Abstract
The angular distribution of \({\varLambda }^{0}_{{b} } \rightarrow \varLambda {\mu }^{+}{\mu }^{-} \) decays can be described as a function of three angles and \({q}^{2}\) when neglecting the production polarisation of the \({\varLambda }^{0}_{{b} }\). The two angles that are relevant for the analysis in this chapter and are defined in Fig. 4.1: \(\theta _\ell \) is the angle between the positive (negative) muon direction in the dimuon rest frame and the dimuon system direction in the \({\varLambda }^{0}_{{b} }\) (\({\overline{\varLambda }}^{0}_{{b} }\)) rest frame; similarly, \(\theta _h\) is defined as the angle between the proton and the \(\varLambda \) baryon directions, in the \(\varLambda \) and \({\varLambda }^{0}_{{b} }\) rest frames.
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Pescatore, L. (2017). Angular Analysis of \({\varLambda }^{0}_{{b} } \rightarrow \varLambda {\mu }^{+}{\mu }^{-} \) Decays. In: Searching for New Physics in b → sℓ+ℓ− Transitions at the LHCb Experiment. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-319-66423-1_4
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