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arXiv 2501.09062hep-phhep-th
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从无质量振幅与在壳质量插入出发的大质量螺旋度-手性旋量形式

Massive Helicity-Chirality Spinor Formalism from Massless Amplitudes with On-shell Mass Insertion

Yu-Han Ni, Yi-Ning Wang, Chao Wu, Jiang-Hao Yu

AI总结:

本文提出大质量螺旋度-手性旋量形式,通过在壳质量插入刻画螺旋度与手性翻转,建立大质量振幅与无质量振幅(含 Higgs 插入)的紫外-红外对应,并用于解释弱衰变质量增强及构造高点多点振幅。

摘要:

我们引入一种螺旋度-手性旋量形式,用于描述任意质量和自旋粒子的散射振幅。Arkani-hamed-Huang-Huang 引入的大质量自旋-旋量被推广为自旋/螺旋度-横性旋量,其中通过扩展庞加莱对称性引入了一个与手性密切相关的新量子数——横性。大质量螺旋度-手性振幅可以按照 $\lambda\sim \sqrt{E}, \eta\sim \mathbf{m}/\sqrt{E}$ 的展开逐阶用无质量旋量 $\lambda$ 和 $\eta$ 的大、小分量写出,从而建立大能量有效理论的功率计数规则。在图形上,振幅中的质量展开源于在壳质量插入:螺旋度翻转和手性翻转,这完全决定了三点大质量振幅。从紫外区的手性-螺旋度统一出发,任何大质量螺旋度-手性振幅都可以与带有(或不带有)额外 Higgs 插入的无质量螺旋度振幅一一对应。这种紫外-红外对应解释了弱衰变过程 $π^+ \to μ^+ ν$ 和 $t \to W^+ b$ 中的质量增强,并分离出 Arkani-hamed-Huang-Huang 形式中三点大质量 QED $F\bar{F}γ$ 振幅的正确紫外来源。基于无质量-大质量对应,无质量在壳技术可用于构造更高点的大质量振幅。

英文摘要:

We introduce a helicity-chirality spinor formalism to describe scattering amplitudes for particles of any masses and spins. The massive spin-spinors introduced by Arkani-hamed-Huang-Huang have been extended to the spin/helicity-transversality spinors, in which a new quantum number transversality, closely related to chirality, is introduced by extending the Poincare symmetry. The massive helicity-chirality amplitudes can be written by the large and small components of massless spinors $λ$ and $η$ following the $λ\sim \sqrt{E}, η\sim \mathbf{m}/\sqrt{E}$ expansion order by order, which formulate the power counting rules of a large energy effective theory. Diagrammatically the mass expansion in amplitudes originates from the on-shell mass insertion: the helicity flip and chirality flip, which completely determines the three-point massive amplitudes. From the chirality-helicity unification at the UV, any massive helicity-chirality amplitude can be one-to-one corresponded to massless helicity amplitudes with (without) additional Higgs insertion. This UV-IR correspondence explains the mass enhancement in the weak decay processes $π^+ \to μ^+ ν$ and $t \to W^+ b$, and isolates the correct UV of the three-point massive QED $F\bar{F}γ$ amplitudes in Arkani-hamed-Huang-Huang formalism. From massless-massive correspondence, the massless on-shell techniques can be utilized to construct higher-point massive amplitudes.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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