ar X iv : n uc l - th / 9 80 20 74 v 1 2 4 Fe b 19 98 Partial U A ( 1 ) Restoration from Bose - Einstein Correlations

ar X iv : n uc l - th / 9 80 20 31 v 1 1 0 Fe b 19 98 Ground State Correlations and Mean Field Using the exp ( S ) Method .

This document gives a detailed account of the terms used in the computation of the ground state mean field and the ground state correlations. While the general approach to this description is given in a separate paper (nucl-th/9802029) we give here the explicite expressions used. PACS: 21.60.−n, 21.60.Gx, 21.60.Cs, 21.60.Jz

ar X iv : n uc l - th / 0 40 20 37 v 1 1 2 Fe b 20 04 A hint at quark deconfinement in 200 GeV Au + Au data at RHIC

We give the emission function of the axially symmetric Buda-Lund hydro model and present its simultaneous, high quality fits to identified particle spectra, two-particle Bose-Einstein or HBT correlations and charged particle pseudorapidity distributions as measured by BRAHMS and PHENIX in 0-30 % central, √ sNN = 200 GeV Au+Au collisions at RHIC. The best fit is achieved when the most central re...

ar X iv : n uc l - th / 9 80 60 97 v 1 2 9 Ju n 19 98 3 P 2 - 3 F 2 pairing in neutron matter with modern nucleon - nucleon potentials

ar X iv : h ep - l at / 9 80 20 29 v 1 2 0 Fe b 19 98 DESY 98 - 017 February 2008 ADVANCED LATTICE

ar X iv : n uc l - th / 9 70 10 23 v 2 1 7 A pr 1 99 7 What can we learn from three - pion interferometry ?

We address the question which additional information on the source shape and dynamics can be extracted from three-particle Bose-Einstein correlations. For chaotic sources the true three-particle correlation term is shown to be sensitive to the momentum dependence of the saddle point of the source and to its asymmetries around that point. For partially coherent sources the three-pion correlator ...