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Effect of parton cascade to the medium. Hanlin Li IOPP, CCNU, Wuhan Fuming Liu IOPP, CCNU, Wuhan Xin-Nian Wang LBNL, USA Yan Zhu IOPP, CCNU, Wuhan. QNP, Beijing , September 21 - 26, 2009. OUTLINE. Introduction Preliminary results Elastic energy loss - PowerPoint PPT Presentation
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Effect of parton cascade to the medium
Hanlin LiIOPP, CCNU, Wuhan
Fuming LiuIOPP, CCNU, Wuhan
Xin-Nian WangLBNL, USA
Yan Zhu IOPP, CCNU, Wuhan
QNP, Beijing , September 21 - 26, 2009
2/14
OUTLINE Introduction
Preliminary results Elastic energy loss Medium modification caused by jet
propagating
Conclusions and Outlook
3/14
Introduction — jet quenching Jet quenching is a good probe of sQGP.
Suppression of High PT hadrons. It’s also important to study the modification of medium d
ue to jet propagation. Azimuthal angle correlation caused by jet medium int
eraction.
Several models: Putting a source current in hydrodynamic (Chaudhuri
and Heinz,2006); Markovian parton scattering (MPS) model (Charles B.
Chiu and Rudolph C. Hwa,2006). ……
4/14
By now only elastic collisions are considered.
where and
Our approach — Parton cascade simulation based on Boltzmann Eq.
5/14
Elastic collision rate:
Energy distribution of thermal parton:
Interaction amplitude:
Interval between successive collisions :
More useful formulae
Gyulassy and Wang,Nucl.Phys.B420,583
6/14
Test our MC with numerical integration
Set jet moving along z-axis
Energy distribution of produce partons from single scattering
for different energy of jet E1.
Angle (theta=ATAN(pz/E) ) distribution of produce partons from single scattering
for different energy of produce particle.
E1=20GeV
7/14
Elastic energy loss for qq collision
w/o. s.a.a.2 2
2
2| |
( )
s uM
t q
$
w. s.a.a.2
2
2 2
2| |
( )
sM
q q
$
Theory (X.N. Wang,Phys.Rept.280:287-371.)
8/14
Modification of medium by propagating jett=2fm/c
Jet moves along z-axis.
r=sqrt(x2+y2)
9/14
Modification of medium by propagating jett=4fm/c
10/14
Modification of medium by propagating jett=8fm/c
11/14
Azimuthal angle distribution —single scattering
Jet moves along z-axis.
Ф=ACOS(pz/sqrt(pz2+px2))
Double-peak appears in single scattering.
Azimuthal angle distribution is energy dependence.
pro.
Double-peak appears in single scattering.
Azimuthal angle distribution is energy dependence.
12/14
Azimuthal angle distribution — multiple scattering
Double-peak at the early time as single scattering
Uniform distribution after enough time.
Double-peak disappears due to the interaction of associate partons.
t
=1
5fm
/c t
=4
fm/c
t=1
fm/c
13/14
Conclusions and Outlook A parton cascade simulation has been construc
ed based on Boltzmann eq.. Elastic energy loss has been investigated. Strict
calculation shows a lower energy loss than that in previous work.
Cone structure of produced parton can be formed when jets propagate in the medium.
The azimuthal angle distribution of produced partons depends strongly on their energy and the medium size.
More realistic medium will be used. Inelastic collision(2 3) will be included.
14
ThanksThanks
for your attention!for your attention!
15
Azimuthal angle correlation —single scattering
Jet move along z-axis.
Ө=ATAN(pz/E)
Azimuthal correlation is energy dependence.
16
Multiple scattering exclude scattering among thermal partons