Table B.1.
Characteristics of the averaged shifts due to magnetic activity.
Frequency range | BiSON | GOLF | ||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|
Δr01 | Δr02 | Δν0 | Δr01 | Δr02 | Δν0 | |||||||
ℛ | 𝒜 | ℛ | 𝒜 | ℛ | 𝒜 | ℛ | 𝒜 | ℛ | 𝒜 | ℛ | 𝒜 | |
Full | −0.56 ± 0.11 | 0.00078 | −0.63 ± 0.02 | 0.00137 | 0.92 ± 0.03 | 0.237 | −0.53 ± 0.02 | 0.00068 | −0.32 ± 0.05 | 0.00106 | 0.90 ± 0.01 | 0.274 |
Low-frequency | −0.42 ± 0.10 | 0.00087 | −0.18 ± 0.08 | - | 0.19 ± 0.04 | - | −0.25 ± 0.07 | - | 0.00 ± 0.13 | - | 0.50 ± 0.04 | 0.100 |
Medium-frequency | −0.38 ± 0.06 | 0.00112 | −0.53 ± 0.09 | 0.00149 | 0.85 ± 0.02 | 0.242 | −0.49 ± 0.06 | 0.00096 | −0.55 ± 0.04 | 0.00125 | 0.89 ± 0.01 | 0.211 |
High-frequency | −0.38 ± 0.08 | 0.00152 | −0.44 ± 0.05 | 0.00228 | 0.89 ± 0.01 | 0.567 | −0.37 ± 0.07 | 0.00121 | −0.27 ± 0.05 | 0.00183 | 0.86 ± 0.04 | 0.541 |
Notes. The correlation between the averaged shift and the activity proxy, the 10.7 cm radio emission flux, is measured with the Spearman rank coefficient ℛ. The symbol 𝒜 denotes the amplitude of the averaged shift, computed by taking the difference between the maximum and minimum of the data smoothed with a Savitzky-Golay filter. The shift amplitude was only evaluated for correlation coefficients strictly larger than 0.25.
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