{"total":12,"items":[{"citing_arxiv_id":"2606.00973","ref_index":13,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Measurements of jet quenching with semi-inclusive hadron-jet correlations in Ru+Ru and Zr+Zr collisions at $\\sqrt{s_\\mathrm{NN}}=200$ GeV","primary_cat":"nucl-ex","submitted_at":"2026-05-31T03:09:01+00:00","verdict":"CONDITIONAL","verdict_confidence":"MODERATE","novelty_score":6.0,"formal_verification":"none","one_line_summary":"First semi-inclusive hadron-jet measurement in Ru+Ru and Zr+Zr at 200 GeV finds recoil-jet suppression and intra-jet broadening in central relative to peripheral collisions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.30816","ref_index":54,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Functional renormalization group study of the jet quenching parameter near the QCD critical end point","primary_cat":"hep-ph","submitted_at":"2026-05-29T04:08:11+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"fRG calculations show the jet quenching parameter hat q is enhanced above the chiral boundary and peaks near the QCD critical end point due to critical sigma fluctuations.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.12791","ref_index":36,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Jet Momentum Broadening in Viscous QCD Matter: A Moment Expansion Approach","primary_cat":"hep-ph","submitted_at":"2026-05-12T22:09:38+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"The jet broadening tensor qhat^ij in near-equilibrium QCD is controlled by the medium shear-stress tensor within the 14-moment approximation.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"rameter ˆq. For thermally equilibrated plasmas, this quan- tity has been computed in a wide range of theoretical frameworks, including weakly coupled QCD [3, 17-27], holographic approaches [28-31], and other methods [32- 35]. Phenomenological estimates of the jet-quenching pa- rameter from model-to-data comparisons have also been carried out by the JET [36, 37] and JETSCAPE [38] col- laborations. More generally, jet momentum broadening can be described by a tensor ˆqij [19, 25, 26, 39, 40], which measures the rate at which momentum fluctuations are accumulated along the jet trajectory. In an isotropic and homogeneous equilibrated plasma, rotational symmetry reduces the spatial momentum- broadening tensor to two scalar functions, a transverse"},{"citing_arxiv_id":"2605.04393","ref_index":48,"ref_count":2,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Medium Characterization with Hard Probes: From Cherenkov Light in QED to Jet Drift in QCD","primary_cat":"nucl-th","submitted_at":"2026-05-06T01:32:26+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"The work presents a dispersive fit for the refractive index of liquid argon incorporating anomalous dispersion and proposes jet drift in simulations of heavy-ion collisions as a way to disentangle medium properties from energy loss.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"a probe of the initial stages in heavy-ion collisions\", Phys. Lett. B803, 135318 (2020), arXiv:1902.03231. [46] CMS Collaboration, A. Hayrapetyan et al.,\"Overview of high-density QCD studies with the CMS experiment at the LHC\",arXiv:2405.10785. [47] I. Vitev & M. Gyulassy,\"Highp T tomography ofd+ Au and Au+Au at SPS, RHIC, and LHC\", Phys. Rev. Lett.89, 252301 (2002),hep-ph/0209161. [48] JET Collaboration, K. M. Burke et al.,\"Extracting the jet transport coefficient from jet quenching in high-energy heavy-ion collisions\", Phys. Rev. C90, 014909 (2014), arXiv:1312.5003. [49] S. Cao & X.-N. Wang,\"Jet quenching and medium response in high-energy heavy-ion collisions: a review\", Rept. Prog. Phys.84, 024301 (2021),arXiv:2002.04028. [50] CMS Collaboration, S."},{"citing_arxiv_id":"2604.19288","ref_index":18,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Geometric Bias and Centrality Dependence of Jet Quenching in High-Energy Nuclear Collisions","primary_cat":"nucl-th","submitted_at":"2026-04-21T09:53:54+00:00","verdict":"CONDITIONAL","verdict_confidence":"MODERATE","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Suppression of high-pT hadrons in peripheral Pb+Pb collisions is predominantly driven by initial-state geometric bias rather than final-state jet quenching.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.15737","ref_index":18,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Bayesian inference constraints on jet quenching across centrality, beam energy, and observable classes in LHC heavy-ion collisions","primary_cat":"hep-ph","submitted_at":"2026-04-17T06:23:04+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Bayesian posteriors from JETSCAPE jet-quenching model are largely compatible across centrality but exhibit shifts across beam energy and observable class, with varying ability to predict complementary datasets.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"Mueller, S. Peigne, and D. Schiff, Nucl. Phys. B484, 265 (1997), arXiv:hep- ph/9608322. [15] K. M. Burkeet al.(JET), Phys. Rev. C90, 014909 (2014), arXiv:1312.5003 [nucl-th]. [16] S. Caoet al.(JETSCAPE), Phys. Rev. C104, 024905 (2021), arXiv:2102.11337 [nucl-th]. [17] W. Fanet al.(JETSCAPE), Phys. Rev. C109, 064903 (2024), arXiv:2307.09641 [hep-ph]. [18] R. Ehlerset al.(JETSCAPE), Phys. Rev. C111, 054913 (2025), arXiv:2408.08247 [hep-ph]. [19] D. Everettet al.(JETSCAPE), Phys. Rev. C103, 054904 (2021), arXiv:2011.01430 [hep-ph]. [20] T. Sj¨ ostrand, S. Ask, J. R. Christiansen, R. Corke, N. Desai, P. Ilten, S. Mrenna, S. Prestel, and P. Skands, Comput. Phys. Commun.191, 159 (2015), arXiv:1410.3012 [hep-ph]."},{"citing_arxiv_id":"2604.10889","ref_index":44,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Heavy-quark transport across the QCD crossover driven by a lattice-constrained in-medium potential","primary_cat":"hep-ph","submitted_at":"2026-04-13T01:35:14+00:00","verdict":null,"verdict_confidence":null,"novelty_score":null,"formal_verification":null,"one_line_summary":null,"context_count":1,"top_context_role":"baseline","top_context_polarity":"baseline","context_text":"curves denote the results evaluated with the central value of the effective screening massM D while the shaded bands indicate the uncertainties arising from the variation ofM D. Phenomenological extractions and theoretical predictions are presented for comparison, including the JET Collaboration at E= 10 GeV (black circles [43]) and the JETSCAPE Collab- oration atE= 100 GeV (shadowed blue band [44]). ing kinematics. For a low-energy heavy quark, the typical momentum transfer during collisions is heavily weighted toward the soft infrared regime, where the non- perturbative string interaction dominates the cross sec- tion. In contrast, an energetic heavy quark undergoes collisions with significantly larger momentum transfers, effectively probing the short-distance structure of the in-"},{"citing_arxiv_id":"2512.07169","ref_index":62,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Bayesian Inference of Heavy-Quark Dissipation and Jet Transport Parameters from D-Meson observables in heavy-ion collisions at the LHC energies","primary_cat":"nucl-th","submitted_at":"2025-12-08T05:02:42+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"First simultaneous Bayesian extraction of 2πT D_s and q-hat/T^3 from D-meson R_AA and v2 at 5.02 TeV, yielding a non-monotonic temperature dependence in their ratio that deviates from the expected value of 2.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2510.25837","ref_index":6,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Deriving a parton shower for jet thermalization in QCD plasmas","primary_cat":"hep-ph","submitted_at":"2025-10-29T18:00:02+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"New parton-shower algorithm that exactly reproduces linearized EKT dynamics for jet thermalization including recoils, holes, quantum statistics and merging.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2510.25669","ref_index":26,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Minijet thermalization and jet transport coefficients in QCD kinetic theory","primary_cat":"hep-ph","submitted_at":"2025-10-29T16:33:17+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Minijet thermalization time in a thermal gluon plasma scales with the jet quenching parameter q-hat once recoiling medium contributions are added to standard transport coefficient definitions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2509.10743","ref_index":34,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Glauber quark and gluon contributions to quark energy loss at next-to-leading order and next-to-leading twist","primary_cat":"hep-ph","submitted_at":"2025-09-12T23:21:07+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Derives four scattering kernels for quark energy loss in nuclei at NLO and NLT, incorporating Glauber quarks and gluons plus mass and coherence effects.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2509.07842","ref_index":45,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Jet cone size dependence of single inclusive jet suppression due to jet quenching in Pb+Pb collisions at $\\sqrt{s_{\\rm NN}}=5.02$ TeV","primary_cat":"hep-ph","submitted_at":"2025-09-09T15:15:48+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Jet nuclear modification factor R_AA increases with cone radius R as in-cone energy loss from elastic recoils and radiated gluons decreases at larger radii.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}