Results And Perspectives From The Na62 Experiment At Cern

G. Aglieri Rinella,R. Aliberti,F. Ambrosino,Roberto Ammendola,B Angelucci,A. Antonelli,G. Anzivino,R. Arcidiacono,I Azhinenko,S. Balev,M. Barbanera,M Bbrunetti,J. Bendotti,A Biagioni,L Bician,C. Biino,A. Bizzeti,T. Blazek,A Blik,B. Bloch-Devaux, Bolotov, Bonaiuto,M Boretto,M. Bragadireanu,D. Britton,G Britvich,D. A. Bryman,F. Bucci,F. Butin,E. Capitolo,C. Capoccia,T Capussela,A. Cassese,A Catinaccio,A. Cecchetti,A. Ceccucci,P. Cenci, 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.B. Dainton,P. Dalpiaz,H. O. Danielsson,J. Degrange,N Desimone,D. Di Filippo,L. Di Lella,S Di Lorenzo,N Dixon,N. Doble,B Dobrich, Duk, Elsha,J. Engelfried,T. Enik,N Estrada, Falaleev,R. Fantechi, Fascianelli,L. Federici,S. Fedotov,M. Fiorini,J. R. Fry,J Fu,A. Fucci,L Fulton,S Galeotti,S. Gallorini,E. Gamberini,L. Gatignon,Georgi Georgiev,A. Gianoli,M. Giorgi,S. Giudici,L. Glonti,A. Goncalves Martins,F Gonnella,E. Goudzovski,R. Guida,E. Gushchin,F. Hahn,B. Hallgren,H. F. Heath,F Herman,T Husek,O Hutanu,D. Hutchcroft,L Iacobuzio,E. Iacopini,E. Imbergamo,O Jamet,P. Jarron,E Jones, T Jones KKampf,J. Kaplon, Kekelidze,S. Kholodenko,G. Khoriauli,A. Khotyantsev,A Khudyakov,Y Kiryushin,A Kleimenova,K. Kleinknecht,A. Kluge,M Koval, Kozhuharov,M. Krivda,Z Kucerova,Y. Kudenko,J Kunze,G. Lamanna,G Latino,C. Lazzeroni,G Lehmann-Miotto,R. Lenci,M. Lenti,E. Leonardi,P. Lichard,R Lietava,L. Litov,R Lollini,D. Lomidze,A Lonardo,M Lupi,N. Lurkin,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,K Mccormick,A Mefodev,E. Menichetti,E. Minucci,M Mirra,Milena Misheva,N. Molokanova,J. Morant,M. Morel,M. Moulson,S. Movchan,D.J. Munday,M. Napolitano,I. Neri,F Newson,A. Norton,M. Noy,G Nuessle,T. Numao, Obraztsov,A. Ostankov,S Padolski,R Page, Palladino,G Paoluzzi,C. J. 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,Y Potrebenikov,D. Protopopescu,F. Raffaelli,M. Raggi,P. Riedler,A. Romano,P. Rubin,G. Ruggiero, Russo, Ryjov,A. Salamon,G. Salina, Samsonov,C. Santoni,G. Saracino,F. Sargeni, Semenov,A. Sergi,M. Serra,A. Shaikhiev,S. Shkarovskiy,I.O. Skillicorn,D. Soldi,A. Sotnikov,M. Sozzi,T. Spadaro,F. Spinella,R. Staley,A Sturgess, Sugonyaev,P. Sutcliffe,N Szilasi,D. Tagnani,S Trilov,M. Valdata-Nappi,Paolo 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

NUOVO CIMENTO C-COLLOQUIA AND COMMUNICATIONS IN PHYSICS（2016）

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Abstract

The NA62 experiment at the CERN SPS collected a large sample of charged kaon decays with a highly efficient trigger for decays into electrons in 2007. The kaon beam represents a source of tagged neutral pion decays in vacuum. A preliminary result of a new measurement of the electromagnetic transition form factor slope of the neutral pion in the time-like momentum region from 1.05 million fully reconstructed pi(0) Dalitz decays is presented in the first part of this report. In the second part, prospects and current status of a new measurement of B( K+ -> pi(+) nu(nu) over bar.)at the NA62 experiment are summarised. The experiment took data in physics runs in 2014 and 2015 reaching the designed beam intensity.

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Key words

Quantum Chromodynamics

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