dc.creatorThe Double Chooz collaboration
dc.creatorAbe Y.
dc.creatorAppel S.
dc.creatorAbrahão T.
dc.creatorAlmazan H.
dc.creatorAlt C.
dc.creatordos Anjos J.C.
dc.creatorBarriere J.C.
dc.creatorBaussan E.
dc.creatorBekman I.
dc.creatorBergevin M.
dc.creatorBezerra T.J.C.
dc.creatorBezrukov L.
dc.creatorBlucher E.
dc.creatorBrugière T.
dc.creatorBuck C.
dc.creatorBusenitz J.
dc.creatorCabrera A.
dc.creatorCamilleri L.
dc.creatorCarr R.
dc.creatorCerrada M.
dc.creatorChauveau E.
dc.creatorChimenti P.
dc.creatorCollin A.P.
dc.creatorConrad J.M.
dc.creatorCrespo-Anadón J.I.
dc.creatorCrum K.
dc.creatorCucoanes A.S.
dc.creatorDamon E.
dc.creatorDawson J.V.
dc.creatorDhooghe J.
dc.creatorDietrich D.
dc.creatorDjurcic Z.
dc.creatorDracos M.
dc.creatorEtenko A.
dc.creatorFallot M.
dc.creatorvon Feilitzsch F.
dc.creatorFelde J.
dc.creatorFernandes S.M.
dc.creatorFischer V.
dc.creatorFranco D.
dc.creatorFranke M.
dc.creatorFuruta H.
dc.creatorGil-Botella I.
dc.creatorGiot L.
dc.creatorGöger-Neff M.
dc.creatorGomez H.
dc.creatorGonzalez L.F.G.
dc.creatorGoodenough L.
dc.creatorGoodman M.C.
dc.creatorHaag N.
dc.creatorHara T.
dc.creatorHaser J.
dc.creatorHellwig D.
dc.creatorHofmann M.
dc.creatorHorton-Smith G.A.
dc.creatorHourlier A.
dc.creatorIshitsuka M.
dc.creatorJochum J.
dc.creatorJollet C.
dc.creatorKaether F.
dc.creatorKalousis L.N.
dc.creatorKamyshkov Y.
dc.creatorKaneda M.
dc.creatorKaplan D.M.
dc.creatorKawasaki T.
dc.creatorKemp E.
dc.creatorde Kerret H.
dc.creatorKryn D.
dc.creatorKuze M.
dc.creatorLachenmaier T.
dc.creatorLane C.E.
dc.creatorLasserre T.
dc.creatorLetourneau A.
dc.creatorLhuillier D.
dc.creatorLima H.P.
dc.creatorLindner M.
dc.creatorLópez-Castaño J.M.
dc.creatorLoSecco J.M.
dc.creatorLubsandorzhiev B.
dc.creatorLucht S.
dc.creatorMaeda J.
dc.creatorMariani C.
dc.creatorMaricic J.
dc.creatorMartino J.
dc.creatorMatsubara T.
dc.creatorMention G.
dc.creatorMeregaglia A.
dc.creatorMiletic T.
dc.creatorMilincic R.
dc.creatorMinotti A.
dc.creatorNagasaka Y.
dc.creatorNavas-Nicolás D.
dc.creatorNovella P.
dc.creatorOberauer L.
dc.creatorObolensky M.
dc.creatorOnillon A.
dc.creatorOsborn A.
dc.creatorPalomares C.
dc.creatorPepe I.M.
dc.creatorPerasso S.
dc.creatorPorta A.
dc.creatorPronost G.
dc.creatorReichenbacher J.
dc.creatorReinhold B.
dc.creatorRöhling M.
dc.creatorRoncin R.
dc.creatorRybolt B.
dc.creatorSakamoto Y.
dc.creatorSantorelli R.
dc.creatorSchilithz A.C.
dc.creatorSchönert S.
dc.creatorSchoppmann S.
dc.creatorShaevitz M.H.
dc.creatorSharankova R.
dc.creatorShrestha D.
dc.creatorSibille V.
dc.creatorSinev V.
dc.creatorSkorokhvatov M.
dc.creatorSmith E.
dc.creatorSoiron M.
dc.creatorSpitz J.
dc.creatorStahl A.
dc.creatorStancu I.
dc.creatorStokes L.F.F.
dc.creatorStrait M.
dc.creatorSuekane F.
dc.creatorSukhotin S.
dc.creatorSumiyoshi T.
dc.creatorSun Y.
dc.creatorSvoboda R.
dc.creatorTerao K.
dc.creatorTonazzo A.
dc.creatorThi H.H.T.
dc.creatorValdiviesso G.
dc.creatorVassilopoulos N.
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dc.creatorYang G.
dc.creatorYermia F.
dc.creatorZimmer V.
dc.date2016
dc.date2017-08-17T19:12:58Z
dc.date2017-08-17T19:12:58Z
dc.date.accessioned2018-03-29T05:19:19Z
dc.date.available2018-03-29T05:19:19Z
dc.identifierJournal Of High Energy Physics. Springer Verlag, v. 2016, n. 1, p. 1 - 29, 2016.
dc.identifier1126-6708
dc.identifier10.1007/JHEP01(2016)163
dc.identifierhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-84957805139&doi=10.1007%2fJHEP01%282016%29163&partnerID=40&md5=0d0456a347fdf09980dac8fd2e889960
dc.identifierhttp://repositorio.unicamp.br/jspui/handle/REPOSIP/323237
dc.identifier2-s2.0-84957805139
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/1357400
dc.descriptionThe Double Chooz collaboration presents a measurement of the neutrino mixing angle θ13 using reactor νe¯ (Formula presented.) observed via the inverse beta decay reaction in which the neutron is captured on hydrogen. This measurement is based on 462.72 live days data, approximately twice as much data as in the previous such analysis, collected with a detector positioned at an average distance of 1050 m from two reactor cores. Several novel techniques have been developed to achieve significant reductions of the backgrounds and systematic uncertainties. Accidental coincidences, the dominant background in this analysis, are suppressed by more than an order of magnitude with respect to our previous publication by a multi-variate analysis. These improvements demonstrate the capability of precise measurement of reactor νe¯ (Formula presented.) without gadolinium loading. Spectral distortions from the νe¯ (Formula presented.) reactor flux predictions previously reported with the neutron capture on gadolinium events are confirmed in the independent data sample presented here. A value of sin2 2θ13 = 0.095− 0.039 + 0.038 (stat+syst) is obtained from a fit to the observed event rate as a function of the reactor power, a method insensitive to the energy spectrum shape. A simultaneous fit of the hydrogen capture events and of the gadolinium capture events yields a measurement of sin2 2θ13 = 0.088 ± 0.033(stat+syst). © 2016, The Author(s).
dc.description2016
dc.description1
dc.description1
dc.description29
dc.languageEnglish
dc.publisherSpringer Verlag
dc.relationJournal of High Energy Physics
dc.rightsaberto
dc.sourceScopus
dc.subjectElectroweak Interaction
dc.subjectFlavor Physics
dc.subjectNeutrino Detectors And Telescopes
dc.subjectOscillation
dc.titleMeasurement Of θ13 In Double Chooz Using Neutron Captures On Hydrogen With Novel Background Rejection Techniques
dc.typeArtículos de revistas


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