2013/12/31 by STAR Collaboration, J. K. Adkins, L. Adamczyk +384 · 6 citations
Physics and Astronomy · #Collision #Hadron #High-Energy Particle Collisions Research #Invariant mass #Mass spectrum #Particle Detector Development and Performance #Particle physics theoretical and experimental studies #Proton #Spectral function #Spectral line #Yield (engineering) #hep-ex #nucl-ex
paper · pdf · doi:10.1103/physrevlett.113.022301
published as Phys. Rev. Lett. 113, 022301 (2014)
openalex publication_date 2014/07/09 · arxiv created 2014/07/15 · arxiv updated 2014/07/16 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
We report the STAR measurements of dielectron (e+e^\ensuremath-) production at midrapidity (|yee|<1) in Au+Au collisions at √sNN=200 GeV. The measurements are evaluated in different invariant mass regions with a focus on 0.30--0.76 (\ensuremathρ-like), 0.76--0.80 (\ensuremathω-like), and 0.98--1.05 (\ensuremathφ-like) GeV/c2. The spectrum in the \ensuremathω-like and \ensuremathφ-like regions can be well described by the hadronic cocktail simulation. In the \ensuremathρ-like region, however, the vacuum \ensuremathρ spectral function cannot describe the shape of the dielectron excess. In this range, an enhancement of 1.77\ifmmode±\else\textpm\fi0.11(stat)\ifmmode±\else\textpm\fi0.24(syst)\ifmmode±\else\textpm\fi0.33(cocktail) is determined with respect to the hadronic cocktail simulation that excludes the \ensuremathρ meson. The excess yield in the \ensuremathρ-like region increases with the number of collision participants faster than the \ensuremathω and \ensuremathφ yields. Theoretical models with broadened \ensuremathρ contributions through interactions with constituents in the hot QCD medium provide a consistent description of the dilepton mass spectra for the measurement presented here and the earlier data at the Super Proton Synchrotron energies.