Sr 1؊x La 1؉x )Zn 1؊x O 3.5؊x/2 (0.014 4x < 0.03), was prepared at 1373 K in the SrO+La 2 O 3 +ZnO system. The X-ray and neutron powder di4raction peaks were indexed with a body-centered tetragonal unit cell (a ؍ 3.75 and c ؍ 13.57 A s for the sample x ؍ 0.01). Weak di4use superstructure re6ec
Crystal Structure and Electronic State of the DisorderedS=1 System (LixV1−x)3BO5withx≃0.3
✍ Scribed by Masashige Onoda
- Publisher
- Elsevier Science
- Year
- 1998
- Tongue
- English
- Weight
- 442 KB
- Volume
- 141
- Category
- Article
- ISSN
- 0022-4596
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✦ Synopsis
The crystal structure and electronic state of the (Li x V 1؊x ) 3 BO 5 system with xK0.3 have been explored through measurements of the X-ray four-circle diffraction, electron transport, and magnetization. The crystal data at 297 K show an orthorhombic structure with space group Pbam; a ؍ 9.195(1) A > , b ؍ 12.209(1) A > , c ؍ 2.9922(9) A > , and Z ؍ 4. The structure determined with the residual factors of R ؍ 0.017 and R w ؍ 0.018 for 1048 independent reflections is of a ludwigite type; Li and V atoms are located at the centers of an octahedron of oxygens with mixed occupancy, and the B atom resides in the middle of the oxygen triangles. The V-V bonded linear trimer may exist there. The variable-range-hopping-like transport and the transition from a localized state with SK1 to a spin-glass-like state are revealed, which are basically consistent with the structural aspect.
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