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arXiv 2302.07288hep-ph
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机会性CP破坏

Opportunistic CP Violation

Quentin Bonnefoy, Emanuele Gendy, Christophe Grojean, Joshua T. Ruderman

AI总结:

本文在SMEFT框架下提出机会性CP破坏概念,通过1551个线性CP奇味不变量和Taylor秩方法刻画Wilson系数与Jarlskog不变量$J_4$的干涉,发现维度4的CP破坏在标准模型中偶然地小。

摘要:

在标准模型的电弱部分中,CP破坏通过三代夸克之间一种非常特殊的相互作用产生,正如Cabibbo–Kobayashi–Maskawa(CKM)机制和唯一的Jarlskog不变量$J_4$所描述的那样。一旦推广到标准模型有效场论(SMEFT),这种特殊的模式会被高维算符所修正,这些算符对应的Wilson系数通常被分为CP偶部分和CP奇部分。然而,在维度四,即在EFT展开的最低阶,CP破坏模糊了这一区分:任何Wilson系数都可以与$J_4$发生干涉并传递CP破坏。在本文中,我们在SMEFT展开的一阶,即$\mathcal{O}(1/Λ^2)$,研究这种干涉,并通过一组1551个线性CP奇味不变量来刻画其相关参数空间。这一构造既描述了新的、真正CP破坏的量,也描述了$J_4$与CP守恒量之间的干涉。我们将后一种可能性称为\textit{机会性CP破坏}。依靠将矩阵秩适当推广到Taylor展开——我们称之为\emph{Taylor秩}——我们定义了一个程序,根据不变量的大小来组织它们,以便在给定精度下只保留相关的不变量。我们探讨了当对SMEFT系数的味结构作出不同假设时,这种刻画如何变化。有趣的是,一些CP奇不变量即使捕捉到机会性CPV,其受抑制程度也比$J_4$更小,这表明标准模型中的CP破坏在维度4是\textit{偶然地小。}

英文摘要:

In the electroweak sector of the Standard Model, CP violation arises through a very particular interplay between the three quark generations, as described by the Cabibbo--Kobayashi--Maskawa (CKM) mechanism and the single Jarlskog invariant $J_4$. Once generalized to the Standard Model Effective Field Theory (SMEFT), this peculiar pattern gets modified by higher-dimensional operators, whose associated Wilson coefficients are usually split into CP-even and odd parts. However, CP violation at dimension four, i.e., at the lowest order in the EFT expansion, blurs this distinction: any Wilson coefficient can interfere with $J_4$ and mediate CP violation. In this paper, we study such interferences at first order in the SMEFT expansion, $\mathcal{O}(1/Λ^2)$, and we capture their associated parameter space via a set of 1551 linear CP-odd flavor invariants. This construction describes both new, genuinely CP-violating quantities as well as the interference between $J_4$ and CP-conserving ones. We call this latter possibility \textit{opportunistic CP violation}. Relying on an appropriate extension of the matrix rank to Taylor expansions, which we dub \emph{Taylor rank}, we define a procedure to organize the invariants in terms of their magnitude, so as to retain only the relevant ones at a given precision. We explore how this characterization changes when different assumptions are made on the flavor structure of the SMEFT coefficients. Interestingly, some of the CP-odd invariants turn out to be less suppressed than $J_4$, even when they capture opportunistic CPV, demonstrating that CP-violation in the SM, at dimension 4, is \textit{accidentally small.}

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