Bounds on the Unitarity Triangle, $\sin 2β$ and $K\toπν\barν$ Decays in Models with Minimal Flavour Violation

Details Bounds on the Unitarity Triangle, $\sin 2β$ and $K\toπν\barν$ Decays in Models with Minimal Flavour Violation Bounds on the Unitarity Triangle, $\sin 2β$ and $K\toπν\barν$ Decays in Models with Minimal Flavour Violation

2001-04-24

arxiv.org/abs/hep-ph/0104238v2

Phys.Rev. D64 (2001) 115010

Physics

High Energy Physics

High Energy Physics - Phenomenology

25 pages, LaTeX, 4 figures. Few comments and one figure in view of new B-factory results added, conclusions unchanged

Scientific paper

We present a general discussion of the unitarity triangle from $\epsilon_K$, $\Delta M_{d,s}$ and $K \to \pi\nu\overline{\nu}$ in models with minimal flavour violation (MFV), allowing for arbitrary signs of the generalized Inami--Lim functions $F_{tt}$ and $X$ relevant for $(\epsilon_K,\Delta M_{d,s})$ and $K \to \pi\nu\overline{\nu}$, respectively. In the models in which $F_{tt}$ has a sign opposite to the one in the Standard Model, i.e. $F_{tt}<0$, the data for $(\epsilon_K, \Delta M_{d,s})$ imply an absolute lower bound on the $B_d\to\psi K_{S}$ CP asymmetry $a_{\psi K_S}$ of 0.69, which is substantially stronger than 0.42 arising in the case of $F_{tt}>0$. An important finding of this paper is the observation that for given $Br(K^+\to\pi^+\nu\overline{\nu})$ and $a_{\psi K_S}$ only two values for $Br(K_{L}\to\pi^0\nu\overline{\nu})$, corresponding to the two signs of $X$, are possible in the full class of MFV models, independently of any new parameters arising in these models. This provides a powerful test for this class of models. Moreover, we derive absolute lower and upper bounds on $Br(K_{L}\to\pi^0\nu\overline{\nu})$ as functions of $Br(K^+\to\pi^+\nu\overline{\nu})$. Using the present experimental upper bounds on $Br(K^+\to\pi^+\nu\overline{\nu})$ and $|V_{ub}/V_{cb}|$, we obtain the absolute upper bound $Br(K_{L}\to\pi^0\nu\overline{\nu})< 7.1 \cdot 10^{-10}$ (90% C.L.).

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