The NA62 experiment at CERN SPS collected a large sample of charged kaon decays with a highly efficient trigger for decays into electrons in 2007 using the experimental setup of the earlier kaon experiment at CERN NA48/2. The kaon beam represents a source of tagged neutral pion decays in vacuum. A measurement of the electromagnetic transition form factor slope of the neutral pion in the time-like region from about 1 million fully reconstructed π0 Dalitz decay is described. The K+ → π+νν¯ decay is one of the theoretically cleanest meson decays where to look for indirect effects of new physics complementary to LHC searches. The new experimental setup used by the NA62 experiment at CERN SPS since 2014 is designed to measure the branching ratio of this decay with 10% precision. NA62 took data with the new setup in pilot runs in 2014 and 2015 reaching the final designed beam intensity. The quality of data acquired in view of the final measurement is reported.

Ruggiero, G., Aglieri Rinella, G., Aliberti, R., Ambrosino, F., Ammendola, R., Angelucci, B., et al. (2016). π0 form factor and K+ → π+νν¯ at NA62. In Proceedings of the 51st Rencontres de Moriond - 2016 Electroweak Interactions and Unified Theories, EW 2016 (pp.101-108). ARISF.

π0 form factor and K+ → π+νν¯ at NA62

Bonaiuto V.;Sargeni F.;
2016-01-01

Abstract

The NA62 experiment at CERN SPS collected a large sample of charged kaon decays with a highly efficient trigger for decays into electrons in 2007 using the experimental setup of the earlier kaon experiment at CERN NA48/2. The kaon beam represents a source of tagged neutral pion decays in vacuum. A measurement of the electromagnetic transition form factor slope of the neutral pion in the time-like region from about 1 million fully reconstructed π0 Dalitz decay is described. The K+ → π+νν¯ decay is one of the theoretically cleanest meson decays where to look for indirect effects of new physics complementary to LHC searches. The new experimental setup used by the NA62 experiment at CERN SPS since 2014 is designed to measure the branching ratio of this decay with 10% precision. NA62 took data with the new setup in pilot runs in 2014 and 2015 reaching the final designed beam intensity. The quality of data acquired in view of the final measurement is reported.
51st Rencontres de Moriond on Electroweak Interactions and Unified Theories, EW 2016
Aosta Valley, ita
2016
Belgian Science Policy (BSP)
Rilevanza internazionale
2016
Settore FIS/04
English
Intervento a convegno
Ruggiero, G., Aglieri Rinella, G., Aliberti, R., Ambrosino, F., Ammendola, R., Angelucci, B., et al. (2016). π0 form factor and K+ → π+νν¯ at NA62. In Proceedings of the 51st Rencontres de Moriond - 2016 Electroweak Interactions and Unified Theories, EW 2016 (pp.101-108). ARISF.
Ruggiero, G; Aglieri Rinella, G; Aliberti, R; Ambrosino, F; Ammendola, R; Angelucci, B; Antonelli, A; Anzivino, G; Arcidiacono, R; Azhinenko, I; Balev, S; Barbanera, M; Bendotti, J; Biagioni, A; Bician, L; Biino, C; Bizzeti, A; Blazek, T; Blik, A; Bloch-Devaux, B; Bolotov, V; Bonaiuto, V; Boretto, M; Bragadireanu, M; Britton, D; Britvich, G; Brunetti, Mb; Bryman, D; Bucci, F; Butin, F; Capitolo, E; Capoccia, C; Capussela, T; Cassese, A; Catinaccio, A; Cecchetti, A; Ceccucci, A; Cenci, P; Cerny, V; Cerri, C; Checcucci, B; Chikilev, O; Chiozzi, S; Ciaranfi, R; Collazuol, G; Conovaloff, A; Cooke, P; Cooper, P; Corradi, G; Cortina Gil, E; Costantini, F; Cotorobai, F; Cotta Ramusino, A; Coward, D; D'Agostini, G; Dainton, J; Dalpiaz, P; Danielsson, H; Degrange, J; de Simone, N; Di Filippo, D; Di Lella, L; Di Lorenzo, S; Dixon, N; Doble, N; Dobrich, B; Duk, V; Elsha, V; Engelfried, J; Enik, T; Estrada, N; Falaleev, V; Fantechi, R; Fascianelli, V; Federici, L; Fedotov, S; Fiorini, M; Fry, J; Fu, J; Fucci, A; Fulton, L; Gallorini, S; Galeotti, 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; Husek, T; Hutanu, O; Hutchcroft, D; Iacobuzio, L; Iacopini, E; Imbergamo, E; Jamet, O; Jarron, P; Jones, E; Jones, T; Kampf, K; Kaplon, J; Kekelidze, V; Kholodenko, S; Khoriauli, G; Khotyantsev, A; Khudyakov, A; Kiryushin, Y; Kleimenova, A; Kleinknecht, K; Kluge, A; Koval, M; Kozhuharov, V; Krivda, M; Kucerova, Z; Kudenko, Y; Kunze, J; Lamanna, G; Latino, G; Lazzeroni, C; Lehmann-Miotto, G; Lenci, R; Lenti, M; Leonardi, E; Lichard, P; Lietava, R; Litov, L; Lollini, R; Lomidze, D; Lonardo, A; Lupi, M; Lurkin, N; Mccormick, K; Madigozhin, D; Maire, G; Mandeiro, C; Mannelli, I; Mannocchi, G; Mapelli, A; Marchetto, F; Marchevski, R; Martellotti, S; Massarotti, P; Massri, K; Matak, P; Maurice, E; Mefodev, A; Menichetti, E; 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; Numao, T; Obraztsov, V; Ostankov, A; Padolski, S; Page, R; Palladino, V; Paoluzzi, G; 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; Polenkevich, I; Pontisso, L; 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; Saracino, G; Sargeni, F; Semenov, V; Sergi, A; Serra, M; Shaikhiev, A; Shkarovskiy, S; Skillicorn, I; Soldi, D; Sotnikov, A; Sugonyaev, V; Sozzi, M; Spadaro, T; Spinella, F; Staley, R; Sturgess, A; Sutcliffe, P; Szilasi, N; Tagnani, D; Trilov, S; Valdata-Nappi, M; Valente, P; Vasile, M; Vassilieva, T; Velghe, B; Veltri, M; Venditti, S; Vicini, P; Volpe, R; Vormstein, M; Wahl, H; Wanke, R; Wertelaers, P; Winhart, A; Winston, R; Wrona, B; Yushchenko, O; Zamkovsky, M; Zinchenko, A
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2108/345784
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