Proc. Neutrino Astrophysics - MPP Theory Group
Proc. Neutrino Astrophysics - MPP Theory Group
Proc. Neutrino Astrophysics - MPP Theory Group
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known true source activity. The combined analysis of both series results in R = 0.93 ± 0.08,<br />
clearly demonstrating the absence of large systematic errors which could account for the<br />
observed 40% solar neutrino deficit.<br />
A similar experiment has also been performed by the Sage collaboration. They got a<br />
quantitative recovery of R = 0.95 ± 0.12 [6].<br />
The fact that both experiments, though employing different chemistry, demonstrated in<br />
these experiments full efficiency, proves the trustworthiness of the radiochemical method and<br />
shows that the 40% solar neutrino deficit observed in the radiochemical gallium experiments<br />
cannot be ascribed to unknown systematic errors. In particular, the 51 Cr neutrino energies<br />
nicely accommodating those from the solar 7 Be-branch, the full efficiency of the gallium<br />
experiments to 7 Be-neutrinos is demonstrated.<br />
71 As experiments<br />
However, though the 51 Cr source in Gallex did outperform the sun by more than a factor<br />
15 after insertion into the target tank, the experiments still are low statistics, involving only<br />
several dozens of neutrino produced 71 Ge atoms. Therefore, at the very end of Gallex the<br />
collaboration has performed a large-scale test of potential effects of hot chemistry, which<br />
might lead to a different chemical behaviour of 71 Ge produced in a nuclear reaction compared<br />
to the stable Ge carrier isotope: The in-situ production of 71 Ge by β−decay of 71 As. A known<br />
quantity of 71 As (O(10 5 ) atoms) has been added to the tank (t-sample), where it decayed with<br />
T 1/2 = 2.9d to 71 Ge. Four runs have been made under different operating conditions (mixing,<br />
carrier addition, standing time), cf. table 2. For every spike a reference sample (e-sample)<br />
was kept aside, making possible to calculate the ratio of t- and e-sample which does not suffer<br />
from most of the systematic uncertainties associated with 71 Ge-counting.<br />
Table 2: Experimental conditions and results (ratio t-sample/e-sample) of the 71 As runs.<br />
run mixing conditions Ge-carrier standing result<br />
[h × m 3 /h] addition time (tank / external)<br />
A1 22 × 5.5 with As 19.9 d 1.01 ± 0.03<br />
+0.17 × 60<br />
A2 6 × 5.5 no Ge-carrier 19.9 d 1.00 ± 0.03<br />
B3-1 24 × 5.5 after As 2.0 d 1.01 ± 0.03<br />
B3-2 — after As 22.0 d 1.00 ± 0.03<br />
In all cases a quantitative recovery of 100% was achieved. This demonstrates on a 3%-level the<br />
absence of withholding effects even under unfavourable conditions like carrier-free operation 1 .<br />
Gallium <strong>Neutrino</strong> Observatory<br />
With the 71 As-tests Gallex has completed its large-scale experimental program. However,<br />
solar neutrino measurements with a gallium target at Gran Sasso will be re-commenced in<br />
spring 1998 in the frame of the Gallium <strong>Neutrino</strong> Observatory (GNO) [2] which is designed for<br />
1 The stable germanium carrier is not only used for determination of the extraction yield, but also plays the<br />
role of an ’insurance’ to saturate potential trace impurities which might capture 71 Ge in non-volatile complexes.