Jet-like correlations of heavy-flavor particles - From RHIC to LHC André Mischke Utrecht University 27 th Winter Workshop on Nuclear Dynamics Winter Park,

Jet-like correlations of heavy-flavor particles

- From RHIC to LHC

André Mischke

Utrecht University

27th Winter Workshop on Nuclear DynamicsWinter Park, Colorado – February 6-13, 2011

WWND 2011

• Introduction

• Results from RHIC

• Simulation studies at LHC energies

• Summary

Andre Mischke (ERC-UU) 2

Outline

Wicks et al., Nucl. Phys. A784, 426 (2007)

Energy loss of heavy quarks

bottomcharm

Gluon radiation probability:

parton

hot and dense medium• Higher penetrating power (mQ>> Tc, QCD)

probe deeper into the medium

• Dead-cone effectgluon radiation suppressed at small angles (q < mQ/EQ)

Y. Dokshitzer, D. Kharzeev, PLB 519, 199 (2001), hep-ph/0106202

• Less energy loss Eg > ELQ > EHQ

€

ω dI

dω HEAVY

=ω

dI

dω LIGHT

1+mQ

EQ

⎛

⎝ ⎜ ⎜

⎞

⎠ ⎟ ⎟

2

1

θ 2

⎛

⎝

⎜ ⎜

⎞

⎠

⎟ ⎟

2

WWND 2011Andre Mischke (ERC-UU) 3

mc ≈ 260 mu,d

mb ≈ 3.5 mc

WWND 2011Andre Mischke (ERC-UU)

RAA of single electrons at RHIC

4

light quark hadrons

• RAA(e) ≈ RAA(h) at pT > 6 GeV/c

• Not in line with expectations from dead-cone effect

– A. Adil and I. Vitev, PLB649, 139 (2007)

Phys. Rev. Lett. 98, 192301 (2007) arXiv:1005.1627, subm. to PRCPhys. Rev. Lett. 98, 172301 (2007)

c e+ + X (BR = 9.6%)b e+ + X (BR = 10.86%)

WWND 2011

D and B contributions to single electrons

NLO pQCD: D/B meson crossing point is largely unknown

M. Cacciari et al., PRL 95, 122001 (2005)

Andre Mischke (ERC-UU) 5

– charm- - bottom

charm production

trigger side

probe side

3.83

%

54%

~

10%

K-

b

b

B-

D*0

D0

+

e

e-

B+

-

K+

D0

like-sign pairs® near-side correlation

unlike-sign pairs® away-side correlation

Identify and separate charm and bottom quark pairs using

• their decay topology

• azimuthal angular correlation of their decay products

Heavy-flavor particle correlations


–

–

–

Near- and away-side correlation peak expected for B decays

6

A.M., PLB 671, 361 (2009)

PYTHIA, pp@200 GeVlike-sign pairs

bottom dominant

charm dominant


Single electron - D0 azimuthal correlations

essentially from B decays only

75% from charm25% from beauty

STAR, Phys. Rev. Lett. 105, 202301 (2010)

7

Extraction of relative B contribution using different models:

1measured B DR R

Exploit different fragmentation of associated jets

Electron-hadron azimuthal correlations


PHENIX, Phys. Rev. Lett. 103, 082002 (2009) STAR, Phys. Rev. Lett. 105, 202301 (2010)

8

X. Lin, arXiv:hep-ph/0602067

Phys. Rev. Lett. 103, 082002 (2009) Phys. Rev. Lett. 105, 202301 (2010)

B and D contributions comparable at pT > 5 GeV/c and consistent with pQCD calculation at Fixed-Order plus Next-to-Leading Logarithm (FONLL)

WWND 2011 9Andre Mischke (ERC-UU)

B contribution to single electrons

Phys. Rev. Lett. 105, 202301 (2010)

I: M. Djordjevic et al., PLB 632, 81 (2006)II: R. Sharma et al., PRC80, 054902 (2009)III: H. van Hees et al., PRL 100, 192301 (2008)


RAA = rB RAAeB + (1-rB) RAA

eD

pT > 5 GeV/c

• B production in heavy ion collisions stronger suppressed at high pT than expected

• Original radiative energy loss calculation excluded

• Direct D and B measurements in heavy-ion collisions will come in the near future (silicon μ-vertex detector upgrades)

Comparison to energy loss models


Single electron-hadron correlations in A+A

• Away-side modification?• Improved statistics and better background rejection

needed for conclusion

PHENIX, arXiv:1011.1477, subm. to Phys. Rev. C G. Wang, Hard Probes 2010

Heavy flavor production at LHC


• Maximal collision energy: √sNN = 5.52 TeV

• Expected initial energy density: ~100 GeV/fm3 (10 times higher than at RHIC)

• Relatively long-lived QGP phase

• Thermal equilibrium reached much faster(?)

Most of the in-medium effects should be enhanced

• Higher heavy-flavor production rates

€

σ LHCcc ≈ 25 ×σ RHIC

cc

σ LHCbb ≈100 ×σ RHIC

bb

system, sNN

pp @ 14 TeVPb-Pb (0-5%) @

5.5 TeV

0.16 / 0.006 115 / 4.6QQtotN

Charm and bottom yields- NLO pQCD predictions using MNR PDF- ~factor 2 uncertainty for Pb-Pb from NLO and shadowing

Single electron RAA and correlations at LHC

T0 = 1 GeVt0 = 0.15 fm/c# quark flavours: 2

Pyquen: Pb-Pb(5%) @ 5.5 TeV

pp: PythiaPb-Pb: Pyquen

• Near side: B decays and charm from gluon splitting

• Away side: charm flavor creation

5 < pTele < 7.5 GeV/c


Light hadrons

• Electron RAA similar to results from “more sophisticated” energy loss model calculations

Single electron – D0 azimuthal correlations2 < pT

trig-ele < 4 GeV/c

• Near side: B decays and gluon splitting charm• Away side: charm flavor creation 900M events

PythiaPyquen



14

different D0 pT bins

Df(e, D0): Near-side width and IAA

2 < pTtrig-ele

< 4 GeV/c

IAA of near-side yield

• Slightly broader peak for Pyquen compared to Pythia• Suppression of D0 yield for Pyquen• Next: fragmentation function


c

cbar

g

g

flavor creation gluon splitting

g

g

g

g

c

cbar

0

Charm production: NLO processesE. Norrbin, T. Sjostrand, Eur. Phys. J. C17, 137 (2000)

Leading order- flavor creation (FC)

Next-to-leading order - gluon splitting (GS)

- flavor excitation

NLO processes become important at LHC energies

RHIC LHC


Gluon splitting contribution

GS charm + B decaysGS charm only

NLO processes become important at LHC


MC@NLOLO PYTHIA

like-sign e-K pairs3 < pT < 7 GeV/c

A. M., Phys. Lett. B671, 361 (2009)

p+p@200 GeV

RHIC LHC

Azimuthal correlations of single electrons and D0: gluon splitting contribution appears at near-side

[email protected] TeV

MC@NLO

LHC ?

Gluon splitting rate

“D* in jet” measurement

- different fragmentation characteristic

- soft charm FF for gluon jets

STAR, Phys. Rev. D79, 112006 (2009)


jet axisD*

hard (FC)soft (GS)

zz = pL(D*)/Egluon-jet

• UA1 jet reconstruction- Rcone size = 0.4

- Ethr = 10 GeV

• standard D*+ reconstruction

• lower background

“D*+ in jet” analysis

• 1.1M 7 TeV pp jet events

• Charged track jets in |η| <

0.5

• 4 jet algorithms compared

• Uncorrected spectra


A. Grelli, HQ2010

gluon splitting +flavor creation

Full PYTHIA simulation, pp@10 TeV

• Prove of principle

• Needs more statistics and efficient trigger


Δ between leading particles and D*+

20

A. Grelli, HQ2010


• Heavy quarks

- particularly good probes to study the properties of hot quark matter (especially the transport properties)

- abundantly produced at LHC energies

• Jet-like correlations of heavy-flavor particles allow to study modification of fragmentation function in the QCD medium

• NLO processes (such as gluon splitting) become important: accessible via “charm content in jets” measurements

• Many more to come!

Summary

Backup


Single electron RAA at LHC

T0 = 1 GeVt0 = 0.15 fm/c# quark flavors: 2


H. van Hees and R. Rapp, 2007

I. Vitev, A. Adil & H. van Hees, 2007Pyquen • Pythia afterburner

• Radiative (generalisation of BDMPS) and collisional energy loss (high-pT approximation)


Df(e,D0) correlations for like-sign pairs


Near-side width and yield


Near-side IAA


Jet-like correlations of heavy-flavor particles - From RHIC to LHC André Mischke Utrecht University 27 th Winter Workshop on Nuclear Dynamics Winter Park,

Documents

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b contributions

b decays

b measurements

r b r aa eb

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