Numéro |
J. Phys. IV France
Volume 12, Numéro 9, November 2002
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Page(s) | 227 - 230 | |
DOI | https://doi.org/10.1051/jp4:20020400 |
J. Phys. IV France 12 (2002) Pr9-227
DOI: 10.1051/jp4:20020400
Polarization catastrophe in doped cuprates and metal-ammonia solutions. Metal-to-superconductor transition versus phase separation
P. Quemerais1, J.-L. Raimbault2 and S. Fratini11 Laboratoire d'Etudes des Propriétés Electroniques des Solides, CNRS, avenue des Martyrs, BP. 166, 38042 Grenoble cedex 9, France
2 Laboratoire Physique et Technologie des Plasmas, Ecole Polytechnique, 91128 Palaiseau cedex, France
Abstract
On doping polar dielectrics, such as cuprates (solid) or amonia (liquid), the polarization induces the
formation of polarons or solvated electrons. However, the exact role of such entities in the metal-to-insulator
transition (MIT) which occurs at some critical densities still remains unclear. We think that their formation
together with their long-range Coulomb interactions are responsable for a polarization catastrophe leading to the
MIT. Moreover, the accompanishing phenomena is the occurence of a negative sign of the static dielectric constant,
which could yield either an insulator-to-superconductor transition in cuprates, either a phase separation in
metal-ammonia solutions. The difference of hehavior possibly could come from the nature of the counter ions of the
doping charges, which are essentially frozen in oxides, while they remain in a liquid state in metal-ammonia
system.
© EDP Sciences 2002