Abstract
Abstract We present a conceptually new framework for describing jet evolution in the dense medium produced in ultra-relativistic nucleus-nucleus collisions using perturbative QCD and its implementation into the Monte Carlo event generator Jewel. The rescattering of hard partons in the medium is modelled by infrared continued pQCD matrix elements supplemented with parton showers. The latter approximate higher order real-emission matrix elements and thus generate medium-induced gluon emissions. The interplay between different emissions is governed by their formation times. The destructive interference between subsequent scattering processes, the non-Abelian version of the Landau-Pomeranchuk-Migdal effect, is also taken into account. In this way the complete radiation pattern is consistently treated in a uniform way. Results obtained within this minimal and theoretically well constrained framework are compared with a variety of experimental data susceptible to jet-quenching effects at both RHIC and the LHC. Overall, a good agreement between data and simulation is found. This new framework also allows to identify and quantify the dominant uncertainties in the simulation, and we show some relevant examples for this.
Highlights
Transverse size of the dense QCD matter produced in the spatially extended overlap region of ultra-relativistic nucleus-nucleus collisions
We present a conceptually new framework for describing jet evolution in the dense medium produced in ultra-relativistic nucleus-nucleus collisions using perturbative QCD and its implementation into the Monte Carlo event generator Jewel
It can be expected that the QCD parton showers introduced and studied in the vacuum will be subjected to medium modifications in nucleus-nucleus collisions
Summary
The ingredients necessary to construct an in-medium parton shower following the paradigms outlined above will be discussed. The rescattering of a hard parton in the medium is discussed, and in section 2.3 the probabilistic interpretation of the LPM-effect in the eikonal limit is recapitulated.
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