Upper critical field of aligned Na_{x}(H_{3}O)_{z}CoO_{2}\cdot yH_{2}O superconductor by magnetization measurement
| dc.creator | Ren, Zhi | |
| dc.creator | Feng, Chunmu | |
| dc.creator | Xu, Zhu'an | |
| dc.creator | Fang, Minghu | |
| dc.creator | Cao, Guanghan | |
| dc.date | 2007-08-31 | |
| dc.date.accessioned | 2026-07-07T08:33:58Z | |
| dc.date.available | 2026-07-07T08:33:58Z | |
| dc.description | We present magnetization measurements for the upper critical field $H_{c2}$ on aligned Na$_{x}$(H$_{3}$O)$_{z}$CoO$_{2}\cdot y$H$_{2}$O superconductors with magnetic field parallel to CoO$_2$ layers. The temperature-dependent part of the normal-state magnetization $M(H,T)$ can be well scaled with Brillouin function, suggesting the existence of impurity moments. By subtracting the contribution of the magnetic impurity moments, a well defined onset of superconducting diamagnetism allows the in-field superconducting transition temperature $T_{c}$($H$) accurately determined. No superconducting transition was observed down to 1.9 K under an applied field of 8 Tesla. The result suggests that the $H^{\|ab}_{c2}(0)$ value is just within the Pauli paramagnetic limit, supporting spin-singlet superconductivity in the cobalt oxyhydrate superconductor. Additionally, the upward curvature near $T_{c}$ in the $H^{\|ab}_{c2}-T$ phase diagram was confirmed to be intrinsic. Possible origin of the anomaly was discussed. | |
| dc.description | 4 pages, 4 figures | |
| dc.identifier | https://arxiv.org/abs/0708.4256 | |
| dc.identifier | http://arxiv.org/abs/0708.4256 | |
| dc.identifier | PHYSICAL REVIEW B 76, 132501 (2007) | |
| dc.identifier | doi:10.1103/PhysRevB.76.132501 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/139275 | |
| dc.subject | Superconductivity | |
| dc.title | Upper critical field of aligned Na_{x}(H_{3}O)_{z}CoO_{2}\cdot yH_{2}O superconductor by magnetization measurement | |
| dc.type | text |