E08-005: A y 0 in Quasi-Elastic 3 He(e,e’n) Scattering Elena Long Hall A Collaboration Meeting December 17 th, 2013 1 12/17/2013Hall A Collaboration MeetingElena.

Slides:



Advertisements
Similar presentations
Two-photon Exchange as a Laboratory for Nucleon Structure Studies The entire response of the nucleon is contained in the two-photon box. A y : Measure.
Advertisements

Extraction of G E n at Q 2 =1 (GeV/c) 2 by Measurements of May 1, 2011 Ge Jin University of Virginia.
Jin Huang PhD Candidate, MIT For MENU 2010 May 31, Williamsburg.
1 First Measurement of the Structure Function b 1 on Tensor Polarized Deuteron Target at HERMES A.Nagaitsev Joint Institute for Nuclear Research, Dubna.
A precise extraction of the induced polarization in 4 He(e,e’p) 3 H from E Simona Malace University of South Carolina Outline.
C x and C x for K + Λ and K +  o Photo-production R. Bradford Department of Physics and Astronomy, University of Rochester R. Schumacher Department of.
BONUS (Barely Off-Shell Nucleon Structure) Experiment Update Thia Keppel CTEQ Meeting November 2007.
Study of two pion channel from photoproduction on the deuteron Lewis Graham Proposal Phys 745 Class May 6, 2009.
Proton polarization measurements in π° photo-production --On behalf of the Jefferson Lab Hall C GEp-III and GEp-2γ collaboration Wei Luo Lanzhou University.
Proton Form Factor ratio GEp/GMp with polarization method --on behalf of Jefferson lab GEp3 collaboration Wei Luo Lanzhou University, China April
Proton polarization measurements in π° photo- production --on behalf of the Jefferson Lab Hall C GEp-III and GEp-2 γ collaboration 2010 Annual Fall Meeting.
Polarisation transfer in hyperon photoproduction near threshold Tom Jude D I Glazier, D P Watts The University of Edinburgh.
Measurements of F 2 and R=σ L /σ T on Deuteron and Nuclei in the Nucleon Resonance Region Ya Li January 31, 2009 Jlab E02-109/E (Jan05)
Rosen07 Two-Photon Exchange Status Update James Johnson Northwestern University & Argonne National Lab For the Rosen07 Collaboration.
Jin Huang PhD Candidate, MIT For Hall A Collaboration Meeting June 10, JLab.
PHENIX Local Polarimeter PSTP 2007 at BNL September 11, 2007 Yuji Goto (RIKEN/RBRC)
Measurement of double- polarized asymmetries in quasi- elastic processes 3 He(e,e’d) and 3 He(e,e’p) Miha Mihovilovič For the E Collaboration.
E. Penel-NottarisLaboratoire de Physique Subatomique et de Cosmologie de Grenoble 1 July, 7 th, 2004 Quasi-elastic 3 He(e,e’p) experiment (E89-044) at.
Deeply Virtual Compton Scattering on the neutron Malek MAZOUZ LPSC Grenoble EINN 2005September 23 rd 2005.
Nucleon Form Factors and the BLAST Experiment at MIT-Bates
Measuring the charged pion polarizability in the  →    −  reaction David Lawrence, JLab Rory Miskimen, UMass, Amherst Elton Smith, JLab.
Λ and Σ photoproduction on the neutron Pawel Nadel-Turonski The George Washington University for the CLAS Collaboration.
A Measurement of Two-Photon Exchange in Unpolarized Elastic Electron-Proton Scattering John Arrington and James Johnson Northwestern University & Argonne.
Target Single Spin Asymmetries in 3 He(e,e’) Nucleon and Nuclear structure studies using two photon exchange with a vertically polarized 3 He target. Program.
Ibrahim H. Albayrak, Hampton University Group Meeting Experiment Rosen07: Measurement of R =  L /  T on Deuterium in the Nucleon Resonance Region. 
Highest Q 2 Polarized Measurement of the Electric Form Factor of the Neutron – E Presented by Jonathan Miller For the Hall A E Collaboration.
Inclusive cross section and single transverse-spin asymmetry of very forward neutron production at PHENIX Spin2012 in Dubna September 17 th, 2012 Yuji.
Envisioned PbWO4 detector Wide-Angle Compton Scattering at JLab-12 GeV with a neutral-particle detector With much input from B. Wojtsekhowski and P. Kroll.
Hall A Collaboration Meeting Slide 0 Measurements of Target Single-Spin Asymmetries in QE 3 He ↑ (e, e’) Update of QE A y (E05-015) experiment.
Understanding the 3 He Nuclei: Asymmetry Measurements in Quasi- Elastic Ge Jin University of Virginia For the E Collaboration.
PowerPoint Template The Coolest Design Type something here
Speaker Name Title of Presentation
Speaker Name Title of Presentation
Insert the title of your presentation here
VILIONLEE的演界小屋 LOREM IPSUM DOLOR SIT AMET.
BUSINESS REPROT TEMPLATE
VILIONLEE的演界小屋 LOREM IPSUM DOLOR SIT AMET.
Sergey Abrahamyan Yerevan Physics Institute APEX collaboration
Metro PowerPoint Template
2017 LOGO ANNUAL REPORT Powerpoint Template Designed By Yexue in 2017.
Collect Cute Uintage style U i n t a g e U i n t a g e
Welcome To Coolsummer 95% From 2015 COOL SUMMER
Precision Measurement of η Radiative Decay Width via Primakoff Effect
PRESENTATION TITLE Subtitle Can Go Here.
NAME OF PRESENTATION Company Name.
Free Powerpoint Template Designed By Guanhai in 2016
Title of Article Topic By: Your Name Homeroom.
Poster Number: Poster Title
Collect Cute Uintage style U i n t a g e U i n t a g e
PROJECT TEAM STRUCTURE
Despicable me, Little YELLOW.
Wei Luo Lanzhou University 2011 Hall C User Meeting January 14, 2011
2016 TEMPLATE FREE BUSINESS Your Logo ENTER NAME About Us Our Team
Lorem Ipsum Dolor Sitamet
This is a sample template
WELCOME Welcome to the Business Presentation Template
Poster Number: Poster Title
Presentation Title Goes Right Here
8 Name Here years PROFILE EXPERIENCE EDUCATION SKILLS of experience
CLICK TO EDIT MASTER TITLE Click to edit Master subtitle style.
59% 34% Welcome To Coolsummer From 2014 From
PRESENTATION TITLE Presentation Subtitle By James Sager – Dec 10, 2020
for the A1 collaboration
Paper/presentation title
Business Flat General Ppt Template LOGO
Title Slide Templates.
2019 PRESENTATION TITLE LOGO
8 Name here years PROFILE EXPERIENCE EDUCATION SKILLS of experience
Presentation transcript:

E08-005: A y 0 in Quasi-Elastic 3 He(e,e’n) Scattering Elena Long Hall A Collaboration Meeting December 17 th, /17/2013Hall A Collaboration MeetingElena Long

Today’s Discussion ◦ Brief background of the physics ◦ Experimental method ◦ Summary of past analysis ◦ Summary of recent analysis ◦ Results 12/17/ Hall A Collaboration MeetingElena Long

Simple 3 He(e,e’n) - PWIA ◦Ideally, the only interaction that occurs is when the incoming electron hits the neutron ◦This model is called Plane Wave Impulse Approximation (PWIA) ◦PWIA predicts the single-spin target asymmetry, A y 0, to be exactly zero 3 12/17/ He Hall A Collaboration MeetingElena Long

3 He(e,e’n) Complications ◦Since other nucleons exist in the 3He nucleus, they cause secondary effects that must be taken into account ◦These effects, particularly FSIs, cause A y 0 to be non-zero 12/17/ ◦Final State Interactions (FSI) ◦Meson Exchange Currents (MEC) Hall A Collaboration MeetingElena Long

Current Measurements ◦A y 0 data will test state-of-the-art calculations at high Q 2 ◦Neutron physics extracted from 3 He (such as EM form factors) must correctly predict this asymmetry ◦Any non-zero result indicates higher order effects 12/17/ Hall A Collaboration MeetingElena Long

Q 2 (GeV/c) 2 Ay0Ay0 Mod. PWIA [3] PWIA Historical Data and Models [1] H.R. Poolman, Ph.D. Thesis, Vrije Universiteit, [2] J. Bermuth et al., Phys. Lett. B564, 199 (2003). [3] J.M. Laget, Phys. Lett. B273, 367 (1991). [4] J. Golak et al., Phys. Rev. C65, (2002). 12/17/2013Hall A Collaboration MeetingElena Long 6 Q 2 (GeV/c) Ay0Ay0 Faddeev Calculations at 0.16 (GeV/c) 2 [1] Mod. PWIA [1] Mod. PWIA [1] Mod. PWIA [3] Q 2 (GeV/c) 2 Ay0Ay0 NIKHEF [1] Faddeev Calculations at 0.16 (GeV/c) 2 [1] Mod. PWIA [1] Mod. PWIA [1] Mod. PWIA [3] MAMI [2] Faddeev calculations by the Bochum group [4] correctly predicted FSI, where other groups expected a much lower value

The Measurement s 12/17/ Hall A Left HRS Right HRSBigBite ARC Compton Polarimeter Raster BCM eP Møller Polarimeter Polarized 3 He Target BPM Wire Chambers Trigger Plane (Scintillators) HAND Preshower Shower VDCs Q Q Q D Scintillators Gas Cerenkov Pion Rejectors (Pb Glass) Beam Dump D Hall A Collaboration MeetingElena Long

The Measurement s 3 He(e,e’n) Channel 12/17/ Hall A Collaboration MeetingElena Long h Incident Polarized Electron Scattered Electron θqθq γ* q -θ e’ pp n n e e

The Measurement s Experimental Set-up Run period was April- June /17/ Hall A Collaboration MeetingElena Long Right HRS Polarized 3 He Target HAND Standard Beamline Target Pol. Q 2 (GeV/c) 2 E 0 (GeV) RHRS (°) RHRS P 0 (GeV) HAND (°) Vertical Vertical Vertical

The Measurement s Polarized 3 He Target 12/17/ Hall A Collaboration MeetingElena Long Polarized 3 He Target

Pumping Chamber Target Chamber (Nuclear Physics Happens Here) The Measurement s 12/17/ Hall A Collaboration MeetingElena Long

The Measurement s Right HRS 12/17/ Hall A Collaboration MeetingElena Long Right HRS

The Measurement s Right HRS Detected scattered electrons from 3 He(e,e’n) and 3 He(e,e’) Provided trigger for HAND Detector package included VDCs, trigger scintillators, gas Cherenkov, and lead- glass calorimeters 12/17/ Hall A Collaboration MeetingElena Long Right HRS

The Measurement s Right HRS Detected scattered electrons from 3 He(e,e’n) and 3 He(e,e’) Provided trigger for HAND Detector package included VDCs, trigger scintillators, gas Cherenkov, and lead- glass calorimeters 12/17/ Hall A Collaboration MeetingElena Long Right HRS

The Measurement s 12/17/2013Hall A Collaboration MeetingElena Long 15 x sieve (m) y sieve (m) Right HRS Details in G. Jin, Ph.D. Thesis, University of Virginia, 2011

The Measurement s 12/17/2013Hall A Collaboration MeetingElena Long 16 Preshower/Shower Right HRS Electron ID Details in E. Long, Ph.D. Thesis, Kent State University, 2012 (arXiv: )

The Measurement s 12/17/2013Hall A Collaboration MeetingElena Long 17 Right HRS Electron ID Details in E. Long, Ph.D. Thesis, Kent State University, 2012 (arXiv: ) Bjorken x

The Measurement s 12/17/2013Hall A Collaboration MeetingElena Long 18 Right HRS 3 He(e,e’) Single-Spin Asymmetry Comparison with Y. Zhang 3 He(e,e’) SSA – Before Charge/LT Corrections χ 2 /dof=2.13 Preliminary

The Measurement s 12/17/2013Hall A Collaboration MeetingElena Long 19 Right HRS 3 He(e,e’) Single-Spin Asymmetry Comparison with Y. Zhang 3 He(e,e’) SSA – After Charge/LT Corrections χ 2 /dof=1.95 Preliminary

The Measurement s 12/17/2013Hall A Collaboration MeetingElena Long 20 Right HRS 3 He(e,e’) Single-Spin Asymmetry Comparison with Y. Zhang Q 2 =0.1 (GeV/c) 2 Q 2 =0.5 (GeV/c) 2 Q 2 =1.0 (GeV/c) 2 χ 2 /dof=1.95 χ 2 /dof=0.70χ 2 /dof=1.29 Preliminary

The Measurement s Hall A Neutron Detector (HAND) 12/17/ Hall A Collaboration MeetingElena Long HAND

The Measurement s Hall A Neutron Detector (HAND) 12/17/ Hall A Collaboration MeetingElena Long HAND

The Measurement s Hall A Neutron Detector (HAND) Plastic scintillator array Detected neutrons from 3 He(e,e’n) in coincidence with the RHRS Details in E. Long, Ph.D. Thesis, Kent State University, 2012 (arXiv: ) 12/17/ x 11 x 70 cm 3 10 x 10 x 100 cm 3 10 x 12.5 x 100 cm 3 10 x 15 x 100 cm 3 10 x 25 x 100 cm 3 Hall A Collaboration MeetingElena Long Front View Side View cm Stacking of scintillator bars in a plane n = 30 (plane 1) 24 (plane 2) 22 (plane 3) 12 (plane 4) Scintillator Light Guide 1 2 … … n PMT

The Measurement s Hall A Neutron Detector (HAND) Plastic scintillator array Detected neutrons from 3 He(e,e’n) in coincidence with the RHRS Details in E. Long, Ph.D. Thesis, Kent State University, 2012 (arXiv: ) 12/17/ Hall A Collaboration MeetingElena Long

The Measurement s Hall A Neutron Detector (HAND) Neutrons detected using veto method Details in E. Long, Ph.D. Thesis, Kent State University, 2012 (arXiv: ) 12/17/ p Hall A Collaboration MeetingElena Long

The Measurement s Hall A Neutron Detector (HAND) Neutrons detected using veto method Details in E. Long, Ph.D. Thesis, Kent State University, 2012 (arXiv: ) 12/17/ n Hall A Collaboration MeetingElena Long

p p p p p p p p p p p p p p p p p p p p p p p p p p p p p p p p p p p p p The Measurement s Hall A Neutron Detector (HAND) Neutrons detected using veto method Details in E. Long, Ph.D. Thesis, Kent State University, 2012 (arXiv: ) 12/17/ n Hall A Collaboration MeetingElena Long p

The Measurement s Hall A Neutron Detector (HAND) Neutrons detected using veto method Details in E. Long, Ph.D. Thesis, Kent State University, 2012 (arXiv: ) 12/17/ Hall A Collaboration MeetingElena Long

The Measurement s Hall A Neutron Detector (HAND) Time-of-Flight background subtracted from the neutron peak Details in E. Long, Ph.D. Thesis, Kent State University, 2012 (arXiv: ) 12/17/ Hall A Collaboration MeetingElena Long Q 2 = 0.1 ToF Background Q 2 = 0.5 & 1.0 ToF Background Neutrons

The Measurement s Hall A Neutron Detector (HAND) Proton contamination Details in E. Long, Ph.D. Thesis, Kent State University, 2012 (arXiv: ) 12/17/2013Hall A Collaboration MeetingElena Long 30

The Measurement s Hall A Neutron Detector (HAND) Proton contamination Details in E. Long, Ph.D. Thesis, Kent State University, 2012 (arXiv: ) 12/17/2013Hall A Collaboration MeetingElena Long 31

Results 12/17/ Hall A Collaboration MeetingElena Long

Results Run-by-run A y 0 12/17/ Hall A Collaboration MeetingElena Long Q 2 =0.1 (GeV/c) 2 Q 2 =0.5 (GeV/c) 2 Q 2 =1.0 (GeV/c) 2 χ 2 /dof=0.517 χ 2 /dof=2.89χ 2 /dof=10.30 Preliminary

Results Run-by-run A y 0 12/17/ Hall A Collaboration MeetingElena Long Q 2 =0.1 (GeV/c) 2 Q 2 =0.5 (GeV/c) 2 Q 2 =1.0 (GeV/c) 2 χ 2 /dof=0.517 χ 2 /dof=1.0 Preliminary

Results Systematic Uncertainties 12/17/2013Hall A Collaboration MeetingElena Long 35

Results A y 0 vs. ν 12/17/2013Hall A Collaboration MeetingElena Long 36 Preliminary

Results A y 0 vs. Q 2 Linear 12/17/2013Hall A Collaboration MeetingElena Long 37 Preliminary

Results A y 0 vs. Q 2 Logarithmic 12/17/2013Hall A Collaboration MeetingElena Long 38 Preliminary

Thank you! 12/17/ Hall A Collaboration MeetingElena Long Graduate Students Spokespersons Run Coordinators Advisors

End 12/17/ Hall A Collaboration MeetingElena Long

Backup Slides 12/17/ Hall A Collaboration MeetingElena Long

The Measurement s 1] G. Jin, Ph.D. Thesis, University of Virginia, /17/2013Hall A Collaboration MeetingElena Long 42 Right HRS Electron ID Reaction Point in z

The Measurement s 12/17/2013Hall A Collaboration MeetingElena Long 43 Right HRS Electron ID Details in E. Long, Ph.D. Thesis, Kent State University, 2012 (arXiv: ) Cerenkov

The Measurement s 1] G. Jin, Ph.D. Thesis, University of Virginia, /17/2013Hall A Collaboration MeetingElena Long 44 Right HRS Electron ID Preshower/Shower

The Measurement s 1] G. Jin, Ph.D. Thesis, University of Virginia, /17/2013Hall A Collaboration MeetingElena Long 45 Right HRS Electron ID Theta/Phi

Simple 3 He(e,e’n) - PWIA ◦Ideally, the only interaction that occurs is when the incoming electron hits the neutron ◦This model is called Plane Wave Impulse Approximation (PWIA) ◦PWIA predicts the single-spin target asymmetry, A y 0, to be exactly zero 46 12/17/ He Hall A Collaboration MeetingElena Long

The Measurement s Hall A Neutron Detector (HAND) Proton contamination Details in E. Long, Ph.D. Thesis, Kent State University, 2012 (arXiv: ) 12/17/2013Hall A Collaboration MeetingElena Long 47

The Measurement s Reference Slide Lorem ipsum dolor sit amet, consectetur adipisicing elit, sed do eiusmod tempor incididunt ut labore et dolore magna aliqua. 12/17/ Hall A Collaboration MeetingElena Long

Results A y 0 vs. Q 2 Linear and Logarithmic 12/17/2013Hall A Collaboration MeetingElena Long 49