Isospin analysis of charmless B-meson decays

Abstract We discuss the determination of the CKM angle $$\alpha $$ α using the non-leptonic two-body decays $$B\rightarrow \pi \pi $$ B → π π , $$B\rightarrow \rho \rho $$ B → ρ ρ and $$B\rightarrow \rho \pi $$ B → ρ π using the latest data available. We illustrate the methods used in each case and...

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Bibliographic Details
Main Authors: J. Charles, O. Deschamps, S. Descotes-Genon, V. Niess
Format: Article
Language:English
Published: SpringerOpen 2017-08-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-017-5126-9
Description
Summary:Abstract We discuss the determination of the CKM angle $$\alpha $$ α using the non-leptonic two-body decays $$B\rightarrow \pi \pi $$ B → π π , $$B\rightarrow \rho \rho $$ B → ρ ρ and $$B\rightarrow \rho \pi $$ B → ρ π using the latest data available. We illustrate the methods used in each case and extract the corresponding value of $$\alpha $$ α . Combining all these elements, we obtain the determination $$\alpha _\mathrm{dir}={({86.2}_{-4.0}^{+4.4} \cup {178.4}_{-5.1}^{+3.9})}^{\circ }$$ α dir = ( 86.2 - 4.0 + 4.4 ∪ 178.4 - 5.1 + 3.9 ) ∘ . We assess the uncertainties associated to the breakdown of the isospin hypothesis and the choice of the statistical framework in detail. We also determine the hadronic amplitudes (tree and penguin) describing the QCD dynamics involved in these decays, briefly comparing our results with theoretical expectations. For each observable of interest in the $$B\rightarrow \pi \pi $$ B → π π , $$B\rightarrow \rho \rho $$ B → ρ ρ and $$B\rightarrow \rho \pi $$ B → ρ π systems, we perform an indirect determination based on the constraints from all the other observables available and we discuss the compatibility between indirect and direct determinations. Finally, we review the impact of future improved measurements on the determination of $$\alpha $$ α .
ISSN:1434-6044
1434-6052