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Related papers: Final state interaction phase in B decays

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A Regge model calculation relates the strong phase in $B \to DK$ to that in $B\to D\pi$. This provides a significant test of a hadronic picture of final state interactions in B decays.

High Energy Physics - Phenomenology · Physics 2009-11-10 G. Calderon , J. -M. Gerard , J. Pestieau , J. Weyers

By using very general and well established features of soft strong interactions we show, contrary to conventional expectations, that (i) soft final state interactions (FSI) do not disappear for large $m_B$, (ii) inelastic rescattering is…

High Energy Physics - Phenomenology · Physics 2009-10-28 John F. Donoghue , Eugene Golowich , Alexey A. Petrov , João M. Soares

A method parametrizing all inelastic final state interactions (FSI) in $B\to PP$ decays is presented ($P$ - pseudoscalar meson). The method explicitly shows how rescattering leads to the replacement of the short-distance amplitudes with the…

High Energy Physics - Phenomenology · Physics 2010-11-23 P. Zenczykowski

The two-body nonleptonic charmed meson decays into two pseudoscalar mesons are studied using one-particle-exchange method. The effects of the final state interactions are analyzed through the strong phases extracted from the experimental…

High Energy Physics - Phenomenology · Physics 2008-11-26 Medina Ablikim , Dong-Sheng Du , Mao-Zhi Yang

Exploiting $B$-meson decays for Standard Model tests and beyond requires a precise understanding of the strong final-state interactions that can be provided model-independently by means of dispersion theory. This formalism allows one to…

High Energy Physics - Phenomenology · Physics 2016-02-17 J. T. Daub , C. Hanhart , B. Kubis

We report a search for $B$ decays to selected final states with the $\eta_c$ meson: $B^{\pm}\to K^{\pm}\eta_c\pi^+\pi^-$, $B^{\pm}\to K^{\pm}\eta_c\omega$, $B^{\pm}\to K^{\pm}\eta_c\eta$ and $B^{\pm}\to K^{\pm}\eta_c\pi^0$. The analysis is…

High Energy Physics - Experiment · Physics 2017-02-07 Belle collaboration , A. Vinokurova , A. Kuzmin , S. Eidelman , A. Abdesselam , I. Adachi , H. Aihara , K. Arinstein , D. M. Asner , T. Aushev , R. Ayad , A. M. Bakich , V. Bansal , V. Bhardwaj , B. Bhuyan , A. Bobrov , A. Bondar , A. Bozek , M. Bračko , T. E. Browder , V. Chekelian , B. G. Cheon , K. Chilikin , R. Chistov , K. Cho , S. -K. Choi , Y. Choi , D. Cinabro , J. Dingfelder , Z. Doležal , Z. Drásal , A. Drutskoy , D. Dutta , D. Epifanov , H. Farhat , J. E. Fast , T. Ferber , V. Gaur , N. Gabyshev , A. Garmash , R. Gillard , Y. M. Goh , B. Golob , J. Haba , K. Hayasaka , H. Hayashii , X. H. He , W. -S. Hou , K. Inami , A. Ishikawa , R. Itoh , Y. Iwasaki , D. Joffe , T. Julius , K. H. Kang , E. Kato , C. Kiesling , D. Y. Kim , H. J. Kim , J. H. Kim , K. T. Kim , M. J. Kim , S. H. Kim , Y. J. Kim , K. Kinoshita , B. R. Ko , P. Kodyš , S. Korpar , P. Križan , P. Krokovny , T. Kuhr , T. Kumita , Y. -J. Kwon , J. S. Lange , L. Li Gioi , J. Libby , D. Liventsev , P. Lukin , D. Matvienko , K. Miyabayashi , H. Miyake , H. Miyata , G. B. Mohanty , A. Moll , T. Mori , R. Mussa , E. Nakano , M. Nakao , Z. Natkaniec , C. Ng , N. K. Nisar , S. Nishida , S. Ogawa , S. Okuno , S. L. Olsen , P. Pakhlov , G. Pakhlova , C. W. Park , H. Park , T. K. Pedlar , R. Pestotnik , M. Petrič , L. E. Piilonen , E. Ribežl , M. Ritter , A. Rostomyan , Y. Sakai , S. Sandilya , D. Santel , L. Santelj , T. Sanuki , Y. Sato , V. Savinov , O. Schneider , G. Schnell , C. Schwanda , D. Semmler , K. Senyo , O. Seon , M. E. Sevior , V. Shebalin , C. P. Shen , T. -A. Shibata , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , Y. -S. Sohn , A. Sokolov , E. Solovieva , S. Stanič , M. Starič , M. Steder , M. Sumihama , T. Sumiyoshi , U. Tamponi , G. Tatishvili , Y. Teramoto , M. Uchida , T. Uglov , Y. Unno , S. Uno , C. Van Hulse , P. Vanhoefer , G. Varner , V. Vorobyev , M. N. Wagner , C. H. Wang , M. -Z. Wang , P. Wang , Y. Watanabe , K. M. Williams , E. Won , J. Yamaoka , S. Yashchenko , Y. Yook , Z. P. Zhang , V. Zhulanov , A. Zupanc

We study the final-state interactions in $B \to \pi K$ decays through $B \to VV \to \pi K$ processes where the inelastic rescattering occurs via single pion exchange. The next-to-leading order low energy effective Hamiltonian and BSW model…

High Energy Physics - Phenomenology · Physics 2009-10-31 Dong-Sheng Du , Xue-Qian Li , Zheng-Tao Wei , Bing-Song Zou

B mesons are bound states of a b quark and a light anti-quark. While the binding is provided by the strong interaction B mesons can only decay by the weak interaction. Since the top quark mass is large, B mesons are the only mesons…

High Energy Physics - Phenomenology · Physics 2008-11-26 Thomas E. Browder , Klaus Honscheid

The observed strong phase difference of 30^{o} between I=(3/2) and I=(1/2) final states for the decay B to D Pi is analyzed in terms of rescattering like D^{∗}Pi to D Pi, etc. It is concluded that for the decay B^{o}to D^{+} Pi^{-}…

High Energy Physics - Phenomenology · Physics 2007-05-23 Lincoln Wolfenstein Ph. D

We present a general analysis on charmless B-meson decays $B\to \pi\pi$ and $\pi K$. It is noticed that the final state interactions and inelastic rescattering effects must be significant in order to understand the consistency of the…

High Energy Physics - Phenomenology · Physics 2014-11-17 Y. F. Zhou , Y. L. Wu , J. N. Ng , C. Q. Geng

We consider the weak decays of a B meson to final states that contain a S-wave radially excited vector meson. We consider vector-pseudoscalar final states and calculate ratios of the type $B \to \rho^{\prime} \pi/B \to \rho \pi$, $B \to…

High Energy Physics - Phenomenology · Physics 2009-11-07 Alakabha Datta , Harry J. Lipkin , Patrick J. O'Donnell

We report a search for $B$ decays to selected final states with the $\eta_c$ meson: $B^{\pm}\to K^{\pm}\eta_c\pi^+\pi^-$, $B^{\pm}\to K^{\pm}\eta_c\omega$, $B^{\pm}\to K^{\pm}\eta_c\eta$ and $B^{\pm}\to K^{\pm}\eta_c\pi^0$. The analysis is…

High Energy Physics - Experiment · Physics 2019-08-22 Anna Vinokurova

We present measurements of B meson decays to the final states omegaK*, omegarho, and omega f_0, where K* indicates a spin 0, 1, or 2 strange meson. The data sample corresponds to 465x10^6 BBbar pairs collected with the BABAR detector at the…

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

Decays of B mesons into final states containing a tau lepton are sensitive to new charged-current interactions that break lepton-flavor universality. These decays have been studied only at e+e- colliders, where the low-background…

High Energy Physics - Experiment · Physics 2014-03-05 Abner Soffer

It is shown that the existing data on two-body B decays, some of them only upper limits, are precise enough to perform an isospin analysis to extract the phase shifts due to final state interaction. Unlike charm decays, no significant final…

High Energy Physics - Phenomenology · Physics 2009-09-25 Hitoshi Yamamoto

The propagation and decay of neutral B-mesons can be described in terms of quantum dynamical semigroups; they provide generalized time-evolutions that take into account possible non-standard effects leading to loss of phase coherence and…

High Energy Physics - Phenomenology · Physics 2014-11-17 F. Benatti , R. Floreanini , R. Romano

We estimate final state interactions in the B-meson decays into two light vector mesons by the Regge model. We consider Pomeron exchange and charmed Regge trajectories that can relate intermediate charmed particles to the final state. The…

High Energy Physics - Phenomenology · Physics 2009-11-10 Massimo Ladisa , Vincenzo Laporta , Giuseppe Nardulli , Pietro Santorelli

The polarization measurement in the inclusive B decay provides us with a simple test of how much the long-distance final-state interaction takes place as the energy of the observed meson varies in the final state. We give the expectation of…

High Energy Physics - Phenomenology · Physics 2014-11-17 M. Suzuki

Analysis of charged and neutral B meson decays into pi+ pi- K, K+ K- K and K0S K0S K0S is performed using a unitary representation of the pi pi and K anti- K final state interactions. Comparison of the theoretical model with the…

High Energy Physics - Phenomenology · Physics 2015-06-25 L. Lesniak , A. Furman , R. Kaminski , B. El-Bennich , B. Loiseau

The decays of $B$ mesons to two-body hadronic final states are analyzed within the context of broken flavor SU(3) symmetry, extending a previous analysis involving pairs of light pseudoscalars to decays involving one or two charmed quarks…

High Energy Physics - Phenomenology · Physics 2010-11-01 Michael Gronau , Oscar F. Hernandez , David London , Jonathan L. Rosner