A Precision Measurement of GEp/GMp with BLAST - PowerPoint PPT Presentation

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A Precision Measurement of GEp/GMp with BLAST

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Title: A Precision Measurement of GEp/GMp with BLAST


1
A Precision Measurement of GEp/GMp with BLAST
  • Chris Crawford
  • Thesis Defense
  • April 29, 2005

2
Outline
  • Introduction
  • Formalism
  • World Data
  • Experiment overview
  • Experimental Setup
  • LDS polarized target
  • BLAST detector
  • Calibrations
  • Analysis
  • Cuts yields
  • Asymmetry
  • Extraction of mGE/GM
  • Systematic errors
  • Conclusion
  • Results mGE/GM
  • Separation of GE, GM

3
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
  • Probe the pion cloud
  • QED Lamb shift

4
Form Factors of the Nucleon
  • Form Factor definition
  • Nucleon current
  • Breit frame

5
Elastic Cross Section
b target spin angle w/r to the beam line
6
World Data
World Unpolarized Data
7
Polarization Transfer
  • Recoil proton polarization
  • Focal Plane Polarimeter
  • recoil proton scatters off secondary 12C target
  • Pt, Pl measured fromf distribution
  • Pb, and analyzing powercancel out in ratio

8
GE/GM World Data
9
Theory and Models
  • Direct QCD calculations
  • pQCD scaling at high Q2
  • Lattice QCD
  • Meson Degrees of Freedom
  • Dispersion analysis, Höhler et al. 1976
  • Soliton Model, Holzwarth 1996
  • VMD Chiral Perturbation Theory, Kubis et al.
    2000
  • Vector Meson Dominance (VMD), Lomon 2002
  • QCD based constituent quark models (CQM)
  • LF quark-diquark spectator, Ma 2002
  • LFCQM CBM, Miller 2002

Nucleon Electromagnetic Form Factors, Haiyan
Gao, Int. J. of Mod. Phys. E, 12, No. 1,
1-40(Review) (2003)
10
Models Consistent with Polarized Data
11
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 0.9 (GeV/c) 2
  • input for P.V. experiments
  • structure of pion cloud

12
Asymmetry Super-ratio Method
  • Beam-Target Double Spin Asymmetry
  • Super-ratio
  • b 45?

13
Polarized Beam and Target
  • Storage Ring
  • E 850 MeV
  • Imax225 mA
  • Pb 0.65
  • Internal ABS Target
  • 60 cm storage cell
  • t 4.9?1013 cm-2
  • Pt 0.80
  • isotopically pure internal target
  • high polarization, fast spin reversal
  • L 3.1 ? 1031 cm-2s-1
  • H2 98 pb-1 D2 126 pb-12005 run

14
Atomic Beam Source
  • Standard technology
  • Dissociator nozzle
  • 2 sextupole systems
  • 3 RF transitions

Spin State Selection
15
Laser Driven Source (LDS)
  • Optical pumping Spin Exchange
  • Spincell design
  • Target and Polarimeter
  • Results

16
Spin-Exchange Optical pumping
17
LDS Experimental Setup
18
Comparison of Polarized Targets
19
BLAST Detector Package
  • Detector Requirements
  • Definition of q
  • ??e ? 2?, ??e ? .?, ?z ? 1 cm
  • e/p/n/?? separation
  • PID ?t ? 1?, Cerenkov
  • Optimize statistics
  • Large Acceptance
  • Asymmetry Super-ratios
  • Symmetric Detector
  • Polarized targets
  • 1 m diameter in target region
  • Zero field at target
  • B-gradients ? 50 mG/cm

20
TOF Scintillators
  • timing resolution s350 ps
  • velocity resolution s 1

coplanarity cuts
ADC spectrum
21
Cosmics TOF Calibration
L 15
L 12
channels
L 9
L 6
L 3
L 0
channels
R 0
R 3
R 6
22
TOF Efficiency
green efficiency magenta non-bias red
misses
23
TOF Scintillator Cuts
TOF paddle, proton
TOF paddle, electron
24
Cerenkov Detectors
  • 1 cm thick aerogel tiles
  • Refractive index 1.02-1.03
  • White reflective paint
  • 80-90 efficiency
  • 5" PMTs, sensitive to 0.5 Gauss
  • Initial problems with B field
  • Required additional shielding
  • 50 efficiency without shielding

25
Wire Chambers
  • 2 sectors 3 chambers
  • 954 sense wires
  • resolution 200µm
  • signal to noise 201

26
Reconstruction
  • Scintillators
  • timing, calibration
  • Wire chamber
  • hits, stubs, segments
  • link, track fit
  • PID, DST

27
Newton-Rhapson Track Fitter
28
Hyperbolic time?dist function
D
TDC
29
Linear T2D Calibration
72 33
1mm resolution
c2
28 MeV 12 MeV
D p (GeV/c)
30
Wire Chamber Efficiency
31
Tracking Efficiency
32
WC Offsets/Resolution/Cuts
pe-pe(qe)
pp-pp(qe)
qp-qp(qe)
pe qe fe ze pp qp fp zp
fp-fp(fe)
z p- z p(ze)
33
Resolution and Yields
preliminary
TOF paddle
34
Experimental Spin Asymmetry
35
i left,right sector j Q2 bin (1..n) b spin
angle
  • Single-asymmetry Method
  • measure P first, use to calculate R
  • model-dependent
  • Super-ratio Method
  • 2 equations in P, R
  • in each Q2 bin j
  • independent measure of polarization in each bin!
  • 2n parameters Pj, Rj
  • Global Fit Method
  • fit for P, R1, R2, from all Aij together
  • model independent
  • better statistics
  • n1 parameters
  • can also fit for b

36
Extractions of m GE/GM
37
Systematic Errors
  • DQ2 (1.8)
  • comparison of qe and qp
  • difference between left/rightsector errors
    mostsignificant
  • TOF timing will help
  • Db (0.8)
  • fieldmap 47.1 1
  • Hohler 47.5 0.8
  • Fit Method 42 3
  • (1st 7 bins) 48 4
  • T20 analysis 46.5 3

38
GE/GM Results
39
Extraction of GE and GM
40
GE and GM Results
BLAST World Data
41
Conclusion
  • 1st measurement of mGE/GM using double spin
    asymmetry
  • 2 3.5 improvement in precision of mGE/GM at
    Q2 0.1 0.5 GeV2
  • sensitive to the pion cloud
  • narrow dip structure observed in GE around
    Q20.3 GeV2 ?
  • systematic errors are being reduced
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