Abstract

The Brightarrow pi pi ,pi K system offers a powerful laboratory to probe strong and weak interactions. Using the isospin symmetry, we determine hadronic Brightarrow pi pi parameters from data where new measurements of direct CP violation in B^0_drightarrow pi ^0pi ^0 resolve a discrete ambiguity. With the help of the SU(3) flavour symmetry, the Brightarrow pi pi parameters can be converted into their Brightarrow pi K counterparts, thereby allowing us to make predictions of observables. A particularly interesting decay is B^0_drightarrow pi ^0 K_mathrm{S} as it exhibits mixing-induced CP violation. Using an isospin relation, complemented with a robust SU(3) input, we calculate correlations between the direct and mixing-induced CP asymmetries of B^0_drightarrow pi ^0 K_mathrm{S}, which are the theoretically cleanest Brightarrow pi K probes. Interestingly, they show tensions with respect to the Standard Model. Should this Brightarrow pi K puzzle originate from New Physics, electroweak penguins offer an attractive scenario for new particles to enter. We present a strategy to determine the parameters characterising these topologies and obtain the state-of-the-art picture from current data. In the future, this method will allow us to reveal the Brightarrow pi K dynamics and to obtain insights into the electroweak penguin sector with unprecedented precision.

Highlights

  • Bd0 d Z, γ d d π0 d (d) Colour-suppressed EW penguin as colour-allowed tree amplitudes, contributing O(10%) to the decay amplitudes

  • New Physics (NP) contributions are associated with new sources of CP violation that can be probed through CPviolating observables

  • As we will demonstrate in this paper, the mixinginduced CP asymmetry of Bd0 → π 0 KS plays an outstanding role for testing the SM with the B → π K system

Read more

Summary

Amplitude structure

We focus on the B → π K system. The B+ → π + K 0 and Bd0 → π − K + amplitudes have only colour-suppressed EW penguins, while B+ → π 0 K + and Bd0 → π 0 K 0 have in addition contributions from colour-allowed EW penguin topologies. The EW penguin contributions are described by the following parameter [17,25]: qeiφ eiω ≡ − PEW + PECW ,. T + Cwhere φ and ω are CP-violating and CP-conserving phases, and PEW (T ) and PECW (C ) denote colour-allowed and colour-suppressed EW penguin (tree) amplitudes, respectively. We include the colour-suppressed EW penguin topologies through the parameters aC and aC as well as the CPconserving phases C and Cfor the Bd0 and B+ decays, respectively. Pt − Pc where Pu is a QCD penguin and A an annihilation amplitude This parameter can be determined through the U -spin symmetry of strong interactions from data for the B+ → K + K 0 decay [17,45]. Describe, in analogy to Eq (14), the colour-allowed and colour-suppressed tree-diagram contributions, respectively

Observables
Hadronic parameters
Determination of the hadronic parameters
Branching ratios
Colour-suppressed electroweak penguins
Direct CP asymmetries and sum rules
Vanishing CP violation in the electroweak penguin sector
Preliminaries
Discrete ambiguities
How to resolve the B → π K puzzle?
Utilizing mixing-induced CP violation in Bd0 → π 0 KS
Findings
Conclusions

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.