Abstract
We present lattice QCD results for masses and magnetic polarizabilities of light and strange pseudoscalar mesons, chiral condensates, decay constants of neutral pion, and neutral kaon in the presence of background magnetic fields with $eB$ ranging up to around 3.35 GeV$^2$ ($\sim70~M_\pi^2$) in the vacuum. The computations were carried out in (2+1)-flavor QCD mostly on $32^3 \times 96$ lattices using the highly improved staggered quark action with $M_{\pi} \approx $ 220 MeV at zero temperature. We find that the masses of neutral pseudoscalar mesons monotonously decrease as the magnetic field strength grows and then saturate at a nonzero value, while there exists a nonmonotonous behavior of charged pion and kaon masses in the magnetic field. We observe a $qB$ scaling of the up and down quark flavor components of neutral pion mass, neutral pion decay constant as well as the quark chiral condensates at 0.05 $\lesssim eB\lesssim$ 3.35 GeV$^2$. We show that the correction to the Gell-Mann-Oakes-Renner relation involving the neutral pion is less than 6% and the correction for the relation involving neutral kaon is less than 30% at $eB\lesssim$ 3.35 GeV$^2$. We also derive the Ward-Takahashi identities for QCD in the magnetic field in the continuum formulation including the relation between integrated neutral pseudoscalar meson correlators and chiral condensates.
Highlights
The properties of strongly interacting matter in the external magnetic field have attracted many studies in recent years as strong magnetic fields appear in heavy-ion collisions [1,2,3], the early Universe [4], and magnetars [5]
It is found from lattice QCD studies using standard staggered fermions that the order parameter of the transition, the chiral condensate, increases with the magnetic field strength eB, which is so-called magnetic catalysis (MC) [6,7]
We focus on the chiral properties of QCD vacuum by studying the light and strange meson masses in the pseudoscalar channel, chiral condensates as well as the neutral pion and kaon decay constants related to the axial vector current in a wide range of magnetic field strength from 0 to ∼3.35 GeV2 in Nf 1⁄4 2 þ 1 QCD
Summary
The properties of strongly interacting matter in the external magnetic field have attracted many studies in recent years as strong magnetic fields appear in heavy-ion collisions [1,2,3], the early Universe [4], and magnetars [5]. We focus on the chiral properties of QCD vacuum by studying the light and strange meson masses in the pseudoscalar channel, chiral condensates as well as the neutral pion and kaon decay constants related to the axial vector current in a wide range of magnetic field strength from 0 to ∼3.35 GeV2 in Nf 1⁄4 2 þ 1 QCD. The lightest pseudoscalar mesons like pions are of particular interest as they are Goldstone bosons at the vanishing magnetic field Their masses are connected to the quark chiral condensate in the vacuum known as the Gell-Mann-Oakes-Renner relation [30].
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