Search for b-->u transitions in B--->DK- and D*K- decays

We report results from an updated study of the suppressed decays B--->DK- and B--->D*K- followed by D-->K+pi-, where D(*) indicates a D(*)0 or a D[over-bar] (*)0 meson, and D*-->Dpi0 or D*-->Dgamma. These decays are sensitive to the Cabibbo-Kobayashi-Maskawa unitarity triangle angle g...

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Main Authors: Sciolla, Gabriella, Zhao, M., Dujmic, Denis, Fisher, Peter H, Cowan, Ray F
Other Authors: Massachusetts Institute of Technology. Department of Physics
Format: Article
Language:en_US
Published: American Physical Society 2011
Online Access:http://hdl.handle.net/1721.1/61346
https://orcid.org/0000-0002-8667-5660
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author Sciolla, Gabriella
Zhao, M.
Dujmic, Denis
Fisher, Peter H
Cowan, Ray F
author2 Massachusetts Institute of Technology. Department of Physics
author_facet Massachusetts Institute of Technology. Department of Physics
Sciolla, Gabriella
Zhao, M.
Dujmic, Denis
Fisher, Peter H
Cowan, Ray F
author_sort Sciolla, Gabriella
collection MIT
description We report results from an updated study of the suppressed decays B--->DK- and B--->D*K- followed by D-->K+pi-, where D(*) indicates a D(*)0 or a D[over-bar] (*)0 meson, and D*-->Dpi0 or D*-->Dgamma. These decays are sensitive to the Cabibbo-Kobayashi-Maskawa unitarity triangle angle gamma due to interference between the b-->c transition B--->D(*)0K- followed by the doubly Cabibbo-suppressed decay D0-->K+pi-, and the b-->u transition B--->D[over-bar] (*)0K- followed by the Cabibbo-favored decay D[over-bar] 0-->K+pi-. We also report an analysis of the decay B--->D(*)pi- with the D decaying into the doubly Cabibbo-suppressed mode D-->K+pi-. Our results are based on 467× 106 Υ(4S)-->BB[over-bar] decays collected with the BABAR detector at SLAC. We measure the ratios R(*) of the suppressed ([K+pi-]DK-/pi-) to favored ([K-pi+]DK-/pi-) branching fractions as well as the CP asymmetries A(*) of those modes. We see indications of signals for the B--->DK- and B--->DDpi0*K- suppressed modes, with statistical significances of 2.1 and 2.2σ, respectively, and we measure: RDK=(1.1±0.6±0.2)×10-2, ADK=-0.86±0.47-0.16+0.12, R(Dpi0)K*=(1.8±0.9± 0.4)×10-2, A(Dpi0)K*=+0.77±0.35±0.12, R(Dgamma)K*=(1.3±1.4±0.8)×10-2,A(Dgamma)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--->D[over-bar] 0K-)/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[over-bar] *0K-)/A(B--->D*0K-)|=(9.6-5.1+3.5)%, with rB*<15.0% at 90% confidence level.
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spelling mit-1721.1/613462023-02-26T08:08:47Z Search for b-->u transitions in B--->DK- and D*K- decays Search for b→u transitions in B-→DK- and D*K- decays Sciolla, Gabriella Zhao, M. Dujmic, Denis Fisher, Peter H Cowan, Ray F Massachusetts Institute of Technology. Department of Physics Massachusetts Institute of Technology. Laboratory for Nuclear Science Fisher, Peter H. Sciolla, Gabriella Fisher, Peter H. Cowan, Ray Franklin Zhao, M. Dujmic, Denis We report results from an updated study of the suppressed decays B--->DK- and B--->D*K- followed by D-->K+pi-, where D(*) indicates a D(*)0 or a D[over-bar] (*)0 meson, and D*-->Dpi0 or D*-->Dgamma. These decays are sensitive to the Cabibbo-Kobayashi-Maskawa unitarity triangle angle gamma due to interference between the b-->c transition B--->D(*)0K- followed by the doubly Cabibbo-suppressed decay D0-->K+pi-, and the b-->u transition B--->D[over-bar] (*)0K- followed by the Cabibbo-favored decay D[over-bar] 0-->K+pi-. We also report an analysis of the decay B--->D(*)pi- with the D decaying into the doubly Cabibbo-suppressed mode D-->K+pi-. Our results are based on 467× 106 Υ(4S)-->BB[over-bar] decays collected with the BABAR detector at SLAC. We measure the ratios R(*) of the suppressed ([K+pi-]DK-/pi-) to favored ([K-pi+]DK-/pi-) branching fractions as well as the CP asymmetries A(*) of those modes. We see indications of signals for the B--->DK- and B--->DDpi0*K- suppressed modes, with statistical significances of 2.1 and 2.2σ, respectively, and we measure: RDK=(1.1±0.6±0.2)×10-2, ADK=-0.86±0.47-0.16+0.12, R(Dpi0)K*=(1.8±0.9± 0.4)×10-2, A(Dpi0)K*=+0.77±0.35±0.12, R(Dgamma)K*=(1.3±1.4±0.8)×10-2,A(Dgamma)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--->D[over-bar] 0K-)/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[over-bar] *0K-)/A(B--->D*0K-)|=(9.6-5.1+3.5)%, with rB*<15.0% at 90% confidence level. Alfred P. Sloan Foundation United States-Israel Binational Science Foundation United States. Dept. of Energy National Science Foundation (U.S.) 2011-02-25T20:21:16Z 2011-02-25T20:21:16Z 2010-10 2010-06 Article http://purl.org/eprint/type/JournalArticle 1550-7998 1550-2368 http://hdl.handle.net/1721.1/61346 The BABAR Collaboration et al. “Search for b-->u transitions in B^{-}-->DK^{-} and D^{*}K^{-} decays.” Physical Review D 82.7 (2010): 072006. © 2010 The American Physical Society. https://orcid.org/0000-0002-8667-5660 en_US http://dx.doi.org/10.1103/PhysRevD.82.072006 Physical Review D Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. application/pdf American Physical Society APS
spellingShingle Sciolla, Gabriella
Zhao, M.
Dujmic, Denis
Fisher, Peter H
Cowan, Ray F
Search for b-->u transitions in B--->DK- and D*K- decays
title Search for b-->u transitions in B--->DK- and D*K- decays
title_full Search for b-->u transitions in B--->DK- and D*K- decays
title_fullStr Search for b-->u transitions in B--->DK- and D*K- decays
title_full_unstemmed Search for b-->u transitions in B--->DK- and D*K- decays
title_short Search for b-->u transitions in B--->DK- and D*K- decays
title_sort search for b u transitions in b dk and d k decays
url http://hdl.handle.net/1721.1/61346
https://orcid.org/0000-0002-8667-5660
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