TY - JOUR
T1 - B-Meson decay, CPviolation, mixing angles and the top quark mass
AU - Buras, A. J.
AU - Słominski, W.
AU - Steger, H.
PY - 1984/6/18
Y1 - 1984/6/18
N2 - We find the domain of the values of mt, τB and R (the top quark mass, the B-meson lifetime and γ(b → u)/γ(b → c) respectively) for which the standard six-quark model is consistent with the observed CP violation in the kaon system and with the recent experimental results for B-meson decays. The mixing angles θ2, θ3, the phase δ and the ratio ε{lunate}′/ε{lunate} are calculated as functions of mt, τB and R. The sensitivity of the analysis to the variation of the "bag" parameter B and the b- and c-quark masses is investigated. Two types of calculations are presented: one which takes into account the KL-KS mass difference and the other one which ignores it. We discuss the implications of a possible discovery of a top quark with mt below 30 GeV and we point out that for B ≤ 1 3 and mt ≈ O(25 GeV) a simultaneous consistency of the standard model with the data for τB, R, ε{lunate} and ε{lunate}′/ε{lunate} cannot be achieved. Furthermore for B ≤ 2 3 and mt ≤ 35 GeV we find ε{lunate}′/ε{lunate} ≥ 0.01. No interesting upper bound on mt follows from KL → μμ.
AB - We find the domain of the values of mt, τB and R (the top quark mass, the B-meson lifetime and γ(b → u)/γ(b → c) respectively) for which the standard six-quark model is consistent with the observed CP violation in the kaon system and with the recent experimental results for B-meson decays. The mixing angles θ2, θ3, the phase δ and the ratio ε{lunate}′/ε{lunate} are calculated as functions of mt, τB and R. The sensitivity of the analysis to the variation of the "bag" parameter B and the b- and c-quark masses is investigated. Two types of calculations are presented: one which takes into account the KL-KS mass difference and the other one which ignores it. We discuss the implications of a possible discovery of a top quark with mt below 30 GeV and we point out that for B ≤ 1 3 and mt ≈ O(25 GeV) a simultaneous consistency of the standard model with the data for τB, R, ε{lunate} and ε{lunate}′/ε{lunate} cannot be achieved. Furthermore for B ≤ 2 3 and mt ≤ 35 GeV we find ε{lunate}′/ε{lunate} ≥ 0.01. No interesting upper bound on mt follows from KL → μμ.
UR - http://www.scopus.com/inward/record.url?scp=33744731685&partnerID=8YFLogxK
U2 - 10.1016/0550-3213(84)90334-1
DO - 10.1016/0550-3213(84)90334-1
M3 - Article
AN - SCOPUS:33744731685
SN - 0550-3213
VL - 238
SP - 529
EP - 560
JO - Nuclear Physics, Section B
JF - Nuclear Physics, Section B
IS - 3
ER -