Title: A Precision Measurement of GEp/GMp with BLAST
1A Precision Measurement of GEp/GMp with BLAST
- Chris Crawford
- MIT Laboratory for Nuclear Science
- June 7, 2005
2Outline
- 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
3Introduction
- 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
4Form Factors of the Nucleon
- Form Factors
- Nucleon current
5Rosenbluth Separation
- Breit frame
- Nucleon Current
- Elastic Cross Section
6World Data
World Unpolarized Data
7Polarization 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
8GE/GM World Data
9Theory 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)
10Models Consistent with Polarized Data
11Form 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
12Elastic Cross Section
b target spin angle w/r to the beam line
13Asymmetry Super-ratio Method
- Beam-Target Double Spin Asymmetry
- Super-ratio
- b 45?
14Polarized 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
15Atomic Beam Source (ABS)
- Standard technology
- Dissociator nozzle
- 2 sextupole systems
- 3 RF transitions
Spin State Selection
16Laser Driven Source (LDS)
- Optical pumping Spin Exchange
- Spincell design
- Target and Polarimeter
- Results
17Spin-Exchange Optical pumping
Spin Temperature Equilibrium (STE)
18LDS Experimental Setup
19Pictures of the LDS
20Atomic Dissociation
21Atomic Polarization
22Comparison of Polarized Targets
23BLAST 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
24TOF Scintillators
- timing resolution s350 ps
- velocity resolution s 1
coplanarity cuts
ADC spectrum
25Cosmics TOF Calibration
L 15
L 12
channels
L 9
L 6
L 3
L 0
channels
R 0
R 3
R 6
26TOF Efficiency
green efficiency magenta non-bias red
misses
27TOF Scintillator Cuts
TOF paddle, proton
TOF paddle, electron
28Cerenkov 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
29Drift Chambers
- 2 sectors 3 chambers
- 954 sense wires
- 200µm wire resolution
- signal to noise ratio 201
30NSED (Online Display)
31Reconstruction
- Scintillators
- timing, calibration
- Wire chamber
- hits, stubs, segments
- link, track fit
- PID, DST
32Newton-Rhapson Track Fitter
33Hyperbolic time?dist function
D
TDC
34Linear T2D Calibration
72 33
1mm resolution
c2
28 MeV 12 MeV
D p (GeV/c)
35Wire Chamber Efficiency
36WC Offsets/Resolution/Cuts
37Tracking Efficiency
38Comparison of Yields with MC
39Experimental Spin Asymmetry
40i 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
41Extractions of m GE/GM
42Single AsymmetryExtraction
43Systematic Errors
- DQ2 (1.8)
- comparison of qe and qp
- difference between left and right sectorsmost
problematic - appeal to TOF timing !
- 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
44GE/GM Results
45Extraction of GE and GM
46GE and GM Results
BLAST World Data
47Q2 Corrections from TOF
48Conclusion
- 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
- is dip in GE around Q20.3 GeV2 real?
- systematic errors are being reduced