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DIFFRACTION 2010, Sep. 10-15, Otranto, Italy
Forward Di-Hadron Correlations in d+Au Collisions in PHENIX Searching for Gluon Saturation with the MPC Oleg Eyser Beau Meredith, Mickey Chiu, Matthias Perdekamp for the PHENIX Collaboration
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The gluon density at low x
At small x we see an increase in gluons. There must be a kinematic region in which the gluon density reaches a saturation! Bremsstrahlung ~ asln(1/x) Recombination ~ asr
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The color glass condensate
log x-1 log Q2 DGLAP non-perturbative log LQCD2 Qs2(x) Saturation Scale BFKL Parton Gas Color Glass Condensate Mid Rapidity Forward Rapidity pT is balanced by gluons d Au Hadronic probe Couple to gluons High A Higher parton densities Asymmetric Probe low x 3
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Signatures of the CGC p0 meson |h|<0.35 PHENIX CGC expectations Kharzeev, Kovchegov,Tuchin Phys.Rev.D68:094013,2003 BRAHMS STAR increased h Gluon saturation is not the only explanation for the reduced yields. There may be other effects. PRL 97, (2006) PRL 98, (2007)
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Shadowing in jet correlations
pQCD 2→2 process = back-to-back di-jet With shadowing in nucleus forward jet d+Au in HIJING (A. Ogawa) d p Au p mid-rapidity jet Vitev, hep-ph/ v2 5
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Mono-jets from the CGC In the saturation regime the jet pT is balanced by many gluons. Kharzeev, Levin, McLerran (NPA748, 627) d Au dense gluon field The gluon field is increased in central vs. peripheral collisions. 6
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The Nuclear Modification Factor
Correlation function Two-particle distribution Including two-particle acceptance Conditional yield Number of particle pairs per trigger particle Including acceptance & efficiency Nuclear modification factor Conditional yield ratio d+A/p+p Indicators of gluon saturation IdA < 1 Angular de-correlation of widths
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Gluon Saturation @ RHIC
PHENIX STAR BRAHMS pp2pp d+Au vs p+p high-x valence quarks 0.25 < xq < 0.7 on low-x gluons 0.001 < xg < 0.1 Signatures of saturation suppressions of nuclear modification factors angular de-correlations of di-jet signals saturation is expected at x≈10-4
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Azimuthal Correlations in PHENIX
Trigger particle Associate particle Correlation Near side peak Away side peak Central Arms | η | < 0.35 Muon Arms 1.2 < | η | < 2.4 Dj Muon Piston Calorimeter 3.1 < | η | < 3.9
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Azimuthal Correlations (prev.)
2003 data Trigger hadron from the muon arms Correlated hadron from the central arm Phys.Rev.Lett.96:222301,2006
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The Muon Piston Calorimeters
Electromagnetic Calorimeters at rapidity 3.1 < |h| < 3.9 2.2 x 2.2 x 18 cm3 PbWO4 crystals 220 cm from nominal interaction point p0 merging effects pT max ~ 2 GeV/c at outside ring For higher pT Reconstructed p0s for 7 GeV < E < 22 GeV Clusters for E > 15 GeV (~ 85% p0) gg invariant mass distribution 11 GeV < E < 15 GeV Signal pairs Mixed event pairs p0 yield
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Forward Di-jet Signal with Dh = 3.4
PHENIX Central region Side View p0 or clusters p0 or h+/- d Au xgluon ~ 10-2 Aueffective xgluon ~ 10-3 peripheral to central
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Forward correlations at h = 3.4
PHENIX Central region Side View p0 or clusters Work in progress Area of away-side peak represents conditional yield No efficiency correction No uncorrelated background yet Conditional yields, widths not shown d Au xgluon ~ 10-3 Aueffective xgluon ~ 10-4
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Forward correlations (minBias)
Trigger particle pT > 2 GeV/c Associate particle pT > GeV/c
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Forward correlations peripheral central
Peripheral d+Au seems more similar to p+p Central d+Au shows a reduced yield, maybe broadening
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pT,trigger pT,associate
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pT,trigger pT,associate
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Summary Central/forward di-hadron correlations
No significant broadening between d+Au vs pp Reduced IdA in more central collisions Model calculations are needed to understand this effect Forward/forward di-hadron correlations Qualitative indications of onset of gluon saturation hypothesis in reduced yields Data also suggests width broadening More work needed on uncorrelated background!
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