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Related papers: CKM Parameters and Rare B Decays

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The potential for a precise measurement of the Unitarity Triangle angle $\gamma$ in future experiments from the decay $B^0 \to DK^{*0}$ is well-known. It has recently been suggested that the sensitivity can be significantly enhanced by…

High Energy Physics - Phenomenology · Physics 2009-11-10 Tim Gershon , Mike Williams

Some recent Babar results on semileptonic decays are presented. They focus on the determination of the CKM matrix elements |V_{ub}| and |V_{cb}| in inclusive and exclusive b --> u l nu and b--> c l nu decays, and on form factors measurement…

High Energy Physics - Experiment · Physics 2009-04-02 Justine Serrano

We review the experimental status of the angles of the Unitarity Triangle of the CKM matrix, as measured by the BABAR and Belle experiments.

High Energy Physics - Experiment · Physics 2019-08-14 Giuseppe Finocchiaro

This paper describes the determination of the direct CP observables R_cp and A_cp, related to the CKM angle gamma, using B- to D0 K- decays in 1.0 inverse fb of data collected with the CDF II detector. This is the first measurement of these…

High Energy Physics - Experiment · Physics 2019-08-13 Karen Gibson

We present expressions for shape variables of B decay distributions in several different mass schemes, to order $\alpha_s^2\beta_0$ and (Lambda_{QCD}/mb)^3. Such observables are sensitive to the b quark mass and matrix elements in the heavy…

High Energy Physics - Phenomenology · Physics 2008-11-26 Christian W. Bauer , Zoltan Ligeti , Michael Luke , Aneesh V. Manohar

These lectures describe CP violation and rare decays of K and B mesons and consist of ten chapters: i) Grand view of the field including CKM matrix and the unitarity triangle, ii) General aspects of the theoretical framework, iii)…

High Energy Physics - Phenomenology · Physics 2007-05-23 Andrzej J. Buras

The decay B^0 -> DK^{*0} is well-known to provide excellent potential for a precise measurement of the Unitarity Triangle angle gamma in future experiments. It is noted that the sensitivity can be significantly enhanced by studying the…

High Energy Physics - Phenomenology · Physics 2009-03-24 Tim Gershon

There are two main ways of looking for new physics, direct searches and precision measurements. The latter are sensitive to a broader spectrum of models; they also can be sensitive to higher energy scales than what can be reached through…

High Energy Physics - Experiment · Physics 2024-05-21 Angel F. Campoverde

The precise measurement of the CKM angle $\phi_3$ is important to further test the Standard Model description of $CP$ violation. The small values of the branching fractions of the decays involved in the measurement limits the precision,…

High Energy Physics - Experiment · Physics 2020-02-19 P. K. Resmi

The rare decays {$B^- \to \tau \bar\nu$}, \mbox{$B \to \tau^+ \tau^-$}, {$b \to X \nu \bar\nu$} and \mbox{$b \to X \tau^+ \tau^-$} all contain third generation leptons in the final state, and hence are sensitive to new physics that couples…

High Energy Physics - Phenomenology · Physics 2008-11-26 Dafne Guetta , Enrico Nardi

Semileptonic decays of charged and neutral $B$ mesons play a critical role in the determination of the magnitudes of the CKM-matrix elements $V_{cb}$ and $V_{ub}$, and in the test of the lepton universality which is a basic assumption of…

High Energy Physics - Experiment · Physics 2018-05-01 Long-Ke Li , Chang-Zheng Yuan

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

Use of semi-leptonic decays has become standard in constraining the Unitarity Triangle. Bearing in mind that precise calculations of these are very challenging, we propose an entirely new approach. In particular the |Vcb| + epsilon_K…

High Energy Physics - Phenomenology · Physics 2014-11-20 E. Lunghi , A. Soni

The most recent measurements of the observables $R_{D^{(*)}}$ are in tension with the Standard Model offering hints of New Physics in $b\rightarrow c \ell \bar{\nu}_{\ell}$ transitions. Motivated by these results, in this work we present an…

High Energy Physics - Phenomenology · Physics 2018-12-14 Giovanni Banelli , Robert Fleischer , Ruben Jaarsma , Gilberto Tetlalmatzi-Xolocotzi

We discuss precision tests of the standard model in radiative and semileptonic rare B-decays and CP-violating asymmetries, and possible signatures of supersymmetry in these processes. Motivated by current data, and with an eye on the…

High Energy Physics - Phenomenology · Physics 2017-08-23 A. Ali

The values of the elements of the Cabibbo-Kobayashi-Maskawa matrix are constrained by direct and indirect measurements. A fit to experimental data and theory calculations allows the indirect determination of the vertex and angles of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Salvatore Mele

A review of the current status of the Cabibbo-Kobayashi-Maskawa matrix ($V_{CKM}$) is presented and a special emphasis is put on the determination of the $\rho$ and $\eta$ parameters. From this study it follows that, in the Standard Model,…

High Energy Physics - Phenomenology · Physics 2009-05-11 P. Paganini , F. Parodi , P. Roudeau , A. Stocchi

Measurements of angular correlations between initial and final particles in $\beta$ decay remain one of the most promising ways of probing the Standard Model and looking for new physics. As experiments reach unprecedented precision well…

Nuclear Theory · Physics 2020-10-07 Leendert Hayen , Albert R. Young

We present a new measurement of the CKM matrix element $|V_{cb}|$ from $B^{0} \to D^{*-} \ell^+ \nu_\ell$ decays, reconstructed with the full Belle data set of $711 \, \rm fb^{-1}$ integrated luminosity. Two form factor parameterizations,…

High Energy Physics - Experiment · Physics 2019-09-25 E. Waheed , P. Urquijo , I. Adachi , K. Adamczyk , H. Aihara , S. Al Said , D. M. Asner , H. Atmacan , T. Aushev , R. Ayad , V. Babu , I. Badhrees , V. Bansal , P. Behera , C. Beleno , F. Bernlochner , B. Bhuyan , T. Bilka , J. Biswal , A. Bobrov , G. Bonvicini , A. Bozek , M. Bracko , T. E. Browder , M. Campajola , D. Cervenkov , P. Chang , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , S. Cunliffe , S. Di Carlo , Z. Dolezal , T. V. Dong , D. Dossett , S. Eidelman , D. Epifanov , J. E. Fast , B. G. Fulsom , R. Garg , V. Gaur , A. Garmash , A. Giri , P. Goldenzweig , B. Golob , O. Grzymkowska , J. Haba , T. Hara , K. Hayasaka , H. Hayashii , M. T. Hedges , W. -S. Hou , C. -L. Hsu , T. Iijima , K. Inami , G. Inguglia , A. Ishikawa , M. Iwasaki , Y. Iwasaki , W. W. Jacobs , H. B. Jeon , S. Jia , Y. Jin , D. Joffe , K. K. Joo , J. Kahn , A. B. Kaliyar , G. Karyan , T. Kawasaki , C. H. Kim , D. Y. Kim , K. T. Kim , S. H. Kim , K. Kinoshita , P. Kodys , S. Korpar , D. Kotchetkov , P. Krizan , R. Kroeger , P. Krokovny , T. Kuhr , R. Kulasiri , A. Kuzmin , Y. -J. Kwon , J. S. Lange , J. Y. Lee , S. C. Lee , C. H. Li , L. K. Li , Y. B. Li , L. Li Gioi , J. Libby , K. Lieret , D. Liventsev , P. -C. Lu , T. Luo , J. MacNaughton , M. Masuda , D. Matvienko , M. Merola , F. Metzner , K. Miyabayashi , H. Miyata , R. Mizuk , G. B. Mohanty , T. Mori , R. Mussa , I. Nakamura , M. Nakao , K. J. Nath , Z. Natkaniec , M. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , K. Nishimura , S. Ogawa , H. Ono , P. Pakhlov , G. Pakhlova , B. Pal , S. Pardi , H. Park , S. -H. Park , S. Paul , R. Pestotnik , L. E. Piilonen , V. Popov , E. Prencipe , M. Prim , A. Rostomyan , G. Russo , Y. Sakai , M. Salehi , S. Sandilya , T. Sanuki , V. Savinov , O. Schneider , G. Schnell , J. Schueler , C. Schwanda , Y. Seino , K. Senyo , O. Seon , M. E. Sevior , V. Shebalin , C. P. Shen , J. -G. Shiu , B. Shwartz , F. Simon , A. Sokolov , E. Solovieva , S. Stanic , M. Staric , Z. S. Stottler , J. F. Strube , T. Sumiyoshi , M. Takizawa , K. Tanida , F. Tenchini , K. Trabelsi , M. Uchida , T. Uglov , Y. Unno , S. Uno , Y. Usov , G. Varner , K. E. Varvell , A. Vinokurova , A. Vossen , C. H. Wang , M. -Z. Wang , P. Wang , E. Won , S. B. Yang , H. Ye , Y. Yusa , Z. P. Zhang , V. Zhilich , V. Zhukova

A method is described which, under the assumption of SU(3) symmetry, allows one to determine the angle gamma=Arg(Vub^*) of the unitarity triangle from time-independent measurements of the branching ratios for the decays B^+ -> pi^0 K^+ and…

High Energy Physics - Phenomenology · Physics 2010-11-23 Matthias Neubert , Jonathan L. Rosner