Gluon splitting into charm-anti-charm pair inside a jet
In ultra-relativistic heavy-ion collisions, the quark-gluon plasma (QGP) significantly alters the behavior of quarks and gluons. Using the Baier-Dokshitzer-Mueller-Peigné-Schiff and Zakharov (BDMPS-Z) formalism, we explored how the QGP modifies gluon splitting into quark-antiquark pairs, with a focus on charm quarks. Our study introduces a compact framework to account for repeated interactions between the splitting particles and the medium (Attems et al., 2023; Attems et al., 2024). Two key effects emerge:
Momentum Broadening – The quark-antiquark pairs gain relative momentum from the medium, increasing their invariant mass.
Enhanced Production – The medium boosts the production of such pairs, especially when the momentum transfer is comparable to the quark mass.
These effects are particularly significant for charm quarks in heavy-ion collisions, as seen in ccbar production. Interestingly, the same QCD formalism that explains jet suppression also predicts enhanced production of cbar pairs in jets, a phenomenon measurable through D⁰-tagged jets. This work highlights how the QGP modifies fundamental processes in QCD, offering a new avenue for probing the medium’s properties.
@article{Attems:2022otp,author={Attems, Maximilian and Brewer, Jasmine and Innocenti, Gian Michele and Mazeliauskas, Aleksas and Park, Sohyun and van der Schee, Wilke and Soyez, Gregory and Wiedemann, Urs Achim},title={{Medium-Enhanced $c\bar{c}$ Radiation}},archiveprefix={arXiv},primaryclass={hep-ph},reportnumber={CERN-TH-2022-046},doi={10.1103/PhysRevLett.132.212301},journal={Phys. Rev. Lett.},volume={132},number={21},pages={212301},year={2024}}
@article{Attems:2022ubu,author={Attems, Maximilian and Brewer, Jasmine and Innocenti, Gian Michele and Mazeliauskas, Aleksas and Park, Sohyun and van der Schee, Wilke and Wiedemann, Urs Achim},title={{The medium-modified $ g\to c\overline{c} $ splitting function in the BDMPS-Z formalism}},archiveprefix={arXiv},primaryclass={hep-ph},reportnumber={CERN-TH-2022-045},doi={10.1007/JHEP01(2023)080},journal={JHEP},volume={01},pages={080},year={2023}}