CERN Accelerating science

001328179 001__ 1328179
001328179 003__ SzGeCERN
001328179 005__ 20210910062546.0
001328179 0247_ $$2DOI$$a10.1088/1367-2630/13/5/053051
001328179 0248_ $$aoai:cds.cern.ch:1328179$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
001328179 037__ $$9arXiv$$aarXiv:1102.1882$$chep-ex
001328179 035__ $$9arXiv$$aoai:arXiv.org:1102.1882
001328179 035__ $$9Inspire$$a889038
001328179 041__ $$aeng
001328179 100__ $$aAgafonova, N.$$uMoscow, INR
001328179 245__ $$aStudy of neutrino interactions with the electronic detectors of the OPERA experiment
001328179 269__ $$c10 Feb 2011
001328179 260__ $$c2011
001328179 300__ $$a22 p
001328179 500__ $$aComments: 17 .eps files + 1 .tex file
001328179 500__ $$9Inspire$$aLong author list - awaiting processing
001328179 500__ $$9arXiv$$a17 .eps files + 1 .tex file
001328179 520__ $$aThe OPERA experiment is based on a hybrid technology combining electronic detectors and nuclear emulsions. OPERA collected muon-neutrino interactions during the 2008 and 2009 physics runs of the CNGS neutrino beam, produced at CERN with an energy range of about 5-35 GeV. A total of $5.3 \times 10^{19}$ protons on target equivalent luminosity has been analysed with the OPERA electronic detectors: scintillator strips target trackers and magnetic muon spectrometers equipped with resistive plate gas chambers and drift tubes, allowing a detailed reconstruction of muon-neutrino interactions. Charged Current (CC) and Neutral Current (NC) interactions are identified, using the measurements in the electronic detectors, and the NC/CC ratio is computed. The momentum distribution and the charge of the muon tracks produced in CC interactions are analysed. Calorimetric measurements of the visible energy are performed for both the CC and NC samples. For CC events the Bjorken-$y$ distribution and the hadronic shower profile are computed. The results are compared to a detailed Monte Carlo simulation of the electronic detectors' response.
001328179 520__ $$9arXiv$$aThe OPERA experiment is based on a hybrid technology combining electronic detectors and nuclear emulsions. OPERA collected muon-neutrino interactions during the 2008 and 2009 physics runs of the CNGS neutrino beam, produced at CERN with an energy range of about 5-35 GeV. A total of $5.3 \times 10^{19}$ protons on target equivalent luminosity has been analysed with the OPERA electronic detectors: scintillator strips target trackers and magnetic muon spectrometers equipped with resistive plate gas chambers and drift tubes, allowing a detailed reconstruction of muon-neutrino interactions. Charged Current (CC) and Neutral Current (NC) interactions are identified, using the measurements in the electronic detectors, and the NC/CC ratio is computed. The momentum distribution and the charge of the muon tracks produced in CC interactions are analysed. Calorimetric measurements of the visible energy are performed for both the CC and NC samples. For CC events the Bjorken-$y$ distribution and the hadronic shower profile are computed. The results are compared to a detailed Monte Carlo simulation of the electronic detectors' response.
001328179 540__ $$aarXiv nonexclusive-distrib. 1.0$$barXiv$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
001328179 595__ $$aLANL EDS
001328179 65017 $$2arXiv$$aParticle Physics - Experiment
001328179 690C_ $$aARTICLE
001328179 690C_ $$aCERN
001328179 693__ $$aCERN SPS$$eOPERA CNGS1
001328179 695__ $$9LANL EDS$$ahep-ex
001328179 700__ $$aAleksandrov, A.$$uINFN, Naples
001328179 700__ $$aAltinok, O.$$iINSPIRE-00339868$$uMiddle East Tech. U., Ankara
001328179 700__ $$aAnokhina, A.$$uSINP, Moscow
001328179 700__ $$aAoki, S.$$uKobe U.
001328179 700__ $$aAriga, A.$$uBern U., LHEP
001328179 700__ $$aAriga, T.$$uBern U., LHEP
001328179 700__ $$aAutiero, D.$$uLyon, IPN
001328179 700__ $$aBadertscher, A.$$uZurich, ETH
001328179 700__ $$aBagulya, A.$$uLebedev Inst.
001328179 700__ $$aBendhabi, A.$$uSfax U.
001328179 700__ $$aBertolin, A.$$uINFN, Padua
001328179 700__ $$aBozza, C.$$uINFN, Salerno$$uSalerno U.
001328179 700__ $$aBrugiere, T.$$uLyon, IPN
001328179 700__ $$aBrugnera, R.$$uINFN, Padua$$uPadua U.
001328179 700__ $$aBrunet, F.$$uAnnecy, LAPP
001328179 700__ $$aBrunetti, G.$$uLyon, IPN$$uBologna U.$$uINFN, Bologna
001328179 700__ $$aBuontempo, S.$$uINFN, Naples
001328179 700__ $$aCazes, A.$$uLyon, IPN
001328179 700__ $$aChaussard, L.$$uLyon, IPN
001328179 700__ $$aChernyavsky, M.$$uLebedev Inst.
001328179 700__ $$aChiarella, V.$$uFrascati
001328179 700__ $$aChukanov, A.$$uDubna, JINR
001328179 700__ $$aD'Ambrosio, N.$$uGran Sasso
001328179 700__ $$aDal Corso, F.$$iINSPIRE-00039708$$uINFN, Padua
001328179 700__ $$aDe Lellis, G.$$uINFN, Naples$$uNaples U.
001328179 700__ $$adel Amo Sanchez, P.$$uAnnecy, LAPP
001328179 700__ $$aDeclais, Y.$$uLyon, IPN
001328179 700__ $$aDe Serio, M.$$uINFN, Bari
001328179 700__ $$aDi Capua, F.$$uINFN, Naples
001328179 700__ $$aDi Crescenzo, A.$$uINFN, Naples$$uNaples U.
001328179 700__ $$aDi Ferdinando, D.$$uINFN, Bologna
001328179 700__ $$aDi Marco, N.$$uL'Aquila U.$$uINFN, Aquila
001328179 700__ $$aDmitrievski, S.$$uDubna, JINR
001328179 700__ $$aDracos, M.$$iINSPIRE-00078038$$uStrasbourg, IPHC
001328179 700__ $$aDuchesneau, D.$$uAnnecy, LAPP
001328179 700__ $$aDusini, S.$$uINFN, Padua
001328179 700__ $$aDzhatdoev, T.$$uSINP, Moscow
001328179 700__ $$aEbert, J.$$uHamburg U.
001328179 700__ $$aEgorov, O.$$uMoscow, ITEP
001328179 700__ $$aEnikeev, R.$$uMoscow, INR
001328179 700__ $$aEreditato, A.$$iINSPIRE-00079760$$uBern U., LHEP
001328179 700__ $$aEsposito, L.S.$$uZurich, ETH
001328179 700__ $$aFavier, J.$$uAnnecy, LAPP
001328179 700__ $$aFerber, T.$$uHamburg U.
001328179 700__ $$aFini, R.A.$$uINFN, Bari
001328179 700__ $$aFrekers, D.$$uMunster U., ITP
001328179 700__ $$aFukuda, T.$$uNagoya U.
001328179 700__ $$aGarfagnini, A.$$uINFN, Padua$$uPadua U.
001328179 700__ $$aGiacomelli, G.$$uBologna U.$$uINFN, Bologna
001328179 700__ $$aGiorgini, M.$$uBologna U.$$uINFN, Bologna
001328179 700__ $$aGollnitz, C.$$qGoellnitz, C.$$uHamburg U.
001328179 700__ $$aGoldberg, J.$$iINSPIRE-00085410$$uTechnion
001328179 700__ $$aGolubkov, D.$$uMoscow, ITEP
001328179 700__ $$aGoncharova, L.$$uLebedev Inst.
001328179 700__ $$aGornushkin, Y.$$uDubna, JINR
001328179 700__ $$aGrella, G.$$uINFN, Salerno$$uSalerno U.
001328179 700__ $$aGrianti, F.$$uFrascati$$uUrbino U.
001328179 700__ $$aGuler, A.M.$$iINSPIRE-00305029$$qGueler, A.M.$$uMiddle East Tech. U., Ankara
001328179 700__ $$aGustavino, C.$$uGran Sasso
001328179 700__ $$aHagner, C.$$uHamburg U.
001328179 700__ $$aHamada, K.$$uNagoya U.
001328179 700__ $$aHara, T.$$uKobe U.
001328179 700__ $$aHierholzer, M.$$uHamburg U.
001328179 700__ $$aHollnagel, A.$$uHamburg U.
001328179 700__ $$aHoshino, K.$$uNagoya U.
001328179 700__ $$aIeva, M.$$uINFN, Bari
001328179 700__ $$aIshida, H.$$iINSPIRE-00374783$$uToho U.
001328179 700__ $$aJakovcic, K.$$uBoskovic Inst., Zagreb
001328179 700__ $$aJollet, C.$$uStrasbourg, IPHC
001328179 700__ $$aJuget, F.$$uBern U., LHEP
001328179 700__ $$aKamiscioglu, M.$$uMiddle East Tech. U., Ankara
001328179 700__ $$aKazuyama, K.$$uNagoya U.
001328179 700__ $$aKim, S.H.$$uGyeongsang Natl. U.
001328179 700__ $$aKimura, M.$$uToho U.
001328179 700__ $$aKitagawa, N.$$uNagoya U.
001328179 700__ $$aKlicek, B.$$uBoskovic Inst., Zagreb
001328179 700__ $$aKnuesel, J.$$uBern U., LHEP
001328179 700__ $$aKodama, K.$$uAichi U. of Education
001328179 700__ $$aKomatsu, M.$$uNagoya U.
001328179 700__ $$aKose, U.$$uINFN, Padua$$uPadua U.
001328179 700__ $$aKreslo, I.$$uBern U., LHEP
001328179 700__ $$aKubota, H.$$uNagoya U.
001328179 700__ $$aLazzaro, C.$$uZurich, ETH
001328179 700__ $$aLenkeit, J.$$uHamburg U.
001328179 700__ $$aLippi, I.$$uINFN, Padua
001328179 700__ $$aLjubicic, A.$$uBoskovic Inst., Zagreb
001328179 700__ $$aLonghin, A.$$uINFN, Padua$$uPadua U.
001328179 700__ $$aLoverre, P.$$uRome U.$$uINFN, Rome
001328179 700__ $$aLutter, G.$$uBern U., LHEP
001328179 700__ $$aMalgin, A.$$iINSPIRE-00356809$$uMoscow, INR
001328179 700__ $$aMandrioli, G.$$uINFN, Bologna
001328179 700__ $$aMannai, K.$$uSfax U.
001328179 700__ $$aMarteau, J.$$uLyon, IPN
001328179 700__ $$aMatsuo, T.$$uToho U.
001328179 700__ $$aMatveev, V.$$uMoscow, INR
001328179 700__ $$aMauri, N.$$uBologna U.$$uINFN, Bologna
001328179 700__ $$aMedinaceli, E.$$uINFN, Bologna
001328179 700__ $$aMeisel, F.$$uBern U., LHEP
001328179 700__ $$aMeregaglia, A.$$uStrasbourg, IPHC
001328179 700__ $$aMigliozzi, P.$$uINFN, Naples
001328179 700__ $$aMikado, S.$$uToho U.
001328179 700__ $$aMiyamoto, S.$$uNagoya U.
001328179 700__ $$aMonacelli, P.$$uL'Aquila U.$$uINFN, Aquila
001328179 700__ $$aMorishima, K.$$uNagoya U.
001328179 700__ $$aMoser, U.$$uBern U., LHEP
001328179 700__ $$aMuciaccia, M.T.$$uINFN, Bari$$uBari U.
001328179 700__ $$aNaganawa, N.$$uNagoya U.
001328179 700__ $$aNaka, T.$$uNagoya U.
001328179 700__ $$aNakamura, M.$$uNagoya U.
001328179 700__ $$aNakano, T.$$uNagoya U.
001328179 700__ $$aNaumov, D.$$uDubna, JINR
001328179 700__ $$aNikitina, V.$$uSINP, Moscow
001328179 700__ $$aNiwa, K.$$uNagoya U.
001328179 700__ $$aNonoyama, Y.$$uNagoya U.
001328179 700__ $$aOgawa, S.$$uToho U.
001328179 700__ $$aOkateva, N.$$uLebedev Inst.
001328179 700__ $$aOlchevski, A.$$uDubna, JINR
001328179 700__ $$aPaniccia, M.$$uFrascati
001328179 700__ $$aPaoloni, A.$$uFrascati
001328179 700__ $$aPark, B.D.$$uGyeongsang Natl. U.
001328179 700__ $$aPark, I.G.$$uGyeongsang Natl. U.
001328179 700__ $$aPastore, A.$$uINFN, Bari$$uBari U.
001328179 700__ $$aPatrizii, L.$$uINFN, Bologna
001328179 700__ $$aPennacchio, E.$$uLyon, IPN
001328179 700__ $$aPessard, H.$$uAnnecy, LAPP
001328179 700__ $$aPretzl, K.$$iINSPIRE-00117685$$uBern U., LHEP
001328179 700__ $$aPilipenko, V.$$uMunster U., ITP
001328179 700__ $$aPistillo, C.$$uBern U., LHEP
001328179 700__ $$aPolukhina, N.$$uLebedev Inst.
001328179 700__ $$aPozzato, M.$$uBologna U.$$uINFN, Bologna
001328179 700__ $$aPupilli, F.$$uL'Aquila U.$$uINFN, Aquila
001328179 700__ $$aRescigno, R.$$uINFN, Salerno$$uSalerno U.
001328179 700__ $$aRoganova, T.$$uSINP, Moscow
001328179 700__ $$aRokujo, H.$$uKobe U.
001328179 700__ $$aRomano, G.$$uINFN, Salerno$$uSalerno U.
001328179 700__ $$aRosa, G.$$uRome U.$$uINFN, Rome
001328179 700__ $$aRostovtseva, I.$$uMoscow, ITEP
001328179 700__ $$aRubbia, A.$$uZurich, ETH
001328179 700__ $$aRusso, A.$$uINFN, Naples
001328179 700__ $$aRyasny, V.$$uMoscow, INR
001328179 700__ $$aRyazhskaya, O.$$uMoscow, INR
001328179 700__ $$aSato, O.$$iINSPIRE-00123410$$uNagoya U.
001328179 700__ $$aSato, Y.$$uUtsunomiya U.
001328179 700__ $$aSchembri, A.$$uGran Sasso
001328179 700__ $$aSchmidt-Parzefall, W.$$uHamburg U.
001328179 700__ $$aSchroeder, H.$$uRostock U.
001328179 700__ $$aScotto Lavina, L.$$iINSPIRE-00034804$$uINFN, Naples$$uNaples U.
001328179 700__ $$aSheshukov, A.$$uDubna, JINR
001328179 700__ $$aShibuya, H.$$uToho U.
001328179 700__ $$aShoziyoev, G.$$uSINP, Moscow
001328179 700__ $$aSimone, S.$$uINFN, Bari$$uBari U.
001328179 700__ $$aSioli, M.$$uBologna U.$$uINFN, Bologna
001328179 700__ $$aSirignano, C.$$uINFN, Salerno$$uSalerno U.
001328179 700__ $$aSirri, G.$$uINFN, Bologna
001328179 700__ $$aSong, J.S.$$uGyeongsang Natl. U.
001328179 700__ $$aSpinetti, M.$$uFrascati
001328179 700__ $$aStanco, L.$$iINSPIRE-00128354$$uINFN, Padua
001328179 700__ $$aStarkov, N.$$uLebedev Inst.
001328179 700__ $$aStipcevic, M.$$uBoskovic Inst., Zagreb
001328179 700__ $$aStrauss, T.$$uZurich, ETH
001328179 700__ $$aStrolin, P.$$uINFN, Naples$$uNaples U.
001328179 700__ $$aTakahashi, S.$$uNagoya U.
001328179 700__ $$aTenti, M.$$uBologna U.$$uINFN, Bologna
001328179 700__ $$aTerranova, F.$$uFrascati
001328179 700__ $$aTezuka, I.$$uUtsunomiya U.
001328179 700__ $$aTioukov, V.$$uINFN, Naples
001328179 700__ $$aTolun, P.$$uMiddle East Tech. U., Ankara
001328179 700__ $$aTrabelsi, A.$$uSfax U.
001328179 700__ $$aTran, T.$$uLyon, IPN
001328179 700__ $$aTufanli, S.$$uMiddle East Tech. U., Ankara
001328179 700__ $$aVilain, P.$$uBrussels U., IIHE
001328179 700__ $$aVladimirov, M.$$uLebedev Inst.
001328179 700__ $$aVotano, L.$$uFrascati
001328179 700__ $$aVuilleumier, J.L.$$uBern U., LHEP
001328179 700__ $$aWilquet, G.$$uTechnion
001328179 700__ $$aWonsak, B.$$uHamburg U.
001328179 700__ $$aYakushev, V.$$uMoscow, INR
001328179 700__ $$aYoon, C.S.$$uGyeongsang Natl. U.
001328179 700__ $$aYoshioka, T.$$uNagoya U.
001328179 700__ $$aYoshida, J.$$uNagoya U.
001328179 700__ $$aZaitsev, Y.$$uMoscow, ITEP
001328179 700__ $$aZemskova, S.$$uDubna, JINR
001328179 700__ $$aZghiche, A.$$uAnnecy, LAPP
001328179 700__ $$aZimmermann, R.$$uHamburg U.
001328179 710__ $$gOPERA Collaboration
001328179 773__ $$c053051$$pNew J. Phys.$$v13$$y2011
001328179 8564_ $$uhttp://arxiv.org/pdf/1102.1882.pdf$$yPreprint
001328179 8564_ $$81338448$$s16318$$uhttp://cds.cern.ch/record/1328179/files/DensTrack.png$$y00006 Length $\times$ density comparison for data (dots with error bars) and MC (solid line) for events classified as CC (i.e. length $\times$ density $> 660$ g~$\times$~cm$^{-2}$). The MC distribution has been normalised to data.
001328179 8564_ $$81338449$$s28067$$uhttp://cds.cern.ch/record/1328179/files/YBjorken_contribution_all.png$$y00013 Bjorken-$y$ variable reconstructed in data (dots with error bars) and MC (shaded areas). The MC distributions are normalised to data. The different contributions of the MC are shown in different colours: QE + RES contribution in light grey, DIS contribution in grey and the NC contamination in dark grey. On the left, all the events with at least one muon are shown whereas on the right the events for which the momentum is measured in the spectrometer are shown.
001328179 8564_ $$81338450$$s15026$$uhttp://cds.cern.ch/record/1328179/files/Ett.png$$y00010 Energy deposit in the TT for events with at least one reconstructed muon (left) and events with no muon (right). Dots with error bars correspond to data and solid lines to MC. MC distributions are normalised to data.
001328179 8564_ $$81338451$$s28612$$uhttp://cds.cern.ch/record/1328179/files/YBjorken_contribution_bending.png$$y00014 Bjorken-$y$ variable reconstructed in data (dots with error bars) and MC (shaded areas). The MC distributions are normalised to data. The different contributions of the MC are shown in different colours: QE + RES contribution in light grey, DIS contribution in grey and the NC contamination in dark grey. On the left, all the events with at least one muon are shown whereas on the right the events for which the momentum is measured in the spectrometer are shown.
001328179 8564_ $$81338452$$s12969$$uhttp://cds.cern.ch/record/1328179/files/figpmu-v1.png$$y00007 Muon momentum comparison (momentum $\times$ charge). Data are shown by dots, errors are statistical only. The MC prediction, normalised to the number of p.o.t. corresponding to the 2008-2009 data sample, is shown by the coloured area. The dominant source of the spread of the MC prediction is due to the 10 \% uncertainty on the expected number of $\nu_{\mu}$ CC events. For illustration purposes only, the lower dashed curve represents the contribution obtained from the $\nu_{\mu}$ to $\nu_{\tau}$ MC events with subsequent decay into $\mu$ of the final state $\tau$ lepton. The normalisation of this contribution is arbitrary.
001328179 8564_ $$81338453$$s9908$$uhttp://cds.cern.ch/record/1328179/files/CC.png$$y00001 Examples of charged current (top) and neutral current (bottom) events as seen in one projection view of the OPERA electronic detectors. In this view, the 2 SM can be recognised: for each one, the target is followed by the muon spectrometer.
001328179 8564_ $$81338454$$s8701$$uhttp://cds.cern.ch/record/1328179/files/NC.png$$y00002 Examples of charged current (top) and neutral current (bottom) events as seen in one projection view of the OPERA electronic detectors. In this view, the 2 SM can be recognised: for each one, the target is followed by the muon spectrometer.
001328179 8564_ $$81338455$$s13149$$uhttp://cds.cern.ch/record/1328179/files/ShowerTrans.png$$y00015 Transverse hadronic shower profile (left), in the X and Y projections, and longitudinal profile (right), in number of TT walls. Data are shown by dots with error bars and MC by the solid line. MC distributions are normalised to data.
001328179 8564_ $$81338456$$s14617$$uhttp://cds.cern.ch/record/1328179/files/Etot_CC.png$$y00012 Total reconstructed energy for events with at least one identified muon for data (dots with error bars) and MC (solid line). The MC distribution is normalised to data.
001328179 8564_ $$81338457$$s10556$$uhttp://cds.cern.ch/record/1328179/files/figqpmu-v1.png$$y00008 Muon charge comparison (momentum $\times$ charge): data (black dots with error bars) and MC (solid line) are normalised to one.
001328179 8564_ $$81338458$$s15924$$uhttp://cds.cern.ch/record/1328179/files/Walls.png$$y00005 Number of hit walls for data (dots with error bars) and MC (solid line) contained events. The first bump is mainly due to NC events (dashed line) whereas the second and the third ones originate from CC events crossing one and two SM, respectively. The MC distribution has been normalised to data.
001328179 8564_ $$81338459$$s14429$$uhttp://cds.cern.ch/record/1328179/files/Ett_NC_AllExt.png$$y00011 Energy deposit in the TT for events with at least one reconstructed muon (left) and events with no muon (right). Dots with error bars correspond to data and solid lines to MC. MC distributions are normalised to data.
001328179 8564_ $$81338460$$s509294$$uhttp://cds.cern.ch/record/1328179/files/arXiv:1102.1882.pdf
001328179 8564_ $$81338461$$s12865$$uhttp://cds.cern.ch/record/1328179/files/fraction.png$$y00004 Integral fraction of selected events as a function of the cut on $N_{ED}$ for MC CC events (solid line) and MC NC events (dashed line). For this figure the contained event requirement is not applied.
001328179 8564_ $$81338462$$s15946$$uhttp://cds.cern.ch/record/1328179/files/ElongShow.png$$y00016 Transverse hadronic shower profile (left), in the X and Y projections, and longitudinal profile (right), in number of TT walls. Data are shown by dots with error bars and MC by the solid line. MC distributions are normalised to data.
001328179 8564_ $$81338463$$s12140$$uhttp://cds.cern.ch/record/1328179/files/Resol.png$$y00017 MC energy resolution computed using the CNGS neutrino energy spectrum.
001328179 8564_ $$81338464$$s1265593$$uhttp://cds.cern.ch/record/1328179/files/detector.png$$y00000 View of the OPERA detector; the neutrino beam enters from the left. The upper horizontal lines indicate the two identical super-modules (SM1 and SM2). The target area is made of walls filled with lead/emulsion bricks interleaved with 31 planes of plastic scintillators (TT) per SM. The VETO detector and a magnet with its inserted RPC planes are indicated by arrows, as well as some PT and XPC planes. The Brick Manipulator System (BMS) is also visible. See \protect{\cite{Detector}} for more details.
001328179 8564_ $$81338465$$s27071$$uhttp://cds.cern.ch/record/1328179/files/simu_data09.png$$y00009 Number of detected p.e. on each extremity of the TT strips as a function of the hit position with respect to the left and right PMTs. The full circles are data, the empty ones are MC expectations.
001328179 8564_ $$81338466$$s2298786$$uhttp://cds.cern.ch/record/1328179/files/njp11_5_053051.pdf$$yFulltext
001328179 8564_ $$82321469$$s9563$$uhttp://cds.cern.ch/record/1328179/files/fig00003.png$$y00003 noimg: Efficiencies for the selection of contained events.: MC efficiencies for CC and NC selection using the cut on $N_{ED}$. If $N_{ED} > 14$ the event is classified as CC, otherwise it is classified as NC.
001328179 916__ $$sn$$w201106
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001328179 980__ $$aARTICLE