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Jet Probes at RHIC

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Title: Jet Probes at RHIC


1
Jet Probes at RHIC
  • Justin Frantz
  • Stony Brook University
  • FRIF Workshop on QCD Power Corrections
  • January 13, 2006

2
The Heavy Ion/QGP Mission
  • in the context of this workshop
  • See qs/gs outside of pQCD
  • (Often delicate) NP effects in pQCD jet event
    shape
  • Lattice QCD predicts deconfinement phase change
    ? a Quark Gluon Plasma
  • Specifically, observe collective behavior of many
    q/gs in this plasma?
  • Larger Scale observables
  • Temperature, Pressure, Density
  • Also how does it modify particle physics?
  • Chiral symmetry restoration?
  • Color screening melts J/Psi?
  • aS modified _at_ finite Temp.

Lattice Calculation
Energy Density / T4
pion gas
T/TC
TC estimates 170 MeV
3
RHIC
  • The Relativistic Heavy Ion Collider QGP Search

STAR
NYC
RHIC
  • Collides AuAu, pp, dAu, CuCu, at energies vs
    , 20, 62, 130, 200, 400, 500 GeV
  • Polarized proton beams, Spin program ? probe
    gluon spin structure

4
Highlights of Basic Results
  • Runs 1/yr 2001-2006 interesting yield of
    results
  • Requisite Densities
  • Thermalization success of statistical models w/
    T in the critical range
  • Hydrodynamic Flow Too large for ideal QGP but
    evidence against hadron gas
  • Baryon/Meson flow vs pT follows (common!) quark
    number scaling instead of mass scaling
  • Hydro-models with only hadrons fail to reproduce
  • Hadron cross sections (esp. strange) too small to
    build it up
  • Large Baryon Excess at soft-hard transition
    energies (p/p 1)
  • Recombination of quarks promising way to explain
  • Strongly interacting QGP
    (sQGP) perfect liquid

5
Hard Scattering Probes
AuAu ? gdirect X
AuAu ? p0 X
pp ? p0 X
  • Hard scattering in AuAu ? pQCD (works well in
    pp)
  • Insert into HI medium, observe differences
  • E.g. high pT hadron and direct photon production
  • High pT spectral shapes clearly power law as
    expected for all centralities
  • And same shape same as pp

6
RAA
  • Ratio of AA/ scaled pp
  • Scaling factor number of equiv NN crossings
    (Ncoll)
  • FLAT
  • Prediction jet energy loss leads to suppression
    effect for fragmentation products
  • But not for EM direct photons
  • Energy loss models depend on dN/dygluons
  • Many models LPM effect, Modified D(z)
  • ? Density!
  • DE E was surprise (just E shift - like NP?)

7
Elliptic Flow (v2)
  • In semi-central events initial state spacial f
    anisotropy ? momentum space
  • v2 second Fourier harmonic w/ w.r.t the
    (measured) global reaction plane
  • 2 Kinds
  • At low pT (soft), hydrodynamic (of quarks we
    believe)
  • At high pT, energy loss of jet partons traversing
    the matter

PHENIX
dN/d?
Incl. Hadrons
pT 3-4 GeV/c
8
Di-Jet Di-Hadron Correlations
  • Huge Soft background (dN/dh 1000)
  • Jet Finding difficult (Impossible?) in HI
    environment
  • Rely on 2-particle opening angle (azimuthal)
    correlations
  • 2 categories in pT Trigger (high pT) Assoc


6 5 4 3 2 1
Nearside Awayside
STAR
200 GeV pTtrig 5-10, pTassoc 1-2 GeV/c
h-h
AuAu
pp
PHENIX
9
Experimental Method Flow Subtraction
  • Assume 2-source correlation Flow Jet
  • Main source of systematic error
  • b0 determined by Zero Yield At Minimum (ZYAM),
    other methods

PHENIX p0h pTtrig 5-10 GeV/c pTassoc 3-5
GeV/c
Note scale
10
First Results (High x Low pT)
  • Jet suppression of awayside shape
  • Nearside per trigger yield same
  • Absolute NS yield suppressed
  • At low pT, recovered

4-6 x 2-4 GeV/c
0.2
0.1
0.0
0
p
w/ pT,assoc ? 0.2 GeV/c
0
p
11
High x High Re-emergence
  • Low/No Background (Flow Sub. Unimportant)
  • Clear emergence of jet structure at the away-side
  • Away side width consistent with constant
  • Away side yield suppressed

STAR Preliminary
8 lt pT(trig) lt 15 GeV/c
pT(assoc)gt6 GeV/c
12
Really Weird! Low x Low
  • Large modication on the awayside!
  • Cone/ Volcano shape
  • Medium response to the jets?
  • Explained by
  • Mach cone sound wave
  • Color cerenkov cone
  • Bending jets
  • If Mach Cone, size ? vsound ? direct measure of
    matter property

2.5-4 GeV/c trig
STAR
1-2.5 GeV/c assoc
PHENIX
p
0
Df
13
How Robust is The Volcano?
  • Still questions about robustness (oversubtraction
    in v2?)
  • Look _at_ trigger w.r.t. RP
  • Over subtraction? opposite effect

In plane
14
IAA etc.
  • Looking for best way to analyze extracted jet
    (f-integrated) yields
  • Good parameter pT, zT,xE ?
  • IAA ratio of integrated per-trigger yield in
    AA/pp
  • How does it fit together with RAA? Better
    quantity? Still open

An Eloss model Wang et. al.
Phys. Lett. B579 (2004) 299308.
STAR Awayside IAA ( RAA !)
15
Direct g-Jet
  • In central AuAu high suppression effect ? higher
    purity of direct g
  • Complement of jet-jet Eloss
  • Probes interior of collision volume
  • Eg proxy for Ejet
  • Extraction of gdirect-jet from ginclusive
    correlations underway

pp 200 GeV
gdir-jet
jet-jet
16
Jet Event Shapes _at_ RHIC
What am I doing _at_ this workshop?
  • Good things _at_ RHIC
  • Not just AA pp, pA, polarized pp ( lots!)
  • Dectectors optimized for soft physics (Good E,p
    resolution/ PID above 50 MeV) in addition to
    hard
  • Bad things
  • As hh, central rapidity restriction
  • Ambiguity of Q/vs12
  • In AuAuwell e.g. no jet finding (jets
    modified!)etc
  • From your standpoint
  • For pp, best source of low Q? (mid-h x ranges
    like Tevatron/LHC, but lower s)
  • AuAu Interesting modification to hadronization
    could Power Correction frameworks say anything
    sensible? How about in dAu ?
  • From HI experimentalist standpoint
  • Want to use jets to probe medium event shapes
    are a natural goal

17
Energy Energy Correlations
  • Instead of muliplicity correlations, energy flow,
    correlations (combining info in all pT bins)
  • No jet finding neccesary
  • auto-convolution of JCEF ?other shape observable
    as correlations?
  • Sensitive to aS , NP effects (plasma?)

(p c)
18
EEC in hh?
  • EEC never measured in hh?
  • Structure Fn complication x1x2 distribution of Q
  • But theory work says it should be possible
  • Basham, Et al Use Tranverse EEC(f)
  • Gale et. al. QGP multiple scatt. ? large effects
    to TEEC (hep-ph/9406208)
  • Measured and used in DIS
    _at_ HERA (1 S.F.)

19
EEC in AA
  • 2 EECs in AA? sQGP has its own? (beyond
    flow?)
  • Large flow harmonic contribution
  • Extract Jet EEC
  • Large underlying ET (shape
    distorting)
  • Combinatoric pair subtraction
  • PHENIX ½ f solid ang. ? missed ET even pp

Lokhtin et al., hep-ph/0402108
20
Effect of Inaccurate ET
  • Pythia study of EEC (200 GeV pp)

In PHENIX
ET (GeV)
Q (GeV)
Q (GeV)
Ratio to Blue (Arbitrary Norm)
EEC w/ Phenix ET Denom
EEC(f) A.U.
EEC w/ real Phx Acc
Q 10-15 GeV/c
EEC w/ true Q in Denom
EEC w/ ET in Denom
Df
Df
21
Idea EEC Direct-Gamma Events
  • Similar to the DIS t-channel
  • Does it probe the same properties? (g/q jet)
  • Ever done before?
  • Two varieties
  • only charged particles-Eg only
  • Including neutral (w/ direct g)
  • Is one better?

2Eg TRIG (GeV)
PYTHIA direct g events
Q (GeV)
PYTHIA direct g events Eg 10-15 GeV
EEC(f) A.U.
f
22
Conclusions
  • Interesting time at RHIC
  • Jet/Hard observables continue to provide key
    information
  • We see jet modification!
  • Can we use traditional event shape?
  • same perturbative inspired frameworks?
  • Need help from theorists
  • What can be calculated?
  • What can be learned?

23
Flat RAA? (Energy Loss)
  • Example of using hard scattering probes

24
Understanding RAA(Npart, ??)
  • Can we find a consistent description of
    centrality and ?? dependence of RAA?
  • Define with
  • Perform survival-weighted average over all
    production points, emission directions.
  • Survival weighting

25
(No Transcript)
26
Energy Loss Calculations
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