Abstract:We analyze the atmospheric neutrino data in the context of three flavor neutrino oscillations taking account of the matter effects in the Earth. With the hierarchy among the vacuum mass eigenvalues 3 2 ӷ 2 2 у 1 2 , the solution of the atmospheric neutrino problem depends on ␦ 31 ϭ 3 2 Ϫ 1 2 and the 13 and 23 mixing angles and . Whereas the sub-GeV atmospheric neutrino data imposes only a lower limit on ␦ 31 Ͼ10 Ϫ3 eV 2 , the zenithangle-dependent suppression observed in the multi-GeV data limits ␦ 31 from abo… Show more
“…The broken lines enclose regions whose predictions fall within the range given by ½ uncertainties. These results have been presented in [23].…”
Section: Results and Conclusionsupporting
confidence: 74%
“…We can now estimate the maximum contribution of the channel to the atmospheric neutrino anomaly using the CHOOZ result. Since the relevant AE ¿½ is about ½¼ ¾ Î ¾ , matter effects are negligible for the problem [23]. Hence the relevant probability is the vacuum ° oscillation probability,…”
Section: Three Flavor Analysis Of Chooz Resultsmentioning
We summarize the constraints on three flavor neutrino mixing coming from data. We first map out the allowed region in the three neutrino parameter space using solar and atmospheric neutrino data. We then incorporate the results of reactor and long baseline experiments in our analysis and show that the parameter space is drastically reduced. We conclude by pointing out that the results of Borexino and SNO will further help in constraining the parameter space.
“…The broken lines enclose regions whose predictions fall within the range given by ½ uncertainties. These results have been presented in [23].…”
Section: Results and Conclusionsupporting
confidence: 74%
“…We can now estimate the maximum contribution of the channel to the atmospheric neutrino anomaly using the CHOOZ result. Since the relevant AE ¿½ is about ½¼ ¾ Î ¾ , matter effects are negligible for the problem [23]. Hence the relevant probability is the vacuum ° oscillation probability,…”
Section: Three Flavor Analysis Of Chooz Resultsmentioning
We summarize the constraints on three flavor neutrino mixing coming from data. We first map out the allowed region in the three neutrino parameter space using solar and atmospheric neutrino data. We then incorporate the results of reactor and long baseline experiments in our analysis and show that the parameter space is drastically reduced. We conclude by pointing out that the results of Borexino and SNO will further help in constraining the parameter space.
“…(1), one can show that the solar neutrino problem depends only on δm 2 21 , ω and φ while the atmospheric neutrino problem depends only on δm 2 32 , ψ and φ. It is this simplification that allows us to analyse the two problems within a 3 − ν framework under reasonable control and one gets a fairly broad and stable set of allowed regions in the 5-parameter space [4,5]. If we temporarily put φ as zero, then the two problems decouple and the results are the following :-There are three solutions of the solar neutrino problem : [6] turns out to be a crucial result.…”
Section: Resultsmentioning
confidence: 99%
“…Extensive literature exists on the solar [4,10] and atmospheric neutrinos [5,11]. So, we shall be brief.…”
Section: Solar Atmospheric and Reactor Neutrinosmentioning
confidence: 99%
“…All these are consistent with ν µ oscillating into ν τ over the distance scale of about 10,000 km ; so it is for the upward-going ν µ travelling through the earth that the effect is most dominant. The effect of earth matter in the atmospheric neutrino problem is not significant [5] at the present level of accuracy and hence one can use Eq.(3). The resulting neutrino prameters were given in Sec 2.…”
Section: Solar Atmospheric and Reactor Neutrinosmentioning
The phenomenology of solar, atmospheric, supernova and laboratory neutrino oscillations is described. Analytical formulae for matter effects are reviewed. The results from oscillations are confronted with neutrinoless double beta decay.
I consider the mixing of the three active neutrino flavours and obtain the constraints on the parameters of this mixing from the solar, atmospheric and reactor neutrino data.
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