1,759 research outputs found
Elliptic flow from a parton cascade
The dependence of elliptic flow at RHIC energies on the effective parton
scattering cross section is calculated using the ZPC parton cascade model. We
show that the v_2 measure of elliptic flow saturates early in the evolution
before the hadronization transition to a rather large value ~0.05-0.15 as
\sigma_g varies from 2-10 mb and thus is a sensitive probe of the dynamics in
the plasma phase.Comment: 13 pages, 4 figure
Energy loss of partons traversing a QGP fluid
We analyse the azimuthal correlation function for high p_T charged hadrons in
Au+Au collisions at the RHIC energy. By using a dynamical model in which
hydrodynamics is combined with explicit propagation of high p_T partons, we
study the effect of the intrinsic transverse momentum of initial partons on the
azimuthal back-to-back correlations.Comment: 4 pages, 2 figures, talk given at PaNic02, Osaka, Japan, September 30
- October 4, 200
Heavy Quark Radiative Energy Loss in QCD Matter
Heavy quark medium induced radiative energy loss is derived to all orders in
opacity, . The analytic expression generalizes the GLV opacity
expansion for massless quanta to heavy quarks with mass in a QCD plasma
with a gluon dispersion characterized by an asymptotic plasmon mass,
. Remarkably, we find that the general result is obtained by
simply shifting all frequencies in the GLV series by .
Numerical evaluation of the first order in opacity energy loss shows that both
charm and bottom energy losses are much closer to the incoherent radiation
limit than light partons in nuclear collisions at both RHIC and LHC energies.
However, the radiation lengths of heavy quarks remain large compared to nuclear
dimensions and hence high heavy quark production is volume rather than
surface dominated.Comment: 32 pages, 14 figure
Jet quenching in thin plasmas
We investigate the energy loss of quarks and gluons produced in hard
processes resulting from final state rescatterings in a finite quark-gluon
plasma. The angular distribution of the soft gluon bremsstrahlung induced by
n_s=1 rescatterings in the plasma is computed in the Gyulassy-Wang model.
Special focus is on how the interference between the initial hard radiation
amplitude, the multiple induced Gunion-Bertsch radiation amplitudes, and gluon
rescattering amplitudes modifies the classical parton cascade results.Comment: 4 pages in Latex and 3 EPS figures, Proceedings of the Quark
Matter'99 Conference, 10-15 May, 1999, Torin
Jet Tomography of Au+Au Reactions Including Multi-gluon Fluctuations
Jet tomography is the analysis of the attenuation pattern of high transverse
momentum hadrons to determine certain line integral transforms of the density
profile of the QCD matter produced in ultra-relativistic nuclear collisions. In
this letter, we calculate the distortion of jet tomography due to multi-gluon
fluctuations within the GLV radiative energy loss formalism. We find that
fluctuations of the average gluon number, ~ 3 for RHIC initial
conditions, reduce the attenuation of pions by approximately a factor Z ~
0.4-0.5. Therefore the plasma density inferred from jet tomography without
fluctuations must be enhanced by a factor 1/Z ~ 2.Comment: 6 pages, 4 .eps figures, uses REVTEX and bbox.st
Finding the remnants of lost jets at RHIC
A fast jet propagating through partonic matter loses energy by medium-induced
gluon radiation. We propose a method to detect the energy loss of jets and the
final-state interaction of the radiated gluons and the jets with the partonic
medium. By embedding jets and radiated energy into a parton cascade, we find
that the fate of lost jets can be studied by analyzing the momentum
distribution of soft hadrons relative to the jet axis.Comment: 5 pages, Revtex, 2 figs, Revised Version, To appear in PL
Where is the charm quark energy loss at RHIC?
Heavy quark energy loss in a hot QCD plasma is computed taking into account
the competing effects due to suppression of zeroth order gluon radiation below
the plasma frequency and the enhancement of gluon radiation due to first order
medium induced Bremsstrahlung.
The results suggest a surprising degree of cancellation between the two
medium effects for charm quarks and provides a possible explanation for the
null effect observed by PHENIX in the prompt electron spectrum in Au+Au at
130 AGeV.Comment: 9 pages with 3 ps figure
Searching for the Next Yukawa Phase of QCD
QCD predicts that the interactions between quarks and gluons change from a
confining to a screened Yukawa form above a critical temperature
MeV. In this talk, I review some of the key observables in heavy ion reactions
which are being used to search for this new partonic Yukawa phase at SPS and
RHIC. These include collective observables such as ,
meson interferometry, jet quenching, and suppression.Comment: 24 pages (PTPTex style files included) with 26 eps,ps figures using
epsf,psfig. To appear in Proc. of 14th Nishinomiya-Yukawa Memorial Symposium
Nov. 1999, Japan; updated with a critique of the CERN press release Feb. 8,
200
The Next Yukawa Phase of QCD at RHIC
QCD predicts the existence of a new partonic Yukawa phase above a critical
temperature MeV. I review some of the key observables which will
be used in heavy ion reactions to search for this new phase at RHIC.
Systematics of collective observables (, flow patterns, meson
interferometry, jet quenching, and suppression are discussed. This
talk is updated with the first data from RHIC.Comment: 18 pages, including 18 figures. Invited talk given at the 7th
International Conference on Nucleus-Nucleus Collisions (NN2000), Strasbourg,
3-7 July 2000, to appear in the Proceedings in Nucl. Phys. A (W. Noerenberg,
D. Guerreau, and V. Metag, editors
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