Charge density distribution of KMnF3 under high pressure

被引:8
作者
Aoyagi, S. [1 ]
Toda, S. [1 ]
Nishibori, E. [1 ]
Kuroiwa, Y. [2 ,3 ]
Ohishi, Y. [4 ]
Takata, M. [3 ,4 ,5 ]
Sakata, M. [4 ]
机构
[1] Nagoya Univ, Dept Appl Phys, Nagoya, Aichi 4648603, Japan
[2] Hiroshima Univ, Dept Phys Sci, Hiroshima 7398526, Japan
[3] Japan Sci & Technol Agcy, CREST, Kawaguchi, Saitama 3320012, Japan
[4] JASRI, SPring 8, Sayo, Hyogo 6795198, Japan
[5] RIKEN, SPring 8, Sayo, Hyogo 6795198, Japan
来源
PHYSICAL REVIEW B | 2008年 / 78卷 / 22期
关键词
antiferromagnetic materials; charge density waves; charge exchange; high-pressure effects; manganese compounds; maximum entropy methods; potassium compounds; valence bands; X-ray diffraction;
D O I
10.1103/PhysRevB.78.224102
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The charge density distributions of KMnF3 under high pressure (0.3, 1.0, 1.7, 2.7, 3.4, 4.0, 4.8, 5.7, and 6.3 GPa) were determined from the synchrotron-radiation powder-diffraction data by the maximum entropy method (MEM). The difference-MEM charge density, which represents deformations from the spherical atomic charge density for each atom, is changed by applying pressure. The excess electrons on the Mn-F bond suggesting a Mn 3d-F 2p orbital hybridization were found in the difference-MEM charge densities at 0.3 GPa. The excess electrons are localized near Mn nuclei by increasing pressure. Two types of Mn-F bonds were found in the high-pressure tetragonal phase. One is parallel and another is perpendicular to the rotation axis of the F-6 octahedra (i.e., c axis). The number of electrons for K, F, and Mn atoms was estimated from the MEM charge densities. The valence statuses of K atom were +1.02e at 0.3 GPa and +0.20e at 6.3 GPa. The valence statuses of F atom were -0.96e at 0.3GPa and -0.60 and -0.77e at 6.3 GPa. On the other hand, the valence status of Mn atom was virtually unchanged with pressure. This fact suggests that the electron charge transfer from F to K atom occurs with increasing pressure.
引用
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页数:8
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