Abstract
In the intermetallic SmNiC 2, the ferromagnetic metallic state competes with the charge-density-wave state. We can switch the charge-density-wave state by applying a magnetic field that is conjugated to the magnetization of the order parameter in the ferromagnetic state, and show the giant negative magnetoresistance. Under the applied magnetic field, the resistivity becomes one order of magnitude smaller than the zero-field resistivity.
| Original language | English |
|---|---|
| Article number | 092402 |
| Journal | Physical Review B - Condensed Matter and Materials Physics |
| Volume | 85 |
| Issue number | 9 |
| DOIs | |
| Publication status | Published - Mar 20 2012 |
Fingerprint
ASJC Scopus subject areas
- Condensed Matter Physics
- Electronic, Optical and Magnetic Materials
Cite this
Magnetic field switching of the charge-density-wave state in the lanthanide intermetallic SmNiC 2 . / Hanasaki, N.; Nogami, Yoshio; Kakinuma, M.; Shimomura, S.; Kosaka, M.; Onodera, H.
In: Physical Review B - Condensed Matter and Materials Physics, Vol. 85, No. 9, 092402, 20.03.2012.Research output: Contribution to journal › Article
}
TY - JOUR
T1 - Magnetic field switching of the charge-density-wave state in the lanthanide intermetallic SmNiC 2
AU - Hanasaki, N.
AU - Nogami, Yoshio
AU - Kakinuma, M.
AU - Shimomura, S.
AU - Kosaka, M.
AU - Onodera, H.
PY - 2012/3/20
Y1 - 2012/3/20
N2 - In the intermetallic SmNiC 2, the ferromagnetic metallic state competes with the charge-density-wave state. We can switch the charge-density-wave state by applying a magnetic field that is conjugated to the magnetization of the order parameter in the ferromagnetic state, and show the giant negative magnetoresistance. Under the applied magnetic field, the resistivity becomes one order of magnitude smaller than the zero-field resistivity.
AB - In the intermetallic SmNiC 2, the ferromagnetic metallic state competes with the charge-density-wave state. We can switch the charge-density-wave state by applying a magnetic field that is conjugated to the magnetization of the order parameter in the ferromagnetic state, and show the giant negative magnetoresistance. Under the applied magnetic field, the resistivity becomes one order of magnitude smaller than the zero-field resistivity.
UR - http://www.scopus.com/inward/record.url?scp=84859032194&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84859032194&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.85.092402
DO - 10.1103/PhysRevB.85.092402
M3 - Article
AN - SCOPUS:84859032194
VL - 85
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
SN - 1098-0121
IS - 9
M1 - 092402
ER -