Raman phonons of $α$-FeTe and Fe$_{1.03}$Se$_{0.3}$Te$_{0.7}$ single crystals
| dc.creator | Xia, Tian-Long | |
| dc.creator | Hou, D. | |
| dc.creator | Zhao, S. C. | |
| dc.creator | Zhang, A. M. | |
| dc.creator | Chen, G. F. | |
| dc.creator | Luo, J. L. | |
| dc.creator | Wang, N. L. | |
| dc.creator | Wei, J. H. | |
| dc.creator | Lu, Z. -Y. | |
| dc.creator | Zhang, Q. M. | |
| dc.date | 2008-11-14 | |
| dc.date | 2009-04-11 | |
| dc.date.accessioned | 2026-07-07T13:12:56Z | |
| dc.date.available | 2026-07-07T13:12:56Z | |
| dc.description | The polarized Raman scattering spectra of nonsuperconducting $α$-FeTe and of the newly discovered, As-free superconductor Fe$_{1.03}$Se$_{0.3}$Te$_{0.7}$ are measured at room temperature on single crystals. The phonon modes are assigned by combining symmetry analysis with first-principles calculations. In the parent compound $α$-FeTe, the A$_{1g}$ mode of the Te atom and the B$_{1g}$ mode of the Fe atom are observed clearly, while in superconducting Fe$_{1.03}$Se$_{0.3}$Te$_{0.7}$, only a softened Fe B$_{1g}$ mode can be seen. No electron-phonon coupling feature can be distinguished in the spectra of the two samples. By contrast, the spectra of the superconducting system show a slight enhancement below 300$cm^{-1}$, which may be of electronic origin. | |
| dc.description | 4 pages, 2 tables, 3 figures | |
| dc.identifier | https://arxiv.org/abs/0811.2350 | |
| dc.identifier | http://arxiv.org/abs/0811.2350 | |
| dc.identifier | Phys. Rev. B 79, 140510(R) (2009) | |
| dc.identifier | doi:10.1103/PhysRevB.79.140510 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/229730 | |
| dc.subject | Superconductivity | |
| dc.title | Raman phonons of $α$-FeTe and Fe$_{1.03}$Se$_{0.3}$Te$_{0.7}$ single crystals | |
| dc.type | text |