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We study B+- -- > K+-K+K- decays using the QCD factorization model with final state interactions between K+ and K- mesons taken into account. The parameters of the model are fitted to the data of the BABAR and LHCb collaborations. We…

High Energy Physics - Phenomenology · Physics 2024-05-29 L. Lesniak , P. Zenczykowski

We study the possible distortion of phase-space in the decays $K \to \pi \pi \pi$, which may result from final state interference among the decay products. Such distortion may influence the values of slope parameters extracted from the…

High Energy Physics - Phenomenology · Physics 2009-11-07 M. I. Martinez , G. Herrera

The Belle~II Collaboration presents four new analyses: The measurement of $V_{ub}$ from $B \to \pi e \nu_e$ decays with a fit to the differential $q^2$ spectrum, the determination of $V_{cb}$ using a fit to the differential $w$ distribution…

High Energy Physics - Experiment · Physics 2022-07-13 Maximilian Welsch

We study CP violation and the contribution of the strong kaon-pion interactions in the three body B --> K pi+ pi- decays. We extend our recent work on the effect of the two-pion S- and P-wave interactions to that of the corresponding…

High Energy Physics - Phenomenology · Physics 2011-03-23 B. El-Bennich , A. Furman , R. Kaminski , L. Lesniak , B. Loiseau , B. Moussallam

This talk contains a short overview of the history of the interplay of the weak and the strong interaction and CP-violation. It describes the phenomenology and the basic physics mechanisms involved in the Standard Model calculations of…

High Energy Physics - Phenomenology · Physics 2017-08-23 Johan Bijnens

We review recent advances in the theory of strong-interaction effects and final-state interactions in hadronic weak decays of heavy mesons. In the heavy-quark limit, the amplitudes for most nonleptonic, two-body B decays can be calculated…

High Energy Physics - Phenomenology · Physics 2009-10-31 Matthias Neubert

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

Motivated by recent measurements, we investigate $B\to \pi \pi, K \pi$ decay modes in the framework of QCD improved factorization, which was recently proposed by Beneke $et al$. We find that all the measured branching ratios are well…

High Energy Physics - Phenomenology · Physics 2009-10-31 Taizo Muta , Akio Sugamoto , Mao-Zhi Yang , Ya-Dong Yang

We make an attempt to clarify the role of the annihilation or "penguin" mode in the description of the $K\rightarrow\pi\pi$ decay within the Standard Model. The attention is concentrated on new operators in the effective $\Delta S=1$…

High Energy Physics - Phenomenology · Physics 2015-06-25 A. A. Penin , A. A. Pivovarov

The decay rates for $B^0 \to K^+ \pi^-$, $B^+ \to K^0 \pi^+$, and the charge-conjugate processes were found to provide information on the weak phase $\gamma \equiv {\rm Arg}(V_{ub}^*)$ when the ratio $r$ of weak tree and penguin amplitudes…

High Energy Physics - Phenomenology · Physics 2014-11-17 Michael Gronau , Jonathan L. Rosner

We consider the hadronic description of the $B^0_d\to \pi^+\pi^-$ decay, with the aim to investigate the strong phases generated by the final state interactions. The derivation of the dispersion relations using the…

High Energy Physics - Phenomenology · Physics 2009-01-07 I. Caprini , L. Micu , C. Bourrely

We compute standard model penguin amplitudes in nonleptonic B-decays to light charmless mesons using tree amplitude data to fix hadronic parameters. The leading calculation is carried out for the alphas(mb) penguin contributions from charm…

High Energy Physics - Phenomenology · Physics 2007-07-17 Ambar Jain , Ira Z. Rothstein , Iain W. Stewart

The large ratio of color-suppressed tree amplitude to color-allowed one in $B \to \pi \pi$ decays is difficult to understand within the Standard Model, which is known as the "$B \to \pi\pi$ puzzle". The two tree diagrams contain the up- and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Seungwon Baek

We suggest two methods (based on flavor SU(3) symmetry) to determine the CKM angle $\gamma$ using the decays $B_d$, $B^+ \to K \eta (\eta')$ and $B_s \to \pi \eta (\eta')$, respectively. Rescattering effects are partly included -- we…

High Energy Physics - Phenomenology · Physics 2010-11-23 K. Agashe , N. G. Deshpande

We discuss all contributions from inelastic SU(3)-symmetric rescattering in B decays into a final pair of pseudoscalar mesons $PP = \pi \pi$, $K\bar{K}$, $\pi K$. FSI-induced modifications of amplitudes obtained from the quark-line approach…

High Energy Physics - Phenomenology · Physics 2014-11-17 P. Zenczykowski

Some rare hadronic decays of B mesons, such as B->pi K, are sensitive to isospin-violating contributions from physics beyond the Standard Model. Although commonly referred to as electroweak penguins, such contributions can often arise…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yuval Grossman , Alexander L. Kagan , Matthias Neubert

Entangled states in high dimensional systems are of great interest due to the extended possibilities they provide in quantum information processing. Recently, Sun et al. [Phys. Rev. A 82, 052323 (2010)] and Kim et al. [Nat. Phys. 8, 117…

Quantum Physics · Physics 2017-07-03 Xing Xiao , Yan-Ling Li

A method is proposed to measure the photon polarisation parameter $\lambda_\gamma$ in $b\to s\gamma$ transitions using an amplitude analysis of $B\to K\pi\pi\gamma$ decays. Simplified models of the $K\pi\pi$ i system are used to simulate…

High Energy Physics - Phenomenology · Physics 2019-09-04 Violaine Bellée , Preema Pais , Albert Puig Navarro , Frédéric Blanc , Olivier Schneider , Karim Trabelsi , Giovanni Veneziano

The QCD factorization (QCDF) method usually contains infrared divergences which introduce large model dependence to its predictions on charmless B decays. The amplitudes of charmless B decays can be decomposed into "tree" and "penguin"…

High Energy Physics - Phenomenology · Physics 2014-11-20 Guohuai Zhu

This paper reviews the Dalitz plot analysis for the decays $B^0(\bar B^0) \to \rho \pi \to \pi^+ \pi^- \pi^0$. We discuss what can be learned about the ten parameters in this analysis from untagged and from tagged time-integrated data. We…

High Energy Physics - Phenomenology · Physics 2011-03-23 Helen R. Quinn , Joao P. Silva