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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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Solar Neutrinos 357<br />

Xu et al. (1994) have discussed a unique relationship between S 17 (0)<br />

and the nuclear vertex constant of the overlap wave function <strong>for</strong> the<br />

virtual decay 8 B → 7 Be+p; the nuclear vertex constant can be predicted<br />

from other nuclear data. These authors’ calculation of S 17 (E) agrees<br />

remarkably well with the data points of Filippone et al. (1983) at low<br />

energies, and with Vaughn et al. (1970) at higher energies; these are<br />

the experiments which gave a low S 17 (0). Xu et al. (1994) find an even<br />

lower value of S 17 (0) ≈ 17.6 eV b.<br />

On the other hand, Brown, Csótó, and Sherr (1995) studied the<br />

relationship between the Coulomb displacement energy <strong>for</strong> the A = 8,<br />

J = 2 + , T = 1 state and S 17 . They found a high value S 17 (20 keV) =<br />

(26.5 ± 2.0) eV b.<br />

The S 17 (0) factor w<strong>as</strong> recently determined from the Coulomb dissociation<br />

of 8 B, i.e. by the Primakoff-type process 8 B → 7 Be + p in<br />

the electric field of a 208 Pb nucleus (Motobay<strong>as</strong>hi et al. 1994). These<br />

authors find a very low preliminary value of S 17 (0) = (16.7 ± 3.2) eV b.<br />

Langanke and Shoppa (1994) think that the true value may be significantly<br />

lower still if allowance is made <strong>for</strong> a possible E2 amplitude in<br />

the Primakoff reaction. However, this possibility is heavily disputed by<br />

Gai and Bertulani (1995); see also the reply by Langanke and Shoppa<br />

(1995).<br />

All of these new results are somewhat preliminary at the present<br />

time. Independently of their ultimate status it is evident that the S 17<br />

factor must be considered the weakest link in the prediction of the<br />

boron neutrino flux.<br />

10.3 Observations<br />

10.3.1 Absorption Reactions <strong>for</strong> Radiochemical Experiments<br />

The longest-running solar neutrino experiment is the Homestake chlorine<br />

detector which is b<strong>as</strong>ed on a reaction proposed by Pontecorvo<br />

(1948) and Alvarez (1949),<br />

ν e + 37 Cl → 37 Ar + e (threshold 0.814 MeV). (10.9)<br />

The two other data-producing radiochemical experiments use gallium<br />

<strong>as</strong> a target according to the reaction<br />

ν e + 71 Ga → 71 Ge + e (threshold 0.233 MeV). (10.10)<br />

Because of its low threshold, the gallium experiments can pick up the<br />

solar pp neutrino flux. The absorption cross sections <strong>as</strong> a function of

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