term to the left hand side, we then obtain q2e2iϕ =b 2 +b ∗ −2 ≃ 2ω2 f0(V2 + ∆V2) ϖ2 ,(88) where ϖ2 =ω 2 f0(1 + ∆ω2 2/ω2 f0)−4[ω−(1 +C f)ΩA]2,(89) which describes the nonlinearly corrected denominator of a Lorentzian
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