Search for B0 decays to invisible final states and to νν̄γ
Physical Review Letters 93:9 (2004)
Abstract:
The disappearance decays of B0 mesons, where the B0 decay contains no observable final state particles or invisible decay products with a single photon, was investigated. The decays have branching fractions below the experimental sensitivity and physics models are used to predict significant contributions from these channels. The limits on branching fractions for B0 decays to an invisible final state and for B0 decays to vv̄y branching fractions.Bound on the ratio of decay amplitudes for B̄0 → J/ψK*0 and B0 → J/ψK*0
Physical Review Letters 93:8 (2004)
Abstract:
The time-dependent decay rate for the process B→J/ψK *(892) in γ(4S)→BB̄ decays detected by BABAR detector, was investigated. The flavor-tagged events, where one neutral B meson was reconstructed in the J/ψK*0 or J/ψK̄ *0 final state, were observed. The coefficients of cosine and sine terms in time-dependent asymmetries were also measured. The results show that for a single ratio of wrong-flavor to favored amplitudes for B0 and ̄0 combined, an upper limit of 0.25 at 90% confidence level (C.L.) was obtained.Measurement of the B → XS ℓ+ℓ branching fraction with a sum over exclusive modes
Physical Review Letters 93:8 (2004)
Abstract:
The measurement of branching fraction for flavor-changing neutral-current process B→XSl+l-, was described. The final state was reconstructed from e+e- or μ+μ- pairs and hadronic system XS, which consists of one K∓ or KS0 and two pions. The systematic uncertainties in signal yield were also evaluated by varying signal gaussian parameters and signal shape. The results show that ratio between generator yield for decay modes which contain KS0 and modes containing a charged kaon was varied within range 0.50∓0.05, allows isospin violation.B meson decays to η(′) K*, η (′) ρ, η(′) π0, ωπ0, and φπ0
Physical Review D - Particles, Fields, Gravitation and Cosmology 70:3 (2004)
Abstract:
We present measurements of the branching fractions and charge asymmetries (where appropriate) of two-body B decays to η(′) K*, η(′) ρ, η(′) π0, ωπ0, and φπ0. The data were recorded with the BABAR detector at PEP-II and correspond to 89×106 BB pairs produced in e +e- annihilation through the Υ (4S) resonance. We find significant signals for two decay modes and measure the branching fractions B(B+→ηK*+)=(25.6 ±4.0±2.4) ×10-6 and B(B0→ηK*0) = (18.6±23±1.2)×10-6, where the first error is statistical and the second systematic. We also find evidence with significance 3,5σ for a third decay mode and measure B(B+ →ηρ+)=(9.2±3.4±1.0)×10 -6. For other channels, we set 90% C.L. upper limits of B(B 0→ηρ0)<1.5 ×10-6, B(B+→η′K*+)<14×10 -6, B(B0→η′K*0)<7. 6×10-6, B(B0→η′K*0) <22×10-6, B(B0 →η′ρ 0)<4.3×10-6, B(B0→ηπ 0)<2.5×10-6, B(B0→η′ π0)<3.7×10-6, B(B0→ωπ 0)<1.2×10-6, and B(B0→φπ 0)<1.0×10-6. For self-flavor-tagging modes with significant signals, the time-integrated charge asymmetries are A ch(ηK*+)=+0.13±0.14±0.02 and Ach(ηK*0)=+0.02±0.11±0.02.Measurement of the time-dependent CP asymmetry in the B0 → φK0 Decay
Physical Review Letters 93:7 (2004)