论文标题

带有HISQ Fermions的外部磁场中的介子质量

Meson masses in external magnetic fields with HISQ fermions

论文作者

Ding, Heng-Tong, Li, Sheng-Tai, Mukherjee, Swagato, Tomiya, Akio, Wang, Xiao-Dan

论文摘要

我们研究了在零温度下存在外部磁场的情况下,在(2+1) - 含有QCD的伪量表中的介体的时间相关函数。模拟使用高度改进的交错夸克(HISQ)操作以$ 32^3 \ times 96 $晶格进行,以$M_π\ $ 230 MEV进行。磁场的强度$ | eb | $从0到3.3 GEV $^2 $($ \ sim 60m_π^2 $)。我们发现中性伪量表颗粒的质量,例如随着磁场的生长,单调呈中性锥子和kaon,单调降低,然后以非零值饱和。观察到,较重的中性伪量表受磁场的影响较小。此外,我们首次发现了带电亲和kaon质量的非单调行为。对于小磁场(0 $ \ \ leq〜 | eb | \ Lessim $ 0.3 GEV $^2〜 \ sim6m_π^2 $),充电的伪盘质量会随着磁场而生长,并且可以通过最低的Landau级别近似,而对于$ | EB | EB | $ | $ | $ | $ | $ | $ | $ | $ | $ |大于0.3 Gev $^$^2 $^2 $ the Mass saste sarte。讨论了$ | eb | $依赖中性亲质量与磁场中伪临界温度的降低行为之间的可能联系。由于中性胎质质量的非零值,我们的模拟表明QCD的超导阶段在磁场的当前窗口中不存在。

We studied the temporal correlation function of mesons in the pseudo-scalar channel in (2+1)-flavor QCD in the presence of external magnetic fields at zero temperature. The simulations were performed on $32^3 \times 96$ lattices using the Highly Improved Staggered Quarks (HISQ) action with $m_π \approx $ 230 MeV. The strength of magnetic fields $|eB|$ ranges from 0 to around 3.3 GeV$^2$ ($\sim 60 m_π^2$). We found that the masses of neutral pseudo-scalar particles, e.g. neutral pion and kaon, monotonouslly decrease as the magnetic field grows and then saturate at a nonzero value. It is observed that heavier neutral pseudo-scalars are less affected by magnetic fields. Moreover, we found a non-monotonous behavior of charged pion and kaon mass in magnetic field for the first time. In the case of small magnetic field (0 $\leq~|eB| \lesssim$ 0.3 GeV$^2~\sim 6m_π^2$ ) the mass of charged pseudo-scalar grows with magnetic field and can be well described by the Lowest Landau Level approximation, while for $|eB|$ larger than 0.3 GeV$^2$ the mass starts to decrease. The possible connection between $|eB|$ dependences of neutral pion mass and the decreasing behavior of pseudo-critical temperature in magnetic field is discussed. Due to the nonzero value of neutral pion mass our simulation indicates that the superconducting phase of QCD does not exist in the current window of magnetic field.

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