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Matter 2012, Washington DC 1 Overview of results on jets from the CMS Collaboration Gábor Veres (CERN) for the CMS Collaboration.

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Presentation on theme: "Matter 2012, Washington DC 1 Overview of results on jets from the CMS Collaboration Gábor Veres (CERN) for the CMS Collaboration."— Presentation transcript:

1 gabor.veres@cern.chQuark Matter 2012, Washington DC 1 Overview of results on jets from the CMS Collaboration Gábor Veres (CERN) for the CMS Collaboration Quark Matter conference, Washington DC 14 th Aug, 2012

2 gabor.veres@cern.chQuark Matter 2012, Washington DC 2 QM’11 – jet energy imbalance Parton energy loss is observed as a pronounced dijet energy imbalance in central PbPb collisions PbPb PbPb PRC 84 (2011) 024906 ppp p

3 gabor.veres@cern.chQuark Matter 2012, Washington DC 3 QM’11 – no  -decorrelation The propagation of high-p T partons in a dense nuclear medium does not lead to a visible angular decorrelation PRC 84 (2011) 024906 PbPb PbPb p p

4 gabor.veres@cern.chQuark Matter 2012, Washington DC 4 QM’11 – energy redistribution The momentum difference in the dijet is balanced by low p T particles mainly at large angles relative to the away side jet axis PRC 84 (2011) 024906

5 gabor.veres@cern.chQuark Matter 2012, Washington DC 5 QM’11 – jet fragmentation Hard part of the fragmentation is independent of energy lost in medium, ~consistent with pp PbPbPbPb  R=0.3 p T > 4GeV/c arXiv:1205.5872 p p

6 gabor.veres@cern.chQuark Matter 2012, Washington DC 6 New research directions for QM’12 Energy loss studies using jets: –Dijet energy imbalance vs jet p T for higher p T jets (120-350 GeV/c) –Jet R AA (100 – 300 GeV/c) –Gamma-jet energy balance –Tagged b-quark jets Jet modification studies using jets and tracks: –Jet shapes: radial distribution of energy flow –Jet fragmentation functions: longitudinal energy flow Energy loss and jet structure studies using tracks: –Charged-hadron R AA up to 100 GeV/c –v 2 of high-p T hadrons up to 60 GeV/c –Two-particle correlations triggered by a high-p T hadron All of them make use of the new, high statistics data taken in 2011! https://twiki.cern.ch/twiki/bin/view/CMSPublic/PhysicsResultsHIN Tue 16:45 M. Nguyen Tue 17:25 M. Tonjes Tue 14:15, Y. Lai Tue 16:45 M. Nguyen Wed 9:50, F. Ma Wed 9:10, P. Kurt Tue 15:55, V. Zhukova Tue 15:15 R. Conway

7 gabor.veres@cern.chQuark Matter 2012, Washington DC 7 How does the dijet imbalance depend on the leading jet energy? ??? Pb+Pb

8 gabor.veres@cern.chQuark Matter 2012, Washington DC 8 Dijet energy ratio (imbalance) Energy imbalance increases with centrality p T -ratio deviates from the unquenched reference in a p T -independent way Tue 16:45, Matt Nguyen PLB 712 (2012) 176 PbPb PbPb

9 gabor.veres@cern.chQuark Matter 2012, Washington DC 9 How much energy do single jets lose? p+pPb+Pb ???

10 gabor.veres@cern.chQuark Matter 2012, Washington DC 10 Nuclear modification factors of jets Suppression: no significant p T –dependence Tue 17:25 Marguerite Tonjes CMS PAS HIN-12-004 PbPb PbPb

11 gabor.veres@cern.chQuark Matter 2012, Washington DC 11 Nuclear modification factors of jets Suppression: no significant cone size dependence Tue 17:25 Marguerite Tonjes CMS PAS HIN-12-004 PbPb PbPb

12 gabor.veres@cern.chQuark Matter 2012, Washington DC 12 PbPb PbPb Charged hadron R AA : update with 2011 data Tue 17:25, Marguerite Tonjes 20 times more data, smaller uncertainties → what is the connection to jet R AA ? EPJC 72 (2012) 1945

13 gabor.veres@cern.chQuark Matter 2012, Washington DC 13 Nuclear modification factors Sampling the ~same parton p T range CMS PAS HIN-12-004 jets Note: jets fragment into high-p T particles in pp and PbPb the same way – see later… charged hadrons

14 gabor.veres@cern.chQuark Matter 2012, Washington DC 14 How can we quantify the jet energy loss with a ‘calibrated’ measurement? ??? Pb+Pb

15 gabor.veres@cern.chQuark Matter 2012, Washington DC 15 How can we quantify the jet energy loss with a ‘calibrated’ measurement? Pb+Pb

16 gabor.veres@cern.chQuark Matter 2012, Washington DC 16  -jet correlations Tue 14:15, Yue Shi Lai arXiv:1206.0206 Photons serve as an unmodified energy tag for the jet partner Ratio of the p T of jets to photons (x J  =p T jet /p T  ) is a direct measure of the jet energy loss Gradual centrality-dependence of the x J  distribution PbPb PbPb

17 gabor.veres@cern.chQuark Matter 2012, Washington DC 17  -jet correlations No  -decorrelation Increasing p T -imbalance Less jet partners above threshold Tue 14:15, Yue Shi LaiarXiv:1206.0206 Jets lose ~14% of their initial energy ~20% of photons lose their jet partner PbPb PbPb x J  =p T jet /p T  R J  = fraction of photons with jet partner >30 GeV/c

18 gabor.veres@cern.chQuark Matter 2012, Washington DC 18 Are heavy-quark jets quenched, too? ??? Pb+Pb p+p b b Pb+Pb p+p udsg

19 gabor.veres@cern.chQuark Matter 2012, Washington DC 19 Tagging and counting b-quark jets Secondary vertex tagged using flight distance significance Tagging efficiency estimated in a data-driven way Purity from template fits to (tagged) secondary vtx mass distributions CMS PAS HIN-12-003

20 gabor.veres@cern.chQuark Matter 2012, Washington DC 20 Pb+Pb p+p Fraction of b-jets among all jets b-jet fraction: similar in pp and PbPb → b-jet quenching is comparable to light-jet quenching (R AA  0.5), within present systematics Tue 16:45 Matt Nguyen, and poster by Jorge Robles CMS PAS HIN-12-003

21 gabor.veres@cern.chQuark Matter 2012, Washington DC 21 How do jets get modified? Do their shape, or fragmentation change? r  Jet shape: p T -flow vs.  -  distance from the jet axis (r): Jet fragmentation function: Distribution of track momenta projected onto the jet axis, presented as a function of  =ln(p jet /p || track ): high  low 

22 gabor.veres@cern.chQuark Matter 2012, Washington DC 22 Track p T distributions in jet cones (R=0.3) High p T (low  ): no change compared to jets in pp collisions In (central) PbPb: excess of tracks compared to pp at low p T (high  ) CMS PAS HIN-12-013 PbPb PbPb (1/GeV)

23 gabor.veres@cern.chQuark Matter 2012, Washington DC 23 Jet fragmentation functions 20 times more data in 2011: decreased uncertainties down to much lower track p T (starting from 1 GeV/c) reveals an excess at high  compared to pp Wed 9:50, Frank Ma CMS PAS HIN-12-013 PbPb PbPb

24 gabor.veres@cern.chQuark Matter 2012, Washington DC 24 What do we expect for the jet shapes? r high  low  Low-  particles tend to be closer to the jet axis; high-  particles extend to large distances (radii). Excess p T -flow is expected at large radii, and no change at r  0 (compared to pp collisions).

25 gabor.veres@cern.chQuark Matter 2012, Washington DC 25 PbPb PbPb Changing jet shapes vs. centrality Compared to pp: same p T -flow close to the jet axis; more p T -flow at large radii; and a bit less in between. Wed 9:10, Pelin Kurt CMS PAS HIN-12-013

26 gabor.veres@cern.chQuark Matter 2012, Washington DC 26 Testing energy loss with high-p T tracks, as a function of azimuthal angle (v 2 ) Overlap zone is almond-shaped → Parton energy loss is smaller along the short axis → More high-p T tracks expected closer to the event plane → Azimuthal asymmetry (v 2 ): → v 2 is sensitive to the path-length dependence of the energy loss Participant plane  pp  EP

27 gabor.veres@cern.chQuark Matter 2012, Washington DC 27 Charged hadron v 2 at very high p T Tue 15:55, Victoria Zhukova v 2 is non-zero up to very high p T Sensitive to the path length dependence of energy loss PRL 109 (2012) 022301 PbPb PbPb

28 gabor.veres@cern.chQuark Matter 2012, Washington DC 28 Studying jet modification: particles associated to a high-p T trigger particle high-p T trigger particle associated particles near side away side High-p T trigger particle from jet fragmentation. Let us subtract all v n harmonics! (n≥2) Expectation on the “near side”: - some excess at low p T (as seen in the jet FF) Expectation on the “away side”: - high p T : deficit compared to pp (quenching) - low p T : excess, due to redistribution of momentum

29 gabor.veres@cern.chQuark Matter 2012, Washington DC 29 High-p T triggered two-particle correlations Tue 15:15, Rylan Conway Away-side: large enhancement below ~3 GeV/c and deficit at higher p T. Near-side: consistent with jet FF’s. All v n harmonics subtracted! (n≥2) CMS PAS HIN-12-010 PbPb Near side Away side

30 gabor.veres@cern.chQuark Matter 2012, Washington DC 30 Summary: jets at QM’12 Energy imbalance and jet R AA independent of jet p T First  -jet measurement shows consistent energy loss Jet-quenching picture is made more precise and quantitative! b-quark jets are also quenched Jet shapes and fragmentation functions show excess at low p T (large radii) but high p T (core) is unchanged v 2 persists to very high p T, reflects path length dependence Two-particle correlations: low-p T enhancement and high-p T suppression on the away side (compared to pp)

31 gabor.veres@cern.chQuark Matter 2012, Washington DC 31 QM’12 talks from CMS on jets Tue 9:30am, Gabor Veres, Overview of results on jets Tue 2:15pm, Yue Shi Lai, Study of jet quenching using photon-jet events in PbPb collisions Tue 3:15pm, Rylan Conway, Short- and long-range very-high-p T triggered dihadron correlations in PbPb collisions Tue 3:55pm, Victoria Zhukova, Azimuthal anisotropy of charged hadrons at very high p T in PbPb collisions Tue 4:45pm, Matthew Nguyen, Studies of jet quenching and b-jet tagging in PbPb collisions Tue 5:25pm, Marguerite Tonjes, Inclusive jet and charged hadron nuclear modification factors in PbPb collisions Wed 9:10am, Pelin Kurt, Jet shapes in pp and PbPb collisions Wed 9:50am, Frank Ma, Jet fragmentation functions in PbPb and pp collisions

32 gabor.veres@cern.chQuark Matter 2012, Washington DC 32 BACKUP

33 gabor.veres@cern.chQuark Matter 2012, Washington DC 33 QM’12 talks from CMS Mon 12:25pm, Gunther Roland, Experimental highlights Mon 5:15pm, Stephen Sanders, Overview of results on flow and correlations Tue 9:30am, Gabor Veres, Overview of results on jets Tue 2:15pm, Yue Shi Lai, Study of jet quenching using photon-jet events in PbPb collisions Tue 2:15pm, Dongho Moon, Detailed measurements of charmonium suppression in PbPb collisions Tue 3:15pm, Rylan Conway, Short- and long-range very-high-p T triggered dihadron correlations in PbPb collisions Tue 3:55pm, Victoria Zhukova, Azimuthal anisotropy of charged hadrons at very high p T in PbPb collisions Tue 4:45pm, Matthew Nguyen, Studies of jet quenching and b-jet tagging in PbPb collisions Tue 4:45pm, Guillermo Rangel, Detailed measurements of bottomonium suppression in PbPb collisions Tue 5:25pm, Marguerite Tonjes, Inclusive jet and charged hadron nuclear modification factors in PbPb collisions Tue 5:45pm, Magdalena Malek, Pseudorapidity and centrality dependence of transverse energy flow in PbPb collisions Wed 8:30am, Hauke Wohrmann, Studies of the nuclear stopping power in PbPb collisions Wed 9:10am, Pelin Kurt, Jet shapes in pp and PbPb collisions Wed 9:50am, Frank Ma, Jet fragmentation functions in PbPb and pp collisions Wed 11:20am, George Stephans, Inclusive isolated photons in pp and PbPb collisions Wed 12:00pm, Lamia Benhabib, W and Z boson production in PbPb collisions Thu 9:45am, Raphael Granier de C., Overview of results on photon and electroweak boson production Thu 11:05am, Camelia Mironov, Overview of results on heavy flavor and quarkonia Fri 2:20pm, Eric Appelt, Elliptic azimuthal anisotropy of charged hadrons and neutral pions in PbPb collisions Fri 3:40pm, Mihee Jo, Suppression of open bottom at high p T via non-prompt J/psi decays in PbPb collisions Fri 5:30pm, Shengquan Tuo, Studies of higher-order flow harmonics and factorization of dihadron correlations in PbPb collisions

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