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
Summary
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
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