New measurement of antineutrino oscillation with the full detector configuration at Daya Bay
We report a new measurement of electron antineutrino disappearance using the fully constructed Daya Bay Reactor Neutrino Experiment. The final two of eight antineutrino detectors were installed in the summer of 2012. Including the 404 days of data collected from October 2012 to November 2013 resulte...
Ausführliche Beschreibung
Autor*in: |
An, F P [verfasserIn] |
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Englisch |
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2015 |
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Übergeordnetes Werk: |
Enthalten in: Physical review letters - Ridge, NY : American Physical Society, 1958, 115(2015), 11 |
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Übergeordnetes Werk: |
volume:115 ; year:2015 ; number:11 |
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DOI / URN: |
10.1103/PhysRevLett.115.111802 |
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OLC1969288574 |
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520 | |a We report a new measurement of electron antineutrino disappearance using the fully constructed Daya Bay Reactor Neutrino Experiment. The final two of eight antineutrino detectors were installed in the summer of 2012. Including the 404 days of data collected from October 2012 to November 2013 resulted in a total exposure of 6.9×10^{5} GW_{th} ton days, a 3.6 times increase over our previous results. Improvements in energy calibration limited variations between detectors to 0.2%. Removal of six ^{241}Am-^{13}C radioactive calibration sources reduced the background by a factor of 2 for the detectors in the experimental hall furthest from the reactors. Direct prediction of the antineutrino signal in the far detectors based on the measurements in the near detectors explicitly minimized the dependence of the measurement on models of reactor antineutrino emission. The uncertainties in our estimates of sin^{2}2θ_{13} and |Δm_{ee}^{2}| were halved as a result of these improvements. An analysis of the relative antineutrino rates and energy spectra between detectors gave sin^{2}2θ_{13}=0.084±0.005 and |Δm_{ee}^{2}|=(2.42±0.11)×10^{-3} eV^{2} in the three-neutrino framework. | ||
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700 | 1 | |a Chen, H S |4 oth | |
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10.1103/PhysRevLett.115.111802 doi PQ20160211 (DE-627)OLC1969288574 (DE-599)GBVOLC1969288574 (PRQ)a1211-a8b0203e85ec8681c800fd9414e05c5128635fe9ccbc0d10f838e6a73f6e989a0 (KEY)0009201020150000115001100000newmeasurementofantineutrinooscillationwiththefull DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk An, F P verfasserin aut New measurement of antineutrino oscillation with the full detector configuration at Daya Bay 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We report a new measurement of electron antineutrino disappearance using the fully constructed Daya Bay Reactor Neutrino Experiment. The final two of eight antineutrino detectors were installed in the summer of 2012. Including the 404 days of data collected from October 2012 to November 2013 resulted in a total exposure of 6.9×10^{5} GW_{th} ton days, a 3.6 times increase over our previous results. Improvements in energy calibration limited variations between detectors to 0.2%. Removal of six ^{241}Am-^{13}C radioactive calibration sources reduced the background by a factor of 2 for the detectors in the experimental hall furthest from the reactors. Direct prediction of the antineutrino signal in the far detectors based on the measurements in the near detectors explicitly minimized the dependence of the measurement on models of reactor antineutrino emission. The uncertainties in our estimates of sin^{2}2θ_{13} and |Δm_{ee}^{2}| were halved as a result of these improvements. An analysis of the relative antineutrino rates and energy spectra between detectors gave sin^{2}2θ_{13}=0.084±0.005 and |Δm_{ee}^{2}|=(2.42±0.11)×10^{-3} eV^{2} in the three-neutrino framework. Instrumentation and Detectors Nuclear Experiment Physics High Energy Physics Experiment Balantekin, A B oth Band, H R oth Bishai, M oth Blyth, S oth Butorov, I oth Cao, G F oth Cao, J oth Cen, W R oth Chan, Y L oth Chang, J F oth Chang, L C oth Chang, Y oth Chen, H S oth Chen, Q Y oth Chen, S M oth Chen, Y X oth Chen, Y oth Cheng, J H oth Cheng, J oth Cheng, Y P oth Cherwinka, J J oth Chu, M C oth Cummings, J P oth de Arcos, J oth Deng, Z Y oth Ding, X F oth Ding, Y Y oth Diwan, M V oth Draeger, E oth Dwyer, D A oth Edwards, W R oth Ely, S R oth Gill, R oth Gonchar, M oth Gong, G H oth Gong, H oth Grassi, M oth Gu, W Q oth Guan, M Y oth Guo, L oth Guo, X H oth Hackenburg, R W oth Han, R oth Hans, S oth He, M oth Heeger, K M oth Heng, Y K oth Higuera, A oth Hor, Y K oth Hsiung, Y B oth Hu, B Z oth Hu, L M oth Hu, L J oth Hu, T oth Hu, W oth Huang, E C oth Huang, H X oth Huang, X T oth Huber, P oth Hussain, G oth Jaffe, D E oth Jaffke, P oth Jen, K L oth Jetter, S oth Ji, X P oth Ji, X L oth Jiao, J B oth Johnson, R A oth Kang, L oth Kettell, S H oth Kramer, M oth Kwan, K K oth Kwok, M W oth Kwok, T oth Langford, T J oth Lau, K oth Lebanowski, L oth Lee, J oth Lei, R T oth Leitner, R oth Leung, K Y oth Leung, J K C oth Lewis, C A oth Li, D J oth Li, F oth Li, G S oth Li, Q J oth Li, S C oth Li, W D oth Li, X N oth Li, X Q oth Li, Y F oth Li, Z B oth Liang, H oth Lin, C J oth Lin, G L oth Lin, P Y oth Lin, S K oth Ling, J J oth ... oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 115(2015), 11 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:115 year:2015 number:11 http://dx.doi.org/10.1103/PhysRevLett.115.111802 Volltext http://www.ncbi.nlm.nih.gov/pubmed/26406819 http://arxiv.org/abs/1505.03456 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 115 2015 11 |
spelling |
10.1103/PhysRevLett.115.111802 doi PQ20160211 (DE-627)OLC1969288574 (DE-599)GBVOLC1969288574 (PRQ)a1211-a8b0203e85ec8681c800fd9414e05c5128635fe9ccbc0d10f838e6a73f6e989a0 (KEY)0009201020150000115001100000newmeasurementofantineutrinooscillationwiththefull DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk An, F P verfasserin aut New measurement of antineutrino oscillation with the full detector configuration at Daya Bay 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We report a new measurement of electron antineutrino disappearance using the fully constructed Daya Bay Reactor Neutrino Experiment. The final two of eight antineutrino detectors were installed in the summer of 2012. Including the 404 days of data collected from October 2012 to November 2013 resulted in a total exposure of 6.9×10^{5} GW_{th} ton days, a 3.6 times increase over our previous results. Improvements in energy calibration limited variations between detectors to 0.2%. Removal of six ^{241}Am-^{13}C radioactive calibration sources reduced the background by a factor of 2 for the detectors in the experimental hall furthest from the reactors. Direct prediction of the antineutrino signal in the far detectors based on the measurements in the near detectors explicitly minimized the dependence of the measurement on models of reactor antineutrino emission. The uncertainties in our estimates of sin^{2}2θ_{13} and |Δm_{ee}^{2}| were halved as a result of these improvements. An analysis of the relative antineutrino rates and energy spectra between detectors gave sin^{2}2θ_{13}=0.084±0.005 and |Δm_{ee}^{2}|=(2.42±0.11)×10^{-3} eV^{2} in the three-neutrino framework. Instrumentation and Detectors Nuclear Experiment Physics High Energy Physics Experiment Balantekin, A B oth Band, H R oth Bishai, M oth Blyth, S oth Butorov, I oth Cao, G F oth Cao, J oth Cen, W R oth Chan, Y L oth Chang, J F oth Chang, L C oth Chang, Y oth Chen, H S oth Chen, Q Y oth Chen, S M oth Chen, Y X oth Chen, Y oth Cheng, J H oth Cheng, J oth Cheng, Y P oth Cherwinka, J J oth Chu, M C oth Cummings, J P oth de Arcos, J oth Deng, Z Y oth Ding, X F oth Ding, Y Y oth Diwan, M V oth Draeger, E oth Dwyer, D A oth Edwards, W R oth Ely, S R oth Gill, R oth Gonchar, M oth Gong, G H oth Gong, H oth Grassi, M oth Gu, W Q oth Guan, M Y oth Guo, L oth Guo, X H oth Hackenburg, R W oth Han, R oth Hans, S oth He, M oth Heeger, K M oth Heng, Y K oth Higuera, A oth Hor, Y K oth Hsiung, Y B oth Hu, B Z oth Hu, L M oth Hu, L J oth Hu, T oth Hu, W oth Huang, E C oth Huang, H X oth Huang, X T oth Huber, P oth Hussain, G oth Jaffe, D E oth Jaffke, P oth Jen, K L oth Jetter, S oth Ji, X P oth Ji, X L oth Jiao, J B oth Johnson, R A oth Kang, L oth Kettell, S H oth Kramer, M oth Kwan, K K oth Kwok, M W oth Kwok, T oth Langford, T J oth Lau, K oth Lebanowski, L oth Lee, J oth Lei, R T oth Leitner, R oth Leung, K Y oth Leung, J K C oth Lewis, C A oth Li, D J oth Li, F oth Li, G S oth Li, Q J oth Li, S C oth Li, W D oth Li, X N oth Li, X Q oth Li, Y F oth Li, Z B oth Liang, H oth Lin, C J oth Lin, G L oth Lin, P Y oth Lin, S K oth Ling, J J oth ... oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 115(2015), 11 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:115 year:2015 number:11 http://dx.doi.org/10.1103/PhysRevLett.115.111802 Volltext http://www.ncbi.nlm.nih.gov/pubmed/26406819 http://arxiv.org/abs/1505.03456 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 115 2015 11 |
allfields_unstemmed |
10.1103/PhysRevLett.115.111802 doi PQ20160211 (DE-627)OLC1969288574 (DE-599)GBVOLC1969288574 (PRQ)a1211-a8b0203e85ec8681c800fd9414e05c5128635fe9ccbc0d10f838e6a73f6e989a0 (KEY)0009201020150000115001100000newmeasurementofantineutrinooscillationwiththefull DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk An, F P verfasserin aut New measurement of antineutrino oscillation with the full detector configuration at Daya Bay 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We report a new measurement of electron antineutrino disappearance using the fully constructed Daya Bay Reactor Neutrino Experiment. The final two of eight antineutrino detectors were installed in the summer of 2012. Including the 404 days of data collected from October 2012 to November 2013 resulted in a total exposure of 6.9×10^{5} GW_{th} ton days, a 3.6 times increase over our previous results. Improvements in energy calibration limited variations between detectors to 0.2%. Removal of six ^{241}Am-^{13}C radioactive calibration sources reduced the background by a factor of 2 for the detectors in the experimental hall furthest from the reactors. Direct prediction of the antineutrino signal in the far detectors based on the measurements in the near detectors explicitly minimized the dependence of the measurement on models of reactor antineutrino emission. The uncertainties in our estimates of sin^{2}2θ_{13} and |Δm_{ee}^{2}| were halved as a result of these improvements. An analysis of the relative antineutrino rates and energy spectra between detectors gave sin^{2}2θ_{13}=0.084±0.005 and |Δm_{ee}^{2}|=(2.42±0.11)×10^{-3} eV^{2} in the three-neutrino framework. Instrumentation and Detectors Nuclear Experiment Physics High Energy Physics Experiment Balantekin, A B oth Band, H R oth Bishai, M oth Blyth, S oth Butorov, I oth Cao, G F oth Cao, J oth Cen, W R oth Chan, Y L oth Chang, J F oth Chang, L C oth Chang, Y oth Chen, H S oth Chen, Q Y oth Chen, S M oth Chen, Y X oth Chen, Y oth Cheng, J H oth Cheng, J oth Cheng, Y P oth Cherwinka, J J oth Chu, M C oth Cummings, J P oth de Arcos, J oth Deng, Z Y oth Ding, X F oth Ding, Y Y oth Diwan, M V oth Draeger, E oth Dwyer, D A oth Edwards, W R oth Ely, S R oth Gill, R oth Gonchar, M oth Gong, G H oth Gong, H oth Grassi, M oth Gu, W Q oth Guan, M Y oth Guo, L oth Guo, X H oth Hackenburg, R W oth Han, R oth Hans, S oth He, M oth Heeger, K M oth Heng, Y K oth Higuera, A oth Hor, Y K oth Hsiung, Y B oth Hu, B Z oth Hu, L M oth Hu, L J oth Hu, T oth Hu, W oth Huang, E C oth Huang, H X oth Huang, X T oth Huber, P oth Hussain, G oth Jaffe, D E oth Jaffke, P oth Jen, K L oth Jetter, S oth Ji, X P oth Ji, X L oth Jiao, J B oth Johnson, R A oth Kang, L oth Kettell, S H oth Kramer, M oth Kwan, K K oth Kwok, M W oth Kwok, T oth Langford, T J oth Lau, K oth Lebanowski, L oth Lee, J oth Lei, R T oth Leitner, R oth Leung, K Y oth Leung, J K C oth Lewis, C A oth Li, D J oth Li, F oth Li, G S oth Li, Q J oth Li, S C oth Li, W D oth Li, X N oth Li, X Q oth Li, Y F oth Li, Z B oth Liang, H oth Lin, C J oth Lin, G L oth Lin, P Y oth Lin, S K oth Ling, J J oth ... oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 115(2015), 11 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:115 year:2015 number:11 http://dx.doi.org/10.1103/PhysRevLett.115.111802 Volltext http://www.ncbi.nlm.nih.gov/pubmed/26406819 http://arxiv.org/abs/1505.03456 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 115 2015 11 |
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10.1103/PhysRevLett.115.111802 doi PQ20160211 (DE-627)OLC1969288574 (DE-599)GBVOLC1969288574 (PRQ)a1211-a8b0203e85ec8681c800fd9414e05c5128635fe9ccbc0d10f838e6a73f6e989a0 (KEY)0009201020150000115001100000newmeasurementofantineutrinooscillationwiththefull DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk An, F P verfasserin aut New measurement of antineutrino oscillation with the full detector configuration at Daya Bay 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We report a new measurement of electron antineutrino disappearance using the fully constructed Daya Bay Reactor Neutrino Experiment. The final two of eight antineutrino detectors were installed in the summer of 2012. Including the 404 days of data collected from October 2012 to November 2013 resulted in a total exposure of 6.9×10^{5} GW_{th} ton days, a 3.6 times increase over our previous results. Improvements in energy calibration limited variations between detectors to 0.2%. Removal of six ^{241}Am-^{13}C radioactive calibration sources reduced the background by a factor of 2 for the detectors in the experimental hall furthest from the reactors. Direct prediction of the antineutrino signal in the far detectors based on the measurements in the near detectors explicitly minimized the dependence of the measurement on models of reactor antineutrino emission. The uncertainties in our estimates of sin^{2}2θ_{13} and |Δm_{ee}^{2}| were halved as a result of these improvements. An analysis of the relative antineutrino rates and energy spectra between detectors gave sin^{2}2θ_{13}=0.084±0.005 and |Δm_{ee}^{2}|=(2.42±0.11)×10^{-3} eV^{2} in the three-neutrino framework. Instrumentation and Detectors Nuclear Experiment Physics High Energy Physics Experiment Balantekin, A B oth Band, H R oth Bishai, M oth Blyth, S oth Butorov, I oth Cao, G F oth Cao, J oth Cen, W R oth Chan, Y L oth Chang, J F oth Chang, L C oth Chang, Y oth Chen, H S oth Chen, Q Y oth Chen, S M oth Chen, Y X oth Chen, Y oth Cheng, J H oth Cheng, J oth Cheng, Y P oth Cherwinka, J J oth Chu, M C oth Cummings, J P oth de Arcos, J oth Deng, Z Y oth Ding, X F oth Ding, Y Y oth Diwan, M V oth Draeger, E oth Dwyer, D A oth Edwards, W R oth Ely, S R oth Gill, R oth Gonchar, M oth Gong, G H oth Gong, H oth Grassi, M oth Gu, W Q oth Guan, M Y oth Guo, L oth Guo, X H oth Hackenburg, R W oth Han, R oth Hans, S oth He, M oth Heeger, K M oth Heng, Y K oth Higuera, A oth Hor, Y K oth Hsiung, Y B oth Hu, B Z oth Hu, L M oth Hu, L J oth Hu, T oth Hu, W oth Huang, E C oth Huang, H X oth Huang, X T oth Huber, P oth Hussain, G oth Jaffe, D E oth Jaffke, P oth Jen, K L oth Jetter, S oth Ji, X P oth Ji, X L oth Jiao, J B oth Johnson, R A oth Kang, L oth Kettell, S H oth Kramer, M oth Kwan, K K oth Kwok, M W oth Kwok, T oth Langford, T J oth Lau, K oth Lebanowski, L oth Lee, J oth Lei, R T oth Leitner, R oth Leung, K Y oth Leung, J K C oth Lewis, C A oth Li, D J oth Li, F oth Li, G S oth Li, Q J oth Li, S C oth Li, W D oth Li, X N oth Li, X Q oth Li, Y F oth Li, Z B oth Liang, H oth Lin, C J oth Lin, G L oth Lin, P Y oth Lin, S K oth Ling, J J oth ... oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 115(2015), 11 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:115 year:2015 number:11 http://dx.doi.org/10.1103/PhysRevLett.115.111802 Volltext http://www.ncbi.nlm.nih.gov/pubmed/26406819 http://arxiv.org/abs/1505.03456 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 115 2015 11 |
allfieldsSound |
10.1103/PhysRevLett.115.111802 doi PQ20160211 (DE-627)OLC1969288574 (DE-599)GBVOLC1969288574 (PRQ)a1211-a8b0203e85ec8681c800fd9414e05c5128635fe9ccbc0d10f838e6a73f6e989a0 (KEY)0009201020150000115001100000newmeasurementofantineutrinooscillationwiththefull DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk An, F P verfasserin aut New measurement of antineutrino oscillation with the full detector configuration at Daya Bay 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We report a new measurement of electron antineutrino disappearance using the fully constructed Daya Bay Reactor Neutrino Experiment. The final two of eight antineutrino detectors were installed in the summer of 2012. Including the 404 days of data collected from October 2012 to November 2013 resulted in a total exposure of 6.9×10^{5} GW_{th} ton days, a 3.6 times increase over our previous results. Improvements in energy calibration limited variations between detectors to 0.2%. Removal of six ^{241}Am-^{13}C radioactive calibration sources reduced the background by a factor of 2 for the detectors in the experimental hall furthest from the reactors. Direct prediction of the antineutrino signal in the far detectors based on the measurements in the near detectors explicitly minimized the dependence of the measurement on models of reactor antineutrino emission. The uncertainties in our estimates of sin^{2}2θ_{13} and |Δm_{ee}^{2}| were halved as a result of these improvements. An analysis of the relative antineutrino rates and energy spectra between detectors gave sin^{2}2θ_{13}=0.084±0.005 and |Δm_{ee}^{2}|=(2.42±0.11)×10^{-3} eV^{2} in the three-neutrino framework. Instrumentation and Detectors Nuclear Experiment Physics High Energy Physics Experiment Balantekin, A B oth Band, H R oth Bishai, M oth Blyth, S oth Butorov, I oth Cao, G F oth Cao, J oth Cen, W R oth Chan, Y L oth Chang, J F oth Chang, L C oth Chang, Y oth Chen, H S oth Chen, Q Y oth Chen, S M oth Chen, Y X oth Chen, Y oth Cheng, J H oth Cheng, J oth Cheng, Y P oth Cherwinka, J J oth Chu, M C oth Cummings, J P oth de Arcos, J oth Deng, Z Y oth Ding, X F oth Ding, Y Y oth Diwan, M V oth Draeger, E oth Dwyer, D A oth Edwards, W R oth Ely, S R oth Gill, R oth Gonchar, M oth Gong, G H oth Gong, H oth Grassi, M oth Gu, W Q oth Guan, M Y oth Guo, L oth Guo, X H oth Hackenburg, R W oth Han, R oth Hans, S oth He, M oth Heeger, K M oth Heng, Y K oth Higuera, A oth Hor, Y K oth Hsiung, Y B oth Hu, B Z oth Hu, L M oth Hu, L J oth Hu, T oth Hu, W oth Huang, E C oth Huang, H X oth Huang, X T oth Huber, P oth Hussain, G oth Jaffe, D E oth Jaffke, P oth Jen, K L oth Jetter, S oth Ji, X P oth Ji, X L oth Jiao, J B oth Johnson, R A oth Kang, L oth Kettell, S H oth Kramer, M oth Kwan, K K oth Kwok, M W oth Kwok, T oth Langford, T J oth Lau, K oth Lebanowski, L oth Lee, J oth Lei, R T oth Leitner, R oth Leung, K Y oth Leung, J K C oth Lewis, C A oth Li, D J oth Li, F oth Li, G S oth Li, Q J oth Li, S C oth Li, W D oth Li, X N oth Li, X Q oth Li, Y F oth Li, Z B oth Liang, H oth Lin, C J oth Lin, G L oth Lin, P Y oth Lin, S K oth Ling, J J oth ... oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 115(2015), 11 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:115 year:2015 number:11 http://dx.doi.org/10.1103/PhysRevLett.115.111802 Volltext http://www.ncbi.nlm.nih.gov/pubmed/26406819 http://arxiv.org/abs/1505.03456 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 115 2015 11 |
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An, F P @@aut@@ Balantekin, A B @@oth@@ Band, H R @@oth@@ Bishai, M @@oth@@ Blyth, S @@oth@@ Butorov, I @@oth@@ Cao, G F @@oth@@ Cao, J @@oth@@ Cen, W R @@oth@@ Chan, Y L @@oth@@ Chang, J F @@oth@@ Chang, L C @@oth@@ Chang, Y @@oth@@ Chen, H S @@oth@@ Chen, Q Y @@oth@@ Chen, S M @@oth@@ Chen, Y X @@oth@@ Chen, Y @@oth@@ Cheng, J H @@oth@@ Cheng, J @@oth@@ Cheng, Y P @@oth@@ Cherwinka, J J @@oth@@ Chu, M C @@oth@@ Cummings, J P @@oth@@ de Arcos, J @@oth@@ Deng, Z Y @@oth@@ Ding, X F @@oth@@ Ding, Y Y @@oth@@ Diwan, M V @@oth@@ Draeger, E @@oth@@ Dwyer, D A @@oth@@ Edwards, W R @@oth@@ Ely, S R @@oth@@ Gill, R @@oth@@ Gonchar, M @@oth@@ Gong, G H @@oth@@ Gong, H @@oth@@ Grassi, M @@oth@@ Gu, W Q @@oth@@ Guan, M Y @@oth@@ Guo, L @@oth@@ Guo, X H @@oth@@ Hackenburg, R W @@oth@@ Han, R @@oth@@ Hans, S @@oth@@ He, M @@oth@@ Heeger, K M @@oth@@ Heng, Y K @@oth@@ Higuera, A @@oth@@ Hor, Y K @@oth@@ Hsiung, Y B @@oth@@ Hu, B Z @@oth@@ Hu, L M @@oth@@ Hu, L J @@oth@@ Hu, T @@oth@@ Hu, W @@oth@@ Huang, E C @@oth@@ Huang, H X @@oth@@ Huang, X T @@oth@@ Huber, P @@oth@@ Hussain, G @@oth@@ Jaffe, D E @@oth@@ Jaffke, P @@oth@@ Jen, K L @@oth@@ Jetter, S @@oth@@ Ji, X P @@oth@@ Ji, X L @@oth@@ Jiao, J B @@oth@@ Johnson, R A @@oth@@ Kang, L @@oth@@ Kettell, S H @@oth@@ Kramer, M @@oth@@ Kwan, K K @@oth@@ Kwok, M W @@oth@@ Kwok, T @@oth@@ Langford, T J @@oth@@ Lau, K @@oth@@ Lebanowski, L @@oth@@ Lee, J @@oth@@ Lei, R T @@oth@@ Leitner, R @@oth@@ Leung, K Y @@oth@@ Leung, J K C @@oth@@ Lewis, C A @@oth@@ Li, D J @@oth@@ Li, F @@oth@@ Li, G S @@oth@@ Li, Q J @@oth@@ Li, S C @@oth@@ Li, W D @@oth@@ Li, X N @@oth@@ Li, X Q @@oth@@ Li, Y F @@oth@@ Li, Z B @@oth@@ Liang, H @@oth@@ Lin, C J @@oth@@ Lin, G L @@oth@@ Lin, P Y @@oth@@ Lin, S K @@oth@@ Ling, J J @@oth@@ ... @@oth@@ |
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550 DNB UA 1000 AVZ rvk New measurement of antineutrino oscillation with the full detector configuration at Daya Bay Instrumentation and Detectors Nuclear Experiment Physics High Energy Physics Experiment |
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New measurement of antineutrino oscillation with the full detector configuration at Daya Bay |
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New measurement of antineutrino oscillation with the full detector configuration at Daya Bay |
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10.1103/PhysRevLett.115.111802 |
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new measurement of antineutrino oscillation with the full detector configuration at daya bay |
title_auth |
New measurement of antineutrino oscillation with the full detector configuration at Daya Bay |
abstract |
We report a new measurement of electron antineutrino disappearance using the fully constructed Daya Bay Reactor Neutrino Experiment. The final two of eight antineutrino detectors were installed in the summer of 2012. Including the 404 days of data collected from October 2012 to November 2013 resulted in a total exposure of 6.9×10^{5} GW_{th} ton days, a 3.6 times increase over our previous results. Improvements in energy calibration limited variations between detectors to 0.2%. Removal of six ^{241}Am-^{13}C radioactive calibration sources reduced the background by a factor of 2 for the detectors in the experimental hall furthest from the reactors. Direct prediction of the antineutrino signal in the far detectors based on the measurements in the near detectors explicitly minimized the dependence of the measurement on models of reactor antineutrino emission. The uncertainties in our estimates of sin^{2}2θ_{13} and |Δm_{ee}^{2}| were halved as a result of these improvements. An analysis of the relative antineutrino rates and energy spectra between detectors gave sin^{2}2θ_{13}=0.084±0.005 and |Δm_{ee}^{2}|=(2.42±0.11)×10^{-3} eV^{2} in the three-neutrino framework. |
abstractGer |
We report a new measurement of electron antineutrino disappearance using the fully constructed Daya Bay Reactor Neutrino Experiment. The final two of eight antineutrino detectors were installed in the summer of 2012. Including the 404 days of data collected from October 2012 to November 2013 resulted in a total exposure of 6.9×10^{5} GW_{th} ton days, a 3.6 times increase over our previous results. Improvements in energy calibration limited variations between detectors to 0.2%. Removal of six ^{241}Am-^{13}C radioactive calibration sources reduced the background by a factor of 2 for the detectors in the experimental hall furthest from the reactors. Direct prediction of the antineutrino signal in the far detectors based on the measurements in the near detectors explicitly minimized the dependence of the measurement on models of reactor antineutrino emission. The uncertainties in our estimates of sin^{2}2θ_{13} and |Δm_{ee}^{2}| were halved as a result of these improvements. An analysis of the relative antineutrino rates and energy spectra between detectors gave sin^{2}2θ_{13}=0.084±0.005 and |Δm_{ee}^{2}|=(2.42±0.11)×10^{-3} eV^{2} in the three-neutrino framework. |
abstract_unstemmed |
We report a new measurement of electron antineutrino disappearance using the fully constructed Daya Bay Reactor Neutrino Experiment. The final two of eight antineutrino detectors were installed in the summer of 2012. Including the 404 days of data collected from October 2012 to November 2013 resulted in a total exposure of 6.9×10^{5} GW_{th} ton days, a 3.6 times increase over our previous results. Improvements in energy calibration limited variations between detectors to 0.2%. Removal of six ^{241}Am-^{13}C radioactive calibration sources reduced the background by a factor of 2 for the detectors in the experimental hall furthest from the reactors. Direct prediction of the antineutrino signal in the far detectors based on the measurements in the near detectors explicitly minimized the dependence of the measurement on models of reactor antineutrino emission. The uncertainties in our estimates of sin^{2}2θ_{13} and |Δm_{ee}^{2}| were halved as a result of these improvements. An analysis of the relative antineutrino rates and energy spectra between detectors gave sin^{2}2θ_{13}=0.084±0.005 and |Δm_{ee}^{2}|=(2.42±0.11)×10^{-3} eV^{2} in the three-neutrino framework. |
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GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 |
container_issue |
11 |
title_short |
New measurement of antineutrino oscillation with the full detector configuration at Daya Bay |
url |
http://dx.doi.org/10.1103/PhysRevLett.115.111802 http://www.ncbi.nlm.nih.gov/pubmed/26406819 http://arxiv.org/abs/1505.03456 |
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author2 |
Balantekin, A B Band, H R Bishai, M Blyth, S Butorov, I Cao, G F Cao, J Cen, W R Chan, Y L Chang, J F Chang, L C Chang, Y Chen, H S Chen, Q Y Chen, S M Chen, Y X Chen, Y Cheng, J H Cheng, J Cheng, Y P Cherwinka, J J Chu, M C Cummings, J P de Arcos, J Deng, Z Y Ding, X F Ding, Y Y Diwan, M V Draeger, E Dwyer, D A Edwards, W R Ely, S R Gill, R Gonchar, M Gong, G H Gong, H Grassi, M Gu, W Q Guan, M Y Guo, L Guo, X H Hackenburg, R W Han, R Hans, S He, M Heeger, K M Heng, Y K Higuera, A Hor, Y K Hsiung, Y B Hu, B Z Hu, L M Hu, L J Hu, T Hu, W Huang, E C Huang, H X Huang, X T Huber, P Hussain, G Jaffe, D E Jaffke, P Jen, K L Jetter, S Ji, X P Ji, X L Jiao, J B Johnson, R A Kang, L Kettell, S H Kramer, M Kwan, K K Kwok, M W Kwok, T Langford, T J Lau, K Lebanowski, L Lee, J Lei, R T Leitner, R Leung, K Y Leung, J K C Lewis, C A Li, D J Li, F Li, G S Li, Q J Li, S C Li, W D Li, X N Li, X Q Li, Y F Li, Z B Liang, H Lin, C J Lin, G L Lin, P Y Lin, S K Ling, J J . |
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doi_str |
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up_date |
2024-07-04T05:08:21.204Z |
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score |
7.400281 |