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The precision measurement of $K^{+} \rightarrow \pi^{+} \nu \bar{\nu}$ at the NA62 experiment requires a kaon identification detector to have a time resolution better than 100ps, at least 95% kaon identification efficiency, and a pion…

High Energy Physics - Experiment · Physics 2024-01-19 Jack Sanders

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…

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 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

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 NA62 experiment is a fixed-target experiment at CERN SPS. The main goal of the experiment is to measure the branching ratio of the ultra-rare kaon decay $K^{+}\to\pi^{+}\nu\bar\nu$. The NA62 detector allows also to study other rare kaon…

The NA62 experiment will begin taking data in 2015. Its primary purpose is a 10% measurement of the branching ratio of the ultrarare kaon decay $K^+ \to \pi^+ \nu \bar{ \nu }$, using the decay in flight of kaons in an unseparated beam with…

High Energy Physics - Experiment · Physics 2014-11-04 G. Aglieri Rinella , R. Aliberti , F. Ambrosino , B. Angelucci , A. Antonelli , G. Anzivino , R. Arcidiacono , I. Azhinenko , S. Balev , J. Bendotti , A. Biagioni , C. Biino , A. Bizzeti , T. Blazek , A. Blik , B. Bloch-Devaux , V. Bolotov , V. Bonaiuto , M. Bragadireanu , D. Britton , G. Britvich , N. Brook , F. Bucci , V. Buescher , F. Butin , E. Capitolo , C. Capoccia , T. Capussela , V. Carassiti , N. Cartiglia , A. Cassese , A. Catinaccio , A. Cecchetti , A. Ceccucci , P. Cenci , V. Cerny , C. Cerri , O. Chikilev , R. Ciaranfi , G. Collazuol , P. Cooke , P. Cooper , G. Corradi , E. Cortina Gil , F. Costantini , 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 , N. Dixon , N. Doble , V. Duk , V. Elsha , J. Engelfried , T. Enik , V. Falaleev , R. Fantechi , L. Federici , M. Fiorini , J. Fry , A. Fucci , L. Fulton , S. Gallorini , L. Gatignon , A. Gianoli , S. Giudici , L. Glonti , A. Goncalves Martins , F. Gonnella , E. Goudzovski , R. Guida , E. Gushchin , F. Hahn , B. Hallgren , H. Heath , F. Herman , D. Hutchcroft , E. Iacopini , O. Jamet , P. Jarron , K. Kampf , J. Kaplon , V. Karjavin , V. Kekelidze , S. Kholodenko , G. Khoriauli , A. Khudyakov , Yu. Kiryushin , K. Kleinknecht , A. Kluge , M. Koval , V. Kozhuharov , M. Krivda , Y. Kudenko , J. Kunze , G. Lamanna , C. Lazzeroni , R. Leitner , R. Lenci , M. Lenti , E. Leonardi , P. Lichard , R. Lietava , L. Litov , D. Lomidze , A. Lonardo , N. Lurkin , D. Madigozhin , G. Maire , A. Makarov , I. Mannelli , G. Mannocchi , A. Mapelli , F. Marchetto , P. Massarotti , K. Massri , P. Matak , G. Mazza , E. Menichetti , M. Mirra , M. Misheva , N. Molokanova , J. Morant , M. Morel , M. Moulson , S. Movchan , D. Munday , M. Napolitano , F. Newson , A. Norton , M. Noy , G. Nuessle , V. Obraztsov , S. Padolski , R. Page , V. Palladino , A. Pardons , E. Pedreschi , M. Pepe , F. Perez Gomez , M. Perrin-Terrin , P. Petrov , F. Petrucci , R. Piandani , M. Piccini , D. Pietreanu , J. Pinzino , M. Pivanti , I. Polenkevich , I. Popov , 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 , E. Santovetti , G. Saracino , F. Sargeni , S. Schifano , V. Semenov , A. Sergi , M. Serra , S. Shkarovskiy , A. Sotnikov , V. Sougonyaev , M. Sozzi , T. Spadaro , F. Spinella , R. Staley , M. Statera , P. Sutcliffe , N. Szilasi , D. Tagnani , M. Valdata-Nappi , P. Valente , M. Vasile , V. Vassilieva , B. Velghe , M. Veltri , S. Venditti , M. Vormstein , H. Wahl , R. Wanke , P. Wertelaers , A. Winhart , R. Winston , B. Wrona , O. Yushchenko , M. Zamkovsky , A. Zinchenko

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 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

The RICH detector of the NA62 experiment at CERN SPS is required to suppress $\mu^+$ contamination in $K^+ \to \pi^+ \nu \bar\nu$ candidate events by a factor at least 100 between 15 and 35 GeV/c momentum, to measure the pion arrival time…

Instrumentation and Detectors · Physics 2017-06-27 Andrea Bizzeti

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

A system for determining the purity of liquid krypton employed in the NA62 rare kaon decay experiment at CERN was developed based on the use of a time projection chamber. The attenuation of drifting ionization electrons from absorption of…

The NA62 experiment at CERN targets the measurement of the ultra-rare $K^{+} \to \pi^{+}\nu\bar{\nu}$ decay, and carries out a broad physics programme that includes probes for symmetry violations and searches for exotic particles. Data were…

High Energy Physics - Experiment · Physics 2023-03-10 The NA62 Collaboration

The NA62 experiment at the CERN SPS reports the first detection of a tagged neutrino candidate based on the data collected in 2022. The candidate consists of a $K^+ \rightarrow \mu^+ \nu_\mu$ decay where the charged particles are…

High Energy Physics - Experiment · Physics 2025-03-07 NA62 Collaboration

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'

We discuss the design and performance of a threshold Cerenkov counter for identification of charged hadrons. The radiator is pressurized gas, which is contained in thin-walled cylindrical modules. A mirror system of novel design transports…

High Energy Physics - Experiment · Physics 2008-11-26 Michael Sivertz , Bruce Berger , Richard Ehrlich , John Bartlet , Steven Csorna , Vivek Jain , Szabolcs Marka , Kay Kinoshita , Paula Pomianowski

A powerful way to test models with feebly interacting particles in the MeV to GeV mass range is through proton beam-dump experiments. In this paper, we compare the current sensitivity of CERN's NA62 experiment running in beam-dump mode with…

High Energy Physics - Experiment · Physics 2026-04-21 Babette Döbrich , Jan Jerhot , Karim Massri , Jonathan L. Schubert , Tommaso Spadaro

The Kaon physics program at CERN will be shortly presented, addressing the most recent results from the NA48/2 and NA62 experiments at the CERN SPS and future prospects.

High Energy Physics - Experiment · Physics 2015-06-19 Patrizia Cenci

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
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