Nano- and Microstructures with Equal Zero Ohmic Losses in a Spontaneously Polarized State

Abstract

Structures with zero ohmic resistance for a constant and sinusoidal electric current are obtained. As in the case of superconductivity, this effect is due to the exchange-correlation interaction of electrons, but for a different reason: polarization of the structure by an electric field, and not Cooper-pair polarization of the lattice.

Substances with zero static permittivity

“…The capacitance of the powder layer has a negative value ( Z = – U m / J m ) and does not depend on the frequency of the sinusoidal field. The effect arises under the condition that the powder layer is placed between the dielectric plates and the current through the powder layer is zero 10 , 11 .…”

“…With a change in the gas pressure, the values of J m , U m , and the dependence J ( t )[ U ( t )] change due to the change in the state of the surface of powder micro particles, on which depends the concentration of free electrons (according to measurements conducted by different methods). The limiting maximum value of J m at Z < 0 corresponds to the linear dependence of J ( t )[ U ( t )] 10 , 11 .…”

Phenomena in Polarized Disperse Systems Caused by Exchange-Correlation Interaction between Particles

“…Owing to this, all chains of the periodic structure reside in self-consistent states and thereby form a unified system. In experiments with the polarization of a finely dispersed semiconductor by a sine-wave field, its layer was placed between two dielectric plates, thus enabling the condition ε < 0 to hold [9] [10].…”

“…is the static dielectric permittivity [8] [9]. For example, this condition has been used to explain the zero ohmic loss for a direct current in Al 2 O 3 and NiO powders containing donor centers on the nanoparticle surfaces in the form of interstitial hydrogen atoms [8].…”

“…For example, this condition has been used to explain the zero ohmic loss for a direct current in Al 2 O 3 and NiO powders containing donor centers on the nanoparticle surfaces in the form of interstitial hydrogen atoms [8]. The zero ohmic loss has also been observed for a sine-wave current in finely dispersed compounds KMnO 4 [8] [10] and KNaC 4 H 4 O 6 •4Н 2 О [9] placed in molecular hydrogen and vacuum, respectively. In the case of the finely dispersed dielectrics KMnO 4 , Pb(NO 3 ) 2 and CsNO 3 with donor centers on the particle surfaces, there is observed spontaneous emergence of a macroscopic electric field [11] [12] [13].…”