English
Related papers

Related papers: CKM Overview and Determinations from B Decays

200 papers

The combination of precise experimental measurements and theoretical predictions allows to extract Cabibbo-Kobayashi-Maskawa (CKM) matrix elements or constrain flavor changing processes in the standard model. Focusing at theoretical…

High Energy Physics - Phenomenology · Physics 2024-09-05 Oliver Witzel

We calculate the partial decay widths of the W boson at one loop in the standard model using the on-shell renormalization scheme endowed with a gauge-independent definition of the Cabibbo-Kobayashi-Maskawa (CKM) mixing matrix. We work in…

High Energy Physics - Phenomenology · Physics 2009-10-31 B. A. Kniehl , F. Madricardo , M. Steinhauser

Within the Standard Model, a review of the current determination of the sides and angles of the CKM unitarity triangle is presented, using experimental constraints from the measurements of |\epsilon_K|, |V_{ub}/V_{cb}|, \Delta m_d and from…

High Energy Physics - Phenomenology · Physics 2010-02-03 M. Ciuchini , G. D'Agostini , E. Franco , V. Lubicz , G. Martinelli , F. Parodi , P. Roudeau , A. Stocchi

We summarize selected up-to-date results related to semileptonic $B$ meson decays, namely results on the exclusive determination of the parameter $|V_{cb}|$ of the CKM matrix, on the inclusive determination of $|V_{ub}|$, and on…

High Energy Physics - Phenomenology · Physics 2018-12-04 Giulia Ricciardi

The data on high-precision flavour observables reveal certain puzzles when compared to Standard Model expectations based on a global fit of the CKM unitarity triangle and general theoretical estimates. The discussion of these tensions in…

High Energy Physics - Phenomenology · Physics 2010-11-02 Martin Jung

The study of charmless two-body decays of B mesons is currently one of the hottest topics in B physics. QCD factorization provides the theoretical framework for a systematic analysis of such decays. A global fit to B->pi K,pi pi branching…

High Energy Physics - Phenomenology · Physics 2010-11-23 Matthias Neubert

The starting point of these lectures is an introduction to the weak interactions of quarks and the Standard-Model description of CP violation, where the central role is played by the Cabibbo-Kobayashi-Maskawa matrix and the corresponding…

High Energy Physics - Phenomenology · Physics 2007-05-23 Robert Fleischer

This letter summarises the status of the global fit of the CKM parameters within the Standard Model performed by the CKMfitter group. Special attention is paid to the inputs for the CKM angles $\alpha$ and $\gamma$ and the status of…

Using the most recent determinations of several theoretical and experimental parameters, we update the Unitarity Triangle analysis in the Standard Model. The basic experimental constraints come from the measurements of epsilon_k, Vub/Vcb…

High Energy Physics - Phenomenology · Physics 2007-05-23 UTfit Collaboration , M. Bona , M. Ciuchini , E. Franco , V. Lubicz , G. Martinelli , F. Parodi , M. Pierini , P. Roudeau , C. Schiavi , L. Silvestrini , A. Stocchi

In Standard Model, CP violation arises from an irreducible complex phase in the quark mixing matrix, now under the name Cabibbo-Kobayashi-Maskawa matrix. This description has shown remarkably overall agreement with various experimental…

High Energy Physics - Phenomenology · Physics 2014-08-06 Wei Wang

A variety of CP violating asymmetries in $B^0$ decays is predicted in the Standard Model in terms of CKM (Cabibbo-Kobayashi-Maskawa) complex phases. These phases can also be determined from rate measurements of certain $B^+$ and $B^-$…

High Energy Physics - Phenomenology · Physics 2009-10-28 Michael Gronau

We discuss the problem of theoretical uncertainties in the combination of observables related to the CKM matrix elements and propose a statistically sensible method for combining them. The overall fit is performed on present data, and…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Plaszczynski , M. H Schune

The value of the V_{ud} matrix element of the Cabibbo-Kobayashi-Maskawa (CKM) matrix can be derived from nuclear superallowed beta decays, neutron decay, and pion beta decay. We survey current world data for all three. Today, the most…

Nuclear Theory · Physics 2008-11-07 I. S. Towner , J. C. Hardy

We review several aspects of the recent theoretical progress in K and B decays including the impact of the top quark discovery on rare and CP violating decays. In particular we summarize the present status of next-to-leading QCD…

High Energy Physics - Phenomenology · Physics 2009-09-25 Andrzej J. Buras

Within a specific texture of the quark mass matrix the notion of a maximal violation of the $CP$ symmetry can be defined. The experimental constraints from weak decays imply that in reality one is close to the case of maximal $CP$…

High Energy Physics - Phenomenology · Physics 2010-11-01 Harald Fritzsch , Zhi-zong Xing

In a large class of models, the only significant new physics effect on the CP asymmetries in $B \to \psi K_S$ and $B \to \pi\pi$ decays is a new contribution to the $B-\bar B$ mixing amplitude. This allows a model independent construction…

High Energy Physics - Phenomenology · Physics 2010-11-23 Yuval Grossman , Yosef Nir , Mihir P. Worah

A status report on the theory of radiative rare $B$ decays in the standard model is presented, with focus on inclusive decays $B \rightarrow X_{(s,d)}\, \gamma$ and exclusive decays $B \rightarrow (K^\ast,\omega,\rho) \, \gamma$. CP…

High Energy Physics - Phenomenology · Physics 2007-05-23 Giulia Ricciardi

We present a measurement of the Cabibbo-Kobayashi-Maskawa unitarity triangle angle $ \phi_{3} $ (also known as~$\gamma$) using a model-independent Dalitz plot analysis of \linebreak $B^+\to D\left(K_{S}^{0}h^{+}h^{-}\right)h^+$, where $D$…

High Energy Physics - Experiment · Physics 2022-03-02 Belle , Belle II Collaborations , : , F. Abudinén , L. Aggarwal , H. Ahmed , H. Aihara , N. Akopov , S. Al Said , A. Aloisio , N. Anh Ky , H. Atmacan , V. Aushev , R. Ayad , V. Babu , S. Bacher , S. Baehr , S. Bahinipati , P. Bambade , Sw. Banerjee , S. Bansal , J. Baudot , J. Becker , P. K. Behera , K. Belous , J. V. Bennett , F. U. Bernlochner , M. Bertemes , E. Bertholet , M. Bessner , S. Bettarini , F. Bianchi , T. Bilka , D. Biswas , A. Bobrov , D. Bodrov , G. Bonvicini , J. Borah , A. Bozek , M. Bračko , P. Branchini , R. A. Briere , T. E. Browder , A. Budano , S. Bussino , M. Campajola , L. Cao , G. Casarosa , C. Cecchi , P. Cheema , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , K. Chirapatpimol , H. -E. Cho , S. -J. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , L. Corona , S. Cunliffe , T. Czank , S. Das , F. Dattola , E. De La Cruz-Burelo , G. de Marino , S. K. Maurya , G. De Nardo , M. De Nuccio , G. De Pietro , R. de Sangro , M. Destefanis , S. Dey , A. De Yta-Hernandez , R. Dhamija , A. Di Canto , Z. Doležal , I. Domínguez Jiménez , T. V. Dong , M. Dorigo , D. Dossett , S. Dubey , G. Dujany , M. Eliachevitch , D. Epifanov , P. Feichtinger , D. Ferlewicz , T. Fillinger , S. Fiore , A. Fodor , F. Forti , B. G. Fulsom , A. Gabrielli , E. Ganiev , M. Garcia-Hernandez , V. Gaur , A. Gaz , R. Giordano , A. Giri , A. Glazov , R. Godang , P. Goldenzweig , B. Golob , W. Gradl , E. Graziani , D. Greenwald , T. Gu , Y. Guan , K. Gudkova , J. Guilliams , C. Hadjivasiliou , S. Halder , T. Hara , O. Hartbrich , K. Hayasaka , H. Hayashii , S. Hazra , I. Heredia de la Cruz , A. Hershenhorn , T. Higuchi , E. C. Hill , W. -S. Hou , C. -L. Hsu , T. Iijima , K. Inami , A. Ishikawa , M. Iwasaki , W. W. Jacobs , E. -J. Jang , Y. Jin , H. Junkerkalefeld , A. B. Kaliyar , K. H. Kang , R. Karl , G. Karyan , Y. Kato , C. Ketter , C. Kiesling , C. -H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , K. Kinoshita , P. Kodyš , T. Koga , S. Kohani , S. Korpar , E. Kovalenko , T. M. G. Kraetzschmar , P. Križan , P. Krokovny , T. Kuhr , J. Kumar , M. Kumar , R. Kumar , K. Kumara , A. Kuzmin , Y. -J. Kwon , S. Lacaprara , Y. -T. Lai , C. La Licata , L. Lanceri , J. S. Lange , R. Leboucher , S. C. Lee , P. Leitl , J. Li , S. X. Li , L. Li Gioi , J. Libby , K. Lieret , Z. Liptak , Q. Y. Liu , D. Liventsev , S. Longo , T. Lueck , C. Lyu , M. Maggiora , R. Maiti , S. Maity , R. Manfredi , E. Manoni , S. Marcello , A. Martini , L. Massaccesi , M. Masuda , K. Matsuoka , D. Matvienko , J. A. McKenna , F. Meier , M. Merola , F. Metzner , M. Milesi , C. Miller , K. Miyabayashi , R. Mizuk , G. B. Mohanty , N. Molina-Gonzalez , H. -G. Moser , F. Mueller , C. Murphy , R. Mussa , K. R. Nakamura , T. Nakano , M. Nakao , M. Naruki , D. Narwal , A. Natochii , L. Nayak , M. Nayak , G. Nazaryan , N. K. Nisar , S. Nishida , K. Nishimura , Y. Onishchuk , H. Ono , P. Oskin , G. Pakhlova , A. Paladino , A. Panta , E. Paoloni , K. Parham , S. -H. Park , A. Passeri , A. Pathak , S. Patra , R. Pestotnik , L. E. Piilonen , T. Podobnik , S. Pokharel , L. Polat , C. Praz , S. Prell , E. Prencipe , M. T. Prim , H. Purwar , A. Rabusov , P. Rados , S. Raiz , S. Reiter , M. Remnev , I. Ripp-Baudot , G. Rizzo , L. B. Rizzuto , S. H. Robertson , M. Röhrken , J. M. Roney , A. Rostomyan , N. Rout , D. Sahoo , D. A. Sanders , S. Sandilya , L. Santelj , Y. Sato , V. Savinov , B. Scavino , G. Schnell , J. Schueler , A. J. Schwartz , Y. Seino , A. Selce , K. Senyo , M. E. Sevior , M. Shapkin , C. Sharma , T. Shillington , B. Shwartz , A. Sibidanov , F. Simon , J. B. Singh , A. Soffer , E. Solovieva , S. Spataro , B. Spruck , S. Stefkova , Z. S. Stottler , R. Stroili , K. Sumisawa , W. Sutcliffe , S. Y. Suzuki , M. Tabata , M. Takizawa , K. Tanida , F. Tenchini , R. Tiwary , D. Tonelli , E. Torassa , K. Trabelsi , M. Uchida , I. Ueda , T. Uglov , K. Uno , S. Uno , Y. Ushiroda , S. E. Vahsen , R. van Tonder , K. E. Varvell , A. Vinokurova , L. Vitale , H. M. Wakeling , E. Wang , M. -Z. Wang , X. L. Wang , A. Warburton , S. Watanuki , O. Werbycka , C. Wessel , E. Won , B. D. Yabsley , W. Yan , H. Ye , K. Yoshihara , Y. Yusa , L. Zani , Y. Zhai , Y. Zhang , V. Zhilich , Q. D. Zhou , X. Y. Zhou , V. I. Zhukova

These lectures contain an elementary introduction to heavy quark symmetry and the heavy quark expansion. Applications such as the expansion of heavy meson decay constants and the treatment of inclusive and exclusive semileptonic B decays…

High Energy Physics - Phenomenology · Physics 2017-08-23 Adam F. Falk

We discuss one-particle inclusive B decays in the limit of heavy b and c quarks. Using the large-N_C limit we factorize the non-leptonic matrix elements, and we employ a short distance expansion. Modeling the remaining nonperturbative…

High Energy Physics - Phenomenology · Physics 2011-01-25 Xavier Calmet , Thomas Mannel , Ingo Schwarze