{"total":18,"items":[{"citing_arxiv_id":"2606.30959","ref_index":6,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"A multi-differential constraint map for quarkonium suppression mechanisms in high-multiplicity pp and pPb collisions","primary_cat":"hep-ph","submitted_at":"2026-06-29T22:33:47+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Multi-differential constraint analysis of Υ(nS) suppression in high-multiplicity pp and pPb collisions favors an early, globally correlated, topology-sensitive mechanism over local-density or total-multiplicity control.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.28282","ref_index":7,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"QCD critical surface from constant entropy contours","primary_cat":"nucl-th","submitted_at":"2026-06-26T17:26:15+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"First mapping of the QCD critical surface in full (T, μ_B, μ_Q, μ_S) space via constant-entropy expansion gives a critical point at (114, 602) MeV in the pure baryon direction, with μ_B,c shifting 40-100 MeV in strangeness-neutral directions while remaining similar in charge-neutral ones.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.28086","ref_index":15,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"The QCD phase diagram for three-flavor M\\\"obius domain-wall fermions","primary_cat":"hep-lat","submitted_at":"2026-06-26T13:49:31+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Lattice simulations with Möbius domain-wall fermions find the three-flavor QCD transition at mu_B=0 is a continuous crossover at pseudocritical quark masses of 184(10) MeV (Nt=6), 36-39 MeV (Nt=8), and 3.5-3.7 MeV (Nt=12) in the MSbar scheme.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.12622","ref_index":31,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Analytic structure of the QCD phase diagram in the complex-temperature plane","primary_cat":"hep-th","submitted_at":"2026-06-10T19:28:44+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Extracts the continuum location of the nearest complex-T singularity from lattice QCD at μ=0 via iterated conformal-Padé and shows its trajectories share the same scaling variables as complex-μ singularities.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.12619","ref_index":4,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Constraining the Low-$p_T$ $\\eta/\\pi^0$ Ratio for Direct-Photon Analyses with Blast-Wave Fits to $\\pi$, $K$, and $p$ Spectra","primary_cat":"nucl-ex","submitted_at":"2026-06-10T19:21:17+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Uses blast-wave fits to pi, K, and p spectra plus measured K/pi to predict low-pT eta/pi0 ratio, finding eta-decay photon uncertainty of order 10% of direct-photon signal at pT~1 GeV/c in central Pb-Pb at 2.76 TeV.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.10356","ref_index":12,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Light and Strange Baryons in Medium","primary_cat":"hep-ph","submitted_at":"2026-06-09T03:10:31+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Parametric study of medium-induced shifts in the GBE quark model for baryon masses and their qualitative effect on ideal-gas yields.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.31280","ref_index":53,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Thermodynamics of the Isospectral family of holographic vector mesons","primary_cat":"hep-ph","submitted_at":"2026-05-29T13:11:38+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Isospectral transformations in softwall AdS/QCD allow tuning the rho meson's decay constant to its experimental value of 226 MeV, producing a predicted melting temperature of 157 MeV from spectral function computations at finite temperature and chemical potential.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.30710","ref_index":8,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Canonical statistical hadronization with local baryon conservation for higher-order cumulants","primary_cat":"hep-ph","submitted_at":"2026-05-29T01:01:32+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Local baryon conservation in a canonical ensemble drives net-proton κ6/κ2 to small or negative values in restricted acceptance, establishing a baseline that must be subtracted before interpreting signals of chiral criticality.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.13934","ref_index":20,"ref_count":2,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Diquark Correlators and Phase Structure in the Quark-Meson-Diquark Model beyond Mean Field","primary_cat":"hep-ph","submitted_at":"2026-05-13T16:12:38+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Including mesonic fluctuations beyond mean field in the quark-meson-diquark model substantially modifies the phase structure, with diquark condensation dominating at strong couplings as revealed by pole masses and the Silver-Blaze property.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Aartset al., Phase transitions in particle physics: Results and perspectives from lattice quantum chromo- dynamics, Prog. Part. Nucl. Phys.133, 104070 (2023), arXiv:2301.04382 [hep-lat]. [19] C. S. Fischer, Qcd at finite temperature and chemical potential from dyson-schwinger equations, Prog. Part. Nucl. Phys.105, 1 (2019), arXiv:1810.12938 [hep-ph]. [20] W.-j. Fu, QCD at finite temperature and density within the fRG approach: an overview, Commun. Theor. Phys. 74, 097304 (2022), arXiv:2205.00468 [hep-ph]. [21] N. Dupuis, L. Canet, A. Eichhorn, W. Metzner, J. M. Pawlowski, M. Tissier, and N. Wschebor, The nonper- turbative functional renormalization group and its ap- plications, Phys. Rept.910, 1 (2021), arXiv:2006."},{"citing_arxiv_id":"2604.22514","ref_index":5,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Quark Number Susceptibilities and Conserved Charge Fluctuations in $(2+1)$-flavor QCD with M\\\"obius domain-wall fermions (MDWF)","primary_cat":"hep-lat","submitted_at":"2026-04-24T12:54:33+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Lattice simulations with Möbius domain-wall fermions find that conserved charge fluctuations in (2+1)-flavor QCD match hadron resonance gas predictions below the pseudocritical temperature and rise toward free-quark limits above it.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.22352","ref_index":17,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Four-dimensional QCD equation of state from a quasi-parton model with physics-informed neural networks","primary_cat":"nucl-th","submitted_at":"2026-04-24T08:38:37+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A PINN-trained quasi-parton model reproduces lattice cumulants at vanishing chemical potentials and supplies a consistent four-dimensional QCD equation of state at finite densities.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"13867 [nucl-th]. [14] R. Kumaret al.(MUSES), Living Rev. Rel.27, 3 (2024), arXiv:2303.17021 [nucl-th]. [15] X.-Y. Wu, G.-Y. Qin, L.-G. Pang, and X.-N. Wang, Phys. Rev. C105, 034909 (2022), arXiv:2107.04949 [hep- ph]. [16] S. Borsanyi, Z. Fodor, C. Hoelbling, S. D. Katz, S. Krieg, and K. K. Szabo, Phys. Lett. B730, 99 (2014), arXiv:1309.5258 [hep-lat]. [17] A. Bazavovet al.(HotQCD), Phys. Lett. B795, 15 (2019), arXiv:1812.08235 [hep-lat]. [18] A. Bazavovet al.(HotQCD), Phys. Rev. D86, 034509 (2012), arXiv:1203.0784 [hep-lat]. [19] A. Bazavovet al.(HotQCD), Phys. Rev. D90, 094503 (2014), arXiv:1407.6387 [hep-lat]. [20] D. Bollweg, J. Goswami, O. Kaczmarek, F. Karsch, S. Mukherjee, P. Petreczky, C. Schmidt, and"},{"citing_arxiv_id":"2604.19649","ref_index":12,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Finite-density equation of state of hot QCD using the complex Langevin equation","primary_cat":"hep-lat","submitted_at":"2026-04-21T16:37:53+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Continuum-extrapolated lattice QCD simulations with complex Langevin produce the equation of state at high baryon chemical potentials above the crossover temperature at the physical point.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"[10] S. Bors' anyi, Z. Fodor, J. N. Guenther, R. Kara, S. D. Katz, P. Parotto, A. P' asztor, C. Ratti, and K. K. Szab' o, Phys. Rev. Lett.126, 232001 (2021), arXiv:2102.06660 [hep-lat]. [11] S. Bors' anyi, J. N. Guenther, R. Kara, Z. Fodor, P. Parotto, A. P' asztor, C. Ratti, and K. Szab' o, Phys. Rev. D105, 114504 (2022), arXiv:2202.05574 [hep-lat]. [12] S. Bors' anyi, Z. Fodor, M. Giordano, S. D. Katz, D. N' ogradi, A. P' asztor, and C. H. Wong, Phys. Rev. D105, L051506 (2022), arXiv:2108.09213 [hep-lat]. [13] D. Bollweg et al. (HotQCD Collaboration), Phys. Rev. D105, 074511 (2022), arXiv:2202.09184 [hep-lat]. [14] S. Bors' anyi, Z. Fodor, M. Giordano, J. N. Guenther, S. D. Katz, A. P' asztor, and C."},{"citing_arxiv_id":"2604.03849","ref_index":37,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Two Lectures on the Phase Diagram of QCD","primary_cat":"hep-ph","submitted_at":"2026-04-04T20:14:54+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"QCD features at least three phases at zero baryon density and three at high density, including a Quarkyonic phase at high density and low temperature, described via large-N_c and a parameter-free 3D string model.","context_count":1,"top_context_role":"dataset","top_context_polarity":"use_dataset","context_text":"plot the resulting chiral condensate as a function of the temperature. The sigma 17 0.10 0.12 0.14 0.16 0.18 0.20 0.22 Temperature T [GeV] 0.0 0.2 0.4 0.6 0.8 1.0 1.2Chiral condensate T/ 0 NG mesons ( , K, ) NG mesons + Open strings Lattice QCD (Wuppertal-Budapest) FIG. 5.Ratio of the chiral condensate at finite temperature to that at zero temperature. The lattice data are taken from Ref. [37]. The averaged sigma term per quark,¯σ≃30 MeV, is obtained from the best fit to the lattice-QCD data and it is varied within15-60MeV to account for uncertainty. The blue curve corresponds to the first term in the square bracket in Eq. (17), and the orange curve includes the contribution from the second term in the square bracket in Eq. (17). Figure from Ref."},{"citing_arxiv_id":"2603.09977","ref_index":1,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Does hot QCD have a conformal manifold in the chiral limit?","primary_cat":"hep-th","submitted_at":"2026-03-10T17:59:59+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"An 't Hooft anomaly at general imaginary baryon chemical potential constrains the QCD chiral transition to three minimal CFT scenarios, with the favored one for N_f >= 3 featuring a conformal manifold of theta_B-dependent universality classes with an exactly marginal operator tied to baryon density.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Understanding the phase diagram of quantum chromodynamics (QCD) as a function of tem- peratureTand baryon chemical potentialµ B is a central challenge in high-energy physics, with implications for heavy-ion collisions, astrophysics, and the early universe. Atµ B = 0, increasingTrestores the spontaneously bro- ken approximate chiral symmetry through a crossover at T∼155MeV [1, 2]. IfN f quarks are massless, chi- ral symmetry becomes exact, and the crossover becomes a genuine phase transition. The standard approach to this nonperturbative phase transition appeals to Landau universality. A Ginzburg-Landau analysis based on the chiral condensateΦ = ¯ψLψR [3] suggests a first-order transition forN f ≥3, and a second-order transition for"},{"citing_arxiv_id":"2602.14811","ref_index":12,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"RG-Invariant Symmetry Ratio for QCD: A Study of $U(1)_A$ and Chiral Symmetry Restoration","primary_cat":"hep-lat","submitted_at":"2026-02-16T15:04:00+00:00","verdict":"CONDITIONAL","verdict_confidence":"MODERATE","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Continuum extrapolation of lattice QCD data shows that SU(2)_L × SU(2)_R chiral and U(1)_A axial symmetry breaking strengths in nonsinglet quark-connected channels converge to the same value near the chiral crossover temperature.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2510.22870","ref_index":14,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Mass and Decay-Constant Evolution of Heavy Quarkonia and $B_c$ States from Thermal QCD Sum Rules","primary_cat":"hep-ph","submitted_at":"2025-10-26T23:27:26+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Thermal QCD sum rules with updated inputs yield a suppression hierarchy Υ < J/ψ < B_c for masses and decay constants near Tc, calibrated to vacuum data and consistent with LHCb B_c splitting.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2510.06712","ref_index":10,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Dissecting the moat regime at low energies I: Renormalization and the phase structure","primary_cat":"hep-ph","submitted_at":"2025-10-08T07:06:46+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"In the random phase approximation, a convenient renormalization scheme for momentum-dependent meson self-energies shows that the moat regime extent in the QCD phase diagram depends critically on in-medium quark-meson interactions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"1907.08179","ref_index":9,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Strangeness neutrality and the QCD phase diagram","primary_cat":"hep-ph","submitted_at":"2019-07-18T17:39:39+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Strangeness neutrality imposes a constraint linking baryon-strangeness correlations to the QCD equation of state, with their dependence on freeze-out conditions computed in a 2+1 flavor Polyakov-quark-meson model using the functional renormalization group.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}