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Related papers: Nonleptonic kaon decays: theory vs. experiment

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We discuss the time dependent interferences between $K_L$ and $K_S$ in the decays in $3\pi$ and $\pi\pi\gamma$, to be studied at interferometry machines such as the $\phi$-factory and LEAR. We emphasize the possibilities and the advantages…

High Energy Physics - Phenomenology · Physics 2010-11-01 G. D'Ambrosio , N. Paver

The combination of simple dynamics, small number of available decay channels, and extremely well controlled radiative and loop corrections, make charged pion decays a sensitive means for testing the underlying symmetries and the…

High Energy Physics - Experiment · Physics 2015-06-22 Dinko Pocanic , Emil Frlez , Andries van der Schaaf

We analyse the semileptonic decay D+ -> K- pi+ l+ nu(l) using an effective Lagrangian developed previously to describe the decays D -> P l nu(l) and D -> V l nu(l). Light vector mesons are included in the model which combines the heavy…

High Energy Physics - Phenomenology · Physics 2009-10-30 B. Bajc , S. Fajfer , R. J. Oakes , T. N. Pham

We use one-loop $\SU(2)_L\times \SU(2)_R$ chiral perturbation theory ($\SU(2)$ ChPT) to study the behaviour of the form-factors for semileptonic $K\to\pi$ decays with the pion mass at $q^2=0$ and at $q^2_{\textrm{max}}=(m_K-m_\pi)^2$, where…

High Energy Physics - Phenomenology · Physics 2009-02-12 J. M. Flynn , C. T. Sachrajda

The status of chiral perturbation theory in the meson sector is illustrated with several topical examples. The longtime discrepancy between theory and experiment for the charged pion polarizabilities has now been resolved in favour of the…

High Energy Physics - Phenomenology · Physics 2015-10-07 Gerhard Ecker

The first study is presented of CP violation with an amplitude analysis of the Dalitz plot of $B^0 \to D K^+ \pi^-$ decays, with $D \to K^+ \pi^-$, $K^+ K^-$ and $\pi^+ \pi^-$. The analysis is based on a data sample corresponding to…

High Energy Physics - Experiment · Physics 2016-10-12 LHCb collaboration , R. Aaij , C. Abellán Beteta , 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 , G. Andreassi , 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 , V. Bellee , N. Belloli , I. Belyaev , E. Ben-Haim , G. Bencivenni , S. Benson , J. Benton , A. Berezhnoy , R. Bernet , A. Bertolin , F. Betti , M. -O. Bettler , M. van Beuzekom , S. Bifani , P. Billoir , T. Bird , A. Birnkraut , A. Bizzeti , T. Blake , F. Blanc , J. Blouw , S. Blusk , V. Bocci , A. Bondar , N. Bondar , W. Bonivento , A. Borgheresi , S. Borghi , M. Borisyak , M. Borsato , T. J. V. Bowcock , E. Bowen , C. Bozzi , S. Braun , M. Britsch , T. Britton , J. Brodzicka , N. H. Brook , E. Buchanan , C. Burr , 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 , 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 , E. Dall'Occo , J. Dalseno , P. N. Y. David , A. Davis , O. De Aguiar Francisco , K. De Bruyn , S. De Capua , M. De Cian , J. M. De Miranda , L. De Paula , P. De Simone , C. -T. Dean , D. Decamp , M. Deckenhoff , L. Del Buono , N. Déléage , M. Demmer , 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 , A. Dovbnya , K. Dreimanis , L. Dufour , G. Dujany , K. Dungs , 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 , N. Farley , S. Farry , R. Fay , D. Fazzini , 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 , F. Fleuret , K. Fohl , M. Fontana , F. Fontanelli , D. C. Forshaw , R. Forty , 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. Garra Tico , L. Garrido , D. Gascon , C. Gaspar , L. Gavardi , G. Gazzoni , D. Gerick , E. Gersabeck , M. Gersabeck , T. Gershon , Ph. Ghez , 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 , P. Griffith , L. Grillo , O. Grünberg , B. Gui , E. Gushchin , Yu. Guz , T. Gys , T. Hadavizadeh , C. Hadjivasiliou , G. Haefeli , C. Haen , S. C. Haines , S. Hall , B. Hamilton , X. Han , S. Hansmann-Menzemer , N. Harnew , S. T. Harnew , J. Harrison , J. He , T. Head , V. Heijne , A. Heister , K. Hennessy , P. Henrard , L. Henry , J. A. Hernando Morata , E. van Herwijnen , M. Heß , A. Hicheur , D. Hill , M. Hoballah , C. Hombach , L. Hongming , W. Hulsbergen , T. Humair , M. Hushchyn , N. Hussain , D. Hutchcroft , M. Idzik , P. Ilten , R. Jacobsson , A. Jaeger , J. Jalocha , E. Jans , A. Jawahery , 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. Kecke , M. Kelsey , I. R. Kenyon , M. Kenzie , T. Ketel , E. Khairullin , B. Khanji , C. Khurewathanakul , T. Kirn , S. Klaver , K. Klimaszewski , O. Kochebina , M. Kolpin , I. Komarov , R. F. Koopman , P. Koppenburg , M. Kozeiha , L. Kravchuk , K. Kreplin , M. Kreps , P. Krokovny , F. Kruse , W. Krzemien , W. Kucewicz , M. Kucharczyk , V. Kudryavtsev , A. K. Kuonen , K. Kurek , T. Kvaratskheliya , D. Lacarrere , G. Lafferty , A. Lai , D. 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 , E. Lemos Cid , O. Leroy , T. Lesiak , B. Leverington , Y. Li , T. Likhomanenko , M. Liles , R. Lindner , C. Linn , F. Lionetto , B. Liu , X. Liu , D. Loh , I. Longstaff , J. H. Lopes , D. Lucchesi , M. Lucio Martinez , H. Luo , A. Lupato , E. Luppi , O. Lupton , A. Lusiani , F. Machefert , F. Maciuc , O. Maev , K. Maguire , S. Malde , A. Malinin , G. Manca , G. Mancinelli , P. Manning , A. Mapelli , J. Maratas , J. F. Marchand , U. Marconi , C. Marin Benito , P. Marino , J. Marks , G. Martellotti , M. Martin , M. Martinelli , D. Martinez Santos , F. Martinez Vidal , D. Martins Tostes , L. M. Massacrier , A. Massafferri , R. Matev , A. Mathad , Z. Mathe , C. Matteuzzi , A. Mauri , B. Maurin , A. Mazurov , M. McCann , J. McCarthy , A. McNab , R. McNulty , B. Meadows , F. Meier , M. Meissner , D. Melnychuk , M. Merk , A Merli , E Michielin , D. A. Milanes , M. -N. Minard , D. S. Mitzel , J. Molina Rodriguez , I. A. Monroy , S. Monteil , M. Morandin , P. Morawski , A. Mordà , M. J. Morello , J. Moron , A. B. Morris , R. Mountain , F. Muheim , D. Müller , J. Müller , K. Müller , V. Müller , M. Mussini , B. Muster , P. Naik , T. Nakada , R. Nandakumar , A. Nandi , I. Nasteva , M. Needham , N. Neri , S. Neubert , N. Neufeld , M. Neuner , A. D. Nguyen , C. Nguyen-Mau , V. Niess , S. Nieswand , R. Niet , N. Nikitin , T. Nikodem , 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. Pappenheimer , W. Parker , 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 , M. Pikies , 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. Popovici , C. Potterat , E. Price , J. D. Price , J. Prisciandaro , A. Pritchard , C. Prouve , V. Pugatch , A. Puig Navarro , G. Punzi , W. Qian , R. Quagliani , B. Rachwal , J. H. Rademacker , M. Rama , M. Ramos Pernas , M. S. Rangel , I. Raniuk , G. Raven , F. Redi , S. Reichert , A. C. dos Reis , V. Renaudin , S. Ricciardi , S. Richards , M. Rihl , K. Rinnert , V. Rives Molina , P. Robbe , A. B. Rodrigues , E. Rodrigues , J. A. Rodriguez Lopez , P. Rodriguez Perez , A. Rogozhnikov , S. Roiser , V. Romanovsky , A. Romero Vidal , J. W. Ronayne , M. Rotondo , T. Ruf , P. Ruiz Valls , J. J. Saborido Silva , N. Sagidova , B. Saitta , V. Salustino Guimaraes , C. Sanchez Mayordomo , B. Sanmartin Sedes , R. Santacesaria , C. Santamarina Rios , M. Santimaria , E. Santovetti , A. Sarti , C. Satriano , A. Satta , D. M. Saunders , D. Savrina , S. Schael , M. Schiller , H. Schindler , M. Schlupp , M. Schmelling , T. Schmelzer , B. Schmidt , O. Schneider , A. Schopper , M. Schubiger , M. -H. Schune , R. Schwemmer , B. Sciascia , A. Sciubba , A. Semennikov , A. Sergi , N. Serra , J. Serrano , L. Sestini , P. Seyfert , M. Shapkin , I. Shapoval , Y. Shcheglov , T. Shears , L. Shekhtman , V. Shevchenko , A. Shires , B. G. Siddi , R. Silva Coutinho , L. Silva de Oliveira , G. Simi , M. Sirendi , N. Skidmore , T. Skwarnicki , 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 , S. Stefkova , O. Steinkamp , O. Stenyakin , 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 , T. Szumlak , S. T'Jampens , A. Tayduganov , T. Tekampe , 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 , E. Tournefier , S. Tourneur , K. Trabelsi , M. Traill , 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 , M. van Veghel , J. J. Velthuis , M. Veltri , G. Veneziano , M. Vesterinen , B. Viaud , D. Vieira , M. Vieites Diaz , X. Vilasis-Cardona , V. Volkov , A. Vollhardt , D. Voong , A. Vorobyev , V. Vorobyev , C. Voß , J. A. de Vries , R. Waldi , C. Wallace , R. Wallace , J. Walsh , J. Wang , D. R. Ward , N. K. Watson , D. Websdale , A. Weiden , M. Whitehead , J. Wicht , 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 , K. Wraight , S. Wright , K. Wyllie , Y. Xie , Z. Xu , Z. Yang , H. Yin , J. Yu , X. Yuan , O. Yushchenko , M. Zangoli , M. Zavertyaev , L. Zhang , Y. Zhang , A. Zhelezov , Y. Zheng , A. Zhokhov , L. Zhong , V. Zhukov , S. Zucchelli

We use the Vector formulation to evaluate vector and axial-vector exchange contributions to the O(p^4) weak Chiral Lagrangian. We recover in this framework the bulk of the contributions found previously by Ecker et al. in the antisymmetric…

High Energy Physics - Phenomenology · Physics 2009-10-30 Giancarlo D'Ambrosio , Jorge Portoles

We use chiral perturbation theory to evaluate the scattering amplitude for the process Pi^+ K^- to Pi^+ K^- at leading and next-to-leading orders in the chiral counting and in the presence of isospin breaking effects. We also discuss the…

High Energy Physics - Phenomenology · Physics 2011-09-13 A. Nehme

Charmed baryon decays play an important role in studying the weak and strong interactions. Charmed baryon decays decaying into an octet baryon and a pseudoscalar meson have been studied in the framework of rescattering dynamics at the…

High Energy Physics - Phenomenology · Physics 2025-07-10 Di Wang

We study dispersive representations of nonlocal form factors in $K^+ \to \pi^+ \ell^+ \ell^-$ and $K^+ \to \pi^+ \nu \bar{\nu}$ decays, with an aim of improving the theoretical description of the spectrum and decay rate of the neutrino…

High Energy Physics - Phenomenology · Physics 2025-12-23 Anshika Bansal , Jack Jenkins , Daniel Winney

Although two pion decays of $K$, $D$ and $B$ have similar isospin structures, there are dramatic differences in the ratios $R_K$ and $R_{D,B}$ of amplitudes from $\Delta I =3/2$ and $\Delta I =1/2$ interactions. In $K\to \pi\pi$ decays…

High Energy Physics - Phenomenology · Physics 2009-11-10 Peng Guo , Xiao-Gang He , Xue-Qian Li

We study the scaling with the number of colors $N_c$ of the weak amplitudes mediating kaon mixing and decay, in the limit of light charm masses ($m_u=m_d=m_s=m_c$). The amplitudes are extracted directly on the lattice for $N_c = 3-7$ (with…

High Energy Physics - Lattice · Physics 2018-04-18 Andrea Donini , Pilar Hernandez , Carlos Pena , Fernando Romero-Lopez

In the chiral limit, the $D=6$ contribution to the Operator Product Expansion (OPE) of the $\mathrm{VV-AA}$ correlator of quark currents only depends on two vacuum condensates, which can be related to hadronic matrix elements associated to…

High Energy Physics - Phenomenology · Physics 2018-11-19 Antonio Rodríguez Sánchez , Antonio Pich

We present a preliminary measurement of CP-violation parameters in the decay B0->K+K-Ks, using approximately 465 million BBbar events collected by the BABAR detector at SLAC. Reconstructing the neutral kaon as Ks->pi+pi- or Ks->pi0pi0, we…

High Energy Physics - Experiment · Physics 2009-05-09 The BABAR Collaboration , B. Aubert

The $K\to\pi\pi$ decay amplitudes are studied within the framework of generalized factorization in which the effective Wilson coefficients are gauge-invariant, renormalization-scale and -scheme independent while factorization is applied to…

High Energy Physics - Phenomenology · Physics 2007-05-23 Hai-Yang Cheng

Long-distance effects in exclusive rare semileptonic transitions B -> (K, K*) are analysed within a relativistic quark model. The meson transition form factors, describing the meson amplitudes of the effective weak Hamiltonian, are…

High Energy Physics - Phenomenology · Physics 2009-10-30 D. Melikhov , N. Nikitin , S. Simula

We use both old and new theoretical developments in QCD dispersion relation constraints on the scalar form factor in the decay K --> \pi l \nu_l to obtain constraints on the strange quark mass. The perturbative QCD side of the calculation…

High Energy Physics - Phenomenology · Physics 2014-11-17 Richard F. Lebed , Karl Schilcher

We study the three-pion decays of the lightest isoscalar vector mesons, omega and phi, in a dispersive framework that allows for a consistent description of final-state interactions between all three pions. Our results are solely dependent…

High Energy Physics - Phenomenology · Physics 2012-06-07 Franz Niecknig , Bastian Kubis , Sebastian P. Schneider

In this paper we use one-loop chiral perturbation theory in order to compare lattice computations of the K+ to pi+ pi0 decay amplitude with the experimental value. This makes it possible to investigate three systematic effects that plague…

High Energy Physics - Lattice · Physics 2016-08-24 Maarten Golterman , Ka Chun Leung

One can analyze the hadronic decay amplitudes for $B\to PP$ decays using flavor SU(3) symmetry in different ways, such as the algebraic and quark diagram approaches. We derive specific relations between these two sets of amplitudes. In the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Xiao-Gang He , Bruce McKellar