An Electron Ion Collider at HIAF

Slides:



Advertisements
Similar presentations
April 06, 2005 JLab 12 GeV upgrade DOE Science Review 1 Fundamental Structure of Hadrons Zein-Eddine Meziani April 06, 2005 DOE Science Review for JLab.
Advertisements

Rolf Ent, ECT-Trento, October 28, 2008 Spin/Flavor Physics with a Future Electron-Ion Collider Electron-Ion Collider: Options and Status (in US) Gluons.
Longitudinal Spin at RHIC 29 th Winter Workshop on Nuclear Dynamics February 7, 2013 Cameron McKinney.
Probing Nucleon Structure at an Electron Ion Collider Long Range Plan Joint Town Meeting on QCD Temple University, Philadelphia September 14, /14/141LRP.
Physics with Polarized Beams at an Electron Ion Collider EIC International Users Meeting Stony Brook University Stony Brook, New York June 24-27, 2014.
Future Sino-US Collaboration in QCD Phyics Ten-Year Anniversary of STAR-China Collaboration Haiyan Gao 高海燕 Duke University 1.
The Science of an EIC Nuclear Science Goals: How do we understand the visible matter in our universe in terms of the fundamental quarks and gluons of QCD?
Working Group on e-p Physics A. Bruell, E. Sichtermann, W. Vogelsang, C. Weiss Antje Bruell, JLab EIC meeting, Hampton, May Goals of this parallel.
An Electron Ion Collider Plan in China Xurong Chen The Institute of Modern Physics CAS, Lanzhou, China The 21st International Symposium on Spin Physics.
Working Group on e-p Physics A. Bruell, E. Sichtermann, W. Vogelsang, C. Weiss Antje Bruell, JLab EIC meeting, Stony Brook, Dec Physics Topics Working.
9/19/20151 Nucleon Spin: Final Solution at the EIC Feng Yuan Lawrence Berkeley National Laboratory.
9/19/20151 Semi-inclusive DIS: factorization Feng Yuan Lawrence Berkeley National Laboratory RBRC, Brookhaven National Laboratory.
THE DEEP INELASTIC SCATTERING ON THE POLARIZED NUCLEONS AT EIC E.S.Timoshin, S.I.Timoshin.
Experimental Study of Single Spin Asymmetries and TMDs Jian-ping Chen, Jefferson Lab QCD Evolution Workshop, JLab, May 6-10, 2013  Recent SSA Results.
Future Opportunities at an Electron-Ion Collider Oleg Eyser Brookhaven National Laboratory.
1 Flavor Symmetry of Parton Distributions and Fragmentation Functions Jen-Chieh Peng Workshop on “Future Prospects in QCD at High Energy” BNL, July 17-22,
Deeply Virtual Exclusive Reactions with CLAS Valery Kubarovsky Jefferson Lab ICHEP July 22, 2010, Paris, France.
 Nucleon spin structure and Imaging in the Valence quark region ➥ Inclusive measurements at large x; quark models tests and Lattice QCD tests ➥ Exclusive.
Spin Azimuthal Asymmetries in Semi-Inclusive DIS at JLAB  Nucleon spin & transverse momentum of partons  Transverse-momentum dependent distributions.
UK Hadron Physics D. G. Ireland 10 October 2014 NuPECC Meeting, Edinburgh.
Experimental Approach to Nuclear Quark Distributions (Rolf Ent – EIC /15/04) One of two tag-team presentations to show why an EIC is optimal to access.
Columbia University Christine Aidala September 4, 2004 Solving the Proton Spin Crisis at ISSP, Erice.
Deliverablesobservables what we learn requirementscomments/competition HP13 (2015) Test unique QCD predictions for relations between single-transverse.
POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF.
Hadronic Multi-particle Final State Measurements with CLAS at Jefferson Lab Laird Kramer Florida International University Neutrino Scattering, March 2003.
1 Transversely polarized target for CLAS and CLAS12  Introduction  Structure of nucleon and 3D parton distributions  Semi-Inclusive processes and TMD.
Spin-Flavor Decomposition J. P. Chen, Jefferson Lab PVSA Workshop, April 26-27, 2007, Brookhaven National Lab  Polarized Inclusive DIS,  u/u and  d/d.
Detector requirement form TMD working group J. P. Chen for the TMD working group June 5, 2010, EIC Detector Workshop, JLab TMD Program - A lot of enthusiasm,
May 18-20, 2005 SIR05 JLab 1 P ? Dependence of SSA -- from nonpert. to pert. Feng Yuan, RBRC, Brookhaven National Laboratory References: Ji, Ma, Yuan,
Zhongbo Kang Los Alamos National Laboratory QCD structure of the nucleon and spin physics Lecture 5 & 6: TMD factorization and phenomenology HUGS 2015,
Future Physics at JLab Andrew Puckett LANL medium energy physics internal review 12/14/
1 EIC Update R. D. McKeown Presentation to EICAC April 10, 2011 (Thanks to R. Ent, A. Hutton, H. Montgomery, M. Farkhondeh, others)
General Discussion some general remarks some questions.
A feasibility study for measurements using electroweak probes at the proposed Electron-Ion Collider: Investigating nucleon structure and the fundamental.
Single-Spin Asymmetries at CLAS  Transverse momentum of quarks and spin-azimuthal asymmetries  Target single-spin asymmetries  Beam single-spin asymmetries.
Operated by the Southeastern Universities Research Association for the U. S. Department of Energy Thomas Jefferson National Accelerator Facility Rolf Ent.
The Quark Structure of the Nucleon Inti Lehmann & Ralf Kaiser University of Glasgow Cosener’s House Meeting 23/05/2007 Nucleon Structure Generalised Parton.
1 Probing Spin and Flavor Structures of the Nucleon with Hadron Beams Flavor and spin structures of the nucleons –Overview and recent results Future prospects.
Measurements with Polarized Hadrons T.-A. Shibata Tokyo Institute of Technology Aug 15, 2003 Lepton-Photon 2003.
EIC — Bring the Glue to Light. Gluons dominate QCD QCD is the fundamental theory that describes structure and interactions in nuclear matter. Without.
The 12 GeV Physics Program at Jefferson Lab R. D. McKeown Jefferson Lab College of William and Mary PTSP 2013 – Charlottesville, VA September 9, 2013.
R.G. Milner2nd EIC Workshop Summary and Outlook science case machine design EIC realization.
Thomas Jefferson National Accelerator Facility Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Anthony.
2/10/20161 What can we learn with Drell-Yan in p(d)-nucleus collisions Feng Yuan Lawrence Berkeley National Laboratory RBRC, Brookhaven National Laboratory.
TMD flavor decomposition at CLAS12 Patrizia Rossi - Laboratori Nazionali di Frascati, INFN  Introduction  Spin-orbit correlations in kaon production.
Nu Xu1/7STAR Analysis Meeting, Junior Meeting, April 16 th, 2012, BNL STAR STAR Experiment Nu Xu - Introduction: Structure of the QCD Matter - Near future.
3/8/20161 Nucleon Tomography --Parton Imaging in 3D Feng Yuan Lawrence Berkeley National Laboratory.
Transverse Momentum Dependent Evolution in Proton-Proton Collisions Oleg Eyser RIKEN/BNL Research Center Workshop Emerging Spin and Transverse Momentum.
JEFFERSON LAB CLOSE-OUT 6 GeV  Finish analysis on CLAS eg1-DVCS (SSAs + DSAs in   production with longitudinally polarized H and D targets) and.
Exclusive Vector Meson Electroproduction at 12 GeV Paul Stoler Rensselaer Polytechnic Institute.
Transverse Spin Physics with an Electron Ion Collider Oleg Eyser 4 th International Workshop on Transverse Polarisation Phenomena in Hard Processes Chia,
6/28/20161 Future Challenges of Spin Physics Feng Yuan Lawrence Berkeley National Laboratory.
The goal of the COMPASS" workshop at CERN on 4 March 2010 at CERN on 4 March 2010 is to better define the key measurements and their outcomes with.
1 Proton Structure Functions and HERA QCD Fit HERA+Experiments F 2 Charged Current+xF 3 HERA QCD Fit for the H1 and ZEUS Collaborations Andrew Mehta (Liverpool.
EIC NAS review Charge-2 What are the capabilities of other facilities, existing and planned, domestic and abroad, to address the science opportunities.
Flavor decomposition at LO
A Chinese Electron-Ion Collider
Electroweak physics at an EIC
Long-range plan of nuclear physics in Japan
EIC Plan at HIAF Xurong Chen The Institute of Modern Physics (IMP)
Explore the new QCD frontier: strong color fields in nuclei
Physics of the EIC Cyrille Marquet Theory Division - CERN.
EIC NAS review Charge-2 What are the capabilities of other facilities, existing and planned, domestic and abroad, to address the science opportunities.
Measurements of quark transversity and orbital motion in hard scattering Yoshiyuki Miyachi Tokyo Institute of Technology.
3/19/20181 Nucleon Spin: Final Solution at the EIC Feng Yuan Lawrence Berkeley National Laboratory.
Gordon Cates, Xiaochao Zheng, Yuxiang Zhao LOI
Selected Physics Topics at the Electron-Ion-Collider
Large-X PDFs in the Drell-Yan Process
PHENIX Transverse-Spin Physics
Feedback from the Temple Town Meeting MEIC Accelerator R&D Meeting
Presentation transcript:

An Electron Ion Collider at HIAF Xurong Chen for the EIC@HIAF study group The Institute of Modern Physics, CAS, Lanzhou, China The 5th Workshop on Hadron Physics in China and Opportunities in USA Huangshan, July 3, 2013

Outline Introduction to IMP EIC@HIAF Physics and Simulations Conclusions

The Institute of Modern Physics (IMP) The institute of Modern Physics(IMP) was founded in 1957. It is affiliated with Chinese Academy of Science (CAS) The national Laboratory for the heavy Ion Research Facility in Lanzhou was established at the IMP in 1991. IMP mainly focuses on basic research in heavy ion physics and its related interdisciplinary science There are about 800 scientists and engineers, including two academicians of CAS and 60 full professors IMP is one of the well-known research centers of low-and intermediate energy heavy ion physics in the world.

IMP @ Lanzhou

Main EIC plans in the world EIC@HIAF LHC  LHeC RHIC  eRHIC CEBAF  MEIC/EIC HERA FAIR  ENC

The Layout of HIAF Complex 2.4GeV ER eLinac-Ring 2.4 GeV (e) 3.0×1013 ICR-43 12.0 GeV (p) 4.1×1012 Key Characteristics: High energy & High intensity & Pulse Cooled intense primary beam & RIBs Beam compression Super long period slow extraction Multi-operation modes CBR-13/12 3.9ms/turn, 173turns, 680 ms (A=400,ε=2.3, f=1.5) ABR-20/18 3.0 GeV (p) 2.8×1012 SLinac 0.34 GeV/u (238U34+) 2.7×1011 17 MeV/u (U34+) 50 MeV/u (p) 40 pmA 5 Hz, 430 μs 1 pmA 1 Hz, 680 μs 6.2ms/turn, 70turns, 430 ms (A=400,ε=5.7, f=1.5) For more details, see Jiancheng Yang’s talk 6 6

Lepton-Nucleon Facilities EIC@HIAF: e(2.4 GeV) +p(12 GeV), both polarized, L = 4 x 1032cm2/s HIAF

e(2.4 GeV) +p(12 GeV), both polarized, L = 4 x 1032cm2/s EIC@HIAF Kinematic Coverage Comparison with JLab 12 GeV e(2.4 GeV) +p(12 GeV), both polarized, L = 4 x 1032cm2/s EIC@HIAF Phase-1: ~2019: 2.4 x12 GeV Both e and p polarized Luminosity: 4 x 1032cm2/s EIC@HIAF Phase-2: ~2030 10 x 100 GeV EIC@HIAF: study sea quarks (x > 0.01) deep exclusive scattering at Q2 > 5-10 higher Q2 in valance region

Unified view of nucleon structure EIC – 3D imaging of nucleon structure: TMDs – confined motion in a nucleon (semi-inclusive DIS) GPDs – Spatial imaging of quarks and gluons (exclusive DIS)

The Unique Advantages of EIC@HIAF The main theme for JLab 12 GeV is the study of the valance quark structure (and confinement) The main theme for full EIC (eRHIC, ELIC, LHeC…) is to understand the gluons The energy reach of the EIC@HIAF is higher than JLab 12GeV but lower than the full EIC being considered in US (at about the lower end) EIC@HIAF phase-1 (3GeV e x 12 GeV p): x is in region[0.01,0.1]. It’s the best region for sea quark study

Spin-Flavor Study at EIC@HIAF Unique opportunity for Δs JLab12 GeV energy not high enough to have clean Ds measurements But, EIC@HIAF, combination of energy and luminosity: By semi-inclusive DIS, in particular, for Kaons , will help to identify strange quark helicity

TMD Study at EIC@HIAF Unique opportunity for TMD in “sea quark” region reach x ~ 0.01 (JLab12 mainly valence quark region, reach x ~ 0.1) Semi-inclusive DIS, for charged hadrons, to measure TMD sea quark distributions Charm-pair production to measure TMD gluon distributions Significant increase in Q2 range for valence region energy reach Q2 ~40 GeV2 at x ~ 0.4 (JLab12, Q2 < 10)

GPD Study at EIC@HIAF Significant increase in range for DVCS Extend the kinematics covered by JLab Unique opportunity for Deeply virtual meson production (DVMP) (pion/Kaon) flavor decomposition needs DVMP energy reach Q2 > 5-10 GeV2 JLab12 energy not high enough to have clean light meson deep exclusive process which is the case for EIC@HIAF design

Hadron Physics at EIC@HIAF Many aspects of hadron’s partonic structure can be naturally addressed by EIC, but, not other machines: e+ e-, pp, pA, AA There are a lot to be done in the meson (including exotic meson) and X-Y-Z particles, where EIC might have an important role to play

Golden Measurements at EIC@HIAF To measure strange quark polarization in kaon Semi-inclusive DIS production TMD Sivers function in Semi-inclusive DIS, Q2 evolution, etc. DVCS/DVMP, to measure quark orbital angular momentum Quark propagation in medium to compare with heavy ion collisions

EIC@HIAF meeting The 2nd International workshop on QCD and Hadron Physics, March 30-April 3, 2013, Lanzhou QCD and hadron physics EIC Physics EIC@HIAF

EIC@HIAF meeting The four experiments were re-affirmed as good candidates for golden measurements Some of the unique advantages of the EIC@HIAF (comparing to fixed target experiments) for SIDIS study were emphasized (Ahbay and Elka), especially the clean separation of the current fragmentation from the target fragmentation (Delta_s, TMDs and hadronization clean measurements) Adjustability of beam energy is needed for flavor separation of GPD study (which is the case for EIC@HIAF design) We decided to do simulation and whitepaper at once, and should be done before July 2013

Two More Golden Measurements Craig Roberts: Pointed out the importance of higher Q2 EIC@HIAF will provide (comparing to JLab12), which are essential for clean measurement in the valence quark region Suggests: (5) the pion and kaon structure function measurment, which can be a benchmark experiment to test non-perturbative QCD calculations Eli: (6): EMC-SRC measurement: which will be a high impact experiment if EIC@HIAF can make precision measurement

Simulation Progress Xiaodong Jiang's group (Los Alamos) is doing the sea-quark polarization simulation and it has been done The TMD simulation is done by Haiyan's group (Duke). The plot is being finalized. The GPD group (Saclay/ODU/JLab) is doing the GPD (DVMP with pi/K) simulation, they are trying to produce results Paul Reimer (Argonne) is doing the pion structure function simulation. Craig has produced first draft of a write-up

The TMD simulation: Projections for SIDIS Asymmetry π+ By Haiyan’s group EIC@HIAF may reach the same precision with SoLID

Sea Quark Sivers Function we can clearly see that the EIC will be a powerful facility enabling access to TMDs with unprecedented precision, and particularly in the currently unexplored sea quark region This precision is not only crucial for the fundamental QCD test of the sign change between the Sivers asymmetries in the DIS and Drell-Yan processes, but also important to investigate the QCD dynamics in the hard processes in SIDIS Exploration of the sea quark Sivers function will provide, for the first time, the unique information on the spin-orbital correlation in the small-x region

Simulated errors for pi structure function measurement By Paul E. Reimer Simulated errors for DIS events using a 3 GeV electron beam on a 12 GeV proton beam with a luminosity of 5 x 1032 cm−2 s−1 and 106 s of running. A precise result could be obtained on the domain x <= 0.9

Our Future Plan Physics Simulations (will be done very soon) Detector simulations Whitepaper writing Jianwei Qiu, Feng Yuan, etc., are working hard on it The first draft will come up very soon Chinese version is needed It really needs international community efforts on simulations and whitepaper writing !

Job Opportunities Welcome! Now we have several immediate openings for postdoctoral researchers/guest Professors to work on EIC related physics (such as QCD, nucleon structure, small x physics, hadron physics, etc.) For further information you may refer to the following links: http://inspirehep.net/record/1189703 http://inspirehep.net/record/1206133 http://inspirehep.net/record/1210538 If one needs further information please contact us: zhpm@impcas.ac.cn (theory) xchen@impcas.ac.cn (experiment)  Welcome!

Summary EIC@HIAF opens up a new window to study/understand nucleon structure, especially the sea quark Anthony Thomas: This proposal at IMP is extremely exciting and to have this working in 6 years would be wonderful. It is a machine ideally suited to a number of important problems. Craig Roberts: Providing the understanding of hadrons, verifying QCD, perhaps, or replacing it, will be one of Nuclear Physics’ greatest contributions to science. It is in a position to make concrete predictions (Predictions for GPDs and TMDs will follow).Such predictions represent consequences of statements about confinement and DCSB (Dynamical Chiral Symmetry Breaking ) If China-EIC is in a position to test those predictions, then we can get to the heart of the most interesting problem in fundamental physics today