TY - JOUR
T1 - Fermi surface in KFe2As2 determined via de Haas-van Alphen oscillation measurements
AU - Terashima, Taichi
AU - Kurita, Nobuyuki
AU - Kimata, Motoi
AU - Tomita, Megumi
AU - Tsuchiya, Satoshi
AU - Imai, Motoharu
AU - Sato, Akira
AU - Kihou, Kunihiro
AU - Lee, Chul Ho
AU - Kito, Hijiri
AU - Eisaki, Hiroshi
AU - Iyo, Akira
AU - Saito, Taku
AU - Fukazawa, Hideto
AU - Kohori, Yoh
AU - Harima, Hisatomo
AU - Uji, Shinya
PY - 2013/6/27
Y1 - 2013/6/27
N2 - We have completely determined the Fermi surface in KFe2As 2 via de Haas-van Alphen (dHvA) measurements. Fundamental frequencies ε, α, ζ, and β are observed in KFe2As 2. The first one is attributed to a hole cylinder near the X point of the Brillouin zone while the others to hole cylinders at the Γ point. We also observe magnetic breakdown frequencies between α and ζ and suggest a plausible explanation for them. The experimental frequencies show deviations from frequencies predicted by band-structure calculations. Large effective masses up to 19 me for Bâ̂¥c have been found, me being the free-electron mass. The carrier number and Sommerfeld coefficient of the specific heat are estimated to be 1.01-1.03 holes per formula unit and 82-94 mJmol-1 K-2, respectively, which are consistent with the chemical stoichiometry and a direct measure of 93 mJmol-1 K-2. The Sommerfeld coefficient is about nine times enhanced over a band value, suggesting the importance of low-energy spin and/or orbital fluctuations, and places KFe2As2 among strongly correlated metals. We have also performed dHvA measurements on Ba 0.07K0.93Fe2As2 and have observed the α and β frequencies.
AB - We have completely determined the Fermi surface in KFe2As 2 via de Haas-van Alphen (dHvA) measurements. Fundamental frequencies ε, α, ζ, and β are observed in KFe2As 2. The first one is attributed to a hole cylinder near the X point of the Brillouin zone while the others to hole cylinders at the Γ point. We also observe magnetic breakdown frequencies between α and ζ and suggest a plausible explanation for them. The experimental frequencies show deviations from frequencies predicted by band-structure calculations. Large effective masses up to 19 me for Bâ̂¥c have been found, me being the free-electron mass. The carrier number and Sommerfeld coefficient of the specific heat are estimated to be 1.01-1.03 holes per formula unit and 82-94 mJmol-1 K-2, respectively, which are consistent with the chemical stoichiometry and a direct measure of 93 mJmol-1 K-2. The Sommerfeld coefficient is about nine times enhanced over a band value, suggesting the importance of low-energy spin and/or orbital fluctuations, and places KFe2As2 among strongly correlated metals. We have also performed dHvA measurements on Ba 0.07K0.93Fe2As2 and have observed the α and β frequencies.
UR - http://www.scopus.com/inward/record.url?scp=84879769685&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84879769685&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.87.224512
DO - 10.1103/PhysRevB.87.224512
M3 - Article
AN - SCOPUS:84879769685
SN - 1098-0121
VL - 87
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 22
M1 - 224512
ER -