Thermal and electrical properties of perovskite-type strontium molybdate

Thermophysical properties of Ba1−Sr MoO3(s)

“…The present data for SrMoO 3 (s) are matching reasonably with that of Agarwal et al [17]. But it deviates from the estimated as well as from Maekawa et al [16].…”

“…Fig. 6 shows the heat capacity data of SrMoO 3 (s) measured in this study along with that reported by Maekawa et al [16] and Agarwal et al [17]. The standard error of the polynomial fit for heat capacity of SrMoO 3 (s) is 0.42 J K À1 mol À1 .…”

“…The thermoelectric properties like electrical resistivity, Seebeck coefficient, and thermal conductivity of BaMoO 3 (s) have been studied by Kurosaki et al [14]. Yamanaka et al [15,16] reported physical properties like thermal expansion coefficient, melting temperature, elastic moduli, Debye temperature, micro-hardness, heat capacity, and thermal conductivity of SrMoO 3 (s) and also predicted the metallic behavior from the positive temperature dependency of electrical resistivity. A few research works on thermodynamic properties of BaMoO 3 (s) and SrMoO 3 (s) have been reported in the literature [17][18][19][20][21][22][23][24][25].…”

Structure and thermoelectric properties of double-perovskite oxides: Sr₂₋<i>_x</i>K<i>_x</i>FeMoO₆

“…7),32), 34) The thermal conductivities of the samples were about 35 W/mK at room temperature, and decreased monotonically with increasing temperature. The samples with x = 0.00.2 showed a systematic decrease in thermal conductivity with increasing temperature, indicating that phononphonon scattering was dominant in the temperature range studied.…”

Determinación de la variación de los parámetros críticos del compuesto superconductor CaLaBaCu3-xCoxO7-δ (x=0, 0.06, 0.12, 0.18, 0.24)

“…Lo anterior puede ser representado como A1-x A'xBO 3 , AB 1 -xB'xO 3 , con vacancias catiónicas como AxB1-xBO3, sistemas con deficiencia de oxígeno y ordenamiento catiónico como en el tipo A (B'B'')O3. Ahora el tipo de estructura se presta para poder acomodar elementos con distintos estados de oxidación lo cual puede ser expresado de la forma A (B'xB''y)O 3 (x+y=1) y son generalmente denominados como sistemas de perovskitas complejas (Maekawa, 2005). Estos sistemas de perovskitas complejos pueden ser divididos en:…”