Abstract

We study hard 1 → 2 final-state parton splittings in the medium, and put special emphasis on calculating the Wilson line correlators that appear in these calculations. As partons go through the medium their color continuously rotates, an effect that is encapsulated in a Wilson line along their trajectory. When calculating observables, one typically has to calculate traces of two or more medium-averaged Wilson lines. These are usually dealt with in the literature by invoking the large-Nc limit, but exact calculations have been lacking in many cases. In our work, we show how correlators of multiple Wilson lines appear, and develop a method to calculate them numerically to all orders in Nc. Initially, we focus on the trace of four Wilson lines, which we develop a differential equation for. We will then generalize this calculation to a product of an arbitrary number of Wilson lines, and show how to do the exact calculation numerically, and even analytically in the large-Nc limit. Color sub-leading corrections, that are suppressed with a factor {N}_c^{-2} relative to the leading scaling, are calculated explicitly for the four-point correlator and we discuss how to extend this method to the general case. These results are relevant for high-pT jet processes and initial stage physics at the LHC.

Highlights

  • Interpreted as a clear sign of the energy loss of jets that suffer final-state interactions with the surrounding QGP

  • We study hard 1 → 2 final-state parton splittings in the medium, and put special emphasis on calculating the Wilson line correlators that appear in these calculations

  • Color sub-leading corrections, that are suppressed with a factor Nc−2 relative to the leading scaling, are calculated explicitly for the four-point correlator and we discuss how to extend this method to the general case

Read more

Summary

Basic elements and notation

We will assume that the partons propagating through the medium are highly energetic and travelling on the light-cone almost strictly in the positive z direction. The trajectory of a particle in the medium between time t0 and t, given by the propagator (x|G(t, t0)|x0), in configuration space, for E (t − t0)−1 gets strongly constrained to the classical path connecting the initial and final transverse positions, see eq (2.1), and leads to (x|GR(t, t0)|x0) G0(x − x0, t − t0) VR(t, t0; [xcl(s)]) ,. This corresponds to the product of a Wilson line, trailing the direction of the particle, times a vacuum propagator, see eq (2.4).

Emission spectra
Derivation of the splitting functions
Nc C21
Numerical results
Calculating Wilson line correlators
Four Wilson lines
General method for Wilson line correlators
Wilson line correlators in the large-Nc limit
Conclusion and outlook
Pair production
Gluon-gluon splitting
Six lines
Quark-gluon splitting in the large-Nc
Eight Wilson lines
C Derivation of differential equation
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call