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In this article, we study the decays $\psi^{\prime}\to {J/\psi}\pi^+\pi^-$ and $\eta_c^{\prime}\to {\eta_c}\pi^+\pi^-$ by taking into account the chiral symmetry breaking effects, the final-state interactions and the heavy quark symmetry.…

High Energy Physics - Phenomenology · Physics 2011-08-11 Zhi-Gang Wang

We quantify the important effect of strong final state interactions in the weak $K\to 2\pi$ amplitudes, using the measured $\pi$-$\pi$ phase shifts with J=0 and $I=0,2$. The main results of this analysis, with their implications for…

High Energy Physics - Phenomenology · Physics 2014-11-17 Elisabetta Pallante , Antonio Pich

The production of $\eta$ mesons in $NN$ collisions in the near threshold region is analyzed with special emphasis on the role of final state interaction which is calculated using three-body scattering theory. The three-body aspects are…

Nuclear Theory · Physics 2009-11-10 A. Fix , H. Arenhoevel

We analyze final state strong interaction effects in $B -> D \rho$ and $B -> D^{*}\pi$ decays using the Regge model. We find that, due to the smallness of the contributions from the non-leading Regge trajectories ($\rho$, $f$, $\pi$ etc.),…

High Energy Physics - Phenomenology · Physics 2009-10-30 G. Nardulli , T. N. Pham

A global previous analysis of two-body nonleptonic decays of $D$ mesons has been extended to the decays involving light scalar mesons. The allowance for final state interaction also in nonresonant channels provides a fit of much improved…

High Energy Physics - Phenomenology · Physics 2008-11-26 F. Buccella , M. Lusignoli , A. Pugliese

Final-state rescattering effects on the hadronic B decays and their impact on direct and mixing-induced CP asymmetries are examined. Implications for some phenomenologies are briefly discussed.

High Energy Physics - Phenomenology · Physics 2009-11-11 Hai-Yang Cheng

A study of $B^0$~and $B^0_s$ meson decays into $J/\psi\eta$~and $J/\psi\eta^{\prime}$ final states is performed using a data set of proton-proton collisions at centre-of-mass energies of 7 and 8TeV, collected by the LHCb experiment and…

High Energy Physics - Experiment · Physics 2015-01-28 LHCb collaboration , R. Aaij , B. Adeva , M. Adinolfi , A. Affolder , Z. Ajaltouni , S. Akar , J. Albrecht , F. Alessio , M. Alexander , S. Ali , G. Alkhazov , P. Alvarez Cartelle , A. A. Alves , S. Amato , S. Amerio , Y. Amhis , L. An , L. Anderlini , J. Anderson , R. Andreassen , M. Andreotti , J. E. Andrews , R. B. Appleby , O. Aquines Gutierrez , F. Archilli , A. Artamonov , M. Artuso , E. Aslanides , G. Auriemma , M. Baalouch , S. Bachmann , J. J. Back , A. Badalov , C. Baesso , W. Baldini , R. J. Barlow , C. Barschel , S. Barsuk , W. Barter , V. Batozskaya , V. Battista , A. Bay , L. Beaucourt , J. Beddow , F. Bedeschi , I. Bediaga , S. Belogurov , K. Belous , I. Belyaev , E. Ben-Haim , G. Bencivenni , S. Benson , J. Benton , A. Berezhnoy , R. Bernet , AB Bertolin , M. -O. Bettler , M. van Beuzekom , A. Bien , S. Bifani , T. Bird , A. Bizzeti , P. M. Bjørnstad , T. Blake , F. Blanc , J. Blouw , S. Blusk , V. Bocci , A. Bondar , N. Bondar , W. Bonivento , S. Borghi , A. Borgia , M. Borsato , T. J. V. Bowcock , E. Bowen , C. Bozzi , D. Brett , M. Britsch , T. Britton , J. Brodzicka , N. H. Brook , H. Brown , A. Bursche , J. Buytaert , S. Cadeddu , R. Calabrese , M. Calvi , M. Calvo Gomez , P. Campana , D. Campora Perez , L. Capriotti , A. Carbone , G. Carboni , R. Cardinale , A. Cardini , L. Carson , K. Carvalho Akiba , RCM Casanova Mohr , G. Casse , L. Cassina , L. Castillo Garcia , M. Cattaneo , Ch. Cauet , R. Cenci , M. Charles , Ph. Charpentier , M. Chefdeville , S. Chen , S. -F. Cheung , N. Chiapolini , M. Chrzaszcz , X. Cid Vidal , G. Ciezarek , P. E. L. Clarke , M. Clemencic , H. V. Cliff , J. Closier , V. Coco , J. Cogan , E. Cogneras , V. Cogoni , L. Cojocariu , G. Collazuol , P. Collins , A. Comerma-Montells , A. Contu , A. Cook , M. Coombes , S. Coquereau , G. Corti , M. Corvo , I. Counts , B. Couturier , G. A. Cowan , D. C. Craik , A. C. Crocombe , M. Cruz Torres , S. Cunliffe , R. Currie , C. D'Ambrosio , J. Dalseno , P. David , P. N. Y. David , A. Davis , K. De Bruyn , S. De Capua , M. De Cian , J. M. De Miranda , L. De Paula , W. De Silva , P. De Simone , C. -T. Dean , D. Decamp , M. Deckenhoff , L. Del Buono , N. Déléage , D. Derkach , O. Deschamps , F. Dettori , A. Di Canto , H. Dijkstra , S. Donleavy , F. Dordei , M. Dorigo , A. Dosil Suárez , D. Dossett , A. Dovbnya , K. Dreimanis , G. Dujany , F. Dupertuis , P. Durante , R. Dzhelyadin , A. Dziurda , A. Dzyuba , S. Easo , U. Egede , V. Egorychev , S. Eidelman , S. Eisenhardt , U. Eitschberger , R. Ekelhof , L. Eklund , I. El Rifai , Ch. Elsasser , S. Ely , S. Esen , H. -M. Evans , T. Evans , A. Falabella , C. Färber , C. Farinelli , N. Farley , S. Farry , R. Fay , D. Ferguson , V. Fernandez Albor , F. Ferreira Rodrigues , M. Ferro-Luzzi , S. Filippov , M. Fiore , M. Fiorini , M. Firlej , C. Fitzpatrick , T. Fiutowski , P. Fol , M. Fontana , F. Fontanelli , R. Forty , O. Francisco , M. Frank , C. Frei , M. Frosini , J. Fu , E. Furfaro , A. Gallas Torreira , D. Galli , S. Gallorini , S. Gambetta , M. Gandelman , P. Gandini , Y. Gao , J. García Pardiñas , J. Garofoli , J. Garra Tico , L. Garrido , D. Gascon , C. Gaspar , U. Gastaldi , R. Gauld , L. Gavardi , G. Gazzoni , A. Geraci , E. Gersabeck , M. Gersabeck , T. Gershon , Ph. Ghez , A. Gianelle , S. Gianì , V. Gibson , L. Giubega , V. V. Gligorov , C. Göbel , D. Golubkov , A. Golutvin , A. Gomes , C. Gotti , M. Grabalosa Gándara , R. Graciani Diaz , L. A. Granado Cardoso , E. Graugés , E. Graverini , G. Graziani , A. Grecu , E. Greening , S. Gregson , P. Griffith , L. Grillo , O. Grünberg , B. Gui , E. Gushchin , Yu. Guz , T. Gys , C. Hadjivasiliou , G. Haefeli , C. Haen , S. C. Haines , S. Hall , B. Hamilton , T. Hampson , X. Han , S. Hansmann-Menzemer , N. Harnew , S. T. Harnew , J. Harrison , J. He , T. Head , V. Heijne , K. Hennessy , P. Henrard , L. Henry , J. A. Hernando Morata , E. van Herwijnen , M. Heß , A. Hicheur , D. Hill , M. Hoballah , C. Hombach , W. Hulsbergen , N. Hussain , D. Hutchcroft , D. Hynds , M. Idzik , P. Ilten , R. Jacobsson , A. Jaeger , J. Jalocha , E. Jans , P. Jaton , A. Jawahery , F. Jing , M. John , D. Johnson , C. R. Jones , C. Joram , B. Jost , N. Jurik , S. Kandybei , W. Kanso , M. Karacson , T. M. Karbach , S. Karodia , M. Kelsey , I. R. Kenyon , T. Ketel , B. Khanji , C. Khurewathanakul , S. Klaver , K. Klimaszewski , O. Kochebina , M. Kolpin , I. Komarov , R. F. Koopman , P. Koppenburg , M. Korolev , L. Kravchuk , K. Kreplin , M. Kreps , G. Krocker , P. Krokovny , F. Kruse , W. Kucewicz , M. Kucharczyk , V. Kudryavtsev , K. Kurek , T. Kvaratskheliya , V. N. La Thi , D. Lacarrere , G. Lafferty , A. Lai , D. Lambert , R. W. Lambert , G. Lanfranchi , C. Langenbruch , B. Langhans , T. Latham , C. Lazzeroni , R. Le Gac , J. van Leerdam , J. -P. Lees , R. Lefèvre , A. Leflat , J. Lefrançois , S. Leo , O. Leroy , T. Lesiak , B. Leverington , Y. Li , T. Likhomanenko , M. Liles , R. Lindner , C. Linn , F. Lionetto , B. Liu , S. Lohn , I. Longstaff , J. H. Lopes , P. Lowdon , D. Lucchesi , H. Luo , A. Lupato , E. Luppi , O. Lupton , F. Machefert , I. V. Machikhiliyan , F. Maciuc , O. Maev , S. Malde , A. Malinin , G. Manca , G. Mancinelli , A. Mapelli , J. Maratas , J. F. Marchand , U. Marconi , C. Marin Benito , P. Marino , R. Märki , J. Marks , G. Martellotti , A. Martín Sánchez , M. Martinelli , D. Martinez Santos , F. Martinez Vidal , D. Martins Tostes , A. Massafferri , R. Matev , Z. Mathe , C. Matteuzzi , A. Mazurov , M. McCann , J. McCarthy , A. McNab , R. McNulty , B. McSkelly , B. Meadows , F. Meier , M. Meissner , M. Merk , D. A. Milanes , M. -N. Minard , N. Moggi , J. Molina Rodriguez , S. Monteil , M. Morandin , P. Morawski , A. Mordà , M. J. Morello , J. Moron , A. -B. Morris , R. Mountain , F. Muheim , K. Müller , M. Mussini , B. Muster , P. Naik , T. Nakada , R. Nandakumar , I. Nasteva , M. Needham , N. Neri , S. Neubert , N. Neufeld , M. Neuner , A. D. Nguyen , T. D. Nguyen , C. Nguyen-Mau , M. Nicol , V. Niess , R. Niet , N. Nikitin , T. Nikodem , A. Novoselov , D. P. O'Hanlon , A. Oblakowska-Mucha , V. Obraztsov , S. Oggero , S. Ogilvy , O. Okhrimenko , R. Oldeman , C. J. G. Onderwater , M. Orlandea , J. M. Otalora Goicochea , A. Otto , P. Owen , A. Oyanguren , B. K. Pal , A. Palano , F. Palombo , M. Palutan , J. Panman , A. Papanestis , M. Pappagallo , L. L. Pappalardo , C. Parkes , C. J. Parkinson , G. Passaleva , G. D. Patel , M. Patel , C. Patrignani , A. Pearce , A. Pellegrino , G. Penso , M. Pepe Altarelli , S. Perazzini , P. Perret , M. Perrin-Terrin , L. Pescatore , E. Pesen , K. Petridis , A. Petrolini , E. Picatoste Olloqui , B. Pietrzyk , T. Pilař , D. Pinci , A. Pistone , S. Playfer , M. Plo Casasus , F. Polci , S. Polikarpov , A. Poluektov , I. Polyakov , E. Polycarpo , A. Popov , D. Popov , B. Popovici , C. Potterat , E. Price , J. D. Price , J. Prisciandaro , A. Pritchard , C. Prouve , V. Pugatch , A. 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Vagnoni , G. Valenti , A. Vallier , R. Vazquez Gomez , P. Vazquez Regueiro , C. Vázquez Sierra , S. Vecchi , J. J. Velthuis , M. Veltri , G. Veneziano , M. Vesterinen , B. Viaud , D. Vieira , M. Vieites Diaz , X. Vilasis-Cardona , A. Vollhardt , D. Volyanskyy , D. Voong , A. Vorobyev , V. Vorobyev , C. Voß , J. A. de Vries , R. Waldi , C. Wallace , R. Wallace , J. Walsh , S. Wandernoth , J. Wang , D. R. Ward , N. K. Watson , D. Websdale , M. Whitehead , D. Wiedner , G. Wilkinson , M. Wilkinson , M. P. Williams , M. Williams , H. W. Wilschut , F. F. Wilson , J. Wimberley , J. Wishahi , W. Wislicki , M. Witek , G. Wormser , S. A. Wotton , S. Wright , K. Wyllie , Y. Xie , Z. Xing , Z. Xu , Z. Yang , X. Yuan , O. Yushchenko , M. Zangoli , M. Zavertyaev , L. Zhang , W. C. Zhang , Y. Zhang , A. Zhelezov , A. Zhokhov , L. Zhong

The effect of the interaction of mesons in the final state is additionally considered within the description of $\tau \to \pi \eta(\eta') \nu_{\tau}$ decays. This interaction is taken into account at the level of production of intermediate…

High Energy Physics - Phenomenology · Physics 2021-11-17 M. K. Volkov , K. Nurlan , A. A. Pivovarov

Instead of the glueball-$\eta'$ mixing ansatz, the latest measured ratios of the branching fractions of $B_{(s)}^0\to J/\psi \eta^{(\prime)}$ decays by LHCb can be understood by including the contribution from the light quark annihilation…

High Energy Physics - Phenomenology · Physics 2025-07-30 Ying Chen , Geng Li

To understand the short-distance vs long-distance final-state interactions, we have performed a detailed amplitude analysis for the two-body decay, J/psi into vector and pseudoscalar mesons. The current data favor a large relative phase…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Suzuki

Recent data on branching ratios for \psi(2S) decays to J/\psi\pi^+\pi^-, J/\psi\pi^0\pi^0 and J/\psi\eta are reviewed. An alternative treatment of data is proposed to get rid of the logical inconsistency which occurs in original…

High Energy Physics - Experiment · Physics 2009-10-31 Y. F. Gu , X. H. Li

We estimate effects of the final state interactions in B -> pi pi decays coming from rescattering of pi pi via exchange of rho, sigma, f_0 mesons. Then we include the rho rho rescattering via exchange of pi, omega, a_1 mesons and finally we…

High Energy Physics - Phenomenology · Physics 2009-11-11 Svjetlana Fajfer , Anita Prapotnik Brdnik , Tri-Nang Pham

The role of final state interaction in $\eta$ photoproduction on a deuteron as well as on three-body nuclei is investigated within few-body scattering theory. Deviation of the theory from the available experimental results is briefly…

Nuclear Theory · Physics 2007-05-23 A. Fix , H. Arenhoevel

An attempt is made to identify circumstances under which the weak decays of $D$ and $B$ mesons may display large differences between eigenphases of strong final-state interactions. There are several cases in which rescattering from other…

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

The availability of data on $B_s$ decays to strange quasi-two-body final states, either with or without charmonium opens new possibilities for understanding different contributions of weak diagrams and in particular the relative…

High Energy Physics - Phenomenology · Physics 2009-10-30 H. J. Lipkin

Involving of elastic rescattering and annihilation of quark-antiquark pairs in a final state allows us to explain a dependence of ratio for cross sections of $\eta'$ and $\eta$ mesons versus transfer momentum in charge exchange reactions.…

High Energy Physics - Phenomenology · Physics 2019-11-28 J. V. Balitsky , V. V. Kiselev , A. K. Likhoded , V. D. Samoylenko

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

I discuss the role of strong final state interactions (FSI) in K \to 2\pi decays. In this case strong FSI effects can be resummed [1,2] by solving the Omn\`es problem for K\to 2\pi amplitudes. Implications for the CP conserving Delta I=1/2…

High Energy Physics - Phenomenology · Physics 2014-11-17 Elisabetta Pallante

It has been long-understood that final state rescattering effects provide $\mathcal{O}(1)$ corrections to hadronic meson decays rates, such as $\eta\to\pi\pi\pi$ and $\eta^{\prime}\to\eta\pi\pi$. Hence, one would expect that such effects…

High Energy Physics - Phenomenology · Physics 2024-02-06 Daniele S. M. Alves , Sergi Gonzàlez-Solís

We discuss all contributions from Zweig-rule-satisfying SU(3)-breaking final state interactions (FSIs)in the B -> PP decays (neglecting charmed intermediate states), where PP=pi pi, pi K, KK, pi eta (eta'), and K eta (eta'). First, effects…

High Energy Physics - Phenomenology · Physics 2009-11-10 P. Zenczykowski , P. Lach