Title: High pT Hadron Correlation
1High pT Hadron Correlation
and No Correlation
Rudolph C. Hwa University of Oregon
Hard Probes 2006 Asilomar, CA, June 10, 2006
2A. Conventional scenario
Hard scattering ? high pT jet ? hadron
correlation
(usual conductor has resistance)
(superconductor has no resistance)
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4same side
STAR
5Associated particle pT distribution
p1 -- trigger
p2 -- associated
6Associated particle distribution in the
recombination model -- for ?? only Hwa
Tan, PRC 72, 057902 (2005)
7Medium modified dihadron fragmentation function
-- more relevant at higher pT.
Majumder, Wang, Wang nucl-th/0412061
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9Away side
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11? production in AuAu central collision at 200 GeV
recombination
fragmentation
Hwa CB Yang, PRC70, 024905 (2004)
1212
8
pT(assoc)
4
0
4
8
12
16
pT(trig)
13Trigger-normalized fragmentation function
Trigger-normalized momentum fraction
14STAR, nucl-ex/0604018
1512
8
pT(assoc)
4
0
4
8
12
16
pT(trig)
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18Correlation on the near side
?? and ?? distributions
STAR, PRL 95, 152301 (2005)
19Chiu Hwa, PRC 72, 034903 (2005)
At low trigger momentum, hard partons can
originate farther in.
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21Away-side distribution
Casalderrey-Solana, Shuryak, Teaney Mach
cone Dremin Cherenkov gluons Ruppert, Muller
color wake Koch, Majumder, Wang
Cherenkov radiation Vitev jet
quenchingfragm . . Chiu, Hwa parton multiple
scattering
22Parton multiple-scattering model
Sample trajectories for 2.5ltp(trig)lt4,
1ltp(assoc)lt2.5
absorbed (thermalized) tracks
exit tracks
23Away-side ?? distribution
Event averaged, background subtracted.
Cannot distinguish between 1-jet and 2-jet
contributions (e.g., Mach cone)
Chius talk in parallel session on Monday
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25Autocorrelation
26Correlation function
Treat 1,2 on equal footing --- no trigger
No ambiguous subtraction procedure only do as
defined.
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28STAR data on Autocorrelation for central AuAu at
130 GeV for ??1.3, 0.15ltpTlt2 GeV/c
NO trigger, no subtraction
nucl-ex/0605021
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30? and ? production at intermediate pT
strange-quark shower is very suppressed.
31Hwa CB Yang, nucl-th/0602024
If they are produced by hard scattering followed
by fragmentation, one expects jets of particles.
32We claim that no shower partons are involved in
???? production, so no jets are involved.
Select events with ? or ? in the 3ltpTlt6 region,
and treat them as trigger particles.
33charged hadrons
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35Forward production of hadrons
Without knowing pT, it is not possible to
determine xF
36Theoretically, can hadrons be produced at xF gt 1?
(TFR)
It seems to violate momentum conservation, pL gt
vs/2.
In the recombination model the produced p and ?
can have smooth distributions across the xF 1
boundary.
37proton
- momentum degradation factor
pion
Hwa Yang, PRC 73,044913 (2006)
38BRAHMS, nucl-ex/0602018
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40Hwa Yang, nucl-th/0605037
Thermal distribution fits well
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42? and p production at high pT at LHC
New feature at LHC density of hard partons is
high.
High pT jets may be so dense that neighboring jet
cones may overlap.
If so, then the shower partons in two nearby jets
may recombine.
43The particle detected has some associated
partners.
There should be no observable jet structure
distinguishable from the background.
44Proton-to-pion ratio at LHC
? -- probability of overlap of 2 jet cones
Hwa Yang nucl-th/0603053
45We predict for 10ltpTlt20 Gev/c at LHC
- NO associated particles above the background
46Summary