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Related papers: $\sin 2\beta$ from $K\to\pi\nu\bar\nu$

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We report new measurements of the decays $B\to\rho^+ \gamma$, $B \to \rho^0 \gamma$ and $B \to \omega\gamma$ using a data sample of $657 \times 10^6$ $B$ meson pairs accumulated with the Belle detector at the KEKB $e^+ e^-$ collider. We…

High Energy Physics - Experiment · Physics 2019-08-13 N. Taniguchi , M. Nakao , S. Nishida

We (re)examine CP violation in the decays B_d -> D K_s, where D represents D^0, D(bar), or one of their excited states. The quantity $\sin^2(2\beta + \gamma)$ can be extracted from the time-dependent rates for $B_d(t) -> {\bar D}^{**0} K_s$…

High Energy Physics - Phenomenology · Physics 2014-11-17 B. Kayser , D. London

The $\Delta S = 2$ $b \to \bar d ss$ transition proceeds via the box - diagram in the Standard Model with a branching ratio calculated to be below $10^{-11}$, thus providing an appropriate testing ground for physics beyond the Standard…

High Energy Physics - Phenomenology · Physics 2014-11-17 S. Fajfer , P. Singer

The approximate symmetry of the strong interactions under isospin transformations is among the most precise tools available to control hadronic matrix elements. It is crucial in extracting fundamental parameters, but also provides avenues…

High Energy Physics - Phenomenology · Physics 2015-12-16 Martin Jung

Decay rates and time-dependent and direct CP asymmetries in the decays $B^0\to K^+K^-K_{S(L)}$ and $K_S K_S K_{S(L)}$ are studied. Resonant and nonresonant contributions to the three-body decays are carefully investigated. Nonresonant…

High Energy Physics - Phenomenology · Physics 2014-11-18 Hai-Yang Cheng , Chun-Khiang Chua , Amarjit Soni

By employing the QCD factorization approach, we calculated the next-to-leading order new physics contributions to the branching ratios, CP asymmetries, isospin and U-spin symmetry breaking of the exclusive decays $B \to V \gamma$ ($V=K^*,…

High Energy Physics - Phenomenology · Physics 2009-11-10 Zhenjun Xiao , Ci Zhuang

In the K and Bd systems, indirect CP violation is quantified by the parameters epsilon_K and sin 2beta respectively. Within the Standard Model, the uniqueness of the CP violating phase implies that the measurement of either between…

High Energy Physics - Phenomenology · Physics 2011-02-15 Diego Guadagnoli

We reemphasize the strong dependence of the branching ratios $B(K^+\to\pi^+\nu\bar\nu)$ and $B(K_L\to\pi^0\nu\bar\nu)$ on $|V_{cb}|$ that is stronger than in rare $B$ decays, in particular for $K_L\to\pi^0\nu\bar\nu$. Thereby the persistent…

High Energy Physics - Phenomenology · Physics 2022-06-03 Andrzej J. Buras , Elena Venturini

In this decade one expects a very significant progress in measuring the branching ratios for several rare $K$ and $B$ decays, in particular for the decays $K^+\to\pi^+\nu\bar\nu$, $K_L\to\pi^0\nu\bar\nu$, $B_s\to\mu^+\mu^+$ and…

High Energy Physics - Phenomenology · Physics 2022-09-20 Andrzej J. Buras

In the two Higgs doublet model, $\tan\beta$ is an important parameter, which is defined as the ratio of the vacuum expectation values of the doublets. We study how accurately $\tan\beta$ can be determined at linear colliders via the…

High Energy Physics - Phenomenology · Physics 2014-01-16 Shinya Kanemura , Koji Tsumura , Hiroshi Yokoya

We measure the branching fractions and $CP$ asymmetries for the decays $B^{0}\to \bar{D}^{0}\pi^{0}$ and $B^{+}\to \bar{D}^{0}\pi^{+}$, using a data sample of $772\times 10^{6}$ $B\bar{B}$ pairs collected at the $\Upsilon(4S)$ resonance…

High Energy Physics - Experiment · Physics 2022-08-11 Belle Collaboration , T. Bloomfield , M. E. Sevior , I. Adachi , H. Aihara , S. Al Said , D. M. Asner , V. Aulchenko , T. Aushev , R. Ayad , V. Babu , S. Bahinipati , P. Behera , J. Bennett , M. Bessner , T. Bilka , J. Biswal , A. Bobrov , G. Bonvicini , A. Bozek , M. Bračko , T. E. Browder , M. Campajola , L. Cao , D. Červenkov , M. -C. Chang , V. Chekelian , A. Chen , 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 , N. Dash , G. De Nardo , R. Dhamija , F. Di Capua , Z. Doležal , T. V. Dong , S. Dubey , S. Eidelman , D. Epifanov , T. Ferber , D. Ferlewicz , B. G. Fulsom , R. Garg , V. Gaur , A. Garmash , A. Giri , P. Goldenzweig , C. Hadjivasiliou , S. Halder , O. Hartbrich , K. Hayasaka , H. Hayashii , M. T. Hedges , M. Hernandez Villanueva , W. -S. Hou , C. -L. Hsu , T. Iijima , G. Inguglia , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , W. W. Jacobs , E. -J. Jang , S. Jia , Y. Jin , C. W. Joo , K. K. Joo , A. B. Kaliyar , K. H. Kang , G. Karyan , T. Kawasaki , C. H. Kim , D. Y. Kim , H. J. Kim , S. H. Kim , Y. -K. Kim , T. D. Kimmel , P. Kodyš , T. Konno , A. Korobov , S. Korpar , E. Kovalenko , P. Križan , R. Kroeger , P. Krokovny , M. Kumar , R. Kumar , K. Kumara , Y. -J. Kwon , K. Lalwani , J. S. Lange , I. S. Lee , S. C. Lee , C. H. Li , J. Li , Y. B. Li , L. Li Gioi , J. Libby , K. Lieret , D. Liventsev , T. Luo , C. MacQueen , M. Masuda , T. Matsuda , D. Matvienko , M. Merola , F. Metzner , K. Miyabayashi , R. Mizuk , G. B. Mohanty , S. Mohanty , H. K. Moon , R. Mussa , M. Nakao , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , H. Ono , Y. Onuki , P. Oskin , P. Pakhlov , G. Pakhlova , S. Pardi , H. Park , S. -H. Park , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , T. Podobnik , V. Popov , E. Prencipe , M. T. Prim , M. Ritter , A. Rostomyan , N. Rout , M. Rozanska , G. Russo , D. Sahoo , Y. Sakai , S. Sandilya , A. Sangal , L. Santelj , T. Sanuki , V. Savinov , G. Schnell , J. Schueler , C. Schwanda , A. J. Schwartz , Y. Seino , K. Senyo , M. Shapkin , C. Sharma , C. P. Shen , J. -G. Shiu , B. Shwartz , F. Simon , A. Sokolov , E. Solovieva , M. Starič , Z. S. Stottler , J. F. Strube , M. Sumihama , K. Sumisawa , T. Sumiyoshi , W. Sutcliffe , M. Takizawa , K. Tanida , Y. Tao , F. Tenchini , K. Trabelsi , M. Uchida , K. Uno , S. Uno , Y. Usov , S. E. Vahsen , R. Van Tonder , G. Varner , K. E. Varvell , A. Vossen , E. Waheed , C. H. Wang , E. Wang , M. -Z. Wang , P. Wang , M. Watanabe , S. Watanuki , O. Werbycka , J. Wiechczynski , E. Won , X. Xu , B. D. Yabsley , W. Yan , S. B. Yang , H. Ye , J. H. Yin , C. Z. Yuan , Z. P. Zhang , V. Zhilich , V. Zhukova , V. Zhulanov

We present a preliminary measurement of the branching fraction and CP-violating parameters S and C for the decay B->omegaKs. The data sample corresponds to 232x10^6 BBbar pairs produced from e+e- annihilation at the Upsilon(4S) resonance.…

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

Color-suppressed decays of $B$ mesons to final states with $\psi(2S)$ mesons have been observed with the CLEO detector. The branching fractions for the decays $B^+ \to \psi(2S) K^+$, $B^+ \to \psi(2S) K^*(892)^+$, $B^0 \to \psi(2S) K^0$,…

High Energy Physics - Experiment · Physics 2010-04-08 S. Richichi , CLEO Collaboration

We present measurements of branching fractions and charge asymmetries for the decays etaK*, where K* indicates a spin 0, 1, or 2 Kpi system. The data sample corresponds to 344x10^6 BBbar pairs collected with the BABAR detector at the PEP-II…

High Energy Physics - Experiment · Physics 2010-03-19 The BABAR Collaboration , B. Aubert

A clean determination of the angle $\alpha$ of the unitary triangle from $B\to \pi\pi$ decays requires an isospin analysis. If the $B \to \pi^0\pi^0$ and $\bar B \to \pi^0\pi^0$ decay rates are small it may be hard to carry out this…

High Energy Physics - Phenomenology · Physics 2010-11-23 Yuval Grossman , Helen R. Quinn

We report the measurement of branching fractions and $CP$-violation asymmetries in $B\to \phi \phi K$ decays based on a $711\,{\rm fb}^{-1}$ data sample containing $772\times 10^6$ $B\bar{B}$ events. The data were recorded at the $\Upsilon…

High Energy Physics - Experiment · Physics 2021-04-07 S. Mohanty , A. B. Kaliyar , V. Gaur , G. B. Mohanty , I. Adachi , K. Adamczyk , H. Aihara , S. Al Said , D. M. Asner , H. Atmacan , V. Aulchenko , T. Aushev , T. Aziz , V. Babu , S. Bahinipati , P. Behera , M. Bessner , V. Bhardwaj , T. Bilka , J. Biswal , A. Bobrov , A. Bozek , M. Bračko , T. E. Browder , M. Campajola , D. Červenkov , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , K. Cho , S. -J. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , S. Cunliffe , S. Das , N. Dash , G. De Nardo , R. Dhamija , F. Di Capua , Z. Doležal , T. V. Dong , S. Eidelman , T. Ferber , B. G. Fulsom , N. Gabyshev , A. Garmash , A. Giri , P. Goldenzweig , B. Golob , O. Grzymkowska , Y. Guan , K. Gudkova , C. Hadjivasiliou , S. Halder , K. Hayasaka , H. Hayashii , W. -S. Hou , C. -L. Hsu , K. Inami , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , H. B. Jeon , S. Jia , Y. Jin , K. K. Joo , K. H. Kang , G. Karyan , B. H. Kim , C. H. Kim , D. Y. Kim , S. H. Kim , Y. -K. Kim , K. Kinoshita , P. Kodyš , T. Konno , S. Korpar , D. Kotchetkov , P. Križan , P. Krokovny , R. Kulasiri , M. Kumar , R. Kumar , K. Kumara , Y. -J. Kwon , K. Lalwani , S. C. Lee , J. Li , L. K. Li , Y. B. Li , L. Li Gioi , J. Libby , Z. Liptak , D. Liventsev , C. MacQueen , M. Masuda , T. Matsuda , M. Merola , K. Miyabayashi , R. Mizuk , T. J. Moon , R. Mussa , M. Nakao , A. Natochii , L. Nayak , M. Nayak , N. K. Nisar , S. Nishida , K. Ogawa , S. Ogawa , Y. Onuki , P. Oskin , G. Pakhlova , S. Pardi , C. W. Park , H. Park , S. -H. Park , S. Patra , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , T. Podobnik , V. Popov , E. Prencipe , M. T. Prim , M. Röhrken , A. Rostomyan , N. Rout , G. Russo , D. Sahoo , Y. Sakai , S. Sandilya , A. Sangal , T. Sanuki , V. Savinov , G. Schnell , J. Schueler , C. Schwanda , A. J. Schwartz , Y. Seino , K. Senyo , M. E. Sevior , M. Shapkin , C. Sharma , J. -G. Shiu , B. Shwartz , F. Simon , E. Solovieva , M. Starič , Z. S. Stottler , J. F. Strube , T. Sumiyoshi , M. Takizawa , K. Tanida , Y. Tao , F. Tenchini , M. Uchida , Y. Unno , S. Uno , Y. Usov , S. E. Vahsen , R. Van Tonder , G. Varner , K. E. Varvell , A. Vinokurova , V. Vorobyev , C. H. Wang , E. Wang , M. -Z. Wang , P. Wang , X. L. Wang , S. Watanuki , J. Wiechczynski , E. Won , X. Xu , B. D. Yabsley , W. Yan , H. Ye , J. H. Yin , Z. P. Zhang , V. Zhilich , V. Zhukova

An isospin analysis of $B\to\pi\pi$ decays yields $\sin 2\alpha$, where $\alpha$ is the usual CKM angle $\alpha\equiv arg [-V_{td}V_{tb}^\ast /(V_{ud}V_{ub}^\ast)]$, without hadronic uncertainty if isospin is a perfect symmetry. Isospin,…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Gardner

We report improved measurements of B decays with an eta meson in the final state using 357 fb^-1 of data collected by the Belle detector at the KEKB e^+ e^- collider. We observe the decays B^+- ->eta pi^+- and B^+- -> eta K^+-; the measured…

High Energy Physics - Experiment · Physics 2007-05-23 The Belle Collaboration , K. Abe

To observe CP-violating asymmetries through the interference of a weaker amplitude with a stronger one in $\bo \to D^{(*)} \pi$ and $\ob \to D^{(*)} \pi$ decays, one must collect enough events that the intensity associated with the weaker…

High Energy Physics - Phenomenology · Physics 2014-11-17 Denis Suprun , Cheng-Wei Chiang , Jonathan L. Rosner

Asymmetric e^+e^- colliders running on the \Upsilon(4S) (B factories) will much more readily measure CP-violating asymmetries in the decays of B_d^0 and B^\pm mesons than in the decays of B_s^0 mesons. As such, they will seemingly not be…

High Energy Physics - Phenomenology · Physics 2010-11-23 David London , Amarjit Soni
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