what can be learned from identifying leading hadrons of jets in star? kolja kauder for the star...
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![Page 1: What Can be Learned from Identifying Leading Hadrons of Jets in STAR? Kolja Kauder for the STAR Collaboration](https://reader035.vdocuments.mx/reader035/viewer/2022081519/56649f435503460f94c62d2b/html5/thumbnails/1.jpg)
What Can be Learned from Identifying Leading Hadrons of Jets in STAR?
Kolja Kauder for the STAR Collaboration
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Outline Introduction / Motivation
Quark Gluon Plasma Experimental Setup Jets as Probes via 2D Correlation Analyses Identifying Trigger Particles to Study Particle
Production Particle Identification Method Results
Jet Cone Dilution by Background Triggers Ridge (and Away-Side): Higher Harmonics
Summary and Outlook
Feb 2013Kolja Kauder, LLWI 2013
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Stages of a Heavy Ion Collision
Feb 2013Kolja Kauder, LLWI 2013
Quark Gluon Plasma: Hot Liquid Strongly Interacting Quark & Gluon DOF
Measured ~400 nucleons
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The STAR Detector
Feb 2013Kolja Kauder, LLWI 2013
Au+Au, 200 GeV
Full azimuthal acceptance Pseudorapidity acceptance |
h|<1.8 Particle Identification
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Tomography
Feb 2013Kolja Kauder, LLWI 2013
Trigger
associates
associates associate
s
Dihadron Correlation
Selecting Trigger ID: Jet Cone “Ridge” Away-Side
STAR, PRL 91 (2003) 072304
0-10% central
4 < pT,trig < 5 GeV/c
1.5 < pT,ssc < 4 GeV/c
4 < pTtrig < 6 GeV/c
2 < pTassc < pT,trig
d+Au
4 < pT,trig < 5 GeV/c
1.5 < pT,ssc < 4 GeV/c
0-10% central
4 < pTtrig < 5 GeV/c
1.5 < pTassc < 4 GeV/c
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Baryon vs. Meson Trigger
Feb 2013Kolja Kauder, LLWI 2013
Between 1.5~5 GeV: Enhanced relative baryon yield
Well captured byrecombination/coalescence
Baryon trigger: Stronger Dilution?
STAR, PRL 97 (2006) 152301
=0Df
a. u.
Fragmentation + Recombination
STAR, PLB 637 (2006) 161
Gluon contribution factor
Albino et al.NPB 725 (2005) 181
AKK NLO FFs describe data well
At high pT: Mesons bias toward q
jets? Color charge effect on
energy loss?
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Kolja Kauder, LLWI 20137
Statistical Separationin Two Steps
Feb 2013
Inclusive, raw
nsp > 0.
97% purity pion sample
nsp < 0,
pion-depleted sample
πKP
nsp < 0, cleaned
pure p+K sample
0-10% central4 < pT
trig < 5
GeV/c1.5 < pT
assc < 4
GeV/c
nsπ = (dE/dx - π prediction) /resolution
nsπ
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Kolja Kauder, LLWI 20138
2D Correlation
Big difference immediately visible with the naked eye: Pion triggers: Small Ridge Large Cone P+K triggers: Large Ridge Small Cone
Feb 2013
(P±+K±) trigger
p± trigger
Dilution? Need d+Au
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Kolja Kauder, LLWI 20139
2D Correlation – d+Au
No appreciable ridge Cone is similar in d+Au
Signs of dilution are there, but subtle
Feb 2013
(P±+K±) trigger
p± trigger
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Kolja Kauder, LLWI 201310
2D Correlation
Jet Cone Yield:p : d+Au Au+Au ~25%P+K: d+Au ~ Au+Au
Feb 2013
(P±+K±) trigger
p± trigger
p increase instead of P decrease
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Kolja Kauder, LLWI 201311
Source of the Ridge
Feb 2013
Front runner:
Hydro: Initial State Anisotropy Final State
Multitude of Ridge models
Radiation + Jet Quenching
Radiation + Longitudinal Flow
Phantom Jet Turbulent Color Fields Momentum Kick Medium Heating and
Parton Recombination ...
Ridge: Odd harmonics not negligible
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Scaling of Fourier Coefficients
Feb 2013Kolja Kauder, LLWI 2013
Expect flow-like harmonics to scale with quark number
Non-Pions: P / K ratio also measured.
Indications that V2 and V3 scale differently
Statistical errors only
0-10% central
4 < pT,trig < 5 GeV/c
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Kolja Kauder, LLWI 201313
Summary
Feb 2013
Identified Triggers Jet Cone: Associated yield much larger for pion
than proton+kaon triggers.
Signs of enhancement compared to d+Au Ridge: Associated yield smaller for pions. Scaling
behavior constrains models
Outlook: Quantify comparison to ReCo Proton-Kaon separation Quark vs. Gluon Jets?
Albino et al.NPB 725 (2005) 181
Gluon contribution factor
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14 Feb 2013Kolja Kauder, LLWI 2013