Key points are not available for this paper at this time.
In the Standard Model effective field theory (SMEFT), the SU(2)L×U(1)Y symmetry of the Standard Model is linearly realized. However, it is possible that more general effective field theories, such as the Higgs effective field theory (HEFT) where this symmetry is realized nonlinearly, are needed to describe the data. Identifying physics beyond SMEFT could shed light on the nature of Higgs and the realization of the electroweak symmetry. We explore the possibility of such an identification by studying the effects of scalar and vector new physics operators on the angular distribution of Λb→Λc(→Λπ)τν¯τ. This decay is sensitive to the six-dimensional effective operator OVLR≡(τ¯γμPLντ)(c¯γμPRb), which is present in HEFT but suppressed in SMEFT. We identify the angular observables that can have significant contributions from OVLR and hence would be useful for probing not only beyond the Standard Model physics but also physics beyond SMEFT. We further find that constraining the branching ratio of Bc→τν¯τ would be crucial for performing this task. Published by the American Physical Society 2024
Karmakar et al. (Mon,) studied this question.