Measurements of Dielectron Production in AuAu Collisions at = 200 GeV from the STAR Experiment
Collaboration
35 pages
Published in:
- Phys.Rev.C 92 (2015) 2, 024912
- Published: Aug 24, 2015
e-Print:
- 1504.01317 [hep-ex]
Experiments:
Citations per year
Abstract: (APS)
We report on measurements of dielectron (e+e−) production in Au+Au collisions at a center-of-mass energy of 200 GeV per nucleon-nucleon pair using the STAR detector at BNL Relativistic Heavy Ion Collider. Systematic measurements of the dielectron yield as a function of transverse momentum (pT) and collision centrality show an enhancement compared to a cocktail simulation of hadronic sources in the low invariant-mass region (Mee<1GeV/c2). This enhancement cannot be reproduced by the ρ-meson vacuum spectral function. In minimum-bias collisions, in the invariant-mass range of 0.30–0.76GeV/c2, integrated over the full pT acceptance, the enhancement factor is 1.76±0.06(stat.)±0.26(sys.)±0.29(cocktail). The enhancement factor exhibits weak centrality and pT dependence in STAR's accessible kinematic regions, while the excess yield in this invariant-mass region as a function of the number of participating nucleons follows a power-law shape with a power of 1.44±0.10. Models that assume an in-medium broadening of the ρ-meson spectral function consistently describe the observed excess in these measurements. Additionally, we report on measurements of ω- and ϕ-meson production through their e+e− decay channel. These measurements show good agreement with Tsallis blast-wave model predictions, as well as, in the case of the ϕ meson, results through its K+K− decay channel. In the intermediate invariant-mass region (1.1Note:
- 40 pages, 49 figures
- 25.75.Cj
- 25.75.Dw
- heavy ion: scattering
- gold
- electron: pair production
- meson: spectral representation
- mass spectrum: (electron positron)
- model: blast wave
- enhancement
- STAR
References(87)
Figures(62)
- [1]
- [1]
- [1]
- [1]
- [2]
- [3]
- [4]
- [5]
- [6]
- [7]
- [8]
- [9]
- [10]
- [11]
- [12]
- [12]
- [12]
- [13]
- [13]
- [14]
- [15]
- [15]
- [15]
- [15]
- [16]