Unconventional superconductivity in Na$_{0.35}$CoO$_{2}\cdot$1.3D$_{2}$O and proximity to a magnetically ordered phase
| dc.creator | Uemura, Y. J. | |
| dc.creator | Russo, P. L. | |
| dc.creator | Savici, A. T. | |
| dc.creator | Wiebe, C. R. | |
| dc.creator | MacDougall, G. J. | |
| dc.creator | Luke, G. M. | |
| dc.creator | Mochizuki, M. | |
| dc.creator | Yanase, Y. | |
| dc.creator | Ogata, M. | |
| dc.creator | Foo, M. L. | |
| dc.creator | Cava, R. J. | |
| dc.date | 2004-03-01 | |
| dc.date.accessioned | 2026-07-07T02:56:44Z | |
| dc.date.available | 2026-07-07T02:56:44Z | |
| dc.description | Muon spin relaxation ($μ$SR) measurements on the new layered cobalt oxide superconductor Na$_{0.35}$CoO$_{2}\cdot$1.3H$_{2}$O and its parent, non-superconducting compounds, have revealed unconventional nature of superconductivity through: (1) a small superfluid energy which implies a surprisingly high effective mass of the charge carriers, approximately 100 times the bare electron mass; (2) the superconducting transition temperature $T_{c}$ scaling with the superfluid energy following the correlations found in high-$T_{c}$ cuprate and some other two-dimensional superconductors; (3) an anisotropic pairing without broken time-reversal symmetry; and (4) the proximity of a magnetically ordered insulating phase at Na$_{0.5}$CoO$_{2}$ below $T_{N}$ = 53 K. | |
| dc.description | 6 pages 4 figures: Contact Y.J. Uemura, E-mail: tomo@lorentz.phys.columbia.edu | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0403031 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0403031 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/23440 | |
| dc.subject | Superconductivity | |
| dc.subject | Strongly Correlated Electrons | |
| dc.title | Unconventional superconductivity in Na$_{0.35}$CoO$_{2}\cdot$1.3D$_{2}$O and proximity to a magnetically ordered phase | |
| dc.type | text |