Fei Fei Li1, Hui Ju Zhang, Li Na Zhang. 1. Department of Physics and Chemistry, Henan Polytechnic University, Jiaozuo, Henan 454000, People's Republic of China.
Abstract
Explorations of phases in the quaternary Fe(III)-B(III)-P(V)-O system prepared by the high temperature solution growth (HTSG) method led to single-crystal growth of anhydrous diiron(III) borotriphosphate, Fe(2)[BP(3)O(12)]. This phase has been synthesized previously as a microcrystalline material and its structure refined in space group P3 from powder X-ray diffraction data using the Rietveld method [Chen et al. (2004 ▶). J. Inorg. Mater.19, 429-432]. In the current single-crystal study, it was shown that the correct space group is P6(3)/m. The three-dimensional structure of the title compound is built up from FeO(6) octa-hedra (3.. symmetry), trigonal-planar BO(3) groups ( symmetry) and PO(4) tetra-hedra (m.. symmetry). Two FeO(6) octa-hedra form Fe(2)O(9) dimers via face-sharing, while the anionic BO(3) and PO(4) groups are connected via corner-sharing to build up the [BP(3)O(12)](6-) anion. Both units are inter-connected via corner-sharing.
Explorations of phases in the quaternary Fe(III)-B(III)-P(V)-O system prepared by the high temperature solution growth (HTSG) method led to single-crystal growth of anhydrous diiron(III) borotriphosphate, Fe(2)[BP(3)O(12)]. This phase has been synthesized previously as a microcrystalline material and its structure refined in space group P3 from powder X-ray diffraction data using the Rietveld method [Chen et al. (2004 ▶). J. Inorg. Mater.19, 429-432]. In the current single-crystal study, it was shown that the correct space group is P6(3)/m. The three-dimensional structure of the title compound is built up from FeO(6) octa-hedra (3.. symmetry), trigonal-planar BO(3) groups ( symmetry) and PO(4) tetra-hedra (m.. symmetry). Two FeO(6) octa-hedra form Fe(2)O(9) dimers via face-sharing, while the anionic BO(3) and PO(4) groups are connected via corner-sharing to build up the [BP(3)O(12)](6-) anion. Both units are inter-connected via corner-sharing.
Reviews on the crystal chemistry of borophosphates were given by Kniep et al. (1998 ▶) and Ewald et al. (2007 ▶). For the previous powder study of Fe2[BP3O12], see: Chen et al. (2004 ▶). For the structure of a related borophosphate, see: Zhao et al. (2009 ▶). Meisel et al. (2004 ▶) have reported the structure of V2[BP3O12] and Mi et al. (2000 ▶) that of Cr2[BP3O12].
Rigaku Mercury70 CCD diffractometerAbsorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T
min = 0.575, T
max = 0.8193247 measured reflections345 independent reflections338 reflections with I > 2σ(I)R
int = 0.042
Refinement
R[F
2 > 2σ(F
2)] = 0.035wR(F
2) = 0.072S = 1.07345 reflections33 parametersΔρmax = 0.58 e Å−3Δρmin = −0.78 e Å−3Data collection: CrystalClear (Rigaku, 2004 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg, 2004 ▶); software used to prepare material for publication: SHELXTL (Sheldrick, 2008 ▶) and PLATON (Spek, 2009 ▶).Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810029818/wm2377sup1.cifStructure factors: contains datablocks I. DOI: 10.1107/S1600536810029818/wm2377Isup2.hklAdditional supplementary materials: crystallographic information; 3D view; checkCIF report
Primary atom site location: structure-invariant direct methods
R[F2 > 2σ(F2)] = 0.035
Secondary atom site location: difference Fourier map
wR(F2) = 0.072
w = 1/[σ2(Fo2) + (0.0168P)2 + 3.P] where P = (Fo2 + 2Fc2)/3
S = 1.07
(Δ/σ)max < 0.001
345 reflections
Δρmax = 0.58 e Å−3
33 parameters
Δρmin = −0.78 e Å−3
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes)
are estimated using the full covariance matrix. The cell e.s.d.'s are taken
into account individually in the estimation of e.s.d.'s in distances, angles
and torsion angles; correlations between e.s.d.'s in cell parameters are only
used when they are defined by crystal symmetry. An approximate (isotropic)
treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s.
planes.
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor
wR and goodness of fit S are based on F2, conventional
R-factors R are based on F, with F set to zero for
negative F2. The threshold expression of F2 >
σ(F2) is used only for calculating R-factors(gt) etc.
and is not relevant to the choice of reflections for refinement.
R-factors based on F2 are statistically about twice as large
as those based on F, and R- factors based on ALL data will be
even larger.