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  • Open Access

Observation of the B0D¯*0K+π and Bs0D¯*0Kπ+ decays

R. Aaij et al. (LHCb Collaboration)
Phys. Rev. D 105, 072005 – Published 20 April 2022

Abstract

The first observations of B0D¯*(2007)0K+π and Bs0D¯*(2007)0Kπ+ decays are presented, and their branching fractions relative to that of the B0D¯*(2007)0π+π decay are reported. These modes can potentially be used to investigate the spectroscopy of charm and charm-strange resonances and to determine the angle γ of the Cabibbo-Kobayashi-Maskawa unitarity triangle. It is also important to understand them as a source of potential background in determinations of γ from B+DK+ and B0DK+π decays. The analysis is based on a sample corresponding to an integrated luminosity of 5.4fb1 of proton-proton collision data at 13 TeV center-of-mass energy recorded with the LHCb detector. The D¯*(2007)0 mesons are fully reconstructed in the D¯0π0 and D¯0γ channels with the D¯0K+π decay. A novel weighting method is used to subtract background while simultaneously applying an event-by-event efficiency correction to account for resonant structures in the decays.

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  • Received 22 December 2021
  • Accepted 4 March 2022

DOI:https://doi.org/10.1103/PhysRevD.105.072005

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. Funded by SCOAP3.

© 2022 CERN, for the LHCb Collaboration

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Vol. 105, Iss. 7 — 1 April 2022

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Images

  • Figure 1
    Figure 1

    Leading diagrams for (a), (c) B0D¯*0K+π and (b), (d) Bs0D¯*0Kπ+ decay channels. In the color-suppressed diagrams, (a) and (b), the decay proceeds through an intermediate K()*0 resonance with additional uu¯ production, while in the color-allowed diagrams the decay proceeds through an excited charm (c) or charm-strange (d) resonance.

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  • Figure 2
    Figure 2

    Difference between the D¯*0 and D¯0 candidate masses in B0D¯*0π+π decays for (top) data and (bottom) simulated signal decays. The left and right plots show D¯*0D¯0γ and D¯0π0 candidates, respectively. The simulation distributions are shown separately for correctly reconstructed and misreconstructed signal components. All selection requirements have been imposed, except those on the plotted variable, which are indicated with dashed vertical lines.

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  • Figure 3
    Figure 3

    Invariant mass distributions of (top) B0D¯*0K+π, (middle) Bs0D¯*0Kπ+ and (bottom) B0D¯*0π+π with (left) D¯*0D¯0γ and (right) D¯*0D¯0π0 candidates, with a linear y axis. The total fit result is shown overlaid as a solid blue line, with individual components illustrated as indicated in the legends.

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  • Figure 4
    Figure 4

    Invariant mass distributions of (top) B0D¯*0K+π, (middle) Bs0D¯*0Kπ+ and (bottom) B0D¯*0π+π with (left) D¯*0D¯0γ and (right) D¯*0D¯0π0 candidates, with a logarithmic y-axis scale. The total fit result is shown overlaid as a solid blue line, with individual components illustrated as indicated in the legends of Fig. 3.

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  • Figure 5
    Figure 5

    Total efficiency as a function of SDP coordinates for (top) B0D¯*0K+π, (middle) Bs0D¯*0Kπ+ and (bottom) B0D¯*0π+π, with (left) D¯*0D¯0γ and (right) D¯*0D¯0π0 decays.

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  • Figure 6
    Figure 6

    SDP (left) and conventional Dalitz (right) plots of background-subtracted and efficiency-corrected data, for (top) B0D¯*0K+π, (middle) Bs0D¯*0Kπ+ and (bottom) B0D¯*0π+π decays.

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