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arxiv: 2401.02840 · v1 · pith:RQWLTFLZnew · submitted 2024-01-05 · ✦ hep-ex

A test of lepton flavor universality with a measurement of R(D^(*)) using hadronic B tagging at the Belle II experiment

Belle II Collaboration: I. Adachi , K. Adamczyk , L. Aggarwal , H. Ahmed , H. Aihara , N. Akopov , A. Aloisio , N. Anh Ky
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D. M. Asner H. Atmacan T. Aushev V. Aushev M. Aversano R. Ayad V. Babu H. Bae S. Bahinipati P. Bambade Sw. Banerjee S. Bansal M. Barrett J. Baudot M. Bauer A. Baur A. Beaubien F. Becherer J. Becker J. V. Bennett F. U. Bernlochner V. Bertacchi M. Bertemes E. Bertholet M. Bessner S. Bettarini B. Bhuyan F. Bianchi L. Bierwirth T. Bilka S. Bilokin D. Biswas A. Bobrov D. Bodrov A. Bolz A. Bondar J. Borah A. Bozek M. Bra\v{c}ko P. Branchini R. A. Briere T. E. Browder A. Budano S. Bussino M. Campajola L. Cao G. Casarosa C. Cecchi J. Cerasoli M.-C. Chang P. Chang R. Cheaib P. Cheema C. Chen B. G. Cheon K. Chilikin K. Chirapatpimol H.-E. Cho K. Cho S.-J. Cho S.-K. Choi S. Choudhury J. Cochran L. Corona L. M. Cremaldi S. Das F. Dattola E. De La Cruz-Burelo S. A. De La Motte G. De Nardo M. De Nuccio G. De Pietro R. de Sangro M. Destefanis R. Dhamija A. Di Canto F. Di Capua J. Dingfelder Z. Dole\v{z}al I. Dom\'inguez Jim\'enez T. V. Dong M. Dorigo K. Dort S. Dreyer S. Dubey G. Dujany P. Ecker M. Eliachevitch D. Epifanov P. Feichtinger T. Ferber D. Ferlewicz T. Fillinger C. Finck G. Finocchiaro A. Fodor F. Forti A. Frey B. G. Fulsom A. Gabrielli E. Ganiev M. Garcia-Hernandez R. Garg G. Gaudino V. Gaur A. Gaz A. Gellrich G. Ghevondyan D. Ghosh H. Ghumaryan G. Giakoustidis R. Giordano A. Giri A. Glazov B. Gobbo R. Godang O. Gogota P. Goldenzweig W. Gradl T. Grammatico E. Graziani D. Greenwald Z. Gruberov\'a T. Gu Y. Guan K. Gudkova Y. Han K. Hara T. Hara K. Hayasaka H. Hayashii S. Hazra C. Hearty M. T. Hedges A. Heidelbach I. Heredia de la Cruz M. Hern\'andez Villanueva T. Higuchi E. C. Hill M. Hoek M. Hohmann P. Horak C.-L. Hsu T. Humair T. Iijima K. Inami G. Inguglia N. Ipsita A. Ishikawa R. Itoh M. Iwasaki P. Jackson W. W. Jacobs D. E. Jaffe E.-J. Jang Q. P. Ji S. Jia Y. Jin K. K. Joo H. Junkerkalefeld H. Kakuno M. Kaleta D. Kalita A. B. Kaliyar J. Kandra K. H. Kang S. Kang T. Kawasaki F. Keil C. Kiesling C.-H. Kim D. Y. Kim K.-H. Kim Y.-K. Kim H. Kindo K. Kinoshita P. Kody\v{s} T. Koga S. Kohani K. Kojima T. Konno A. Korobov S. Korpar E. Kovalenko R. Kowalewski T. M. G. Kraetzschmar P. Kri\v{z}an P. Krokovny T. Kuhr Y. Kulii J. Kumar M. Kumar R. Kumar K. Kumara T. Kunigo A. Kuzmin Y.-J. Kwon S. Lacaprara Y.-T. Lai T. Lam L. Lanceri J. S. Lange M. Laurenza R. Leboucher F. R. Le Diberder M. J. Lee D. Levit P. M. Lewis C. Li L. K. Li Y. Li Y. B. Li J. Libby Q. Y. Liu Z. Q. Liu D. Liventsev S. Longo T. Lueck C. Lyu Y. Ma M. Maggiora S. P. Maharana R. Maiti S. Maity G. Mancinelli R. Manfredi E. Manoni A. C. Manthei M. Mantovano D. Marcantonio S. Marcello C. Marinas L. Martel C. Martellini A. Martini T. Martinov L. Massaccesi M. Masuda T. Matsuda K. Matsuoka D. Matvienko S. K. Maurya J. A. McKenna R. Mehta F. Meier M. Merola F. Metzner M. Milesi C. Miller M. Mirra K. Miyabayashi H. Miyake R. Mizuk G. B. Mohanty N. Molina-Gonzalez S. Mondal S. Moneta H.-G. Moser M. Mrvar R. Mussa I. Nakamura K. R. Nakamura M. Nakao Y. Nakazawa A. Narimani Charan M. Naruki D. Narwal Z. Natkaniec A. Natochii L. Nayak M. Nayak G. Nazaryan M. Neu C. Niebuhr S. Nishida S. Ogawa Y. Onishchuk H. Ono Y. Onuki P. Oskin F. Otani P. Pakhlov G. Pakhlova A. Paladino A. Panta E. Paoloni S. Pardi K. Parham H. Park S.-H. Park B. Paschen A. Passeri S. Patra S. Paul T. K. Pedlar R. Peschke R. Pestotnik F. Pham M. Piccolo L. E. Piilonen G. Pinna Angioni P. L. M. Podesta-Lerma T. Podobnik S. Pokharel C. Praz S. Prell E. Prencipe M. T. Prim H. Purwar P. Rados G. Raeuber S. Raiz N. Rauls M. Reif S. Reiter M. Remnev I. Ripp-Baudot G. Rizzo S. H. Robertson M. Roehrken J. M. Roney A. Rostomyan N. Rout G. Russo D. A. Sanders S. Sandilya A. Sangal L. Santelj Y. Sato V. Savinov B. Scavino C. Schmitt C. Schwanda A. J. Schwartz Y. Seino A. Selce K. Senyo J. Serrano M. E. Sevior C. Sfienti W. Shan C. Sharma X. D. Shi T. Shillington T. Shimasaki J.-G. Shiu D. Shtol A. Sibidanov F. Simon J. B. Singh J. Skorupa K. Smith R. J. Sobie M. Sobotzik A. Soffer A. Sokolov E. Solovieva S. Spataro B. Spruck M. Stari\v{c} P. Stavroulakis S. Stefkova R. Stroili Y. Sue M. Sumihama K. Sumisawa W. Sutcliffe H. Svidras M. Takahashi M. Takizawa U. Tamponi S. Tanaka K. Tanida F. Tenchini O. Tittel R. Tiwary D. Tonelli E. Torassa K. Trabelsi I. Tsaklidis M. Uchida I. Ueda Y. Uematsu T. Uglov K. Unger Y. Unno K. Uno S. Uno P. Urquijo Y. Ushiroda S. E. Vahsen R. van Tonder K. E. Varvell M. Veronesi A. Vinokurova V. S. Vismaya L. Vitale V. Vobbilisetti R. Volpe B. Wach M. Wakai S. Wallner E. Wang M.-Z. Wang X. L. Wang Z. Wang A. Warburton M. Watanabe S. Watanuki C. Wessel J. Wiechczynski E. Won X. P. Xu B. D. Yabsley S. Yamada S. B. Yang J. Yelton J. H. Yin K. Yoshihara C. Z. Yuan Y. Yusa B. Zhang Y. Zhang V. Zhilich Q. D. Zhou X. Y. Zhou V. I. Zhukova R. \v{Z}leb\v{c}\'ik
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The ratio of branching fractions $R(D^{*}) = \mathcal{B}(\overline{B} \rightarrow D^{*} \tau^{-} \overline{\nu}_{\tau})$/$\mathcal{B} (\overline{B} \rightarrow D^{*} \ell^{-} \overline{\nu}_{\ell})$, where $\ell$ is an electron or muon, is measured using a Belle~II data sample with an integrated luminosity of $189~\mathrm{fb}^{-1}$ at the SuperKEKB asymmetric-energy $e^{+} e^{-}$ collider. Data is collected at the $\Upsilon(\mathrm{4S})$ resonance, and one $B$ meson in the $\Upsilon(\mathrm{4S})\rightarrow B\overline{B}$ decay is fully reconstructed in hadronic decay modes. The accompanying signal $B$ meson is reconstructed as $\overline{B}\rightarrow D^{*} \tau^{-}\overline{\nu}_{\tau}$ using leptonic $\tau$ decays. The normalization decay, $\overline{B}\rightarrow D^{*} \ell^{-} \overline{\nu}_{\ell}$, where $\ell$ is an electron or muon, produces the same observable final state particles. The ratio of branching fractions is extracted in a simultaneous fit to two signal-discriminating variables in both channels and yields $R(D^{*}) = 0.262~_{-0.039}^{+0.041}(\mathrm{stat})~_{-0.032}^{+0.035}(\mathrm{syst})$. This result is consistent with the current world average and with standard model predictions.

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