TY - JOUR
T1 - Crystal Structure and Thermoelectric Properties of the Incommensurate Chimney–Ladder Compound VGeγ (γ ~1.82)
AU - Hamada, Haruki
AU - Kikuchi, Yuta
AU - Hayashi, Kei
AU - Miyazaki, Yuzuru
PY - 2016/3/1
Y1 - 2016/3/1
N2 - A single-phase sample of a Nowotny chimney–ladder phase known as V17Ge31 has been prepared and its modulated crystal structure has been determined by means of a (3+1)-dimensional superspace approach. As in the case of higher manganese silicides (HMSs) MnSiγ, the compound consists of two tetragonal subsystems of [V] and [Ge] with an irrational c-axis ratio (Formula presented.) = (Formula presented.) / (Formula presented.) 1.82, and hence the structure formula is represented as VGeγ. As expected from the valence electron count estimated from the refined γ, the present germanide exhibits a metallic behavior with the electrical conductivity σ = 6.25 × 103 S/cm and the Seebeck coefficient S = 10.2 μV/K at 900 K. The resulting thermoelectric power factor of (Formula presented.) = 6.56 × 10-5 W/mK2 and the dimensionless figure-of-merit, ZT, = 3.7 × 10-3 at 900 K demonstrate that the germanide is not a promising thermoelectric material. However, as the determined lattice thermal conductivity is comparable to that of HMSs, thermoelectric properties can be maximized through the partial substitution of V with group 6–8 elements to decrease hole carrier concentration.
AB - A single-phase sample of a Nowotny chimney–ladder phase known as V17Ge31 has been prepared and its modulated crystal structure has been determined by means of a (3+1)-dimensional superspace approach. As in the case of higher manganese silicides (HMSs) MnSiγ, the compound consists of two tetragonal subsystems of [V] and [Ge] with an irrational c-axis ratio (Formula presented.) = (Formula presented.) / (Formula presented.) 1.82, and hence the structure formula is represented as VGeγ. As expected from the valence electron count estimated from the refined γ, the present germanide exhibits a metallic behavior with the electrical conductivity σ = 6.25 × 103 S/cm and the Seebeck coefficient S = 10.2 μV/K at 900 K. The resulting thermoelectric power factor of (Formula presented.) = 6.56 × 10-5 W/mK2 and the dimensionless figure-of-merit, ZT, = 3.7 × 10-3 at 900 K demonstrate that the germanide is not a promising thermoelectric material. However, as the determined lattice thermal conductivity is comparable to that of HMSs, thermoelectric properties can be maximized through the partial substitution of V with group 6–8 elements to decrease hole carrier concentration.
KW - Nowotny chimney–ladder phase
KW - VGe
KW - Vanadium germanide
KW - modulated structure
KW - thermoelectric properties
KW - valence electron counts
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U2 - 10.1007/s11664-015-4036-6
DO - 10.1007/s11664-015-4036-6
M3 - Article
AN - SCOPUS:84959451071
VL - 45
SP - 1365
EP - 1368
JO - Journal of Electronic Materials
JF - Journal of Electronic Materials
SN - 0361-5235
IS - 3
ER -