Exciting opportunities at JLab GeV!
|
|
|
- Mervyn Scott
- 5 years ago
- Views:
Transcription
1 Exciting opportunities at JLab GeV! JLab users town meeting, Newport News! March ! Kawtar Hafidi!
2 Develop a common vision for the future! The future starts today! 40 - Today (2012), we are JLab 6 GeV users! 42 - Tomorrow (2014), we will be JLab 12 GeV users! 58 - After tomorrow (2030), we will be JLab GeV users! JLab EIC RHIC EIC users! users!???? users! Politics apart: We need to come up with the best physics! program with comparable or lower cost facility!
3 Lepton-nucleon/nucleus facilities! JLab 25-75! JLab12 (nucleon) (nucleon)
4 A Possible Phase II : GeV Courtesy of Larry Cardman! Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 4 Strategic Planning Exercise
5 Courtesy of Larry Cardman! 50 GeV: Five Passes through Three 3.33 GeV Linacs 22 x C150 or 17 x C m long 400 m radius Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 5 Strategic Planning Exercise
6 High luminosity: Exclusive reactions Pion form factor! Q 2 F π Garth Huber & Dave Gaskell! JLab 50! EIC! The pion is the lightest and simplest QCD system! Study the transition to perturbative QCD regime in confined system!
7 3D Structure of the nucleon! Nucleon Spin Quark Spin Semi-inclusive processes and transverse momentum distributions! Quark / Nucleon Quark polariza4on Un Polarized Longitudinally Polarized Transversely Polarized U f 1 = h 1 = Nucleon Polariza0on L T f 1T = g 1 = g 1T = h 1L = h 1T = h 1T =
8 SIDIS Kinematic coverage:!e p e π + X Harut Avakian! 24 GeV 50 GeV For a given luminosity (30min of runtime with L = cm -2 s -1 ) and a given bin in hadron z and P T, higher energy provides higher counts and wider coverage in x and Q 2!
9 Higher energies leads to better Kinematic coverage:! Counts GeV GeV 50 GeV 0.9<P T <1.1 GeV 0.5<z<0.6 Counts Harut Avakian! 0.09<x<0.11 GeV 0.5<z< GeV 11 GeV x Wider x range allow studies of transverse distributions of sea quarks and gluons! P T 2(GeV 2 ) Wider P T range will be important in extraction of -dependences of PDFs! For a given luminosity and given bin in hadron z and P T, higher energy provides higher counts and wider coverage in x and P T to allow studies of correlations between longitudinal and transverse degrees of freedom!
10 Q 2 evolution of transverse momentum distributions! Counts <x< <P T < <z<0.6 Harut Avakian! GeV 10 2 Aybat,Prokudin&Rogers arxiv: ! Q 2 (GeV 2 ) For the same luminosity and bin in z and p T, higher energy provides higher counts and wider coverage in Q 2 allowing studies of Q 2 evolution of 3D partonic distributions in a wide Q 2 range!
11 Nucleon angular momentum! 24 GeV Ji Sum rule (1997)! Spin of quarks! Contribution:! Measured in DIS! Orbital angular momentum of quarks:! Input from Lattice! and measurements at JLab 12 GeV! Total angular momentum of gluons! Through the momentum sum rule and HERA DVMP with J/Psi data we have a glimpse on GPD H g! Nothing is known about GPD E g!
12 Peter Kroll! JLab Users Mee0ng 2011, Newport News, VA 3/16/12 12
13 A Golden Experimental Program! γ 0.10!""""""#!""""""#!!!! Courtesy of Zein-Eddine Meziani! J/ψ 0.08 AU T (J/Ψ) P. Kroll! t [GeV2] black: δe = 0.0, αe! = 0.25 blue: δe = ln (mc /GeV), αe! = 0.45 magenta: δe = 0.1, αe! = 0.15 AU T (Υ) nearly twice as large s = 55 GeV P Glue imaging using unpolarized targets and accessing gluon GPD H through exclusive meson production in the valence region! Transversely polarized nucleon to access gluon GPD E and the Spin Sum Rule.!!"#"$$% JLab Users Meeting 2011, Newport News, VA! $&% 3/16/12 13
14 A UT (J/ψ)! W = 8 GeV t = -0.7 GeV 2! K.H, Meziani & Mustapha! J. Koempel, P. Kroll, A. Metz & J. Zhou, arxiv: v1! 50 GeV electron beam! cm -2 s -1 luminosity! 90 days running! V1 V2 V3 V4 V Q 2 (GeV 2 )
15 Double spin asymmetry A LS (J/ψ) with longitudinally polarized proton target and polarimetry of the recoil proton! 0.6 W = 8 GeV t = -0.7 GeV 2! K.H, Meziani & Mustapha! A LS (J/ψ) E B = 75 GeV! L = cm -2 s -1! Beam time = 365 days! 0.3 E B = 50 GeV! V1 V2 V3 V4 V J. Koempel, P. Kroll, A. Metz & J. Zhou, arxiv: v1! Q 2 (GeV 2 )
16 Process fractions for charm production Photon-gluon fusion! 82% Resolved photons processes 0% 5% 10%
17 x vs Q 50 GeV electron beam! D 0 K - π + (3.8%) D *+ D 0 π + (68%)
18 Momentum and angular distribution of π + and K - from open charm! π + K π + K
19 ΔG/G Projections for open charm production A. El Alaoui & KH! JLab 50 GeV! 200 days running!
20 Summary & outlook! JLab GeV seems like a natural extension of JLab 12 although for the physics I am interested in, JLab 50 is even a better option than 11 GeV! It looks promising! Do we want and are we allowed to investigate further the JLab option?! What is the lab management position?! How about the nuclear physics community at large?!
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)
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 +
Deeply 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
THE 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
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.
Electron-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
Generalized Parton Distributions Program at COMPASS. QCD Evolution 2015
Generalized Parton Distributions Program at COMPASS Eric Fuchey (CEA Saclay) On behalf of COMPASS Collaboration QCD Evolution 2015 Thomas Jefferson National Accelerator Facility (May 26-30 2014) Generalized
JAMboree. 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):
erhic: 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.
Hadronization with JLab 6/12 GeV
Hadronization with JLab 6/12 GeV Next generation nuclear physics with JLab12 and EIC Florida International University February 10-13th, 2016 Lamiaa El Fassi (On behalf of EG2 and CLAS Collaborations) Outline
Experimental 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
Central 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
Gluons at high x in Nuclei at EIC
Gluons at high x in Nuclei at EIC in collaboration with: E. Chudakov, D. Higinbotham, C. Hyde, C. Weiss Jefferson Lab DNP 2015 Fall meeting, Santa Fe, NM Outline Motivation HERA and ZEUS experience EIC
Probing 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
Jefferson Lab 12 GeV Science Program
QCD Evolution Workshop 2014 International Journal of Modern Physics: Conference Series Vol. 37 (2015) 1560019 (8 pages) c The Author DOI: 10.1142/S2010194515600198 Jefferson Lab 12 GeV Science Program
Transverse 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
The Electron-Ion Collider: Exploring the science of Nuclear Femtography
The Nature of Hadron Mass and Quark-Gluon Confinement from JLab Experiments in the 12-GeV Era The Electron-Ion Collider: Exploring the science of Nuclear Femtography Jianwei Qiu Theory Center, Jefferson
Helicity: 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
MEIC Physics. Tanja Horn for the MEIC group. Jlab Users Meeting
MEIC Physics Tanja Horn for the MEIC group Jlab Users Meeting The Structure of the Proton Naïve Quark Model: proton = uud (valence quarks) QCD: proton = uud + uu + dd + ss + The proton sea has a non-trivial
E , E , E
JLab Experiments E12-09-017, E12-09-011, E12-09-002 First-Year of Hall C experiments towards a complete commissioning of the SHMS for precision experiments Spokespersons: P. Bosted, D. Dutta, R. Ent, D.
Project. 1 Introduction. EPJ Web of Conferences 66, (2014)
EPJ Web of Conferences 66, 6 (4) DOI:.5/ epjconf/ 4666 C Owned by the authors, published by EDP Sciences, 4 Probing Sea Quarks and Gluons: Project The Electron-Ion Collider Tanja Horn,a Catholic University
The Physics Program of CLAS12
1 The Physics Program of CLAS1 S. Niccolai a, for the CLAS collaboration a Institut de Physique Nucléaire d Orsay, Orsay (France) The experimental program to study nucleon structure at the 1-GeV upgraded
Deeply 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,
What is new about the Electron Ion Collider (EIC) in the US?
1 What is new about the Electron Ion Collider (EIC) in the US? We recommend a high-energy highluminosity polarized EIC as the highest priority for new facility construction following the completion of
Transverse 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
Physics Opportunities at the MEIC at JLab
Physics Opportunities at the MEIC at JLab Pawel Nadel-Turonski Jefferson Lab QCD Evolution Workshop, JLab, May 16, 2012 1 The physics program of an EIC Map the spin and spatial structure of sea quarks
Deeply Virtual Compton Scattering and Meson Production at JLab/CLAS
Deeply Virtual Compton Scattering and Meson Production at JLab/CLAS Hyon-Suk Jo for the CLAS collaboration IPN Orsay PANIC 2011 M.I.T. Cambridge - July 25, 2011 19th Particles & Nuclei International Conference
Present and Future of Polarized Target Experiment at CLAS12. Harut Avakian (JLab)
Present and Future of Polarized Target Experiment at CLAS12 Harut Avakian (JLab) CLAS Collaboration Meeting February 20th 1 QCD: from testing to understanding 0h DIS Testing stage: pqcd predictions observables
Experimental Overview Generalized Parton Distributions (GPDs)
Experimental Overview Generalized Parton Distributions (GPDs) Latifa Elouadrhiri Jefferson Lab Lattice Hadron Physics July 31 August 3, 2006 Outline Generalized Parton Distributions - a unifying framework
QCD 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
Plans to measure J/ψ photoproduction on the proton with CLAS12
Plans to measure J/ψ photoproduction on the proton with CLAS12 Pawel Nadel-Turonski Jefferson Lab Nuclear Photoproduction with GlueX, April 28-29, 2016, JLab Outline Introduction J/ψ on the proton in CLAS12
a medium energy collider taking nucleon structure beyond the valence region
EIC@JLAB a medium energy collider taking nucleon structure beyond the valence region Tanja Horn INT09-43W, Seattle, WA 19 October 2009 Tanja Horn, CUA Colloquium 1 A high-luminosity EIC at JLab Use CEBAF
Summary of Workshop on Spin of Nucleons from Low to High Energy Scales
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, 2015 1 Three Sessions of the Spin Workshop
Single and double polarization asymmetries from deeply virtual exclusive π 0 electroproduction
Single and double polarization asymmetries from deeply virtual exclusive π electroproduction University of Connecticut E-mail: kenjo@jlab.org Harut Avakian, Volker Burkert et al. (CLAS collaboration) Jefferson
Drell-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
COMPASS 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
The Electron-Ion Collider (EIC)
The Electron-Ion Collider (EIC) A. Accardi, R. Ent, V. Guzey, T. Horn, C. Hyde, P. Nadel-Turonski, A. Prokudin, C. Weiss,... + CASA / accelerator team + lots of JLab of users! JLab Users' Town Hall Meeting,
Measurements 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.
Overview 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
The Electron-Ion Collider
The Electron-Ion Collider Daria Sokhan UK Nuclear Physics Community Meeting, University of Warwick, 5th January 2017 Electron-Ion Collider World s first polarized electron-proton/light ion and electron-nucleus
3-D Imaging and the Generalized Parton Distribution Program at an Electron Ion Collider
Workshop on Precision Radiative Corrections for Next Generation Experiments 6 9 May 6, Jefferson Lab, Newport News VA 3-D Imaging and the Generalized Parton Distribution Program at an Electron Ion Collider
Strong interaction physics with an Electron Ion Collider
Strong interaction physics with an Electron Ion Collider C. Weiss (JLab), UNAM, Mexico City, 03 April 17 [E-mail] Internal structure of nucleon Quantum Chromodynamics Concepts and methods for structure
The Jlab 12 GeV Upgrade
The Jlab 12 GeV Upgrade R. D. McKeown Jefferson Lab College of William and Mary 1 12 GeV Science Program The physical origins of quark confinement (GlueX, meson and baryon spectroscopy) The spin and flavor
Hadron Physics with Real and Virtual Photons at JLab
Hadron Physics with Real and Virtual Photons at JLab Elton S. Smith Jefferson Lab Virtual photons shape of the nucleon Elastic scattering (form factors) Inelastic scattering (uark distributions) Exclusive
GPDs. -- status of measurements -- a very brief introduction prerequisites and methods DVCS & DVMP: selected results on the way to an EIC
Delia Hasch GPDs -- status of measurements -- a very brief introduction prerequisites and methods & DVMP: selected results on the way to an EIC see additional slides for results not covered POETIC 01,
Generalized Parton Distributions and Nucleon Structure
Generalized Parton Distributions and Nucleon Structure Volker D. Burkert Jefferson Lab With pqcd established we have the tool to understand matter at a deeper level. Nobel prize 2004 - D. Gross, D. Politzer,
Studies of OAM at JLAB
Studies of OAM at JLAB Harut Avakian Jefferson Lab UNM/RBRC Workshop on Parton Angular Momentum, NM, Feb 2005 Introduction Exclusive processes Semi-Inclusive processes Summary * In collaboration with V.Burkert
Next-generation nuclear physics with JLab12 and EIC
Next-generation nuclear physics with JLab12 and EIC Topical Workshop, Florida International University, 10 13 Feb 2016 W. Brooks, R. Dupre, Ch. Hyde, M. Sargsian, C. Weiss (Organizers) Welcome! Physics
Simulation of measured DVCS cross-section on STAR Detector
Simulation of measured DVCS cross-section on STAR Detector XXX October 0, 01 Abstract Cross-section measurements of DVCS process in a proposed electron ion collider (EIC at RHIC are simulated. The acceptance
Imaging the Proton via Hard Exclusive Production in Diffractive pp Scattering
Exclusive Reactions at High Momentum Transfer Jefferson Lab, Newport News, VA May 21-24, 2007 Imaging the Proton via Hard Exclusive Production in Diffractive pp Scattering Charles Earl Hyde Old Dominion
Proposal Physics Contact Rating Days Group New equipment Energy Run Group Target
Run Groups Proposal Physics Contact Rating Days Group New equipment Energy Run Group Target E12-06-8 Hard exclusive electro-production of π 0, η Stoler B 80 E12-06-8A Exclusive N*->KY Studies with CLAS12
Overview 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
Spin 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
PoS(CD12)001. Overview of Nuclear Physics at Jefferson Lab. R. D. McKeown Thomas Jefferson National Accelerator Facility
Overview of Nuclear Physics at Jefferson Lab Thomas Jefferson National Accelerator Facility E-mail: bmck@jlab.org The Continuous Electron Beam Accelerator Facility (CEBAF) and associated experimental equipment
Hall 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
Experimental 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
Polarized deuterium physics with EIC C. Weiss (JLab), Tensor Polarized Solid Target Workshop, JLab, 11 Mar 14
Polarized deuterium physics with EIC C. Weiss (JLab), Tensor Polarized Solid Target Workshop, JLab, 11 Mar 14 1 e e x, 0000000 1111111 D pol. Q 2 X p, n Electron-Ion Collider overview Design specifications
Coherent 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
hunting the OAM Delia Hasch a very brief review of the spin sum rule observables of OAM some attempts to quantify OAM conclusion
INT workshop on gluons and the quark sea at high energies, INT Seattle, Sep-Nov, 2010 Delia Hasch hunting the OAM a very brief review of the spin sum rule observables of OAM some attempts to quantify OAM
Electron-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
Overview on the Future Electron-Ion Collider Projects
Overview on the Future Electron-Ion Collider Projects Emlyn W. Hughes W.K. Kellogg Radiation Laboratory California Institute of Technology Pasadena, CA 91125 Abstract. One of the large new projects envisioned
Summary of subtopic Imaging QCD Matter : Generalized parton distributions and exclusive reactions
Summary of subtopic Imaging QCD Matter : Generalized parton distributions and exclusive reactions of weeks 8 and 9 of the INT program Gluons and the quark sea at high energy: distributions, polarization,
The Detector Design of the Jefferson Lab EIC
The Detector Design of the Jefferson Lab EIC Jefferson Lab E-mail: mdiefent@jlab.org The Electron-Ion Collider (EIC) is envisioned as the next-generation U.S. facility to study quarks and gluons in strongly
Measuring the gluon Sivers function at a future Electron-Ion Collider
Measuring the gluon Sivers function at a future Electron-Ion Collider Speaker: Liang Zheng Central China Normal University In collaboration with: E.C. Aschenauer (BNL) J.H.Lee (BNL) Bo-wen Xiao (CCNU)
The Neutral-Particle Spectrometer
The Neutral-Particle Spectrometer White Paper outlining the Science and Path to Realization of the NPS The Neutral-Particle Spectrometer (NPS) Collaboration at Jefferson Lab November 26, 2014 The two-arm
The Jefferson Lab 12 GeV Program
The Jefferson Lab 12 GeV Program The Jefferson Lab facilities have undergone a substantial upgrade, both of accelerator, CEBAF, and of the experimental installations. We will discuss the progress to completion
An Electron Ion Collider in China Xurong Chen
An Electron Ion Collider in China Xurong Chen The Institute of Modern Physics CAS, Lanzhou, China 1 EIC@China Project IMP Introduction and HIAF Project EIC@HIAF Project 3 GeV (pol. e) X 12 GeV (pol. p),
Contributions to our Understanding of TMDs from Polarized Proton Collisions at STAR
Contributions to our Understanding of TMDs from Polarized Proton Collisions at STAR Stephen Trentalange University of California at Los Angeles, for the STAR Collaboration QCD-N16 Bilbao, Spain July 15,
Measuring Form Factors and Structure Functions With CLAS
Measuring Form Factors and Structure Functions With CLAS Jerry Gilfoyle for the CLAS Collaboration Physics Department, University of Richmond, Virginia Outline: 1. Jefferson Lab and the CLAS Detector..
An Assessment of U.S.-Based Electron-Ion Collider Science
BOARD ON PHYSICS AND ASTRONOMY (BPA) An Assessment of U.S.-Based Electron-Ion Collider Science A study under the auspices of the U.S. National Academies of Sciences, Engineering, and Medicine Gordon Baym
Generalized TMDs in Hadronic collisions. Shohini bhattacharya Temple university Light cone 2018
Generalized TMDs in Hadronic collisions Shohini bhattacharya Temple university Light cone 2018 OUTLINE Generalized TMDs (GTMDs) Quark GTMDs in Exclusive Double Drell-Yan Process (S. Bhattacharya, A. Metz,
Progress on the DVCS program at Compass E. Burtin CEA Saclay Irfu/SPhN GDR nucléon, Ecole Polytechnique, 12 décembre 2008
Progress on the DVCS program at Compass E. Burtin CEA Saclay Irfu/SPhN GDR nucléon, Ecole Polytechnique, 12 décembre 2008 Today and tomorrow 2010 and beyond 2008 (Today) : Target region Ring B Ring A 2008
Nucleon 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
TMDs at Electron Ion Collider Alexei Prokudin
TMDs at Electron Ion Collider Alexei Prokudin 2 3 Why Electron Ion Collider? Eur. Phys. J. A (2016) 52: 268 DOI 10.1140/epja/i2016-16268-9 THE EUROPEAN PHYSICAL JOURNAL A Review Electron-Ion Collider:
Opportunities in low x physics at a future Electron-Ion Collider (EIC) facility
1 Opportunities in low x physics at a future Electron-Ion Collider (EIC) facility Motivation Quantum Chromo Dynamics Proton=uud Visible Universe Galaxies, stars, people, Silent Partners: Protons & Neutrons
The Electron-Ion Collider at BNL: Capabilities and Physics Highlights
Hadron 2011 Munich 1 The Electron-Ion Collider at BNL: Capabilities and Physics Highlights D. Leinweber J.H. Lee Brookhaven National Laboratory Outline Why do we need electron-ion collider What can we
Exclusive Physics with the HERMES Recoil Detector
Exclusive Physics with the HERMES Recoil Detector Erik Etzelmüller on behalf of the HERMES Collaboration!!! workshop on! Exploring Hadron Structure with Tagged Structure Functions! Thomas Jefferson National
Timelike Compton Scattering
Timelike Compton Scattering Tanja Horn In collaboration with: Y. Illieva, F.J. Klein, P. Nadel-Turonski, R. Paremuzyan, S. Stepanyan 12 th Int. Conference on Meson-Nucleon Physics and the Structure of
Lessons 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
Development of a framework for TMD extraction from SIDIS data. Harut Avakian (JLab)
Development of a framework for TMD extraction from SIDIS data Harut Avakian (JLab) DPWG, JLab, 2015, Oct 22 Spin-Azimuthal asymmetries in SIDIS Defining the output (multiplicities, asymmetries, ) Examples
Probing the Intrinsic Charm in the nucleon at EIC. Ahmed El Alaoui POETIC2012 Workshop, Bloomington, IN August 20-22, 2012
Probing the Intrinsic Charm in the nucleon at EIC Ahmed El Alaoui POETIC2012 Workshop, Bloomington, IN August 20-22, 2012 Outline Motivation Extraction of Intrinsic charm component from D meson electroproduction
Partonic 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
Asmita Mukherjee Indian Institute of Technology Bombay, Mumbai, India
. p.1/26 Sivers Asymmetry in e + p e + J/ψ + X Asmita Mukherjee Indian Institute of Technology Bombay, Mumbai, India Single spin asymmetry Model for J/ψ production Formalism for calculating the asymmetry
TMD Theory and TMD Topical Collaboration
3D Nucleon Tomography Workshop Modeling and Extracting Methodology March 15-17, 2017 Jefferson Lab, Newport News, VA TMD Theory and TMD Topical Collaboration Jianwei Qiu Theory Center, Jefferson Lab 3D
Recent transverse spin results from STAR
1 STAR! Recent transverse spin results from STAR Qinghua Xu, Shandong University PanSpin215, Taipei, October 8, 215! Outline 2 Introduction Single spin asymmetries in the forward region Mid-rapidity hadron-jet
Opportunities in Hadron Structure. Guided by Key Questions
Opportunities in Hadron Structure Overarching Goal: Explore and Understand QCD Guided by Key Questions 1. What is the role of gluons in nucleons and nuclei? Gluons 2. What is the internal spin and flavor
Quark/gluon orbital motion and nucleon spin. Alexei Prokudin. JLab December 8, Alexei Prokudin,
Quark/gluon orbital motion and nucleon spin Alexei Prokudin JLab December 8, 20 EIC Golden Topic # 2 talk Bob McKeown @ INT workshop Map the spin and spatial quark-gluon structure of nucleons Image the
QCD Factorization and Transverse Single-Spin Asymmetry in ep collisions
QCD Factorization and Transverse Single-Spin Asymmetry in ep collisions Jianwei Qiu Brookhaven National Laboratory Theory seminar at Jefferson Lab, November 7, 2011 Jefferson Lab, Newport News, VA Based
The Longitudinal Photon, Transverse Nucleon, Single-Spin Asymmetry in Exclusive Pion Production
The Longitudinal Photon, Transverse Nucleon, Single-Spin Asymmetry in Exclusive Pion Production Garth Huber SoLID Collaboration, Jefferson Lab, May 15, 2015. Complementarity of Different Reactions Deep
arxiv: v1 [nucl-ex] 3 Sep 2018
![arxiv: v1 [nucl-ex] 3 Sep 2018](/thumbs/96/129176849.jpg "arxiv: v1 [nucl-ex] 3 Sep 2018")
A Plan for Electron Ion Collider in China arxiv:89.448v [nucl-ex] 3 Sep 28 Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou, 73, China E-mail: xchen@impcas.ac.cn One of the frontier research
Update 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
THE 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
Shape 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
Probing Nuclear Color States with J/Ψ and φ
Probing Nuclear Color States with J/Ψ and φ Michael Paolone Temple University Next Generation Nuclear Physics with JLab12 and the EIC FIU - Miami, Florida February 12th 2016 J/Ψ and φ experiments at a
Quarkonium 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
MEIC Central Detector Zhiwen Zhao for JLab MEIC Study Group
MEIC Central Detector Zhiwen Zhao for JLab MEIC Study Group MEIC Collaboration Meeting 2015/10/07 MEIC Design Goals Energy Full coverage of s from 15 to 65 GeV Electrons 3-10 GeV, protons 20-100 GeV, ions
Possible 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
Electron Ion Collider: The next QCD frontier Understanding the Glue that Binds Us All
Abhay Deshpande arxiv 1212.1701.v3 Eur. Phy. J. A52, 9 (2016) Electron Ion Collider: The next QCD frontier Understanding the Glue that Binds Us All EIC Project Overview and The Path Forward Nuclei QCD:
The JLAB12 Collaboration
The JLAB12 Collaboration M.Battaglieri on behalf of the JLAB12 Collaboration INFN -GE, Italy 1 The CEBAF parameters Primary Beam: Electrons Beam Energy: 4 GeV (original) 6 GeV now 10 > λ > 0.1 fm 12 GeV
Hall 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
Measuring the gluon Sivers function at a future Electron-Ion Collider
Measuring the gluon Sivers function at a future Electron-Ion Collider Speaker: Liang Zheng Central China Normal University In collaboration with: E.C. Aschenauer (BNL) J.H.Lee (BNL) Bo-wen Xiao (CCNU)