Isobaric heat capacities,
Cp, of La
0.207Co
0.207O
0.586, La
0.179Sr
0.032Co
0.210O
0.579 and La
0.109Sr
0.109Co
0.218O
0.564 from near absolute zero Kelvin (2 K) to high temperature (1340 K) were measured by a relaxation method and differential scanning calorimetry. In the
Cp values for La
0.207Co
0.207O
0.586, two peaks at 628 K and 788 K were observed, consistent with the phase transition of from semi-conductor to metal and the phase transition at which magnetic moment increased as a function of temperature, respectively. Also, in the
Cp values for La
0.179Sr
0.032Co
0.210O
0.579, such two-kinds of the phase transitions, that is the phase transition of semi-conductor to metal and the phase transition increasing the magnetic moment, were observed in the lower temperature ranges than in La
0.207Co
0.207O
0.586. The phase transition from ferromagnetic- to paramagnetic-metal was caused at 239 K in La
0.109Sr
0.109Co
0.218O
0.564, while such two kinds of phase transitions observed in La
0.207Co
0.207O
0.586 and La
0.179Sr
0.032Co
0.210O
0.579 were disappeared. The Debye temperature, Θ
D, of La
0.207Co
0.207O
0.586 was determined from the measured
Cp values below 10 K. Its isochoric heat capacity,
CV, was calculated by inserting Θ
D into the Debye function, and the isochoric entropies of vibration, Δ
0TSV, was determined, followed by calculating the entropy of vibration of oxygen vacancy, Δ
fSTvib.V(Vö), by differentiation of Δ
0TSV with the Vö content. The Δ
fSTvib.V(Vö) obtained at 298 K and 800 K were 42.86 J·K
-1·mol
-1 and 44.00 J·K
-1·mol
-1, respectively. Such a large Δ
fSTvib.V(Vö) appears to be one of important reason for foming Vö.
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