Table 2.
Significant periodic photometric variability seen in the UBr and BAb BRITE photometry of o Lupi.
ID | Origin | UBr |
BAb |
||||||
---|---|---|---|---|---|---|---|---|---|
f | δf | A | S/N | f | δf | A | S/N | ||
(d−1) | (10−4 d−1) | (±0.17 ppt) | (d−1) | (10−4 d−1) | (±0.35 ppt) | ||||
f1 | frot | 0.33869 | 1.5 | 4.63 | 9.6 | 0.33792 | 2.9 | 5.02 | 4.7 |
f2 | 2frot | 0.67706 | 1.3 | 5.03 | 8.5 | 0.67687 | 3.2 | 4.62 | 5.0 |
f3 | g mode | 1.10572 | 0.9 | 7.14 | 10.0 | 1.10611 | 1.9 | 7.65 | 5.8 |
f4 | finst | 1.00078 | 3.5 | 1.91 | 5.9 | ||||
f5 | 3frot | 1.01586 | 5.2 | 1.29 | 4.5 | ||||
f6 | g mode | 1.29852 | 4.8 | 1.40 | 4.8 |
Notes. We indicate the frequency and corresponding amplitude, A, together with their respective uncertainties, as well as the S/N of the detection in the Lomb-Scargle periodogram during the iterative prewhitening procedure. The frequency and amplitude uncertainties are determined from Montgomery & O’Donoghue (1999), under the assumption of white noise and uncorrelated data. These conditions are not always fullfilled and result in a typical underestimation of the frequency error by a factor 10 (e.g., Degroote et al. 2009b). We also indicate the proposed origin of the observed periodic photometric variability and remark that a more precise value for the rotation period was obtained through the magnetometric analysis in Sect. 5.
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