TY - JOUR
T1 - The CKM matrix and the unitarity triangle
T2 - Another look
AU - Buras, Andrzej J.
AU - Parodi, Fabrizio
AU - Stocchi, Achille
PY - 2003/1/1
Y1 - 2003/1/1
N2 - The unitarity triangle can be determined by means of two measurements of its sides or angles. Assuming the same relative errors on the angles (α, β, γ) and the sides (Rb, Rt), we find that the pairs (γ, β) and (γ, Rb) are most efficient in determining (scipt Q sign̄, η̄) that describe the apex of the unitarity triangle. They are followed by (α,β), (α, R b,), (Rt, β), (Rt, Rb) and (Rb, β)- As the set |Vus|, |Vcb|, R t and β appears to be the best candidate for the fundamental set of flavour violating parameters in the coming years, we show various constraints on the CKM matrix in the (Rt, β) plane. Using the best available input we determine the universal unitarity triangle for models with minimal flavour violation (MFV) and compare it with the one in the Standard Model. We present allowed ranges for sin 2/β, sin 2α, γ, Rb, Rt and ΔMs within the Standard Model and MFV models. We also update the allowed range for the function Ftt that parametrizes various MFV-models.
AB - The unitarity triangle can be determined by means of two measurements of its sides or angles. Assuming the same relative errors on the angles (α, β, γ) and the sides (Rb, Rt), we find that the pairs (γ, β) and (γ, Rb) are most efficient in determining (scipt Q sign̄, η̄) that describe the apex of the unitarity triangle. They are followed by (α,β), (α, R b,), (Rt, β), (Rt, Rb) and (Rb, β)- As the set |Vus|, |Vcb|, R t and β appears to be the best candidate for the fundamental set of flavour violating parameters in the coming years, we show various constraints on the CKM matrix in the (Rt, β) plane. Using the best available input we determine the universal unitarity triangle for models with minimal flavour violation (MFV) and compare it with the one in the Standard Model. We present allowed ranges for sin 2/β, sin 2α, γ, Rb, Rt and ΔMs within the Standard Model and MFV models. We also update the allowed range for the function Ftt that parametrizes various MFV-models.
KW - Heavy Quarks Physics
KW - Quark Masses and SM Parameters
KW - Weak Decays
UR - http://www.scopus.com/inward/record.url?scp=23044510896&partnerID=8YFLogxK
U2 - 10.1088/1126-6708/2003/01/029
DO - 10.1088/1126-6708/2003/01/029
M3 - Article
AN - SCOPUS:23044510896
SN - 1029-8479
VL - 7
SP - 635
EP - 657
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 1
ER -