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A Precision Measurement of GEpGMp with BLAST

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... of GEp/GMp with BLAST. Chris Crawford. MIT Laboratory for Nuclear Science ... Spokespersons: H. Gao, J. Calarco, H. Kolster. Form Factor Ratio _at_ BATES ... – PowerPoint PPT presentation

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Title: A Precision Measurement of GEpGMp with BLAST


1
A Precision Measurement of GEp/GMp with BLAST
  • Chris Crawford
  • MIT Laboratory for Nuclear Science
  • for the BLAST collaboration

2
Introduction
  • GE,GM fundamental quantities describing
    charge/magnetization in the nucleon
  • Test of QCD based calculations and models
  • Provide basis for understanding more complex
    systems in terms of quarks and gluons
  • QED Lamb shift

3
World Data
  • Unpolarized Data
  • CEA, Bonn, DESY, SLAC
  • Christy et al. (JLab 2004)
  • Arrington et al. (JLab )
  • Polarization Transfer
  • Milbrath et al. (BATES) 1999
  • Jones et al. (JLab), 2000
  • Dieterich et al. (MAMI), 2001
  • Gayou et al. (JLab), 2002
  • Theory
  • quark orbital momentum
  • 2g effects

4
World Data
  • Unpolarized Data
  • CEA, Bonn, DESY, SLAC
  • Christy et al. (JLab 2004)
  • Arrington et al. (JLab )
  • Polarization Transfer
  • Milbrath et al. (BATES) 1999
  • Jones et al. (JLab), 2000
  • Dieterich et al. (MAMI), 2001
  • Gayou et al. (JLab), 2002
  • Theory
  • quark orbital momentum
  • 2g effects

5
World Data
  • Unpolarized Data
  • CEA, Bonn, DESY, SLAC
  • Christy et al. (JLab 2004)
  • Arrington et al. (JLab )
  • Polarization Transfer
  • Milbrath et al. (BATES) 1999
  • Jones et al. (JLab), 2000
  • Dieterich et al. (MAMI), 2001
  • Gayou et al. (JLab), 2002
  • Theory
  • quark orbital momentum
  • 2g effects

6
MIT-Bates Exp. 01-01
Spokespersons H. Gao, J. Calarco, H. Kolster
  • new technique
  • precision test
  • of theories
  • at low Q2
  • meson cloud structure

7
Form Factor Ratio _at_ BATES
  • Exploits unique features of BLAST
  • internal target low dilution, fast spin reversal
  • large acceptance simultaneously measure all Q2
    points
  • symmetric detector ratio measurement
  • Different systematics
  • also insensitive to Pb and Pt
  • no spin transport
  • Q2 0.1 0.8 (GeV/c) 2
  • overlap with JLab data

8
Asymmetry Super-ratio Method
  • Helicity Asymmetry
  • Super-ratio
  • b 45

9
Polarized Beam and Target
  • Storage Ring
  • E 850 MeV
  • Iinj175 mA
  • Pb 0.65
  • Internal ABS Target
  • 40 cm storage cell
  • t 2.7?1013 cm-2
  • Pt 0.40
  • isotopically pure internal target
  • high polarization, fast spin reversal
  • L 1.6 ? 1031 cm-2s-1

10
Detector Package
  • BLAST Coils
  • Backward-Angle TOF
  • TOF Scintillators
  • Wire Chambers
  • Cerenkov Detectors
  • Neutron Detectors
  • LADS Detectors

11
BLAST
12
Data Sets
  • 1H run 1, December 2003
  • reversed BLAST field electrons out-bending
  • 20 kC beam (3.4 pb-1) 480k elastic events
  • 1H run 2, April 2004
  • nominal BLAST field electrons in-bending
  • 57 kC beam (9.6 pb-1) 950k elastic events
  • 2D run, May October 2004
  • 450 kC beam (76 pb-1) Pz.75
  • 1H run 3, November 2004
  • 250 kC (42 pb-1) planned

13
TOF Scintillator Cuts
TOF paddle, proton
TOF paddle, electron
14
Resolution and Yields
preliminary
TOF paddle
15
Experimental Spin Asymmetry
16
GE/GM by Super-ratio Method
17
GE/GM by Fit Method
  • fit for
  • take advantage of large acceptance
  • optional also fit for b (spin angle)
  • super-ratio method
  • in each Q2 bin
  • redundant measurement of polarization

18
Preliminary Results
  • combineddatasets(77 kC)
  • preliminary results based on ¼ of the projected
    data

19
Preliminary Results
  • combineddatasets(77 kC)
  • preliminary results based on ¼ of the projected
    data

20
Conclusion
  • new precision measurement of GEp/GMp
  • exploits unique capabilities of BLAST
  • 2 4 projected errors at low Q2
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