A feasibility study for measurements using electroweak probes at the proposed Electron-Ion Collider: Investigating nucleon structure and the fundamental.

Slides:



Advertisements
Similar presentations
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.
Advertisements

Longitudinal Spin at RHIC 29 th Winter Workshop on Nuclear Dynamics February 7, 2013 Cameron McKinney.
Polarized Semi-Inclusive Physics Measurements at HERMES and Future Prospects at the Colliders E.R. Kinney University of Colorado 2nd Electron-Ion Collider.
1 Partonic Substructure of Nucleons and Nuclei with Dimuon Production Partonic structures of the nucleons and nuclei with dimuon production –Overview and.
Constraining the polarized gluon PDF in polarized pp collisions at RHIC Frank Ellinghaus University of Colorado (for the PHENIX and STAR Collaborations)
Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.
Current: –Experiment: Extensive Drell-Yan p-p and p-d Expt. (E866) ; Charm production in Neutrino Scattering (CCFR, NuTeV) … etc. –Expected Advances in.
The new Silicon detector at RunIIb Tevatron II: the world’s highest energy collider What’s new?  Data will be collected from 5 to 15 fb -1 at  s=1.96.
K. Kumar, W. Marciano, Y. Li Electroweak physics at EIC - Summary of week 7 INT Workshop on Pertubative and Non-Pertubative Aspects of QCD at Collider.
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.
1 Hyperons in polarized pp collisions and the nucleon spin structure Qinghua Xu( 徐庆华 ), Shandong University/LBNL July 10, 2008, QCD workshop,USTC The strange.
Jefferson Lab Status Hall A collaboration Dec. 16, 2013 R. D. McKeown Deputy Director For Science.
An Electron Ion Collider at HIAF
1 Updates on Transversity Experiments and Interpretations Jen-Chieh Peng Transversity Collaboration Meeting, JLab, March 4, 2005 University of Illinois.
THE DEEP INELASTIC SCATTERING ON THE POLARIZED NUCLEONS AT EIC E.S.Timoshin, S.I.Timoshin.
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,
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.
Possibilities to perform DVCS measurement at COMPASS E. Burtin CEA-Saclay Irfu/SPhN On Behalf of the COMPASS Collaboration DIS Madrid - 29 April,
Xiaodong Jiang Gluon spin with longitudinal asymmetries at RHIC. Parton angular motion - transverse spin asymmetries. Spin at RHIC : p+p. Spin at JLab:
Columbia University Christine Aidala September 4, 2004 Solving the Proton Spin Crisis at ISSP, Erice.
Longitudinal Spin Physics at RHIC and a Future eRHIC Brian Page Brookhaven National Laboratory CIPANP 2015 – Vail, CO.
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.
Spin Physics with PHENIX (an overview, but mainly  G) Abhay Deshpande Stony Brook University RIKEN BNL Research Center July 28, 2011.
Future Physics at JLab Andrew Puckett LANL medium energy physics internal review 12/14/
HERA-LHC, CERN Oct Preliminary study of Z+b in ATLAS /1 A preliminary study of Z+b production in ATLAS The D0 measurement of  (Z+b)/  (Z+jet)
Jim Stewart DESY Measurement of Quark Polarizations in Transversely and Longitudinally Polarized Nucleons at HERMES for the Hermes collaboration Introduction.
General Discussion some general remarks some questions.
UMass Amherst Christine Aidala Jacksonville, FL Measuring the Gluon Helicity Distribution at a Polarized Electron-Proton Collider APS April Meeting 2007.
Quark Structure of the Proton – The Horizons Broaden! On behalf of the HERMES collaboration H. E. Jackson highlights.
Precision Cross section measurements at LHC (CMS) Some remarks from the Binn workshop André Holzner IPP ETH Zürich DIS 2004 Štrbské Pleso Štrbské Pleso.
CERN Evaluation Meeting, Bergen, April 2009Joakim Nystrand, University of Bergen Future electron-proton and electron-nucleus colliders, eRHIC and.
Report from India Topical Conference on Hadron Collider Physics XIII Jan 14-20, TIFR, India Naohito Saito RIKEN/ RIKEN BNL Research Center.
Liu Minghui Nanjing MC study of W polarization and ttbar spin correlation Liu Minghui, Zhu Chengguang April 27, 2008.
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.
 Introduction  The ZEUS PDF fit: an overview  Impact of future HERA data on the ZEUS fit - end of current HERA-II running scenario - additional studies.
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.
Discussion Global Analysis of Polarized RHIC and DIS data: How do we get there? Global Analysis Workshop at BNL, Oct. 8, 2007.
SWADHIN TANEJA (STONY BROOK UNIVERSITY) K. BOYLE, A. DESHPANDE, C. GAL, DSSV COLLABORATION 2/4/2016 S. Taneja- DIS 2011 Workshop 1 Uncertainty determination.
Measurement of Flavor Separated Quark Polarizations at HERMES Polina Kravchenko (DESY) for the collaboration  Motivation of this work  HERMES experiment.
ZEUS Physics Overview A sampling of recent physics results –Charged current cross-section –Charm production in DIS –Exotic hadrons (glueballs and pentaquarks)
Introduction and Updates (work in progress) LHeC Workshop, Chavannes-de-Bogis, January 20 th, 2014.
1 Heavy Flavour Content of the Proton Motivation Experimental Techniques charm and beauty cross sections in DIS for the H1 & ZEUS Collaborations Paul Thompson.
A. Bertolin on behalf of the H1 and ZEUS collaborations Charm (and beauty) production in DIS at HERA (Sezione di Padova) Outline: HERA, H1 and ZEUS heavy.
1 Dubna, September, 2005 Aram Kotzinian Spin effects in MC generators The spin and azimuthal asymmetries in the current and target fragmentation regions.
Tensor and Flavor-singlet Axial Charges and Their Scale Dependencies Hanxin He China Institute of Atomic Energy.
Mass states of light vector mesons are considered to be sensitive probes of partial chiral symmetry restoration theoretically expected in high energy and/or.
H1 and ZEUS Combined PDF Fit DIS08 A M Cooper Sarkar on behalf of ZEUS and H1 HERA Structure Function Working Group NLO DGLAP PDF fit to the combined HERA.
Spin Physics with PHENIX (an overview, but mainly  G) Abhay Deshpande Stony Brook University RIKEN BNL Research Center PANIC’11 at MIT July 28, 2011.
Kazutaka Sudoh (KEK) INPC2007, Tokyo June 5, 2007 Global Analysis of Hadron-production Data in e + e - Annihilation for Determining Fragmentation Functions.
Future studies of TMDs Delia Hasch SIR05- International Workshop on Semi-inclusive reactions and 3D-parton distributions May 18-20, 2005; Jefferson Lab,
11/18/2008 Global Design Effort 1 Summary for Gamma-Gamma Mayda M. Velasco Northwestern University November 20, 2008 LCWS08 -- UIC, Chicago.
6/28/20161 Future Challenges of Spin Physics Feng Yuan Lawrence Berkeley National Laboratory.
Recent results on non-DDbar decays of  (3770) at BES HaiLong Ma [For BES Collaboration] The IVIIth Rencontres de Moriond session devoted to QCD AND HIGH.
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.
Electroweak physics at an EIC
Explore the new QCD frontier: strong color fields in nuclei
EIC NAS review Charge-2 What are the capabilities of other facilities, existing and planned, domestic and abroad, to address the science opportunities.
Gordon Cates, Xiaochao Zheng, Yuxiang Zhao LOI
Recent Results on Proton Helicity Structure Studies from PHENIX
Polarized PDF (based on DSSV) Global Analysis of World Data
Electroweak and SM Physics at EIC
B2B hadron production in SIDIS
Large-X PDFs in the Drell-Yan Process
On behalf of the HERMES collaboration
Shingo Sakai for PHENIX Collaborations (Univ. of Tsukuba)
Parton Density Functions
Presentation transcript:

A feasibility study for measurements using electroweak probes at the proposed Electron-Ion Collider: Investigating nucleon structure and the fundamental electroweak couplings to light quarks 1 Christine Aidala, Ming Liu, ?

Outline (LDRD ER Format) Research Goals Background & Significance R&D Approach – Preliminary Studies – Methods, Technical Challenges, & Alternatives – Expected Results – Schedule & Milestones Mission Relevance & Program Development Plan Budget Justification Request Qualifications of Research Team 2

Research Goals Determine expected uncertainties for measurements of the unpolarized and polarized electroweak structure functions of the nucleon F3 and g5, as a function of the beam energies and luminosities at the proposed EIC Determine expected uncertainties on the unpolarized and polarized strangeness distributions in the nucleon that could be extracted from such measurements Determine expected uncertainties on the fundamental coupling of the Z boson to the up and down quarks that could be extracted from such measurements Provide feedback critical to design of the accelerator: – How much gain from (unpolarized) positrons? – How much gain from pushing to higher energies than current default expectations for the EIC? Proposals for higher energies are on the table (up to 30 on 325 GeV at eRHIC), but the physics case has not yet been made. 3

Background & Significance EIC will be first machine capable of colliding beams of polarized electrons against polarized protons and polarized light ions, as well as unpolarized heavy ions. – Unique capability to measure the polarized electroweak structure function of the nucleon, g5! No previous measurements exist, and no other facilities are planned or proposed that could perform this measurement! EIC will have at least 100x the instantaneous electron- proton luminosity than the HERA collider, which ran polarized electrons and positrons on unpolarized protons – Expect great improvement in measurement of the unpolarized electroweak structure function of the nucleon, F3 4

Background & Significance (cont.) Flavor structure of the nucleon sea a current hot topic (see next slides) – E906 investigating unpolarized u-bar, d-bar – RHIC W program investigating polarized u-bar, d-bar (Still need to understand what JLab data will contribute on unpolarized and polarized strangeness in the meantime, but expect it to depend on fragmentation functions, while extraction of strangeness distributions from inclusive structure function measurements would not--complementarity) 5

let’s compare the two most recent fits within their quoted uncertainties: find: error bands largely overlap surprising tension for up and down valence quarks some offset for strange density likely due to data selection likely due to different ansatz for s(x,  0 ) PRD78 (2008) arXiv: Flavor structure of unpolarized proton

 indications for an SU(2) breaking of light u,d sea  breaking of similar size than in unpol. case  mainly determined by SIDIS data  “bands”: error estimate from Lagr. mult.  similar patterns in many models: large-N C, chiral quark soliton, meson cloud Thomas, Signal, Cao; Diakonov, Polyakov, Weiss; …  a strange strangeness polarization   s(x) always thought to be negative, but …  mainly determined from SIDIS kaon data  consistent with LO-type analyses by HERMES and COMPASS x needs further studies – exp. & theory !

NC CC EW unification at high Q 2 MW2MW2 MZ2MZ2 Max Q 2 (=s) for 20 x 250 GeV Max Q 2 (=s) for 11 x 60 GeV 8

F3 from HERA—large uncertainties 9

Extraction of EW coupling parameters to up quark 10 EIC constraint would be best measurement in DIS, and better than any current experimental constraints. LHC p+p data may reduce constraint compared to CDF in the meantime.

R&D Approach: Preliminary study for g 5 at EIC 11 2 fb^-1, compare to 5 fb^-1 expected per year  feasible. 1 st measurement ever! Only possible at the EIC.

R&D Approach: Methods Use existing MC generator and detector simulations currently being developed by others to perform simulation studies for observables as a function of beam energies, luminosities... No significant technical challenges expected 12

R&D Approach: Schedule & Milestones Goal to provide input for the 2012/13 Long Range Plan – Regarding issues potentially affecting accelerator design – To possibly attract support from individuals from other communities, e.g. electroweak and/or those interested in precision calculations for the LHC (electroweak coupling to up, down) 13

Budget Justification Request 1.0 FTE postdoc and M&S for PD’s computer and travel Partial support of staff member (Ming)? Modest additional M&S for Ming’s or my EIC- related travel? 14

Qualifications of Research Team Involved in experimental nuclear/HEP for many years, nucleon structure at PHENIX, polarized HERA (CA), E906 (Ming), already involved in EIC planning... 15