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Related papers: $\beta(\phi_1)$ from $ B $ Decays to Charm

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We report measurements of time-dependent CP asymmetries related to the CKM angle $\beta/\phi_1$, using decays of neutral B mesons to charmonium, open charm and in $b\to s$ loop processes. A preliminary measurement of time-dependent CP…

High Energy Physics - Experiment · Physics 2019-08-14 J. Ocariz

It is well known that $\sin(2\beta)$, where $\beta$ is one of the angles of the unitarity triangle of the CKM matrix, can be determined in a theoretically clean way by measuring mixing-induced CP violation in the decay $B_d \to J/\psi K_S$.…

High Energy Physics - Phenomenology · Physics 2009-10-31 Amol Dighe , Isard Dunietz , Robert Fleischer

A new method for model-independent measurement of the CKM angle $\beta$ is proposed, that employs time-dependent analysis of flavour-tagged $B^0\to D\pi^+\pi^-$ decays with $D$ meson decays into CP-specific and~$K_S^0\pi^+\pi^-$ final…

High Energy Physics - Phenomenology · Physics 2018-04-05 A. Bondar , A. Kuzmin , V. Vorobyev

In this article we will review recent BABAR measurements of Unitarity Triangle angle beta in B meson decays to charm and charmonium.

High Energy Physics - Experiment · Physics 2008-11-26 BABAR Collaboration , M. Bomben

We summarize the results presented in Working Group 5 (WG5) of the CKM 2006 Workshop in Nagoya. The charge of WG5 was to discuss the measurements of unitarity triangle angles $\beta/\phi_1$ and $\gamma/\phi_3$ from $B$-meson decays…

High Energy Physics - Phenomenology · Physics 2007-06-29 G. Cavoto , R. Fleischer , K. Trabelsi , J. Zupan

In this talk we show that, unlike other pure $b\to d$ penguin processes, the decay $\bs(t)\to\phi\ks$ is dominated by a single amplitude, that of the internal $t$-quark. Thus, the indirect CP asymmetry in this decay probes $\sin 2\beta$.…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alakabha Datta , C. S. Kim , David London

We consider the possibility of measuring both $\sin (2 \beta)$ and $\cos (2 \beta)$ in the KM unitarity triangle using the process $B^0 \to D^{*+}D^{*-}K_s$. This decay mode has a higher branching fraction (O(1%)) than the mode $B^0 \to…

High Energy Physics - Phenomenology · Physics 2009-10-31 T. E. Browder , A. Datta , Patrick. J. O'Donnell , S. Pakvasa

I describe the experimental determination of the CKM angle beta from measurements of the decay time separation delta t between B0 mesons produced as B Bbar pairs in e+e- annihilation. The current results from leading and non-leading decay…

High Energy Physics - Experiment · Physics 2010-11-23 W. T. Ford

Because the Bd -> J/psi Ks asymmetry determines only sin(2 beta), a discrete ambiguity in the true value of beta remains. This note reviews how the ambiguity can be removed. Extractions of the CKM angle alpha are discussed next. Some of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Isard Dunietz

The CKM angle $\phi_3$ is less precisely known than the angle $\phi_1$ and the only one that is accessible with tree-level decays in a theoretically clean way. The key method to measure $\phi_3$ is through the interference between $B^+\to…

High Energy Physics - Experiment · Physics 2018-12-11 P. K. Resmi

In this article I report on new and updated measurements of the CP-violating parameter beta (phi_1), which is related to the phase of the Cabibbo-Kobayashi-Maskawa (CKM) quark-mixing matrix of the electroweak interaction. Over the past few…

High Energy Physics - Experiment · Physics 2009-11-11 Rainer Bartoldus

The Belle experiment has measured branching fractions and CP asymmetries for the charmless decays B0->pi+pi- and B0->rho+-pi-+. From these measurements, constraints upon the CKM angle phi_2 can be obtained. These constraints indicate that…

High Energy Physics - Experiment · Physics 2019-08-14 A. J. Schwartz

We report a determination of the CKM angle $\phi_{3}$, also known as $\gamma$, from a combination of measurements using samples of up to 711~fb$^{-1}$ from the Belle experiment and up to 362~fb$^{-1}$ from the Belle II experiment. We…

High Energy Physics - Experiment · Physics 2024-08-13 Belle , Belle II Collaborations , : , I. Adachi , L. Aggarwal , H. Aihara , N. Akopov , A. Aloisio , S. Al Said , N. Anh Ky , D. M. Asner , H. Atmacan , V. Aushev , M. Aversano , R. Ayad , V. Babu , H. Bae , S. Bahinipati , P. Bambade , Sw. Banerjee , S. Bansal , M. Barrett , J. Baudot , A. Baur , A. Beaubien , F. Becherer , J. Becker , K. Belous , J. V. Bennett , F. U. Bernlochner , V. Bertacchi , M. Bertemes , E. Bertholet , M. Bessner , S. Bettarini , B. Bhuyan , F. Bianchi , L. Bierwirth , T. Bilka , S. Bilokin , D. Biswas , A. Bobrov , D. Bodrov , A. Bolz , A. Bondar , A. Bozek , M. Bračko , P. Branchini , R. A. Briere , T. E. Browder , A. Budano , S. Bussino , M. Campajola , L. Cao , G. Casarosa , C. Cecchi , J. Cerasoli , M. -C. Chang , P. Chang , R. Cheaib , P. Cheema , B. G. Cheon , K. Chilikin , K. Chirapatpimol , H. -E. Cho , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , L. Corona , S. Das , F. Dattola , E. De La Cruz-Burelo , S. A. De La Motte , G. de Marino , G. De Nardo , M. De Nuccio , G. De Pietro , R. de Sangro , M. Destefanis , R. Dhamija , A. Di Canto , F. Di Capua , J. Dingfelder , Z. Doležal , T. V. Dong , M. Dorigo , K. Dort , D. Dossett , S. Dreyer , S. Dubey , G. Dujany , P. Ecker , M. Eliachevitch , D. Epifanov , P. Feichtinger , T. Ferber , D. Ferlewicz , T. Fillinger , G. Finocchiaro , A. Fodor , F. Forti , A. Frey , B. G. Fulsom , A. Gabrielli , E. Ganiev , M. Garcia-Hernandez , R. Garg , G. Gaudino , V. Gaur , A. Gaz , A. Gellrich , G. Ghevondyan , D. Ghosh , H. Ghumaryan , G. Giakoustidis , R. Giordano , A. Giri , B. Gobbo , R. Godang , O. Gogota , P. Goldenzweig , W. Gradl , T. Grammatico , S. Granderath , E. Graziani , D. Greenwald , Z. Gruberová , T. Gu , Y. Guan , K. Gudkova , S. Halder , Y. Han , T. Hara , H. Hayashii , S. Hazra , M. T. Hedges , A. Heidelbach , I. Heredia de la Cruz , M. Hernández Villanueva , T. Higuchi , M. Hoek , M. Hohmann , P. Horak , C. -L. Hsu , T. Humair , T. Iijima , K. Inami , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , P. Jackson , W. W. Jacobs , E. -J. Jang , Q. P. Ji , S. Jia , Y. Jin , H. Junkerkalefeld , D. Kalita , A. B. Kaliyar , J. Kandra , T. Kawasaki , F. Keil , C. Kiesling , C. -H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , H. Kindo , K. Kinoshita , P. Kodyš , T. Koga , S. Kohani , K. Kojima , A. Korobov , S. Korpar , E. Kovalenko , R. Kowalewski , T. M. G. Kraetzschmar , P. Križan , P. Krokovny , T. Kuhr , J. Kumar , M. Kumar , R. Kumar , K. Kumara , T. Kunigo , A. Kuzmin , Y. -J. Kwon , S. Lacaprara , Y. -T. Lai , T. Lam , L. Lanceri , J. S. Lange , M. Laurenza , M. J. Lee , D. Levit , P. M. Lewis , C. Li , L. K. Li , Y. Li , Y. B. Li , J. Libby , M. H. Liu , Q. Y. Liu , Z. Q. Liu , D. Liventsev , S. Longo , T. Lueck , C. Lyu , Y. Ma , M. Maggiora , S. P. Maharana , R. Maiti , S. Maity , G. Mancinelli , R. Manfredi , E. Manoni , M. Mantovano , D. Marcantonio , S. Marcello , C. Marinas , L. Martel , C. Martellini , A. Martini , T. Martinov , L. Massaccesi , M. Masuda , D. Matvienko , S. K. Maurya , J. A. McKenna , R. Mehta , F. Meier , M. Merola , F. Metzner , C. Miller , M. Mirra , K. Miyabayashi , H. Miyake , G. B. Mohanty , N. Molina-Gonzalez , S. Mondal , S. Moneta , H. -G. Moser , M. Mrvar , R. Mussa , I. Nakamura , K. R. Nakamura , M. Nakao , Y. Nakazawa , A. Narimani Charan , M. Naruki , D. Narwal , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , G. Nazaryan , M. Neu , C. Niebuhr , S. Nishida , S. Ogawa , Y. Onishchuk , H. Ono , P. Oskin , F. Otani , P. Pakhlov , G. Pakhlova , A. Panta , S. Pardi , K. Parham , H. Park , S. -H. Park , A. Passeri , S. Patra , S. Paul , T. K. Pedlar , R. Peschke , R. Pestotnik , M. Piccolo , L. E. Piilonen , G. Pinna Angioni , P. L. M. Podesta-Lerma , T. Podobnik , S. Pokharel , C. Praz , S. Prell , E. Prencipe , M. T. Prim , H. Purwar , P. Rados , G. Raeuber , S. Raiz , N. Rauls , M. Reif , S. Reiter , M. Remnev , I. Ripp-Baudot , G. Rizzo , S. H. Robertson , M. Roehrken , J. M. Roney , A. Rostomyan , N. Rout , G. Russo , D. A. Sanders , S. Sandilya , L. Santelj , Y. Sato , V. Savinov , B. Scavino , C. Schmitt , G. Schnell , C. Schwanda , M. Schwickardi , Y. Seino , A. Selce , K. Senyo , J. Serrano , M. E. Sevior , C. Sfienti , W. Shan , X. D. Shi , T. Shillington , T. Shimasaki , J. -G. Shiu , D. Shtol , B. Shwartz , A. Sibidanov , F. Simon , J. B. Singh , J. Skorupa , R. J. Sobie , M. Sobotzik , A. Soffer , A. Sokolov , E. Solovieva , S. Spataro , B. Spruck , M. Starič , P. Stavroulakis , S. Stefkova , R. Stroili , M. Sumihama , K. Sumisawa , W. Sutcliffe , N. Suwonjandee , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , O. Tittel , R. Tiwary , D. Tonelli , E. Torassa , K. Trabelsi , I. Tsaklidis , M. Uchida , I. Ueda , Y. Uematsu , T. Uglov , K. Unger , Y. Unno , K. Uno , S. Uno , P. Urquijo , Y. Ushiroda , S. E. Vahsen , R. van Tonder , K. E. Varvell , M. Veronesi , A. Vinokurova , V. S. Vismaya , L. Vitale , V. Vobbilisetti , R. Volpe , B. Wach , M. Wakai , S. Wallner , E. Wang , M. -Z. Wang , X. L. Wang , Z. Wang , A. Warburton , S. Watanuki , C. Wessel , E. Won , X. P. Xu , B. D. Yabsley , S. Yamada , W. Yan , S. B. Yang , J. Yelton , J. H. Yin , K. Yoshihara , C. Z. Yuan , B. Zhang , Y. Zhang , V. Zhilich , Q. D. Zhou , V. I. Zhukova

We give an overview of various determinations of $\gamma/\phi_3$ with the help of $B_s$ decays into charmed final states, distinguishing between transitions with tree and penguin contributions and pure tree decays. In the corresponding…

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

We show that the CKM phase $2 \beta+\gamma$ can be extracted from measurement of the time dependent rates in the decays $\bar{B}^0 \to D^{(*)\pm} M^\mp$ and $B^0 \to D^{(*)\pm} M^\mp$, where $M=a_0$, $\pi(1300)$, $b_1$, $a_2$, $\pi_2$,…

High Energy Physics - Phenomenology · Physics 2014-11-17 M. Diehl , G. Hiller

The Belle experiment has used several methods to measure or constrain the angles phi_1, phi_2, and phi_3 (or beta, alpha, and gamma) of the CKM unitarity triangle. The results are sin(2phi_1) = 0.728 \pm 0.056 (stat) \pm 0.023 (syst) or…

High Energy Physics - Experiment · Physics 2007-05-23 A. J. Schwartz

We present a feasibility study of a method to measure the cosine of twice the CKM Unitarity Triangle angle beta using a time-dependent Dalitz plot analysis of B0 -> D pi+ pi- decays, where the neutral D meson is reconstructed in decays to…

High Energy Physics - Phenomenology · Physics 2008-12-18 Thomas Latham , Tim Gershon

The measurement of $\sin 2 \beta$ is discussed within and beyond the standard model. In the presence of new physics, the angle $\beta$ extracted from the global fit(denoted by $\beta^{SM}_{fit}$) and the one extracted from $B\to J/\psi K_S$…

High Energy Physics - Phenomenology · Physics 2014-11-17 Yue-Liang Wu , Yu-Feng Zhou

The recent Belle collaboration measurements of B decays to open and hidden charm are discussed. Color-suppressed decay branching fractions are measured with an improved accuracy. The branching fractions of the $\bar{B}^0 \to D_s^+ K^-$ and…

High Energy Physics - Experiment · Physics 2017-08-23 A. Drutskoy

A doubly CKM-suppressed amplitude in $B^0\to J/\psi K_S$ leads to corrections in CP asymmetries $S = \sin 2\beta, C=0$, which may be enhanced by long-distance rescattering. It has been suggested that this enhancement may lead to several…

High Energy Physics - Phenomenology · Physics 2009-10-16 Michael Gronau , Jonathan L. Rosner
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