jet quenching of massive quark in nuclear medium

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Jet Quenching of Massive Quark in Nuclear Medium. Ben-Wei Zhang Institute of Particle Physics Central China Normal Univeristy ICHEP, Beijing --- Augest 16, 2004. Thanks to my collaborators: Xin-Nian Wang and Enke Wang. Outline. Motivation Modified heavy quark fragmentation function - PowerPoint PPT Presentation

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Jet Quenching of Massive Quark in Nuclear Medium

Ben-Wei ZhangInstitute of Particle Physics

Central China Normal Univeristy

ICHEP, Beijing --- Augest 16, 2004

Thanks to my collaborators: Xin-Nian Wang and Enke Wang

2--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Outline

• Motivation

• Modified heavy quark fragmentation function

• Heavy quark energy loss

------ Heavy VS. Light

• Conclusion

3--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Jet QuenchingJet Quenching

Jet quenching has been discovered at RHIC as a good probe of the hot/dense matter.

hadrons

ph

parton

E

X.N. Wang, nucl-th/0405017

4--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

From Light to Heavy

Theory:• A lot of theoretical studies have been devoted to the

calculations of the energy loss of a light quark.

• For massive quarks, the formalism of medium-induced gluon radiation is not developed to the same extent.

Experiment:• Open charm suppression, which can now be measured at

RHIC by comparing pt distributions of D-mesons in D-Au and Au-Au collisions, is a novel probe of QGP dynamics.

5--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Heavy Quark Energy Loss

• There are several theoretical calculations to obtain the heavy quark energy loss:

Yu.L. Dokshitzer and D.E. Kharzeev M. Djordjevic and M. Gyulassy B.W.Zhang, E. Wang and X.N. Wang N. Armesto, C. Salgado and U. Wiedemann

……• Twist Expansion approach in pQCD

B.W. Zhang, E. Wang and X.N. Wang, PRL 93(2004) 072301

6--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Jet quenching with pQCD

• How to measure the parton energy loss?

• Direct measurement is impossible

• Particle distributions within a jet

• Modification to Fragmentation Function

• Obtain the energy loss indirectly from measuring the modification of FF

hadrons

ph

parton

E

7--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Heavy QuarkHeavy Quark

In eA DIS, for the heavy quark production we obtain :In eA DIS, for the heavy quark production we obtain :

8--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Multiple Scattering in NucleiMultiple Scattering in Nuclei

In order to calculate the heavy quark energy loss induced by gluon radiation in pQCD, we should separate the ‘hard’ part from the ‘soft’ part:

factorizing.

9--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Generalized Factorization

Luo, Qiu, Sterman, PLB 279(1992)377;Luo, Qiu, Sterman, PRD 49(1994)4493; PRD 50(1994)1951

10--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Tensor Structure

• Making a collinear approximation:

• The tensor structure can be factorized as:

11--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

LPM Effect

LMP interference effect.

The formation time of gluon radiation.

12--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Other ProcessesOther Processes

13--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Dead-Cone Effect

Dead-cone effect of heavy quark propagating will suppress gluon radiation at small angles.

14--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Modified FF of Heavy Quark With the generalized factorization theorem we With the generalized factorization theorem we

obtain the semi- inclusive hadronic tensor:obtain the semi- inclusive hadronic tensor:

The modified effective fragmentation function is

15--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Two-parton Correlation FunctionTwist-4 parton correlation function is in principle not calculable.

With some approximations we can estimate the twist-4 correlation functions approximated as

J. Osborne and Xin-Nian Wang, NPA 710(2002)281

16--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Heavy Quark Energy Loss

Heavy quark energy loss can be derived as:

Xiao-fen Guo, Xin-Nian Wang, PRL 85(2000)3591;

Xin-Nian Wang, Xiao-fen Guo, NPA 696(2001) 788

Ben-Wei Zhang, Xin-Nian Wang, NPA 720(2003) 429

When M=0, we will recover the result of the light quark energy loss.

17--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Two Distinct Limits

(1) When

2QQ^2

(2) For large values of Q(2) For large values of Q2 2 or small xor small xBB, we have, we have

18--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Nuclear Size Dependence

19--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Heavy Quark VS. Light Quark

Energy loss of heavy quark is significantly suppressed due to mass effect, in particular, the dead-cone effect.

20--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Conclusion• Heavy quark energy loss induced by gluon radiation is

derived in terms of Modified FF with pQCD.

• Two mass effects:

(I) Gluon formation time of the heavy quark is reduced relative to that of a light quark:

Medium size dependence of heavy quark enegy loss is found to change from a linear to a quadratic form when the initial energy and momentum scale are increasing.

(II) Dead-cone effect: Heavy quark energy loss is significantly suppressed

relative to a light quark.

21--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Thank you very much!

谢谢 !

Thank you very much!

谢谢 !

22--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Twist-4 Parton Correlation

23--------------------------------------------Ben-Wei Zhang, ICHEP’04, Beijing

Factorization of Twist-4 Matries

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