2005
DOI: 10.1088/1126-6708/2005/07/051
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Low energy solar neutrinos and spin flavour precession

Abstract: The possibility that the Gallium data effectively indicates a time modulation of the solar active neutrino flux in possible connection to solar activity is examined on the light of spin flavour precession to sterile neutrinos as a subdominant process in addition to oscillations. We distinguish two sets of Gallium data, relating them to high and low solar activity. Such modulation affects principally the low energy neutrinos (pp and 7 Be) so that the effect, if it exists, will become most clear in the forthcomi… Show more

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Cited by 21 publications
(37 citation statements)
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“…Because solar rotation should not produce variations in the solar nuclear fusion rate, nonstandard neutrino properties have been proposed as an explanation. For example, the coupling of a neutrino magnetic moment to rotating magnetic fields inside the Sun might cause solar neutrinos to transform into other flavors through a resonant spin flavor precession mechanism [11][12][13]. Periodicities in the solar neutrino flux, if confirmed, could provide evidence for new neutrino physics beyond the commonly accepted picture of matter-enhanced oscillation of massive neutrinos.…”
Section: Introductionmentioning
confidence: 99%
“…Because solar rotation should not produce variations in the solar nuclear fusion rate, nonstandard neutrino properties have been proposed as an explanation. For example, the coupling of a neutrino magnetic moment to rotating magnetic fields inside the Sun might cause solar neutrinos to transform into other flavors through a resonant spin flavor precession mechanism [11][12][13]. Periodicities in the solar neutrino flux, if confirmed, could provide evidence for new neutrino physics beyond the commonly accepted picture of matter-enhanced oscillation of massive neutrinos.…”
Section: Introductionmentioning
confidence: 99%
“…Our results are depicted in fig.4 for the best fit LMA+SFP prediction with ∆m 2 21 = 8.2 × 10 −5 eV 2 , tan 2 θ = 0.31 (middle curve), for the set ∆m 2 21 = 8.4 × 10 −5 eV 2 , tan 2 θ = 0.27 (upper curve) and for the LMA best fit, ∆m 2 21 = 7.9 × 10 −5 eV 2 , tan 2 θ = 0.46 (lower curve). For the average source-detector distance of 180 km, as reported by KamLAND, we get from fig.4, P = 0.576 (LMA), 0.623 (Best fit SFP), 0.651 (Table 4 fit) (18) to be compared with the data, P = 0.658 ± 0.064 [23]. Interestingly enough it is seen that the best of the three fits lies in this case for the parameter choice as in table 4, namely the one leading to the Gallium data sets which lie the furthest apart: 74.7 and 60.5 SNU.…”
Section: Global Fits and Survival Probabilitymentioning
confidence: 77%
“…Time variation for 7 Be neutrinos and other low energy neutrinos in the real time experiments BOREXINO and LENS has been examined in [12]. Our main motivation in this work is, as indicated by the title itself, to give predictions for the 7 Be neutrino time variation in KamLAND experiment.…”
Section: Jhep02(2006)035mentioning
confidence: 99%