TY - JOUR
T1 - Split fermi surface properties of VSi2 without mirror planes in the chiral crystal structure
AU - Tsutsumi, Hiroki
AU - Miura, Yasunao
AU - Harima, Hisatomo
AU - Honda, Fuminori
AU - Onuki, Yoshichika
PY - 2013/9
Y1 - 2013/9
N2 - VSi2 is hexagonal in the crystal structure, and the basal plane stacks along the [0001] direction. Interestingly, each plane is rotated by 60° relative to the neighboring one. Therefore, there exist no mirror planes in this chiral structure. We carried out a de Haas-van Alphen (dHvA) experiment and clarified the Fermi surface properties. Each dHvA branch was found to be split into two branches on the basis of the antisymmetric spin-orbit interaction. The magnitude of the antisymmetric spin-orbit interaction in this chiral structure was determined for the first time to be 19 K for dHvA branch α (dHvA frequency F - 7:9 × 107 Oe and cyclotron mass m c* = 1:6 m0), 39 K for branch β (F = 4:1 × 107Oe and mc* = 3:4 m 0), and 110K for branch γ(F=1:8×107Oe and m c* = 23 m0). These dHvA branches correspond to the main Fermi surfaces, which are well explained by the results of the energy band calculations based on the full potential linear augmented plane wave (FLAPW) method. The present values are mainly due to the V-3d conduction electrons.
AB - VSi2 is hexagonal in the crystal structure, and the basal plane stacks along the [0001] direction. Interestingly, each plane is rotated by 60° relative to the neighboring one. Therefore, there exist no mirror planes in this chiral structure. We carried out a de Haas-van Alphen (dHvA) experiment and clarified the Fermi surface properties. Each dHvA branch was found to be split into two branches on the basis of the antisymmetric spin-orbit interaction. The magnitude of the antisymmetric spin-orbit interaction in this chiral structure was determined for the first time to be 19 K for dHvA branch α (dHvA frequency F - 7:9 × 107 Oe and cyclotron mass m c* = 1:6 m0), 39 K for branch β (F = 4:1 × 107Oe and mc* = 3:4 m 0), and 110K for branch γ(F=1:8×107Oe and m c* = 23 m0). These dHvA branches correspond to the main Fermi surfaces, which are well explained by the results of the energy band calculations based on the full potential linear augmented plane wave (FLAPW) method. The present values are mainly due to the V-3d conduction electrons.
UR - http://www.scopus.com/inward/record.url?scp=84883301856&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84883301856&partnerID=8YFLogxK
U2 - 10.7566/JPSJ.82.094604
DO - 10.7566/JPSJ.82.094604
M3 - Article
AN - SCOPUS:84883301856
SN - 0031-9015
VL - 82
JO - journal of the physical society of japan
JF - journal of the physical society of japan
IS - 9
M1 - 094604
ER -