Literature DB >> 21578040

Rietveld refinement of the mixed boracite Fe(1.59)Zn(1.41)B(7)O(13)Br.

Sandra Ulloa-Godínez, Ivonne Rosales, Lauro Bucio, Mario H Farías, Jorge Campa-Molina.   

Abstract

The structural characterization of the new iron-zinc hepta-borate bromide with composition Fe(1.59)Zn(1.41)B(7)O(13)Br, prepared by chemical transport is reported. A rigid-body model with constrained generalized coordinates was defined in order to hold the positions of the B atoms at reasonable inter-atomic distances that typically would reach unacceptable values because of the weak scattering power of boron. There are three independent sites for the B atoms of which two are tetra-hedrally coordinated. The bond-valence sum around the third B atom, located on a threefold rotation axis, was calculated considering two cases of coordination of boron with oxygens: trigonal-planar and tetrahedral. The contribution of the fourth O atom to the bond-valence sum was found to be only 0.06 v.u., indicating the presence of a very weak bond in the right position to have a distorted tetra-hedral coordination in favour of the trigonal-planar coordination for the third B atom. X-ray fluorescence (XRF) was used to determinate the Fe/Zn ratio.

Entities:  

Year:  2009        PMID: 21578040      PMCID: PMC2971062          DOI: 10.1107/S1600536809044407

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

The method of preparation was based on Schmid (1965 ▶). For related structures, see: Mao et al. (1991 ▶); Dowty & Clark (1972 ▶, 1973 ▶); Mendoza-Alvarez et al. (1985 ▶); Schindler & Hawthorne (1998 ▶); Knorr et al. (2007 ▶). For properties and potential applications of boracites, see: Campa-Molina et al. (1994 ▶, 2002 ▶); Dana (1951 ▶); Mathews et al. (1997 ▶); Smart & Moore (1992 ▶). For bond-valence parameters for oxides, see: Brese & O’Keeffe (1991 ▶).

Experimental

Crystal data

Fe1.59Zn1.41B7O13Br M = 544.65 Trigonal, a = 8.6081 (1) Å c = 21.0703 (3) Å V = 1352.12 (3) Å3 Z = 6 Cu Kα radiation T = 300 K Specimen shape: irregular 20 × 20 × 0.2 mm Specimen prepared at 1173 K Particle morphology: irregular, pale pink

Data collection

Bruker D8 Advance diffractometer Specimen mounting: packed powder sample container Specimen mounted in reflection mode Scan method: step 2θmin = 8.1, 2θmax = 110.0° Increment in 2θ = 0.02°

Refinement

R p = 0.018 R wp = 0.025 R exp = 0.014 R B = 0.06 S = 1.89 Profile function: pseudo-Voigt modified by Thompson et al. (1987 ▶) 397 reflections 18 parameters Data collection: DIFFRAC/AT (Siemens, 1993 ▶); cell refinement: FULLPROF (Rodríguez-Carvajal, 2006 ▶; Rodriguez & Rodriguez-Carvajal, 1997 ▶, a strongly modified version of that described by Wiles & Young, 1981); data reduction: FULLPROF; method used to solve structure: coordinates were taken from an isotypic compound (Mao et al., 1991 ▶); program(s) used to refine structure: FULLPROF; software used to prepare material for publication: DIAMOND. Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809044407/br2119sup1.cif Rietveld powder data: contains datablocks I. DOI: 10.1107/S1600536809044407/br2119Isup2.rtv Additional supplementary materials: crystallographic information; 3D view; checkCIF report Enhanced figure: interactive version of Fig. 4
Fe1.59Zn1.41B7O13BrF(000) = 1546.0
Mr = 544.65Dx = 4.013 Mg m3
Trigonal, R3cCu Kα radiation, λ = 1.54175 Å
Hall symbol: R 3 -2"cT = 300 K
a = 8.6081 (1) ÅParticle morphology: irregular
c = 21.0703 (3) Åpale pink
V = 1352.12 (3) Å3irregular, 20 × 20 mm
Z = 6Specimen preparation: Prepared at 1173 K
Bruker D8 Advance diffractometerData collection mode: reflection
Radiation source: sealed X-ray tube, Cu KαScan method: step
graphitemin = 8.12°, 2θmax = 110.01°, 2θstep = 0.02°
Specimen mounting: packed powder sample container
Least-squares matrix: full with fixed elements per cycle5240 data points
Rp = 0.018Profile function: pseudo-Voigt modified by Thompson et al. (1987)
Rwp = 0.02518 parameters
Rexp = 0.014Weighting scheme based on measured s.u.'s
RBragg = 0.06(Δ/σ)max = 0.02
R(F2) = 0.06Background function: linear interpolation between a set of 72 background points with refinable heights
χ2 = 3.572
xyzUiso*/UeqOcc. (<1)
Br0.000000.000000.266700.0084 (9)
Zn0.1488 (8)0.3037 (3)0.3347 (2)0.0113 (8)0.47000
Fe0.1488 (8)0.3037 (3)0.3347 (2)0.0113 (8)0.53000
B1−0.184 (1)0.1519 (1)−0.080 (1)0.00304
B20.1130 (2)−0.0902 (1)−0.0259 (1)0.00304
B30.000000.000000.105 (1)0.00304
O10.000000.00000−0.008 (1)0.0025 (9)
O20.010 (1)−0.157 (2)0.107 (1)0.0025 (9)
O30.282 (1)0.274 (1)−0.032 (1)0.0025 (9)
O40.206 (1)−0.006 (1)−0.085 (1)0.0025 (9)
O50.242 (1)−0.059 (1)0.024 (1)0.0025 (9)
Zn—Br2.680 (3)B1—O4vii1.451 (13)
Zn—Bri3.412 (1)B1—O5vi1.49 (3)
Zn—O2ii2.130 (4)B2—O11.566 (3)
Zn—O3iii2.081 (7)B2—O3viii1.452 (8)
Zn—O4iv2.035 (4)B2—O41.463 (18)
Zn—O5v2.012 (7)B2—O51.453 (17)
B1—O2vi1.506 (14)B3—O21.397 (14)
B1—O3vii1.48 (2)B3—O12.38 (3)
Zn—Br—Znvii94.1 (2)O2—B3—O2vii119.9 (9)
Zn—Br2.680 (3)
Zn—Bri3.412 (1)
Zn—O2ii2.130 (4)
Zn—O3iii2.081 (7)
Zn—O4iv2.035 (4)
Zn—O5v2.012 (7)
B1—O2vi1.506 (14)
B1—O3vii1.48 (2)
B1—O4vii1.451 (13)
B1—O5vi1.49 (3)
B2—O11.566 (3)
B2—O3viii1.452 (8)
B2—O41.463 (18)
B2—O51.453 (17)
B3—O21.397 (14)
B3—O12.38 (3)
O2—B3—O2vii119.9 (9)

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) ; (v) ; (vi) ; (vii) ; (viii) .

  2 in total

1.  Electron and light microscopy studies on the domain structures of Zn3B7O13Cl, Zn3B7O13Br and Zn3B7O13I ferroic boracites.

Authors:  J Campa-Molina; O Blanco; A Correa-Gomez; M Czank; A G Castellanos-Guzman
Journal:  J Microsc       Date:  2002-12       Impact factor: 1.758

2.  Ferroelectric Field Effect Transistor Based on Epitaxial Perovskite Heterostructures

Authors: 
Journal:  Science       Date:  1997-04-11       Impact factor: 47.728

  2 in total

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