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We make the simple observation that there exists a universal unitarity triangle for all models, like the SM, the Two Higgs Doublet Models I and II and the MSSM with minimal flavour violation, that do not have any new operators beyond those…

High Energy Physics - Phenomenology · Physics 2010-11-23 A. J. Buras , P. Gambino , M. Gorbahn , S. Jager , L. Silvestrini

In presenting an up-to-date account of the experimental knowledge of the CKM matrix, special emphasis is placed on the exceptional degree of consistency shown by the current Standard Model determination of the unitarity triangle; some…

High Energy Physics - Phenomenology · Physics 2010-11-23 Pietro Faccioli

We explore the would-be consequences of a low value of the CP-violating phase $\sin2\beta_{\psi K}$. The importance of a reference triangle obtained from measurements that are independent of $B$--$\bar B$ and $K$--$\bar K$ mixing is…

High Energy Physics - Phenomenology · Physics 2010-11-23 Alexander L. Kagan , Matthias Neubert

The angles of all unitarity triangles of the Cabibbo-Kobayashi-Maskawa matrix are determined from the experimental data. Our analysis is independent of the parameterization of the CKM matrix and it is based on the predictions of the…

High Energy Physics - Phenomenology · Physics 2022-12-07 S. Rebeca Juárez Wysozka , Piotr Kielanowski , Liliana Vazquez Mercado

We report several recent updates from the BABAR Collaboration on the matrix elements $|V_{cb}|$, $|V_{ub}|$, and $|V_{td}|$ of the Cabibbo-Kobayashi-Maskawa (CKM) quark-mixing matrix, and the angles $\beta$ and $\alpha$ of the unitarity…

High Energy Physics - Experiment · Physics 2010-04-21 Chih-hsiang Cheng

The unitarity triangles of the $3\times 3$ Cabibbo-Kobayashi-Maskawa (CKM) matrix are studied in a systematic way. We show that the phases of the nine CKM rephasing invariants are indeed the outer angles of the six unitarity triangles and…

High Energy Physics - Phenomenology · Physics 2010-11-01 Dan-di WU , Zhi-zhong XING

Results by the BaBar and Belle experiments of the measurements $\sin 2\alpha$, $\sin 2\beta$ and $\sin (2\beta + \gamma)$ along with the CKM matrix elements $V_{cb}$ and $V_{ub}$ are presented. The BaBar and Belle experiments $b \to…

High Energy Physics - Experiment · Physics 2010-11-23 E. O. Olaiya

The CKM paradigm has been proven to be successful in explaining the flavour structure of the standard model and the non-trivial imaginary phase of the CKM matrix is the only know source of CP-violation. B-meson decays allow us to precisely…

High Energy Physics - Experiment · Physics 2010-05-26 Alessandro Gaz

The 3 X 3 CKM matrix defines six unitarity triangles in the complex plane, which will be carefully explored in the LHCb experiment and at the Super-B factory. We calculate the running effects of nine different inner angles and eighteen…

High Energy Physics - Phenomenology · Physics 2014-11-20 Shu Luo , Zhi-zhong Xing

In this letter, using a rephasing invariant formula $\delta = \arg [ { V_{ud} V_{us} V_{c b} V_{tb} / V_{ub} \det V_{\rm CKM} }]$, we evaluate the CP phase $\delta$ of the CKM matrix $V_{\rm CKM}$ perturbatively for small quark mixing…

High Energy Physics - Phenomenology · Physics 2026-02-03 Masaki J. S. Yang

A shape of the unitary triangle versus a CP violating parameter \delta depends on the phase conventions of the CKM matrix, because the CP violating parameter \delta cannot directly be observed, so that it is not rephasing-invariant. In…

High Energy Physics - Phenomenology · Physics 2014-11-18 Yoshio Koide

We construct the CKM unitarity triangle from CP invariant quantities, using the coupling constant of weak decays with flavor change from b to u, and the particle - antiparticle mixing probability in the B_s and B_d systems. Also included…

High Energy Physics - Phenomenology · Physics 2008-11-26 K. Kleinknecht , B. Renk

Under the hypothesis that the CP violating phase parameter \delta in the CKM matrix V takes own value so that the radius R(\delta) of the circle circumscribed about the unitary triangle takes its minimum value, possible phase conventions of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yoshio Koide

Concise variable transformations between the four angles of the CKM matrix in the standard representation advocated by the Particle Data Group and the angles of the unitarity triangles are derived. The behavior of these transformations in…

High Energy Physics - Phenomenology · Physics 2008-11-26 Richard F. Lebed

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

The current analysis of the Cabibbo-Kobayashi-Maskawa(CKM) quark mixing matrix uses the standard parametrisation by 3 mixing angles and the CP-violating KM phase. However it would be more convenient to express these mixing angle parameters…

High Energy Physics - Phenomenology · Physics 2011-12-08 T. N. Pham

We perform a global fit to the CKM unitarity triangle using the latest experimental and theoretical constraints. We present results for three different sets of constraints: the standard inputs used by CKMfitter and UTFit, the standard…

High Energy Physics - Phenomenology · Physics 2011-11-10 Jack Laiho , Enrico Lunghi , Ruth Van De Water

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

In this presentation, I review the status of selected Cabibbo-Kobayashi-Maskawa (CKM) matrix elements and their role in the Unitarity Triangle (UT). Since this conference concluded, many new results have been finalized and are included in…

High Energy Physics - Phenomenology · Physics 2010-11-23 Helmut Marsiske

The structure of the mixing matrix, in the electroweak quark sector with four generations of quarks is investigated. We conclude that the area of the unitarity quadrangle is not a good choice as a possible measure of the CP~violation. In…

High Energy Physics - Phenomenology · Physics 2021-07-07 S. R. Juárez Wysozka , P. Kielanowski