2018
DOI: 10.1007/jhep11(2018)186
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Tensor polarizability of the vector mesons from SU(3) lattice gauge theory

Abstract: The magnetic dipole polarizabilities of the vector ρ 0 and ρ ± mesons in SU (3) pure gauge theory are calculated in the article. Based on this the authors explore the contribution of the dipole magnetic polarizabilities to the tensor polarization of the vector mesons in external abelian magnetic field. The tensor polarization leads to the dilepton asymmetry observed in non-central heavy ion collisions and can be also estimated in lattice gauge theory.

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Cited by 9 publications
(4 citation statements)
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“…For instance, it contains the contribution of the intermediate π þ π − mesons or the ρ meson peak which has a large spectral weight in the confined phase [12]. It is reasonable to expect that the external magnetic field modifies the spectral function, for instance through the light meson masses modification [55][56][57][58]. Thus, in order to check the presence of CME in the confined phase one has to separate the contribution to the spectral function due to the conductivity, ω ∼ 0, from the contribution of the light mesons ω ∼ 2m π ; m ρ ; ….…”
Section: Discussionmentioning
confidence: 99%
“…For instance, it contains the contribution of the intermediate π þ π − mesons or the ρ meson peak which has a large spectral weight in the confined phase [12]. It is reasonable to expect that the external magnetic field modifies the spectral function, for instance through the light meson masses modification [55][56][57][58]. Thus, in order to check the presence of CME in the confined phase one has to separate the contribution to the spectral function due to the conductivity, ω ∼ 0, from the contribution of the light mesons ω ∼ 2m π ; m ρ ; ….…”
Section: Discussionmentioning
confidence: 99%
“…The calculation of hadron masses is a strong area of lattice QCD. The mass shifts in the magnetic fields were investigated for many hadrons: pseudo-scalar mesons [10,11,12,13,14,15,16,17], vector mesons [11,12,13,15,18,19], and nucleons [20,21,22]. The calculation is straightforward in most cases.…”
Section: Hadron Propertymentioning
confidence: 99%
“…The electromagnetic structure of hadrons has been the target of LQCD investigations since the 1980s; the first LQCD computations of the nucleon's response to uniform magnetic fields were performed in the quenched approximation, starting with calculations of the nucleon magnetic moments [204,205,475,476], and more recently extending to other baryons in the baryon octet [477] and decuplet [478,479]. A series of subsequent calculations were able to extract not only magnetic moments, but also polarizabilities, for several members of the lowest-lying baryon and meson octets [480][481][482][483][484][485][486][487][488][489][490][491][492][493][494]. Computations of EM properties involving more than one hadron have only been achieved recently, with the first calculation of the leading contribution to the magnetic-field response of s-shell nuclei being presented in Ref.…”
Section: Electromagnetic Interactions Of Light Nucleimentioning
confidence: 99%