“…The mechanism can be summarized by saying that reasonably high values of the electric field, comparable to the so-called critical field E c (T ), can accelerate the fluctuating paired carriers to the depairing current, and thus, suppress the lifetime of the fluctuations, leading to deviation from Ohm's law. The non-Ohmic behavior of the fluctuation paraconductivity in sufficiently strong electric fields was studied about three decades ago in connection with the low temperature superconductors both theoretically, for the isotropic case [6,7,8], and experimentally, on thin aluminum films [9,10], with a good agreement between experiment and theory. The issue of the non-Ohmic fluctuation conductivity for a layered superconductor, a situation very much resembling the crystal structure in the HTS, has been addressed theoretically a decade ago starting from a microscopic approach [11], and more recently, in the frame of the time-dependent Ginzburg-Landau (TDGL) theory, in the Gaussian approximation [12], and in the self-consistent Hartree approach [13].…”