oalib

Publish in OALib Journal

ISSN: 2333-9721

APC: Only $99

Submit

Any time

2019 ( 403 )

2018 ( 704 )

2017 ( 696 )

2016 ( 968 )

Custom range...

Search Results: 1 - 10 of 401182 matches for " Asakawa M "
All listed articles are free for downloading (OA Articles)
Page 1 /401182
Display every page Item
Comment on: "Transverse-Mass $M_\perp$ Dependence of Dilepton Emission from Preequilibrium and Quark-Gluon Plasma in High Energy Nucleus-Nucleus Collisions"
M. Asakawa
Physics , 1994, DOI: 10.1103/PhysRevLett.74.1486
Abstract: In a recent Letter, Geiger presents calculations of the dilepton emission from the early stage of ultrarelativistic heavy ion collisions using the parton cascade model (PCM). He shows that the $M_\perp$ scaling is not observed. In this Comment, we point out that this is largely due to a defect in the PCM.
What Thermodynamics tells about QCD Plasma near Phase Transition
M. Asakawa,T. Hatsuda
Physics , 1995, DOI: 10.1103/PhysRevD.55.4488
Abstract: Due to a rapid change of the entropy density $s(T)$ across the critical temperature $T_c$ of the QCD phase transition, the pressure $P(T)$ and the energy density $e(T)$ above $T_c$ generally deviate from their Stefan-Boltzmann values. We shall demonstrate this both analytically and numerically for a general class of $s(T)$ consistent with thermodynamical constraints and make a qualitative comparison of the result with the lattice QCD data. Quantities related to $ds(T)/dT$ such as the specific heat and sound velocity are also discussed.
Charmonia above the Deconfinement Phase Transition
M. Asakawa,T. Hatsuda
Physics , 2003, DOI: 10.1016/S0920-5632(03)02649-5
Abstract: Analyzing correlation functions of charmonia at finite temperature ($T$) on $32^3\times(32-96)$ anisotropic lattices by the maximum entropy method (MEM), we find that $J/\psi$ and $\eta_c$ survive as distinct resonances in the plasma even up to $T \simeq 1.6 T_c$ and that they eventually dissociate between $1.6 T_c$ and $1.9 T_c$ ($T_c$ is the critical temperature of deconfinement). This suggests that the deconfined plasma is non-perturbative enough to hold heavy-quark bound states. The importance of having sufficient number of temporal data points in the MEM analysis is also emphasized.
$J/ψ$ and $η_c$ in the Deconfined Plasma from Lattice QCD
M. Asakawa,T. Hatsuda
Physics , 2003, DOI: 10.1103/PhysRevLett.92.012001
Abstract: Analyzing correlation functions of charmonia at finite temperature ($T$) on $32^3\times(32-96)$ anisotropic lattices by the maximum entropy method (MEM), we find that $J/\psi$ and $\eta_c$ survive as distinct resonances in the plasma even up to $T \simeq 1.6 T_c$ and that they eventually dissociate between $1.6 T_c$ and $1.9 T_c$ ($T_c$ is the critical temperature of deconfinement). This suggests that the deconfined plasma is non-perturbative enough to hold heavy-quark bound states. The importance of having sufficient number of temporal data points in MEM analyses is also emphasized.
Strangeness Correlation: A Clue to Hadron Modification in Dense Matter?
M. Asakawa,T. Csorgo
Physics , 1996,
Abstract: We discuss the possibility to observe hadron modification in hot matter via the correlation of identical particles. We find that the hadron modification causes a new type of correlation, back-to-back correlation.
Two-mode squeezed states in high energy physics
M. Asakawa,T. Csorgo
Physics , 1997,
Abstract: We discuss the possibility to observe hadron modification in hot and dense matter via the correlation of identical particles. We find that a modification of hadronic masses in medium leads to two-mode squeezing which signals itself in a back-to-back correlations of hadrons. This effect leads to a signal of a shift of $\phi$-meson mass.
Critical End Point and Its Consequences
M. Asakawa,C. Nonaka
Physics , 2005, DOI: 10.1016/j.nuclphysa.2006.06.130
Abstract: Recently a lot of evidence that there exists a critical end point (CEP) in the QCD phase diagram has been accumulating. However, so far, no reliable equation of state with the CEP has been employed in hydrodynamical calculations. In this article, we construct the equations of state with the CEP on the basis of the universality hypothesis and show that the CEP acts as an attractor of isentropic trajectories. We also consider the time evolution in the case with the CEP and discuss how the CEP affects the final state observables.
Secondary phi meson peak as an indicator of QCD phase transition in ultrarelativistic heavy ion collisions
M. Asakawa,C. M. Ko
Physics , 1994, DOI: 10.1103/PhysRevC.50.3064
Abstract: In a previous paper, we have shown that a double phi peak structure appears in the dilepton invariant mass spectrum if a first order QCD phase transition occurs in ultrarelativistic heavy ion collisions. Furthermore, the transition temperature can be determined from the transverse momentum distribution of the low mass phi peak. In this work, we extend the study to the case that a smooth crossover occurs in the quark-gluon plasma to the hadronic matter transition. We find that the double phi peak structure still exists in the dilepton spectrum and thus remains a viable signal for the formation of the quark-gluon plasma in ultrarelativistic heavy ion collisions.
Seeing the QCD phase transition with phi mesons
M. Asakawa,C. M. Ko
Physics , 1994, DOI: 10.1016/0370-2693(94)90487-1
Abstract: A double phi peak structure in the dilepton invariant mass spectrum from ultrarelativistic heavy ion collisions is proposed as a signal for the phase transition from the quark-gluon plasma to the hadronic matter. The low mass phi peak results from the decay of phi mesons with reduced in-medium mass during the transition. Furthermore, the measurement of the transverse momentum distribution of these low mass phi mesons offers a viable means for determining the temperature of the phase transition.
Squeezed Correlations and Spectra for Mass-Shifted Bosons
M. Asakawa,T. Csorgo,M. Gyulassy
Physics , 1998, DOI: 10.1103/PhysRevLett.83.4013
Abstract: Huge back-to-back correlations are shown to arise for thermal ensembles of bosonic states with medium-modified masses. The effect is experimentally observable in high energy heavy ion collisions.
Page 1 /401182
Display every page Item


Home
Copyright © 2008-2017 Open Access Library. All rights reserved.