TY - JOUR
T1 - Anisotropic optical spectra of BaCo1−xNixS2
T2 - Effect of Ni substitution on the electronic structure of the Co1−xNixS
AU - Takenaka, K.
AU - Kashima, S.
AU - Osuka, A.
AU - Sugai, S.
AU - Yasui, Y.
AU - Shamoto, S.
AU - Sato, M.
N1 - Copyright:
Copyright 2017 Elsevier B.V., All rights reserved.
PY - 2001
Y1 - 2001
N2 - Polarized optical reflectivity is studied in single crystals of BaCo1−xNixS2 over a wide compositional range 0 ≤ x ≤ 0.28 from the antiferromagnetic insulating to the paramagnetic metallic phase. BaCoS2 is a charge-transfer-type Mott insulator with an anisotropic optical gap of about (or less than) 1 eV for E⊥c (parallel to the CoS plane) and 3.5 eV for Ec (perpendicular to the CoS plane). Ni substitution for Co has different effects on the in-plane σab(ω) and out-of-plane σc(ω) conductivities. As the Ni substitution proceeds, a Drude-like peak develops in σab(ω) above x=0.18, while a mid-infrared absorption band develops and a Drude-like peak is not confirmed in σc(ω). This indicates that the two-dimensionality is stronger than predicted from band calculations. However, the mid-infrared spectral weight induced in σc(ω) is much larger than that of high-Tc cuprates. This suggests that the charge carriers are not so tightly confined within the plane as in high-Tc cuprates. The looseness of the charge confinement probably originates from a strong interlayer-coupling effect via the 3d3z2−r2 orbital.
AB - Polarized optical reflectivity is studied in single crystals of BaCo1−xNixS2 over a wide compositional range 0 ≤ x ≤ 0.28 from the antiferromagnetic insulating to the paramagnetic metallic phase. BaCoS2 is a charge-transfer-type Mott insulator with an anisotropic optical gap of about (or less than) 1 eV for E⊥c (parallel to the CoS plane) and 3.5 eV for Ec (perpendicular to the CoS plane). Ni substitution for Co has different effects on the in-plane σab(ω) and out-of-plane σc(ω) conductivities. As the Ni substitution proceeds, a Drude-like peak develops in σab(ω) above x=0.18, while a mid-infrared absorption band develops and a Drude-like peak is not confirmed in σc(ω). This indicates that the two-dimensionality is stronger than predicted from band calculations. However, the mid-infrared spectral weight induced in σc(ω) is much larger than that of high-Tc cuprates. This suggests that the charge carriers are not so tightly confined within the plane as in high-Tc cuprates. The looseness of the charge confinement probably originates from a strong interlayer-coupling effect via the 3d3z2−r2 orbital.
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U2 - 10.1103/PhysRevB.63.115113
DO - 10.1103/PhysRevB.63.115113
M3 - Article
AN - SCOPUS:85038935148
SN - 1098-0121
VL - 63
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 11
ER -