The Jiangmen Underground Neutrino Observatory (JUNO) features a 20 kt multi-purpose underground liquid scintillator sphere as its main detector. Some of JUNO's features make it an excellent location for $ ^8 $ B solar neutrino measurements, such as its low-energy threshold, high energy resolution compared with water Cherenkov detectors, and much larger target mass compared with previous liquid scintillator detectors. In this paper, we present a comprehensive assessment of JUNO's potential for detecting $ ^8 $ B solar neutrinos via the neutrino-electron elastic scattering process. A reduced 2 MeV threshold for the recoil electron energy is found to be achievable, assuming that the intrinsic radioactive background $ ^8 $ U and $ ^8 $ Th in the liquid scintillator can be controlled to 10 $ ^8 $ g/g. With ten years of data acquisition, approximately 60,000 signal and 30,000 background events are expected. This large sample will enable an examination of the distortion of the recoil electron spectrum that is dominated by the neutrino flavor transformation in the dense solar matter, which will shed new light on the inconsistency between the measured electron spectra and the predictions of the standard three-flavor neutrino oscillation framework. If $ ^8 $ eV $ ^8 $ , JUNO can provide evidence of neutrino oscillation in the Earth at approximately the 3 $ ^8 $ (2 $ ^8 $ ) level by measuring the non-zero signal rate variation with respect to the solar zenith angle. Moreover, JUNO can simultaneously measure $ ^8 $ using $ ^8 $ B solar neutrinos to a precision of 20% or better, depending on the central value, and to sub-percent precision using reactor antineutrinos. A comparison of these two measurements from the same detector will help understand the current mild inconsistency between the value of $ ^8 $ reported by solar neutrino experiments and the KamLAND experiment.
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
"country": "Italy",
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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],
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
"country": "China",
"value": "Xiamen University, Xiamen, China"
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],
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{
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{
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{
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{
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{
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{
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],
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"given_names": "Qiumei",
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{
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{
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{
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{
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"given_names": "Xiaoyan",
"full_name": "Ma,Xiaoyan"
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{
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{
"country": "China",
"value": "North China Electric Power University, Beijing, China"
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],
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{
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{
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{
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{
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{
"affiliations": [
{
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"value": "Department of Physics and Earth Science, University of Ferrara and INFN Sezione di Ferrara, Ferrara, Italy"
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"surname": "Mantovani",
"given_names": "Fabio",
"full_name": "Mantovani,Fabio"
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{
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{
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"value": "Dipartimento di Fisica e Astronomia dell’Universita’ di Padova and INFN Sezione di Padova, Padova, Italy"
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"given_names": "Francesco",
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{
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{
"country": "China",
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],
"surname": "Mao",
"given_names": "Xin",
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{
"affiliations": [
{
"country": "China",
"value": "School of Physics, Peking University, Beijing, China"
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],
"surname": "Mao",
"given_names": "Yajun",
"full_name": "Mao,Yajun"
},
{
"affiliations": [
{
"country": "Italy",
"value": "University of Roma Tre and INFN Sezione Roma Tre, Roma, Italy"
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],
"surname": "M. Mari",
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},
{
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{
"country": "Italy",
"value": "Dipartimento di Fisica e Astronomia dell’Universita’ di Padova and INFN Sezione di Padova, Padova, Italy"
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{
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{
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{
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{
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"value": "University of Roma Tre and INFN Sezione Roma Tre, Roma, Italy"
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{
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{
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{
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{
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{
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{
"affiliations": [
{
"country": "Germany",
"value": "Eberhard Karls Universität Tübingen, Physikalisches Institut, Tübingen, Germany"
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{
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{
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{
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{
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{
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{
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{
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{
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"value": "INFN Sezione di Milano and Dipartimento di Fisica dell Università di Milano, Milano, Italy"
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{
"affiliations": [
{
"country": "Germany",
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],
"surname": "Meyh\u00f6fer",
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{
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{
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{
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{
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],
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{
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{
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"value": "INFN Sezione di Milano and Dipartimento di Fisica dell Università di Milano, Milano, Italy"
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{
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{
"country": "Italy",
"value": "INFN Catania and Dipartimento di Fisica e Astronomia dell Università di Catania, Catania, Italy"
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"full_name": "Monforte,Salvatore"
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{
"affiliations": [
{
"country": "Italy",
"value": "University of Roma Tre and INFN Sezione Roma Tre, Roma, Italy"
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],
"surname": "Montini",
"given_names": "Paolo",
"full_name": "Montini,Paolo"
},
{
"affiliations": [
{
"country": "Italy",
"value": "Department of Physics and Earth Science, University of Ferrara and INFN Sezione di Ferrara, Ferrara, Italy"
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{
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{
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{
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},
{
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{
"country": "Italy",
"value": "INFN Milano Bicocca and University of Milano Bicocca, Milano, Italy"
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],
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{
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{
"country": "Russia",
"value": "Joint Institute for Nuclear Research, Dubna, Russia"
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"given_names": "Dmitry V.",
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{
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{
"country": "Russia",
"value": "Joint Institute for Nuclear Research, Dubna, Russia"
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{
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{
"country": "Russia",
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{
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{
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"value": "Lomonosov Moscow State University, Moscow, Russia"
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],
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{
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{
"country": "China",
"value": "Institute of High Energy Physics, Beijing, China"
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],
"surname": "Ning",
"given_names": "Feipeng",
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{
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{
"country": "China",
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"full_name": "Ning,Zhe"
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{
"affiliations": [
{
"country": "Brazil",
"value": "Pontificia Universidade Catolica do Rio de Janeiro, Rio, Brazil"
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],
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"full_name": "Nunokawa,Hiroshi"
},
{
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{
"country": "Germany",
"value": "Technische Universität München, München, Germany"
}
],
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"given_names": "Lothar",
"full_name": "Oberauer,Lothar"
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{
"affiliations": [
{
"country": "USA",
"value": "Department of Physics and Astronomy, University of California, Irvine, California, USA"
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{
"country": "Chile",
"value": "Pontificia Universidad Católica de Chile, Santiago, Chile"
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],
"surname": "Ochoa-Ricoux",
"given_names": "Juan Pedro",
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{
"affiliations": [
{
"country": "Russia",
"value": "Joint Institute for Nuclear Research, Dubna, Russia"
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"given_names": "Alexander",
"full_name": "Olshevskiy,Alexander"
},
{
"affiliations": [
{
"country": "Italy",
"value": "University of Roma Tre and INFN Sezione Roma Tre, Roma, Italy"
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],
"surname": "Orestano",
"given_names": "Domizia",
"full_name": "Orestano,Domizia"
},
{
"affiliations": [
{
"country": "Italy",
"value": "INFN Sezione di Perugia and Dipartimento di Chimica, Biologia e Biotecnologie dell’Università di Perugia, Perugia, Italy"
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"surname": "Ortica",
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{
"affiliations": [
{
"country": "Taiwan",
"value": "Department of Physics, National Taiwan University, Taipei"
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],
"surname": "Pan",
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"full_name": "Pan,Hsiao-Ru"
},
{
"affiliations": [
{
"country": "Italy",
"value": "Laboratori Nazionali di Frascati dell’INFN, Roma, Italy"
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{
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{
"affiliations": [
{
"country": "Italy",
"value": "INFN Sezione di Milano and Dipartimento di Fisica dell Università di Milano, Milano, Italy"
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"given_names": "Sergio",
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{
"affiliations": [
{
"country": "Thailand",
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],
"surname": "Payupol",
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{
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{
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{
"country": "Italy",
"value": "INFN Sezione di Perugia and Dipartimento di Chimica, Biologia e Biotecnologie dell’Università di Perugia, Perugia, Italy"
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{
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{
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],
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{
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{
"country": "China",
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],
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{
"affiliations": [
{
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{
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{
"country": "Belgium",
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],
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{
"affiliations": [
{
"country": "Italy",
"value": "University of Roma Tre and INFN Sezione Roma Tre, Roma, Italy"
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],
"surname": "Petrucci",
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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{
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"titles": [
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"source": "IOP",
"title": "Feasibility and physics potential of detecting B solar neutrinos at JUNO "
}
],
"dois": [
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"value": "10.1088/1674-1137/abd92a"
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"publication_info": [
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"journal_title": "Chinese Physics C",
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"journal_volume": "45",
"artid": "023004",
"year": 2021,
"journal_issue": "2"
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"submission_number": "63c6cb64c6f011ec8a3e56f45b8e1a22"
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18
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"url": "http://creativecommons.org/licenses/by/3.0/",
"license": "CC-BY-3.0"
}
],
"copyright": [
{
"statement": "\u00a9 2021Chinese Physical Society and the Institute of High Energy Physics of the Chinese Academy of Sciences and the Institute of Modern Physics of the Chinese Academy of Sciences and IOP Publishing Ltd",
"year": "2021"
}
],
"control_number": "59543",
"collaborations": [
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"value": "JUNO Collaboration"
}
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"abstracts": [
{
"source": "IOP",
"value": "The Jiangmen Underground Neutrino Observatory (JUNO) features a 20 kt multi-purpose underground liquid scintillator sphere as its main detector. Some of JUNO's features make it an excellent location for $ ^8 $ B solar neutrino measurements, such as its low-energy threshold, high energy resolution compared with water Cherenkov detectors, and much larger target mass compared with previous liquid scintillator detectors. In this paper, we present a comprehensive assessment of JUNO's potential for detecting $ ^8 $ B solar neutrinos via the neutrino-electron elastic scattering process. A reduced 2 MeV threshold for the recoil electron energy is found to be achievable, assuming that the intrinsic radioactive background $ ^8 $ U and $ ^8 $ Th in the liquid scintillator can be controlled to 10 $ ^8 $ g/g. With ten years of data acquisition, approximately 60,000 signal and 30,000 background events are expected. This large sample will enable an examination of the distortion of the recoil electron spectrum that is dominated by the neutrino flavor transformation in the dense solar matter, which will shed new light on the inconsistency between the measured electron spectra and the predictions of the standard three-flavor neutrino oscillation framework. If $ ^8 $ eV $ ^8 $ , JUNO can provide evidence of neutrino oscillation in the Earth at approximately the 3 $ ^8 $ (2 $ ^8 $ ) level by measuring the non-zero signal rate variation with respect to the solar zenith angle. Moreover, JUNO can simultaneously measure $ ^8 $ using $ ^8 $ B solar neutrinos to a precision of 20% or better, depending on the central value, and to sub-percent precision using reactor antineutrinos. A comparison of these two measurements from the same detector will help understand the current mild inconsistency between the value of $ ^8 $ reported by solar neutrino experiments and the KamLAND experiment."
}
],
"imprints": [
{
"date": "2021-02-01",
"publisher": "IOP"
}
]
}