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Recent results a future prospects of the NA62 experiment at CERN SPS are presented. The NA62 experiment performed the most precise measurement of the ratio $R_K$ of the $K^+\rightarrow e^\pm\nu$ and K^+\rightarrow \mu^\pm\nu$ decay rates…

High Energy Physics - Experiment · Physics 2012-12-21 Giuseppe Ruggiero

NA62 is a fixed target kaon experiment at the CERN SPS which aims at measuring the branching ratio of the $K^+\to\pi^+\nu\bar{\nu}$ decay with 10% precision. This ultra-rare kaon decay is theoretically extremely clean and an ideal place to…

High Energy Physics - Experiment · Physics 2019-07-31 Nicolas Lurkin

The NA62 experiment at the CERN SPS aims to measure the branching ratio of the rare decay $K^+\to\pi^+\nu\bar\nu$ with a relative precision of $\sim10%$. To achieve that goal, it is designed to be exposed to $1.2\times 10^{13}$ $K^+$ decays…

High Energy Physics - Experiment · Physics 2015-06-17 Evgueni Goudzovski

The decay $K^+ \to \pi^+ \nu \bar{\nu}$, with a very precisely predicted branching ratio of less than $10^{-10}$, is one of the best candidates to reveal indirect effects of new physics at the highest mass scales. The NA62 experiment at the…

High Energy Physics - Experiment · Physics 2019-10-22 Roberta Volpe

The decay $K^+ \to \pi^+\nu\bar{\nu}$ is highly suppressed in the Standard Model (SM), while its rate can be predicted with minimal theoretical uncertainty. The branching ratio (BR) for this decay is thus a sensitive probe of the flavor…

High Energy Physics - Experiment · Physics 2013-10-30 Matthew Moulson

NA62 is a fixed-target kaon experiment at the CERN SPS. The recent measurement of the ultra-rare decay $K^+\to\pi^+\nu\bar\nu$, based on data collected between 2016 and 2024 is reported. The measurement is compatible with previous…

High Energy Physics - Experiment · Physics 2026-05-05 Jonathan Leon Schubert

The main physics goal of the NA62 experiment at CERN is to precisely measure the branching ratio of the kaon rare decay $K^+\rightarrow \pi^+ \nu \bar\nu$. This decay is strongly suppressed in the Standard Model and its branching ratio is…

Instrumentation and Detectors · Physics 2015-10-20 Silvia Martellotti

Rare kaon decays provide unique opportunity to test the Standard Model and probe its possible extensions. The final result on the lepton universality test by measuring the ratio R_K = G(K+- to e+- nu)/G(K+- to mu+- nu) is presented as well…

High Energy Physics - Experiment · Physics 2014-12-02 Venelin Kozhuharov

Searches for violation of lepton flavour universality and lepton number conservation in kaon decays by the NA62 and NA48/2 experiments at CERN, status and future plans of the CERN kaon programme are presented. A precision measurement of the…

High Energy Physics - Experiment · Physics 2020-06-17 Evgueni Goudzovski

The NA62 experiment at CERN aims to use rare kaon decays to search for new phenomena beyond the Standard Model. During the current short term phase (data taking completed in years 2007-8), the ratio $R_K = \Gamma(K^+ \rightarrow e \nu_e…

High Energy Physics - Experiment · Physics 2015-05-27 Cristina Lazzeroni

$K\rightarrow \pi\nu \bar\nu$ 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 branching ratio of…

High Energy Physics - Experiment · Physics 2019-03-27 Silvia Martellotti

The future program of the NA62 experiment at CERN SPS is currently in advanced stage of development. The main goal of the experiment is to measure the branching ratio of the ultra-rare decay K^+ -> pi+\nu\nubar, by detecting approximately…

High Energy Physics - Experiment · Physics 2011-02-01 Tommaso Spadaro

The experiment NA62 at CERN collected a large sample of K+- leptonic decays in order to perform precise test of lepton universality, by measuring the helicity suppressed ratio R_K=Gamma(K+- --> e+- nu)/Gamma(K+- --> mu+- nu). The…

High Energy Physics - Experiment · Physics 2010-06-08 Spasimir Balev

NA62 is a fixed-target experiment at the CERN SPS dedicated to measurements of rare kaon decays. Such measurements, like the branching fraction of the $K^{+} \rightarrow \pi^{+} \nu \bar\nu$ decay, have the potential to bring significant…

Instrumentation and Detectors · Physics 2017-06-28 NA62 collaboration

The ratio $R_K = \Gamma(K^{\pm}\to e^{\pm}\nu(\gamma)) / \Gamma(K^{\pm}\to\mu^{\pm}\nu(\gamma))$ provides a powerful probe of the structure of weak interactions. It is calculated with very high precision within the Standard Model, but…

High Energy Physics - Experiment · Physics 2008-04-30 Evgueni Goudzovski

The main aim of the NA62 experiment at CERN is to study the rare $K^+ \rightarrow \pi^+ \nu \bar{\nu}$ decay and measure its Branching Ratio (BR) with $10%$ precision. Due to its theoretical precision, this decay is an excellent probe to…

High Energy Physics - Experiment · Physics 2014-11-25 Angela Romano

The NA62 experiment at CERN collected a large sample of $K^+\to e^+\nu$ decays during a dedicated run in 2007, which allows a precise test of lepton universality by measurement of the helicity suppressed ratio $R_K = \Gamma(K^+\to…

High Energy Physics - Experiment · Physics 2011-07-19 Evgueni Goudzovski

The NA62 experiment at CERN SPS aims to measure the branching ratio of the ultra-rare kaon decay $K^+\to\pi^+\nu\bar{\nu}$ with 10\% precision, collecting $\sim 100$ events, assuming the Standard Model~(SM) branching ratio of $8.4 \times…

Instrumentation and Detectors · Physics 2016-11-23 Karim Massri

$K^{+}\rightarrow\pi^{+}\nu\overline{\nu}$ 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

The ratio of the leptonic charged kaon decays $R_K= \Gamma(K^{\pm} \to e^{\pm}\nu) / \Gamma(K^{\pm} \to \mu^{\pm}\nu)$ is sensitive to the structure of the week interactions and can be precisely calculated within the Standard Model.…

High Energy Physics - Experiment · Physics 2015-06-23 Venelin Kozhuharov
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