“…Here, ⌬ 0 Ϸ 50-75 meV = 600-900 K, 0 Ϸ 1.7 Thz, ប 0 = T 0 Ϸ 7 meVϷ 80 K, T c = 180 K, u =2ϫ 10 4 m / s, v F =2ϫ 10 5 m / s; then  Ϸ 2.5. For NbSe 3 , the data on phonon modes are contradictory, 35 but can be estimated from the bare frequency as T 0 ഛ 8 meV Ϸ 90 K; then we expect, for the second CDW, a similar value  = v F / 4u = ⌬ 0 / 2ប 0 Ϸ 3. These values of the exponent  are quite high to provide a fast fall of the current within the pseudogap, in qualitative accordance with the experiment, but the price is that the temperature limitations pool the theory to the 3D ordered phase, where more studies of the combined effects of the temperature and the long range order are necessary to be developed, in particular, the prefactors need to be calculated.…”