The LPM effect in sequential bremsstrahlung: 1/ N c 2 $$ {\mathrm{N}}_{\mathrm{c}}^2 $$ corrections

Abstract

Abstract An important question concerning in-medium high-energy parton showers in a quark-gluon plasma or other QCD medium is whether consecutive splittings of the partons in a given shower can be treated as quantum mechanically independent, or whether the formation times for two consecutive splittings instead have significant overlap. Various previous calculations of the effect of overlapping formation times have either (i) restricted attention to a soft bremsstrahlung limit, or else (ii) used the large-N c limit (where N c = 3 is the number of quark colors). In this paper, we make a first study of the accuracy of the large-N c limit used by those calculations of overlap effects that avoid a soft bremsstrahlung approximation. Specifically, we calculate the 1/ N c 2 $$ {N}_{\mathrm{c}}^2 $$ correction to previous N c = ∞ results for overlap g → gg → ggg of two consecutive gluon splittings g → gg. At order 1/ N c 2 $$ {N}_{\mathrm{c}}^2 $$ , there is interesting and non-trivial color dynamics that must be accounted for during the overlap of the formation times.

Keywords

• Finite Temperature or Finite Density
• Quark-Gluon Plasma