论文标题

CP侵入运算符的短流动时间系数

Short flow-time coefficients of CP-violating operators

论文作者

Rizik, Matthew D., Monahan, Christopher J., Shindler, Andrea

论文摘要

永久性中子电偶极矩(EDM)的测量可能是标准模型(BSM)源的探测源。在低能量下,CP侵略BSM相互作用是通过高于四个的尺寸的cp侵入式操作员来参数化的。这些操作员的核子矩阵元素的QCD计算需要完全重建对核子EDM的不同CP侵略贡献的源和大小。本文中,我们研究了夸克 - 奇罗莫电动偶极矩(QCEDM)操作员和三纤维Weinberg操作员。使用晶状体QCD的非扰动测定对这些CP侵略算子的核子基质元件的短距离行为阻碍了这些核子基质元素。在重新规定下,这些操作员与较低维操作员混合在一起,该操作员在接近连续性限制时会诱导晶格间距中的功率差异。我们使用梯度流研究了QCEDM和Weinberg操作员的短途行为。我们执行短流动时间的扩展,并在扰动理论中确定源于与拟尺度密度和拓扑电荷的呈线性发散术语的扩展系数,从而证实了操作员产品扩展的期望。我们引入了一种新方法,以在非零流动时进行计算,以实现外部动量的任意值。这种方法使我们可以在本文中描述的大多数计算中在四个维度上工作,从而避免了与定义$γ_5$在通用d维度中的并发症相关的并发症。我们表明,可以使用't Hooft-Veltman-Breitenlohner-Maison-Maison方案定义$γ_5$来复制外部动量的主要贡献。

Measurements of a permanent neutron electric dipole moment (EDM) potentially probe Beyond-the-Standard Model (BSM) sources of CP-violation. At low energy the CP-violating BSM interactions are parametrized by flavor-conserving CP-violating operators of dimension higher than four. QCD calculations of the nucleon matrix elements of these operators are required to fully reconstruct the sources and magnitudes of the different CP-violating contributions to the nucleon EDM. Herein we study the quark-chromo electric dipole moment (qCEDM) operator and the three-gluon Weinberg operator. The non-perturbative determination, using lattice QCD, of the nucleon matrix elements of these CP-violating operators is hampered by their short-distance behavior. Under renormalization these operators mix with lower dimensional operators, which induces power divergences in the lattice spacing, as the continuum limit is approached. We study the short-distance behavior of the qCEDM and the Weinberg operators using the gradient flow. We perform a short flow time expansion and determine, in perturbation theory, the expansion coefficients of the linearly-divergent terms stemming from the mixing with the pseudoscalar density and the topological charge, confirming the expectations of the operator product expansion. We introduce a new method to perform calculations at non-zero flow-time for arbitrary values of the external momenta. This method allows us to work in four dimensions for most of the calculations described in this paper, avoiding the complications associated with defining $γ_5$ in generic d dimensions. We show that leading contributions in the external momenta can be reproduced by defining $γ_5$ using the 't Hooft-Veltman-Breitenlohner-Maison scheme.

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