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Spontaneous Symmetry Breaking for Scalar QED with Non-minimal Chern-Simons Coupling

机译:非最小Chern-Simons耦合的标量QED自发对称性破裂

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摘要

We investigate the two-loop effective potential for both minimally and non-minimally coupled Maxwell-Chern-Simons theories. The non-minimal gauge interaction represents the magnetic moment interaction between a charged scalar and the electromagnetic field. In a previous paper we have shown that the two loop effective potential for this model is renormalizable with an appropriate choice of the non-minimal coupling constant. We carry out a detailed analysis of the spontaneous symmetry breaking induced by radiative corrections. As long as the renormalization point for all couplings is chosen to be the true minimum of the effective potential, both models predict the presence of spontaneous symmetry breaking. Two loop corrections are small compared to the one loop result, and thus the symmetry breaking is perturbatively stable.
机译:我们研究了最小和非最小耦合麦克斯韦-切尔-西蒙斯理论的两环有效势。非最小轨距相互作用表示带电标量和电磁场之间的磁矩相互作用。在先前的论文中,我们显示了该模型的两个回路有效电势可以通过适当选择非最小耦合常数来重新规范化。我们对辐射修正引起的自发对称性破坏进行了详细分析。只要将所有耦合的重归一化点选择为有效电位的真正最小值,两个模型都将预测自发对称破坏的存在。与一个循环的结果相比,两个循环的校正量较小,因此对称性破坏是稳定的。

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