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Kazuya Aoki For the PHENIX Collaborations. Kyoto Univ. / RIKEN

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1 Kazuya Aoki For the PHENIX Collaborations. Kyoto Univ. / RIKEN
Double Helicity Asymmetry of Inclusive Neutral Pion Production in Polarized pp Collisions at sqrt(s)=62.4 GeV Kazuya Aoki For the PHENIX Collaborations. Kyoto Univ. / RIKEN

2 CONTENTS Introduction Experiment Results (ALL) Conclusions
Motivation and physics channel xT scaling What we need to measure ALL Experiment RHIC beams and PHENIX global detectors. Local Polarimeter PHENIX Central Arms – EMC p0 reconstruction Results (ALL) Conclusions

3 Introduction PHENIX ‘s measured ALL p0 at
Proton spin puzzle, triggered by EMC(’88), has stimulated various efforts towards the understanding of proton spin structure. Measurement of DG Double Helicity Asymmetry(ALL) of p0 production in pol pp collisions is sensitive to DG p0 production is dominated by g+g , q+g s++= ALL is defined as the asymmetry between helicity parallel and anti-parallel collisions. s+-= PHENIX ‘s measured ALL p0 at This talk

4 Why 62.4GeV? – xT scaling xT scaling Yield xT
Independent of s Lower energy has higher yield at fixed xT (~ x500) xT We can probe higher x with better statistics even by short run at 62GeV !! (compared to 200GeV)

5 Measurement of ALL N : p0 yield L : Luminosity R : Relative Lumi.
Beam polarization Relative Luminosity Spin-dependent p0 yield ALL background subtraction Remaining transverse component What we measure. What we want.

6 RHIC and PHENIX global detectors.
Run6(2006) <p>=48% , ~1week, 60nb-1 ZDC 10*10cm  2.8 mrad 3 module 150X0 5.1λI BBC <|h|<3.9 Quartz Cherenkov det. Luminosity measurement ZDC +/- 2.8mrad. Hadron Calorimeter SMD (+ ZDC). Scintillator hodoscopes. Local polarimetry ZDC/BBC dALL~0.0028 ZDC+SMD ( Local Polarimeter ) BBC Proton beams are running in RHIC-beam pipes in transversely polarized state. Then it is rotated to ….

7 Longitudinality Longitudinal 100% (-2.2%)
neutron Longitudinal 100% (-2.2%) Transverse % (1s uncertainty) What we want. What we measure. Blue beam Forward Blue Beam Backward Horiz-position(cm) Horiz-position(cm) ZDC detector Yellow Beam Forward Yellow Beam Backward Red : Rotator OFF Blue : Rotator ON Horiz-position(cm) Horiz-position(cm)

8 PHENIX Central Arms for g detection.
EMCal Trigger Acceptance - |h|<0.35 , Df=90 x 2 Energy resolution Position resolution high energy cluster at EMCal. (~800MeV) w/o BBC BBC efficiency for p0 event(hard scattering) is low (~40%) p0 reconstruction Minimal photon energy cut 0.1 GeV for PbSc 0.2 GeV for PbGl Shower profile cut Energy asymmetry cut Trigger tile matching. (for higher energy cluster)

9 p0 Cosmic rays + hadrons peak move towards p0 peak.
pT = 1.~1.5GeV/c pT = 1.5~2GeV/c Cosmic rays + hadrons peak move towards p0 peak. The amount of the tail under p0 signal region is negligible up to used pT cosmic rays + hadrons p0 pT = 2.~2.5GeV/c pT = 2.5-3.GeV/c pT = 3.~3.5GeV/c pT = 3.5~4.GeV/c

10 Results Theory curve by W. Vogelsang

11 Results 500GeV pb-1 62.4GeV pb-1

12 summary Proton spin puzzle inspired measurements on DG
PHENIX has reported ALL of p0 at sqrt(s)=200GeV and gave constraint on DG. Thanks to xT scaling, lower energy collisions can probe higher x region with better statistics. ALL of p0 in pp collisions at sqrt(s)=62.4 GeV was measured at RHIC-PHENIX RUN6 pp sqrt(s)=62.4GeV , <p>~48% , 60 nb-1 Consistent with zero up to pT = 4GeV/c When cross-section analysis finishes and tests pQCD applicability, ( to be shown in QM ) this measurement will have strong statement on DG.

13 backups

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16 Measurement of ALL Beam polarization -- PB,PY Longitudinality
CNI polarimeter. <p> ~ 48% Longitudinality Measured by Local polarimeter ~98% Relative Luminosity – R BBC , ZDC are independent luminosity detector. dALL ~ ALL background subtraction N : p0 yield L : Luminosity R : Relative Lumi.

17 200GeV  62GeV from exp. point of view
BBC trigger bias ~80%  ~40% BBC coincidence was removed from trigger. AN of neutron at forward rapidity decriese Affected Local polarimeter performance.

18 Systematic errors Scale uncertainty ( CNI pol. Meas.)
20% Uncertainty of Relative Luminosity dALL ~ 2.8 x 10-3 Effect of ATT Remaining transverse component ~21% 0.212ATT ~ 0.04ATT on ALL

19 p0 reconstruction Energy calibration Cuts for photon or p0
Tower by tower -- done by Kenichi Non linearity correction – same as In RUN5 Scale correction for PbSc – ( by Sasha ) x for PbSc Cuts for photon or p0 Minimal photon energy cut 0.1 GeV for PbSc 0.2 GeV for PbGl Shower profile cut > 0.02 Energy asymmetry cut a < 0.8 Trigger tile matching. (for higher energy cluster) Cuts for global ERT 2x2 triggered events

20 BBC trigger bias for pi0 f0 = N0(ERT2x2&BBC) / N0(ERT2x2)
PbSc vs PbGl PbSc+PbGl Results from PbSc and PbGl are well consistent No global systematics shown (~2.5% expected), common for PbSc and PbGl Trigger bias at sqrt(s)=62 GeV is pT dependent? PYTHIA MC (without detector response simulation) at sqrt(s)=62 GeV shows qualitatively the similar effect: for jet pT=5, 10 and 20 GeV fMB~0.42, 0.27 and 0.05 correspondingly At sqrt(s)=200 GeV fMB~0.79, no pT dependency (again, PYTHIA is in qualitative agreement)

21 ERT2x2 trigger efficiency for pi0
0 = N0(BBC&ERT2x2) / N0(BBC) PbGl PbSc Plateau level: (882)% MC: 88% (7 of 64 SMs masked) Plateau level: (98.10.5)% MC: 98.5% (2 of 108 SMs masked)

22 RHIC

23 NLO pQCD applicability
s=62GeV:Comparison to fit to data s=200GeV:Comparison to data D d’Enterria, AN291 Seems to work at both energies, within ~30% or so

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