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Recently, several indications of lepton non-universality observables have been perceived in semileptonic $B$ meson decay processes, both in the neutral-current ($b \to s ll $) and charged-current ($b \to c l \bar \nu_l$) transitions.…

High Energy Physics - Phenomenology · Physics 2025-07-16 Aishwarya Bhatta , Rukmani Mohanta

Based on the full BaBar data sample, we report improved measurements of the ratios R(D(*)) = B(B -> D(*) Tau Nu)/B(B -> D(*) l Nu), where l is either e or mu. These ratios are sensitive to new physics contributions in the form of a charged…

High Energy Physics - Experiment · Physics 2015-03-20 The BaBar Collaboration

Using a full BABAR data sample of 426 $fb^{-1}$, we present improved measurements of the ratio ${\cal{R}}(D^{(*)}) = {\cal{B}} (\bar{B} \to D^{(*)}\tau^{-}\bar{\nu}_{\tau})/$ ${\cal{B}} (\bar{B} \to D^{(*)}\ell_{\ell}^{-}\bar{\nu}_{\ell})$,…

High Energy Physics - Experiment · Physics 2015-06-15 Romulus Godang

We study \tau\to \mu \bar{\nu_i} \nu_i, i=e,\mu,\tau decay in the model III version of the two Higgs doublet model. We calculated the BR at the order of the magnitude of 10^{-6}-10^{-4} for the intermediate values of the Yukawa couplings.…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. Iltan , H. Sundu

We study the $L\to l l' l' \nu_l \nu_L$ decays ($L=\tau,\mu$; $l,l'=\mu,e$) in the Standard Model (SM) and in the effective field theory (EFT) description of the weak charged current at low energy, both for polarized and unpolarized $L$,…

High Energy Physics - Phenomenology · Physics 2016-08-15 A. Flores-Tlalpa , G. López-Castro , P. Roig

We investigate a new constraint on new-physics interpretations of the anomalies observed in $B\to D^{(*)}\tau\nu$ decays making use of the lifetime of the $B_c^-$ meson. A constraint is obtained by demanding that the rate for…

High Energy Physics - Phenomenology · Physics 2017-03-01 Rodrigo Alonso , Benjamín Grinstein , Jorge Martin Camalich

For any new physics possibly emerging in the future B experiments, the problem is how to extract the signals from the SM background. We consider the decay $b\to s s\bar d$ which is very small in the SM. In the MSSM this decay is possibly…

High Energy Physics - Phenomenology · Physics 2009-10-31 Katri Huitu , Cai-Dian Lü , Paul Singer , Da-Xin Zhang

Transitions of the type $b \to s l^+ l^-$ are flavour changing neutral current processes where new physics can enter in competing loop diagrams with respect to the Standard Model contributions. In these decays several observables sensitive…

High Energy Physics - Experiment · Physics 2015-03-20 Nicola Serra

We establish improved upper limits on branching fractions for $B^{0}$ decays to final states where the decay products are purely invisible (i.e., no observable final state particles) and for final states where the only visible product is a…

High Energy Physics - Experiment · Physics 2019-08-14 A. Rossi

We measure the branching fractions for the decays $\bar{B}^0 \to D^{*+} e^{-} \bar{\nu}_e$ and $\bar{B}^0 \to D^{*+} \mu^{-} \bar{\nu}_\mu$ using $8.70 \pm 0.09~{\rm fb}^{-1}$ of data collected by the Belle II experiment at the SuperKEKB…

High Energy Physics - Experiment · Physics 2020-06-15 Belle II Collaboration , F. Abudinén , I. Adachi , R. Adak , K. Adamczyk , P. Ahlburg , J. K. Ahn , H. Aihara , N. Akopov , A. Aloisio , F. Ameli , L. Andricek , N. Anh Ky , D. M. Asner , H. Atmacan , V. Aulchenko , T. Aushev , V. Aushev , T. Aziz , V. Babu , S. Bacher , S. Baehr , S. Bahinipati , A. M. Bakich , P. Bambade , Sw. Banerjee , S. Bansal , M. Barrett , W. Bartel , G. Batignani , J. Baudot , A. Beaulieu , J. Becker , P. K. Behera , M. Bender , J. V. Bennett , E. Bernieri , F. U. Bernlochner , M. Bertemes , M. Bessner , S. Bettarini , V. Bhardwaj , B. Bhuyan , F. Bianchi , T. Bilka , S. Bilokin , D. Biswas , A. Bobrov , A. Bondar , G. Bonvicini , A. Bozek , M. Bračko , P. Branchini , N. Braun , R. A. Briere , T. E. Browder , D. N. Brown , A. Budano , L. Burmistrov , S. Bussino , M. Campajola , L. Cao , G. Caria , G. Casarosa , C. Cecchi , D. Červenkov , M. -C. Chang , P. Chang , R. Cheaib , V. Chekelian , Y. Q. Chen , Y. -T. Chen , B. G. Cheon , K. Chilikin , H. -E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , S. Choudhury , D. Cinabro , L. Corona , L. M. Cremaldi , D. Cuesta , S. Cunliffe , T. Czank , N. Dash , F. Dattola , E. De La Cruz-Burelo , G. De Nardo , M. De Nuccio , G. De Pietro , R. de Sangro , B. Deschamps , M. Destefanis , S. Dey , A. De Yta-Hernandez , F. Di Capua , S. Di Carlo , J. Dingfelder , Z. Doležal , I. Domínguez Jiménez , T. V. Dong , K. Dort , D. Dossett , S. Dubey , S. Duell , G. Dujany , S. Eidelman , M. Eliachevitch , D. Epifanov , J. E. Fast , T. Ferber , D. Ferlewicz , G. Finocchiaro , S. Fiore , P. Fischer , A. Fodor , F. Forti , A. Frey , M. Friedl , B. G. Fulsom , M. Gabriel , N. Gabyshev , E. Ganiev , M. Garcia-Hernandez , R. Garg , A. Garmash , V. Gaur , A. Gaz , U. Gebauer , M. Gelb , A. Gellrich , J. Gemmler , T. Geßler , D. Getzkow , R. Giordano , A. Giri , A. Glazov , B. Gobbo , R. Godang , P. Goldenzweig , B. Golob , P. Gomis , P. Grace , W. Gradl , E. Graziani , D. Greenwald , Y. Guan , C. Hadjivasiliou , S. Halder , K. Hara , T. Hara , O. Hartbrich , T. Hauth , K. Hayasaka , H. Hayashii , C. Hearty , M. Heck , M. T. Hedges , I. Heredia de la Cruz , M. Hernández Villanueva , A. Hershenhorn , T. Higuchi , E. C. Hill , H. Hirata , S. Hirose , M. Hoek , M. Hohmann , S. Hollitt , T. Hotta , C. -L. Hsu , Y. Hu , K. Huang , T. Iijima , K. Inami , G. Inguglia , J. Irakkathil Jabbar , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , S. Iwata , P. Jackson , W. W. Jacobs , I. Jaegle , D. E. Jaffe , E. -J. Jang , M. Jeandron , H. B. Jeon , S. Jia , Y. Jin , C. Joo , K. K. Joo , I. Kadenko , J. Kahn , H. Kakuno , A. B. Kaliyar , J. Kandra , K. H. Kang , P. Kapusta , G. Karyan , Y. Kato , H. Kawai , T. Kawasaki , T. Keck , C. Ketter , H. Kichimi , C. Kiesling , B. H. Kim , C. -H. Kim , D. Y. Kim , H. J. Kim , J. B. Kim , K. -H. Kim , K. Kim , S. -H. Kim , Y. -K. Kim , Y. Kim , T. D. Kimmel , H. Kindo , K. Kinoshita , B. Kirby , C. Kleinwort , B. Knysh , P. Kodyš , T. Koga , S. Kohani , S. Koirala , I. Komarov , T. Konno , S. Korpar , N. Kovalchuk , T. M. G. Kraetzschmar , P. Križan , R. Kroeger , J. F. Krohn , P. Krokovny , H. Krüger , W. Kuehn , T. Kuhr , J. Kumar , M. Kumar , R. Kumar , K. Kumara , T. Kumita , T. Kunigo , M. Künzel , S. Kurz , A. Kuzmin , P. Kvasnička , Y. -J. Kwon , S. Lacaprara , Y. -T. Lai , C. La Licata , K. Lalwani , L. Lanceri , J. S. Lange , K. Lautenbach , P. J. Laycock , F. R. Le Diberder , I. -S. Lee , S. C. Lee , P. Leitl , D. Levit , P. M. Lewis , C. Li , L. K. Li , S. X. Li , Y. M. Li , Y. B. Li , J. Libby , K. Lieret , L. Li Gioi , J. Lin , Z. Liptak , Q. Y. Liu , Z. A. Liu , D. Liventsev , S. Longo , A. Loos , P. Lu , M. Lubej , T. Lueck , F. Luetticke , T. Luo , C. MacQueen , Y. Maeda , M. Maggiora , S. Maity , R. Manfredi , E. Manoni , S. Marcello , C. Marinas , A. Martini , M. Masuda , T. Matsuda , K. Matsuoka , D. Matvienko , J. McNeil , F. Meggendorfer , J. C. Mei , F. Meier , M. Merola , F. Metzner , M. Milesi , C. Miller , K. Miyabayashi , H. Miyake , H. Miyata , R. Mizuk , K. Azmi , G. B. Mohanty , H. Moon , T. Moon , J. A. Mora Grimaldo , A. Morda , T. Morii , H. -G. Moser , M. Mrvar , F. Mueller , F. J. Müller , Th. Muller , G. Muroyama , R. Mussa , K. Nakagiri , I. Nakamura , K. R. Nakamura , E. Nakano , M. Nakao , H. Nakayama , H. Nakazawa , T. Nanut , Z. Natkaniec , M. Nayak , G. Nazaryan , D. Neverov , C. Niebuhr , M. Niiyama , J. Ninkovic , N. K. Nisar , S. Nishida , K. Nishimura , M. Nishimura , M. H. A. Nouxman , B. Oberhof , K. Ogawa , S. Ogawa , S. L. Olsen , Y. Onishchuk , H. Ono , Y. Onuki , P. Oskin , E. R. Oxford , H. Ozaki , P. Pakhlov , G. Pakhlova , A. Paladino , T. Pang , A. Panta , E. Paoloni , C. Park , H. Park , S. -H. Park , B. Paschen , A. Passeri , A. Pathak , S. Patra , S. Paul , T. K. Pedlar , I. Peruzzi , R. Peschke , R. Pestotnik , M. Piccolo , L. E. Piilonen , P. L. M. Podesta-Lerma , V. Popov , C. Praz , E. 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Zhilich , Q. D. Zhou , X. Y. Zhou , V. I. Zhukova , V. Zhulanov , A. Zupanc

$R_{D^{(*)}}$ is the ratio of branching ratio $\overline{B} \rightarrow D^{(*)}\tau\overline{\nu}_{\tau}$ to $\overline{B} \rightarrow D^{(*)}l\overline{\nu}_{l}~(l=e,~\mu)$. There is a gap of 2$\sigma_{exp}$ or more between its…

High Energy Physics - Phenomenology · Physics 2023-09-08 Xin-Xin Long , Shu-Min Zhao , Ming-Yue Liu , Xi Wang , Yi-Tong Wang , Zhong-Jun Yang , Xing-Xing Dong , Tai-Fu Feng

Recently, the BaBar collaboration reported first evidence for new physics in B->D\tau\nu and B->D*\tau\nu. Combining both processes the significance is 3.4\sigma. This result cannot be explained in a two Higgs doublet model of type II.…

High Energy Physics - Phenomenology · Physics 2013-09-04 Andreas Crivellin , Christoph Greub , Ahmet Kokulu

We examine the $q^2$-binned distributions of the $D\to K\mu\nu$ decay rate and of the corresponding forward-backward asymmetry which were recently measured by BESIII, showing a mild deviation from the Standard Model predictions. We point…

High Energy Physics - Phenomenology · Physics 2026-03-30 D. Bečirević , M. Martines , S. Rosauro-Alcaraz , O. Sumensari

We analyze the rare decay mode $B \to \phi \pi $, which is a pure penguin induced process, receiving dominant contribution from the electroweak penguins. Thus the standard model branching ratio is expected to be very small, which makes it…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. K. Giri , R. Mohanta

We review possible impact of beyond Standard Model physics in the third generation leptonic and semileptonic B decays.

High Energy Physics - Phenomenology · Physics 2013-01-18 Svjetlana Fajfer , Ivan Nisandzic

Using a sample of 3.3 million B-meson decays collected with the CLEO detector at the Cornell Electron Storage Ring, we have studied $B^- \to D^0 \ell\nu$ and $\bar{B}^0 \to D^+ \ell\nu$ decays, where $\ell$ can be either an electron or…

High Energy Physics - Experiment · Physics 2010-04-08 J. Bartelt

The $\bar{B}_s^0 \to D_s^{(*)+} l^- \bar{\nu}_l$ semileptonic decays were calculated in the framework of the standard model (SM) by employing the perturbative QCD (pQCD) factorization approach. We defined four ratios of the branching ratios…

High Energy Physics - Phenomenology · Physics 2014-02-05 Ying-Ying Fan , Wen-Fei Wang , Zhen-Jun Xiao

I describe the theoretical progress in the study of semileptonic tree-level B decays, and its interplay with recent experimental results. In particular, I focus on two anomalies: the ratios $R(D^{(*)})=\displaystyle\frac{{\cal B}(B \to…

High Energy Physics - Phenomenology · Physics 2017-11-10 Fulvia De Fazio

Leptonic rare decays of $B^0_{s,d}$ mesons offer a powerful tool to search for physics beyond the Standard Model. The $B^0_{s}\to\mu^+\mu^-$ decay has been observed at the Large Hadron Collider and the first measurement of the effective…

High Energy Physics - Phenomenology · Physics 2017-09-13 Robert Fleischer , Ruben Jaarsma , Gilberto Tetlalmatzi-Xolocotzi

In this proceeding we will review the current theoretical status of rare $B$ decays. These decays are indeed excellent indirect probes for New Physics searches, and in the current situation where no new states have been directly observed at…

High Energy Physics - Phenomenology · Physics 2024-02-07 Marco Fedele
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