The crystal structure of the a phase of malonic acid has been determined ab initio from high-resolution neutron powder diffrao tion data at 373 K. Thestructure is orthorhombic: a-7.64800( 1) A, b=5.0211 I (I) A, c= 11.55803(2) A, V,=443.84\_A3 with four molecules in the unit cell and is character&d
Ab Initio Determination of Bi4.86La1.14O9 Monoclinic Structure from Powder Neutron Diffraction Data. Characterization of the Related Solid Solution
โ Scribed by S. Obbade; M. Drache; P. Conflant; E. Suard
- Publisher
- Elsevier Science
- Year
- 2001
- Tongue
- English
- Weight
- 558 KB
- Volume
- 162
- Category
- Article
- ISSN
- 0022-4596
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โฆ Synopsis
This paper deals with the ab initio determination of -Bi 4.86 La 1.14 O 9 monoclinic structure from powder neutron data using the Rietveld method, and with physical properties characterization of a related solid solution. -Bi 4.86 La 1.14 O 9 , obtained from the annealing of a quenched rhombohedral hightemperature 1 sample, is monoclinic, P 2/c, a โซุโฌ 9.4956(3) A > , b โซุโฌ 3.9742(1) A > , c โซุโฌ 7.0425(2) A > , โซุโฌ 104.700(2)3; Z โซุโฌ 1. The structure re5nement converged to R F โซุโฌ 0.043 and R Bragg โซุโฌ 0.047. The structure is built from cationic slabs parallel to (100) faces of the monoclinic cell. Each cell corresponds to one slab containing a mixed Bi 0.86 La 1.14 cationic layer (Bi (1) ) sandwiched between two equivalent bismuth layers (Bi (2) ). The cohesion of the cations in the slabs results from the presence of the oxygen atoms distributed over three sites. Six O (1) and two O (2) atoms form a slightly distorted cubical polyhedron around the mixed cationic site (Bi (1) ). Bi (2) atoms are surrounded by seven oxygen atoms in a very distorted polyhedron. The important delocalization of Bi (2) lone pairs toward the interslab spaces leads to signi5cant bonds with the adjacent slabs and to the cohesion of the structure. -Bi 4.86 La 1.14 O 9 is the low symmetry variety of a particular sample of a wide solid solution domain that, formulated Bi 1ุx La x O 1.5 , has been investigated for 0.154x40.325. The formation of this phase from the irreversible transformation of quenched-1 on heating and the subsequent transitions P 2 P 1 have been evidenced by thermodi4ractometry, conductivity measurements versus temperature, dilatometry, and thermal analyses. Thermal expansion coe7cients (ุ10 5 ) are for a, c, and/or lattice volume for a quenched-1 , , 2 , or 1
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