Result of the LHCD efficiency studyThe most efficient method for sustaining the quasisteady plasma current by means of lower hybrid (LH) waves can be implemented only at relatively low plasma densities not exceeding a certain density limit, n DL . The existence of the density limit for LH current drive (LHCD) was attributed to various mechanisms: linear absorption by ions, which increases as the density tends to the resonance LH value; collision losses; scattering by drift turbulence; parametric instabilities; etc. The density limit effect has been studied and discussed for several past decades; however, it has not received comprehensive physical explanation [1].In the present work the main attention is paid to investigation of current drive by lower hybrid waves on the FT-2 (R = 0.55 m, a = 0.08 m, B T ≤ 3 T, I p = 19÷40 kA, f 0 = 920 МHz) tokamak. The results of experiments carried out at the FT-2 tokamak allow us to conclude that the most probable reason for LHCD termination in both hydrogen and deuterium plasmas at a relatively low plasma current of I = 22 kA and, accordingly, a low electron temperature is an additional reduction in T e at the periphery of the plasma column during the LH pulse [2]. This results in a lower threshold for the parametric decay (~T e /n e ) of the pumping wave. The parametric decay satellites, the frequencies of which are down-shifted, (f sat = f 0 -kf Ci ), (k = 1, 2, 3…), are slowed down more than the pumping wave. Therefore, the plasma density, at which linear conversion of slowed down satellite waves occurs, is lower than that for the pumping wave; hence, the LH wave after parametric decay can be absorbed by ions even at the plasma periphery, without penetrating into the plasma column. At a higher plasma current (I OH = 32 kA) and higher electron temperature (T e0 = 600 eV), the density at which the LHCD in hydrogen plasma terminates is close to the resonance value (n DL H ≈ n LH H ≈ 3.5 10 19 m -3 ). After the plasma density reaches this value, the interaction of the LH wave with electrons is replaced with direct absorption by ions, when ω 0 ~ ω pl, i . As a result of the experimental study of the influence of the plasma isotopic composition on the LHCD efficiency, it is established that the efficiency η CD D in deuterium plasma on FT-2 is higher than in hydrogen plasma η CD H [2]. As it is seen from Fig. 1 , takes place proved to be higher than n DL D . There is an appreciable gap between the values of n DL D and FN D . Apparently, the main reason for LHCD termination in this case is the parametric decay of the pumping wave. The experimental results confirm that parametric processes intensify with increasing density during the RF pulse (see Fig. 3 in [2]). Nevertheless, we cannot exclude the influence of a substantial slowing down (up to ≈||N 10) of the pumping wave as it propagates into the plasma column. The experimental evidence of influence of isotopic effect on characteristics of the ion heating observed at rise and after LHCD termination, which demo...