“…To solve the problem of taking into account the shielding effect, we use the first-order perturbation theory in the framework of the screening Lindhardt and expand on the potential of wave function where V is the volume studied structure generally and is the potential. By definition, the Fourier component k � −k is determined via the integral of the form (11) In linear approximation, induced charge is given by [9] where f k is the Fermi-Dirac equilibrium function. We introduce the replacement: q =k � −k,Q = (k � +k)∕2− which are the difference and the sum of the pulses, respectively.…”