“…Because of this, the mean-field theory was not able to explain the reason of other second-order phase transitions, e.g., superfluidity helium, liquid crystals, etc. Theoretically the range of temperature around T c and within which the fluctuations are effective, for pure SC, is ξ~ d. In this theory, the GL free energy functional for the order parameter and with modified temperature dependence of the coefficients was taken as the effective Hamiltonian [7,8]. Several works, therefore, stressed on the possibility of using the same modified GL theory for the case of HTS [9][10][11][12].…”