${\mu }^{-}{\mu }^{+}\to {\nu }_{\mu }{\bar{\nu }}_{\mu }t\bar{t}H$ amplitudes in the Feynman-diagram gauge

Abstract

We study the process ${\mu }^{-}{\mu }^{+}\to {\nu }_{\mu }{\bar{\nu }}_{\mu }t\bar{t}H$ with complex CP violating $ttH$ couplings in the SMEFT with a dimension-6 operator. When the amplitudes are expressed in the Feynman-Diagram gauge, the dominance of the total cross section via the weak boson fusion diagrams is manifest. The high energy behaviour is dictated by the higher-dimensional vertices in the dimension-6 SMEFT operator. These properties are not manifest in the unitary gauge because of subtle cancellation among diagrams.

arXiv comment4 pages, 2 figures; Contribution to the proceedings of International Workshop on Future Linear Colliders (LCWS2024), University of Tokyo, Japan

References in corpus (4)

• The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations
• Electroweak Splitting Functions and High Energy Showering
• An Equivalent Gauge and the Equivalence Theorem
• QED and QCD helicity amplitudes in parton-shower gauge