{"total":16,"items":[{"citing_arxiv_id":"2607.02042","ref_index":50,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Probing hot QCD medium with heavy quarkonium in small and large collision systems","primary_cat":"nucl-th","submitted_at":"2026-07-02T11:09:33+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"A time-dependent Schrödinger equation model reproduces suppression of Υ(nS)/Υ(1S) and ψ(2S)/J/ψ yield ratios versus multiplicity in p-Pb collisions at 8.16 TeV, supporting transient hot QCD medium in small systems.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2607.01783","ref_index":57,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Subensemble Acceptance Method 3.0: General Corrections to Cumulants from Exact Conservation Constraints","primary_cat":"hep-ph","submitted_at":"2026-07-02T06:54:27+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"SAM-3.0 derives canonical cumulants from grand-canonical joint cumulants via a closed recursion with multivariate partial exponential Bell polynomials for arbitrary numbers of conserved charges and observables.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.26326","ref_index":229,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Studying the QCD Matter produced in Heavy-Ion Collisions using the MUSES Calculation Engine","primary_cat":"nucl-th","submitted_at":"2026-06-24T19:12:40+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"The MUSES Calliope engine computes multi-dimensional QCD equations of state, merges them consistently, and feeds them into viscous hydrodynamic simulations of heavy-ion collisions with movable critical points and critical scaling in transport coefficients.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"is archived on Zenodo at [228]. B. EoS Inverter EoSs generated using heavy-ion collisions modules of the MUSES Calculation Engine are tabulated as func- tions of the thermodynamic variables, namely (T, µ X). Quantities such assorn X can then be expressed as: (s, nX) =F EoS(T, µX).(44) 26 In heavy-ion simulations, the natural variables are the dynamicalvariables,s(orε) andn X [62, 64, 229]. The choice betweenεorsusually depends on the specific hydrodynamic code, wherein most grid-based codes cur- rently useεand most smoothed particle hydrodynamics (SPH) codes uses. Since the proof-of-principle external solver used in this work isCCAKE, which is a mesh-free Lagrangian hydrodynamics code, our examples here are written in terms of (s, nX)."},{"citing_arxiv_id":"2606.22558","ref_index":30,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Event-by-event fluctuations of elliptic flow in ultrarelativistic O+O collisions","primary_cat":"nucl-th","submitted_at":"2026-06-21T15:33:04+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"In O+O collisions, initial eccentricity and elliptic flow are fluctuation-driven and can be reproduced from a small set of uncorrelated modes.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.10526","ref_index":6,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Tensor Decomposition for Energy-Momentum Correlation Functions","primary_cat":"hep-ph","submitted_at":"2026-06-09T07:55:05+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Energy-momentum tensor correlator is reduced to fewer spectral functions via rotational symmetry decomposition and conservation-derived differential relations at zero and finite temperature.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.09984","ref_index":3,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Tame the Umklapp Processes in Real-Time Lattice Simulation for Hydrodynamics: An Ising Field Theory Study","primary_cat":"hep-lat","submitted_at":"2026-06-08T18:00:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Real-time lattice Hamiltonian simulation of a three-particle Ising field theory suppresses Umklapp processes and produces relativistic hydrodynamics sound modes, extracting ζ/s=14.19±0.90 and c_s/c=0.76±0.02 at T≈7.14.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.06283","ref_index":3,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Diffusion of multiple conserved charges from entropy production","primary_cat":"hep-ph","submitted_at":"2026-06-04T15:23:56+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Derives diffusion matrix elements for baryon, charge, and strangeness transport in relativistic hydrodynamics from entropy production within the relaxation-time approximation.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.00171","ref_index":32,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Dependence of two-particle azimuthal correlations on the forward rapidity gap width in pPb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 8.16 TeV","primary_cat":"nucl-ex","submitted_at":"2026-05-29T13:12:07+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"CMS measures V_nΔ in pPb events at √s_NN = 8.16 TeV as a function of forward rapidity gap width, p_T, and multiplicity in γPb and IP Pb enriched samples, comparing to prior pp, pPb, and γp data plus event generators.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.30180","ref_index":69,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"The polarization of thermal dileptons emitted in high-energy heavy-ion collisions","primary_cat":"nucl-th","submitted_at":"2026-05-28T16:27:49+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Thermal dilepton polarization in LHC heavy-ion collisions is sensitive to QGP in-medium properties, with a one-to-one mapping derived between dielectron and dimuon channels.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.26766","ref_index":59,"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":"2605.26737","ref_index":69,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Cumulants of mean transverse momentum and elliptic flow in the hydrodynamic model of heavy-ion collisions","primary_cat":"nucl-th","submitted_at":"2026-05-26T09:12:07+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Hydrodynamic simulations of heavy-ion collisions demonstrate that cumulants linking mean pT and elliptic flow quantitatively match relations derived from initial-state entropy predictors and moments of harmonic flow.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.27254","ref_index":11,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Species-Resolved Scaling of Azimuthal Anisotropy: Constraining Attenuation, Collective Expansion, and Hadronic Dynamics in Hydrodynamic Simulations","primary_cat":"nucl-th","submitted_at":"2026-04-29T22:58:25+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Species-resolved scaling functions for azimuthal anisotropy from iEBE-VISHNU simulations of Pb+Pb collisions collapse robustly across kinematics and species, enabling constraints on attenuation, collective expansion, and hadronic re-scattering via an energy-dependent baseline.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Heinz, T. Hirano, and C. Shen, Phys. Rev. Lett.106, 192301 (2011), arXiv:1011.2783 [nucl-th]. [8] C. Shen, Z. Qiu, and U. Heinz, Phys. Rev. C92, 014901 (2015), arXiv:1502.04636 [nucl-th]. [9] W. Zhao, H.-j. Xu, and H. Song, Eur. Phys. J. C77, 645 (2017), arXiv:1703.10792 [nucl-th]. [10] B. Schenke, S. Jeon, and C. Gale, Phys. Rev.C82, 014903 (2010). [11] B. Schenke, S. Jeon, and C. Gale, Phys. Rev. Lett.106, 042301 (2011), arXiv:1009.3244 [hep-ph]. [12] S. McDonald, C. Shen, F. Fillion-Gourdeau, S. Jeon, and C. Gale, Phys. Rev. C95, 064913 (2017), arXiv:1609.02958 [hep-ph]. [13] M. Bleicheret al., J. Phys. G25, 1859 (1999), arXiv:hep- ph/9909407. [14] S. A. Basset al., Prog. Part. Nucl. Phys.41, 255 (1998),"},{"citing_arxiv_id":"2604.09198","ref_index":47,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Unified Extraction of In-Medium Heavy Quark Potentials from RHIC to LHC Energies via Deep Learning","primary_cat":"nucl-th","submitted_at":"2026-04-10T10:33:40+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Deep learning extracts a unified in-medium heavy quark potential from multi-energy bottomonium data, finding the real part close to vacuum Cornell form with weak screening while the imaginary part dominates suppression.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"09215]. [45]LHCbcollaboration,Study ofχ b meson production inp pcollisions at √s= 7and8 TeV and observation of the decayχ b(3P)→Υ(3S)γ,Eur. Phys. J. C74(2014) 3092 [1407.7734]. [46] C.M.S. Collaboration,Measurement of the production cross section ratioσ(χ b2(1p)) / σ(χb1(1p)) in pp collisions at √s= 8 TeV,Physics Letters B743(2015) 383 [1409.5761]. [47] J.-P. Lansberg,New observables in inclusive production of quarkonia,Physics Reports889 (2020) 1 [1903.09185]. [48]PHENIXcollaboration,υ(1S+ 2S+ 3S)production ind+Au andp+pcollisions at√sN N = 200GeV and cold-nuclear matter effects,Phys. Rev. C87(2013) 044909 [1211.4017]. [49]STARcollaboration,Suppression ofΥproduction in d+Au and Au+Au collisions at√sN N=200 GeV,Phys."},{"citing_arxiv_id":"2512.08007","ref_index":21,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"(3+1)D event-by-event pre-equilibrium dynamics in heavy-ion collisions","primary_cat":"hep-ph","submitted_at":"2025-12-08T19:55:31+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Extension of KoMPoST to (3+1)D non-boost-invariant pre-equilibrium dynamics via kinetic theory response functions, chained into a full McDIPPER+KoMPoST-3D+CLVisc+SMASH simulation chain to study sensitivity of longitudinal flow to hydrodynamic start time.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2510.25837","ref_index":23,"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":"2504.02726","ref_index":45,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Constraining hot and cold nuclear matter properties from heavy-ion collisions and deep-inelastic scattering","primary_cat":"nucl-th","submitted_at":"2025-04-03T16:10:25+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Global analysis of HERA DIS and ALICE Pb+Pb data using saturation initial-state model determines early-time non-equilibrium η/s of QGP.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}