Au Au vs. p p @ 200 GeV (p0) - PowerPoint PPT Presentation

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Au Au vs. p p @ 200 GeV (p0)

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Peripheral data agree well with Strong suppression in ... First time a large 'shadowing' is seen at small-x and high pT in nuclear syst. ... – PowerPoint PPT presentation

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Title: Au Au vs. p p @ 200 GeV (p0)


1
AuAu vs. pp _at_ 200 GeV (p0)
  • AuAu? p0 X (peripheral)
    AuAu? p0 X (central)
  • Peripheral data agree well with
    Strong suppression in
  • pp (datapQCD) plus Ncoll scaling
    central AuAu collisions

2
Nuclear modification factor (p0)
PHENIX Collab. PRL 91, 072303 (2003)
nucl-ex/0304022

RAA ltlt 1 well below pQCD (collinear
factorization) expectations for hard
scattering cross-section
3
Nuclear modification factor (p0) ?vsNN dependence
  • CERN-SPS PbPb central (vsNN 17.3 GeV) no
    suppression() (within errors)
  • CERN-ISR aa (vsNN 31 GeV) Cronin
    enhancement.
  • RHIC AuAu (vsNN 130, 200 GeV) x 4-5
    suppression.

A.L.S.Angelis, PLB 185, 213 (1987) WA98, EPJ C
23, 225 (2002) () Reanalysis D.d'E.
nucl-ex/0403055 PHENIX, PRL 88 022301
(2002) PHENIX, PRL 91, 072303 (2003)
4
High pT azimuthal correlations jet signals in
AuAu pp
  • dNpair/d?? for trigger (pT gt 4GeV/c)
    associated (pT 2- 4 GeV/c) charg. hadrons

Red histogram pp (flow) Black points
AuAu Blue curve flow contribution
Periph. Central
  • Near-side peak AuAu pp.
  • Trigger hadrons (pT gt 4GeV/c)
  • from jet fragmentation.
  • Away-side peak AuAu ltlt pp
  • Back-to-back jets suppressed
  • ("mono-jet") in central AuAu !

5
High pT azimuthal correlations AuAu dijet
signal disappearance
  • Ratio of AuAu (- flow) over pp azimuthal
    correlation strengths

Near-side peak IAA 1 Away-side peak
IAA 0
6
Unquenched dAu production at high pT
  • Suppression in central AuAu not due to
    initial-state effects

7
dAu nuclear modification factor (? 3.2)
  • Factor 2 suppression
  • pT 1-3 GeV/c hadron
  • production at ? 3.2
  • (x2 10-4 in Au).
  • First time a large shadowing is seen at small-x
    and high pT in nuclear syst.
  • So far unexplored perturbative region of nuclear
    (x,Q2) plane.

Perturbative
non-perturbative
8
Overview (Status of QGP CGC search)
  • 1. Introduction
  • The goal Study Quantum Chromo many-body
    Dynamics QGP, CGC.
  • The means Compare hard scattering production in
    diff. colliding had. systems.
  • 2. QCD vacuum reference results high pT in
    pp
  • Baseline hard scattering data in free space.
  • 3. Hot QCD medium highlights high pT in
    central AA
  • ??dN/dpT light hadrons (u,d,s) suppressed
  • ?s, pT, centrality, and meson-baryon
    dependence
  • ??dNpair/df azimuthal anisotropies
  • dissapearence of away-side dijet correlations
  • ??dN/dpT colorless probes (g) unsuppressed
  • 4. Cold QCD medium highlights high pT in dAu



CGC ?

9
The quest for gluon saturation effects _at_ RHIC ...
  • RHIC kinematical regime
  • High pT _at_ midrapidity
  • y 0, Q2 1-100 GeV2/c2
  • - pQCD collinear factorization
  • - DGLAP evolution (g splitting)
  • - small nuclear effects in PDFs
  • (LT shadowing).
  • Moderate pT, rapidities
  • y 1-3, Q2 10 GeV2/c2
  • - kT factorization
  • - linear BFKL evolution (g splitt.)
  • - moderate nuclear effects (LT
  • shadowing).

(2 ? 2)
x small Look forward in rapidity !
10
AuAu collisions _at_ 200 GeV

600 charged particles per
unit rapidity at midrapidity (top 10 central)
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