TY - JOUR
T1 - Crystal growth, thermoelectric properties, and electronic structure of AgBi 3S 5 and AgSb xBi 3-xS 5 (x = 0.3)
AU - Kim, Jun Ho
AU - Chung, Duck Young
AU - Bilc, Daniel
AU - Loo, Sim
AU - Short, Jarrod
AU - Mahanti, Subhendra D.
AU - Hogan, Tim
AU - Kanatzidis, Mercouri G.
PY - 2005/7/12
Y1 - 2005/7/12
N2 - The compound AgBi 3S 5 (I) (synthetic pavonite) and its solid solution AgSb xBi 3-xS 5 (x = 0.3) (II) were prepared by direct combination of elemental Ag, Bi, Sb, and S. They crystallize in the monoclinic space group C2/m with a = 13.345(3) Å,b = 4.0416(8) Å, c = 16.439(3) Å, and β= 94.158(3)° for I and a = 13.302(4) Å, b = 4.0381(11) Å, c = 16.388(5) Å, and β= 94.347(5)° for II. The Bridgman technique was used to grow bulk crystals of these materials. The crystal structure refinements, physicochemical properties, and thermoelectric properties of these materials are presented. The thermoelectric power for AgBi 3S 5 and AgSb 0.3Bi 2.7S 5 showed -64 and -98 μV/K, respectively, with room-temperature electrical conductivity of 489 and 260 S/cm. The thermal conductivity for both compounds at room temperature was measured to be very low at ∼1 W/m·K, respectively. Electronic band structure calculations for AgBi 3S 5 suggest the importance of silver d-states to the charge transport and also indicate the presence of an indirect energy gap.
AB - The compound AgBi 3S 5 (I) (synthetic pavonite) and its solid solution AgSb xBi 3-xS 5 (x = 0.3) (II) were prepared by direct combination of elemental Ag, Bi, Sb, and S. They crystallize in the monoclinic space group C2/m with a = 13.345(3) Å,b = 4.0416(8) Å, c = 16.439(3) Å, and β= 94.158(3)° for I and a = 13.302(4) Å, b = 4.0381(11) Å, c = 16.388(5) Å, and β= 94.347(5)° for II. The Bridgman technique was used to grow bulk crystals of these materials. The crystal structure refinements, physicochemical properties, and thermoelectric properties of these materials are presented. The thermoelectric power for AgBi 3S 5 and AgSb 0.3Bi 2.7S 5 showed -64 and -98 μV/K, respectively, with room-temperature electrical conductivity of 489 and 260 S/cm. The thermal conductivity for both compounds at room temperature was measured to be very low at ∼1 W/m·K, respectively. Electronic band structure calculations for AgBi 3S 5 suggest the importance of silver d-states to the charge transport and also indicate the presence of an indirect energy gap.
UR - http://www.scopus.com/inward/record.url?scp=22944445151&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=22944445151&partnerID=8YFLogxK
U2 - 10.1021/cm0502931
DO - 10.1021/cm0502931
M3 - Article
AN - SCOPUS:22944445151
SN - 0897-4756
VL - 17
SP - 3606
EP - 3614
JO - Chemistry of Materials
JF - Chemistry of Materials
IS - 14
ER -