Looking for new physics in leptonic and semileptonic decays of B-meson-Reference-Cited by-同舟云学术

Looking for new physics in leptonic and semileptonic decays of B-meson

Published:2017-09 Issue:5 Volume:14 Page:669-676
ISSN:1547-4771
Container-title:Physics of Particles and Nuclei Letters
language:en
Short-container-title:Phys. Part. Nuclei Lett.

Author:

Ivanov M. A.,Körner J. G.,Tran C. T.

Publisher

Pleiades Publishing Ltd

Subject

Radiology Nuclear Medicine and imaging,Nuclear and High Energy Physics,Atomic and Molecular Physics, and Optics,Radiation

Link

http://link.springer.com/content/pdf/10.1134/S1547477117050053.pdf

Reference28 articles.

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2. M. Huschle et al. (Belle Collab.), “Measurement of the branching ratio of $$\overline B \to {D^{\left( * \right)}}{\tau ^ - }{\overline \upsilon _\tau }$$ B ¯ → D ( * ) τ − υ ¯ τ relative to $$\overline B \to {D^{\left( * \right)}}{l^ - }{\overline \upsilon _l}$$ B ¯ → D ( * ) l − υ ¯ l decays with hadronic tagging at Belle,” Phys. Rev. D 92, 072014 (2015); arXiv:1507.03233 [hepex]. doi 10.1103/PhysRevD.92.07201410.1103/Phys-RevD.92.072014

3. Y. Sato et al. (Belle Collab.), “Measurement of the branching ratio of $${\bar B^0} \to {D^{* + }}{\tau ^ - }{\bar \upsilon _\tau }$$ B ¯ 0 → D * + τ − υ ¯ τ relative to $${\bar B^0} \to {D^{* + }}{l^ - }{\bar \upsilon _l}$$ B ¯ 0 → D * + l − υ ¯ l decays with a semileptonic tagging method,” Phys. Rev. D 94, 072007 (2016); arXiv:1607.07923 [hep-ex]. doi 10.1103/Phys-RevD.94.07200710.1103/PhysRevD.94.072007

4. S. Hirose et al. (Belle Collab.), “Measurement of the lepton polarization and R(D*) in the decay $$\bar B \to {D^{* + }}{\tau ^ - }{\bar \upsilon _\tau }$$ B ¯ → D * + τ − υ ¯ τ ” arXiv:1607.07923 [hep-ex] (2016).

5. R. Aaij et al. (LHCb Collab.), “Measurement of the ratio of branching fractions $${{B\left( {{{\bar B}^0} \to {D^{\left( * \right)}}\tau \bar \upsilon } \right)} \mathord{\left/ {\vphantom {{B\left( {{{\bar B}^0} \to {D^{\left( * \right)}}\tau \bar \upsilon } \right)} {B\left( {{{\bar B}^0} \to {D^{* + }}{\mu ^ - }\bar \upsilon } \right)}}} \right. \kern-\nulldelimiterspace} {B\left( {{{\bar B}^0} \to {D^{* + }}{\mu ^ - }\bar \upsilon } \right)}}{\text{ }}$$ B ( B ¯ 0 → D ( * ) τ υ ¯ ) / B ( B ¯ 0 → D * + μ − υ ¯ ) ,” Phys. Rev. Lett. 115, 111803 (2015); arXiv:1506.08614 [hep-ex]. doi 10.1103/PhysRevLett.115.15990110.1103/PhysRevLett.115.159901

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