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Table 1:

Observational results.
  V Cam R Leo

Phase of optical lightcurve(1)
0.08 0.10
Oscillation period of circular polarization(2) $(5.4\pm 0.1)$ h $(6.3 \pm 0.3)$ h
False-alarm probability(3) 4% 16%
Radial velocity of maser spots(4) 7.5 km s-1 4.4 km s-1
Mean circular polarization $-0.3\%$ $+2.0\%$
Mean magnetic flux density in maser(5) $\sim$100 mG $\sim$1 G
Peak-to-peak variation of fractional polarization $2.8\% = 5.6~\sigma_{\rm rms}$ $3.7\% = 7.4~\sigma_{\rm rms}$
Fluctuation of magnetic field(5) $\sim$1 G $\sim$1 G
(1) With respect to the maximum of the optical lightcurve; (2) for V Cam the second harmonic of the modelled rotation period; (3) with respect to the null hypothesis (data are Gaussian noise); (4) with respect to the local standard of rest; (5) order-of-magnitude estimate based on the Zeeman hypothesis, and for a linewidth of 1 km s-1. This corresponds to a maser at $3~r_{\rm J}$ and a planetary magnetic dipole field eight times stronger than Jupiter's (Wiesemeyer 2008).

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