TY - JOUR
T1 - 195Pt-NMR evidence for opening of partial charge-density-wave gap in layered LAPt2Si2 with CaBe2Ge2 structure
AU - Aoyama, Taisuke
AU - Kubo, Tetsuro
AU - Matsuno, Haruki
AU - Kotegawa, Hisashi
AU - Tou, Hideki
AU - Mitsuda, Akihiro
AU - Nagano, Yutaro
AU - Araoka, Nobutaka
AU - Wada, Hirohumi
AU - Yamada, Yuh
N1 - Funding Information:
H.T. would like to thank Dr. I. Hase for valuable discussion and comments. This work was supported by JPSK KAKENHI Grant numbers 15H05885 (J-Physics), 15H05882 (J-Physics), 26400359, 15H05745, and 15H03689.
PY - 2018
Y1 - 2018
N2 - We carried out 195Pt-NMR measurements for a single-crystal LaPt2Si2, which is expected to show the coexistence of a superconducting state and a charge density wave (CDW) state. LaPt2Si2 crystallizes to a quasi-two-dimensional CaBe2Ge2-type crystal structure consisting of two types of Pt2Si2 layers: Pt1 and Pt2. From both the Knight shift, 195K, and the NMR relaxation rate divided by the temperature, 1=T1T, the electronic density of states at the Fermi level, N(εF), for only the Pt1 site decreases below the CDW transition temperature T+ = 112 K, whereas N(εF) for the Pt2 site does not change. These results suggest that the CDW occurs only in the Pt1 layers below 112 K. Furthermore, above T+, we also found that both195K and 1=T1T decrease upon cooling only for the Pt1 site. The temperature dependences of K and 1=T1T for the Pt1 site can be explained by assuming a two bands model consisting of a wide band and a narrow band near the Fermi level. The CDW transition is expected to occur only in the narrow band of the Pt1 site, while the wide band of the Pt1-site does not contribute to the CDW transition. The present result strongly indicates that the CDW gap opens partially at the Fermi surface.
AB - We carried out 195Pt-NMR measurements for a single-crystal LaPt2Si2, which is expected to show the coexistence of a superconducting state and a charge density wave (CDW) state. LaPt2Si2 crystallizes to a quasi-two-dimensional CaBe2Ge2-type crystal structure consisting of two types of Pt2Si2 layers: Pt1 and Pt2. From both the Knight shift, 195K, and the NMR relaxation rate divided by the temperature, 1=T1T, the electronic density of states at the Fermi level, N(εF), for only the Pt1 site decreases below the CDW transition temperature T+ = 112 K, whereas N(εF) for the Pt2 site does not change. These results suggest that the CDW occurs only in the Pt1 layers below 112 K. Furthermore, above T+, we also found that both195K and 1=T1T decrease upon cooling only for the Pt1 site. The temperature dependences of K and 1=T1T for the Pt1 site can be explained by assuming a two bands model consisting of a wide band and a narrow band near the Fermi level. The CDW transition is expected to occur only in the narrow band of the Pt1 site, while the wide band of the Pt1-site does not contribute to the CDW transition. The present result strongly indicates that the CDW gap opens partially at the Fermi surface.
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U2 - 10.7566/JPSJ.87.124713
DO - 10.7566/JPSJ.87.124713
M3 - Article
AN - SCOPUS:85058964768
SN - 0031-9015
VL - 87
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 12
M1 - 124713
ER -