000889009 001__ 889009 000889009 005__ 20210425193442.0 000889009 0247_ $$2doi$$a10.1140/epjc/s10052-020-08534-2 000889009 0247_ $$2ISSN$$a1434-6044 000889009 0247_ $$2ISSN$$a1434-6052 000889009 0247_ $$2Handle$$a2128/26602 000889009 0247_ $$2altmetric$$aaltmetric:94962358 000889009 0247_ $$2WOS$$aWOS:000595779500001 000889009 037__ $$aFZJ-2020-05384 000889009 082__ $$a530 000889009 1001_ $$0P:(DE-HGF)0$$aAgostini, M.$$b0$$eCorresponding author 000889009 245__ $$aSensitivity to neutrinos from the solar CNO cycle in Borexino 000889009 260__ $$aHeidelberg$$bSpringer$$c2020 000889009 3367_ $$2DRIVER$$aarticle 000889009 3367_ $$2DataCite$$aOutput Types/Journal article 000889009 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1619337508_9734 000889009 3367_ $$2BibTeX$$aARTICLE 000889009 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000889009 3367_ $$00$$2EndNote$$aJournal Article 000889009 520__ $$aNeutrinos emitted in the carbon, nitrogen, oxygen (CNO) fusion cycle in the Sun are a sub-dominant, yet crucial component of solar neutrinos whose flux has not been measured yet. The Borexino experiment at the Laboratori Nazionali del Gran Sasso (Italy) has a unique opportunity to detect them directly thanks to the detector’s radiopurity and the precise understanding of the detector backgrounds. We discuss the sensitivity of Borexino to CNO neutrinos, which is based on the strategies we adopted to constrain the rates of the two most relevant background sources, $pep$ neutrinos from the solar pp-chain and $^{210}$Bi beta decays originating in the intrinsic contamination of the liquid scintillator with $^{210}$Pb. Assuming the CNO flux predicted by the high-metallicity Standard Solar Model and an exposure of 1000 days $\times $ 71.3 t, Borexino has a median sensitivity to CNO neutrino higher than 3 $\sigma $. With the same hypothesis the expected experimental uncertainty on the CNO neutrino flux is 23%, provided the uncertainty on the independent estimate of the $^{210}\text {Bi}$ interaction rate is 1.5 $\hbox {cpd}/100~\hbox {ton}$. Finally, we evaluated the expected uncertainty of the C and N abundances and the expected discrimination significance between the high and low metallicity Standard Solar Models (HZ and LZ) with future more precise measurement of the CNO solar neutrino flux. 000889009 536__ $$0G:(DE-HGF)POF3-612$$a612 - Cosmic Matter in the Laboratory (POF3-612)$$cPOF3-612$$fPOF III$$x0 000889009 536__ $$0G:(DE-Juel1)jikp20_20190501$$aSolar and Geo-neutrino Analysis with Borexino (jikp20_20190501)$$cjikp20_20190501$$fSolar and Geo-neutrino Analysis with Borexino$$x1 000889009 588__ $$aDataset connected to CrossRef 000889009 7001_ $$0P:(DE-HGF)0$$aAltenmüller, K.$$b1 000889009 7001_ $$0P:(DE-HGF)0$$aAppel, S.$$b2 000889009 7001_ $$0P:(DE-HGF)0$$aAtroshchenko, V.$$b3 000889009 7001_ $$0P:(DE-Juel1)156420$$aBagdasarian, Z.$$b4 000889009 7001_ $$0P:(DE-HGF)0$$aBasilico, D.$$b5 000889009 7001_ $$0P:(DE-HGF)0$$aBellini, G.$$b6 000889009 7001_ $$aBenziger, J.$$b7 000889009 7001_ $$aBiondi, R.$$b8 000889009 7001_ $$aBravo, D.$$b9 000889009 7001_ $$aCaccianiga, B.$$b10 000889009 7001_ $$aCalaprice, F.$$b11 000889009 7001_ $$aCaminata, A.$$b12 000889009 7001_ $$aCavalcante, P.$$b13 000889009 7001_ $$aChepurnov, A.$$b14 000889009 7001_ $$aD’Angelo, D.$$b15 000889009 7001_ $$aDavini, S.$$b16 000889009 7001_ $$aDerbin, A.$$b17 000889009 7001_ $$aDi Giacinto, A.$$b18 000889009 7001_ $$aDi Marcello, V.$$b19 000889009 7001_ $$aDing, X. 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