Domain-wall Skyrmion phase of QCD in magnetic field: Gauge field dynamics

Yuki Amari, Minoru Eto, Muneto Nitta
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Abstract

The ground state of QCD in sufficiently strong magnetic field at finite baryon density is an inhomogeneous state consisting of an array of solitons, called the chiral soliton lattice (CSL). It is, however, replaced in a region with higher density and/or magnetic field by the so-called domain-wall Skyrmion(DWSk) phase where Skyrmions are created on top of the CSL. This was previously proposed within the Bogomol'nyi-Prasad-Sommerfield (BPS) approximation neglecting a gauge field dynamics and taking into account its effect by a flux quantization condition. In this paper, by taking into account dynamics of the gauge field, we show that the phase boundary between the CSL and DWSk phases beyond the BPS approximation is identical to the one obtained in the BPS approximation. We also find that domain-wall Skyrmions are electrically charged with the charge one as a result of the chiral anomaly.
磁场中 QCD 的域壁 Skyrmion 相:量子场动力学
在有限重子密度下,QCD 在足够强的磁场中的基态是一种非均质态,由称为手性孤子晶格(CSL)的孤子阵列组成。然而,在密度和/或磁场较高的区域,它被所谓的畴壁天顶子(DWSk)相所取代,在 CSL 的顶部产生了天顶子。这是在 Bogomol'nyi-Prasad-Sommerfield (BPS) 近似中提出的,该近似忽略了量规场动力学,并通过通量量化条件考虑了量规场的影响。在本文中,通过考虑量子场动力学,我们证明了超越 BPS 近似的 CSL 和 DWSk 相之间的相界与 BPS 近似中得到的相界完全相同。我们还发现,由于手性反常现象,畴壁天幕带电,电荷量为 1。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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