Structural properties and high-temperature spin and electronic transitions in GdCoO3: Experiment and theory

被引:33
|
作者
Orlov, Yu. S. [1 ,2 ]
Solovyov, L. A. [3 ]
Dudnikov, V. A. [1 ]
Fedorov, A. S. [1 ,2 ]
Kuzubov, A. A. [2 ]
Kazak, N. V. [1 ]
Voronov, V. N. [1 ]
Vereshchagin, S. N. [3 ]
Shishkina, N. N. [3 ]
Perov, N. S. [4 ]
Lamonova, K. V. [5 ]
Babkin, R. Yu [5 ]
Pashkevich, Yu. G. [5 ]
Anshits, A. G. [2 ,3 ]
Ovchinnikov, S. G. [1 ,2 ,6 ]
机构
[1] Russian Acad Sci, LV Kirensky Inst Phys, Siberian Branch, Krasnoyarsk 660036, Russia
[2] Siberian Fed Univ, Krasnoyarsk 660041, Russia
[3] Russian Acad Sci, Siberian Branch, Inst Chem & Chem Technol, Krasnoyarsk 660049, Russia
[4] Moscow MV Lomonosov State Univ, Fac Phys, Moscow 119991, Russia
[5] Natl Acad Sci Ukraine, OO Galkin Donetsk Inst Phys & Engn, UA-83114 Donetsk, Ukraine
[6] MF Reshetnev Siberian State Aerosp Univ, Krasnoyarsk 660014, Russia
基金
俄罗斯基础研究基金会;
关键词
MAGNETIC-PROPERTIES; PROFILE REFINEMENT; STATE; NUCLEAR; IONS;
D O I
10.1103/PhysRevB.88.235105
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We have investigated the x-ray diffraction (XRD) structure, magnetic susceptibility, and heat capacity of GdCoO3 in a wide temperature range. A model of phase separation of the low-spin (LS) and high-spin (HS) states has been proposed based on the analysis of XRD peak shape anomalies in the temperature range 200-800 K. From magnetic measurements we separated the HS Co3+ contribution and fitted it with the temperature-dependent spin gap. We found a smooth LS-HS crossover at T = 800 K. The possible contribution of the intermediate spin (IS) state to the thermodynamics is excluded by the calculation IS-LS excitation energy within the modified crystal-field approach. In the two-phase model, with HS/LS probabilities calculated from the found spin gap and the LS and HS volumes calculated by the DFT-GGA method, we were able to reproduce the temperature dependence of the unit-cell volume and thermal expansion. Thus, we conclude that in GdCoO3 the main mechanism of the lattice expansion is not the conventional lattice anharmonicity, but the HS/LS fluctuations. The electronic structure has been calculated by the LDA+GTB method. At zero temperature, we have obtained the charge-transfer insulator with the charge gap E-g = 0.5 eV. The thermal population of the HS term results in the in-gap band formation inside the insulator gap and smooth insulator-metal transition at T-IMT = 780 K. Heat-capacity measurements revealed a smooth maximum near the T-IMT.
引用
收藏
页数:14
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