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Nov 2001 Craig Ogilvie 1 Angular Correlations at High pt: Craig Ogilvie for the Phenix Collaboration Energy-loss: increased medium-induced gluon-radiation hadron distribution softened, broadened? hard-scattered parton during Au+Au hard-scattered parton from e.g. p+p gluon radiation cone of hadrons p p
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Nov 2001 Craig Ogilvie 2 Correlations 2-particle angular correlation functions Medium-induced gluon emission within QGP –predicted to be broad angles (>10 deg shown later in talk) –fragmentation angular-width may be broader –correlations at small may be broadened study correlations from peripheral => central reactions –complementary to single-particle pt spectra and +hadron back-to-back correlations.
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Nov 2001 Craig Ogilvie 3 Outline Examples of angular correlation data from p+p, e+p Angle correlations from Au+Au at s 1/2 = 130 AGeV –pt dependence –centrality dependence Simulations of possible sources of angular correlations –work in progress Measurements for this year-2 Which observable makes a link between experiment and theory
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Nov 2001 Craig Ogilvie 4 ISR Data p+p s 1/2 = 62 GeV CCOR Collaboration (M. J. Tannenbaum) Trigger particle (neutral) with pt > 7.0 GeV/c –azimuthal distribution of charged particles –strong back-to-back and near-side emission back-to-back near-side
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Nov 2001 Craig Ogilvie 5 Transverse Momentum Within Jet j T transverse momentum with respect to “jet” axis Trigger P T jTjT Jet PTPT jTjT P out kTkT = 400 MeV/c, use as one check for what we observe in HI CCOR Collaboration Phys. Lett. 97B, 163 (1980))
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Nov 2001 Craig Ogilvie 6 HERA e+p Angular Distribution Within a Jet Within a jet Yield of two particles separated by angle 12 Transformed to Yield peaked at small 12, More complicated variable chosen to match expt. with what can be calculated.
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Nov 2001 Craig Ogilvie 7 Au+Au s 1/2 = 130 AGeV 1.5M events, summer 2000 Phenix data -20 < collision vertex < 20 cm Central arm tracks –momenta from drift chamber tracks –1 < pt < 2.5 GeV/c Centrality cuts expressed as a % of int =7.2b –(zero degree energy) vs (charge in beam counters) Correlation functions –mixed events from similar beam-vertex, centrality –2-track acceptance cuts on both real, mixed pairs
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Nov 2001 Craig Ogilvie 8 Correlations Presented Today Both hadrons between 1< pt < 2.5 GeV/c Two correlations formed –both hadrons in west arm of PHENIX –one hadron in east, west arm of PHENIX Studied as a function of pt, centrality
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Nov 2001 Craig Ogilvie 9 Possible Causes of Angular Correlation Elliptic flow, jet fragmentation produce azimuthal correlations Analysis challenge to extract both –jet fragmentation extends to narrow angles »near-side ~ 0-30 deg –flow extends over full range with a harmonic oscillation
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Nov 2001 Craig Ogilvie 10 40-92% Centrality, 1.0 < pt < 2.5 GeV/c Near-angle correlation falls more steeply than back-to-back correlation Add correlations by ensuring symmetry near 90 o Both hadrons in west arm One hadron in west arm, other in east arm
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Nov 2001 Craig Ogilvie 11 1<pt<2.5 GeV/c (40-92%) symmetric (elliptic flow) fit (poor) stronger near-angle correlation than back-to-back phenix preliminary
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Nov 2001 Craig Ogilvie 12 Centrality Dependence 40 to 92% 0 to 5% 1)near-angle correlation in central reactions: broader, smaller amplitude 2)elliptic flow v.small in central reactions phenix preliminary 1< pt < 2.5 GeV/c
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Nov 2001 Craig Ogilvie 13 Au+Au Centrality Dependence npart width of correlation broadens for more central reactions systematic errors: how fit changes for different normalization criteria 1< pt < 2.5 GeV/c phenix preliminary
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Nov 2001 Craig Ogilvie 14 First-Order Comparison to p+p npart for peripheral data, on average both hadrons comparable pt pp running this year impt. phenix preliminary
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Nov 2001 Craig Ogilvie 15 Pt Dependence of Correlation Fit to full function, display only near-angle correlation strongest for high-pt 1.0 < pt < 2.5 GeV/c 0.5 < pt < 1.0 GeV/c 0.2 < pt < 0.5 GeV/c central 40 –92%
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Nov 2001 Craig Ogilvie 16 Feasible Causes of Near-Angle Correlation (next slides) Resonance decay leading to correlated particles Decay of K 0 s (in progress, not shown today) Fragmentation of high-pt parton Other….?
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Nov 2001 Craig Ogilvie 17 1) UrQMD Au+Au 2) tag all resonances 3) decay, apply pt cut correlation strength 0.001 due to decay of resonances 5-10 times smaller than data Resonance Study 1.0 < pt < 2.5 GeV/c | | <0.35
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Nov 2001 Craig Ogilvie 18 PYTHIA 6 p+p at s 1/2 = 130 GeV Hard-Processes 1.0 < pt < 2.5 GeV/c, | | <0.35 C C near-angle correlation stronger than back-to-back small acceptance reduces back-to-back acceptance for different x 1, x 2 width of 0.35 rad = 20 deg comparable to periph. Au+Au scattered parton ~ 3GeV/c
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Nov 2001 Craig Ogilvie 19 Possible Reach With Year-2 Data p+p baseline data 30-100 times more Au+Au statistics Higher-pt reach, pt > 5 GeV/c Asymmetric pt cuts, pt1 > 5 GeV/c, pt2 > 2 GeV/c –better match to transverse momentum within jet Tag PID of leading hadron, correlate with all others – 0 correlated with others »heading towards correlated with others –leading p or p » speculative possible sensitivity to gluon vs quark jets
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Nov 2001 Craig Ogilvie 20 Making Connection With E-Loss Theory Recent calculations, e.g. Baier, Schiff, Zakharov, calculate how much energy is radiated to outside a given cone angle 250 GeV jet 1/3 of E is radiated > 20 o Can this formalism calc C( )? Do we need new observable that expt and theory can both use Ann. Rev. Nucl. Sci 2000, 50, p37
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Nov 2001 Craig Ogilvie 21 Summary High-pt near-angle correlations slightly stronger than back- angle correlations –well reproduced by Gaussian superimposed on oscillation –width of correlation broadens for more central reactions Possible causes of near-angle correlation –decay of resonances »factor of 5-10 smaller than observed signal –weak decay of K 0 s , in progress –fragmenting hard-physics »needs higher pt reach to be convincing »in this scenario, increasing width, broader fragmentation »open question: medium-induced gluon emission?
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