{"paper":{"title":"$J/\\psi$ and $\\eta_c$ in asymmetric hot magnetized nuclear matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Arvind Kumar, Rajesh Kumar","submitted_at":"2018-10-22T11:37:16Z","abstract_excerpt":"We investigate the mass-shift of vector channel $J/\\psi$ and pseudoscalar channel $\\eta_c$ in strongly magnetized asymmetric nuclear medium at finite temperature using the conjunction of chiral $SU(3)$ model with the QCD sum rules. The magnetic field dependence of scalar gluon condensate $\\left\\langle \\frac{\\alpha_{s}}{\\pi} G^a_{\\mu\\nu} {G^a}^{\\mu\\nu} \\right\\rangle$ as well as the twist-2 gluon condensate $\\left\\langle \\frac{\\alpha_{s}}{\\pi} G^a_{\\mu\\sigma} {{G^a}_\\nu}^{\\sigma} \\right\\rangle $ calculated from chiral SU($3$) model, are implemented in QCD sum rules to calculate the magnetic fiel"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.09185","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}