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φ, bv = b cos θ , andgk = g sin θ cos φ with b and g the magnitudes of the Voigt andFaraday effects. ... These can be calculatedfrom the Fresnel equations [23],. tan ϕh = 2 cos ϑi.

VS / hz sin 2uME (6). VA / hx sin uME sin 2uME hy cos uME sin 2uME (7). ... The. direction of the current is represented by j. b, Coefficients of the cos uM2E and sin uM2E fits to the angle dependence of the out-of-plane SOT field for

1ρL. ρav= CI cos 2(ψ θ) CIC cos(2ψ 2θ) CC cos 4ψ (4). ... 1uniL = CsIU cos 2θ C. sU cos 2ψ,. ()1uniT = CsIU sin 2θ C.

Both symmetric and antisymmetriccomponents follow a sin 2θ cos θ angle dependence [Fig. ... 2 1μ0Meff. μ0Hrot μ0Hexch cos(θ θexch). μ0HU cos[2(θ θU )]. (E6)For the given frequency, larger Meff leads to a smaller Hrot andvice versa.