The measurable angular distribution of decay
arXiv:2011.05912 · doi:10.1007/JHEP02(2021)183
Abstract
In decay, the solid angle of the final-state particle cannot be determined precisely since the decay products of the include an undetected . Therefore, the angular distribution of this decay cannot be measured. In this work, we construct a {\it measurable} angular distribution by considering the subsequent decay . The full cascade decay is . The three-momenta of the final-state particles , , and can be measured. Considering all Lorentz structures of the new physics (NP) effective operators and an unpolarized initial state, the five-fold differential angular distribution can be expressed in terms of ten angular observables . By integrating over some of the five kinematic parameters, we define a number of observables, such as the spin polarization and the forward-backward asymmetry of meson , both of which can be represented by the angular observables . We provide numerical results for the entire set of the angular observables and both within the Standard Model and in some NP scenarios, which are a variety of best-fit solutions in seven different NP hypotheses. We find that the NP which can resolve the anomalies in decays has obvious effects on the angular observables , except and .
36 pages, 2 figures, 5 tables, matches to the version published in JHEP
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- Time-reversal asymmetries in semileptonic decays
- decays with visible final-state kinematics
- An Imperative study of the angular observables in decay and probing the footprint of new physics
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