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Exploring Hot Dense Matter at RHIC and LHC Peter Jacobs Lawrence Berkeley National Laboratory Lecture 4: Jets and jet quenching 6/23/111 Hot Matter at.

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Presentation on theme: "Exploring Hot Dense Matter at RHIC and LHC Peter Jacobs Lawrence Berkeley National Laboratory Lecture 4: Jets and jet quenching 6/23/111 Hot Matter at."— Presentation transcript:

1 Exploring Hot Dense Matter at RHIC and LHC Peter Jacobs Lawrence Berkeley National Laboratory Lecture 4: Jets and jet quenching 6/23/111 Hot Matter at RHIC and LHC - Lecture 4

2 2 QCD: running of  S 0.2 fm0.02 fm0.002 fm ConfinementAsymptotic Freedom 6/23/11 Low momentu m High momentum

3 Hot Matter at RHIC and LHC - Lecture 43 Perturbative QCD factorization in hadronic collisions pQCD factorization: + fragmentation fn D h/c + partonic cross section  parton distribution fn f a/A Hard process scale Q 2 >>   QCD 6/23/11

4 What really happens to produce a jet… 4 Beam Remnants Beam Remnants p = (uud) p = ,K,p,n,…} Jet Initial State Radiation (ISR) Hadronization Final State Radiation (FSR) Detector 6/23/11Hot Matter at RHIC and LHC - Lecture 4

5 Jets at CDF/Tevatron Good agreement with NLO pQCD 5Hot Matter at RHIC and LHC - Lecture 46/23/11

6 Jets in heavy ion collisions 6/23/11Hot Matter at RHIC and LHC - Lecture 46 Controlled “beams” with well-calibrated intensity Final-state interactions with colored matter are calculable using controlled approximations → tomographic probe of the Quark-Gluon Plasma

7 6/23/11Hot Matter at RHIC and LHC - Lecture 47 Jet

8 Jets in real heavy ion collisions Hot Matter at RHIC and LHC - Lecture 48 RHIC/Star LHC/CMS 6/23/11

9 Jet quenching 9 Total medium-induced energy loss: Plasma transport coefficient : 6/23/11Hot Matter at RHIC and LHC - Lecture 4 Radiative energy loss in QCD (multiple soft scattering):

10 Leading hadron as a jet surrogate 10 - Energy loss  softening of fragmentation  suppression of leading hadron yield Binary collision scaling p+p reference 6/23/11Hot Matter at RHIC and LHC - Lecture 4 PHENIX Phys Rev D76, 051106  p+p √s=200 GeV

11 Jet quenching I: leading hadrons are suppressed, photons are not 11 Jet fragments (color-charged) Photons (color- neutral) Jet quenching 6/23/11Hot Matter at RHIC and LHC - Lecture 4

12 Jet quenching at the LHC: ALICE 6/23/11Hot Matter at RHIC and LHC - Lecture 412 Phys. Lett. B 696 (2011) peripheral central pTpT pTpT p+p reference at 2.76 TeV: interpolated

13 Jet quenching: RHIC vs LHC 6/23/11Hot Matter at RHIC and LHC - Lecture 413 RHIC  0, , direct  RHIC/LHC charged hadrons RHIC/LHC: Qualitatively similar, quantitatively different Where comparable, LHC quenching is larger  higher color charge density

14 Hot Matter at RHIC and LHC - Lecture 414 LHC jet quenching: comparison to pQCD-based models Main variation amongst models: implementations of radiative and elastic energy loss Models calibrated at RHIC, scaled to LHC via multiplicity growth Key prediction: p T -dependence of R AA (  E ~ log (E) ) - OK Qualitatively: pQCD-based energy loss picture consistent with measurements We can now refine the details towards a quantitative description 6/23/11

15 Di-hadron correlations as a jet surrogate 15 STAR, Phys Rev Lett 90, 082302 trigger 6/23/11Hot Matter at RHIC and LHC - Lecture 4 trigger

16 Jet quenching II: di-hadrons 6/23/11Hot Matter at RHIC and LHC - Lecture 416 Recoiling jet is strongly altered by medium Clear evidence for presence of very high density matter STAR, Phys Rev Lett 91, 072304 Azimuthal separation of high pT hadron pairs trigger recoil X Jet quenching

17 Di-hadron correlations at high-pt Central collisions High-pT Reaperance of the away side peak at high-assoc.-pT: similar suppression as inclusive spectra no angular broadening Differential measurement of jets w/o interaction 176/23/11Hot Matter at RHIC and LHC - Lecture 4

18 QCD analysis of jet quenching 18  Model calculation: ASW quenching weights, detailed geometry Simultaneous fit to data. Armesto et al. 0907.0667 [hep-ph] Conditional yield 6/23/11Hot Matter at RHIC and LHC - Lecture 4 ~Self-consistent fit of independent observables Data have good precision: limitation is accuracy of the theory

19 19 Hot Matter at RHIC and LHC - Lecture 4 Jet quenching: pQCD vs AdS/CFT Weak-coupling pQCD (Baier et al.): Strong-coupling N=4 SYM (Liu, Rajagopal and Wiedemann): NOT proportional to N C 2 ~ entropy density Proportional to N C 2 ~ entropy density Roughly

20 Full jet reconstruction Hot Matter at RHIC and LHC - Lecture 420 Jet quenching is a partonic process: can we study it at the partonic level? Jet reconstruction: capture the entire spray of hadrons to reconstruct the kinematics of the parent quark or gluon 6/23/11

21 Jet measurements in practice: experiment and theory 21 colinear safety: finite seed threshold misses jet on left? infrared safety: one or two jets? Fermilab Run II jet physics hep-ex/0005012 Algorithmic requirements: same jets at parton/particle/detector levels independence of algorithmic details (ordering of seeds etc) 6/23/11Hot Matter at RHIC and LHC - Lecture 4

22 22 Modern jet reconstruction algorithms Cone algorithms – Mid Point Cone (merging + splitting) – SISCone (seedless, infr-red safe) Sequential recombination algorithms k T anti-k T Cambridge/ Aachen Algorithms differ in recombination metric:  different ordering of recombination  different event background sensitivities Jet Fragmentation Hard scatter Cone jet K T jet 6/23/11Hot Matter at RHIC and LHC - Lecture 4 Modern implementation: FastJet (M. Cacciari, G. Salam, G. Soyez JHEP 0804:005 (2008))

23 Jets at CDF/Tevatron Good agreement with NLO pQCD Multiple algorithms give consistent results 23Hot Matter at RHIC and LHC - Lecture 46/23/11

24 Jet measurements over large background Background fluctuations distort measured inclusive cross section 24 unfolding Pythia Pythia smeared Pythia unfolded Hot Matter at RHIC and LHC - Lecture 46/23/11

25 Inclusive jet cross sections at √s=200 GeV 256/23/11Hot Matter at RHIC and LHC - Lecture 4 M. Ploskon QM09 Consistent results from different algorithms Background correction ~ factor 2 uncertainty in xsection

26 Inclusive cross-section ratio: p+p R=0.2/R=0.4 26 Narrowing of the jet structure with increasing jet energy Solid lines: Pythia – particle level 6/23/11Hot Matter at RHIC and LHC - Lecture 4 compare within same dataset: systematically better controlled than R AA

27 Inclusive cross-section ratio in p+p: compare to NLO pQCD 27 Narrowing of structure with increasing energy NLO pQCD calculation W. Vogelsang – priv. comm. 2009 Solid lines: Pythia – particle level NLO: narrower jet profile  hadronization effects? 6/23/11Hot Matter at RHIC and LHC - Lecture 4

28 28 Jet hadronization pQCD factorization: + fragmentation fn D h/c + partonic cross section  parton distribution fn f a/A 6/23/11

29 Hadronization effects: HERWIG vs. PYTHIA 6/23/11Hot Matter at RHIC and LHC - Lecture 429 Different hadronization models generate closely similar ratios

30 σ(R=0.2)/σ(R=0.4) : NNLO calculation |η|<0.6 30Hot Matter at RHIC and LHC - Lecture 46/23/11 G. Soyez, private communication QCD NLO QCD NNLO PYTHIA parton level PYTHIA hadron level HERWIG hadron level p+p √s=200 GeV Broadening due to combined effects of higher order corrections and hadronization

31 Incl. cross-section ratio: Au+Au R=0.2/R=0.4 6/23/1131Hot Matter at RHIC and LHC - Lecture 4 Marked suppression of ratio relative to p+p  medium-induced jet broadening Main result of this analysis

32 Incl. cross-section ratio Au+Au: compare to NLO 6/23/1132Hot Matter at RHIC and LHC - Lecture 4 NLO with jet quenching (GLV) B.-W. Zhang and I. Vitev Phys. Rev. Lett. 104, 132001 (2010) Stronger broadening in measurement than NLO …work in progress for both experiment and theory…

33 Jets at LHC LHC: jet energies up to ~200 GeV in Pb+Pb from 1 ‘short’ run Large energy asymmetry observed for central events 6/23/1133Hot Matter at RHIC and LHC - Lecture 4

34 6/23/11Hot Matter at RHIC and LHC - Lecture 434

35 6/23/11Hot Matter at RHIC and LHC - Lecture 435

36 LHC Pb+Pb: Dijet energy imbalance 6/23/11Hot Matter at RHIC and LHC - Lecture 436 Purely calorimetric measurement: significant (unknown?) systematic uncertainties due to cutoffs and non-linearities for low p T hadrons  connection to jet quenching? Large energy asymmetry in central collisions: seen by CMS and ATLAS

37 Recall the summary of Lecture 1: scorecard 6/23/11Hot Matter at RHIC and LHC - Lecture 437 What is the nature of QCD Matter at finite temperature? What is its phase structure? What is its equation of state? What are its effective degrees of freedom? Is it a (trivial) gas of non-interacting quarks and gluons, or a fluid of interacting quasi-particles? What are its symmetries? Is it correctly described by Lattice QCD or does it require new approaches, and why? What are the dynamics of QCD matter at finite temperature? What is the order of the (de-)confinement transition? How is chiral symmetry restored at high T, and how? Is there a QCD critical point? What are its transport properties? Can QCD matter be related to other physical systems? Can we study hot QCD matter experimentally? Red=progress Blue=interesting ideas Black=still thinking

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