The weak mixing angle from low energy neutrino measurements: A global update
Taking into account recent theoretical and experimental inputs on reactor fluxes we reconsider the determination of the weak mixing angle from low energy experiments. We perform a global analysis to all available neutrino–electron scattering data from reactor antineutrino experiments, obtaining sin2...
Ausführliche Beschreibung
Autor*in: |
B.C. Cañas [verfasserIn] E.A. Garcés [verfasserIn] O.G. Miranda [verfasserIn] M. Tórtola [verfasserIn] J.W.F. Valle [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2016 |
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Übergeordnetes Werk: |
In: Physics Letters B - Elsevier, 2015, 761(2016), C, Seite 450-455 |
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Übergeordnetes Werk: |
volume:761 ; year:2016 ; number:C ; pages:450-455 |
Links: |
Link aufrufen |
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DOI / URN: |
10.1016/j.physletb.2016.08.047 |
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Katalog-ID: |
DOAJ009724532 |
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10.1016/j.physletb.2016.08.047 doi (DE-627)DOAJ009724532 (DE-599)DOAJa9cd6579219f4c4c9486232475430f5a DE-627 ger DE-627 rakwb eng QC1-999 B.C. Cañas verfasserin aut The weak mixing angle from low energy neutrino measurements: A global update 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Taking into account recent theoretical and experimental inputs on reactor fluxes we reconsider the determination of the weak mixing angle from low energy experiments. We perform a global analysis to all available neutrino–electron scattering data from reactor antineutrino experiments, obtaining sin2θW=0.252±0.030. We discuss the impact of the new theoretical prediction for the neutrino spectrum, the new measurement of the reactor antineutrino spectrum by the Daya Bay collaboration, as well as the effect of radiative corrections. We also reanalyze the measurements of the νe−e cross section at accelerator experiments including radiative corrections. By combining reactor and accelerator data we obtain an improved determination for the weak mixing angle, sin2θW=0.254±0.024. Physics E.A. Garcés verfasserin aut O.G. Miranda verfasserin aut M. Tórtola verfasserin aut J.W.F. Valle verfasserin aut In Physics Letters B Elsevier, 2015 761(2016), C, Seite 450-455 (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:761 year:2016 number:C pages:450-455 https://doi.org/10.1016/j.physletb.2016.08.047 kostenfrei https://doaj.org/article/a9cd6579219f4c4c9486232475430f5a kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269316304671 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei https://doaj.org/toc/1873-2445 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 761 2016 C 450-455 |
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10.1016/j.physletb.2016.08.047 doi (DE-627)DOAJ009724532 (DE-599)DOAJa9cd6579219f4c4c9486232475430f5a DE-627 ger DE-627 rakwb eng QC1-999 B.C. Cañas verfasserin aut The weak mixing angle from low energy neutrino measurements: A global update 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Taking into account recent theoretical and experimental inputs on reactor fluxes we reconsider the determination of the weak mixing angle from low energy experiments. We perform a global analysis to all available neutrino–electron scattering data from reactor antineutrino experiments, obtaining sin2θW=0.252±0.030. We discuss the impact of the new theoretical prediction for the neutrino spectrum, the new measurement of the reactor antineutrino spectrum by the Daya Bay collaboration, as well as the effect of radiative corrections. We also reanalyze the measurements of the νe−e cross section at accelerator experiments including radiative corrections. By combining reactor and accelerator data we obtain an improved determination for the weak mixing angle, sin2θW=0.254±0.024. Physics E.A. Garcés verfasserin aut O.G. Miranda verfasserin aut M. Tórtola verfasserin aut J.W.F. Valle verfasserin aut In Physics Letters B Elsevier, 2015 761(2016), C, Seite 450-455 (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:761 year:2016 number:C pages:450-455 https://doi.org/10.1016/j.physletb.2016.08.047 kostenfrei https://doaj.org/article/a9cd6579219f4c4c9486232475430f5a kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269316304671 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei https://doaj.org/toc/1873-2445 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 761 2016 C 450-455 |
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Taking into account recent theoretical and experimental inputs on reactor fluxes we reconsider the determination of the weak mixing angle from low energy experiments. We perform a global analysis to all available neutrino–electron scattering data from reactor antineutrino experiments, obtaining sin2θW=0.252±0.030. We discuss the impact of the new theoretical prediction for the neutrino spectrum, the new measurement of the reactor antineutrino spectrum by the Daya Bay collaboration, as well as the effect of radiative corrections. We also reanalyze the measurements of the νe−e cross section at accelerator experiments including radiative corrections. By combining reactor and accelerator data we obtain an improved determination for the weak mixing angle, sin2θW=0.254±0.024. |
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Taking into account recent theoretical and experimental inputs on reactor fluxes we reconsider the determination of the weak mixing angle from low energy experiments. We perform a global analysis to all available neutrino–electron scattering data from reactor antineutrino experiments, obtaining sin2θW=0.252±0.030. We discuss the impact of the new theoretical prediction for the neutrino spectrum, the new measurement of the reactor antineutrino spectrum by the Daya Bay collaboration, as well as the effect of radiative corrections. We also reanalyze the measurements of the νe−e cross section at accelerator experiments including radiative corrections. By combining reactor and accelerator data we obtain an improved determination for the weak mixing angle, sin2θW=0.254±0.024. |
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Taking into account recent theoretical and experimental inputs on reactor fluxes we reconsider the determination of the weak mixing angle from low energy experiments. We perform a global analysis to all available neutrino–electron scattering data from reactor antineutrino experiments, obtaining sin2θW=0.252±0.030. We discuss the impact of the new theoretical prediction for the neutrino spectrum, the new measurement of the reactor antineutrino spectrum by the Daya Bay collaboration, as well as the effect of radiative corrections. We also reanalyze the measurements of the νe−e cross section at accelerator experiments including radiative corrections. By combining reactor and accelerator data we obtain an improved determination for the weak mixing angle, sin2θW=0.254±0.024. |
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