Plasma model of superconducting crystals

Nadezhda P. Netesova

doi:10.1117/12.2230730

21 April 2016 Plasma model of superconducting crystals

Nadezhda P. Netesova

Proceedings Volume 9884, Nanophotonics VI; 98843R (2016) https://doi.org/10.1117/12.2230730
Event: SPIE Photonics Europe, 2016, Brussels, Belgium

Abstract

Within inharmonious plasma oscillation model the superconducting crystal AB is considered consisting of two subsystems 2AB=A2+B2. In high-temperature superconductors spontaneous division into two phases: superconducting and isolating was revealed. Phase separation was caused by plasma instability. It is obtained the transition superconducting phase temperature dependence T_c = F (q₁₂, q₁, q₂, V₁₂, V₁, V₂) on the isotopic substitution physical parameters: q – initial and component interaction parameters, V - volume in initial and component crystal lattices. The isotopic transition superconducting phase temperature displacement ΔT_c is associated with the change of the initial and component interaction and crystal lattice parameters. From the plasma mechanism of superconductivity follows superconducting crystals exist at room temperature.

Citation Download Citation

Nadezhda P. Netesova "Plasma model of superconducting crystals", Proc. SPIE 9884, Nanophotonics VI, 98843R (21 April 2016); https://doi.org/10.1117/12.2230730

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