{"total":13,"items":[{"citing_arxiv_id":"2606.30164","ref_index":3,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Isospin-Driven Splitting of Chemical Potentials in Isobar Collisions from Lattice QCD","primary_cat":"hep-lat","submitted_at":"2026-06-29T11:42:19+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Lattice QCD yields first-principles splitting ratios for chemical potentials in Ru+Ru vs Zr+Zr collisions that are comparable in size to Bayesian STAR extractions, with Δμ_Q negative, Δμ_S positive, and only moderate magnetic-field dependence.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.28111","ref_index":7,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Dense and Cold Magnetized Quark Matter: A Review of Magnetic-Field-Independent Regularization and the Medium Separation Scheme","primary_cat":"hep-ph","submitted_at":"2026-06-26T14:11:56+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"Review of MFIR and MSS schemes showing the superconducting gap stays finite at high chemical potential in magnetized cold quark matter with no zero-temperature transition to normal phase.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.02723","ref_index":23,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Magnetized bottom-up thermalization in heavy-ion collisions","primary_cat":"hep-ph","submitted_at":"2026-06-01T18:00:08+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Strong magnetic fields may accelerate early quark production via gluon decay in the bottom-up scenario when |eB| approaches Q_s^2, modifying pre-equilibrium chemical composition.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.25487","ref_index":4,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"A higher-harmonic observable for the chiral magnetic effect in heavy-ion collisions","primary_cat":"nucl-th","submitted_at":"2026-05-25T06:43:13+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"The hexadecapole component of Δγ(φ_pair) is proposed as a CME-sensitive and background-insensitive observable based on magnetic field fluctuations in heavy-ion collision models.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.12554","ref_index":197,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Spin dynamics and polarization in relativistic systems: recent developments","primary_cat":"nucl-th","submitted_at":"2026-05-11T09:31:06+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":1.0,"formal_verification":"none","one_line_summary":"The review summarizes developments in spin hydrodynamics, polarization from spin-vorticity coupling, pseudo-gauge freedom, and heavy-flavor spin dynamics in relativistic systems.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"clear experimental signal of such magnetic fields has not yet been conclusively identified. Several proposed observables are expected to be sensitive to the presence of these fields, most notably the Chiral Magnetic Effect (CME)- a charge separation phenomenon along the magnetic field direction arising from the interplay between the chiral anomaly and the strong magnetic field [197, 207]. Although charge-dependent azimuthal correlations consistent with CME expectations have been reported by the STAR [208, 209] and ALICE [210] collaborations, subsequent analyses, including the recent isobar run at RHIC, indicate that the observed signals can largely be attributed to background effects related to elliptic flow, leaving the CME interpretation unconfirmed."},{"citing_arxiv_id":"2605.01807","ref_index":45,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Relativistic BDNK MHD Evolution in a Boost-Invariant Medium and Its Impact on Dilepton Production","primary_cat":"nucl-th","submitted_at":"2026-05-03T10:23:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Coupled BDNK MHD evolution in boost-invariant flow enhances cooling and suppresses the low-mass dilepton spectrum via magnetic-thermal feedback.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"[hep-th]. 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B848, 138342"},{"citing_arxiv_id":"2604.24595","ref_index":17,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Mass spectra of charged mesons and the quenching of vector meson condensation via exact phase-space diagonalization","primary_cat":"hep-ph","submitted_at":"2026-04-27T15:20:07+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"In the NJL model with exact phase-space diagonalization, magnetic catalysis of the chiral condensate quenches the tachyonic instability of the spin-aligned rho+ by driving the 2M threshold above the Zeeman-lowered mass, preventing condensation.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Shushpanov, Gell-Mann-Oakes-Renner relation in a magnetic field at finite temperature, JHEP 10, 006, arXiv:hep-ph/0107128. [15] J. O. Andersen, Thermal pions in a magnetic background, Phys. Rev. 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B710, 171 (2012), arXiv:1111.1949 [hep-ph]. [46] W.-T. Deng and X.-G. Huang, Phys. Rev. C85, 044907 (2012), arXiv:1201.5108 [nucl-th]. [47] S. Pu, V. Roy, L. Rezzolla, and D. H. Rischke, Phys. Rev. D93, 074022 (2016), arXiv:1602.04953 [nucl-th]. [48] L. Adamczyket al.(STAR), Nature548, 62 (2017), arXiv:1701.06657 [nucl-ex]. [49] W.-T. Deng and X.-G. Huang, Phys. Rev. C93, 064907 (2016), arXiv:1603."},{"citing_arxiv_id":"2604.15897","ref_index":10,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Delineating neutral and charged mesons in magnetic fields","primary_cat":"hep-ph","submitted_at":"2026-04-17T09:55:18+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Neutral mesons conserve continuous transverse momenta in magnetic fields while charged mesons exhibit quantized transverse dynamics, with high-spin charged mesons stabilized by cancellation of internal zero-point energy against orbital Zeeman energy.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"de la Incera, Phase transitions and resilience of the magnetic dual chiral density wave phase at finite temperature and density, Phys. Rev. D106, 016011 (2022), arXiv:2203.14209 [nucl-th]. [9] E. J. Ferrer and V. de la Incera, Magnetic Dual Chi- ral Density Wave: A Candidate Quark Matter Phase for the Interior of Neutron Stars, Universe7, 458 (2021), arXiv:2201.04032 [hep-ph]. [10] E. J. Ferrer and V. de la Incera, Novel Topological Effects in Dense QCD in a Magnetic Field, Nucl. Phys. B931, 192 (2018), arXiv:1512.03972 [nucl-th]. [11] P. Adhikariet al., Strongly interacting matter in extreme magnetic fields, Prog. Part. Nucl. Phys.146, 104199 (2026), arXiv:2412.18632 [nucl-th]. [12] K. Hattori and X.-G. Huang, Novel quantum phenomena"},{"citing_arxiv_id":"2601.18354","ref_index":3,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Chiral Properties of $(2\\!+\\!1)$-Flavor QCD in Magnetic Fields at Zero Temperature","primary_cat":"hep-lat","submitted_at":"2026-01-26T11:01:58+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Continuum-extrapolated lattice simulations show monotonic magnetic catalysis in chiral condensates, non-monotonic charged-meson mass response, and valence-quark dominance at zero temperature up to eB ≈ 1.2 GeV².","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2510.17597","ref_index":43,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Photon radiation induced by rescattering in strong-interacting medium with a magnetic field","primary_cat":"nucl-th","submitted_at":"2025-10-20T14:47:42+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Photon emission rate and electromagnetic energy loss from rescattering in magnetized QGP are derived in the high-energy limit, showing slight suppression over broad jet energies.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2509.02228","ref_index":45,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Polarized tau decay and CP violation in ultraperipheral heavy-ion collisions","primary_cat":"hep-ph","submitted_at":"2025-09-02T11:49:48+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Proposes that the relative polarization of tau+ and tau- decay products in UPCs, aligned to the magnetic field, provides a sensitive probe for CP violation.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2508.17757","ref_index":3,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Stationary States for Fermions in an External Electric Field","primary_cat":"nucl-th","submitted_at":"2025-08-25T07:56:04+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Stationary solutions of the Dirac equation for fermions in an external electric field exhibit asymptotic oscillations, absence of bound states in infinite systems, and deconfining behavior when electric coupling exceeds confinement coupling, with MIT bag boundaries enabling finite-system confinement","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}