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Related papers: Semileptonic b to u transition

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We present a preliminary determination of the CKM matrix element |Vub| based on the analysis of semileptonic B decays from a sample of 88 million Upsilon(4S) decays collected with the BaBar detector at the e+e- storage ring. Charmless…

High Energy Physics - Experiment · Physics 2007-05-23 B. Aubert , The BaBar Collaboration

We propose an approach for measuring the moments of the hadronic invariant mass distribution in semileptonic $B_{s}^{0}$ meson decays using a sum-of-exclusive technique. Using the present and foreseen knowledge about exclusive semileptonic…

High Energy Physics - Phenomenology · Physics 2024-07-04 Michel De Cian , Natalia Feliks , Marcello Rotondo , K. Keri Vos

We present results on semileptonic B decays obtained with the BABAR detector. The large data set accumulated at the PEP-II asymmetric-energy B-Factory allows a new measurement technique, where the hadronic decay of one B meson is fully…

High Energy Physics - Experiment · Physics 2010-11-23 Urs Langenegger

The inclusive charm hadron semileptonic branching fractions B(c to e) and B(c to mu) in Z to ccbar events have been determined using 4.4 million hadronic Z decays collected with the OPAL detector at LEP. A charm-enriched sample is obtained…

High Energy Physics - Experiment · Physics 2008-11-26 The OPAL Collaboration , G. Abbiendi et al

I report results from the CLEO collaboration on semileptonic B decays, highlighting measurements of the Cabibbo-Kobayashi-Maskawa matrix elements Vcb and Vub. I describe the techniques used to obtain the recent improvements in precision for…

High Energy Physics - Experiment · Physics 2019-08-14 Karl M. Ecklund

We use Omnes representations of the form factors f_+ and f_0 for exclusive semileptonic B to pi decays, paying special attention to the treatment of the B* pole and its effect on f_+. We apply them to combine experimental partial branching…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jonathan M Flynn , Juan Nieves

Inclusive semileptonic $B\to X_c \ell\bar{\nu}$ decays can be described in the Heavy Quark Expansion (HQE) and allow for a precision determination of the CKM element $|V_{cb}|$. We calculate the terms of $1/m_b^5$ and derive a ``trace…

High Energy Physics - Phenomenology · Physics 2025-02-05 Thomas Mannel , Ilija S. Milutin , K. Keri Vos

We present a measurement of the Cabibbo-Kobayashi-Maskawa matrix element |V_ub|, based on 253 fb^-1 of data collected by the Belle detector at the KEKB e^+e^- asymmetric collider. Events are tagged by fully reconstructing one of the B…

High Energy Physics - Experiment · Physics 2008-11-26 Belle Collaboration , I. Bizjak

We present a combined measurement of Rb = \Gamma(Z -> bb) / \Gamma(Z ->hadrons) and the semileptonic branching ratio of b quarks in Z decays, BR(b-> l nu X), using double-tag methods. Two analyses are performed on one million hadronic Z…

High Energy Physics - Experiment · Physics 2012-08-27 L3 Collaboration

We present a study of B semileptonic decays into charm final states based on 211.7 fb^{-1} of data collected at the \Upsilon(4S) resonance with the babar detector at the pep2 e^+e^- storage ring. Using a novel technique based on the…

High Energy Physics - Experiment · Physics 2007-05-23 The BABAR Collaboration , B. Aubert

Precision tests of the CKM mechanism and searches for new physics in the flavour sector require dedicated QCD calculations of decay widths and spectra. Significant progress has been achieved in recent years in computing inclusive B decay…

High Energy Physics - Phenomenology · Physics 2008-06-30 Einan Gardi

We present a measurement of the ratio of partial branching fractions of the semi-leptonic inclusive decays, $\overline{B} \to X_{u} \ell \overline{\nu}$ to $\overline{B} \to X_{c} \ell \overline{\nu}$, where $\ell = (e, \mu)$, using the…

High Energy Physics - Experiment · Physics 2025-06-03 Belle Collaboration , M. Hohmann , P. Urquijo , I. Adachi , H. Aihara , D. M. Asner , T. Aushev , R. Ayad , V. Babu , Sw. Banerjee , M. Bauer , J. Bennett , F. Bernlochner , M. Bessner , B. Bhuyan , T. Bilka , D. Biswas , A. Bobrov , D. Bodrov , G. Bonvicini , J. Borah , A. Bozek , M. Bračko , P. Branchini , T. E. Browder , A. Budano , M. Campajola , L. Cao , M. -C. Chang , B. G. Cheon , K. Cho , S. -K. Choi , Y. Choi , S. Das , N. Dash , G. De Nardo , G. De Pietro , R. Dhamija , J. Dingfelder , Z. Doležal , T. V. Dong , S. Dubey , P. Ecker , T. Ferber , D. Ferlewicz , A. Frey , B. G. Fulsom , V. Gaur , A. Giri , P. Goldenzweig , E. Graziani , T. Gu , K. Gudkova , C. Hadjivasiliou , O. Hartbrich , K. Hayasaka , H. Hayashii , S. Hazra , M. T. Hedges , D. Herrmann , W. -S. Hou , C. -L. Hsu , K. Inami , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , Q. P. Ji , S. Jia , Y. Jin , T. Kawasaki , C. Kiesling , D. Y. Kim , K. -H. Kim , Y. -K. Kim , K. Kinoshita , A. Korobov , E. Kovalenko , P. Križan , T. Kuhr , M. Kumar , R. Kumar , K. Kumara , Y. -J. Kwon , T. Lam , M. Laurenza , S. C. Lee , D. Levit , P. Lewis , L. K. Li , L. Li Gioi , D. Liventsev , M. Masuda , T. Matsuda , D. Matvienko , S. K. Maurya , F. Meier , M. Merola , F. Metzner , R. Mizuk , K. Miyabayashi , G. B. Mohanty , R. Mussa , M. Nakao , Z. Natkaniec , A. Natochii , L. Nayak , S. Nishida , S. Ogawa , H. Ono , P. Oskin , G. Pakhlova , S. Pardi , H. Park , J. Park , S. -H. Park , A. Passeri , S. Patra , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , T. Podobnik , E. Prencipe , M. T. Prim , M. Röhrken , M. Rozanska , G. Russo , S. Sandilya , V. Savinov , G. Schnell , C. Schwanda , A. J. Schwartz , Y. Seino , K. Senyo , W. Shan , C. Sharma , J. -G. Shiu , B. Shwartz , E. Solovieva , M. Starič , M. Sumihama , K. Sumisawa , M. Takizawa , K. Tanida , F. Tenchini , K. Trabelsi , M. Uchida , S. Uno , S. E. Vahsen , K. E. Varvell , A. Vinokurova , M. -Z. Wang , E. Won , B. D. Yabsley , W. Yan , S. B. Yang , Y. Yook , V. Zhilich , V. Zhukova

We review the experimental measurements and theoretical descriptions of leptonic and semileptonic decays of particles containing a single heavy quark, either charm or bottom. Measurements of bottom semileptonic decays are used to determine…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jeffrey D. Richman , Patricia R. Burchat

A brief review of the theoretical description of exclusive and inclusive semileptonic charm decays is given. In light of the recent experimental puzzles in leptonic charm decays, the complementary role of semileptonic modes is emphasized.…

High Energy Physics - Phenomenology · Physics 2009-09-16 Jernej F. Kamenik

We calculate the radiative corrections to the nonleptonic inclusive B decay mode $b\to c ud$ taking into account the charm quark mass. The corrections increase the decay rate by (4--8)\%, depending on the renormalization point. Using these…

High Energy Physics - Phenomenology · Physics 2009-10-28 P. Ball

Decays $B\to DP\ell^+\nu_\ell~(\ell=e,\mu,\tau)$ with the non-resonance, the charmed vector resonances, the charmed scalar resonances and the charmed tensor resonances are calculated by using the SU(3) flavor symmetry. Firstly, the decay…

High Energy Physics - Phenomenology · Physics 2024-12-03 Ru-Min Wang , Yi-Jie Zhang , Meng-Yuan Wan , Xiao-Dong Cheng , Yuan-Guo Xu

The semileptonic $B$ meson decays of the type $B \to X_u \ell \nu$ are important for measuring the magnitude of the CKM matrix element $V_{ub}$. Recent measurements of inclusive $B \to X_u e \nu_e$ and hadronically tagged $B^0 \to \pi^-…

High Energy Physics - Experiment · Physics 2021-04-19 Andrea Fodor

The principal difficulty in deducing weak interaction properties from experimental measurements of $B$-decays lies in controlling the strong interaction effects. In this talk I review the status of theoretical calculations of the amplitudes…

High Energy Physics - Phenomenology · Physics 2009-10-09 C. T. Sachrajda

We review the theory of the determination of the CKM elements Vcb and Vub. Particular attention is paid to the determination of Vcb through inclusive semileptonic B decays to charm using a moment analysis, since this has shown most progress…

High Energy Physics - Phenomenology · Physics 2007-05-23 Benjamin Grinstein

The $\tau$ polarization in semileptonic $B$ decays provides probes of new physics complementary to decay rate distributions of the three-body final state. Prior calculations for inclusive decays used a definition for the polarization axis…

High Energy Physics - Phenomenology · Physics 2023-05-24 Florian U. Bernlochner , Zoltan Ligeti , Michele Papucci , Dean J. Robinson
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