According to Fresnel's equations for the magnetic field parallel to the surface of a dielectric, the reflection coefficient is this: $$r_{s}=\frac{\cos\theta^{i}-\frac{n_2}{n_1}\cos\theta^{t}}{\cos\theta^{i}+\frac{n_2}{n_1}\cos\theta^{t}}\tag{R}$$
In all the examples I have found, the magnetic field's direction "looks"(I'm not sure what is the correct term) at the reader (like this)
However, when the magnetic field "looks down", like this
the reflection coefficient I have found is the negative of Fresnel's. $$r_{s}=\frac{-\cos\theta^{i}+\frac{n_2}{n_1}\cos\theta^{t}}{\cos\theta^{i}+\frac{n_2}{n_1}\cos\theta^{t}}\tag{R}$$ Is this correct or are my calculations wrong? Here the user concludes that this is caused by a phase shift, is that the case here too?