TY - JOUR
T1 - Transformation processes in LaAl O3
T2 - Neutron diffraction, dielectric, thermal, optical, and Raman studies
AU - Hayward, S. A.
AU - Morrison, F. D.
AU - Redfern, S. A.T.
AU - Salje, E. K.H.
AU - Scott, J. F.
AU - Knight, K. S.
AU - Tarantino, S.
AU - Glazer, A. M.
AU - Shuvaeva, V.
AU - Daniel, P.
AU - Zhang, M.
AU - Carpenter, M. A.
PY - 2005/8/1
Y1 - 2005/8/1
N2 - The behavior of the Pm 3̄ m-R 3̄ c phase transition in LaAl O3 (TC =813 K from differential scanning calorimetry measurements) has been studied using temperature-dependent measurements of the crystal structure, dielectric relaxation, specific heat, birefringence, and the frequencies of the two soft modes (via Raman spectroscopy). While all these experiments show behavior near TC consistent with a second-order Landau transition, there is extensive evidence for additional anomalous behavior below 730 K. Below this temperature, the two soft mode frequencies are not proportional to each other, the spontaneous strain is not proportional to the square of the Al O6 rotation angle, and anomalies are seen in the birefringence. Twin domains, which are mobile above 730 K, are frozen below 730 K. These anomalies are consistent with biquadratic coupling between the primary order parameter of the transition (Al O6 rotation) and a second process. From the dielectric results, which indicate a smooth but rapid increase in conductivity in the temperature range 500-800 K, we propose that this second process is hopping of intrinsic oxygen vacancies. These vacancies are essentially static below 730 K and dynamically disordered above 730 K. The interaction between static vacancies and the displacive phase transition is unfavorable. A similar anomaly may be observed in other aluminate perovskites undergoing the same transition.
AB - The behavior of the Pm 3̄ m-R 3̄ c phase transition in LaAl O3 (TC =813 K from differential scanning calorimetry measurements) has been studied using temperature-dependent measurements of the crystal structure, dielectric relaxation, specific heat, birefringence, and the frequencies of the two soft modes (via Raman spectroscopy). While all these experiments show behavior near TC consistent with a second-order Landau transition, there is extensive evidence for additional anomalous behavior below 730 K. Below this temperature, the two soft mode frequencies are not proportional to each other, the spontaneous strain is not proportional to the square of the Al O6 rotation angle, and anomalies are seen in the birefringence. Twin domains, which are mobile above 730 K, are frozen below 730 K. These anomalies are consistent with biquadratic coupling between the primary order parameter of the transition (Al O6 rotation) and a second process. From the dielectric results, which indicate a smooth but rapid increase in conductivity in the temperature range 500-800 K, we propose that this second process is hopping of intrinsic oxygen vacancies. These vacancies are essentially static below 730 K and dynamically disordered above 730 K. The interaction between static vacancies and the displacive phase transition is unfavorable. A similar anomaly may be observed in other aluminate perovskites undergoing the same transition.
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U2 - 10.1103/PhysRevB.72.054110
DO - 10.1103/PhysRevB.72.054110
M3 - Article
AN - SCOPUS:33644937901
SN - 1098-0121
VL - 72
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 5
M1 - 054110
ER -