Hybrid gap structure in the heavy-fermion superconductor CeIrIn$_5$
| dc.creator | Shakeripour, H. | |
| dc.creator | Tanatar, M. A. | |
| dc.creator | Li, S. Y. | |
| dc.creator | Taillefer, Louis | |
| dc.creator | Petrovic, C. | |
| dc.date | 2006-10-02 | |
| dc.date | 2006-10-05 | |
| dc.date.accessioned | 2026-07-07T09:18:19Z | |
| dc.date.available | 2026-07-07T09:18:19Z | |
| dc.description | The thermal conductivity $κ$ of the heavy-fermion superconductor CeIrIn$_5$ was measured as a function of temperature down to $T_c$/8, for current directions perpendicular ($J \parallel a$) and parallel ($J \parallel c$) to the tetragonal c axis. For $J \parallel a$, a sizable residual linear term $κ_0 / T$ is observed, as previously, which confirms the presence of line nodes in the superconducting gap. For $J \parallel c$, on the other hand, $κ/ T \to 0$ as $T \to 0$. The resulting precipitous decline in the anisotropy ratio $κ_c / κ_a$ at low temperature rules out a gap structure with line nodes running along the c-axis, such as the d-wave state favoured for CeCoIn$_5$, and instead points to a hybrid gap of $E_g$ symmetry. It therefore appears that two distinct superconducting states are realized in the Ce$M$In$_5$ family. | |
| dc.description | 4 pages, 3 figures, submitted to Phys. Rev. Lett | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0610052 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0610052 | |
| dc.identifier | Phys. Rev. Lett. 99, 187004 (2007) | |
| dc.identifier | doi:10.1103/PhysRevLett.99.187004 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/153981 | |
| dc.subject | Strongly Correlated Electrons | |
| dc.subject | Superconductivity | |
| dc.title | Hybrid gap structure in the heavy-fermion superconductor CeIrIn$_5$ | |
| dc.type | text |