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Precise measurements of the branching ratios for the flavor-changing neutral current decays $K\to\pi\nu\bar{\nu}$ can provide unique constraints on CKM unitarity and, potentially, evidence for new physics. It is important to measure both…

Instrumentation and Detectors · Physics 2018-12-06 Matthew Moulson

Precise measurements of the branching ratios for the $K\to\pi\nu\bar{\nu}$ decays can provide unique constraints on CKM unitarity and, potentially, evidence for new physics. It is important to measure both decay modes,…

High Energy Physics - Experiment · Physics 2016-11-16 M. Moulson

The ultra-rare decay $K^+\to\pi^+\nu\bar\nu$ is a golden mode in flavor physics. The Standard Model prediction for its branching ratio is below $10^{-10}$. This decay mode is highly sensitive to new physics models at mass scales up to…

High Energy Physics - Experiment · Physics 2026-05-08 Xiafei Chang , for the NA62 Collaboration

Searches for heavy neutrinos can be successfully performed by fixed target experiments at the CERN SPS. New results obtained by the NA62 and NA48/2 kaon experiments are summarized in this paper. The physics potential of future projects…

High Energy Physics - Experiment · Physics 2018-05-04 Patrizia Cenci

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

$K\rightarrow \pi\nu \bar\nu$ 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

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

Precision studies of flavour-changing processes involving quarks and leptons provide a number of ways to improve knowledge of the Standard Model and search for physics beyond it. There are excellent short- and mid-term prospects for…

High Energy Physics - Experiment · Physics 2025-05-07 The ATLAS Collaboration , Belle II Collaboration , CMS Collaboration , LHCb Collaboration

The NA62 experiment reports an investigation of the $K^+\rightarrow\pi^+\nu\bar{\nu}$ mode from a sample of $K^+$ decays collected in 2017 at the CERN SPS. The experiment has achieved a single event sensitivity of $(0.389\pm…

High Energy Physics - Experiment · Physics 2020-12-02 NA62 Collaboration

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 aims to make a precision measurement of the ultra-rare decay $K^{+} \rightarrow \pi^{+}\nu\overline{\nu}$, and relies on a differential Cherenkov detector (KTAG) to identify charged kaons at an average rate of 50…

The NA62 experiment at CERN SPS aims to measure the Branching Ratio of the very rare kaon decay K+ -> pi+ nu nubar collecting O(100) events with a 10% background to make a stringent test of the Standard Model. One of the main backgrounds to…

The NA62 experiment at CERN SPS aims to measure the Branching Ratio of the very rare kaon decay K+ -> pi+ nu nubar collecting O(100) events with a 10% background to make a stringent test of the Standard Model. One of the main backgrounds to…

Instrumentation and Detectors · Physics 2012-01-17 V. Bonaiuto , A. Fucci , G. Paoluzzi , A. Salamon , G. Salina , E. Santovetti , F. Sargeni , F. M. Scarfi'

The NA62 experiment at CERN SPS is aimed to measure the branching ratio of the ultra-rare decay $K^+\rightarrow\pi^+ \nu \bar{\nu}$ with 10\% accuracy. The experiment operates with a 75 GeV/c high intensity (750 MHz) secondary beam. A new…

Instrumentation and Detectors · Physics 2017-08-02 S. Kholodenko

The NA48/2 and NA62-$R_K$ experiments at the CERN SPS collected large samples of charged kaon decays in flight in 2003--07. The data analysis is still on-going (with over 20 publications produced so far); the recent results from these…

High Energy Physics - Experiment · Physics 2016-12-21 Evgueni Goudzovski

Kaon experiments are now focusing on searching for new physics beyond the standard model. For example, CERN NA62, J-PARC KOTO and J-PARC TREK-E36 experiments are starting up to study K->pi nu nu-bar decay modes, a lepton flavor violation,…

High Energy Physics - Experiment · Physics 2014-12-19 Taku Yamanaka

The CERN SuperProtoSynchrotron (SPS) represents an ideal facility for fixed-target heavy-ion experiments exploring the phase diagram of strongly interacting matter in the region $200\le\mu_{\rm B}\le500$ MeV. It can deliver high-intensity…

Nuclear Experiment · Physics 2023-07-24 E. Scomparin

Recent results from the NA48/2 and NA62 kaon decay-in-flight experiments at CERN are presented. A precision measurement of the helicity-suppressed ratio RK of the K+- to e+- nu and K+- to mu+- nu decay rates has been performed using the…

High Energy Physics - Experiment · Physics 2019-08-14 Evgueni Goudzovski

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

Meson decays offer a good opportunity to probe new physics. The rare kaon decay $K^+ \rightarrow \pi^+ \nu\bar{\nu}$ is one of the cleanest of them and, for this reason, is rather sensitive to new physics, in particular, vector mediators.…

High Energy Physics - Phenomenology · Physics 2021-06-09 Téssio B. de Melo , Sergey Kovalenko , Farinaldo S. Queiroz , C. Siqueira , Yoxara S. Villamizar