Development of a Liquid Scintillator and of Data ... - Borexino - Infn
Development of a Liquid Scintillator and of Data ... - Borexino - Infn
Development of a Liquid Scintillator and of Data ... - Borexino - Infn
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2.1 Physics Goals<br />
- For the LOW solution there is also an incomplete conversion <strong>of</strong> in the sun, but there is<br />
a resonant regeneration <strong>of</strong> inside the earth which would lead to a significantly higher<br />
count rate during the night hours than during the day, the so-called “day-night effect”.<br />
This effect is maximal in the energy region below 1 MeV(see fig. 2.3). BOREXINO,<br />
which is the only real-time experiment measuring neutrinos at these low energies, would<br />
see a day-night difference <strong>of</strong> 10 - 20 %.<br />
- The eccentricity <strong>of</strong> the earth’s orbit causes an annual variation <strong>of</strong> the solar neutrino flux,<br />
with a difference <strong>of</strong> 7 % between perihelion <strong>and</strong> aphelion. For ¡Ñ ¡ Î the<br />
vacuum oscillation length for Be neutrinos is about 3 % <strong>of</strong> the sun-earth distance.<br />
This would lead to significant seasonal variations <strong>of</strong> the counting rate (see fig. 2.4), as<br />
the oscillation probability changes with the distance from the sun.<br />
- In the case <strong>of</strong> oscillations into sterile neutrinos, the conversion <strong>of</strong> the electron<br />
neutrinos is almost complete. As the sterile neutrinos don’t interact in any way in the<br />
detector, the measured count rate in BOREXINO would range from 0 to 25 % <strong>of</strong> the SSM<br />
flux.<br />
Figure 2.3: Energy dependent survival probabilities <strong>of</strong> electron neutrinos for the different MSW<br />
scenarios. The time averaged probability is shown in addition to the separate probabilities for<br />
day <strong>and</strong> night hours. Only for the LOW solution there is a significant day-night effect for the Be<br />
neutrinos.<br />
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