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Related papers: ChPT tests at the NA48 and NA62 experiments at CER…

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The results of a search for $\pi^0$ decays to a photon and an invisible massive dark photon at the NA62 experiment at the CERN SPS are reported. From a total of $4.12\times10^8$ tagged $\pi^0$ mesons, no signal is observed. Assuming a…

High Energy Physics - Experiment · Physics 2019-07-04 NA62 collaboration

A sample of $4.687\times 10^6$ fully reconstructed $K^\pm\to\pi^\pm\pi^0_D$, $\pi^0_D\to\gamma e^+e^-$ decay candidates in the kinematic range $m_{ee}>10~{\rm MeV}/c^2$ with a negligible background contamination collected by the NA48/2…

High Energy Physics - Experiment · Physics 2019-08-21 Evgueni Goudzovski

We review recent progress in the understanding of low-energy baryon structure by means of chiral perturbation theory. In particular, we discuss the application of this formalism to the description of the quark mass dependence of recent…

High Energy Physics - Lattice · Physics 2010-11-15 J. Martin Camalich , L. S. Geng , M. J. Vicente Vacas

A search for the decay $K_S\to\pi^0\gamma\gamma$ has been made using the NA48 detector at the CERN SPS. Using data collected in 1999 during a 40-hour run with a high-intensity $K_S$ beam, an upper limit for the branching ratio…

High Energy Physics - Experiment · Physics 2008-11-26 A. Lai

The anomaly (cusp) in the mass spectrum of two neutral pions from the three-pion decays of charged kaon has been observed in the NA48/2 experiment. Using the recently developed interpretation of this effect in terms of Chiral Perturbative…

High Energy Physics - Experiment · Physics 2019-08-14 D. Madigozhin

The first search for ultra-rare $K^+$ decays into the $\pi^+e^+e^-e^+e^-$ final state is reported, using a dataset collected by the NA62 experiment at CERN in 2017-2018. An upper limit of $1.4\times 10^{-8}$ at 90% CL is obtained for the…

High Energy Physics - Experiment · Physics 2023-09-20 NA62 collaboration

We present the results of a search for relations between observables that are independent of the Chiral Perturbation Theory (ChPT) Next-to-Next-to-Leading Order (NNLO) Low-Energy Constants (LECs). We have found some relations between…

High Energy Physics - Phenomenology · Physics 2014-11-20 Johan Bijnens , Ilaria Jemos

The KS->gamma gamma decay rate has been measured with the NA48 detector using a high intensity short neutral beam from the CERN SPS. The measured branching ratio BR(KS->gamma gamma)=(2.78+-0.06(stat)+-0.04(syst))x10-6, obtained from…

High Energy Physics - Experiment · Physics 2008-11-26 A. Lai

Non-leptonic kaon decays are often described through an effective chiral weak Hamiltonian, whose couplings ("low-energy constants") encode all non-perturbative QCD physics. It has recently been suggested that these low-energy constants…

High Energy Physics - Lattice · Physics 2010-02-03 P. Hernandez , M. Laine

We calculate the form factors of the $K \to \pi l \nu$ semileptonic decays in three-flavor lattice QCD, and study their chiral behavior as a function of the momentum transfer and the Nambu-Goldstone boson masses. Chiral symmetry is exactly…

High Energy Physics - Lattice · Physics 2017-05-03 JLQCD Collaboration , S. Aoki , G. Cossu , X. Feng , H. Fukaya , S. Hashimoto , T. Kaneko , J. Noaki , T. Onogi

Numerous recent measurements of kaon decays are described, with an emphasis on results offering constraints on chiral perturbation theory calculations. An up-to-date estimate of |Vus|f+(0) based on semileptonic kaon decay rates is…

High Energy Physics - Experiment · Physics 2007-05-23 Matthew Moulson

The rare kaon decay $K_L\to\pi^0\nu\bar{\nu}$ is extremely sensitive to new physics, because the contribution to this decay in the Standard Model (SM) is highly suppressed and known very accurately; the branching ratio is $3\times 10^{-11}$…

High-intensity proton beams impinging on a fixed target or beam dump allow to probe new physics via the production of new weakly-coupled particles in hadron decays. The CERN SPS provides opportunities to do so with the running NA62…

High Energy Physics - Experiment · Physics 2017-12-06 P. Mermod

A sample of 7253 $K^\pm\to\pi^\pm e^+e^-(\gamma)$ decay candidates with 1.0% background contamination has been collected by the NA48/2 experiment at the CERN SPS, allowing a precise measurement of the decay properties. The branching ratio…

High Energy Physics - Experiment · Physics 2014-11-18 2 collaboration

Recent results and future prospects in the rare kaon-decay experiments at KEK, BNL, CERN and FNAL are reviewed. Emphasis is placed on the quark flavor dynamics in the flavor-changing neutral current processes. Experimental and data-analysis…

High Energy Physics - Experiment · Physics 2007-05-23 T. K. Komatsubara

A comprehensive overview of kaon decays is presented. The Standard Model predictions are discussed in detail, covering both the underlying short-distance electroweak dynamics and the important interplay of QCD at long distances. Chiral…

High Energy Physics - Phenomenology · Physics 2015-05-30 V. Cirigliano , G. Ecker , H. Neufeld , A. Pich , J. Portoles

$K^{+}\rightarrow\pi^{+}\nu\overline{\nu}$ is one of the theoretically cleanest meson decay where to look for indirect effects of new physics complementary to LHC searches. The NA62 experiment at CERN SPS is designed to measure the…

High Energy Physics - Experiment · Physics 2019-08-12 NA62 Collaboration , G. Aglieri Rinella , R. Aliberti , F. Ambrosino , R. Ammendola , B. Angelucci , A. Antonelli , G. Anzivino , R. Arcidiacono , I. Azhinenko , S. Balev , M. Barbanera , J. Bendotti , A. Biagioni , L. Bician , C. Biino , A. Bizzeti , T. Blazek , A. Blik , B. Bloch-Devaux , V. Bolotov , V. Bonaiuto , M. Boretto , M. Bragadireanu , D. Britton , G. Britvich , M. B. Brunetti , D. Bryman , F. Bucci , F. Butin , J. Calvo , E. Capitolo , C. Capoccia , T. Capussela , A. Cassese , A. Catinaccio , A. Cecchetti , A. Ceccucci , P. Cenci , V. Cerny , C. Cerri , B. Checcucci , O. Chikilev , S. Chiozzi , R. Ciaranfi , G. Collazuol , A. Conovaloff , P. Cooke , P. Cooper , G. Corradi , E. Cortina Gil , F. Costantini , F. Cotorobai , A. Cotta Ramusino , D. Coward , G. D'Agostini , J. Dainton , P. Dalpiaz , H. Danielsson , J. Degrange , N. De Simone , D. Di Filippo , L. Di Lella , S. Di Lorenzo , N. Dixon , N. Doble , B. Dobrich , V. Duk , V. Elsha , J. Engelfried , T. Enik , N. Estrada , V. Falaleev , R. Fantechi , V. Fascianelli , L. Federici , S. Fedotov , A. Filippi , M. Fiorini , J. Fry , J. Fu , A. Fucci , L. Fulton , S. Gallorini , S. Galeotti , E. Gamberini , L. Gatignon , G. Georgiev , S. Ghinescu , A. Gianoli , M. Giorgi , S. Giudici , L. Glonti , A. Goncalves Martins , F. Gonnella , E. Goudzovski , R. Guida , E. Gushchin , F. Hahn , B. Hallgren , H. Heath , F. Herman , T. Husek , O. Hutanu , D. Hutchcroft , L. Iacobuzio , E. Iacopini , E. Imbergamo , O. Jamet , P. Jarron , E. Jones , T. Jones K. Kampf , J. Kaplon , V. Kekelidze , S. Kholodenko , G. Khoriauli , A. Khotyantsev , A. Khudyakov , Yu. Kiryushin , A. Kleimenova , K. Kleinknecht , A. Kluge , M. Koval , V. Kozhuharov , M. Krivda , Z. Kucerova , Yu. Kudenko , J. Kunze , G. Lamanna , G. Latino , C. Lazzeroni , G. Lehmann-Miotto , R. Lenci , M. Lenti , E. Leonardi , P. Lichard , R. Lietava , V. Likhacheva , L. Litov , R. Lollini , D. Lomidze , A. Lonardo , M. Lupi , N. Lurkin , K. McCormick , D. Madigozhin , G. Maire , C. Mandeiro , I. Mannelli , G. Mannocchi , A. Mapelli , F. Marchetto , R. Marchevski , S. Martellotti , P. Massarotti , K. Massri , P. Matak , E. Maurice , M. Medvedeva , A. Mefodev , E. Menichetti , E. Migliore , E. Minucci , M. Mirra , M. Misheva , N. Molokanova , J. Morant , M. Morel , M. Moulson , S. Movchan , D. Munday , M. Napolitano , I. Neri , F. Newson , J. Noël , A. Norton , M. Noy , G. Nuessle , T. Numao , V. Obraztsov , A. Ostankov , S. Padolski , R. Page , V. Palladino , G. Paoluzzi , C. Parkinson , E. Pedreschi , M. Pepe , F. Perez Gomez , M. Perrin-Terrin , L. Peruzzo , P. Petrov , F. Petrucci , R. Piandani , M. Piccini , D. Pietreanu , J. Pinzino , I. Polenkevich , L. Pontisso , Yu. Potrebenikov , D. Protopopescu , F. Raffaelli , M. Raggi , P. Riedler , A. Romano , P. Rubin , G. Ruggiero , V. Russo , V. Ryjov , A. Salamon , G. Salina , V. Samsonov , C. Santoni , G. Saracino , F. Sargeni , V. Semenov , A. Sergi , M. Serra , A. Shaikhiev , S. Shkarovskiy , I. Skillicorn , D. Soldi , A. Sotnikov , V. Sugonyaev , M. Sozzi , T. Spadaro , F. Spinella , R. Staley , A. Sturgess , P. Sutcliffe , N. Szilasi , D. Tagnani , S. Trilov , M. Valdata-Nappi , P. Valente , M. Vasile , T. Vassilieva , B. Velghe , M. Veltri , S. Venditti , P. Vicini , R. Volpe , M. Vormstein , H. Wahl , R. Wanke , P. Wertelaers , A. Winhart , R. Winston , B. Wrona , O. Yushchenko , M. Zamkovsky , A. Zinchenko

These lectures are an introduction to the subject of chiral effective Lagrangians of the Standard Model and their applications, mostly in the sector of non--leptonic kaon decays, with special emphasis on CP--violation. The first lecture…

High Energy Physics - Phenomenology · Physics 2016-09-01 Eduardo de Rafael

In Ref [1] we have presented the results of an exploratory lattice QCD computation of the long-distance contribution to the $K^+\to\pi^+\nu\bar{\nu}$ decay amplitude. In the present paper we describe the details of this calculation, which…

High Energy Physics - Lattice · Physics 2018-10-24 Ziyuan Bai , Norman H. Christ , Xu Feng , Andrew Lawson , Antonin Portelli , Christopher T. Sachrajda

We present the inconsistencies which arise in quenched QCD in $\Delta I=1/2$ non-leptonic kaon decays using chiral perturbation theory (ChPT) to one loop. In particular we discuss how the lack of unitarity of the quenched theory invalidates…

High Energy Physics - Lattice · Physics 2016-09-01 C. J. D. Lin , G. Martinelli , E. Pallante , C. T. Sachrajda , G. Villadoro
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