“…(1), it is necessary to suppose the appearance of an additional oscillator in the low-frequency range; the best fit is achieved by introducing a low-frequency oscillator at 200 cm −1 . This value is reasonable, as an oscillator at about this frequency was observed in optical spectra of organic conductors of a similar crystal and band structure [11,12], although it was assigned to different effects. Figures 3 and 4 show that the calculated R(ω) and σ(ω) spectra for T = 10 K with Drude parameters of ω p = 2000, Γ = 400, ε ∞ = 3, and two Lorentz oscillators (l = 1, 2) with parameters ω T1 = 4000, ω L1 = 5300, γ L1 = 4400, ω T2 = 200, ω L2 = 5200, γ T2 = 140 cm −1 are in a good agreement with the experimental spectra.…”