Experimental Results on Jets in Heavy Ion Collisions Yen-Jie Lee - - PowerPoint PPT Presentation

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Experimental Results on Jets in Heavy Ion Collisions Yen-Jie Lee - - PowerPoint PPT Presentation

Experimental Results on Jets in Heavy Ion Collisions Yen-Jie Lee Massachusetts Institute of Technology XLVII International Symposium on Multiparticle Dynamics 12 September, 2017 1 Yen-Jie Lee XLVII International Symposium on Multiparticle


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SLIDE 1

Yen-Jie Lee 1 XLVII International Symposium on Multiparticle Dynamics

Yen-Jie Lee Massachusetts Institute of Technology

XLVII International Symposium on Multiparticle Dynamics 12 September, 2017

Experimental Results on Jets in Heavy Ion Collisions

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SLIDE 2

Yen-Jie Lee

Reconstruct the Quark Gluon Plasma

2 XLVII International Symposium on Multiparticle Dynamics

O(10-15 m) O(1m) O(1013 m) O(1027 m) QGP

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SLIDE 3

Yen-Jie Lee

Prepare the Quark Soup

3 XLVII International Symposium on Multiparticle Dynamics

Particle Multiplicity

  • Collision impact parameter of the ions
  • Energy density of the medium

Azimuthal anisotropy

  • Early thermalization <1 fm/c
  • Shear viscosity
  • Fluctuation of vN coefficients

from particle azimuthal correlation: Initial-state geometry fluctuation

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SLIDE 4

Yen-Jie Lee

Beyond the Analysis of Debris

4 XLVII International Symposium on Multiparticle Dynamics

  • How does the strongly interacting medium

emerge from an asymptotic free theory (QCD)?

  • Can we see quasi particles

(quarks and gluons) and medium resonse in the Quark Gluon Plasma?

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SLIDE 5

Yen-Jie Lee

Beyond the Analysis of Debris

5 XLVII International Symposium on Multiparticle Dynamics

  • How does the strongly interacting medium

emerge from an asymptotic free theory (QCD)?

  • Can we see quasi particles

(quarks and gluons) and medium resonse in the Quark Gluon Plasma?

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SLIDE 6

Yen-Jie Lee

Hard Probes in Heavy Ion Collisions

6 XLVII International Symposium on Multiparticle Dynamics

Photons / Z Quark Gluon Plasma

In medium parton energy loss

 “Jet quenching” (Bjorken, 1982) Jets and hadrons from High energy quarks and gluons Studies of the medium properties Photons, electroweak bosons

Transport coefficient 𝑟, stopping power dE/dx, gluon density

𝑒𝑂𝑕 𝑒𝑧 , temperature 𝑈…

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SLIDE 7

Yen-Jie Lee

Parton Energy Loss Models

XLVII International Symposium on Multiparticle Dynamics

Collisional energy loss Radiative energy loss

AdS/CFT “drag force”

Perturbative QCD Weak coupling limit

Holographic calculation

Strong coupling limit

  • Two theoretical approaches:

(neither of them are the full stories and both of them are effective descriptions in proper regimes)

7

  • The main problem: we don’t know how to describe the interaction

between the hard scattered parton and QGP (a multi-scale problem)

JEWEL SCETG HYBRID

CCNU

Q-PYTHIA CUJet3.0 JETSCAPE

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SLIDE 8

Yen-Jie Lee

Jet Quenching

8 XLVII International Symposium on Multiparticle Dynamics

QGP

What is the mechanism of jet quenching?

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SLIDE 9

Yen-Jie Lee

Jet RAA up to pT ~ 1 TeV

9 XLVII International Symposium on Multiparticle Dynamics

  • Jet RAA < 1 : quenched energy goes out of the jet cone
  • Similar results from the STAR measurement on the h-jet at RHIC
  • Significant jet suppression at high pT (up to ~ 1 TeV!)
  • If the suppression is purely due to energy loss

→ Energy transported out of the cone is O(100) GeV! What is the fraction of parton energy going out of the jet cone? Can we capture all the quenched energy by jet reconstruction? Anti-kT R=0.4 Jet RAA in 2.76 and 5.02 TeV

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SLIDE 10

Yen-Jie Lee

Absolute Energy Loss with Z+Jet at 5 TeV

10 XLVII International Symposium on Multiparticle Dynamics

Z Boson Jet

arXiv 1702.01060 PRL 119, 082301 (2017)

pp PbPb

x=pT

Jet / pT boson

1 pp PbPb

Jet quenching (E-loss)

~ 15% of the energy went out of the jet cone (R=0.3)

Momentum conservation in the transverse direction

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SLIDE 11

Yen-Jie Lee

Absolute Energy Loss with γ+Jet at 5 TeV

11 XLVII International Symposium on Multiparticle Dynamics

xJγ=pT

Jet / pT γ

CMS-PAS-HIN-16-002 (2017)

ATLAS-CONF-2016-110

pp PbPb

PbPb

Photon Jet

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SLIDE 12

Yen-Jie Lee

Photon-Jet Data vs. Theoretical Predictions

12 XLVII International Symposium on Multiparticle Dynamics

CMS-PAS-HIN-16-002 (2017)

PbPb

Photon pT 40-50 GeV/c 50-60 GeV/c 60-80 GeV/c

  • JEWEL: pQCD 2 to 2 scattering extrapolated to infrared region +

recoil parton

  • LBT: pQCD Transport model with medium recoil and thermalization
  • f the quenched energy
  • HYBRID Model: PYTHIA8 + AdS/CFT drag force (strong coupling)
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SLIDE 13

Yen-Jie Lee 13 XLVII International Symposium on Multiparticle Dynamics 13 XLVII International Symposium on Multiparticle Dynamics

“QGP Rutherford experiment”

Jet Jet Photon Photon

“Backscattering”?

Search for Quasi-Particles in the QGP

PbPb

ATLAS-CONF-2016-110

No significant modification

QGP probed looks smooth

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SLIDE 14

Yen-Jie Lee

Hadron-Jet Angular Correlation

14 XLVII International Symposium on Multiparticle Dynamics

Df

No significant broadening QGP probed looks smooth

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SLIDE 15

Yen-Jie Lee

Jet Quenching

15 XLVII International Symposium on Multiparticle Dynamics

QGP

Do gluons lose more energy than the quarks?

If Yes: Gluon jet to quark jet ratio will decrease (Gluon jets are more suppressed)

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SLIDE 16

Yen-Jie Lee

Charged Jet pTD (Dispersion) and Jet Girth

16 XLVII International Symposium on Multiparticle Dynamics

Quark Gluon Gluon Quark

  • Jets in PbPb are more Quark-like! (Gluon jets suppressed)

PbPb PbPb Anti-kT R=0.2 40<pT<60 GeV

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SLIDE 17

Yen-Jie Lee 17 5th Heavy Ion Jet Workshop

Jet Longitudinal Structure

  • Fragmentation functions Ratio RD(z) between PbPb and pp collisions at 5 TeV
  • Enhancement at large z (high pT particles in jet): smaller gluon/quark ratio in PbPb
  • Weak or no dependence on the jet pT

→ If switch to γ-tagged jet (mainly quarks), will this enhancement go away?

QGP Jet axis Δr

ATLAS-CONF-2017-005

Projection to jet axis

RD(z) = PbPb / pp

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SLIDE 18

Yen-Jie Lee

Photon-Tagged Fragmentation Function

18 XLVII International Symposium on Multiparticle Dynamics

  • First γ-tagged fragmentation function!
  • Decrease the population of gluon jets:

~70% of the tagged jets are quark jets

  • Significant modification in PbPb

with respect to pp reference is observed

Photon Jet

  • No high z (or small ξ=ln(1/z) ) enhancement observed!
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SLIDE 19

Yen-Jie Lee

Jet Quenching

19 XLVII International Symposium on Multiparticle Dynamics

QGP

Do we see medium response?

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SLIDE 20

Yen-Jie Lee

Δ Jet axis

QGP

20 XLVII International Symposium on Multiparticle Dynamics

Where does the Quenched Energy Go?

Leading jet Subleading jet

JHEP 01 (2016) 006

  • Quenched energy carried by
  • Average momentum of those

particles are higher than that from medium debris → Not Completely Thermalized?

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SLIDE 21

Yen-Jie Lee

Jet Transverse Structure

21 XLVII International Symposium on Multiparticle Dynamics

Anti-kT R=0.4 Ratio: PbPb/pp 0.7-1 GeV 1-2 GeV 3-4 GeV Δr Jet axis

  • Jet shapes and fragmentation functions in pp and PbPb collisions at 5 TeV
  • Sensitive to the possible medium response to hard probes and induced radiation

Jet shapes in pp and PbPb at 5.02 TeV

CMS-PAS-HIN-16-020

pp PbPb

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SLIDE 22

Yen-Jie Lee

Theoretical Interpretation of the excess

22 XLVII International Symposium on Multiparticle Dynamics arXiv:1701.07951

arXiv:1707.01539

JEWEL SCETG HYBRID

CCNU

Different explanation of the large angle enhancement in jet shape measurement

  • SCETG: Splitting function (large angle radiation)
  • JEWEL & JETSCAPE: medium recoil parton
  • CCNU: recoil parton + hydro dynamical evolution
  • HYBRID: fully thermalized medium response

See talk from Ivan Vitev, Yasuki Tachibana, Abhijit Majumder

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SLIDE 23

Yen-Jie Lee

Jet Quenching

23 XLVII International Symposium on Multiparticle Dynamics

QGP

Can we groom away the soft radiation? (focus on the hard jet core) Can jet quenching depends on the structure of parton shower?

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SLIDE 24

Yen-Jie Lee

Groomed Jet Substructure with Soft Drop

CMS: used two grooming settings with ΔR>0.1 cut

XLVII International Symposium on Multiparticle Dynamics

subjet From Yi Chen “Jet Core” “Default”

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SLIDE 25

Yen-Jie Lee

Groomed Jet Mass

25 XLVII International Symposium on Multiparticle Dynamics

0-10% 0-10%

(zcut,β) = (0.1,0.0) (zcut,β) = (0.5,1.5)

  • Enhancement of large mass when looking

at a less aggressive grooming setting

  • Results with a “more aggressive grooming”
  • No significant modification of the “jet core”

“Jet Core” ΔR>0.1 ΔR>0.1 Anti-kT R=0.4 “Default”

CMS-PAS-HIN-16-024

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SLIDE 26

Yen-Jie Lee

Momentum Sharing of Subjets

26 XLVII International Symposium on Multiparticle Dynamics

  • Quark and gluon Zg distributions are very similar in pp
  • Jets with two hard subjets (large Zg) “relatively” more

suppressed than jets with a single core (small Zg)

(Or small Zg is enhanced)

pT,1 pT,1 pT,2 pT,2 One hard subjet Two hard subjets Zg small Zg ~ 0.5 (zcut,β) = (0.1,0.0)

arXiv:1708.09429

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SLIDE 27

Yen-Jie Lee

CMS Groomed Jet Splitting Function

27 XLVII International Symposium on Multiparticle Dynamics

  • JEWEL: enhancement of low Zg jets (due to medium recoil)
  • SCETG: modification due to medium induced splitting function
  • HT & Coherent antenna BDMPS: Data prefer coherent energy loss
  • Measurement of rg and groomed RAA would help to separate models

arXiv:1708.09429

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SLIDE 28

Yen-Jie Lee

Summary

28 XLVII International Symposium on Multiparticle Dynamics

  • Consistent picture of energy flow with respect to jet at LHC

from ALICE, ATLAS and CMS

  • Modification of jet shapes and fragmentation function
  • Jet substructure become more quark-like
  • Quenched energy out of the cone (R>0.5) carried by low pT particle
  • Hint of medium response from LHC data
  • Different interpretations from theory groups
  • Situation at RHIC is not as clear as at LHC
  • Opportunity for STAR and sPHENIX
  • “Parton shower shape dependence” of jet quenching:
  • Groomed jet substructure: a power tool for the highly differential

studies of jet quenching

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SLIDE 29

Yen-Jie Lee 29 XLVII International Symposium on Multiparticle Dynamics

Backup slides

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SLIDE 30

Yen-Jie Lee

Compilation of the charged hadron RAA

30 XLVII International Symposium on Multiparticle Dynamics

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SLIDE 31

Yen-Jie Lee

Jet RAA vs. rapidity

31 XLVII International Symposium on Multiparticle Dynamics

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SLIDE 32

Yen-Jie Lee

Dijet asymmetry

32 XLVII International Symposium on Multiparticle Dynamics

  • Progress on the 2-D unfolding from ATLAS
  • Hint of peak structure in the low pT bin
  • bserved at the threshold
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SLIDE 33

Yen-Jie Lee 33 XLVII International Symposium on Multiparticle Dynamics

Jet Longitudinal Structure

Charged hadron RAA Jet RAA

ATLAS-CONF-2017-005

RD(z) = PbPb / pp

  • Fragmentation functions Ratio RD(z) between PbPb and pp collisions at 5 TeV
  • Enhancement at large z: consistent with smaller gluon/quark ratio in PbPb data
  • Modified fragmentation could be the reason why

high pT charged hadron RAA > jet RAA

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SLIDE 34

Yen-Jie Lee

Comparison between Z-Jet and Photon-Jet

34 XLVII International Symposium on Multiparticle Dynamics

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SLIDE 35

Yen-Jie Lee

STAR Jet Splitting function

35 XLVII International Symposium on Multiparticle Dynamics

 Direct comparison to embedded p+p – no unfolding  Selected di-jets with hard cores:

No significant modification of the splitting function in Au+Au observed with zg

pT

Trig,Recoil: Calculated with pT,cut>2 GeV/c

zg: Measured on matched jets with pT,cut>0.2 GeV/c

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SLIDE 36

Yen-Jie Lee

Groomed jet pT fraction

36 XLVII International Symposium on Multiparticle Dynamics

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SLIDE 37

Yen-Jie Lee

CMS Jet Mass

37 XLVII International Symposium on Multiparticle Dynamics

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SLIDE 38

Yen-Jie Lee

CMS Jet Mass vs. Jet energy

38 XLVII International Symposium on Multiparticle Dynamics

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SLIDE 39

Yen-Jie Lee

ALICE Hadron-Jet

39 XLVII International Symposium on Multiparticle Dynamics

No sizable modification of jet shape

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SLIDE 40

Yen-Jie Lee

Missing pT from high pT particles increases as a function of AJ In pp Balanced by 2-8 GeV/c particles In 0-10% PbPb Balanced by particles with pT < 4 GeV/c

XLVII International Symposium on Multiparticle Dynamics

PP

0-10% PbPb

More energy flow in the leading jet direction More energy flow in the subleading jet direction

40

JHEP 1601 (2016) 006

Missing pT

|| vs. AJ

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SLIDE 41

Yen-Jie Lee

CMS Groomed Jet Splitting Function

41 XLVII International Symposium on Multiparticle Dynamics

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SLIDE 42

Yen-Jie Lee

CMS Groomed Jet Splitting Function

42 XLVII International Symposium on Multiparticle Dynamics

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SLIDE 43

Yen-Jie Lee

Groomed Jet Mass (Q vs G)

43 XLVII International Symposium on Multiparticle Dynamics

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SLIDE 44

Yen-Jie Lee

Groomed Jet Mass (Q vs G)

44 XLVII International Symposium on Multiparticle Dynamics

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SLIDE 45

Yen-Jie Lee

Charged Particle RAA vs. Theoretical Models

45 XLVII International Symposium on Multiparticle Dynamics

  • General trend described by pQCD based and Hybrid models
  • A full description of the RAA is still challenging for some models

SCETG CUJet3.0 HYBRID

2.76 TeV

JEWEL

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SLIDE 46

Yen-Jie Lee

Jet RAA vs. Theory

46 XLVII International Symposium on Multiparticle Dynamics

HYBRID JEWEL

CCNU

SCETG

arXiv:1509.07257

R=0.9 R=0.6 Large effect from recoil

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SLIDE 47

Yen-Jie Lee

Z-Jet vs calculations

47 XLVII International Symposium on Multiparticle Dynamics

  • Important to have correct pp baseline
  • Reasonable agreement between data and theory curves from JEWEL, HYBRID and GLV
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SLIDE 48

Yen-Jie Lee

N-Subjettiness in PbPb at 2.76 TeV

48 XLVII International Symposium on Multiparticle Dynamics

  • Small τ2/ τ1 related to leading parton splitting into 2 resolvable partons
  • Medium modification could shift τ2/ τ1 to higher values
  • No significant difference between PbPb data and PYTHIA within the uncertainties
  • Could JEWEL, HYBRID, CCNU and SCETG reproduce this data?
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SLIDE 49

Yen-Jie Lee

Missing pT

|| vs. Δ

High pT imbalance at small Δ

Balanced by low pT particles in subleading jet direction Extends upto large Δ

XLVII International Symposium on Multiparticle Dynamics

JHEP 1601 (2016) 006

Inclusive AJ

Subleading jet direction Leading jet direction

Slight modification of the cumulative energy flow

49

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SLIDE 50

Yen-Jie Lee

“Shooting Jets with Different Width” through the Medium

XLVII International Symposium on Multiparticle Dynamics

Small R parameter Large R parameter

  • Quenched energy distribution depends on the R parameter used

in the Anti-kT algorithm

  • Hint of narrower leading jet (or wider subleading jet) in PbPb

collisions.

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JHEP 1601 (2016) 006

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SLIDE 51

Yen-Jie Lee

“Shooting Jets with Different Width” through the Medium

XLVII International Symposium on Multiparticle Dynamics

Narrower jets Wider jets

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HYBRID

  • Medium response from HYBRID is farer away from the jet axis.
  • Shower not completely thermalized?
  • Where are the calculations from JEWEL, CCNU, QPYTHIA and SCETG?
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SLIDE 52

Yen-Jie Lee

Jet Quenching with Inclusive Charged Particles

52 XLVII International Symposium on Multiparticle Dynamics

  • Similar Charged particle RAA in PbPb

at 5 TeV compared to

  • Good agreement between ATLAS, CMS

and ALICE measurements

JHEP 04 (2017) 039 ATLAS-CONF-2017-012

5 TeV

RAA

  • Almost no suppression at very high pT

compared to pp reference

  • Charged particle RAA measured up to

pT = 400 GeV for the first time!

Charged particle RAA

  • Strong suppression of charged particles

(up to a factor of 6) in PbPb compared to pp

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SLIDE 53

Yen-Jie Lee

Charged Particle RAA vs. Theoretical Models

53 XLVII International Symposium on Multiparticle Dynamics

  • General trend described by pQCD based and Hybrid models
  • A full description of the RAA is still challenging for some models

SCETG CUJet3.0 HYBRID

0-10% 30-50%

SCETG CUJet3.0

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SLIDE 54

Yen-Jie Lee

Description of the D0 Meson Data

54 XLVII International Symposium on Multiparticle Dynamics

  • At high D0 pT: Trend captured by pQCD and AdS/CFT based models
  • Reasonable description of the data could be achieved
  • Details doesn’t work perfectly, especially the slope of the D0 RAA vs. pT

arXiv:1708.04962

SCETG CUJet3.0

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SLIDE 55

Yen-Jie Lee

Dijet Transverse Momentum Correlation

55 XLVII International Symposium on Multiparticle Dynamics

arXiv:1609.03878 R=0.2 R=0.4 XJ=pT,2/pT,1

  • STAR: Di-jet pairs seeded with “hard core”
  • No significant energy flow out of the jet

cone R~0.4 in this subset of dijets

  • ATLAS: inclusive dijet (resolution unfolded)
  • Peak at ~ 0.5
  • Check from CMS?
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SLIDE 56

Yen-Jie Lee

Nuclear Modification Factors (RAA)

56 XLVII International Symposium on Multiparticle Dynamics

X

RAA =

  • From a Glauber model calculation
  • Validated by isolated photon, W and Z

production studies (RAA~ 1)

Z boson RAA (PbPb at 5 TeV)

No significant modification of colorless probes in PbPb collisions

ATLAS-CONF-2017-010

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SLIDE 57

Yen-Jie Lee

Jet Quenching with Inclusive Charged Particles

57 XLVII International Symposium on Multiparticle Dynamics

  • Similar Charged particle RAA in PbPb

at 5 TeV compared to

  • Good agreement between ATLAS, CMS

and ALICE measurements

JHEP 04 (2017) 039 ATLAS-CONF-2017-012

5 TeV

RAA

  • Almost no suppression at very high pT

compared to pp reference

  • Charged particle RAA measured up to

pT = 400 GeV for the first time!

Charged particle RAA

  • Strong suppression of charged particles

(up to a factor of 6) in PbPb compared to pp

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SLIDE 58

Yen-Jie Lee

Flavor Dependence of Parton Energy Loss

58 XLVII International Symposium on Multiparticle Dynamics

arXiv:1708.04962

  • RAA is meson flavor dependent at low hadron pT
  • Disappearance of the effect at high hadron pT
  • Results are consistent with the expectation from models with parton flavor

dependent energy loss

b→J/ψ B+

D0 h±

b→J/ψ

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SLIDE 59

Yen-Jie Lee

PHENIX Photon-Hadron Correlation

59 XLVII International Symposium on Multiparticle Dynamics

Low pT Photon 5-7 GeV High pT Photon 12-20 GeV γ Indication of wide angle radiation carried by soft particle. Significant modification of jet FF No modification of jet fragmentation (?) Something in between Significant modification

  • f jet FF

Plot from Wei Chen

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SLIDE 60

Yen-Jie Lee

ALICE Charged Jet Mass

60 XLVII International Symposium on Multiparticle Dynamics

HYBRID

  • Data sit between JEWEL recoil on and off
  • HYBRID need medium recoil to describe the ALICE data
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SLIDE 61

Yen-Jie Lee

STAR Hadron-Jet Correlation

61 XLVII International Symposium on Multiparticle Dynamics

arXiv:1702.01108

R=0.2 R=0.3 R=0.4 R=0.5

  • R=0.2-0.4
  • ICP significantly lower than unity; significant out-of-cone Eloss
  • R=0.5 ICP > R=0.2 ICP
  • indication of the recovery of the quenched energy
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SLIDE 62

Yen-Jie Lee

Jet Flavor Composition in Dijet and γ-Jet

62 XLVII International Symposium on Multiparticle Dynamics

50% Gluon 20% Gluon From Doga Gulhan

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SLIDE 63

Yen-Jie Lee

STAR Splitting Function

63 XLVII International Symposium on Multiparticle Dynamics

  • STAR: Di-jet pairs seeded with “hard core”
  • No significant modification in this subset of dijet
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SLIDE 64

Yen-Jie Lee 64 XLVII International Symposium on Multiparticle Dynamics

Quenched Energy out of the Jet Cone

Leading jet Subleading jet

JHEP 01 (2016) 006

  • Quenched energy carried by
  • Average momentum of those

particles are higher than that from medium debris → Not Completely Thermalized?

CCNU Model

Δ Jet axis

QGP “Reheating” the QGP

See talk from Yasuki Tachibana

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SLIDE 65

Yen-Jie Lee

Medium Response

65 XLVII International Symposium on Multiparticle Dynamics

SCETG HYBRID JEWEL

Medium Recoil without re-scattering

We also don’t know how much the medium response (recoil) plays a role in the description of the jet quenching observables and how to describe it correctly

No Medium Recoil Medium Recoil and Back-reaction With Re-scattering “Reheating the QGP” Medium response

CUJet3.0

CCNU

Q-PYTHIA JETSCAPE