Dileptons from the nonequilibrium Quark-Gluon Plasma

TL;DR

This paper models dilepton production from a nonequilibrium quark-gluon plasma using off-shell cross sections derived from the dynamical quasiparticle model, and compares results with experimental data.

Contribution

It introduces off-shell cross sections for dilepton production processes in the sQGP based on the DQPM and implements them into the PHSD transport approach for heavy-ion collision simulations.

Findings

The model reproduces low-mass dilepton spectra with vector meson broadening.

Intermediate mass spectra are dominated by off-shell q-qbar annihilation and Bremsstrahlung.

The softening of the m_T spectra at intermediate masses is approximately reproduced.

Abstract

According to the dynamical quasiparticle model (DQPM) -- matched to reproduce lattice QCD results in thermodynamic limit, -- the constituents of the strongly interacting quark-gluon plasma (sQGP) are massive and off-shell quasi-particles (quarks and gluons) with broad spectral functions. In order to address the electromagnetic radiation of the sQGP, we derive off-shell cross sections of $q\bar q\to\gamma^*$, $q\bar q\to\gamma^*+g$ and $qg\to\gamma^*q$($\bar q g\to\gamma^* \bar q$) reactions taking into account the effective propagators for quarks and gluons from the DQPM. Dilepton production in In+In collisions at 158 AGeV is studied by implementing these processes into the parton-hadron-string dynamics (PHSD) transport approach. The microscopic PHSD transport approach describes the full evolution of the heavy-ion collision: from the dynamics of quasi-particles in the sQGP phase (when the local energy density is above $\sim 1$ GeV/fm$^3$) through hadronization and to the following hadron interactions and off-shell propagation after the hadronization. A comparison to the data of the NA60 Collaboration shows that the low mass dilepton spectra are well described by including a collisional broadening of vector mesons, while the spectra in the intermediate mass range are dominated by off-shell quark-antiquark annihilation, quark Bremsstrahlung and gluon-Compton scattering in the nonperturbative QGP. In particular, the observed softening of the $m_T$ spectra at intermediate masses (1 GeV $\le M \le$ 3 GeV) is approximately reproduced.