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We present preliminary results of a time-dependent measurement of CP-violating asymmetry in fully reconstructed B0->D^(*)+-pi-+ decays in a data sample of approximately 88 million Y(4S)->BB decays collected with the BaBar detector at the…

High Energy Physics - Experiment · Physics 2008-11-26 The BABAR Collaboration , B. Aubert

We explore some ways of minimally modifying the neutrino mixing matrix from tribimaximal, characterized by introducing at most one mixing angle and a CP violating phase thus extending our earlier work. One minimal modification, motivated to…

High Energy Physics - Phenomenology · Physics 2015-05-28 Xiao-Gang He , A. Zee

We present updated results on time-dependent CP-violating asymmetries in neutral B decays to several CP eigenstates. The measurements use a data sample of about 62 million Upsilon(4S) --> B anti-B decays collected between 1999 and 2001 by…

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

The electrodynamics modified by the Chern-Simons term $\mathcal{L}_{cs}\sim p_{\mu}A_{\nu}\tilde F^{\mu\nu}$ with a non-vanishing $p_{\mu}$ violates the {\it Charge-Parity-Time Reversal} symmetry (CPT) and rotates the linear polarizations…

Cosmology and Nongalactic Astrophysics · Physics 2015-03-13 Jun-Qing Xia , Hong Li , Xinmin Zhang

The phenomenon of CP violation and strategies for extracting the angles of the unitarity triangle are reviewed. Special emphasis is given to the B-meson system, as it plays an outstanding role to test the Standard Model description of CP…

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

The angle gamma of the standard CKM unitarity triangle can be determined from B -> D K decays with a very small irreducible theoretical error, which is only due to second-order electroweak corrections. We study these contributions and…

High Energy Physics - Phenomenology · Physics 2015-06-17 Joachim Brod , Jure Zupan

Recent experimental results on CP violation in the B sector from BABAR and BELLE, experiments at asymmetric e+e- B-Factories, are summarized in these proceedings. The constraint on the position of the apex of the unitary triangle, obtained…

High Energy Physics - Experiment · Physics 2014-11-17 Sergey Ganzhur

We present the first model-independent measurement of the CKM unitarity triangle angle $\phi_3$ using $B^{\pm}\to D(K_{\rm S}^0\pi^+\pi^-\pi^0)K^{\pm}$ decays, where $D$ indicates either a $D^{0}$ or $\overline{D}^{0}$ meson. Measurements…

High Energy Physics - Experiment · Physics 2019-10-29 Belle Collaboration , P. K. Resmi , J. Libby , K. Trabelsi , I. Adachi , H. Aihara , S. Al Said , D. M. Asner , V. Aulchenko , T. Aushev , V. Babu , I. Badhrees , A. M. Bakich , C. Beleño , J. Bennett , V. Bhardwaj , B. Bhuyan , T. Bilka , J. Biswal , A. Bozek , M. Bračko , M. Campajola , D. Červenkov , A. Chen , B. G. Cheon , H. E. Cho , K. Cho , Y. Choi , S. Choudhury , D. Cinabro , S. Cunliffe , N. Dash , G. De Nardo , F. Di Capua , S. Di Carlo , Z. Doležal , T. V. Dong , S. Eidelman , D. Epifanov , J. E. Fast , T. Ferber , B. G. Fulsom , R. Garg , V. Gaur , N. Gabyshev , A. Garmash , A. Giri , P. Goldenzweig , B. Golob , Y. Guan , K. Hayasaka , H. Hayashii , W. -S. Hou , K. Huang , T. Iijima , K. Inami , G. Inguglia , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , W. W. Jacobs , H. B. Jeon , Y. Jin , D. Joffe , A. B. Kaliyar , K. H. Kang , G. Karyan , T. Kawasaki , C. Kiesling , D. Y. Kim , K. T. Kim , S. H. Kim , K. Kinoshita , P. Kodyš , D. Kotchetkov , P. Križan , R. Kroeger , P. Krokovny , T. Kuhr , R. Kumar , A. Kuzmin , Y. -J. Kwon , S. C. Lee , Y. B. Li , K. Lieret , D. Liventsev , P. -C. Lu , T. Luo , C. MacQueen , M. Masuda , T. Matsuda , D. Matvienko , M. Merola , K. Miyabayashi , R. Mizuk , G. B. Mohanty , H. K. Moon , T. Nakano , M. Nakao , K. J. Nath , M. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , K. Nishimura , S. Ogawa , H. Ono , Y. Onuki , P. Pakhlov , G. Pakhlova , B. Pal , S. Pardi , H. Park , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , E. Prencipe , M. T. Prim , M. Ritter , M. Röhrken , G. Russo , D. Sahoo , Y. Sakai , S. Sandilya , L. Santelj , T. Sanuki , V. Savinov , O. Schneider , G. Schnell , C. Schwanda , A. J. Schwartz , Y. Seino , K. Senyo , M. E. Sevior , V. Shebalin , C. P. Shen , J. -G. Shiu , B. Shwartz , E. Solovieva , M. Starič , Z. S. Stottler , J. F. Strube , T. Sumiyoshi , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , M. Uchida , T. Uglov , S. Uno , Y. Usov , R. Van Tonder , G. Varner , A. Vinokurova , V. Vorobyev , A. Vossen , B. Wang , C. H. Wang , M. -Z. Wang , X. L. Wang , S. Watanuki , E. Won , S. B. Yang , H. Ye , Z. P. Zhang , V. Zhilich , V. Zhukova

Natural 4 zeros texture mass matrices recently proposed by Fritzsch and Xing have been investigated by including `non-leading'corrections in the context of latest data regarding m_t^{pole} and V_{CKM} matrix elements. Apart from…

High Energy Physics - Phenomenology · Physics 2009-10-30 P. S. Gill , Manmohan Gupta

We present constraints on the angle gamma of the Unitarity Triangle with a Dalitz analysis of neutral D decays to K_Spi^+pi^- from the processes B^0 -> barD^0 K^*0 (barB^0 -> D^0 barK^*0) and B0 -> D0 K*0 (barB^0 -> barD^0 barK^*0) with…

High Energy Physics - Experiment · Physics 2010-04-12 The BABAR Collaboration , B. Aubert

We review the present status of the CKM matrix and we offer some visions of its future. After a brief presentation of the theoretical framework for weak decays we discuss the following topics: i) CKM matrix from tree level decays, ii)…

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

We present results of a unitary triangle fit based on the scan method. This frequentist approach employs Gaussian uncertainties for experimental quantities, but makes no arbitrary assumptions about the distribution of theoretical errors.…

High Energy Physics - Experiment · Physics 2015-06-12 Gerald Eigen , Gregory Dubois-Felsmann , David G. Hitlin , Frank C. Porter

Recent time-dependent CP asymmetry measurements in the $B_d \to J/\psi K_S$ channel by the BaBar and Belle Collaborations yield somewhat lower values of $\sin 2\beta$ compared to the one obtained from the standard model fit. If the…

High Energy Physics - Phenomenology · Physics 2014-11-17 Gautam Bhattacharyya , Amitava Datta , Anirban Kundu

Recent interest in flavour or horizontal symmetry building (mass textures) has been spurred mainly by the large top mass and, hence, the strong hierarchy in quark masses. Recently, various symmetry breaking schemes have been proposed based…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Mondragon , E. Rodriguez-Jauregui

The purpose of this paper is to provoke a discussion about the right next step in accelerator-based neutrino physics. In the next five years many experiments will be done to determine the neutrino mixing parameters. However, the small…

High Energy Physics - Phenomenology · Physics 2007-05-23 Burton Richter

In view of recent measurements of the mixing angle \theta_{13} a possibility to determine the difference of two CP Majorana phases of the neutrino mixing matrix from the study of neutrinoless double-beta decay is investigated. We show that…

High Energy Physics - Phenomenology · Physics 2015-06-11 F. Simkovic , S. M. Bilenky , Amand Faessler , Th. Gutsche

Current experimental data indicate that two unitarity triangles of the CKM quark flavor mixing matrix V are almost the right triangles with \alpha \approx 90^\circ. We find that \alpha = 90^\circ actually points to {\rm…

High Energy Physics - Phenomenology · Physics 2009-08-17 Zhi-zhong Xing

Although the unitarity triangles ($UTs$) carry information about the Kobayashi-Maskawa (KM) quark mixing matrix, it explicitly contains just three parameters which is one short to completely fix the KM matrix. It has been shown recently, by…

High Energy Physics - Phenomenology · Physics 2014-11-20 Paul H. Frampton , Xiao-Gang He

It is shown that following experimentally viable expressions for quark mixing angles $\theta_{12}$, $\theta_{23}$, $\theta_{13}$ and CP-violating phase $\delta$: $\sin\theta_{12} = \sqrt{m_{d} / |m_{s}|}$, $\sin\theta_{23} = 2 \, |m_{s}| /…

High Energy Physics - Phenomenology · Physics 2023-06-22 Boris Altshuler

We present the update of the Unitarity Triangle (UT) analysis within the Standard Model (SM) and beyond. Within the SM, combining the direct measurements on sides and angles, the UT turns out to be overconstraint in a consistent way,…

High Energy Physics - Phenomenology · Physics 2010-02-25 Cecilia Tarantino