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Measurement of branching fractions in radiative B decays to η K γ and search for B decays to η ′ K γ
We present measurements of the B → η K γ branching fractions and upper limits for the B → η ′ K γ branching fractions. For B + → η K + γ we also measure the time-integrated charge asymmetry. The data sample, collected with the BABAR detector at the Stanford Linear Accelerator Center, represents 232...
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Published in: | Physical review. D, Particles, fields, gravitation, and cosmology Particles, fields, gravitation, and cosmology, 2006, Vol.74 (3), Article 031102 |
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format: | Article |
Language: | English |
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Online Access: | Get full text |
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Summary: | We present measurements of the B → η K γ branching fractions and upper limits for the B → η ′ K γ branching fractions. For B + → η K + γ we also measure the time-integrated charge asymmetry. The data sample, collected with the BABAR detector at the Stanford Linear Accelerator Center, represents 232 × 10 6 produced B ¯¯¯ B pairs. The results for branching fractions and upper limits at 90% confidence level in units of 10 − 6 are: B ( B 0 → η K 0 γ ) = 11.3 + 2.8 − 2.6 ± 0.6 , B ( B + → η K + γ ) = 10.0 ± 1.3 ± 0.5 , B ( B 0 → η ′ K 0 γ ) < 6.6 , B ( B + → η ′ K + γ ) < 4.2 . The charge asymmetry in the decay B + → η K + γ is A ch = − 0.09 ± 0.12 ± 0.01 . The first errors are statistical and the second systematic. |
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ISSN: | 1550-7998 1550-2368 |
DOI: | 10.1103/PhysRevD.74.031102 |