Resumen
Measurements of the critical temperature Tc (n, P) as a function of Ce concentration n and pressure P ≤ 20 kbar are reported for the reentrant superconductors (La1 - nCen)Al2 and (La0.8Th0.2)1 - nCen. No evidencce was found for a third transition back to the superconducting state. Monte Carlo calculations including strong electron-phonon coupling may explain our experiments, although the effects of interimpurity interactions remain uncertain.
| Idioma original | English |
|---|---|
| Páginas (desde-hasta) | 500-502 |
| Número de páginas | 3 |
| Publicación | Physica B: Condensed Matter |
| Volumen | 199-200 |
| N.º | C |
| DOI | |
| Estado | Published - abr 2 1994 |
Nota bibliográfica
Funding Information:The authors wish to thank Profs. Mark Jarrell, A. Overhauser, John Ruvalds and Pedro Schlottmann for informative discussions. Research at the University of Kentucky was supported by Research Corporation under a Research Opportunity Award. Research at UCSD was supported by Basic Energy Sciences, US Department of Energy. Research at Tufts University was supported by the National Science Foundation Division of Materials Research.
Financiación
The authors wish to thank Profs. Mark Jarrell, A. Overhauser, John Ruvalds and Pedro Schlottmann for informative discussions. Research at the University of Kentucky was supported by Research Corporation under a Research Opportunity Award. Research at UCSD was supported by Basic Energy Sciences, US Department of Energy. Research at Tufts University was supported by the National Science Foundation Division of Materials Research.
| Financiadores |
|---|
| National Science Foundation Division of Materials Research |
| US Department of Energy |
| Research Corporation for Science Advancement |
| DOE Basic Energy Sciences |
ASJC Scopus subject areas
- Electronic, Optical and Magnetic Materials
- Condensed Matter Physics
- Electrical and Electronic Engineering
Huella
Profundice en los temas de investigación de 'Reentrant superconductivity at high pressures in (La1 - nCen)Al2 and (La0.8Th0.2)1 - nCen'. En conjunto forman una huella única.Citar esto
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