Date post: | 01-Jan-2016 |
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COMPTON POLARIMETRY
• Collected data
• Cavity power
• Status on counting methods
• Systematic errors and hardware issues
Collected Data
Good Runs
Ebeam
(GeV)k’Max
(MeV)
<A>int
(%)AMax
(%)
4He ~450 2.76 129 2.3 4.8
LH2 ~450 3.18 171 2.7 5.5
Cavity Power• Laser power supply changed in June, tested OK: 1200W
• Down to 300W few days before the experiment
• Incident laser power still nominal• Laser beam waist measured in agreement with simulation• Alignment optimized• Back to 500W after optics cleaning
• Slow exponential decay of cavity power seen during part of the run• Cavity mirrors? Two finesse measurements so far, differ by a factor 2 to be done again…
Counting Analysis
650 m strips
PbW04
4.5 mm gap
Differential
Semi-integrated
Calibration e- Detector
Ee-
Position of the Compton edge calibrates the detector and determine the vertical gap Ydet.
Can use the rate or the asym spectra.Discrepancy taken as syst error.
Pe/Pe ~ 2 Y/Y
Y=200m Pe/Pe = 3.5% @ 3 GeV
Ee- Bdl, lever arm after D3 (~4.1m)
Calibration e- Detector
Compton edge position sensitiveto beam motion (coil pulsing)
Extracted Ydet is always underestimated
Comtpon+BackgroundBackgroundS/B
Calibration e- Detector
•Fit of the asymmetry spectra of the 4 planes is more robust because it uses information from all strips.
•Systematic error could be pinned down by simulation
•Stringent cross-check available on line…
Calibration cross-check•The response function of the detector is determined using the e- det as an energy tagger reference run.
•When fitting the photon spectrum, corrects for gain drift and error in the e- det calibration. expect =1 for the fit of the reference run itself
-1 = 10-4 !!
Had to correct for the fact that strip planes are 1 cm appart and use survey data for the lever arm after dipole 3 (4.11 m instead of 4.10)
Photon Analysis
No dependence on the software threshold over a wide rangeSystematics of the response function under control.
Comparison e- -
03/08/05 19/09/05
Comparison e- -
01/11/0515/10/05
Laser Polarization
Laser Polarization
Laser Polarizatione- and data are not compatibleorigin found to be electronic pickup: ADC pedestal changes by 4 channels depending on the cavity state!
Wasn’t there last year…
Could be due to logical signals of cavity ON/OFF,Left/Right present in several electronic crates?Easy to test.
Laser PolarizationAfter pedestal correction, all analysis are compatible at 1 level. Compton polarimetry is a tedious way to check pedestal correlations…
The correction doesn’t affect the mean value,but reduces the LeftRight discrepancy.
Left laser polarizationis ~0.6% lower than Right polarization?
Laser Polarization
Laser
/4 plates
CIP
Exit L
ine
Transfer Function
Monitoring of the laser polarization downstream the cavity
/4 Scans
x
x
y
y
Wollaston Prism
Integrating Sphere S1
Integrating Sphere S2
Incoming Polarization Ellipse
TE pol. state
TM pol. state
Rotatable/4 plate
Slow
9.88.8
0
0
1
1
2sin2sin2cos2cos2
132
2101 PPPPS
0
0
1
1
2sin2sin2cos2cos2
132
2102 PPPPS
Stokes Parameters: P0,P1,P2,P3
Laser Polarization
•30 /4 scans performed during helium run.
•We do find a 0.5% difference in laser polarization states but with opposite sign
Need to check the Left-Right definitions in both analysis…
Accumulated cavity power: Left state = Right state at few % level (~500W)
Conclusion
Significant improvements in the counting analysis Best agreement between the two methods ever achieved On track for 2% accuracy or better.
Hardware issues: compton is getting old…
• Should revise all cabling at some point• Need cross-talk study before GE
n starts• Numerous « end of run failed » remove 600Hz part of the aquisition?• Cavity power is low? How long before very low?
Systematic Errors
Source Last Year To Do Expect.
P 0.70% Open cavity?
0.7%-1%
Resp. Func. 1.25% Ana.+Simul. 1.1%
Dead Time 1.00% - ~0%
Pile up 1.00% Simulation 0.5%
Rad. Corr. 0.25% - ~0%
TOTAL 2.0% 1.4%-1.6%
Expect to reduce syst. error as well because of better calibration.(3.5% for now)
Counting photon
Counting electron