We report on a recent next-to-leading order perturbative determination of the dilepton rate from a hot QCD plasma for frequency and momentum of the order of the temperature and for much smaller invariant mass M∼gT. We briefly review the calculation, which generalizes the previous one for the photon case (M=0). We then analyze the consequences of the new calculation for the extraction of the photon rate from the small mass dilepton measurements. We then review a recent NLO determination at large M and we show how to match and merge its results with the low-mass ones, resulting in a single rate which is NLO-accurate over the phenomenologically relevant region
The thermal QCD dilepton production rate is calculated at next-to-leading order in the strong coupli...
International audienceDileptons produced during heavy-ion collisions represent a unique probe of the...
We study the invariant-mass distributions of dileptons produced in ultrarelativistic heavy-ion colli...
The vector channel spectral function and the dilepton production rate from a QCD plasma at a tempera...
Next-to-leading order analyses of the dilepton production rate from a hot QCD plasma are reviewed. I...
We present a computation, within weakly-coupled thermal QCD, of the production rate of low invariant...
International audienceThe thermal QCD dilepton production rate is calculated at next-to-leading orde...
19 pages, 7 postscript figures, test program available at http://www-spht.cea.fr/articles/T02/150/li...
19 pages, 7 postscript figures, test program available at http://www-spht.cea.fr/articles/T02/150/li...
19 pages, 7 postscript figures, test program available at http://www-spht.cea.fr/articles/T02/150/li...
In this talk, I review new developments of QCD calculations of photon and dilepton production rates ...
Strict next-to-leading order (NLO) results for the dilepton production rate from a QCD plasma at tem...
We consider the thermal emission rate of dileptons from a QCD plasma in the small invariant mass ($Q...
Karsch F, Laermann E, Petreczky P, Stickan S, Wetzorke I. A lattice calculation of thermal dilepton ...
Using clover improved Wilson fermions we calculate thermal vector meson correlation functions above ...
The thermal QCD dilepton production rate is calculated at next-to-leading order in the strong coupli...
International audienceDileptons produced during heavy-ion collisions represent a unique probe of the...
We study the invariant-mass distributions of dileptons produced in ultrarelativistic heavy-ion colli...
The vector channel spectral function and the dilepton production rate from a QCD plasma at a tempera...
Next-to-leading order analyses of the dilepton production rate from a hot QCD plasma are reviewed. I...
We present a computation, within weakly-coupled thermal QCD, of the production rate of low invariant...
International audienceThe thermal QCD dilepton production rate is calculated at next-to-leading orde...
19 pages, 7 postscript figures, test program available at http://www-spht.cea.fr/articles/T02/150/li...
19 pages, 7 postscript figures, test program available at http://www-spht.cea.fr/articles/T02/150/li...
19 pages, 7 postscript figures, test program available at http://www-spht.cea.fr/articles/T02/150/li...
In this talk, I review new developments of QCD calculations of photon and dilepton production rates ...
Strict next-to-leading order (NLO) results for the dilepton production rate from a QCD plasma at tem...
We consider the thermal emission rate of dileptons from a QCD plasma in the small invariant mass ($Q...
Karsch F, Laermann E, Petreczky P, Stickan S, Wetzorke I. A lattice calculation of thermal dilepton ...
Using clover improved Wilson fermions we calculate thermal vector meson correlation functions above ...
The thermal QCD dilepton production rate is calculated at next-to-leading order in the strong coupli...
International audienceDileptons produced during heavy-ion collisions represent a unique probe of the...
We study the invariant-mass distributions of dileptons produced in ultrarelativistic heavy-ion colli...