1. E02-013: at high Q 2 Status of Analysis Sergey Abrahamyan Yerevan Physics Institute for the E02-013 collaboration TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AAA A A A

2. Overview  Form factors  E02-013 Experiment  1.2 GeV 2 analysis  Status 2Hall A Collaboration Meeting6/11/2009

3. E02-013 Collaboration Universität Basel, CH-4056 Basel, Switzerland; University of Virginia, Charlottesville, VA 22903; Yerevan Physics Institute, Yerevan 375036, Armenia; North Carolina A&T State University, Greensboro, NC 27411; Tel Aviv University, Tel Aviv, 69978 Israel; Florida International University, Miami, FL 33199; University of Maryland, College Park, Maryland 20742; Ohio University, Athens, OH 45071; Thomas Jefferson National Accelerator Facility, Newport News, VA 23606; Mississippi State University, Mississippi State, MI 39762; Hampton University, Hampton, VA 23668; Southern University at New Orleans, New Orleans, LU 70126; Louisiana Tech University, Ruston, LU 71272; North Carolina Central University, Durham, NC 27707; Syracuse University, Syracuse, NY 13244; Kent State University, Kent, OH 44242; Norfolk State University, Norfolk, VA 23504; Old Dominion University, Norfolk, VA 23529; Carnegie Mellon University, Pittsburgh, PA 15213; University of Glasgow, Glasgow G12 8QQ, Scotland, U.K.; California State University Los Angeles Los Angeles, CA 90032; Massachusetts Institute of Technology, Cambridge, MA 02139; Budker Institute for Nuclear Physics Novosibirsk 630090, Russia; Institute for Nuclear Physics Tomsk 634050, Russia; University of New Hampshire, Durham, NH 03824; College of William and Mary, Williamsburg, VA 23187; Temple University, Philadelphia, PA 19122; Kharkov Institute of Physics and Technology Kharkov 61108, Ukraine; St. Petersburg Nuclear Physics Institute Gatchina, 188350, Russia; Duke University and TUNL, Durham, NC 27708; Université Blaise Pascal/IN2P3, F-63177 Aubière, France; IPN Orsay B.P. n ○ 1, F-91406, Orsay, France; CEA Saclay, DAPNIA/SPhN, F-91191 Gif sur Yvette, France; University of Maryland, College Park, MD 20742; INFN, Sezione di Sanitá and Institute Superiore di Sanitá, I-00161 Rome Italy; Rutgers, The State University of New Jersey, Piscataway, NJ 08854; University of Massachusetts, Amherst, MA 01003; Kyungpook National University, Taegu City, South Korea; Madrid University, Madrid, Spain; University of Kentucky, Lexington, KY 40506; Argonne National Laboratory, Argonne, IL 60439. 6/11/2009Hall A Collaboration Meeting3

4. Analysis group Spokespersons: – Gordon Cates, University of Virginia – Nilanga Liyanage, University of Virginia – Bogdan Wojtsekhowski, Jefferson Laboratory Post Docs and analysis coordinators: – Robert Feuerbach, Jefferson Laboratory, College of William and Mary – Seamus Riordan, Carnegie Mellon University (graduated 2008), University of Virginia PhD Students: – Sergey Abrahamyan, Yerevan Physics Institute – Brandon Craver, University of Virginia – Aidan Kelleher, College of William and Mary – Ameya Kolarkar, University of Kentucky (graduated 2007) – Jonathan Miller, University of Maryland Master Students: – Tim Ngo, University of California (graduated 2007) 4Hall A Collaboration Meeting6/11/2009

5. Form Factors For electron scattering on point-like spin ½ unpolarized particle cross-section is: where and is Mott cross-section for electron scattering. 5Hall A Collaboration Meeting6/11/2009

6. Form Factors  Cross-section for electron scattering on structured particle in terms of Dirac and Pauli form factors is  In terms of Sachs form factors 6Hall A Collaboration Meeting6/11/2009 Fourier transform of charge and magnetization density distributions in Breit frame

7. Measurement Technique extracted by measuring quasielastic cross-section asymmetry in reaction. 7Hall A Collaboration Meeting6/11/2009

8. E02-013 E02-013 experiment ran February-May 2006 8Hall A Collaboration Meeting6/11/2009

9. Experimental Setup Neutron Arm 7 scintillator planes for hadron detection 2 veto-detector planes for charge identification BigBite Dipole Magnet (1.0 T·m) 15 MWDC planes Scintillator (timing) plane 2-plane Electromagnetic Calorimeter 9Hall A Collaboration Meeting6/11/2009 Polarized 3 He Target spin exchange between optically pumped Rb-K mixture and 3 He gas 50% polarization achieved

10. Calibration BigHand TOF calibration for bars in 1-st plane, scale in ns. Resolution ~ 350 ps BigBite DC U1 plane resolution with new time offsets and positions. Resolution < 200µm 6/11/2009Hall A Collaboration Meeting10

11. Quasielastic Events Selection Q 2 = 1.7 GeV 2 Quasielastic selection based on 11Hall A Collaboration Meeting6/11/2009 P miss,|| vs WP miss, ┴ vs W

12. Quasielastic Events Selection Neutron arm momentum resolution on higher Q 2 becomes less effective due to higher γ-factor Q 2 = 3.5 GeV 2 12Hall A Collaboration Meeting6/11/2009 P miss,|| vs WP miss, ┴ vs W

13. Quasielastic Events Selection Quasielastic selection based on Q 2 = 3.5 GeV 2 Q 2 = 1.7 GeV 2 13Hall A Collaboration Meeting6/11/2009 M miss vs W

14. Quasielastic Cuts Summary To select quasieleastic cuts applied on Q 2 = 1.7 GeV 2 Q 2 = 2.5 GeV 2 14Hall A Collaboration Meeting6/11/2009 Q 2 = 3.5 GeV 2

15. Charge Identification Cluster in NA should be correlated with veto-signal in space and in time Proton contamination to neutron sample due to charge conversion before veto plane evaluated through uncharged/charged ratios for different targets 15Hall A Collaboration Meeting6/11/2009 Due to charge conversion in material before veto-layers charge misidentification may occur. Proton contamination measured to be 10-25% which is within 5% agreement with MC

16. Target Polarization 50% Target polarization was achieved during E02-013 experiment. For most part of the experiment value of target polarization was over 45%. 16Hall A Collaboration Meeting6/11/2009

17. Inelastic contribution and MC 6/11/2009Hall A Collaboration Meeting17 MC shows a good agreement with data on the lowest Q 2 =1.7 GeV 2 point in both quasielastic and inelastic region. Developed MC-simulation will be used to eliminate a proper cuts for quasielastic events selection on higher Q 2 kinematic points.

18. FSI 6/11/2009Hall A Collaboration Meeting18 Isobar CurrentMeson Exchange Current FSIImpulse Approximation IC – the virtual photon produces isobar which reinteracts with residual nuclear system producing final hadronic state MEC – the virtual photon interacts with the exchanged (between two-nucleon system) mesons IA – virtual photon knocks-out the bound nucleon which propagates to the final state without further interactions FSI – in which the knocked-out nucleon reinteracts with residual hadronic system FSI and Charge Exchange effects will be calculated using the Generalized Eikonal Approximation (Misak Sargsian)

19. Physics Asymmetry and  To extract a physics asymmetry raw experimental asymmetry corrected on:  Accidental background  Proton contamination to neutron sample  Nitrogen dilution  Target Polarization  Beam Polarization  Extraction of includes:  Finite acceptance correction  FSI (not included in current results) 19Hall A Collaboration Meeting6/11/2009

20. Results 20Hall A Collaboration Meeting6/11/2009

21. Status Done  BigHand and BigBite calibrations finalized  3 higher Q 2 kinematic points data replayed with new calibration for both electron and hadron detectors.  Semifinal results for Q 2 = 1.7, 2.5, 3.5 GeV 2 Need to be finalized (end of June)  Pion asymmetry contribution  FSI correction  Wider cuts (based on MC) to improve statistics  Final results for Q 2 = 1.7, 2.5, 3.5 GeV 2 21Hall A Collaboration Meeting6/11/2009