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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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Solar Neutrinos 373<br />

of order the annual distance variation, the 7 Be flux me<strong>as</strong>ured in the<br />

chlorine and gallium detectors could vary between zero and its predicted<br />

full rate. Moreover, at different times of the year the neutrinos have<br />

to traverse on average a different amount of terrestrial matter which<br />

could affect neutrino oscillations and thus lead to an annual variation.<br />

There is no evidence <strong>for</strong> such an effect in any of the detectors.<br />

GALLEX reports a counting rate of (82 ± 15 stat ) SNU <strong>for</strong> October−<br />

March and (78 ± 14 stat ) SNU <strong>for</strong> April−September, i.e. there is no significant<br />

difference (GALLEX collaboration 1994).<br />

A semiannual variation could be caused by nonstandard neutrino interactions<br />

with the solar magnetic field (Sect. 10.7). The solar equatorial<br />

plane is at an angle of 7 ◦ 15 ′ relative to the Earth’s orbital plane (the<br />

ecliptic). Around 7 June and 8 December, the solar core is viewed from<br />

Earth through the solar equator where the magnetic field is thought<br />

to be weaker than at higher latitudes. The Kamiokande II data (1040<br />

live detector days in 1987−1990) were subdivided into three-months<br />

periods which include (rate Γ I ) or exclude (Γ II ) the intersection points,<br />

respectively. The relative difference in counting rate w<strong>as</strong> found to be<br />

(Γ I − Γ II )/(Γ I + Γ II ) = −0.06 ± 0.11 stat ± 0.02 syst , i.e. there w<strong>as</strong> no indication<br />

<strong>for</strong> a time variation (Hirata et al. 1991). The Homestake data<br />

also do not show any evidence <strong>for</strong> a semiannual variation.<br />

10.4.3 Correlation with Solar Cycle at Homestake<br />

The Sun shows a prominent magnetic activity cycle which is thought<br />

to be due to dynamo action within the convective surface layers, driven<br />

by the nonuni<strong>for</strong>m rotation of the Sun (Stix 1989). One of the bestknown<br />

manifestations of this activity is the cycle of sunspots, me<strong>as</strong>ured<br />

by their total number appearing on the solar disk. 54 A given solar cycle<br />

l<strong>as</strong>ts <strong>for</strong> about 11 years from one minimum of sunspot number to<br />

the following; the first recorded cycle begins with the minimum around<br />

A.D. 1755. Sunspots are caused by magnetic flux tubes which break<br />

through the surface; they are thought to be manifestations of a subsurface<br />

toroidal magnetic field with opposite directions between the<br />

southern and northern hemisphere. In addition, the Sun h<strong>as</strong> a poloidal<br />

(dipole) field. The fields reverse polarity after 11 years so that the full<br />

magnetic cycle l<strong>as</strong>ts 22 years.<br />

54 In the following, the “number of sunspots” refers to the international sunspot<br />

index according to the Zürich system where both spots and spot groups are counted<br />

and averaged from the reports of many solar observatories. The sunspot index is<br />

regularly published in Solar Geophysical Data.

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