CNI polarizations in Run09: Summary
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Transcript of CNI polarizations in Run09: Summary
Run9 results
Released on Feb 4, 2010: http://www4.rcf.bnl.gov/~cnipol/pubdocs/Run09Offline/
Gives: Fill#, Polarization, Stat. error, Syst. ErrorGlobal syst. errors (to all fills)
Short analysis description: NOTE_2009_Polarizations_RHIC.txt
Detailed analysis description: pC_2009.pdf
Briefly
Hjet:Absolute beam polarizationContinuously running in a fillAbsolute stat. uncertainty in a fill: 0.04-0.07~50% fills at s=500 GeV and ~80% fills at s=200 GeV Statistics accumulated in many fills used to normalize pC
pC (two polarimeters in a ring):3-4 measurements in a fill (every 2-3 hours) in target scan modePol. profileMany more parameters: pol. decay in a fill, pol. vector in trans. plane, beam emittance etc.Polarization for experiments (in collisions), after normalization to Hjet and correction for pol. profile
Syst. Errors: HJet
Jet normalization, stat: 2.5% for 250 GeV and 1.0% for 100 GeVThat’s what existing data gave us
Jet normalization, syst (dilution): 2%That’s what we’ve been using since Run4 (molecular contribution)
Jet normalization, syst (backgr): 2-3% From the measurements of backgr. asymmetriesRun8: 1.3-2.4%; Run6: 1.3-1.9%
pC: Time dependence in a fill
Time, hrTime, hr
0.68
0.56
0.64
0.49
0.60
0.53
0.62
0.44
0.64
0.52
0.60
0.40
0.70
0.57
0.62
0.54
Pol. decay!
pC: average over a fill
dttL
dttLtPP
fill )(
)()()/exp()( L
decayTttL )/exp()( PdecayTttP
Tpdecay – from pC
TLdecay = 5 hr
Comparison of <P>with TL
decay = 5 hr and (TL
decay = is equivalent to a
weighted average)
Only few fills showed syst. problems assign additional syst. error for these fills
pC in 2009: issues and strategy
Rate related systematicsParticularly at s=500 GeV
Failed to find a way to correct it (rate is defined by prompts which are already cut off by DAQ)
Strategy:Two polarimeters in a ring are averaged
Fill-by-fill systematic uncertainties evaluated from the comparison between two polarimeters and between pC and HJet
Fill dependence (Pol1 vs Pol2)250 GeV
RMS of the variation 12% fill-by-fill syst. uncertainty
Not yet normalized to HJet
Fill dependence (Pol1 vs Pol2)100 GeV
RMS of the variation 6% fill-by-fill syst. uncertainty
Not yet normalized to HJet
Pol. Profile: summary
250GeV: <R>=0.360.14; with fill-by-fill variation 0.36100GeV: <R>=0.080.04; with fill-by-fill variation 0.08
<R>=0.360.14 (155)% correction from Hjet to experiments<R>=0.080.04 (42)% correction from Hjet to experiments
Summary
Global systematic uncertainties:
Blue, s=500 GeV: 8.3%Yell, s=500 GeV: 12.1%Blue, s=200 GeV: 4.7%Yell, s=200 GeV: 4.7%
http://www4.rcf.bnl.gov/~cnipol/pubdocs/Run09Offline/
Run5: 5.9% and 6.2%Run6: 4.7% and 4.8%Run8: 4.2% and 7.2%
%4.4
2
2%8.8:200
YB
YB
YB
YB
PP
PP
PP
PPGeVs
%2.9
2
2%5.18:500
YB
YB
YB
YB
PP
PP
PP
PPGeVs
Sookhyun: Background raw asymmetries
Target Asymmetry (raw)
Beam Asymmetry (raw)
Possible Effect on Polarization
Blue single 250GeV
0.001477+-0.004277
0.003105+-0.004277
<2.1%
Blue double 250GeV
-0.001656+-0.001303
0.003274+-0.001303
<2.2%
Blue 100GeV -0.000704+-0.000734
0.002949+-0.000734
<1.1%
Yellow 250GeV -0.000969+-0.001999
-0.006447+-0.001999
<4.0%
Yellow 100GeV -0.000552+-0.000722
-0.002235+-0.000722
<0.9%
From MeanSigma
pC: pol. Decay in a fills=500 GeV
1/Tdecay
Affected by rates!
<Tdecay> = 10-100 hours
<Tdecay> = 10-100 hours
(<Tdecay>=100 hr 1%/hr)
Run6:
<Tdecay> ~150 hours
Run8:
<Tdecay> ~400 hours
<Tdecay> ~100 hours
In a fill: fit to exp(-t/Tdecay)
pC: pol. Decay in a fills=200 GeV1/Tdecay
<Tdecay> = 50-200 hours
<Tdecay> = 50-200 hours
(<Tdecay>=100 hr 1%/hr)
Run6:
<Tdecay> ~150 hours
Run8:
<Tdecay> ~400 hours
<Tdecay> ~100 hours
Affected by rates!
In a fill: fit to exp(-t/Tdecay)
pC: Intensity Profile
Bad profile: Non-gaussianHigh rate
Rate problem?
Good profile: Perfect gaussianLow rate
Bad profile: Non-gaussianLow rate
Target positionig problem?
pC: Polarization Profile
pC
Scan C target over the beam cross:
Target Position
Inte
nsity
Pola
rizati
on
2
2
P
IR
I
P
2. Obtain R directly from the P(I) fit:
2
2
max 2exp)(
P
xPxP
2
2
max 2exp)(
I
xIxI
R
L
LPP
maxmax
P
I
Precise target positioning is NOT necessary
1. Directly measure I and P :
R=0.290.07