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Related papers: New Bounds On The CKM Matrix From B -> K pi pi Dal…

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We discuss the determination of the CKM parameters from the forthcoming $CP$ violation observables in $B_s \to K^+ K^-$ decays. Combining the information on mixing induced CP violation in $B_s \to K^+ K^-$, with the $B_d \to J/\psi K_s$…

High Energy Physics - Phenomenology · Physics 2010-11-23 A. Salim Safir

We report on dispersive and finite energy sum rule analyses of the electroweak penguin matrix elements < (pi pi) | Q_{7,8} | K > in the chiral limit. We accomplish the correct perturbative matching (scale and scheme dependence) at NLO in…

High Energy Physics - Phenomenology · Physics 2009-11-07 V. Cirigliano , J. F. Donoghue , E. Golowich , K. Maltman

The role of penguin amplitudes in CP violating $B$ decays is reviewed, emphasizing recent progress in the analysis of electroweak penguin contributions. It is shown how these terms are included in a model-independent manner when measuring…

High Energy Physics - Phenomenology · Physics 2007-05-23 Michael Gronau

We give a simple expression in linear and quadratic Dalitz--plot slopes which does not depend on the charge combination of the $3\pi$ state $(K^\pm \to \pi^{\pm}\pi^{+}\pi^{-}$ or $\pi^{\pm}\pi^{0}\pi^{0}$ and $K_L^{0} \to…

High Energy Physics - Phenomenology · Physics 2009-09-25 A. A. Bel'kov , G. Bohm , F. Matthäi , A. V. Lanyov , A. Schaale

A new method to measure the angle $\phi_3$ of the CKM unitarity triangle using a Dalitz analysis of the three-body decay of the $D^0$ meson from the $B\to D^0 K$ process has been introduced recently. The method employs the interference…

High Energy Physics - Experiment · Physics 2012-08-27 Belle Collaboration

We derive constraints for $B\to VV$ modes ($V= vector meson) that allow aquantitative assessment of the contributions from electroweak penguins (EWP) and/or new physics. Interplay of direct CP with oscillation studies then leads to the…

High Energy Physics - Phenomenology · Physics 2009-10-31 David Atwood , Amarjit Soni

FOCUS results from Dalitz plot analysis of D_s+ and D+ to pi+pi-pi+ are presented. The K-matrix formalism is applied to charm decays for the first time to fully exploit the already existing knowledge coming from the light-meson spectroscopy…

High Energy Physics - Experiment · Physics 2012-08-27 FOCUS Collaboration

Unitarity triangles and characteristic measurables of the $3\times 3$ Cabibbo-Kobayashi-Maskawa (CKM) matrix are discussed. Beyond the $3\times 3$ CKM scheme we make a rephasing-invariant generalization of the Gronau-Wyler-Dunietz approach…

High Energy Physics - Phenomenology · Physics 2015-06-25 Zhi-zhong Xing

An enhanced electroweak penguin amplitude due to the presence of unknown new physics can explain the discrepancies found between theory and experiment in the B -> pi K decays, in particular in A_CP(B^- -> pi^0 K^-) - A_CP(\bar{B}^0 -> pi^+…

High Energy Physics - Phenomenology · Physics 2015-05-28 Lars Hofer , Dominik Scherer , Leonardo Vernazza

We present a new method using Dalitz plot and Bose symmetry of pions that allows the complete determination of the magnitudes and phases of weak decay amplitudes. We apply the method to process like B->K^* pi, with the subsequent decay of…

High Energy Physics - Phenomenology · Physics 2015-05-27 Rahul Sinha , N. G. Deshpande , Sandip Pakvasa , Chandradew Sharma

The measurements of B -> pi K decays have been in disagreement with the predictions of the Standard Model (SM) for some time. In this paper, we perform an update of this puzzle using the latest (2008) data. We find that the situation has…

High Energy Physics - Phenomenology · Physics 2014-11-18 Seungwon Baek , Cheng-Wei Chiang , David London

Results from the Belle and BaBar experiments on measurement of the weak angle phi_3 using a Dalitz plot analysis of the KSpi+pi- decay of the neutral D meson from the B+=>D(*)K(*)+ process are presented. The method employs the interference…

High Energy Physics - Experiment · Physics 2008-11-26 Alexei Garmash

Over the last two decades, $B \to \pi K$ modes have received a lot of attention. They are particularly interesting since the main contribution to these decays comes from QCD penguin topologies. Furthermore, electroweak penguin amplitudes…

High Energy Physics - Phenomenology · Physics 2018-12-07 Robert Fleischer , Ruben Jaarsma , Eleftheria Malami , K. Keri Vos

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

We present a measurement of the angle phi1 of the CKM Unitarity Triangle using time-dependent Dalitz analysis of D -> Ks pi+ pi- decays produced in neutral B meson decay to a neutral D meson and a light meson (B0bar -> D(*) h0). The method…

High Energy Physics - Experiment · Physics 2019-08-14 P. Krokovny

A brief review of CP violation in the $B$-meson system and of strategies to determine the angles $\alpha$, $\beta$ and $\gamma$ of the unitarity triangle of the CKM matrix is given. Both general aspects and some recent developments are…

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

We present a measurement of the unitarity triangle angle phi_3 using a Dalitz plot analysis of the three-body decay of the neutral D meson from the B->D(*)K process. The method employs the interference between D0 and D0bar to extract both…

High Energy Physics - Experiment · Physics 2012-08-27 Belle Collaboration

In the past, it was believed that one cannot obtain clean weak-phase information from the measurement of CP-violating asymmetries in 3-body B decays. Recently it was shown that this is not true -- by expressing the decay amplitudes in terms…

High Energy Physics - Phenomenology · Physics 2012-12-14 David London

We present first evidence that the cosine of the CP-violating weak phase $2\beta$ is positive, and hence exclude trigonometric multifold solutions of the CKM Unitarity Triangle using a time-dependent Dalitz plot analysis of $B^{0} \to…

High Energy Physics - Experiment · Physics 2019-01-02 The BaBar , Belle Collaborations , : , I. Adachi , T. Adye , H. Ahmed , J. K. Ahn , H. Aihara , S. Akar , M. S. Alam , J. Albert , F. Anulli , N. Arnaud , D. M. Asner , D. Aston , H. Atmacan , T. Aushev , R. Ayad , V. Babu , I. Badhrees , A. M. Bakich , Sw. Banerjee , V. Bansal , R. J. Barlow , G. Batignani , A. Beaulieu , P. Behera , M. Bellis , E. Ben-Haim , D. Bernard , F. U. Bernlochner , S. Bettarini , D. Bettoni , A. J. Bevan , V. Bhardwaj , B. Bhuyan , F. Bianchi , M. Biasini , J. Biswal , V. E. Blinov , M. Bomben , A. Bondar , G. R. Bonneaud , A. Bozek , C. Bozzi , M. Bračko , T. E. Browder , D. N. Brown , D. N. Brown , C. Bünger , P. R. Burchat , A. R. Buzykaev , R. Calabrese , A. Calcaterra , G. Calderini , S. Di Carlo , M. Carpinelli , C. Cartaro , G. Casarosa , R. Cenci , D. S. Chao , J. Chauveau , R. Cheaib , A. Chen , C. Chen , C. H. Cheng , B. G. Cheon , K. Chilikin , K. Cho , Y. Choi , S. Choudhury , M. Chrzaszcz , G. Cibinetto , D. Cinabro , J. Cochran , J. P. Coleman , M. R. Convery , G. Cowan , R. Cowan , L. Cremaldi , S. Cunliffe , N. Dash , M. Davier , C. L. Davis , F. De Mori , G. De Nardo , A. G. Denig , R. de Sangro , B. Dey , F. Di Lodovico , S. Dittrich , Z. Doležal , J. Dorfan , Z. Drásal , V. P. Druzhinin , W. Dunwoodie , M. Ebert , B. Echenard , S. Eidelman , G. Eigen , A. M. Eisner , S. Emery , D. Epifanov , J. A. Ernst , R. Faccini , J. E. Fast , M. Feindt , T. Ferber , F. Ferrarotto , F. Ferroni , R. C. Field , A. Filippi , G. Finocchiaro , E. Fioravanti , K. T. Flood , F. Forti , M. Fritsch , B. G. Fulsom , E. Gabathuler , D. Gamba , R. Garg , A. Garmash , J. W. Gary , I. Garzia , V. Gaur , A. Gaz , M. Gelb , T. J. Gershon , L. Li Gioi , M. A. Giorgi , A. Giri , R. Godang , P. Goldenzweig , B. Golob , V. B. Golubev , R. Gorodeisky , W. Gradl , M. T. Graham , E. Grauges , K. Griessinger , A. V. Gritsan , O. Grünberg , Y. Guan , E. Guido , N. Guttman , J. Haba , A. Hafner , T. Hara , P. F. Harrison , C. Hast , K. Hayasaka , H. Hayashii , C. Hearty , M. Heck , M. T. Hedges , M. Heß , S. Hirose , D. G. Hitlin , K. Honscheid , W. -S. Hou , C. -L. Hsu , Z. Huard , C. Van Hulse , D. E. Hutchcroft , K. Inami , G. Inguglia , W. R. Innes , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , J. M. Izen , W. W. Jacobs , A. Jawahery , C. P. Jessop , S. Jia , Y. Jin , K. K. Joo , T. Julius , A. B. Kaliyar , K. H. Kang , G. Karyan , R. Kass , H. Kichimi , D. Y. Kim , J. B. Kim , K. T. Kim , S. H. Kim , J. Kim , P. Kim , G. J. King , K. Kinoshita , H. Koch , P. Kodyš , Yu. G. Kolomensky , S. Korpar , D. Kotchetkov , R. Kowalewski , E. A. Kravchenko , P. Križan , R. Kroeger , P. Krokovny , T. Kuhr , R. Kulasiri , T. Kumita , A. Kuzmin , Y. -J. Kwon , H. M. Lacker , G. D. Lafferty , L. Lanceri , J. S. Lange , D. J. Lange , A. J. Lankford , T. E. Latham , T. Leddig , F. Le Diberder , I. S. Lee , S. C. Lee , J. P. Lees , D. W. G. S. Leith , L. K. Li , Y. B. Li , Y. Li , J. Libby , D. Liventsev , W. S. Lockman , O. Long , J. M. LoSecco , X. C. Lou , M. Lubej , T. Lueck , S. Luitz , T. Luo , E. Luppi , A. Lusiani , A. M. Lutz , D. B. MacFarlane , J. MacNaughton , U. Mallik , E. Manoni , G. Marchiori , M. Margoni , S. Martellotti , F. Martinez-Vidal , M. Masuda , T. Matsuda , T. S. Mattison , D. Matvienko , J. A. McKenna , B. T. Meadows , M. Merola , K. Miyabayashi , T. S. Miyashita , H. Miyata , R. Mizuk , G. B. Mohanty , H. K. Moon , T. Mori , D. R. Muller , T. Müller , R. Mussa , E. Nakano , M. Nakao , T. Nanut , K. J. Nath , M. Nayak , H. Neal , N. Neri , N. K. Nisar , S. Nishida , I. M. Nugent , B. Oberhof , J. Ocariz , S. Ogawa , P. Ongmongkolkul , H. Ono , A. P. Onuchin , Y. Onuki , A. Oyanguren , P. Pakhlov , G. Pakhlova , B. Pal , A. Palano , F. Palombo , W. Panduro Vazquez , E. Paoloni , S. Pardi , H. Park , S. Passaggio , C. Patrignani , P. Patteri , S. Paul , I. Pavelkin , D. J. Payne , T. K. Pedlar , D. R. Peimer , I. M. Peruzzi , R. Pestotnik , M. Piccolo , L. E. Piilonen , A. Pilloni , G. Piredda , V. Poireau , V. Popov , F. C. Porter , M. Posocco , S. Prell , R. Prepost , E. M. T. Puccio , M. V. Purohit , B. G. Pushpawela , M. Rama , A. Randle-Conde , B. N. Ratcliff , G. Raven , P. K. Resmi , J. L. Ritchie , M. Ritter , G. Rizzo , D. A. Roberts , S. H. Robertson , M. Röhrken , J. M. Roney , A. Roodman , A. Rossi , M. Rotondo , M. Rozanska , G. Russo , R. Sacco , S. Al Said , Y. Sakai , M. Salehi , S. Sandilya , L. Santelj , V. Santoro , T. Sanuki , V. Savinov , O. Schneider , G. Schnell , T. Schroeder , K. R. Schubert , C. Schwanda , A. J. Schwartz , R. F. Schwitters , C. Sciacca , R. M. Seddon , Y. Seino , S. J. Sekula , K. Senyo , O. Seon , S. I. Serednyakov , M. E. Sevior , V. Shebalin , C. P. Shen , T. -A. Shibata , N. Shimizu , J. -G. Shiu , G. Simi , F. Simon , F. Simonetto , Yu. I. Skovpen , J. G. Smith , A. J. S. Smith , R. Y. So , R. J. Sobie , A. Soffer , M. D. Sokoloff , E. P. Solodov , E. Solovieva , S. M. Spanier , M. Starič , R. Stroili , M. K. Sullivan , K. Sumisawa , T. Sumiyoshi , D. J. Summers , L. Sun , M. Takizawa , U. Tamponi , K. Tanida , P. Taras , N. Tasneem , F. Tenchini , V. Tisserand , K. Yu. Todyshevx , C. Touramanis , M. Uchida , T. Uglov , Y. Unno , S. Uno , S. E. Vahsen , G. Varner , G. Vasseur , J. Va'vra , D. Červenkov , M. Verderi , L. Vitale , V. Vorobyev , C. Voß , S. R. Wagner , E. Waheed , R. Waldi , J. J. Walsh , B. Wang , C. H. Wang , M. -Z. Wang , P. Wang , Y. Watanabe , F. F. Wilson , J. R. Wilson , W. J. Wisniewski , E. Won , G. Wormser , D. M. Wright , S. L. Wu , H. Ye , C. Z. Yuan , Y. Yusa , S. Zakharov , A. Zallo , L. Zani , Z. P. Zhang , V. Zhilich , V. Zhukova , V. Zhulanov , A. Zupanc

We analyse the B -> pi pi, pi K modes in the light of the most recent B-factory data, and obtain the following new results: (i) the B0 -> pi+ pi-, pi- K+ modes prefer gamma=(74+-6)deg, which - together with |V_ub/V_cb| - allows us to…

High Energy Physics - Phenomenology · Physics 2009-01-07 Andrzej J. Buras , Robert Fleischer , Stefan Recksiegel , Felix Schwab