab 6 and 12 GeV
Spin Structure with JLab 6 and 12 GeV Jian-ping Chen ( 陈剑平 ), Jefferson Lab, USA 4 th Hadron Workshop / KITPC Program, Beijing, China, July, 2012 Introduction Selected Results from JLab 6 GeV Moments of
More informationMeasurements with Polarized Hadrons
Aug 15, 003 Lepton-Photon 003 Measurements with Polarized Hadrons T.-A. Shibata Tokyo Institute of Technology Contents: Introduction: Spin of Proton Polarized Deep Inelastic Lepton-Nucleon Scattering 1.
More informationProton longitudinal spin structure- RHIC and COMPASS results
Proton longitudinal spin structure- RHIC and COMPASS results Fabienne KUNNE CEA /IRFU Saclay, France Gluon helicity PHENIX & STAR: pp jets, pp p 0 COMPASS g 1 QCD fit + DG direct measurements Quark helicity
More informationProbing nucleon structure by using a polarized proton beam
Workshop on Hadron Physics in China and Opportunities with 12 GeV Jlab July 31 August 1, 2009 Physics Department, Lanzhou University, Lanzhou, China Probing nucleon structure by using a polarized proton
More informationMeson Structure with Dilepton Production
Meson Structure with Dilepton Production Jen-Chieh Peng University of Illinois at Urbana-Champaign 9 th Workshop on Hadron Physics in China and Opportunities Worldwide Nanjing University, July 24-28, 2017
More informationCentral Questions in Nucleon Structure
Central Questions in Nucleon Structure Werner Vogelsang BNL Nuclear Theory QCD and Hadron Physics Town Meeting, 01/13/2007 Exploring the nucleon: Of fundamental importance in science Know what we are made
More informationSixth International Conference on Perspectives in Hadronic Physics May Highlights from the COMPASS experiment at CERN.
1942-43 Sixth International Conference on Perspectives in Hadronic Physics 12-16 May 2008 Highlights from the COMPASS experiment at CERN. F. Bradamante University of trieste / INFN Trieste Italy HIGHLIGHTS
More informationDetermining Strangeness Quark Spin in Neutrino-Nucleon Scattering at J-PARC
Aug 25, 2004 NP04, KEK Determining Strangeness Quark Spin in Neutrino-Nucleon Scattering at J-PARC T.-A. Shibata (Tokyo Tech) in collaboration with N. Saito (Kyoto Univ) and Y. Miyachi (Tokyo Tech) for
More informationDrell-Yan experiments at Fermilab/RHIC/J-PARC. QCD Frontier 2013 Jefferson Lab October 21, 2013 Yuji Goto (RIKEN)
Drell-Yan experiments at Fermilab/RHIC/J-PARC QCD Frontier 2013 Jefferson Lab October 21, 2013 Yuji Goto (RIKEN) Outline Fermilab Drell-Yan experiments Unpolarized program Flavor asymmetry of sea-quark
More informationNucleon polarised parton distribution functions
Nucleon polarised parton distribution functions Gerhard K. Mallot CERN, 111 Geneva 3, Switzerland Abstract An introduction to the present status of spin-dependent parton distribution functions is given.
More informationExperimental Program of the Future COMPASS-II Experiment at CERN
Experimental Program of the Future COMPASS-II Experiment at CERN Luís Silva LIP Lisbon lsilva@lip.pt 24 Aug 2012 On behalf of the COMPASS Collaboration co-financed by THE COMPASS EXPERIMENT Common Muon
More informationSSA Measurements with Primary Beam at J-PARC
SSA Measurements with Primary Beam at J-PARC Joint UNM/RBRC Workshop on Orbital Angular Momentum in Albuquerque February 25 th, 2006 Yuji Goto (RIKEN/RBRC) February 25, 2006 Yuji Goto (RIKEN/RBRC) 2 Introduction
More informationSea-quark spin/flavor with Drell-Yan experiments. INT Workshop Orbital Angular Momentum in QCD February 15, 2012 Yuji Goto (RIKEN)
Sea-quark spin/flavor with Drell-Yan experiments INT Workshop Orbital Angular Momentum in QCD February 15, 2012 Yuji Goto (RIKEN) February 15, 2012 2 Outline Fermilab Drell-Yan experiments Unpolarized
More informationNucleon spin and parton distribution functions
Nucleon spin and parton distribution functions Jörg Pretz Physikalisches Institut, Universität Bonn on behalf of the COMPASS collaboration COMPASS Hadron 2011, Munich Jörg Pretz Nucleon Spin and pdfs 1
More informationPolarized Drell-Yan Experiment at J-PARC. J-PARC Meeting for Spin and Hadron Physics Nishina Hall at RIKEN April 7 th, 2008 Yuji Goto (RIKEN/RBRC)
Polarized Drell-Yan Experiment at J-PARC J-PARC Meeting for Spin and Hadron Physics Nishina Hall at RIKEN April 7 th, 2008 Yuji Goto (RIKEN/RBRC) J-PARC proposals P04: measurement of high-mass dimuon production
More informationTHE NUCLEUS AS A QCD LABORATORY: HADRONIZATION, 3D TOMOGRAPHY, AND MORE
rhtjhtyhy EINN 2017 NOVEMBER 1, 2017 PAPHOS, CYPRUS THE NUCLEUS AS A QCD LABORATORY: HADRONIZATION, 3D TOMOGRAPHY, AND MORE KAWTAR HAFIDI Argonne National Laboratory is a U.S. Department of Energy laboratory
More informationUpdate on the Hadron Structure Explored at Current and Future Facilities
3D Nucleon Tomography Workshop Modeling and Extracting Methodology Update on the Hadron Structure Explored at Current and Future Facilities Jianwei Qiu September 25-29, 2017 Salamanca, Spin Atomic Structure
More informationNucleon Spin. Tyler Corbett
Nucleon Spin Tyler Corbett Abstract: In 1988 the European Muon Collaboration showed that the quark contribution to spin only accounts for 20-30 percent of the nucleon spin; The "naive quark parton model
More informationLessons from Lepton-Nucleon and Lepton-Nuclei Interactions Probing the structure of the atomic nucleus
Lessons from Lepton-Nucleon and Lepton-Nuclei Interactions Probing the structure of the atomic nucleus Raphaël Dupré Disclaimer This will be only a selection of topics Like any review of a field I encourage
More informationGoodbye to Large G? Marek Karliner. Cambridge University and Tel Aviv University. with John Ellis, hep-ph/ ph/
Goodbye to Large G? Marek Karliner Cambridge University and Tel Aviv University with John Ellis, hep-ph/0501115 ph/0501115 LC2005, Cairns, 7/2005 nucleon spin quark helicities: q = Z 1 0 h q (x) q (x)
More informationTransverse SSA Measured at RHIC
May 21-24, 2007 Jefferson Lab Transverse SSA Measured at RHIC Jan Balewski, IUCF Exclusive Reactions Where does the proton s spin come from? p is made of 2 u and 1d quark S = ½ = Σ S q u u Explains magnetic
More informationExciting opportunities at JLab GeV!
Exciting opportunities at JLab 25-75 GeV! JLab users town meeting, Newport News! March 16 2012! Kawtar Hafidi! Develop a common vision for the future! The future starts today! 40 - Today (2012), we are
More informationRecent Development in Proton Spin Physics
Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720,USA RIKEN BNL Research Center, Building 510A, Brookhaven National Laboratory, Upton, NY 11973, USA E-mail: fyuan@lbl.gov
More informationerhic: Science and Perspective
erhic: Science and Perspective Study of the Fundamental Structure of Matter with an Electron-Ion Collider A. Deshpande, R. Milner, R. Venugopalan, W. Vogelsang hep-ph/0506148, Ann. Rev. Nucl. Part. Sci.
More information陽子スピンの分解 八田佳孝 ( 京大基研 )
陽子スピンの分解 八田佳孝 ( 京大基研 ) Outline QCD spin physics Proton spin decomposition: Problems and resolution Orbital angular momentum Twist analysis Transverse polarization Method to compute G on a lattice 1101.5989
More informationOverview of Low Energy Spin Structure Experiments
Overview of Low Energy Spin Structure Experiments Jian-ping Chen, Jefferson Lab, USA Spin Workshop at EINN015, Cyprus, November 4, 015! Introduction! Moments of Spin Structure Functions g1: GDH/Bjorken
More informationThe nucleon is an excitation of 3 quarks in the QCD vacuum. Understanding the vacuum structure and its properties, such as color confinement, is
The nucleon is an excitation of 3 quarks in the QCD vacuum. Understanding the vacuum structure and its properties, such as color confinement, is essential. Light quarks (up and down) are nearly massless,
More informationHall A/C collaboration Meeting June Xuefei Yan Duke University E Collaboration Hall A collaboration
Hall A SIDIS Hall A/C collaboration Meeting June 24 2016 Xuefei Yan Duke University E06-010 Collaboration Hall A collaboration The Incomplete Nucleon: Spin Puzzle [X. Ji, 1997] DIS DΣ 0.30 RHIC + DIS Dg
More informationFundamental Open Questions in Spin Physics
Fundamental Open Questions in Spin Physics p. 1/55 Fundamental Open Questions in Spin Physics Jacques Soffer Physics Department, Temple University, Philadelphia,PA, USA Fundamental Open Questions in Spin
More informationThe RHIC SPIN Program
2014 Draft The RHIC SPIN Program Achievements and Future Opportunities Writers, for the RHIC Spin Collaboration1 Elke-Caroline Aschenauer, Alexander Bazilevsky, James Drachenberg, Markus Diehl, Kjeld Oleg
More informationHERMES at HERA: Quark-Gluon Spin Structure of the Nucleon
HERMES at HERA: Quark-Gluon Spin Structure of the Nucleon Introduction The year 2002, marked the 75th anniversary of Dennison s discovery that the proton, just like the electron, carries spin. The electron
More informationThe Resolution of the Proton Spin Crisis
The Resolution of the Proton Spin Crisis Anthony W. Thomas JLab: October 5 th 2007 Outline A reminder: the proton spin crisis Progress over the last 20 years The resolution of the problem - one-gluon-exchange
More informationStudy of the hadron structure using the polarised Drell-Yan process at COMPASS
Study of the hadron structure using the polarised Drell-Yan process at COMPASS Márcia Quaresma, LIP - Lisbon on behalf of the COMPASS collaboration 7 th July 6, MENU 6 Kyoto COMPASS CERN/FIS-NUC/7/5 Márcia
More informationDeeply Virtual Compton Scattering off 4. He: New results and future perspectives
Deeply Virtual Compton Scattering off 4 He: New results and future perspectives M. Hattawy (On behalf of the CLAS collaboration) 2016 JLab Users Group Workshop and Annual Meeting June 20-22, Jefferson
More informationHERMES Status Report
HERMES Status Report Sergey Yaschenko for the Collaboration DESY PRC, Hamburg, April 1, 008 Outline Introduction Physics Highlights from HERMES Isoscalar extraction of ΔS Model-dependent constraint on
More informationTransverse Momentum Dependent Parton Distributions
Transverse Momentum Dependent Parton Distributions Feng Yuan Lawrence Berkeley National Laboratory 8/14/2012 1 Feynman Parton: one-dimension Inclusive cross sections probe the momentum (longitudinal) distributions
More informationHigh-energy hadron physics at J-PARC
KEK theory center workshop on Hadron and Nuclear Physics in 2017 KEK, January 7-10, 2017 High-energy hadron physics at J-PARC Wen-Chen Chang Institute of Physics, Academia Sinica Outline High-momentum
More informationFlavor Decomposition
SIDIS Workshop for PAC30 April 14, 2006 Flavor Decomposition in Semi-Inclusive DIS Wally Melnitchouk Jefferson Lab Outline Valence quarks unpolarized d/u ratio polarized d/d ratio Sea quarks flavor asymmetry
More informationNucleon Valence Quark Structure
Nucleon Valence Quark Structure Z.-E. Meziani, S. Kuhn, O. Rondon, W. Melnitchouk Physics Motivation Nucleon spin and flavor structure High-x quark distributions Spin-flavor separation Moments of structure
More informationJAMboree. Theory Center Jamboree Jefferson Lab, Dec 13, Pedro Jimenez Delgado
JAMboree Theory Center Jamboree Jefferson Lab, Dec 13, 2013 Introduction Hadrons composed of quarks and gluons scattering off partons Parton distribution functions Plausible at high energies (from GeV):
More informationLongitudinal Double Spin Asymmetry in Inclusive Jet Production at STAR
Longitudinal Double Spin Asymmetry in Inclusive Jet Production at STAR Katarzyna Kowalik for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley, California 94720 Abstract. This contribution
More informationCOMPASS results on inclusive and semi inclusive polarised DIS
COMPASS results on inclusive and semi inclusive polarised DIS Helena Santos LIP - Lisboa on behalf of the COMPASS Collaboration The nucleon spin The COMPASS experiment Longitudinal spin structure functions
More informationFlavor Decomposition of Nucleon Spin via polarized SIDIS: JLab 12 GeV and EIC. Andrew Puckett Los Alamos National Laboratory INT 09/24/2010
Flavor Decomposition of Nucleon Spin via polarized SIDIS: JLab 12 GeV and EIC Andrew Puckett Los Alamos National Laboratory INT 09/24/2010 Outline Nucleon Structure Nucleon spin structure Flavor decomposition
More informationHigh Energy Physics. Lecture 9. Deep Inelastic Scattering Scaling Violation. HEP Lecture 9 1
High Energy Physics Lecture 9 Deep Inelastic Scattering Scaling Violation HEP Lecture 9 1 Deep Inelastic Scattering: The reaction equation of DIS is written e+ p e+ X where X is a system of outgoing hadrons
More informationDeeply Virtual Compton Scattering off 4. He: New results and future perspectives
Deeply Virtual Compton Scattering off 4 He: New results and future perspectives M. Hattawy (On behalf of the CLAS collaboration) Next generation nuclear physics with JLab12 and EIC 10-13 February 2016,
More informationSpin-dependent PDFs at large x
Physics Opportunities at an Electron-Ion Collider (POETIC V) Yale University September 22, 24 Spin-dependent PDFs at large Wally Melnitchouk Outline Why is nucleon (spin) structure at large interesting?
More informationNucleon spin in perspective
Nucleon spin in perspective Barbara Badelek University of Warsaw and University of Uppsala Epiphany 009 Cracow, January 5 7, 009 B. Badelek (Warsaw ) Nucleon spin in perspective Epiphany 009 1 / 47 Introduction
More informationSpin Structure of the Proton and Deuteron
Spin Structure of the Proton and Deuteron K. Griffioen College of William & Mary griff@physics.wm.edu Spin Structure at Long Distances Jefferson Lab 12 March 2009 Inelastic Scattering Q 2 increases 12
More informationOverview of Science Goals, Golden Measurements and Implications for the Energy and Luminosity Reach of the EIC
Overview of Science Goals, Golden Measurements and Implications for the Energy and Luminosity Reach of the EIC Introduction and Motivation The Golden Measurements, University of Colorado Nucleon Quark-Gluon
More informationShape and Structure of the Nucleon
Shape and Structure of the Nucleon Volker D. Burkert Jefferson Lab Science & Technology Peer Review June 25-27, 2003 8/7/2003June 25, 2003 Science & Technology Review 1 Outline: From form factors & quark
More informationCOMPASS Drell-Yan Results and Future Prospect
COMPA Drell-Yan Results and Future Prospect Jen-Chieh Peng University of Illinois at Urbana-Champaign IN Workshop on he Flavor tructure of Nucleon ea Oct. 2-13, 2017 On behalf of COMPA Collaboration (hanks
More informationRecent STAR Jet Results of the High-Energy Spin Physics Program at RHIC
Recent STAR Jet Results of the High-Energy Spin Physics Program at RHIC Daniel L. Olvitt Jr. Temple University E-mail: daniel.olvitt@temple.edu The production of jets from polarized proton+proton collisions
More informationLepton Angular Distributions in Drell-Yan Process
Lepton ngular Distributions in Drell-Yan Process Jen-Chieh Peng University of Illinois at Urbana-Champaign QCD Evolution 08 Santa Fe May 0-4, 08 Based on the paper of JCP, Wen-Chen Chang, Evan McClellan,
More informationPANDA. antiproton Annihilation at DArmstadt
antiproton Annihilation at DArmstadt Physics programme Quark confinement: Charmonium spectroscopy Excited gluons: Exotic hybrid mesons & glueballs Nucleon spin puzzle: transverse quark spin distribution
More informationOverview of Jefferson Lab Physics Program. David Richards 1 st June, 2008 HUGS
Overview of Jefferson Lab Physics Program David Richards 1 st June, 2008 HUGS Why are we here? Describe how the fundamental building blocks of the nucleus, the protons and neutrons, are built from the
More informationStudying Evolution with Jets at STAR. Renee Fatemi University of Kentucky May 28 th, 2015
Studying Evolution with Jets at STAR Renee Fatemi University of Kentucky May 28 th, 2015 Relativistic Heavy Ion Collider Absolute Polarimeter (H jet) RHIC pc Polarimeters Siberian Snakes PHOBOS PHENIX
More informationPolarizing Helium-3 for down quark spin enrichment. Nigel Buttimore
Polarizing Helium-3 for down quark spin enrichment Nigel Buttimore Trinity College Dublin 12 September 2012 Diffraction 2012 Polarized Helium-3 OUTLINE Introduction to the spin structure of polarized protons
More informationCOMPASS Drell-Yan. Michela Chiosso, University of Torino and INFN. TMD ECT* Workshop April 2016
COMPASS Drell-Yan Michela Chiosso, University of Torino and INFN TMD ECT* Workshop 11-15 April 2016 Outline Single polarized Drell-Yan at COMPASS DY vs SIDIS at COMPASS Experimental setup Spin-dependent
More informationConstituent Quarks and the Gluonic Contribution to the Spin of the Nucleon
Constituent Quarks and the Gluonic Contribution to the Spin of the Nucleon Ludwig-Maximilians-Universität München Faculty of Physics Thesis submitted By Gamal Eldahoumi from Benghazi/Libya Munich January
More informationTransverse Spin Effects and k T -dependent Functions
Transverse Spin Effects and k T -dependent Functions Daniël Boer Free University, Amsterdam Outline Left-right single spin asymmetries Azimuthal spin asymmetries; Sivers and Collins effects Transversity
More informationCOMPASS Measurements of Asymmetry Amplitudes in the Drell-Yan Process Observed from Scattering Pions off a Transversely Polarized Proton Target
COMPASS Measurements of Asymmetry Amplitudes in the Drell-Yan Process Observed from Scattering Pions off a Transversely Polarized Proton Target University of Illinois E-mail: rsheitz2@illinois.edu On behalf
More informationPhysics of the Proton Spin Problem. Anthony W. Thomas
Physics of the Proton Spin Problem Anthony W. Thomas 10 th Circum-Pan-Pacific Symposium on High Energy Spin Physics Academia Sinica : October 6 th 2015 Background The structure of the proton is a fundamental
More informationOnline Evaluation der Lehrveranstaltung https://evaluation.physik.ruhr-uni-bochum.de/login.php. Preis: Netbook, 2. Preis: Buchgutschein über 00,- EUR, 3. Preis: Buchgutschein über 50,- EUR. Bitte informieren
More informationPossible relations between GPDs and TMDs
Possible relations between GPDs and TMDs Marc Schlegel, Theory Center, Jefferson Lab Hall C summer meeting: Physics opportunities in Hall C at 12 GeV Generalized Parton Distributions Exclusive processes
More informationTransverse Spin Structure with muon beam and Drell-Yan measurements at COMPASS
Transverse Spin Structure with muon beam and Drell-Yan measurements at COMPASS Anna Martin Trieste University and INFN on behalf of the COMPASS Collaboration SPIN-Praha Praha-009 ADVANCED STUDIES INSTITUTE
More informationLattice QCD and Hadron Structure
Lattice QCD and Hadron Structure Huey-Wen Lin University of Washington 1 Human Exploration Matter has many layers of structure 10 2 m 10 9 m Materials Molecules 10 15 m The scientific cycle Proton 2 Parton
More informationFlavor decomposition of collinear PDFs and FFs
EIC User Group Meeting CUA, Washington DC, August 1, 218 Flavor decomposition of collinear PDFs and FFs Wally Melnitchouk JLab Angular Momentum collaboration Outline Unravel flavor (and spin) structure
More informationModels of the Nucleon & Parton Distribution Functions
11th CTEQ Summer School on QCD Analysis and Phenomenology Madison, Wisconsin, June 22-30, 2004 Models of the Nucleon & Parton Distribution Functions Wally Melnitchouk Jefferson Lab Outline Introduction
More informationSmall angle (Low Q 2 ) GDH sum rule experiments
Small angle (Low Q 2 ) GDH sum rule experiments A. Deur Jefferson Lab. Outline: Sum rules, GDH, Bjorken, spin polarizability sum rules; Usefulness and context; Measurements (published, being analyzed,
More informationElectron-Ion Collider Taking us to the next QCD Frontier
QCD Evolution 2014 Workshop at Santa Fe, NM (May 12 16, 2014) Electron-Ion Collider Taking us to the next QCD Frontier Jianwei Qiu Brookhaven National Laboratory Acknowledgement: Much of the physics presented
More informationDouble-Longitudinal Spin Asymmetry in Single- Inclusive Lepton Scattering
QCD Evolution 2017, JLab, May 22-26, 2017 Double-Longitudinal Spin Asymmetry in Single- Inclusive Lepton Scattering Marc Schlegel Institute for Theoretical Physics University of Tübingen in collaboration
More informationSelected Results from the Nucleon Spin Program at Jefferson Lab
Selected Results from the Nucleon Spin Program at Jefferson Lab Xiaochao Zheng Univ. of Virginia October 17, 009 Challenges of the Standard Model and the Nucleon Spin Puzzle Thomas Jefferson National Accelerator
More informationQCD Collinear Factorization for Single Transverse Spin Asymmetries
INT workshop on 3D parton structure of nucleon encoded in GPD s and TMD s September 14 18, 2009 QCD Collinear Factorization for Single Transverse Spin Asymmetries Iowa State University Based on work with
More informationSPIN STRUCTURE OF THE NUCLEON AND POLARIZATION. Charles Y. Prescott Stanford Linear Accelerator Center Stanford University, Stanford CA 94309
SLAC-PUB-662 September 1994 (TE) SPIN STRUCTURE OF THE NUCLEON AND POLARIZATION Charles Y. Prescott Stanford Linear Accelerator Center Stanford University, Stanford CA 9439 Work supported by Department
More informationExperimental investigation of the nucleon transverse structure
Electron-Nucleus Scattering XIII Experimental investigation of the nucleon transverse structure Silvia Pisano Laboratori Nazionali di Frascati INFN. The unsolved proton How do the lagrangian degrees of
More informationPolarized Structure Functions
Polarized Structure Functions Gerard van der Steenhoven (NIKHEF) JLab, Newport News, 4 March 22 u u d 9 th Int. Conference on the Structure of Baryons Introduction The origin of spin in the baryon octet:
More informationQCD and the Spin Structure of the Nucleon
Graduiertenkolleg: Physik an Hadronbeschleunigern QCD and the Spin Structure of the Nucleon Gerhard K. Mallot CERN/PH 16 January 2013 Plan Introduction Tools: DIS SIDIS pp, Experiments Helicity structure
More informationCoherent and Incoherent Nuclear Exclusive Processes
Coherent and Incoherent Nuclear Exclusive Processes Vadim Guzey Electron-Ion Collider Workshop: Electron-Nucleon Exclusive Reactions Rutgers University, March 14-15, 2010 Outline Coherent and incoherent
More informationSpin dependent en cross section at small and medium Q2
NuInt04@Gran Sasso, 004/03/18 Session 3, Talk ID 3.5 Spin dependent en cross section at small and medium Q Contents: Introduction Kinematic DIS Regime (Q>1GeV, W>4GeV) Small Q Limit (Q=0 GeV) GDH sum rule
More informationGPDs and TMDs at Electron-Ion Collider. Workshop on hadron tomography at J-PARC and KEKB January 6 th, 2017 KEK, Tsukuba, Japan Yuji Goto (RIKEN)
GPDs and TMDs at Electron-Ion Collider Workshop on hadron tomography at J-PARC and KEKB January 6 th, 2017 KEK, Tsukuba, Japan Yuji Goto (RIKEN) Electron-Ion Collider World s first polarized electron +
More informationTransverse Target Asymmetry in Exclusive Charged Pion Production at 12 GeV
Transverse Target Asymmetry in Exclusive Charged Pion Production at 12 GeV Dipangkar Dutta Mississippi State University (with Dave Gaskell & Garth Huber) Polarized Target Workshop: June 17-18, 2010 Outline
More informationPresent and Future Exploration of the Nucleon Spin and Structure at COMPASS
Present and Future Exploration of the Nucleon Spin and Structure at COMPASS 1 2 3 4 5 6 Longitudinal spin structure Transverse spin structure Gluon polarization Primakov: pion polarizabilities DY: Transverse
More informationIterative Monte Carlo analysis of spin-dependent parton distributions
Iterative Monte Carlo analysis of spin-dependent parton distributions (PRD.93.745) Nobuo Sato In Collaboration with: W. Melnitchouk, S. E. Kuhn, J. J. Ethier, A. Accardi Precision Radiative Corrections
More informationPartonic Structure of Light Nuclei
Partonic Structure of Light Nuclei M. Hattawy - Physics motivations - Recent results from CLAS - Proposed measurements with CLAS12 INT 17-3, Thursday, August 31st 2017 EMC Effect EMC effect: the modification
More informationScale dependence of Twist-3 correlation functions
Scale dependence of Twist-3 correlation functions Jianwei Qiu Brookhaven National Laboratory Based on work with Z. Kang QCD Evolution Workshop: from collinear to non collinear case Thomas Jefferson National
More informationDeconstructing the Partonic Origins of the Proton Spin. Renee Fatemi University of Kentucky March 24th, 2016
Deconstructing the Partonic Origins of the Proton Spin Renee Fatemi University of Kentucky March 24th, 2016 The search for the Underlying Mechanisms of Matter drives many areas of science QUARKS are fundamental
More informationA High Luminosity Electron-Ion Collider to Study the Structure of Matter
A High Luminosity Electron-Ion Collider to Study the Structure of Matter Introduction Scientific motivation Realization Summary Study of the Fundamental Structure of Matter with an Electron-Ion Collider
More informationThe dbar/ubar Ratio in Proton
The dbar/bar Ratio in Proton Lingyan Zh HUGS 2009 1 What s the expection with dbar and bar? Peng & Garvey, Prog.Part.Ncl.Phys.47(2001)203 [+sbar]: 493.68 MeV K0[d+sbar]: 497.65 MeV π+[+dbar]: 139.57 MeV
More informationTHE GPD EXPERIMENTAL PROGRAM AT JEFFERSON LAB. C. Muñoz Camacho 1
Author manuscript, published in "XIX International Baldin Seminar on High Energy Physics Problems, Relativistic Nuclear Physics and Quantum Chromodynamics, Dubna : Russie (8)" THE GPD EXPERIMENTAL PROGRAM
More informationElectron-Ion Collider for Nuclear and Particle Physics. Hugh Montgomery Jefferson Lab
Electron-Ion Collider for Nuclear and Particle Physics Hugh Montgomery Jefferson Lab Input to this Talk Abhay Deshpande's EICAC talk to Jefferson Lab Users http://www.jlab.org/conferences/ugm/talks/monday/deshpande.pdf
More informationRealistic parameterization of GPDs and its applications. Simonetta Liuti University of Virginia. Jlab Theory Group Seminar November 10th, 2008.
Realistic parameterization of GPDs and its applications Simonetta Liuti University of Virginia Jlab Theory Group Seminar November 10th, 2008. Collaborations Gary Goldstein (Tufts University) Leonard Gamberg
More informationHall C SIDIS Program basic (e,e p) cross sections
Hall C SIDIS Program basic (e,e p) cross sections Linked to framework of Transverse Momentum Dependent Parton Distributions Validation of factorization theorem needed for most future SIDIS experiments
More informationPolarized parton distributions: present status and prospects
QCD@Work 23 - International Workshop on QCD, Conversano, Italy, 14 18 June 23 Polarized parton distributions: present status and prospects Giovanni Ridolfi a a INFN Sezione di Genova, Via Dodecaneso 33,
More informationTopics on QCD and Spin Physics
Topics on QCD and Spin Physics (sixth lecture) Rodolfo Sassot Universidad de Buenos Aires HUGS 21, JLAB June 21 Spin (revisited)? naive quark spin parton spin QCD parton spin polarized DIS:? EMC experiment:
More information