{ "id": "2209.01872", "version": "v1", "published": "2022-09-05T10:10:09.000Z", "updated": "2022-09-05T10:10:09.000Z", "title": "Mass splitting and spin alignment for $φ$ mesons in a magnetic field in NJL model", "authors": [ "Xin-Li Sheng", "Shu-Yun Yang", "Yao-Lin Zou", "Defu Hou" ], "comment": "11 pages, 8 figures", "categories": [ "nucl-th", "hep-ph" ], "abstract": "Based on the Nambu-Jona-Lasinio (NJL) model, we develop a framework for calculating the spin alignment of vector mesons and applied it to study $\\phi$ mesons in a magnetic field. We calculate mass spectra for $\\phi$ mesons and observe mass splitting between the longitudinally polarized state and the transversely polarized state. The $\\phi$ meson in a thermal equilibrium system is preferred to occupy the state with spin $\\lambda=0$ than those with spin $\\lambda=\\pm1$, because the former state has smaller energy. As a consequence, we conclude that the spin alignment will be larger than 1/3 if one measures along the direction of the magnetic field, which is qualitatively consistent with the recent STAR data. Around the critical temperature $T_{C}=150$ MeV, the positive deviation from 1/3 is proportional to the square of the magnetic field strength, which agrees with the result from the non-relativistic coalescence model. Including the anomalous magnetic moments for quarks will modify the dynamical masses of quarks and thus influence the mass spectra and spin alignment of $\\phi$ mesons. The discussion of spin alignment in the NJL model may help us better understand the formation of hadron's spin structure during the chiral phase transition.", "revisions": [ { "version": "v1", "updated": "2022-09-05T10:10:09.000Z" } ], "analyses": { "keywords": [ "spin alignment", "njl model", "mass splitting", "mass spectra", "hadrons spin structure" ], "note": { "typesetting": "TeX", "pages": 11, "language": "en", "license": "arXiv", "status": "editable" } } }