Tachibana, Yuki; Sirimanna, Chamod; Majumder, Abhijit; Angerami, Aaron; Arora, Raghav; Bass, Steffen A.; Chen, Yang; Datta, Raktim; Du, Lijuan; Ehlers, Raymond; Elfner, Hannah; Fries, Rainer J.; Gale, Charles; He, Yuxin; Jacak, Barbara V.; Jacobs, Peter M.; Jeon, Sangyong; Ji, Yifan; Jonas, Fabian; Kasper, Lukas; Kordell, Michael; Kumar, Ashish; Kunnawalkam-Elayavalli, Rajeev; Latessa, Joseph; Lee, Yen-Jie; Lemmon, Richard; Luzum, Matthew; Mak, Simon; Mankolli, Abhishek; Martin, Clint; Mehryar, Hamidreza; Mengel, Tobias; Nattrass, Christine; Norman, Jennifer; Parker, Christine; Paquet, Jean-Fran癟ois; Putschke, J繹rg H.; Roch, Henri; Roland, Gunther; Schenke, Bj繹rn; Schwiebert, Lyle; Sengupta, Abhijit; Shen, Chun; Singh, Manpreet; Soeder, Daniel; Soltz, Ron A.; Soudi, Iman; Velkovska, Julia; Vujanovic, Gojko; Wang, Xin-Nian; Wu, Xiaojian; Zhao, Wei (2026).泭.泭Physical Review C, 113(3), 034910.泭
This study looks at how high-energy particle jets (narrow sprays of particles produced in collisions) are altered when they pass through the extremely hot, dense medium created in heavy-ion collisionsspecifically leadlead (PbPb) collisions at very high energy. The researchers use detailed computer simulations (Monte Carlo methods, which rely on repeated random sampling) to model how these jets evolve as they travel through this medium. They focus on differences between two types of jets: quark jets and gluon jets (quarks and gluons are the fundamental particles that make up protons and neutrons, and they produce jets with slightly different properties). By studying specific features of the jets internal structuresuch as the angle between its main branches (called the soft drop prong angle, (r_g)), how momentum is shared between those branches ((k_{T,g})), and the jets effective mass after removing softer components ((m_g))they find that quark jets change in a more complex, non-linear way compared to gluon jets when interacting with the medium.
An especially useful case involves gamma-tagged jets, where a high-energy photon (帠) is produced alongside the jet. Because these events are more likely to involve quark jets, they provide a cleaner way to isolate how the medium affects jet structure. Interestingly, the modifications seen in these gamma-tagged jets stand out clearly and are not just due to biases in how the jets are selected for study. The results suggest that much of the observed change comes from the mediums response to the jetessentially how the surrounding particles recoil and interact after being disturbed by the jet. Overall, the study shows that examining the fine details of jet structure, especially in gamma-tagged events, can be a powerful way to better understand how jets interact with and are modified by the dense medium created in high-energy nuclear collisions.

Fig 1: Distributions of jet splitting momentum fraction泭攻泭normalized by the number of all triggered jets (upper panel) and the number of jets passing the soft-drop condition (lower panel) for the leading jets in events generated with泭pgun. The jet shower evolution is performed by vacuum泭matter泭for the parent parton having泭init=140泭GeV. Jets are reconstructed with泭=0.4泭at midrapidity泭| | |jet|<2.0. The results are shown for quark jets (solid) and gluon jets (dashed) with different泭jet泭triggers, 112, 84, 56, and 28 GeV. The soft-drop parameters are泭cut=0.2泭and泭=0.