1 / 18

David Winter

Jets and High-p T (Di-hadron) Correlations in PHENIX Lake Louise Winter Institute 2005 Lake Louise, Alberta CA. David Winter. Outline. RHIC and PHENIX The nuclear medium and jet modifications Correlation Functions Hard scattering Near (Same)-side and Away-side (di-jet) correlations

howard
Télécharger la présentation

David Winter

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Jets and High-pT (Di-hadron) Correlations in PHENIXLake Louise Winter Institute 2005Lake Louise, Alberta CA David Winter

  2. Outline • RHIC and PHENIX • The nuclear medium and jet modifications • Correlation Functions • Hard scattering • Near (Same)-side and Away-side (di-jet) correlations • Jet modifications in Heavy-Ion Collisions • Future measurement technique • Summary David Winter Jets and High-pt Azimuthal Correlations in PHENIX 2

  3. Event characterization detectors in center Two central arms for measuring hadrons, photons and electrons Two forward arms for measuring muons RHIC and PHENIX • Brookhaven National Laboratory • 70 mi from Manhattan • Two rings / 3.83 km circumference • Capable of colliding ~ any nuclear species on ~ any other species • Energy: • 500 GeV for p-p • 200 GeV for Au-Au (per N-N collision) • Luminosity • Au-Au: 2 x 1026 cm-2 s-1 • p-p : 2 x 1032 cm-2 s-1 (polarized) David Winter Jets and High-pt Azimuthal Correlations in PHENIX 3

  4. d+Au p0 x4-5 suppression Au+Au The Nuclear Medium • Nuclear modification factor • Multiple scattering in the medium results in kT broadening • Thought to be source of Cronin Enhancement • Nuclear modification factor • Medium-induced energy loss? Let’s go beyond single-particle observables -- What can study of jet observables tell us? David Winter Jets and High-pt Azimuthal Correlations in PHENIX 4

  5. Same-event pairs 3.0<pT<6.0 Mixed-event pairs Correct for limited h acceptance and single-particle efficiency Observed yield per trigger Real yield per trigger particle Correlation Functions • Azimuthal correlations are an alternative approach to jet studies where full reconstruction is impractical • Df is f between leading and associated particles • Correlation functions typically defined as : p+p h± Correlation Function Fit with: 2 Gaussians + Constant Bg term • Conditional Yields can be extracted from correlation when properly normalized and corrected for acceptance and efficiency: David Winter Jets and High-pt Azimuthal Correlations in PHENIX 5

  6. jet Hard-scattering • Partons scatter with large Q2 • Outgoing partons fragment into cone of hadrons • Parameters of interest • Spread of particles around jet axis (jT) • Acoplanarity of back-to-back jets (kT) • Hadronic spectrum (Frag. Func. D(z)) Leading hadron Transverse plane: jT Partons have intrinsic transverse momentum kT: jT = hadron’s momentum transverse to the jet axis David Winter Jets and High-pt Azimuthal Correlations in PHENIX 6

  7. Near-side Correlation • Leading (highest pT) “Trigger” particle used as estimator for jet axis • “Near-Side”: particles from same jet will be correlated in a peak around Df ~ 0 • Simple relations can be derived (assume pT,trig >> jTy): Projection onto transverse plane ftjtrigger-parton fajassociated-parton Assume angles are statistically independent Near-side peak Note there are corrections to these expressions, but they are small See J. Jia, nucl-ex/0409024 for further details David Winter Jets and High-pt Azimuthal Correlations in PHENIX 7

  8. Away-side Correlation • “Away-Side”: particles from (nearly) back-back jets form a peak at Df ~ p • Average di-jet acoplanarity kT can be extracted from angles btn hadrons: Projection onto transverse plane ftjtrigger-parton fajassociated-parton fjj parton-parton Assume angles are statistically independent Away-side peak Again, there are small corrections… cf. nucl-ex/0409024 David Winter Jets and High-pt Azimuthal Correlations in PHENIX 8

  9. Jet Modifications • One of the most exciting results at RHIC has been the behavior of the away-side peak in azimuthal correlations PHENIX Preliminary Courtesy W.Holzmann, 21st WWND There is little if any difference between p+p, d+Au away-side peak (esp. at high pT), but the broadening of away-side peak in Au+Au is striking! David Winter Jets and High-pt Azimuthal Correlations in PHENIX 9

  10. p+p p+A A+A kT comparison • Comparison of p+p/d+Au/Au+Au allows separation of medium effects • We see little, if any, difference between kT of p+p & d+Au • Disappearance of away-side in Au+Au complicates this comparison... PHENIX Preliminary p0 PHENIX Preliminary PHENIX Preliminary 1d RMS kTztrig product using p0 and p± as triggers David Winter Jets and High-pt Azimuthal Correlations in PHENIX 10

  11. Future Measurements • Correlation method requires rough binning in pT • Observables extracted as averages within these rough bins • Corresponding bin widths also need to be “extracted” • Alternatively, statistical weighting can be used to extract distributions directly • Example: • Away-side dN/dxE sensitive to the fragmentation function (e.g.. at high-pT, slopes of dN/dxE and D(z) are related) • See upcoming d+Au Correlations paper, to be submitted to PRC PHENIX Preliminary p± p± PHENIX Preliminary David Winter Jets and High-pt Azimuthal Correlations in PHENIX 11

  12. Summary • Traditional jet-finding methods are unpractical in RHIC collisions. Azimuthal Correlations make jet studies possible this high multiplicity environment • Study of the jet structure (jT, kT) allows us to distinguish between vacuum, initial-state, and final-state effects • Evolution of jet structure from pp to AuAu collisions • No difference btn pp & dAu, but broadening of di-jet peak in AuAu • Look for upcoming publications • (nucl-ex/0410003) “Formation of dense partonic matter in relativistic heavy-ion nucleus-nucleus collisions at RHIC: Experimental evaluation by the PHENIX collaboration” • (nucl-ex/0408007) “Jet Structure of Baryon Excess in Au+Au collisions at sNN = 200 GeV” • (nucl-ex/0404024) J. Jia, HotQuarks04 proceedings • Jets and correlations: p+p, d+Au, and Au+Au David Winter Jets and High-pt Azimuthal Correlations in PHENIX 12

  13. Backup Slides David Winter Jets and High-pt Azimuthal Correlations in PHENIX 13

  14. qg+gq qq Fraction of produced p0s gg pT (GeV/c) Relative Gluon/Quark Contrib. • In current measurement, p0s mainly produced by gg and qg scattering Kretzler, hep-ph/0410219 David Winter Jets and High-pt Azimuthal Correlations in PHENIX 14

  15. Au+Au p0 + X (peripheral) Peripheral spectra agree well with p+p (data & pQCD) scaled by Ncoll Is It Hard-scattering? • Single-particle spectrum and QCD predictions Au+Au p0 + X (central) PHENIX Collab. PRL91, 241803 hep-ex/0304038 Strong suppression David Winter Jets and High-pt Azimuthal Correlations in PHENIX 15

  16. Correlations Example d+Au s=200 GeV 5<pT,trig<10 GeV/c 2<pT,assoc<3 GeV/c Same-event Mixed-event Mimics acceptance Same / Mixed Fully-corrected Acceptance divides out David Winter Jets and High-pt Azimuthal Correlations in PHENIX 16

  17. Red: data Blue: pythia 5<pT,trig<6 Comparison with Pythia p+p s=200 GeV (Run3) Pythia results agree within ~20% David Winter Jets and High-pt Azimuthal Correlations in PHENIX 17

  18. How high is high (multiplicity)? • Central events: Npart ~ 300 • dNch/dh ~ 450 • Most particles are p’s dN/dh ~ 670 David Winter Jets and High-pt Azimuthal Correlations in PHENIX 18

More Related