TY - JOUR
T1 - Bounds on the unitarity triangle, sin 2β and K → πνν̄ decays in models with minimal flavor violation
AU - Buras, Andrzej J.
AU - Fleischer, Robert
PY - 2001/12/1
Y1 - 2001/12/1
N2 - We present a general discussion of the unitarity triangle from εK, ΔMd,s and K → πνν̄ in models with minimal flavor violation (MFV), allowing for arbitrary signs of the generalized Inami-Lim functions Ftt and X relevant for (εK,ΔMd,s) and K → πνν̄, respectively. In the models in which Ftt has a sign opposite to the one in the standard model, i.e. Ftt<0, the data for (εK,ΔMd,s) imply an absolute lower bound on the Bd → ψKS CP asymmetry aψKS of 0.69, which is substantially stronger than 0.42 arising in the case of Ftt>0. An important finding of this paper is the observation that forgiven Br(K+ → π+νν̄) and aψKS only two values for Br (KL → π0νν̄), 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(KL → π0νν̄) as functions of Br(K+ → π+νν̄). Using the present experimental upper bounds on Br(K+ → π+νν̄) and |Vub/Vcb|, we obtain the absolute upper bound Br(KL → π0νν̄)<7.1×10-10 (90% C.L.).
AB - We present a general discussion of the unitarity triangle from εK, ΔMd,s and K → πνν̄ in models with minimal flavor violation (MFV), allowing for arbitrary signs of the generalized Inami-Lim functions Ftt and X relevant for (εK,ΔMd,s) and K → πνν̄, respectively. In the models in which Ftt has a sign opposite to the one in the standard model, i.e. Ftt<0, the data for (εK,ΔMd,s) imply an absolute lower bound on the Bd → ψKS CP asymmetry aψKS of 0.69, which is substantially stronger than 0.42 arising in the case of Ftt>0. An important finding of this paper is the observation that forgiven Br(K+ → π+νν̄) and aψKS only two values for Br (KL → π0νν̄), 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(KL → π0νν̄) as functions of Br(K+ → π+νν̄). Using the present experimental upper bounds on Br(K+ → π+νν̄) and |Vub/Vcb|, we obtain the absolute upper bound Br(KL → π0νν̄)<7.1×10-10 (90% C.L.).
UR - http://www.scopus.com/inward/record.url?scp=0035581023&partnerID=8YFLogxK
U2 - 10.1103/PhysRevD.64.115010
DO - 10.1103/PhysRevD.64.115010
M3 - Article
AN - SCOPUS:0035581023
SN - 0556-2821
VL - 64
JO - Physical Review D
JF - Physical Review D
IS - 11
M1 - 115010
ER -