B meson decays to η(′) K*, η (′) ρ, η(′) π0, ωπ0, and φπ0

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) r...

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Main Authors: Aubert, B, Barate, R, Boutigny, D, Couderc, F, Gaillard, J, Hicheur, A, Karyotakis, Y, Lees, J, Tisserand, V, Zghiche, A, Palano, A, Pompili, A, Chen, J, Qi, N, Rong, G, Wang, P, Zhu, Y, Eigen, G, Ofte, I, Stugu, B, Abrams, G, Borgland, A, Breon, AB, Brown, D, Button-Shafer, J
Format: Journal article
Language:English
Published: 2004
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author Aubert, B
Barate, R
Boutigny, D
Couderc, F
Gaillard, J
Hicheur, A
Karyotakis, Y
Lees, J
Tisserand, V
Zghiche, A
Palano, A
Pompili, A
Chen, J
Qi, N
Rong, G
Wang, P
Zhu, Y
Eigen, G
Ofte, I
Stugu, B
Abrams, G
Borgland, A
Breon, AB
Brown, D
Button-Shafer, J
author_facet Aubert, B
Barate, R
Boutigny, D
Couderc, F
Gaillard, J
Hicheur, A
Karyotakis, Y
Lees, J
Tisserand, V
Zghiche, A
Palano, A
Pompili, A
Chen, J
Qi, N
Rong, G
Wang, P
Zhu, Y
Eigen, G
Ofte, I
Stugu, B
Abrams, G
Borgland, A
Breon, AB
Brown, D
Button-Shafer, J
author_sort Aubert, B
collection OXFORD
description 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.
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spelling oxford-uuid:9dcc4190-96cd-4ee2-941e-7f767da5507e2022-03-27T00:45:45ZB meson decays to η(′) K*, η (′) ρ, η(′) π0, ωπ0, and φπ0Journal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:9dcc4190-96cd-4ee2-941e-7f767da5507eEnglishSymplectic Elements at Oxford2004Aubert, BBarate, RBoutigny, DCouderc, FGaillard, JHicheur, AKaryotakis, YLees, JTisserand, VZghiche, APalano, APompili, AChen, JQi, NRong, GWang, PZhu, YEigen, GOfte, IStugu, BAbrams, GBorgland, ABreon, ABBrown, DButton-Shafer, JWe 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.
spellingShingle Aubert, B
Barate, R
Boutigny, D
Couderc, F
Gaillard, J
Hicheur, A
Karyotakis, Y
Lees, J
Tisserand, V
Zghiche, A
Palano, A
Pompili, A
Chen, J
Qi, N
Rong, G
Wang, P
Zhu, Y
Eigen, G
Ofte, I
Stugu, B
Abrams, G
Borgland, A
Breon, AB
Brown, D
Button-Shafer, J
B meson decays to η(′) K*, η (′) ρ, η(′) π0, ωπ0, and φπ0
title B meson decays to η(′) K*, η (′) ρ, η(′) π0, ωπ0, and φπ0
title_full B meson decays to η(′) K*, η (′) ρ, η(′) π0, ωπ0, and φπ0
title_fullStr B meson decays to η(′) K*, η (′) ρ, η(′) π0, ωπ0, and φπ0
title_full_unstemmed B meson decays to η(′) K*, η (′) ρ, η(′) π0, ωπ0, and φπ0
title_short B meson decays to η(′) K*, η (′) ρ, η(′) π0, ωπ0, and φπ0
title_sort b meson decays to η k η ρ η π0 ωπ0 and φπ0
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