{"total":15,"items":[{"citing_arxiv_id":"2605.25487","ref_index":3,"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":"2605.23021","ref_index":6,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Finite-Size Effects on the Critical End Point of Magnetized Quark Matter in the Nonlocal PNJL Model","primary_cat":"hep-ph","submitted_at":"2026-05-21T20:45:28+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Finite-size effects in the nonlocal PNJL model shift the critical end point of magnetized quark matter toward higher chemical potentials and lower temperatures as droplet radius decreases.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.17438","ref_index":39,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Holographic entanglement entropy in the QCD phase diagram under external magnetic field","primary_cat":"hep-th","submitted_at":"2026-05-17T13:20:12+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Holographic entanglement entropy exhibits a swallow-tail structure indicating connected-to-disconnected transitions for perpendicular magnetic fields in the QCD phase diagram while remaining monotonic for parallel fields, consistent with black hole thermodynamics.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.12554","ref_index":192,"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":"Examples include the heavy-flavor diffusion coefficient [188, 189], heavy-quark suscep- tibilities [190], and mesonic correlation functions [191]. Although these observables are not directly measurable in experiments, they provide essential theoretical benchmarks and constraints for transport models, thereby establishing a crucial link between first-principles QCD calculations and experimental data [192]. In studies of QCD matter created in heavy-ion collisions, the large mass of heavy quarks,m Q, combined with flavor conservation in strong interactions, lead to several important consequences. These features provide the theoretical foundation for formulating the Brownian motion framework of heavy quarks propagating through a thermalized medium: 1."},{"citing_arxiv_id":"2605.04743","ref_index":87,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Chiral Magnetic Effect and Negative Magnetoresistance across the phase diagram of finite-density SU(2) gauge theory","primary_cat":"hep-lat","submitted_at":"2026-05-06T10:47:41+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"In SU(2) lattice QCD at finite density, the chiral magnetic effect from axial-vector correlators remains close to the free massless quark value with weak T and mu dependence in the plasma, while negative magnetoresistance from vector correlators is strongly suppressed at high density or temperature.","context_count":1,"top_context_role":"background","top_context_polarity":"unclear","context_text":"Laer- mann, and W. Soeldner, Phys. Rev. D83, 034504 (2011), 1012.4963. [84] K. Fukushima and Y. Hidaka, JHEP04, 162, arXiv:1906.02683 [hep-ph]. [85] A. Shaikh, S. Rath, S. Dash, and B. Panda, Phys. Rev. D108, 056021 (2023), arXiv:2210.15388 [hep-ph]. [86] L. Thakur and P. K. Srivastava, Phys. Rev. D100, 076016 (2019), arXiv:1910.12087 [hep-ph]. 13 [87] V. Skokov, A. Illarionov, and V. Toneev, Int. J. Mod. Phys. A24, 5925 (2009), 0907.1396. [88] K. Tuchin, Phys. Rev. C88, 024911 (2013), arXiv:1305.5806 [hep-ph]."},{"citing_arxiv_id":"2605.01807","ref_index":43,"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":"Hoult and A. Shukla, JHEP04, 172, arXiv:2410.22855 [hep-th]. [39] N. Weickgenannt, Phys. Rev. D108, 076011 (2023), arXiv:2307.13561 [nucl-th]. [40] A. Jain and P. Kovtun, JHEP01, 162, arXiv:2309.00511 [hep-th]. [41] J. Armas and F. Camilloni, JCAP10, 039, arXiv:2201.06847 [hep-th]. [42] R. E. Hoult and P. Kovtun, JHEP04, 009, arXiv:2411.04966 [hep-th]. [43] V. Skokov, A. Y. Illarionov, and V. Toneev, Int. J. Mod. Phys. A24, 5925 (2009), arXiv:0907.1396 [nucl-th]. [44] A. Bzdak and V. Skokov, Phys. Lett. B710, 171 (2012), arXiv:1111.1949 [hep-ph]. [45] W.-T. Deng and X.-G. Huang, Phys. Rev. C85, 044907 (2012), arXiv:1201.5108 [nucl-th]. [46] U. Gursoy, D. Kharzeev, and K. Rajagopal, Phys. Rev. C89, 054905 (2014), arXiv:1401."},{"citing_arxiv_id":"2604.24595","ref_index":16,"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":"Zhang, Chiral Properties of (2 + 1)-Flavor QCD in Magnetic Fields at Zero Temperature (2026), arXiv:2601.18354 [hep-lat]. [14] N. O. Agasian and I. A. 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. D86, 025020 (2012), arXiv:1202.2051 [hep-ph]. [16] V. D. Orlovsky and Y. A. Simonov, Nambu-Goldstone mesons in strong magnetic field, JHEP09, 136, arXiv:1306.2232 [hep-ph]. [17] G. Colucci, E. S. Fraga, and A. Sedrakian, Chiral pions in a magnetic background, Phys. Lett. B728, 19 (2014), arXiv:1310.3742 [nucl-th]. [18] S. S. Avancini, R. L. S. Farias, M. Benghi Pinto, W. R. Tavares, and V. S. Tim' oteo,π 0 pole mass calculation in a strong"},{"citing_arxiv_id":"2604.15897","ref_index":9,"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, and C. Manuel, Magnetic color flavor locking phase in high density QCD, Phys. Rev. Lett.95, 152002 (2005), arXiv:hep-ph/0503162. [8] W. Gyory and V. 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."},{"citing_arxiv_id":"2604.08431","ref_index":21,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Lifshitz-like Magnetic Black Branes: Third Law of Thermodynamics and the Null Energy Condition","primary_cat":"hep-th","submitted_at":"2026-04-09T16:34:05+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"In three Lifshitz-like black brane models, the null energy condition and third law of thermodynamics show no correlation in two cases but the former implies the latter in the third.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Anisotropic models are of particular inter- est, since QGP is a highly anisotropic medium in the early stages after its formation in heavy-ion collisions (HIC), occurring within 10 −24 s [1]. In such models, the AdS metric is modified by a warp factor and spatial anisotropy [3-20]. The early stages of HIC, as experiments suggest, show signs of a very strong magnetic field [21], which is incorporated via Maxwell fields in the gravity dual [7]. Another Maxwell field gives rise to the quark chemical potential [22, 23]. Holographic anisotropic setups are rich gravitational and thermodynamic systems in their own right and can be studied independently of their direct application to QGP phenomenology. Analyzing these anisotropic models is far from a purely abstract ex-"},{"citing_arxiv_id":"2604.06248","ref_index":11,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Relativistic Barnett effect and Curie law in a rigidly rotating free Fermi gas","primary_cat":"nucl-th","submitted_at":"2026-04-06T17:37:35+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"In a rigidly rotating free Fermi gas, the relativistic Barnett effect produces different Fermi energies for spin-up and spin-down fermions, leading to a moment of inertia that scales as 1/T at high temperature, analogous to the Curie law.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"In noncentral HICs, large mag- netic fields, ranging from1018-1020 Gauß, are generated byelectriccurrentsproducedfromtheacceleratedmotion of positively charged spectator nucleons that do not par- ticipate in the collision [7-10]. Additionally, large angu- lar momentum of the colliding nuclei results in extremely high global angular velocities, reaching up to1021 rad/s [11]. These extreme conditions significantly influence the early-time dynamics of the quark-gluon plasma (QGP) formed in these collisions. Beyond the well-known ef- fects of large magnetic fields, such as chiral magnetic effect [12, 13] and magnetic catalysis as well as inverse magnetic catalysis, that modify the phase diagram of quantum chromodynamics (QCD) [14-24], extreme ro-"},{"citing_arxiv_id":"2603.01061","ref_index":23,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"QCD phase transition at finite isospin density and magnetic field","primary_cat":"nucl-th","submitted_at":"2026-03-01T11:36:22+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"In the NJL model, increasing isospin chemical potential favors pion superfluidity at small magnetic fields and rho superconductivity at large magnetic fields.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2601.18354","ref_index":2,"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":41,"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":44,"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":"1907.03990","ref_index":27,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Effect of anomalous magnetic moment of quarks on the phase structure and mesonic properties in the NJL model","primary_cat":"nucl-th","submitted_at":"2019-07-09T05:30:43+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"In the two-flavor NJL model with anomalous magnetic moment of quarks, external magnetic field produces inverse magnetic catalysis and a magnetic-field-dependent drop in the Mott temperature for the Goldstone mode.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}