002632390 001__ 2632390
002632390 005__ 20210715052112.0
002632390 0248_ $$aoai:cds.cern.ch:2632390$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
002632390 037__ $$9arXiv$$aarXiv:1807.09101$$chep-ex
002632390 035__ $$9arXiv$$aoai:arXiv.org:1807.09101
002632390 035__ $$9Inspire$$aoai:inspirehep.net:1683771$$d2021-07-05T13:58:36Z$$h2021-07-14T19:23:35Z$$mmarcxml$$ttrue$$uhttps://inspirehep.net/api/oai2d
002632390 035__ $$9Inspire$$a1683771
002632390 041__ $$aeng
002632390 100__ $$aPinzino, Jacopo$$iINSPIRE-00646735
002632390 245__ $$9arXiv$$aSearch for $K^{+}\rightarrow\pi^{+}\nu\overline{\nu}$ at NA62
002632390 269__ $$c2018-07-24
002632390 260__ $$c2018
002632390 300__ $$a8 p
002632390 500__ $$a* Temporary entry *
002632390 500__ $$9Inspire$$a* Temporary entry *
002632390 500__ $$9arXiv$$aproceeding of the conference New Trends in High-Energy Physics 2016
002632390 520__ $$9arXiv$$a$K^{+}\rightarrow\pi^{+}\nu\overline{\nu}$ is one of the theoretically cleanest meson decay where to look for indirect effects of new physics complementary to LHC searches. The NA62 experiment at CERN SPS is designed to measure the branching ratio of this decay with 10\% precision. NA62 took data in pilot runs in 2014 and 2015 reaching the final designed beam intensity. The quality of 2015 data acquired, in view of the final measurement, will be presented.
002632390 540__ $$3preprint$$aarXiv nonexclusive-distrib 1.0$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
002632390 65017 $$2arXiv$$aphysics.ins-det
002632390 65017 $$2SzGeCERN$$aDetectors and Experimental Techniques
002632390 65017 $$2arXiv$$ahep-ex
002632390 65017 $$2SzGeCERN$$aParticle Physics - Experiment
002632390 690C_ $$aCERN
002632390 690C_ $$aPREPRINT
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002632390 700__ $$aAzhinenko, I.
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002632390 700__ $$aCotta Ramusino, A.$$iINSPIRE-00293524
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002632390 700__ $$aIacobuzio, L.$$iINSPIRE-00646900
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002632390 700__ $$aJamet, O.
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002632390 700__ $$aJones, E.$$iINSPIRE-00647515
002632390 700__ $$aKampf, T. Jones K.
002632390 700__ $$aKaplon, J.
002632390 700__ $$aKekelidze, V.$$iINSPIRE-00187700
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002632390 700__ $$aKhudyakov, A.$$iINSPIRE-00647109
002632390 700__ $$aKiryushin, Yu.
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002632390 700__ $$aKozhuharov, V.$$iINSPIRE-00169974
002632390 700__ $$aKrivda, M.
002632390 700__ $$aKucerova, Z.$$iINSPIRE-00658154
002632390 700__ $$aKudenko, Yu.
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002632390 700__ $$aLamanna, G.$$iINSPIRE-00184369
002632390 700__ $$aLatino, G.
002632390 700__ $$aLazzeroni, C.$$iINSPIRE-00100355
002632390 700__ $$aLehmann-Miotto, G.
002632390 700__ $$aLenci, R.$$iINSPIRE-00646604
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002632390 700__ $$aLeonardi, E.$$iINSPIRE-00191014
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002632390 700__ $$aLietava, R.
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002632390 700__ $$aMaire, G.$$iINSPIRE-00314159
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002632390 700__ $$aMartellotti, S.
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002632390 700__ $$aMorant, J.
002632390 700__ $$aMorel, M.
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002632390 700__ $$aMovchan, S.$$iINSPIRE-00109340
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002632390 700__ $$aSkillicorn, I.
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002632390 700__ $$aTrilov, S.$$iINSPIRE-00658186
002632390 700__ $$aValdata-Nappi, M.
002632390 700__ $$aValente, P.$$iINSPIRE-00224909
002632390 700__ $$aVasile, M.
002632390 700__ $$aVassilieva, T.$$iINSPIRE-00646650
002632390 700__ $$aVelghe, B.$$iINSPIRE-00534512
002632390 700__ $$aVeltri, M.$$iINSPIRE-00258261
002632390 700__ $$aVenditti, S.$$iINSPIRE-00293723
002632390 700__ $$aVicini, P.$$iINSPIRE-00646829
002632390 700__ $$aVolpe, R.$$iINSPIRE-00312874
002632390 700__ $$aVormstein, M.$$iINSPIRE-00645616
002632390 700__ $$aWahl, H.$$iINSPIRE-00288993
002632390 700__ $$aWanke, R.$$iINSPIRE-00134925
002632390 700__ $$aWertelaers, P.
002632390 700__ $$aWinhart, A.$$iINSPIRE-00293628
002632390 700__ $$aWinston, R.$$iINSPIRE-00326834
002632390 700__ $$aWrona, B.
002632390 700__ $$aYushchenko, O.$$iINSPIRE-00200283
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002632390 710__ $$gNA62 Collaboration
002632390 773__ $$wC16-10-02
002632390 8564_ $$81422120$$s31468$$uhttps://cds.cern.ch/record/2632390/files/mmisssigma.png$$y00002 Resolution of the $m^{2}_{miss}$ miss vs momentum. Empty squares correspond to the values obtained with the nominal kaon momentum, black points - with the kaon momentum measured by GTK.
002632390 8564_ $$81422121$$s345673$$uhttps://cds.cern.ch/record/2632390/files/mmiss3.png$$y00003 $m^{2}_{miss}$ distributions for signal and backgrounds from the main $ \mathrm{K^{+}} $ decay modes. The backgrounds are normalized according to their branching fraction; the espected signal is shown multiplied by a factor $10^{10}$.
002632390 8564_ $$81422122$$s771810$$uhttps://cds.cern.ch/record/2632390/files/1807.09101.pdf$$yFulltext
002632390 8564_ $$81422123$$s131264$$uhttps://cds.cern.ch/record/2632390/files/detectors.png$$y00000 Longitudinal view of the NA62 experimental setup.
002632390 8564_ $$81422124$$s73648$$uhttps://cds.cern.ch/record/2632390/files/missingmass_nokaon.png$$y00004 $m^{2}_{miss}$ distribution under $\pi^{+}$ mass hypothesis as a function of the momentum of the track measured in the straw spectrometer after selection for single track from kaon decays (left). Same distribution as left-side picture, but asking for single track without a positive kaon tag in time in KTAG (right).
002632390 8564_ $$81422125$$s75260$$uhttps://cds.cern.ch/record/2632390/files/missingmass_kaon.png$$y00001 $m^{2}_{miss}$ distribution under $\pi^{+}$ mass hypothesis as a function of the momentum of the track measured in the straw spectrometer after selection for single track from kaon decays (left). Same distribution as left-side picture, but asking for single track without a positive kaon tag in time in KTAG (right).
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