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Are in-medium quark-gluon showers strongly coupled? Results in the large-$N_f$ limit

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arxiv 2408.07129 v2 pith:UQC6PKPQ submitted 2024-08-13 hep-ph nucl-th

classification hep-phnucl-th
keywords showerslarge-effecteffectsgluoniclimitmediumoverlap
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

Inside a medium, showers originating from a very high energy particle develop via medium-induced splitting processes such as bremsstrahlung and pair production. During shower development, two consecutive splittings sometimes overlap quantum mechanically, so that they cannot be treated independently. Some of these effects can be absorbed into an effective value of a medium parameter known as $\hat q$. Previous calculations (with certain simplifying assumptions) have found that, after adjusting the value of $\hat q$, the leftover effect of overlapping splittings is quite small for purely gluonic large-$N_c$ showers but is very much larger for large-$N_f$ QED showers, at comparable values of $N\alpha$. Here, by investigating the same problem for QCD with *quarks* in the large-$N_f$ limit of many quark flavors, we make a first study of whether the small effect in purely gluonic showers (i) was merely an accident or (ii) is more broadly characteristic of such overlap effects in QCD. We also offer a qualitative explanation for the large size of the effect in QED vs. QCD.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Revisiting extremely high energy QED bremsstrahlung in matter: large modifications to the LPM effect

    hep-ph 2025-08 conditional novelty 7.0 of 10

    Pair production overlapping soft bremsstrahlung enhances the in-medium radiation rate above the standard LPM value, opposite to the 1964 prediction of Galitsky and Gurevich.

  2. Gluon radiation from a QCD antenna with realistic parton-medium interactions

    hep-ph 2026-07 unverdicted novelty 6.0 of 10

    The in-medium antenna gluon spectrum is obtained by numerical solution of Dyson-type equations that fully resum multiple scatterings for Yukawa and HTL rates, without harmonic-oscillator or opacity truncations.

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