{"total":14,"items":[{"citing_arxiv_id":"2607.01496","ref_index":129,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Towards triggerless four-dimensional detectors for High Energy Physics collider experiments","primary_cat":"physics.ins-det","submitted_at":"2026-07-01T21:53:41+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"Reviews precision timing integration in LHC upgrades and discusses a possible shift to triggerless detectors enabled by timing and networking, with reflections on physics benefits.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.20028","ref_index":18,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Probing flavor effects in the QCD parton shower using $\\mathbf{{\\rm D}^0}$-tagged jet angularities in proton$-$proton collisions at $\\mathbf{ \\sqrt{s} = 5.02}$ TeV","primary_cat":"nucl-ex","submitted_at":"2026-06-18T09:59:09+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"First measurement of D0-tagged jet angularities in pp collisions at 5.02 TeV shows smaller values at low angular weight, consistent with the QCD dead-cone effect for massive quarks.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.03552","ref_index":25,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"$D^0$-$D_s^+$ Elliptic-Flow Splitting under Event-Shape Engineering: A Probe of Sequential Charm Hadronization","primary_cat":"hep-ph","submitted_at":"2026-06-02T12:14:11+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Event-shape engineering via q2 selection in 0-10% and 30-50% Pb-Pb collisions at 5.02 TeV is shown to separate geometry-driven flow from hadronization-time effects, producing a positive growing Δv2(D0-Ds+) and species-dependent χ slope only in the sequential scenario.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.02693","ref_index":66,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Stochastic Dynamics of Heavy Quarks in Strongly Coupled Plasma","primary_cat":"hep-ph","submitted_at":"2026-06-01T18:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Kolmogorov dynamics for heavy quarks in hot plasma shows significantly delayed large-momentum equilibration compared to Fokker-Planck with matched drag, due to rare low-momentum-loss events.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.31527","ref_index":53,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Accessing Exotic Hadronic States via Charmed-Meson Femtoscopy in Relativistic Heavy-Ion Collisions","primary_cat":"nucl-th","submitted_at":"2026-05-29T16:40:55+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Simulations indicate that heavy-ion collisions enhance the visibility of charmed-meson femtoscopic correlations compared to pp collisions, providing a probe for exotic hadronic states.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.26766","ref_index":57,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Sensitivity of Heavy-Quark Dipolar Flow to its Initial Spatial Distributions in Cu+Au Collisions","primary_cat":"nucl-th","submitted_at":"2026-05-26T09:37:55+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"In Cu+Au collisions, heavy-quark directed flow is an order of magnitude larger than charged-hadron flow and shows strong sensitivity to initial spatial distributions and temperature-dependent drag.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.21222","ref_index":41,"ref_count":2,"confidence":0.98,"is_internal_anchor":true,"paper_title":"System-size dependence of the $D^0$--$D_s^+$ flow splitting from early $D_s^+$ formation at $\\sqrt{s_{NN}} = 5.36$~TeV","primary_cat":"hep-ph","submitted_at":"2026-05-20T14:14:18+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Sequential hadronization predicts v2(D0) > v2(Ds+) from extra partonic flow accumulated by D0 parents between 1.2 Tc and Tc, with universal linear scaling of the hadronic splitting across O-O and Pb-Pb systems.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.16019","ref_index":28,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Inclusive charm and bottom quark pair production cross sections at hadron colliders at next-to-next-to-leading-order accuracy","primary_cat":"hep-ph","submitted_at":"2026-05-15T14:52:04+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"NNLO QCD calculations using the MaunaKea code enhance c cbar and b bbar production cross sections by up to a factor of two over NLO predictions, reduce scale uncertainties, and match experimental data from 10 GeV to 14 TeV while suggesting PDF and mass constraints.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.11574","ref_index":38,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"SemiCharmTag: a tool for Semileptonic Charm tagging","primary_cat":"hep-ex","submitted_at":"2026-04-13T14:52:52+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":"anticharm hadron pair, taking into account the combined average fragmentation and decay fractions from LEP Γ( c → l)/Γ(c → anything) = 0.096 ± 0.004 (Γ(b → l)/Γ(b → anything) = 0.1069 ± 0.0022) [15]. For the beauty cross-section, B mixing is not taken 5 into account. The procedure was validated by comparison with single charm fixed-order next to leading logarithm (FONLL) calculations [38,39], giving compatible results at the inclusive partonic cross section level. The fiducial cross-section values for each process are: σpp→Z0/γ→µ+µ− = 451.5 pb, σpp→c¯c→µ+µ− = 2.1 · 104 pb and σpp→b¯b→µ+µ− = 5.4 · 104 pb. Finally, the resulting signal/background ratio for charm is S c = 2+3.01 −1.35% while for beauty is S b = 0.84+0.34 −0.31%. The uncertainty is given by the charm and beauty total NLO cross"},{"citing_arxiv_id":"2604.07982","ref_index":101,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Memory effect on the heavy quark dynamics in hot QCD matter","primary_cat":"hep-ph","submitted_at":"2026-04-09T08:53:55+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Time-correlated thermal noise modeled with a fractional derivative substantially alters heavy quark momentum correlations, displacement, and transverse-momentum moments in hot QCD matter.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.07968","ref_index":36,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Multiplicity dependence of prompt and non-prompt J/$\\psi$ production at midrapidity in pp collisions at $\\sqrt{s} = 13$ TeV","primary_cat":"hep-ex","submitted_at":"2026-04-09T08:32:37+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Self-normalized yields of prompt and non-prompt J/ψ increase stronger than linearly with charged-particle multiplicity in pp collisions at 13 TeV, with stronger effect in the toward azimuthal region.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"of MC signals are therefore corrected with multiplicity-dependent weights. These weights are taken from a parametrization of the multiplicity-dependent J/ψyield and of the non-prompt fraction obtained after the first iteration of the algorithm. Thep T distributions also vary with multiplicity. Following a method similar to the one described in Ref. [36], theNtrks dependence of⟨p T⟩of inclusive J/ψmesons is determined. The⟨p T⟩increases with multiplicity. Ap T-dependent weight is applied in every multiplicity interval in order to reproduce the hardening of the spectrum. Finally, since thep T dependence of the ratios between different beauty hadrons is not reproduced in PYTHIA 8 by the Monash tune, for non-"},{"citing_arxiv_id":"2604.02944","ref_index":90,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Non-equilibrium Dynamical Attractors and Thermalisation of Charm Quarks in Nuclear Collisions at the LHC Energy","primary_cat":"hep-ph","submitted_at":"2026-04-03T10:23:51+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Charm quarks develop dynamical attractors in expanding QGP but with lattice-QCD diffusion coefficients require ~5 fm to relax, leading to O(1) deviations from equilibrium already at pT ~ 3 GeV and incomplete thermalization in small systems.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"we explore a variety of initial conditions in momentum space: ∙FONLL,𝑓 FONLL(𝑝𝑇 )and𝑌=𝜂 𝑠;𝑓 FONLL(𝑝𝑇 )is obtained by setting2.75TeV as the beam energy and the PDF set NNPDF30_nlo_as_0118 and taking the central value. This is the typical initial condition used in HQ transport simulations and is able to describe the𝐷-meson spectra in proton-proton collisions after fragmentation [90]; ∙EPOS4HQ,𝑓 EPOS4HQ(𝑝𝑇 )and𝑌=𝜂 𝑠. The𝑝 𝑇- distribution is the one in𝑝𝑝collisions of the Monte Carlo simulator EPOS. It includes for HQ productions the Born processes and both space-like and time-like cascades. The 𝑓EPOS4HQ(𝑝𝑇 )is consistent with FONLL for high𝑝 𝑇, but predicts a large bump localized in the low𝑝𝑇 (<2 GeV region), for details Ref. [91]."},{"citing_arxiv_id":"2512.07169","ref_index":78,"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":"2506.22616","ref_index":7,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"A novel phenomenological approach to total charm cross-section measurements at the LHC","primary_cat":"hep-ph","submitted_at":"2025-06-27T20:26:38+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"A data-driven ddFONLL extrapolation method accounts for LHC-observed charm fragmentation non-universality to derive higher total charm cross sections from D0 fiducial measurements at 5 and 13 TeV, consistent with NNLO QCD predictions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}