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GNO Solar Neutrino Observations: Results for GNOI
High Energy Physics - Experiment · Submitted 29 Jun 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim With counting completed for all but the last 3 runs (SR17 - SR19), the GNO I result is [65.8 +10.2 -9.6 (stat.) +3.4 -3.6 (syst.)]SNU (1sigma) or [65.8 + 10.7 -10.2 (incl. syst.)]SNU (1sigma) with errors combined.
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The abstract, sentence by sentence
We report the first GNO solar neutrino results for the measuring period GNOI, solar exposure time May 20, 1998 till January 12, 2000. In the present analysis, counting results for solar runs SR1 - SR19 were used till April 4, 2000. With counting completed for all but the last 3 runs (SR17 - SR19), the GNO I result is [65.8 +10.2 -9.6 (stat.) +3.4 -3.6 (syst.)]SNU (1sigma) or [65.8 + 10.7 -10.2 (incl. syst.)]SNU (1sigma) with errors combined. This may be compared to the result for Gallex(I-IV), which is [77.5 +7.6 -7.8 (incl. syst.)] SNU (1sigma). A combined result from both GNOI and Gallex(I-IV) together is [74.1 + 6.7 -6.8 (incl. syst.)] SNU (1sigma).
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We report the first GNO solar neutrino results for the measuring period GNOI, solar exposure time May 20, 1998 till January 12, 2000. | contribution 1.00 | 0.95 | 0.07 | asserted 0.99 |
| s1 | In the present analysis, counting results for solar runs SR1 - SR19 were used till April 4, 2000. | method 0.95 | 0.84 | 0.02 | asserted 0.99 |
| s2 | With counting completed for all but the last 3 runs (SR17 - SR19), the GNO I result is [65.8 +10.2 -9.6 (stat.) +3.4 -3.6 (syst.)]SNU (1sigma) or [65.8 + 10.7 -10.2 (incl. syst.)]SNU (1sigma) with errors combined. | result 1.00 | 0.96 | 0.71 | asserted 1.00 |
| s3 | This may be compared to the result for Gallex(I-IV), which is [77.5 +7.6 -7.8 (incl. syst.)] SNU (1sigma). | background 0.47 | 0.23 | 0.09 | hedged possibility 0.69 |
| s4 | A combined result from both GNOI and Gallex(I-IV) together is [74.1 + 6.7 -6.8 (incl. syst.)] SNU (1sigma). | result 1.00 | 0.87 | 0.26 | asserted 1.00 |
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The paper
Original abstract
We report the first GNO solar neutrino results for the measuring period GNOI, solar exposure time May 20, 1998 till January 12, 2000. In the present analysis, counting results for solar runs SR1 - SR19 were used till April 4, 2000. With counting completed for all but the last 3 runs (SR17 - SR19), the GNO I result is [65.8 +10.2 -9.6 (stat.) +3.4 -3.6 (syst.)]SNU (1sigma) or [65.8 + 10.7 -10.2 (incl. syst.)]SNU (1sigma) with errors combined. This may be compared to the result for Gallex(I-IV), which is [77.5 +7.6 -7.8 (incl. syst.)] SNU (1sigma). A combined result from both GNOI and Gallex(I-IV) together is [74.1 + 6.7 -6.8 (incl. syst.)] SNU (1sigma).
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References
How the literature uses it
17 arXiv papers cite this in 17 sentences
Papers citing it · 9 sentences without a confident label
Uses its data or values 2 papers
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Starting from the observed values for the electron neutrino disappearance probabilities by Borexino [ref] [equation] and adding the spectral information on the $^8B$ neutrinos by SNO [ref] [Additional solar neutrino information from the dedicated pp experiments SAGE, GALEX, and GNO [ref] and $^8$B measurements Super-Kamiokande [ref] will add some additional information, but will not significantly enhance the constraint.], we then compute the $χ^2$ function defined as [equation] where $p$ are all the neutrino components already mentioned, $P_obs^p$ are the observed probabilities with their uncertainties $(σ^p_obs)^2$ in eq.
Solar Neutrinos and the Strongest Oscillation Constraints on Scalar NSI · Solar data analysis in presence of diagonal scalar NSI parameters · 1.00
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Recent real-time high-precision solar neutrino data from Sudbury Neutrino Observatory (SNO) [ref] and SuperKamiokande (SK) [ref] experiments combined with data from radiochemical Homestake [ref] , SAGE [ref] , Gallex [ref] , and Gallium Neutrino Observatory (GNO) [ref] experiments pinpointed neutrino parameters, especially the value of the mixing angle usually referred to as $θ_⊙$.
Contrasting solar and reactor neutrinos with a non-zero value of theta13 · Introduction · 0.84
Cites it as background 6 papers
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Following the seminal experiment of Davis [ref] , experiments were performed to measure the predominant pp neutrinos [ref] , as well as the higher energy neutrinos: Borexino measured the line flux coming from $^7$Be neutrinos [ref] .
Solar Neutrino Matter Effects Redux · Introduction · 0.90
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The discovery of neutrino masses from the solar and atmospheric data [ref] has very significantly advanced our understanding of the basic nature of these particles.
An MSSM Extension with a Mirror Fourth Generation, Neutrino Magnetic Moments and LHC Signatures · Neutrino magnetic moment · 0.86
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Experiments carried out in the last two decades have categorically confirmed the neutrino oscillation phenomenon as the mechanism responsible for the flavour transitions observed in the neutrino fluxes coming from the sun [ref] , the atmosphere [ref] , reactors [ref] and accelerators [ref] .
Visible neutrino decay in the light of appearance and disappearance long baseline experiments · Introduction · 0.86
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