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Related papers: Three loop calculations and inclusive $V_{cb}$

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I identify a source of Lambda_{QCD}/m_Q corrections to the assumption of quark-hadron duality in the application of heavy quark methods to inclusive heavy quark semileptonic decays Q->q l nu_l. These corrections could substantially affect…

High Energy Physics - Phenomenology · Physics 2007-05-23 Nathan Isgur

The Heavy Quark Expansion (HQE) is the major tool to perform calculations for inclusive semileptonic $B\to X_cl\bar{\nu}$ and, consequently, for precision determinations of the CKM matrix element $V_{cb}$. To further improve precision, we…

High Energy Physics - Phenomenology · Physics 2024-10-22 Ilija S. Milutin , Thomas Mannel , K. Keri Vos

The calculation of the moments in inclusive B meson semileptonic decays is upgraded to O(alphas^2). The first three moments of the lepton energy and invariant hadronic mass distributions are computed for arbitrary cuts on the lepton energy…

High Energy Physics - Phenomenology · Physics 2015-05-28 Paolo Gambino

We demonstrate the feasibility of determining the strong coupling constant, $\alpha_s$, from the inclusive semileptonic decay width of $B$ mesons. We express the semileptonic $B$ decay width as a function of $\alpha_s(5\mathrm{\,GeV})$, the…

High Energy Physics - Phenomenology · Physics 2025-10-07 Yuzhi Che , Long Chen , Jinfei Wu , Xinchou Lou , Xiang Chen , Xin Guan , Yan-Qing Ma , Manqi Ruan

The Belle experiment at the KEKB asymmetric energy e+e- collider recorded large data sets of both, B and Bs decays. Semileptonic decays B(s) -> X l nu (l = electron or muon) constitute approximately one fifth of the total decay width of…

High Energy Physics - Experiment · Physics 2013-05-17 Christian Oswald

The decay width of b to c,c,c,l,nu has been computed as an expansion in limit (1- 3*(m_c/m_b)) << 1 with zero lepton invariant mass. Considering O(alpha_s^2) corrections to b to c,l,nu with zero invariant lepton mass, inclusion of our…

High Energy Physics - Phenomenology · Physics 2007-05-23 Matthew Dowling , Alexey Pak

A summary of the calculation of the color-planar and complete light quark contributions to the massive three-loop form factors is presented. Here a novel calculation method for the Feynman integrals is used, solving general uni-variate…

High Energy Physics - Phenomenology · Physics 2019-06-14 J. Ablinger , J. Blümlein , P. Marquard , N. Rana , C. Schneider

We present the first analytic results of N$^3$LO QCD corrections to the top-quark decay width. We focus on the dominant leading color contribution, which includes light-quark loops. At NNLO, this dominant contribution accounts for 95% of…

High Energy Physics - Phenomenology · Physics 2024-04-26 Long-Bin Chen , Hai Tao Li , Zhao Li , Jian Wang , Yefan Wang , Quan-feng Wu

We present recent results on newly calculated 2- and 3-loop contributions to the heavy quark parts of the structure functions in deep-inelastic scattering due to charm and bottom.

High Energy Physics - Phenomenology · Physics 2016-09-21 J. Ablinger , A. Behring , J. Blümlein , G. Falcioni , A. De Freitas , A. Hasselhuhn , A. von Manteuffel , M. Round , C. Schneider , F. Wißbrock

We demonstrate that Borel QCD sum rules for heavy-light currents entail a very strong correlation between the $b$-quark mass $m_b$ and the $B$-meson decay constant $f_B,$ that is, $\delta f_B/f_B\approx-8\delta m_b/m_b.$ By starting from…

High Energy Physics - Phenomenology · Physics 2014-04-15 Wolfgang Lucha , Dmitri Melikhov , Silvano Simula

The first simultaneous determination of the absolute value of the Cabibbo-Kobayashi-Maskawa matrix element $V_{ub}$ using inclusive and exclusive decays is performed with the full Belle data set at the $\Upsilon(4S)$ resonance,…

High Energy Physics - Experiment · Physics 2023-11-23 Belle Collaboration , L. Cao , F. Bernlochner , K. Tackmann , I. Adachi , H. Aihara , S. Al Said , D. M. Asner , H. Atmacan , T. Aushev , R. Ayad , V. Babu , S. Bahinipati , Sw. Banerjee , P. Behera , K. Belous , J. Bennett , M. Bessner , B. Bhuyan , T. Bilka , D. Biswas , A. Bobrov , D. Bodrov , J. Borah , A. Bozek , M. Bračko , P. Branchini , T. E. Browder , A. Budano , M. Campajola , D. Červenkov , M. -C. Chang , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , S. Cunliffe , S. Das , G. de Marino , G. De Nardo , G. De Pietro , R. Dhamija , F. Di Capua , J. Dingfelder , Z. Doležal , T. V. Dong , T. Ferber , D. Ferlewicz , A. Frey , B. G. Fulsom , V. Gaur , A. Garmash , A. Giri , P. Goldenzweig , E. Graziani , T. Gu , Y. Guan , K. Gudkova , C. Hadjivasiliou , S. Halder , T. Hara , O. Hartbrich , K. Hayasaka , H. Hayashii , M. T. Hedges , D. Herrmann , W. -S. Hou , C. -L. Hsu , T. Iijima , K. Inami , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , E. -J. Jang , S. Jia , Y. Jin , K. K. Joo , D. Kalita , K. H. Kang , C. Kiesling , C. H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , K. Kinoshita , P. Kodyš , T. Konno , A. Korobov , S. Korpar , E. Kovalenko , P. Križan , P. Krokovny , T. Kuhr , R. Kumar , K. Kumara , A. Kuzmin , Y. -J. Kwon , J. S. Lange , M. Laurenza , S. C. Lee , P. Lewis , J. Li , L. K. Li , Y. Li , J. Libby , Y. -R. Lin , D. Liventsev , T. Luo , Y. Ma , A. Martini , M. Masuda , T. Matsuda , D. Matvienko , S. K. Maurya , F. Meier , M. Merola , F. Metzner , K. Miyabayashi , R. Mizuk , G. B. Mohanty , M. Mrvar , R. Mussa , I. Nakamura , M. Nakao , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , N. K. Nisar , S. Nishida , K. Ogawa , S. Ogawa , H. Ono , P. Oskin , P. Pakhlov , G. Pakhlova , T. Pang , 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 , N. Rout , M. Rozanska , G. Russo , S. Sandilya , A. Sangal , L. Santelj , V. Savinov , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , M. E. Sevior , W. Shan , M. Shapkin , C. Sharma , C. P. Shen , J. -G. Shiu , B. Shwartz , A. Sokolov , E. Solovieva , M. Starič , Z. S. Stottler , M. Sumihama , W. Sutcliffe , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , R. Tiwary , K. Trabelsi , M. Uchida , T. Uglov , Y. Unno , K. Uno , S. Uno , Y. Ushiroda , Y. Usov , S. E. Vahsen , G. Varner , K. E. Varvell , A. Vossen , D. Wang , E. Wang , M. -Z. Wang , S. Watanuki , O. Werbycka , E. Won , X. Xu , B. D. Yabsley , W. Yan , S. B. Yang , J. H. Yin , Y. Yook , Y. Yusa , Z. P. Zhang , V. Zhilich , V. Zhukova

We report updates on two analyses of inclusive semileptonic B decays based on a dataset of 89 million BB events recorded with the BABAR detector at the Y(4S) resonance. Events are selected by fully reconstructing the decay of one B meson…

High Energy Physics - Experiment · Physics 2019-08-14 Urs Langenegger

We determine $|V_{cb}|$ from the inclusive semileptonic decay width of the $B$ meson with the known N$^3$LO perturbative coefficients for the first time in the $\overline{\mathrm{MS}}$ mass scheme. We make use of a recently developed…

High Energy Physics - Phenomenology · Physics 2023-10-31 Yuuki Hayashi , Go Mishima , Yukinari Sumino , Hiromasa Takaura

By analyzing B -> X_u l nu_l spectra with a model based on soft-gluon resummation and an analytic time-like QCD coupling, we obtain |V_ub| = (3.76 +-0.13 +- 0.22)*10^(-3), where the first and the second error refers to experimental and…

High Energy Physics - Phenomenology · Physics 2009-09-27 Ugo Aglietti , Francesca Di Lodovico , Giancarlo Ferrera , Giulia Ricciardi

We compute the effects of a finite $W$ boson mass on the inclusive $b\rightarrow c \ell \nu$ decay rate and the semileptonic moments. To this end we keep terms of $\mathcal{O}\left(q^2/m_W^2 \right)$ when integrating out the $W$ boson in…

High Energy Physics - Phenomenology · Physics 2023-05-10 Dante Bigi , Sandro Mächler

We compute one-loop QCD corrections to the triple differential width of the inclusive decay $\bar{B} \to X_c \ell \bar{\nu}_\ell$ including contributions from all relevant dimension-six operators in the Weak Effective Theory (WET), at…

High Energy Physics - Phenomenology · Physics 2026-01-23 Alexandre Carvunis , Gael Finauri

Nonperturbative QCD contributions to the inclusive semileptonic decay of the B meson consist of the dynamic and kinematic components. We calculate the decay width in an approach based on the light-cone expansion and the heavy quark…

High Energy Physics - Phenomenology · Physics 2014-11-17 Changhao Jin

The current status of the determinations of CKM matrix element |Vub| via exclusive and inclusive charmless semileptonic B decays is reviewed.

High Energy Physics - Experiment · Physics 2009-03-31 Antonio Petrella

We compute the $O(\alpha_s)$ corrections to the Wilson coefficients of the dimension five operators in inclusive semileptonic $B$ decays in the limit of a massless final quark. Our calculation agrees with reparameterization invariance and…

High Energy Physics - Phenomenology · Physics 2022-07-15 Bernat Capdevila , Paolo Gambino , Soumitra Nandi

We present the measurement of the first to fourth order moments of the four-momentum transfer squared, $q^{2}$, of inclusive $B \rightarrow X_{c} \ell \nu$ decays using the full Belle data set consisting of $711~\rm fb^{-1}$ of integrated…

High Energy Physics - Experiment · Physics 2021-05-18 Raynette van Tonder