Literature DB >> 25161509

β-K3Fe(MoO4)2Mo2O7.

Amira Souilem1, Mohamed Faouzi Zid1, Ahmed Driss1.   

Abstract

The title compound, tripotassium iron(III) bis-(ortho-molyb-date) dimolybdate, was obtained by a solid-state reaction. The main structural building units are one FeO6 octa-hedron, two MoO4 tetra-hedra and one Mo2O7 dimolybdate group, all with point group symmetries m. These units are linked via corner-sharing to form ribbons parallel to [010]. The three K(+) cations are located between the ribbons on mirror planes and have coordination numbers of 10 and 12. Two O atoms of one of the MoO4 tetra-hedra of the dimolybdate group are disordered over two positions in a 0.524 (11):0.476 (11) ratio. The structure of the title compound is compared briefly with that of Rb3FeMo4O15.

Entities:  

Year:  2014        PMID: 25161509      PMCID: PMC4120611          DOI: 10.1107/S1600536814013087

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


Related literature

For properties of related molybdates, see: Zhang et al. (2000 ▶); Muessig et al. (2003 ▶); Bramnik et al. (2003 ▶); Soares & Portela (2005 ▶); Bowker et al. (2008 ▶); Otko et al. (1978 ▶); Klimin et al. (2003 ▶); Jorge et al. (2004 ▶); Maczka et al. (2005 ▶). The closely related crystal structures of α-K3Fe(MoO4)2(Mo2O7) and Rb3Fe(MoO4)2Mo2O7 were determined by Maczka et al. (2009 ▶) and Khal’baeva et al. (2010 ▶), respectively. For bond-valence sums, see: Brown & Altermatt (1985 ▶).

Experimental

Crystal data

K3Fe(MoO4)2Mo2O7 M = 796.91 Monoclinic, a = 32.873 (2) Å b = 5.7137 (7) Å c = 7.9177 (9) Å β = 91.143 (8)° V = 1486.9 (3) Å3 Z = 4 Mo Kα radiation μ = 5.15 mm−1 T = 298 K 0.36 × 0.22 × 0.18 mm

Data collection

Enraf–Nonius CAD-4 diffractometer Absorption correction: ψ scan (North et al., 1968 ▶) T min = 0.286, T max = 0.488 3443 measured reflections 1789 independent reflections 1636 reflections with I > 2σ(I) R int = 0.028 2 standard reflections every 120 min intensity decay: 1.3%

Refinement

R[F 2 > 2σ(F 2)] = 0.029 wR(F 2) = 0.076 S = 1.06 1789 reflections 138 parameters Δρmax = 1.22 e Å−3 Δρmin = −1.57 e Å−3 Data collection: CAD-4 EXPRESS (Duisenberg, 1992 ▶; Macíček & Yordanov, 1992 ▶); cell refinement: CAD-4 EXPRESS; data reduction: XCAD4 (Harms & Wocadlo, 1995 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg & Putz, 1999 ▶); software used to prepare material for publication: WinGX (Farrugia, 2012 ▶). Crystal structure: contains datablock(s) I. DOI: 10.1107/S1600536814013087/wm5025sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814013087/wm5025Isup2.hkl CCDC reference: 1006924 Additional supporting information: crystallographic information; 3D view; checkCIF report
K3Fe(MoO4)2Mo2O7F(000) = 1484
Mr = 796.91Dx = 3.560 Mg m3
Monoclinic, C2/mMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2yCell parameters from 25 reflections
a = 32.873 (2) Åθ = 11–15°
b = 5.7137 (7) ŵ = 5.15 mm1
c = 7.9177 (9) ÅT = 298 K
β = 91.143 (8)°Prism, green
V = 1486.9 (3) Å30.36 × 0.22 × 0.18 mm
Z = 4
Enraf–Nonius CAD-4 diffractometer1636 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.028
Graphite monochromatorθmax = 27.0°, θmin = 2.5°
ω/2θ scansh = −41→41
Absorption correction: ψ scan (North et al., 1968)k = −1→7
Tmin = 0.286, Tmax = 0.488l = −10→5
3443 measured reflections2 standard reflections every 120 min
1789 independent reflections intensity decay: 1.3%
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.029w = 1/[σ2(Fo2) + (0.0306P)2 + 20.6944P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.076(Δ/σ)max = 0.001
S = 1.06Δρmax = 1.22 e Å3
1789 reflectionsΔρmin = −1.57 e Å3
138 parametersExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.00379 (16)
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*/UeqOcc. (<1)
Mo10.568576 (15)0.5000−0.03610 (7)0.01354 (16)
Mo20.649834 (16)0.00000.73776 (7)0.01577 (16)
Mo30.718491 (15)0.00000.18432 (7)0.01355 (16)
Mo40.55700 (2)0.50000.49609 (8)0.0375 (2)
Fe10.68040 (3)0.5000−0.01846 (11)0.0118 (2)
K10.51309 (5)0.00000.7616 (2)0.0253 (3)
K20.60638 (5)0.00000.2307 (2)0.0340 (4)
K30.68689 (5)0.50000.4756 (2)0.0361 (5)
O10.62085 (14)0.50000.0211 (7)0.0257 (11)
O20.73729 (17)0.00000.3855 (7)0.0373 (15)
O30.54601 (11)0.7403 (7)0.0504 (5)0.0277 (8)
O40.68711 (12)0.7469 (9)0.1610 (6)0.0459 (13)
O50.60430 (19)0.50000.4216 (9)0.053 (2)
O60.75919 (14)0.00000.0434 (6)0.0223 (11)
O70.67523 (14)0.2575 (11)0.8080 (7)0.0669 (19)
O80.55792 (18)0.50000.7337 (6)0.0329 (13)
O90.64948 (18)0.00000.5221 (7)0.0346 (14)
O100.60110 (17)0.00000.8120 (8)0.0396 (15)
O110.5491 (2)0.1696 (14)0.4498 (9)0.031 (2)0.524 (11)
O120.5224 (3)0.3608 (15)0.3916 (10)0.034 (3)0.476 (11)
U11U22U33U12U13U23
Mo10.0084 (3)0.0180 (3)0.0142 (3)0.000−0.00063 (19)0.000
Mo20.0111 (3)0.0210 (3)0.0151 (3)0.000−0.00068 (19)0.000
Mo30.0080 (2)0.0163 (3)0.0164 (3)0.000−0.00035 (19)0.000
Mo40.0169 (3)0.0820 (6)0.0137 (3)0.0000.0003 (2)0.000
Fe10.0092 (4)0.0101 (4)0.0160 (4)0.000−0.0006 (3)0.000
K10.0184 (7)0.0324 (9)0.0250 (8)0.000−0.0022 (6)0.000
K20.0195 (7)0.0563 (12)0.0260 (8)0.000−0.0046 (6)0.000
K30.0226 (8)0.0665 (14)0.0191 (8)0.000−0.0004 (6)0.000
O10.010 (2)0.042 (3)0.025 (3)0.000−0.0025 (19)0.000
O20.023 (3)0.065 (4)0.023 (3)0.000−0.008 (2)0.000
O30.0224 (17)0.0242 (18)0.037 (2)0.0016 (16)0.0069 (15)−0.0049 (17)
O40.031 (2)0.051 (3)0.058 (3)−0.029 (2)0.0281 (19)−0.040 (2)
O50.027 (3)0.085 (6)0.048 (4)0.0000.011 (3)0.000
O60.009 (2)0.032 (3)0.026 (3)0.0000.0045 (18)0.000
O70.038 (2)0.087 (4)0.077 (4)−0.036 (3)0.026 (2)−0.068 (3)
O80.035 (3)0.048 (4)0.015 (2)0.000−0.006 (2)0.000
O90.033 (3)0.056 (4)0.015 (2)0.000−0.004 (2)0.000
O100.018 (3)0.056 (4)0.045 (4)0.0000.005 (2)0.000
O110.031 (4)0.036 (4)0.025 (4)0.005 (3)0.002 (3)−0.002 (3)
O120.036 (5)0.033 (5)0.031 (4)−0.017 (4)−0.003 (3)−0.015 (4)
Mo1—O31.710 (4)K1—O3x2.882 (4)
Mo1—O3i1.710 (4)K1—O102.913 (6)
Mo1—O11.768 (5)K1—O3xi2.916 (4)
Mo1—O8ii1.849 (5)K1—O3xii2.916 (4)
Mo2—O91.708 (5)K1—O11iii2.924 (7)
Mo2—O101.717 (6)K1—O112.924 (7)
Mo2—O71.776 (5)K1—O8iv3.224 (3)
Mo2—O7iii1.776 (5)K2—O92.683 (6)
Mo3—O21.697 (5)K2—O112.762 (7)
Mo3—O61.759 (5)K2—O11iii2.762 (7)
Mo3—O4iv1.784 (4)K2—O3iv2.841 (4)
Mo3—O4i1.784 (4)K2—O3i2.841 (4)
Mo4—O121.605 (7)K2—O4i3.082 (5)
Mo4—O12i1.605 (7)K2—O4iv3.082 (5)
Mo4—O51.674 (6)K2—O53.233 (3)
Mo4—O81.881 (5)K2—O5iv3.233 (3)
Mo4—O111.940 (8)K2—O10ii3.317 (7)
Mo4—O11i1.940 (8)K2—O1iv3.343 (3)
Fe1—O7ii1.956 (4)K2—O13.343 (3)
Fe1—O7v1.956 (4)K3—O2xiii2.704 (6)
Fe1—O11.989 (5)K3—O52.740 (7)
Fe1—O6vi2.000 (5)K3—O4i2.863 (5)
Fe1—O42.011 (4)K3—O42.863 (5)
Fe1—O4i2.011 (4)K3—O7i3.005 (7)
K1—O12vii2.650 (8)K3—O73.005 (7)
K1—O12viii2.650 (8)K3—O93.135 (3)
K1—O11vii2.789 (8)K3—O9xiv3.135 (3)
K1—O11viii2.789 (8)K3—O2xiv3.386 (3)
K1—O3ix2.882 (4)K3—O23.386 (3)
O3—Mo1—O3i106.8 (3)O12—Mo4—O1147.9 (4)
O3—Mo1—O1108.94 (15)O12i—Mo4—O11107.1 (4)
O3i—Mo1—O1108.94 (15)O5—Mo4—O1193.2 (2)
O3—Mo1—O8ii108.63 (16)O8—Mo4—O11100.9 (2)
O3i—Mo1—O8ii108.63 (16)O12—Mo4—O11i107.1 (4)
O1—Mo1—O8ii114.6 (2)O12i—Mo4—O11i47.9 (4)
O9—Mo2—O10110.8 (3)O5—Mo4—O11i93.2 (2)
O9—Mo2—O7107.9 (2)O8—Mo4—O11i100.9 (2)
O10—Mo2—O7109.20 (18)O11—Mo4—O11i153.4 (4)
O9—Mo2—O7iii107.9 (2)O7ii—Fe1—O7v90.2 (4)
O10—Mo2—O7iii109.20 (18)O7ii—Fe1—O192.22 (17)
O7—Mo2—O7iii111.9 (4)O7v—Fe1—O192.22 (17)
O2—Mo3—O6109.2 (3)O7ii—Fe1—O6vi90.18 (17)
O2—Mo3—O4iv107.2 (2)O7v—Fe1—O6vi90.18 (17)
O6—Mo3—O4iv112.33 (14)O1—Fe1—O6vi176.6 (2)
O2—Mo3—O4i107.2 (2)O7ii—Fe1—O4178.6 (2)
O6—Mo3—O4i112.33 (14)O7v—Fe1—O490.4 (3)
O4iv—Mo3—O4i108.3 (3)O1—Fe1—O489.03 (15)
O12—Mo4—O12i59.4 (7)O6vi—Fe1—O488.54 (16)
O12—Mo4—O5118.2 (4)O7ii—Fe1—O4i90.4 (3)
O12i—Mo4—O5118.2 (4)O7v—Fe1—O4i178.6 (2)
O12—Mo4—O8120.8 (3)O1—Fe1—O4i89.03 (15)
O12i—Mo4—O8120.8 (3)O6vi—Fe1—O4i88.54 (16)
O5—Mo4—O8110.9 (3)O4—Fe1—O4i89.1 (3)
  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.  Structural and vibrational properties of K(3)Fe(MoO(4))(2)(Mo(2)O(7))-a novel layered molybdate.

Authors:  M Maczka; A Pietraszko; W Paraguassu; A G Souza Filho; P T C Freire; J Mendes Filho; J Hanuza
Journal:  J Phys Condens Matter       Date:  2009-01-29       Impact factor: 2.333

3.  Structural investigation of the Na-Fe-Mo-O system.

Authors:  E Muessig; K G Bramnik; H Ehrenberg
Journal:  Acta Crystallogr B       Date:  2003-09-25
  3 in total

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