Anisotropy and Penetration Depth of MgB$_{2}$ from ${}^{11}$B NMR
| dc.creator | Chen, Bo | |
| dc.creator | Sengupta, Pratim | |
| dc.creator | Halperin, W. P. | |
| dc.creator | Sigmund, E. E. | |
| dc.creator | Mitrovic, V. F. | |
| dc.creator | Lee, M. H. | |
| dc.creator | Kang, K. H. | |
| dc.creator | Mean, B. J. | |
| dc.creator | Kim, J. Y. | |
| dc.creator | Cho, B. K. | |
| dc.date | 2006-11-17 | |
| dc.date | 2007-01-24 | |
| dc.date.accessioned | 2026-07-07T07:42:34Z | |
| dc.date.available | 2026-07-07T07:42:34Z | |
| dc.description | The ${}^{11}$B NMR spectra in polycrystalline MgB$_2$ were measured for several magnetic fields (1.97 T and 3.15 T) as a function of temperature from 5 K to 40 K. The composite spectra in the superconducting state can be understood in terms of anisotropy of the upper critical field, $γ_{H}$, which is determined to be 5.4 at low temperature. Using Brandt's algorithm\cite{Brandt} the full spectrum, including satellites, was simulated for the temperature 8 K and a magnetic field of 1.97 T. The penetration depth $λ$ was determined to be $1,152\pm50$ Å, and the anisotropy of the penetration depth, $γ_λ$, was estimated to be close to one at low temperature. Therefore, our findings establish that there are two different anisotropies for upper critical field and penetration depth at low temperatures. | |
| dc.description | 10 pages, 7 figures | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0611473 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0611473 | |
| dc.identifier | New Journal of Physics,Vol. 8, P. 274, 2006 | |
| dc.identifier | doi:10.1088/1367-2630/8/11/274 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/122488 | |
| dc.subject | Superconductivity | |
| dc.subject | Strongly Correlated Electrons | |
| dc.title | Anisotropy and Penetration Depth of MgB$_{2}$ from ${}^{11}$B NMR | |
| dc.type | text |