Metal-insulator (fermion-boson)-crossover origin of pseudogap phase of cuprates I: anomalous heat conductivity, insulator resistivity boundary, nonlinear entropy
B. Abdullaev, C.-H. Park, K.-S. Park, and I. -J. Kang

TL;DR
This paper explains the pseudogap phase in cuprates as a crossover from bosonic to fermionic behavior, linking various anomalous phenomena to a Coulomb two-liquid model involving single bosons and fermions.
Contribution
It introduces a Coulomb two-liquid model to unify the understanding of the metal-insulator crossover and related anomalies in cuprates.
Findings
MIC is a crossover from bosonic insulator to fermionic metal.
The model explains heat conductivity downturn and resistivity boundary.
All phenomena are derived from Coulomb two-liquid interactions.
Abstract
Among all experimental observations of cuprate physics, the metal-insulator-crossover (MIC), seen in the pseudogap (PG) region of the temperature-doping phase diagram of copper-oxides under a strong magnetic field, when the superconductivity is suppressed, is most likely the most intriguing one. Since it was expected that the PG-normal state for these materials, as for conventional superconductors, is conducting. This MIC, revealed in such phenomena as heat conductivity downturn, anomalous Lorentz ratio, insulator resistivity boundary, nonlinear entropy, resistivity temperature upturn, insulating ground state, nematicity- and stripe-phases and Fermi pockets, unambiguously indicates on the insulating normal state, from which the high-temperature superconductivity (HTS) appears. In the present work (article I), we discuss the MIC phenomena mentioned in the title of article. The second…
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