Structural, magnetic and electronic properties of LaNi0.5Fe0.5O3 in the temperature range 5-1000 K

被引:27
作者
Gateshki, M. [2 ]
Suescun, L. [1 ]
Kolesnik, S. [3 ]
Mais, J. [3 ]
Swierczek, K. [1 ,3 ]
Short, S. [1 ]
Dabrowski, B. [1 ,3 ]
机构
[1] Argonne Natl Lab, Div Mat Sci, Argonne, IL 60439 USA
[2] Australian Nucl Sci & Technol Org, Bragg Inst, Menai, NSW 2234, Australia
[3] No Illinois Univ, Dept Phys, De Kalb, IL 60115 USA
基金
美国国家科学基金会;
关键词
solid oxide fuel cells; perovskites; phase transitions;
D O I
10.1016/j.jssc.2008.03.041
中图分类号
O61 [无机化学];
学科分类号
070301 ; 081704 ;
摘要
The structure, magnetism, transport and thermal expansion of the perovskite oxide LaNi0.5Fe0.5O3 were studied over a wide range of temperatures. Neutron time-of-flight data have shown that this compound undergoes a first-order phase transition between similar to 275 and similar to 310K. The structure transforms from orthorhombic (Pbnm) at low temperatures to rhombohedral (R (3) over barc) above room temperature. This phase transition is the cause for the previously observed co-existence of phases at room temperature. The main structural modification associated with the phase transition is the change of tilting pattern of the octahedra from a(+)b(-)b(-) at low temperatures to a(-)a(-)a(-) at higher. Magnetic data strongly suggests that a spin-glass magnetic state exists in the sample below 83 K consistent with the absence of magnetic ordering peaks in the neutron data collected at 30K. At high temperatures the sample behaves as a small polaron electronic conductor with two regions of slightly different activation energies of 0.07 and 0.05 eV above and below 553 K, respectively. The dilatometric data show an average thermal expansion coefficient of 14.7 x 10(-6) K-1 which makes this material compatible with frequently used electrolytes in solid oxide fuel cells. (C) 2008 Elsevier Inc. All rights reserved.
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页码:1833 / 1839
页数:7
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