abstract

• The main goal of the NA62 experiment at CERN is to measure the branching ratio of the ultra-rare K →π vv decay with 10%25 accuracy. NA62 will use a 750 MHz high-energy un-separated charged hadron beam, with kaons corresponding to ~ 6%25 of the beam, and a kaon decay-in-flight technique. The positive identification of kaons is performed with a differential Cherenkov detector (CEDAR), filled with Nitrogen gas and placed in the incoming beam. To stand the kaon rate (45 MHz average) and meet the performances required in NA62, the Cherenkov detector has been upgraded (KTAG) with new photon detectors, readout, mechanics and cooling systems. The KTAG provides a fast identification of kaons with an efficiency of at least 95%25 and precise time information with a resolution below 100 ps. A half-equipped KTAG detector has been commissioned during a technical run at CERN in 2012, while the fully equipped detector, its readout and front-end have been commissioned during a pilot run at CERN in October 2014. The measured time resolution and efficiency are within the required performances. © 2015 IEEE.
• The main goal of the NA62 experiment at CERN is to measure the branching ratio of the ultra-rare K%2b →π%2b vv decay with 10%25 accuracy. NA62 will use a 750 MHz high-energy un-separated charged hadron beam, with kaons corresponding to ~ 6%25 of the beam, and a kaon decay-in-flight technique. The positive identification of kaons is performed with a differential Cherenkov detector (CEDAR), filled with Nitrogen gas and placed in the incoming beam. To stand the kaon rate (45 MHz average) and meet the performances required in NA62, the Cherenkov detector has been upgraded (KTAG) with new photon detectors, readout, mechanics and cooling systems. The KTAG provides a fast identification of kaons with an efficiency of at least 95%25 and precise time information with a resolution below 100 ps. A half-equipped KTAG detector has been commissioned during a technical run at CERN in 2012, while the fully equipped detector, its readout and front-end have been commissioned during a pilot run at CERN in October 2014. The measured time resolution and efficiency are within the required performances. © 2015 IEEE.

authors

• Aglieri Rinella G.
• Aliberti R.
• Ambrosino F.
• Angelucci B.
• Antonelli A.
• Anzivino G.
• Arcidiacono R.
• Azhinenko I.
• Balev S.
• Bendotti J.
• Biagioni A.
• Biino C.
• Bizzeti A.
• Blazek T.
• Blik A.
• Bloch-Devaux B.
• Bolotov V.
• Bonaiuto V.
• Bragadireanu M.
• Britton D.
• Britvich G.
• Bucci F.
• Butin F.
• Capitolo E.
• Capoccia C.
• Capussela T.
• Carassiti V.
• Cartiglia N.
• Cassese A.
• Catinaccio A.
• Cecchetti A.
• Ceccucci A.
• Cenci P.
• Cerny V.
• Cerri C.
• Checcucci B.
• Chikilev O.
• Ciaranfi R.
• Collazuol G.
• Conovaloff A.
• Cooke P.
• Cooper P.
• Corradi G.
• Cortina Gil E.
• Costantini F.
• Cotta Ramusino A.
• Coward D.
• D'Agostini G.
• Dainton J.
• Dalpiaz P.
• Danielsson H.
• De Simone N.
• Degrange J.
• Di Filippo D.
• Di Lella L.
• Dixon N.
• Doble N.
• Duk V.
• Elsha V.
• Engelfried Jatzkowski Jurgen
• Enik T.
• Falaleev V.
• Fantechi R.
• Fascianelli V.
• Federici L.
• Fiorini M.
• Fry J.
• Fucci A.
• Fulton L.
• Gallorini S.
• Gamberini E.
• Gatignon L.
• Georgiev G.
• Gianoli A.
• Giorgi M.
• Giudici S.
• Glonti L.
• Goncalves Martins A.
• Gonnella F.
• Goudzovski E.
• Guida R.
• Gushchin E.
• Hahn F.
• Hallgren B.
• Heath H.
• Herman F.
• Hutchcroft D.
• Iacopini E.
• Imbergamo E.
• Jamet O.
• Jarron P.
• Kampf K.
• Kaplon J.
• Karjavin V.
• Kekelidze V.
• Kholodenko S.
• Khoriauli G.
• Khudyakov A.
• Kiryushin Y.
• Kleinknecht K.
• Kluge A.
• Koval M.
• Kozhuharov V.
• Krivda M.
• Kudenko Y.
• Kunze J.
• Lamanna G.
• Lazzeroni C.
• Lenci R.
• Lenti M.
• Leonardi E.
• Lichard P.
• Lietava R.
• Litov L.
• Lomidze D.
• Lonardo A.
• Lurkin N.
• Madigozhin D.
• Maire G.
• Makarov A.
• Mandeiro C.
• Mannelli I.
• Mannocchi G.
• Mapelli A.
• Marchetto F.
• Marchevski R.
• Martellotti S.
• Massarotti P.
• Massri K.
• Matak P.
• Maurice E.
• Menichetti E.
• Mila G.
• Minucci E.
• Mirra M.
• Misheva M.
• Molokanova N.
• Morant J.
• Morel M.
• Moulson M.
• Movchan S.
• Munday D.
• Napolitano M.
• Neri I.
• Newson F.
• Norton A.
• Noy M.
• Nuessle G.
• Obraztsov V.
• Ostankov A.
• Padolski S.
• Page R.
• Palladino V.
• Pardons A.
• Parkinson C.
• Pedreschi E.
• Pepe M.
• Perez Gomez F.
• Perrin-Terrin M.
• Peruzzo L.
• Petrov P.
• Petrucci F.
• Piandani R.
• Piccini M.
• Pietreanu D.
• Pinzino J.
• Pivanti M.
• Polenkevich I.
• Popov I.
• Potrebenikov Y.
• Protopopescu D.
• Raffaelli F.
• Raggi M.
• Riedler P.
• Romano A.
• Rubin P.
• Ruggiero G.
• Russo V.
• Ryjov V.
• Salamon A.
• Salina G.
• Samsonov V.
• Santoni C.
• Santovetti E.
• Saracino G.
• Sargeni F.
• Schifano S.
• Semenov V.
• Sergi A.
• Serra M.
• Shkarovskiy S.
• Soldi D.
• Sotnikov A.
• Sougonyaev V.
• Sozzi M.
• Spadaro T.
• Spinella F.
• Staley R.
• Statera M.
• Sutcliffe P.
• Szilasi N.
• Tagnani D.
• Valdata-Nappi M.
• Valente P.
• Vasile M.
• Vassilieva T.
• Velghe B.
• Veltri M.
• Venditti S.
• Volpe R.
• Vormstein M.
• Wahl H.
• Wanke R.
• Wertelaers P.
• Winhart A.
• Winston R.
• Wrona B.
• Yushchenko O.
• Zamkovsky M.
• Zinchenko A.

publication date

• 2015-01-01

funding provided via

• Science and Technology Facilities Council, STFC: ST/K001256/1  Grant
• Science and Technology Facilities Council, STFC: ST/N000250/1  Grant

published in

• 2015 4th International Conference on Advancements in Nuclear Instrumentation Measurement Methods and their Applications, ANIMMA 2015  Proceedings

keywords

• Cherenkov light; gas detector; kaons; NA62; PID Bosons; Cerenkov counters; Cooling systems; Gas detectors; Particle detectors; Photons; Charged hadrons; Cherenkov Detectors; Cherenkov light; Kaon identification; kaons; NA62; Photon detector; Time information; Hadrons

Digital Object Identifier (DOI)

• 10.1109/ANIMMA.2015.7465642

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