“…The systems of Eqs. (12,13) can be simplified by employing the linear approximation for ∆ 0,−1 (ω, θ) = δ 0,−1 (θ)[ω − ω 0,−1 (θ)] and constant approximation for the other parameters κ(ω, θ) = κ(ω ± −1 , θ), Γ 0 (ω, θ) = Γ 0 (ω ± 0 , θ). This approximation well describes reflection in the spectral range close to the resonance.…”