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High p T flow and jet quenching at CMS Yongsun Kim (Korea University) Nov. 2 nd 2013, HIM meeting Inha University, Incheon, Korea.

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Presentation on theme: "High p T flow and jet quenching at CMS Yongsun Kim (Korea University) Nov. 2 nd 2013, HIM meeting Inha University, Incheon, Korea."— Presentation transcript:

1 High p T flow and jet quenching at CMS Yongsun Kim (Korea University) Nov. 2 nd 2013, HIM meeting Inha University, Incheon, Korea

2 Yongsun Kim (Korea University) Overview Motivation of Probing QGP by high energy partons Reconstruction of particles, jets and photons in CMS Analysis and results –Hard probe scale 1 : 100 - 300GeV  Di-jet counting –Hard probe scale 2 : 60 - 100GeV  Gamma-jet counting –Hard probe scale 3 : 10 - 60GeV  Particle correlation Summary 3

3 Yongsun Kim (Korea University) Probing QGP with a high energy parton Study of QED using Deep inelastic scattering using a charged particle as a probe Analogy for a QCD system –Charge : QCD (EM)  QCD (color) –Probe : Electron  Parton (q,g) –Observable Modification of momentum of probe 4 Probe from outside Probes from inside QGP Pb

4 Yongsun Kim (Korea University) But, we can not directly measure partons Problem : Quarks and gluons can not be detected in isolated state Solution : Jet –Indirect measurement of partons –Bunch of fragmentation of high energy partons –SNOWMASS accords, including Collinear, infrared safety. High p T hadrons –Most of them are from jet fragmentation –Indirect probe for quenching 5

5 Yongsun Kim (Korea University) CMS Detector 6 Ecal Hcal Barrel, Edncap Si tracker Charged particles reconstructed by tracker Photon reconstructed by Ecal Jet reconstructed by tracker + Ecal + Hcal 100% 50% 30% 10% 0% HF Determines Impact parameter

6 Yongsun Kim (Korea University) Reconstruction of hadrons in CMS Individual objects sorted into 3 classes –Particle Flow in CMS terminoloty Charged particles –Silicon Tracker –Nice momentum resolution < 2% for 100GeV Neutral hadrons –Energy in Calorimenter but no tracks Photons ( neutral meason) –Energy concetrated in ECAL 7 Arxiv:0802.1189

7 Yongsun Kim (Korea University) Reconstruction of Jet in CMS Anti-kt jet algorithm –A sequential clustering algorithm, but shaped in a circular cone –Infrared- & Collinear- safe (by construction) –Only single parameter. R = Jet Resolution (or radius) –Known to be favored by theorists (P. Schieferdeckers in lecture) Particle flow objects are uses as the ingredients Background subtraction algorithm for PbPb and pPb –To subtract the energy piled up from underlying events –UE subtracted tower-by-tower ( size = 0.087 x 0.087 ) before jet clustering In CMS heavy ion group, R = 0.3 ( relatively small ) is used to reduce the fluctuation of underlying events 8 Arxiv:0802.1189 JHEP 0804 (2008) 063

8 Yongsun Kim (Korea University) Reconstruction of isolated photon in CMS Isolated photons comes from hard scattering. –Not decayed from neutral meson –Not thermal photon Superclustering algorithm in CMS –Find the EM shower and recover the bremsstrahlung energy In pp, energy resolution 100GeV 9

9 Yongsun Kim (Korea University) Analysis/results Jets in 100GeV < p T < 300GeV –Correlation of Di-jet events Charged particles in O(1) GeV < p T < 60GeV –Correlation of particles Jets around 50 GeV –Gamma-jet correlation 10

10 Yongsun Kim (Korea University) Correlation of di-jets 11 PLB 712 (2012) 176 Increase of mono-jet events in central collisions compared to pp, while the angular correlation is consistent with pp Leading jet p T > 100GeV Sub-leading jet p T > 30GeV ΔΦ > 2π/3

11 Yongsun Kim (Korea University) Correlation of di-jets : Momentum ratio Asymmetry of p T 1 /p T 2 gradually increases by collision centrality 12 PLB 712 (2012) 176

12 Yongsun Kim (Korea University) Momentum correlation of di-jets 13 PLB 712 (2012) 176 Compared with (Unquenched) PYTHIA embedded in HYDJET (uncerlying events) simulation to exclude detector bias and generic asymmetry from initial state in pp( or pn, nn) collision. DATA – MC of the ratio was flat as a function of p T leading

13 Yongsun Kim (Korea University) Jet fragmentation 14 Jet fragmentation - Energy fraction and momentum direction of each hadrons in the jet Gluon radiation by QGP modifies the virtuality of parton can modify the Fragmentation pattern CMS measured the inclusive jets above 100TeV in PbPb and compared with pp Observable 1 : Fragmentation function Observable 2 : Jet shape (arxiv:1310.0878) PYTHIA hadrons

14 Yongsun Kim (Korea University) Modification of jet fragmentation -1 15 Significant excess of low energy hadrons observed and the effect gradually increases in more central collisions.

15 Yongsun Kim (Korea University) Modification of jet fragmentation -2 16 Re-distribution of jet energy observed. Depletion of intermediate radii ( 0.1 < r < 0.2) and Excess of distant fragmentation ( r > 0.2 )

16 Yongsun Kim (Korea University) Two Particle correlation In the traditional particle correlation, the low p T particle correlation characterizes the collective particle dynamics In high p T trigger particle correlation, jet plays the major role 17 PRL 109 (2012) 022301 Jet Total Anisotropy harmonics = + Both Jet and harmonics delivers jet quenching message, but in different ways

17 Yongsun Kim (Korea University) 1. Observation of anisotropy Event plane method using HF calorimeter Non-zero v 2 of High p T particles (10 - 30GeV) implies the path length dependence of jet quenching 18

18 Yongsun Kim (Korea University) 2. Extraction of jet-like 2 particle correlation ZYAM procedure used to determine a 0 coefficient –Assumed Jet-like correlation is 0 around ΔΦ = π/2 19 JetTotal Anisotropy harmonics

19 Yongsun Kim (Korea University) 2. Extraction of jet-like 2 particle correlation Then integrated the yield in near side and away side Definition of I AA –PbPb/pp Ratio of yield of associated particles in a same p T trigger bin 20 JetTotal Anisotropy harmonics

20 Yongsun Kim (Korea University) Near side I AA (ΔΦ <1) Excess of low p T particles <2GeV Energy lost by jet quenching transforms into multiple low energy particles 21

21 Yongsun Kim (Korea University) Away side I AA (ΔΦ >1) 22 Even more excess of low p T particles <2GeV and suppression of high p T particles Jet quenching happened for the away side jet

22 Yongsun Kim (Korea University) Lessons from particle correlation analysis Suppression of high p T particles in the away side –Trigger particle selection has a surface bias –path length dependence of energy loss Energy lost by quenching transforms into low p T particles 23 Trigger particle Near side Away side

23 Yongsun Kim (Korea University) Can we remove the surface bias? 24 R AA : ratio of cross sections of heavy ion collision to pp after binary collision scaling Jet γ (photon)γ (photon) YES using photon-jet! PLB 710 (2012) 256 CMS has excellent photon isolation power to control S/(S+B) to be 70% - 90%. Remaining background photons are statistically subtracted using shower shape fitting Smaller width Larger width π0π0

24 Yongsun Kim (Korea University)  -jet correlations Event selection –Photon p T > 40GeV –Jet p T >30GeV –Back-to-Back : ΔΦ > 7π/8 Observables –1. Angular correlation –2. Rate of finding Jets –3. Momentum correlation –4. Yield of jets per photon –5. p T dependence of each observables 25 p T Jet pTγpTγ Combinatorial backgrounds are subtracted 1.Jets from underlying events 2.Photons from neutral meson

25 Yongsun Kim (Korea University) 1. Angular Correlation 26 All data points and MC reference have consistent width around 0.25

26 Yongsun Kim (Korea University) 2. Rate  -jet /  In Pb+Pb data, number of jet partners are significantly less than in MC reference Indicates that the jet lost energy and goes below 30GeV threshold 27 pp More jet partners disappeared

27 Yongsun Kim (Korea University) 3. Momentum Ratio 28 p T Jet pTγpTγ Gradual shift of to lower x was observed

28 Yongsun Kim (Korea University) Summary of  -jet correlation Observation 1 High momentum parton is NOT distracted by the medium Observation 2 Significant number of jet partners are submerged (below the jet p T threshold) Observation 3 Overall momentum ratio p T Jet /p T γ are reduced 29 Jet γ p T Jet pTγpTγ

29 Yongsun Kim (Korea University) pPb collision First jet anlaysis in pPb –Di-jet correlation in pPb collisions pPb collsions at LHC –March 2013 –Sqrt(s NN ) = 5.02 TeV Di-jet selection –p T leading > 120GeV –p T subl > 30GeV –back-to-back : ΔΦ = 2π/3 30

30 Yongsun Kim (Korea University) Exclusion of cold nuclear effect in quenching Momenta of di-jet pairs are balanced Confirms that the momentum asymmetry in PbPb is not from initial state 31 Events divided into 5 bins by Forward energy activity

31 Yongsun Kim (Korea University) Di-jet pesudo-rapidity constrains nPDF 32 p pb CT10+EPS09 matches better than CT10. What does this indicate? Escola, Paukkunen, Salgado. arxiv:1308.6733

32 Yongsun Kim (Korea University) Di-jet pesudo-rapidity constrains nPDF 33 EMC Anti-shadowing Shadowing Pseudo-rapidity of di-jet reflects the parton momentum fraction in Pb ion Modification indicates the EMC, Anti-shadowing and shadowing effect in various momentum fraction regimes p pbpb

33 Yongsun Kim (Korea University) Di-jet η modification vs HF energy Strong modification of di-jet pseudo-rapidity distribution –longitudinal momentum fraction tends to be larger as proton scatters the Pb ion near the center. 34

34 Yongsun Kim (Korea University) Summary Hard probes in heavy ion experiments are very useful to understand the QCD interaction of the hot and dense matter CMS has excellent apparatus to reconstruct hard probes and has carried out heavy ion collision experiments with PbPb at 2.76TeV from 2010 and pPb in 2013 Significant energy loss of partons in PbPb collisions were observed in di-jet, gamma-jet and particle correlation study Those effects were confirmed not to be initial state modification by analyzing pPb collisions at 5.02TeV Modification of momentum fraction in Pb ions were measured which provides strong constraints of nPDF New Hard Probe results will be public soon  35

35 Yongsun Kim (Korea University) BACK UP 36

36 Yongsun Kim (Korea University) LHC Heavy Ion Program 37 LHC CMS Heavy ion (Pb) beam began to circulate the LHC ring from Nov. 2010 √s NN = 2.76TeV. ALICE ATLAS

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