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SAGE |
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All four solar neutrino experiments (Chlorine,
SUPERKAMIOKANDE, SAGE, and GALLEX) show that the measured solar neutrino
flux at the orbit of the Earth is considerably less than predicted by the
Standard Solar Model. Because the reduction of the solar neutrino spectrum
is most pronounced at intermediate energies (~1 MeV), new detectors that
can measure the neutrino radiation from the Sun in this energy regime are
especially needed. Several such detectors are in various stages of development
and deployment, such as BOREXINO at Gran Sasso, KAMLAND in Japan, and the
iodine detector at Homestake. To be certain of their response to low-energy
neutrinos, these detectors must be calibrated by exposure to an intense
artificially-produced source of neutrinos of about 1 MeV. Because of the
extremely small cross section for neutrino capture, source intensities
of about 1 MCi are necessary.
Two possible sources for this purpose are 51Cr and 37Ar. Sources of 51Cr of ~1 MCi activity have been used to measure the low-energy neutrino cross section of Ga. An even more useful source is 37Ar, which decays by electron capture and emits a monoenergetic neutrino. 37Ar has several advantages compared to 51Cr. The neutrino is higher energy (814 keV vs. 747 keV). It has a longer half-life (35 d vs. 28 d). Because the Ar is easy to separate, there are almost no accompanying gamma rays from contamination thus reducing the need for bulky shielding and simplifying source transportation. Finally an Ar source can be very precisely calibrated by counting a small aliquot. Both KAMLAND and the iodine project have expressed an interest to calibrate their detectors with an intense 37Ar source. These experiments are sensitive to Compton scattered electrons and thus require a calibration source, like 37Ar, that has a reduced high-energy photon emission.
The use of 37Ar to calibrate solar neutrino detectors was originally proposed by Haxton in 1988(W. Haxton, Phys. Rev. Lett. 60, 768 (1988).). 37Ar will be produced by fast neutrons using the reaction 4040Ca(n,a)37Ar. Previous work(V.N. Gavrin, et al., Preprint INR 777/92 (1992); and J.N. Abdurashitov, et al., to be published in Instruments and Experimental Techniques.) showed that calcium oxide, CaO (2.4 g Ca/cm3) was the most suitable calcium-containing target. A 1-MCi 37Ar source could be produced by placing about 200 kg of Ca in a fast flux reactor. Argon is easily removed from this target by dissolving the CaO in water or acid and flowing a carrier gas (such as He) through the solution. Argon is easily separated from helium with a trap at low temperature and reactive gases, such as hydrogen, can be removed from argon by flowing the gas through a getter at high temperature. After purification, the 37Ar will be encapsulated in a minimal volume as the prototype of a source. The activity of this prototype will be determined by various methods, such as by measuring the rate of decay of a small aliquot of Ar in a proportional counter and by measuring the inner bremsstrahlung activity.
The project is funded by the International
Scientific and Technology Center (ISTC) award number 1431.