Search for b→u transitions in B-→DK- and D*K- decays
Creators
- Amo Sanchez, P. del1
- Lees, J. P.1
- Poireau, V.1
- Prencipe, E.1
- Tisserand, V.1
- Garra Tico, J.2
- Grauges, E.2
- Martinelli, M.3, 4
- Palano, A.3, 4
- Pappagallo, M.3, 4
- Eigen, G.5
- Stugu, B.5
- Sun, L.5
- Battaglia, M.6
- Brown, D. N.6
- Hooberman, B.6
- Kerth, L. T.6
- Kolomensky, Yu. G.6
- Lynch, G.6
- Osipenkov, I. L.6
- and others
- BABAR Collaboration
- 1. Laboratoire d'Annecy-le-Vieux de Physique des Particules (LAPP), Universite de Savoie, CNRS/IN2P3, F-74941 Annecy-Le-Vieux (France)
- 2. Universitat de Barcelona, Facultat de Fisica, Departament ECM, E-08028 Barcelona (Spain)
- 3. Dipartimento di Fisica, Universita di Bari, I-70126 Bari (Italy)
- 4. INFN Sezione di Bari, I-70126 Bari (Italy)
- 5. University of Bergen, Institute of Physics, N-5007 Bergen (Norway)
- 6. Lawrence Berkeley National Laboratory and University of California, Berkeley, California 94720 (United States)
Description
We report results from an updated study of the suppressed decays B-→DK- and B-→D*K- followed by D→K+π-, where D(*) indicates a D(*)0 or a D(*)0 meson, and D*→Dπ0 or D*→Dγ. These decays are sensitive to the Cabibbo-Kobayashi-Maskawa unitarity triangle angle γ due to interference between the b→c transition B-→D(*)0K- followed by the doubly Cabibbo-suppressed decay D0→K+π-, and the b→u transition B-→D(*)0K- followed by the Cabibbo-favored decay D0→K+π-. We also report an analysis of the decay B-→D(*)π- with the D decaying into the doubly Cabibbo-suppressed mode D→K+π-. Our results are based on 467x 106 Υ(4S)→BB decays collected with the BABAR detector at SLAC. We measure the ratios R(*) of the suppressed ([K+π-]DK-/π-) to favored ([K-π+]DK-/π-) branching fractions as well as the CP asymmetries A(*) of those modes. We see indications of signals for the B-→DK- and B-→DDπ0*K- suppressed modes, with statistical significances of 2.1 and 2.2σ, respectively, and we measure: RDK=(1.1±0.6±0.2)x10-2, ADK=-0.86±0.47-0.16+0.12, R(Dπ0)K*=(1.8±0.9± 0.4)x10-2, A(Dπ0)K*=+0.77±0.35±0.12, R(Dγ)K*=(1.3±1.4±0.8)x10-2,A(Dγ)K*=+0.36 ±0.94-0.41+0.25, where the first uncertainty is statistical and the second is systematic. We use a frequentist approach to obtain the magnitude of the ratio rB≡|A(B-→D0K-)/A(B-→D0K-)|=(9.5-4.1+5.1)%, with rB<16.7% at 90% confidence level. In the case of B-→D*K- we find rB*≡|A(B-→D*0K-)/A(B-→D*0K-)|=(9.6-5.1+3.5)%, with rB*<15.0% at 90% confidence level.
Additional details
Identifiers
- DOI
- 10.1103/PhysRevD.82.072006;
- arXiv
- arXiv:1006.4241v1;
Publishing Information
- Journal Title
- Physical Review. D, Particles Fields
- Journal Volume
- 82
- Journal Issue
- 7
- Journal Page Range
- p. 072006-072006.18
- ISSN
- 0556-2821
- CODEN
- PRVDAQ
INIS
- Country of Publication
- United States
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 42015736
- Subject category
- S72: PHYSICS OF ELEMENTARY PARTICLES AND FIELDS;
- Descriptors DEI
- ASYMMETRY; B MINUS MESONS; BRANCHING RATIO; CP INVARIANCE; D MESONS; INTERFERENCE; KAONS MINUS; KAONS PLUS; PARTICLE DECAY; PIONS MINUS; PIONS PLUS; STANFORD LINEAR ACCELERATOR CENTER; UNITARITY
- Descriptors DEC
- B MESONS; BEAUTY MESONS; BEAUTY PARTICLES; BOSONS; CHARM PARTICLES; CHARMED MESONS; DECAY; DIMENSIONLESS NUMBERS; ELEMENTARY PARTICLES; HADRONS; INVARIANCE PRINCIPLES; KAONS; MESONS; NATIONAL ORGANIZATIONS; PIONS; PSEUDOSCALAR MESONS; STRANGE MESONS; STRANGE PARTICLES; US DOE; US ERDA; US ORGANIZATIONS
Optional Information
- Notes
- (c) 2010 American Institute of Physics
- Collaborations
- BABAR Collaboration