Abstract

AbstractA bisoliton model of high‐temperature superconductivity is formulated in terms of one‐particle states. The transition to a superconducting state is shown to be accompanied by the energy spectrum rearrangement. The dielectric gap typical for BCS theory is appeared. Its dependence on concentration of carriers is of nonmonotonous character. The conditions for realization of a bisoliton mechanism of superconductivity are considered.

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