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We briefly review the recent results obtained by Fermilab experiment E791 on the Dalitz plot analysis of the decay D+ -> K- pi+ pi+, where indication for a light Kpi scalar resonance, the kappa, was found. We also present preliminary…

High Energy Physics - Experiment · Physics 2019-08-14 Carla Gobel

Dalitz analyses in charm give access to both magnitudes and phases of the charm decay amplitudes. They play a significant role in charm-mixing measurements, in the measurement of the CP-violating phase gamma in B decays to charm, and in the…

High Energy Physics - Experiment · Physics 2009-05-08 CLEO Collaboration , Jonas Rademacker

We perform a Dalitz plot analysis of about 100,000 Ds+ decays to K+ K- pi+ and measure the complex amplitudes of the intermediate resonances which contribute to this decay mode. We also measure the relative branching fractions of Ds+ --> K+…

High Energy Physics - Experiment · Physics 2011-03-10 P. del Amo Sanchez et al.

We describe Dalitz plots arising in studies of $D$-meson decays, and what we have learned from them in recent years. After some mention of technique and history, we focus on decay of the $D^\pm$ and $D_s^\pm$ mesons to the $K^-K^+\pi^\pm$…

High Energy Physics - Experiment · Physics 2012-10-10 Milind V. Purohit

We study the Dalitz plot of the Cabibbo-favored charmed-meson decay $D^+\to K^-\pi^+\pi^+$ using dispersion theory. The formalism respects all constraints from analyticity and unitarity, and consistently describes final-state interactions…

High Energy Physics - Phenomenology · Physics 2015-10-28 Franz Niecknig , Bastian Kubis

We study the Dalitz plot of the decay D^+ --> K^- pi^+ pi^+ with a sample of 15090 events from Fermilab experiment E791. Modeling the decay amplitude as the coherent sum of known K pi resonances and a uniform nonresonant term, we do not…

High Energy Physics - Experiment · Physics 2012-08-27 E791 Collaboration

A new approach to the analysis of three body decays is presented. Measurements of the S-wave K pi amplitude are made in independent ranges of invariant mass from threshold up to the upper kinematic limit in D+ to K-pi+pi+ decays. These are…

High Energy Physics - Experiment · Physics 2012-08-27 Fermilab E791 , : , E. Aitala

We will discuss how the decays of charm mesons can be used to study light mesons spectroscopy, by presenting recent results of Dalitz plot analyses using data from Fermilab experiment E791. Emphasis will be on scalar mesons, which are found…

High Energy Physics - Experiment · Physics 2019-08-14 Carla Gobel

We propose a phenomenological three component model describing the decay amplitude of the process $D_{s}^{+} \ra 3\pi$. The first component is a constant background, the second one is a Breit-Wigner amplitude associated to a quasi two-body…

High Energy Physics - Phenomenology · Physics 2016-09-01 M. GOURDIN , Y. Y. KEUM , X. Y. PHAM

We have studied the Cabibbo-suppressed decay mode D^0 into K^+ K^- pi^0 using a Dalitz plot technique and find the strong phase difference delta_D [defined as delta_(K*^- K^+) - delta_(K*^+ K^-)] = 332 degrees +- 8 degrees +- 11 degrees and…

High Energy Physics - Experiment · Physics 2010-04-08 C. Cawlfield , CLEO Collaboration

Charm meson decay dynamics have been studied extensively over the last decade. We describe the Dalitz-plot analysis technique which has been applied by many experiments to three-body D0, D+ and Ds decays. We discuss experimental results…

High Energy Physics - Experiment · Physics 2007-05-23 D. Asner

We formulate the final state interaction of the $a_1(1260)$ resonance decay in a manifestly three-body unitary parameterization and fit it to the $a_1(1260)$ lineshape measured by the ALEPH experiment. Dalitz plots calculated from this fit…

Nuclear Theory · Physics 2021-04-09 Daniel Sadasivan , Maxim Mai , Hakan Akdag , Michael Döring

The complex-rotated hyperspherical adiabatic method is used to study the decay of low-lying $^9$Be and $^9$B resonances into $\alpha$, $\alpha$ and $n$ or $p$. We consider six low-lying resonances of $^9$Be ($1/2^\pm$, $3/2^\pm$ and…

Nuclear Theory · Physics 2011-05-25 R. Alvarez-Rodriguez , A. S. Jensen , D. V. Fedorov , E. Garrido

We introduce parametrizations of hadronic three-body $B$ and $D$ weak decay amplitudes that can be readily implemented in experimental analyses and are a sound alternative to the simplistic and widely used sum of Breit-Wigner type…

High Energy Physics - Phenomenology · Physics 2017-12-20 D. Boito , J. -P. Dedonder , B. El-Bennich , R. Escribano , R. Kaminski , L. Lesniak , B. Loiseau

Some years ago, a method was proposed for measuring the CP-violating phase gamma using pairs of two-body decays that are related by U-spin reflection (d <-> s). In this paper we adapt this method to charmless B -> PPP decays. Time-dependent…

High Energy Physics - Phenomenology · Physics 2015-05-05 Bhubanjyoti Bhattacharya , David London

The Dalitz plot distribution of $B^0 \rightarrow \bar{D}^0 K^+ \pi^-$ decays is studied using a data sample corresponding to $3.0\rm{fb}^{-1}$ of $pp$ collision data recorded by the LHCb experiment during 2011 and 2012. The data are…

High Energy Physics - Experiment · Physics 2016-08-10 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 , M. Andreotti , J. E. Andrews , R. B. Appleby , O. Aquines Gutierrez , F. Archilli , P. d'Argent , 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 , L. J. Bel , I. Belyaev , E. Ben-Haim , G. Bencivenni , S. Benson , J. Benton , A. Berezhnoy , R. Bernet , A. Bertolin , M. -O. Bettler , M. van Beuzekom , A. Bien , S. Bifani , T. Bird , A. Birnkraut , A. Bizzeti , T. Blake , F. Blanc , J. Blouw , S. Blusk , V. Bocci , A. Bondar , N. Bondar , W. Bonivento , S. Borghi , M. Borsato , T. J. V. Bowcock , E. Bowen , C. Bozzi , S. Braun , D. Brett , M. Britsch , T. Britton , J. Brodzicka , N. H. Brook , 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 , P. Carniti , L. Carson , K. Carvalho Akiba , R. Casanova Mohr , G. Casse , L. Cassina , L. Castillo Garcia , M. Cattaneo , Ch. Cauet , G. Cavallero , 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 , B. Couturier , G. A. Cowan , D. C. Craik , A. Crocombe , M. Cruz Torres , S. Cunliffe , R. Currie , C. D'Ambrosio , J. Dalseno , 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 , B. Dey , A. Di Canto , F. Di Ruscio , H. Dijkstra , S. Donleavy , F. Dordei , M. Dorigo , A. Dosil Suárez , D. Dossett , A. Dovbnya , K. Dreimanis , L. Dufour , 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. Ferrari , F. Ferreira Rodrigues , M. Ferro-Luzzi , S. Filippov , M. Fiore , M. Fiorini , M. Firlej , C. Fitzpatrick , T. Fiutowski , K. Fohl , 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 , D. Gerick , E. Gersabeck , M. Gersabeck , T. Gershon , Ph. Ghez , A. Gianelle , S. Gianì , V. Gibson , O. G. Girard , 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 , T. Humair , N. Hussain , D. Hutchcroft , D. Hynds , M. Idzik , P. Ilten , R. Jacobsson , A. Jaeger , J. Jalocha , E. Jans , 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 , M. Kenzie , 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 , A. K. Kuonen , 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. 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Müller , V. 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 , V. Niess , R. Niet , N. Nikitin , T. Nikodem , D. Ninci , A. Novoselov , D. P. O'Hanlon , A. Oblakowska-Mucha , V. Obraztsov , S. Ogilvy , O. Okhrimenko , R. Oldeman , C. J. G. Onderwater , B. Osorio Rodrigues , J. M. Otalora Goicochea , A. Otto , P. Owen , A. Oyanguren , A. Palano , F. Palombo , M. Palutan , J. Panman , A. Papanestis , M. Pappagallo , L. L. Pappalardo , C. Parkes , G. Passaleva , G. D. Patel , M. Patel , C. Patrignani , A. Pearce , A. Pellegrino , G. Penso , M. Pepe Altarelli , S. Perazzini , P. Perret , L. Pescatore , K. Petridis , A. Petrolini , M. Petruzzo , E. Picatoste Olloqui , B. Pietrzyk , T. Pilař , D. Pinci , A. Pistone , A. Piucci , S. Playfer , M. Plo Casasus , T. Poikela , F. Polci , A. Poluektov , I. Polyakov , E. Polycarpo , A. Popov , D. Popov , B. 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Schubiger , M. -H. Schune , R. Schwemmer , B. Sciascia , A. Sciubba , A. Semennikov , I. Sepp , N. Serra , J. Serrano , L. Sestini , P. Seyfert , M. Shapkin , I. Shapoval , Y. Shcheglov , T. Shears , L. Shekhtman , V. Shevchenko , A. Shires , R. Silva Coutinho , G. Simi , M. Sirendi , N. Skidmore , I. Skillicorn , T. Skwarnicki , E. Smith , E. Smith , I. T. Smith , J. Smith , M. Smith , H. Snoek , M. D. Sokoloff , F. J. P. Soler , F. Soomro , D. Souza , B. Souza De Paula , B. Spaan , P. Spradlin , S. Sridharan , F. Stagni , M. Stahl , S. Stahl , O. Steinkamp , O. Stenyakin , F. Sterpka , S. Stevenson , S. Stoica , S. Stone , B. Storaci , S. Stracka , M. Straticiuc , U. Straumann , L. Sun , W. Sutcliffe , K. Swientek , S. Swientek , V. Syropoulos , M. Szczekowski , P. Szczypka , T. Szumlak , S. T'Jampens , T. Tekampe , M. Teklishyn , G. Tellarini , F. Teubert , C. Thomas , E. Thomas , J. van Tilburg , V. Tisserand , M. Tobin , J. Todd , S. Tolk , L. Tomassetti , D. Tonelli , S. Topp-Joergensen , N. Torr , E. Tournefier , S. Tourneur , K. Trabelsi , M. T. Tran , M. Tresch , A. Trisovic , A. Tsaregorodtsev , P. Tsopelas , N. Tuning , A. Ukleja , A. Ustyuzhanin , U. Uwer , C. Vacca , V. 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 , A. Weiden , M. Whitehead , D. Wiedner , G. Wilkinson , M. Wilkinson , M. Williams , M. P. Williams , M. Williams , T. Williams , F. F. Wilson , J. Wimberley , J. Wishahi , W. Wislicki , M. Witek , G. Wormser , S. A. Wotton , S. Wright , K. Wyllie , Y. Xie , Z. Xu , Z. Yang , J. Yu , X. Yuan , O. Yushchenko , M. Zangoli , M. Zavertyaev , L. Zhang , Y. Zhang , A. Zhelezov , A. Zhokhov , L. Zhong

An analysis of the Dalitz plots for the decays $D^+\to K^-\pi^+\pi^+$ and $D^+\to\pi^-\pi^+\pi^+$ indicates that structure with significant phase variation is required in the s-wave $K^-\pi^+$ and $\pi^-\pi^+$ systems in the region below 1…

High Energy Physics - Experiment · Physics 2007-05-23 Brian T. Meadows

We describe the $\pi\pi$ $S$-wave in $D^+ \to\pi^+ \pi^- \pi^+$ decays using a unitary model for the $\pi\pi$ Final State Interactions (FSI). The three body decay is treated as a quasi two-body process where, at the weak vertex, the D meson…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. R. Boito , B. El-Bennich , B. Loiseau , O. Leitner

We have calculated the radiative corrections to the Dalitz plot of baryon semileptonic decays with angular correlation between polarized emitted baryons and charged leptons. This work covers both charged and neutral decaying baryons and is…

High Energy Physics - Phenomenology · Physics 2009-01-09 M. Neri , J. J. Torres , Ruben Flores-Mendieta , A. Martinez , A. Garcia

The control of the optical quality of a laser beam requires a complex amplitude measurement able to deal with strong modulus variations and potentially highly perturbed wavefronts. The method proposed here consists in an extension of phase…