ARPES on Na$_{0.6}$CoO$_{2}$: Fermi surface, extended flat dispersion, and unusual band splitting
| dc.creator | Yang, H. -B. | |
| dc.creator | Wang, S. -C. | |
| dc.creator | Sekharan, A. K. P. | |
| dc.creator | Matsui, H. | |
| dc.creator | Souma, S. | |
| dc.creator | Sato, T. | |
| dc.creator | Takahashi, T. | |
| dc.creator | Takeuchi, T. | |
| dc.creator | Campuzano, J. C. | |
| dc.creator | Jin, R. | |
| dc.creator | Sales, B. C. | |
| dc.creator | Mandrus, D. | |
| dc.creator | Wang, Z. | |
| dc.creator | Ding, H. | |
| dc.date | 2003-10-22 | |
| dc.date.accessioned | 2026-07-07T02:54:21Z | |
| dc.date.available | 2026-07-07T02:54:21Z | |
| dc.description | The electronic structure of single crystals Na$_{0.6}$CoO$_2$, which are closely related to the superconducting Na$_{0.3}$CoO$_2$.$y$H$_2$O ($T_c \sim 5K$), is studied by angle-resolved photoelectron spectroscopy. While the measured Fermi surface is found to be consistent with the prediction of a local density band theory, the energy dispersion is highly renormalized, with an anisotropy along the two principle axes ($Γ$-$K$, $Γ$-$M$). Our ARPES result also indicates that an extended flat band is formed slightly above $E_F$ along $Γ$-$K$. In addition, an unusual band splitting is observed in the vicinity of the Fermi surface along the $Γ$-$M$ direction, which differs from the predicted bilayer splitting. | |
| dc.description | 4 figures | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0310532 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0310532 | |
| dc.identifier | Phys. Rev. Lett. 92, 246403 (2004) | |
| dc.identifier | doi:10.1103/PhysRevLett.92.246403 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/22514 | |
| dc.subject | Superconductivity | |
| dc.subject | Strongly Correlated Electrons | |
| dc.title | ARPES on Na$_{0.6}$CoO$_{2}$: Fermi surface, extended flat dispersion, and unusual band splitting | |
| dc.type | text |