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1 Oliver Busch for the ALICE collaboration Jet Physics with ALICE Oliver Busch – Tsukuba 2014 /03/13.

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Presentation on theme: "1 Oliver Busch for the ALICE collaboration Jet Physics with ALICE Oliver Busch – Tsukuba 2014 /03/13."— Presentation transcript:

1 1 Oliver Busch for the ALICE collaboration Jet Physics with ALICE Oliver Busch – Tsukuba 2014 /03/13

2 2 introduction results from pp jets in heavy-ion collisions results from Pb-Pb collisions jets in p-Pb collisions outlook: LHC run 2 Outline Oliver Busch – Tsukuba 2014 /03/13

3 3 Introduction Oliver Busch – Tsukuba 2014 /03/13

4 4 Jets: seeing quarks and gluons jet: collimated spray of hadrons quasi-free parton scattering at high Q 2 : the best available experimental equivalent to quarks and gluons Oliver Busch – Tsukuba 2014 /03/13

5 5 Jet fragmentation initial hard scattering: high-p T partons cascade of gluons: parton shower at soft scale (O(Λ QCD )): hadronization Oliver Busch – Tsukuba 2014 /03/13

6 Jet reconstruction Establish correspondence between detector measurements / final state particles / partons two types of jet finder: - iterative cone - sequential recombination (e.g. anti-k T ) resolution parameter R hep-ph/0802.1189

7 LHC aerial view 7 Oliver Busch – Tsukuba 2014 /03/13

8 Jets at ALICE (LHC run 1) jet trigger with EMCal and TRD `charged’ (tracking) jets and `full’ jets full jets from charged particle tracking and EM energy: conceptually different and complementary to traditional approach charged particle tracking: - Inner Tracking System (ITS) - Time Projection Chamber - full azimuth, |η |< 0.9 p T > 150 MeV/c EMCal : - neutral particles - Δ φ = 107°, |η|<0.7 cluster E T > 300 MeV 8

9 9 Results from pp collisions Oliver Busch – Tsukuba 2014 /03/13

10 Full jets in pp at = 2.76 TeV good agreement to NLO calculations for R = 0.2 and R = 0.4 reference for Pb-Pb at same energy Phys. Lett. B 722 (2013) 262 10 R = 0.2 R = 0.4 Oliver Busch – Tsukuba 2014 /03/13

11 measured in minimum bias collisions at = 7 TeV good agreement with ATLAS charged jet measurements (despite slightly different acceptance and track p T range) pp charged jet cross-sections 11 R = 0.4R = 0.6 nucl-ex/1411.4969 Oliver Busch – Tsukuba 2014 /03/13

12 pp jet fragmentation at = 7 TeV distributions of charged particles in charged jets scaling for z > 0.2 bulk production at low z: ~ 5-10 charged particles per jet nucl-ex/1411.4969

13 PID in jets : `TPC coherent fit’ particle identification via specific ionization in TPC ('dE/dx'): TPC coherent fit: use energy loss model parameterization as input, adjust model parameters and particle fractions `on the fly’ during fit regularization requiring continuity of particle fractions complementary and consistent: multi-template fit 13 Oliver Busch – Tsukuba 2014 /03/13

14 Particle identified fragmentation identified charged hadrons in charged jets at = 7 TeV π, K, p, 5 < p T ch jet < 20 GeV/c scaling for z ch > 0.2 for higher jet p T bins 14 Oliver Busch – Tsukuba 2014 /03/13

15 Particle ratios in jets strangeness content strongly enhanced for z ch → 1 leading baryons suppressed 15 Oliver Busch – Tsukuba 2014 /03/13

16 Event generator comparison comparison to PYTHIA (p T ordered parton shower, Lund string fragmentation) data reasonably well described best reproduced by Perugia tune without color reconnections

17 17 Jets and Quark-Gluon Plasma Oliver Busch – Tsukuba 2014 /03/13

18 in heavy-ion collisions at ultra-relativistic energies, a quasi macroscopic fireball of hot, strongly interacting matter in local thermal equilibrium is created lattice QCD predicts phase transition to deconfined, chirally symmetric matter energy density from the lattice: rapid increase around T C, indicating increase of degrees of freedom (pion gas -> quarks and gluons) T C = 154+/- 9 MeV E C = 340 +/- 45 MeV/fm 3 QCD phase transition HotQCD, PRD 90, 094503

19 hard partons are produced early and traverse the hot and dense QGP enhanced energy loss: `jet quenching’ ‘vacuum’ expectation calculable by pQCD : ‘calibrated probe of QGP’ jets sensitive to properties of the medium (energy density,, mfp, coupling... )... but also jet/medium interaction not trivial (strong / weak coupling, parton mass / type, fireball dynamics... ) Partons in heavy-ion collisions JET collaboration, arXiv: 1312.5003

20 20 high- p T hadrons `proxy’ for jet jet quenching for charged hadrons, Pb-Pb collisions at √s NN = 2.76 TeV hadron observables biased towards leading fragment → study the effect for fully reconstructed jets PLB 720 (2013) 250 Hadrons in heavy-ion collisions Oliver Busch – Tsukuba 2014 /03/13

21 centralperipheral jet reconstruction in heavy-ion collisions : difficult due to the high underlying event background not related to hard scattering correct spectra for background fluctuations and detector effects via unfolding not possible down to 0 p T jet area ~ 0.5 (R = 0.4) Underlying event in heavy-ion collisions

22 Jet nuclear modification factor strong suppression observed, similar to hadron R AA -> parton energy not recovered inside jet cone increase of suppression with centrality mild p T dependence JEWEL and YaJEM jet quenching models reproduce suppression nucl-ex/1502.01689 JEWEL: PLB 735 (2014) YaJEM:PRC 88 (2013) 014905

23 Jet structure ‘ jet structure ratio’ R=0.2 / R=0.3 for charged jets sensitive to potential broadening of jet shape consistent with PYTHIA pp: no modification observed within small radii (jet core ) JHEP 03 (2014) 013

24 24 Results from p-Pb collisions Oliver Busch – Tsukuba 2014 /03/13

25 25 p + Pb collisions at √s NN = 5.02 TeV check potential initial state effects (nuclear modification of PDF) and effects of cold nuclear matter measured spectrum consistent with POWHEG NLO calculations ( = NLO + PYTHIA fragmentation) Charged jets in p-Pb collisions nucl-ex/1503.00681 Oliver Busch – Tsukuba 2014 /03/13

26 26 R pPb using scaled charged jet spectrum measured at 7 TeV as reference no jet suppression observed in p-Pb -> suppression in Pb-Pb is final state effect Charged jet R pPb nucl-ex/1503.00681 Oliver Busch – Tsukuba 2014 /03/13

27 `jet structure ratio’ R=0.2 / R=0.4 for different centrality classes no modification, even for most central p-Pb Jet structure in p-Pb 27 Oliver Busch – Tsukuba 2014 /03/13

28 28 Perspectives for LHC run 2 Oliver Busch – Tsukuba 2014 /03/13

29 LHC run 2: 2015 - 2017 increased CMS energy for Pb-Pb collisions from 2.76 → 5.1 TeV quenching strength ~ s ~ ε 3/4 expect (modest) increase in ε, T → measure energy density dependence of jet quenching note: also a dependence on parton ‘input spectrum’ (increased R AA ??? ) LHC run 2 ALICE, PRL 105, 252301

30 ALICE in run 2: DCal run 2: DCal upgrade - significantly extended jet acceptance - back-to-back in azimuth (di-jet topology) 30 Oliver Busch – Tsukuba 2014 /03/13

31 Summary jet cross sections and properties in pp identified jet fragmentation in pp strong jet suppression observed in Pb-Pb collisions p-Pb results: initial-state and cold-nuclear-matter effects negligible looking forward to LHC run 2 ! 31 Oliver Busch – Tsukuba 2014 /03/13

32 Jet reconstruction Establish correspondence between detector measurements / final state particles / partons two types of jet finder: - iterative cone - sequential recombination (e.g. anti-k T ) resolution parameter R hep-ph/0802.1189

33 Jet finder comparison ● k T : sequential recombination ● SISCone: cone algorithm 33 nucl-ex/1411.4969

34 34 Multi Template Fit TPC multi-template fit - best possible description of dE/dx from external reference - parametrize dependences on η, TPC nClusters - templates in transverse momentum (z, xi) slices dE/dx in one z slice (0.6 < z < 0.65), 10-15 GeV/c fitted with 4 templates

35 Method comparison uncorrected hadron fractions from Multi-Template Fit and TPC Coherent Fit 2 complementary methods obtain consistent results

36 transverse structure: p T sum in radial slices increasing collimation for higher p T jets fragmentation and jet structure reasonably described by event generators pp jet structure at = 7 TeV 36 nucl-ex/1411.4969

37 direct photons: thermal radiation from the early stage of the fireball indicates initial temperature way above T C QCD matter at LHC 37

38 38 Reaction plane dependence different medium thickness in- and out-of plane sensitive to path length dependence of jet quenching pQCD radiative E-loss : ~L 2 collisional E-loss : ~L strong coupling (ADS/CFT) : ~L 3

39 39 Local background subtraction prerequisite: take event plane dependence of background density into account event-by-event local ρ fit

40 40 Jet v2 : results charged jets, R = 0.2 quantify azimuthal asymmetry via 2 nd Fourier harmonic v2 strongly hints to non-zero jet v2

41 jet uncorrected Recoil jets semi – inclusive recoil jet spectra : - reduce fake jet background through ‘dijet’ topology - residual combinatorics subtracted in Δ recoil observable trigger hadron surface biased maximize path length for jet →

42 fully corrected Δ recoil : R=0.2 and R=0.4 measurement down to constituent p T of 150 MeV/c, for large radii (up to R = 0.5) and low jet p T, without biasing leading constituent Δ recoil 42

43 ΔI AA : compare to PYTHIA pp reference suppression observed ΔI AA 43

44 Δ recoil Ratio R=0.2 / R=0.5 : sensitive to potential broadening of jet structure consistent with PYTHIA within large experimental uncertainties Jet structure ratio 44

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