Literature DB >> 21588470

Redetermination of Fe(2)[BP(3)O(12)].

Fei Fei Li1, Hui Ju Zhang, Li Na Zhang.   

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.

Entities:  

Year:  2010        PMID: 21588470      PMCID: PMC3007966          DOI: 10.1107/S1600536810029818

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


Related literature

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].

Experimental

Crystal data

Fe2[BP3O12] M = 407.42 Hexagonal, a = 8.0347 (8) Å c = 7.4163 (13) Å V = 414.63 (9) Å3 Z = 2 Mo Kα radiation μ = 4.15 mm−1 T = 293 K 0.15 × 0.05 × 0.05 mm

Data collection

Rigaku Mercury70 CCD diffractometer Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.575, T max = 0.819 3247 measured reflections 345 independent reflections 338 reflections with I > 2σ(I) R int = 0.042

Refinement

R[F 2 > 2σ(F 2)] = 0.035 wR(F 2) = 0.072 S = 1.07 345 reflections 33 parameters Δρmax = 0.58 e Å−3 Δρmin = −0.78 e Å−3 Data 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.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810029818/wm2377Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Fe2[BP3O12]Dx = 3.263 Mg m3
Mr = 407.42Mo Kα radiation, λ = 0.71073 Å
Hexagonal, P63/mCell parameters from 1049 reflections
Hall symbol: -P 6cθ = 4.0–27.4°
a = 8.0347 (8) ŵ = 4.15 mm1
c = 7.4163 (13) ÅT = 293 K
V = 414.63 (9) Å3Prism, light-red
Z = 20.15 × 0.05 × 0.05 mm
F(000) = 396
Rigaku Mercury70 CCD diffractometer345 independent reflections
Radiation source: fine-focus sealed tube338 reflections with I > 2σ(I)
Graphite MonochromatorRint = 0.042
Detector resolution: 14.6306 pixels mm-1θmax = 27.4°, θmin = 2.9°
ω scansh = −10→10
Absorption correction: multi-scan (ABSCOR; Higashi, 1995)k = −10→10
Tmin = 0.575, Tmax = 0.819l = −9→6
3247 measured reflections
Refinement on F20 restraints
Least-squares matrix: fullPrimary atom site location: structure-invariant direct methods
R[F2 > 2σ(F2)] = 0.035Secondary atom site location: difference Fourier map
wR(F2) = 0.072w = 1/[σ2(Fo2) + (0.0168P)2 + 3.P] where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
345 reflectionsΔρmax = 0.58 e Å3
33 parametersΔρmin = −0.78 e Å3
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.
xyzUiso*/Ueq
Fe10.66670.33330.45190 (12)0.0072 (3)
P11.04513 (17)0.68473 (17)0.25000.0064 (3)
O20.8735 (5)0.4782 (5)0.25000.0080 (7)
O10.9428 (5)0.8099 (5)0.25000.0097 (8)
B11.00001.00000.25000.0101 (19)
O31.1626 (3)0.7289 (3)0.4200 (4)0.0115 (6)
U11U22U33U12U13U23
Fe10.0076 (3)0.0076 (3)0.0063 (5)0.00381 (15)0.0000.000
P10.0055 (6)0.0057 (6)0.0077 (7)0.0025 (5)0.0000.000
O20.0067 (15)0.0059 (16)0.0099 (19)0.0021 (13)0.0000.000
O10.0060 (16)0.0056 (16)0.017 (2)0.0022 (13)0.0000.000
B10.008 (2)0.008 (2)0.014 (5)0.0040 (12)0.0000.000
O30.0116 (12)0.0115 (12)0.0127 (15)0.0066 (10)−0.0045 (11)−0.0019 (10)
Fe1—O3i1.929 (2)P1—O21.538 (3)
Fe1—O3ii1.929 (2)P1—O11.586 (3)
Fe1—O3iii1.929 (2)O2—Fe1iv2.103 (2)
Fe1—O2iv2.103 (2)O1—B11.357 (3)
Fe1—O22.103 (2)B1—O1vii1.357 (3)
Fe1—O2v2.103 (2)B1—O1viii1.357 (3)
P1—O31.507 (3)O3—Fe1i1.929 (2)
P1—O3vi1.507 (3)
O3i—Fe1—O3ii97.83 (11)O3—P1—O3vi113.6 (2)
O3i—Fe1—O3iii97.83 (11)O3—P1—O2111.85 (12)
O3ii—Fe1—O3iii97.83 (11)O3vi—P1—O2111.85 (12)
O3i—Fe1—O2iv93.65 (11)O3—P1—O1108.24 (12)
O3ii—Fe1—O2iv91.53 (11)O3vi—P1—O1108.24 (12)
O3iii—Fe1—O2iv164.04 (11)O2—P1—O1102.37 (18)
O3i—Fe1—O291.53 (11)P1—O2—Fe1129.13 (10)
O3ii—Fe1—O2164.04 (11)P1—O2—Fe1iv129.14 (10)
O3iii—Fe1—O293.65 (11)Fe1—O2—Fe1iv90.78 (13)
O2iv—Fe1—O274.92 (10)B1—O1—P1136.3 (3)
O3i—Fe1—O2v164.04 (11)O1vii—B1—O1viii120.000 (1)
O3ii—Fe1—O2v93.65 (11)O1vii—B1—O1120.000 (1)
O3iii—Fe1—O2v91.53 (11)O1viii—B1—O1120.000 (1)
O2iv—Fe1—O2v74.92 (10)P1—O3—Fe1i142.54 (17)
O2—Fe1—O2v74.92 (10)
Table 1

Selected bond lengths (Å)

Fe1—O3i1.929 (2)
Fe1—O22.103 (2)
P1—O31.507 (3)
P1—O21.538 (3)
P1—O11.586 (3)
O1—B11.357 (3)

Symmetry code: (i) .

  3 in total

1.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

2.  KMBP2O8 (M = Sr, Ba): a new kind of noncentrosymmetry borophosphate with the three-dimensional diamond-like framework.

Authors:  Dan Zhao; Wen-Dan Cheng; Hao Zhang; Shu-Ping Huang; Zhi Xie; Wei-Long Zhang; Song-Lin Yang
Journal:  Inorg Chem       Date:  2009-07-20       Impact factor: 5.165

3.  Structure validation in chemical crystallography.

Authors:  Anthony L Spek
Journal:  Acta Crystallogr D Biol Crystallogr       Date:  2009-01-20
  3 in total

北京卡尤迪生物科技股份有限公司 © 2022-2023.