Fig. 2

Fractional linear polarization as a function of TbΔΩ for the 183 GHz, 313−220 (top), and the 325 GHz, 515−422 (bottom) H2O rotational transitions, both within the ground-vibrational level, for four values of the angle between the magnetic field lines and the direction of propagation of the maser radiation, θ. We considered the magnetic field strength and decay rate listed in Table 3 for H2O. Positive and negative pL values mean that the vector of polarization is either perpendicular or parallel the magnetic field lines projected on the plane of the sky. The vertical line sets the TbΔΩ value such that gΩ = 10R.
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