Fermi surface in BaNi$_2$P$_2$
| dc.creator | Terashima, Taichi | |
| dc.creator | Kimata, Motoi | |
| dc.creator | Satsukawa, Hidetaka | |
| dc.creator | Harada, Atsushi | |
| dc.creator | Hazama, Kaori | |
| dc.creator | Imai, Motoharu | |
| dc.creator | Uji, Shinya | |
| dc.creator | Kito, Hijiri | |
| dc.creator | Iyo, Akira | |
| dc.creator | Eisaki, Hiroshi | |
| dc.creator | Harima, Hisatomo | |
| dc.date | 2009-01-22 | |
| dc.date | 2009-02-06 | |
| dc.date.accessioned | 2026-07-07T12:50:13Z | |
| dc.date.available | 2026-07-07T12:50:13Z | |
| dc.description | We report measurements of the de Haas-van Alphen (dHvA) oscillation and a band structure calculation for the pnictide superconductor BaNi$_2$P$_2$, which is isostructural to BaFe$_2$As$_2$, the mother compound of the iron-pnictide high-$T_c$ superconductor (Ba$_{1-x}$K$_x$)Fe$_2$As$_2$. Six dHvA-frequency branches with frequencies up to $\sim$8 kT were observed, and they are in excellent agreement with results of the band-structure calculation. The determined Fermi surface is large, enclosing about one electron and hole per formula unit, and three-dimensional. This is in contrast to the small two-dimensional Fermi surface expected for the iron-pnictide high-$T_c$ superconductors. The mass enhancement is about two. | |
| dc.description | To appear in J. Phys. Soc. Jpn., Vol. 78, No. 3 | |
| dc.identifier | https://arxiv.org/abs/0901.3394 | |
| dc.identifier | http://arxiv.org/abs/0901.3394 | |
| dc.identifier | J. Phys. Soc. Jpn. 78 (2009) 033706 (4 pages) | |
| dc.identifier | doi:10.1143/JPSJ.78.033706 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/222619 | |
| dc.subject | Superconductivity | |
| dc.title | Fermi surface in BaNi$_2$P$_2$ | |
| dc.type | text |