TY - JOUR
T1 - Correlation between thermoelectric properties and magnetic phases in the charge-ordered Pr0.5Sr0.5-xCaxMnO3
AU - Niebieskikwiat, D.
AU - Sánchez, R. D.
N1 - Funding Information:
This work was supported by CNEA (Argentine Atomic Energy Commission), CONICET (Argentine National Research Council), and Fundación Antorchas. We thank Dr. D.G. Lamas and L. Morales for their help with the XRD data. We acknowledge Dr. J. Sofo for the useful discussions about the TEP.
PY - 2000/11
Y1 - 2000/11
N2 - We have performed measurements of thermoelectric power (TEP), electrical resistivity, DC magnetization and X-ray powder diffraction in polycrystalline samples of the charge-ordered manganite Pr0.5Sr0.5-xCaxMnO3 for x = 0, 0.1 and 0.2. All the studied samples revealed three magnetic phases: paramagnetic at high temperatures, ferromagnetic below TC down to TN, below which the antiferromagnetic phase is established. At the paramagnetic-ferromagnetic transition, the TEP presents a clear break, and the three samples show metallic resistivity below TC. On the other hand, below TN all the samples turn to an insulating-like resistivity, but the TEP shows striking differences between the x = 0 sample and the other two. These differences are compatible with the different lattice and magnetic structures of the samples. These results support the idea that below TN a 2D-metal is present and no charge-order accompanies the A-type antiferromagnetic phase.
AB - We have performed measurements of thermoelectric power (TEP), electrical resistivity, DC magnetization and X-ray powder diffraction in polycrystalline samples of the charge-ordered manganite Pr0.5Sr0.5-xCaxMnO3 for x = 0, 0.1 and 0.2. All the studied samples revealed three magnetic phases: paramagnetic at high temperatures, ferromagnetic below TC down to TN, below which the antiferromagnetic phase is established. At the paramagnetic-ferromagnetic transition, the TEP presents a clear break, and the three samples show metallic resistivity below TC. On the other hand, below TN all the samples turn to an insulating-like resistivity, but the TEP shows striking differences between the x = 0 sample and the other two. These differences are compatible with the different lattice and magnetic structures of the samples. These results support the idea that below TN a 2D-metal is present and no charge-order accompanies the A-type antiferromagnetic phase.
UR - http://www.scopus.com/inward/record.url?scp=0343431482&partnerID=8YFLogxK
U2 - 10.1016/S0304-8853(00)00500-X
DO - 10.1016/S0304-8853(00)00500-X
M3 - Artículo
AN - SCOPUS:0343431482
SN - 0304-8853
VL - 221
SP - 285
EP - 292
JO - Journal of Magnetism and Magnetic Materials
JF - Journal of Magnetism and Magnetic Materials
IS - 3
ER -