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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Jul 31;64(Pt 8):i51. doi: 10.1107/S1600536808023040

The iron phosphate NaBaFe2(PO4)3

Mourad Hidouri a,*, Hasna Jerbi a, Mongi Ben Amara a
PMCID: PMC2961906  PMID: 21202994

Abstract

A new iron phosphate, sodium barium diiron tris­(phosphate), NaBaFe2(PO4)3, has been synthesized by the flux method and shown to exhibit the well known langbeinite type structure. The Na, Ba and Fe atoms all lie on threefold axes, while the P and O atoms occupy general positions, one of the O atoms being disordered over two positions, with site occupancy factors of ca 0.7 and 0.3. The [Fe2(PO4)3] framework consists of FeO6 octa­hedra sharing all their corners with the PO4 tetra­hedra. The Na+ and Ba2+ cations are almost equally distributed over two distinct cavities, in which they occupy slightly different positions.

Related literature

For related literature, see: Baur (1974); Moffat (1978); Padhi et al. (1997); Shannon (1976). For the structure of langbeinite, see Zemann & Zemann (1957); Battle et al. (1986, 1988).

Experimental

Crystal data

  • NaBaFe2(PO4)3

  • M r = 556.94

  • Cubic, Inline graphic

  • a = 9.796 (1) Å

  • V = 940.1 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 7.82 mm−1

  • T = 293 (2) K

  • 0.1 × 0.1 × 0.1 mm

Data collection

  • Enraf–Nonius CAD4 diffractometer

  • Absorption correction: ψ scan (North et al., 1968) T min = 0.35, T max = 0.46

  • 2114 measured reflections

  • 657 independent reflections

  • 644 reflections with I > 2σ(I)

  • R int = 0.082

  • 2 standard reflections frequency: 120 min intensity decay: 1%

Refinement

  • R[F 2 > 2σ(F 2)] = 0.025

  • wR(F 2) = 0.059

  • S = 0.92

  • 657 reflections

  • 70 parameters

  • 4 restraints

  • Δρmax = 0.57 e Å−3

  • Δρmin = −0.49 e Å−3

  • Absolute structure: Flack (1983), 123 Friedel pairs

  • Flack parameter: −0.03 (3)

Data collection: CAD-4 EXPRESS (Enraf–Nonius, 1994); 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, 1998); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808023040/br2076sup1.cif

e-64-00i51-sup1.cif (20.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808023040/br2076Isup2.hkl

e-64-00i51-Isup2.hkl (32.3KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Selected bond angles (°).

O4Bi—Fe2—O1ii 89.8 (8)
O3—P—O4A 115.1 (3)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

supplementary crystallographic information

Comment

Iron phosphates are of increasing interst because of their potential applications in various fields ranging from catalysis (Moffat, 1978) to ionic conductivity (Padhi et al., 1997). Moreover, these materials are very attractive in terms of basic reasearch because they exhibit a rich structural chemistry owing to the possible (+2/+3) mixed valence of iron and its tendency to exhibit various coordination polyhedra.

The title cmpound, sodium barium diiron phosphate NaBaFe2(PO4)3 was isolated during a systematic investigation of the Na2O–MO–Fe2O3–P2O5 systems where M is a divalent cation. Its structure (Fig. 1) exhibits a three-dimensional [Fe2(PO4)3] framework built up from corner-sharing FeO6 octahedra and PO4 tetrahedra. Each octahedron is linked to six adjacent tetrahedra and reciprocally each tetrahedron is connected to four neighboring octahedra. This framework delimits two sorts of large cavities, statistically occupied by the Na+ and Ba2+ cations.

The two symmetry distinct FeO6 octahedra contained in this structure are somewhat distorted as indicated by the Fe—O distances ranging from 1.963 (5) to 1.991 (4) Å. The average <Fe—O> distances of 1.986 Å for Fe(1) and 1.973 Å for Fe(2) are slightly lower than the value 2.03 Å predicted by Shannon for octahedral Fe3+ ions (Shannon, 1976).

The PO4 tetrahedron is strongly distorted with P—O distances scattering from 1.47 (2) to 1.547 (7) Å. Corresponding average value of 1.511 Å agrees with those frequently observed in anhydrous monophosphates (Baur, 1974).

The Na+ and Ba2+ cations are statistically distributed over two distinct cavities in which they occupy slightly different positions and have partial occupancies of 0.47, 0.53, 0.53 and 0.47 for Na(1), Ba(1), Na(2) and Ba(2), respectively. The environments of these cations (Fig. 2) were determined assuming all cation-oxygen distances are shorter than the shortest to next cationic site. Each of the Na(1), Ba(1) and Ba(2) environments consists of nine O atoms with cation-oxygen distances in the ranges 2.76 (2)–3.04 (2) Å, 2.753 (7)–2.950 (6) Å and 2.722 (5)–3.047 (7) Å for Na(1), Ba(1) and Ba(2), respectively. The Na(2) environment consists of six O atoms with Na—O distances varying from 2.604 (8) and 3.004 (6) Å.

The as-described structure is closely related to the langbeinite-like phosphates KBaM2(PO4)3 (M = Fe, Cr) (Battle et al., 1986, 1988). However, it differs by the fact that the atom O4, which occupies a single site in the potassium phosphates, is, in the title compound, statistically occupying two distinct positions, O4A and O4B which exhibit partial occupancies of 0.7 and 0.3, respectively. These different values can be explained by the fact that the O4A site is occupied if it is bonded to Na(1), Ba(1) or Ba(2) whereas the O4B site is occupied if it is bonded to Na(1) or Ba(1).

Experimental

Single crystals of the title compund were grown in a flux of sodium dimolybdate Na2Mo2O7 with an atomic ratio P:Mo = 6:1. A starting mixture of 1.071 g of Na2CO3, 1.993 g of BaCO3, 8.162 g of Fe(NO3)3.9H2O, 4.002 g of (NH4)2HPO4 and 1.454 g of MoO3 was dissolved in nitric acid and the obtained solution was evaporated to dryness. The dry residue was transferred into a platinum crucible and then heated up 600°C to decompose H2O and NH3. In a second step, the sample was melted for 1 h at 900°C and then cooled down to room temperature with a 10° h-1 rate. The final product, obtained after washing with warm water to dissolve the flux is essentially composed of pink and prismatic shaped crystals. Their qualitative elemental analysis using electron microprobe analysis indicated the presence of Na, Ba, Fe and P and no impurity elements have been detected.

Refinement

The Ba and Fe atoms were located by direct methods and the remaining atoms were found by successive difference Fourier maps. All atomic positions were refined anisotropically.

Figures

Fig. 1.

Fig. 1.

A projection of the structure along the [111] direction.

Fig. 2.

Fig. 2.

The environments of the Na and Ba sites showing the anisotropic atomic displacements at the 50% level.

Crystal data

NaBaFe2(PO4)3 Z = 4
Mr = 556.94 F000 = 1040
Cubic, P213 Dx = 3.935 Mg m3
Hall symbol: P 2ac 2ab 3 Mo Kα radiation λ = 0.71073 Å
a = 9.796 (1) Å Cell parameters from 25 reflections
b = 9.796 (1) Å θ = 9.0–13.0º
c = 9.796 (1) Å µ = 7.82 mm1
α = 90º T = 293 (2) K
β = 90º Prism, pink
γ = 90º 0.1 × 0.1 × 0.1 mm
V = 940.1 (3) Å3

Data collection

Enraf–Nonius CAD-4 diffractometer Rint = 0.082
Radiation source: fine-focus sealed tube θmax = 29.9º
Monochromator: graphite θmin = 2.9º
T = 293(2) K h = −1→13
ω/2θ scans k = −1→13
Absorption correction: ψ scan(North et al., 1968) l = −1→13
Tmin = 0.35, Tmax = 0.46 2 standard reflections
2114 measured reflections every 120 min
657 independent reflections intensity decay: 1%
644 reflections with I > 2σ(I)

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full   w = 1/[σ2(Fo2) + 5.7579P] where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.025 (Δ/σ)max = 0.002
wR(F2) = 0.059 Δρmax = 0.57 e Å3
S = 0.92 Δρmin = −0.49 e Å3
657 reflections Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
70 parameters Extinction coefficient: 0.0145 (15)
4 restraints Absolute structure: Flack (1983), with how many Friedel pairs?
Primary atom site location: structure-invariant direct methods Flack parameter: −0.03 (3)

Special details

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq Occ. (<1)
Na1 0.9427 (12) 0.9427 (12) 0.9427 (12) 0.0144 (3) 0.4738 (16)
Ba1 0.92953 (9) 0.92953 (9) 0.92953 (9) 0.0144 (3) 0.5262 (16)
Na2 0.6862 (8) 0.6862 (8) 0.6862 (8) 0.0232 (4) 0.5262 (16)
Ba2 0.70555 (8) 0.70555 (8) 0.70555 (8) 0.0232 (4) 0.4738 (16)
Fe1 0.35313 (6) 0.85313 (6) 0.64687 (6) 0.0104 (2)
Fe2 0.91362 (6) 0.08638 (6) 0.58638 (6) 0.0101 (2)
P 0.03742 (10) 0.77099 (11) 0.62578 (10) 0.0068 (2)
O1 0.9926 (5) 0.9134 (4) 0.6562 (7) 0.0461 (14)
O2 0.9463 (5) 0.6999 (6) 0.5243 (5) 0.0440 (13)
O3 0.1846 (4) 0.7653 (6) 0.5752 (5) 0.0368 (12)
O4A 0.0112 (7) 0.6985 (10) 0.7629 (8) 0.0389 (18) 0.701 (4)
O4B 0.0527 (17) 0.672 (2) 0.738 (2) 0.0389 (18) 0.299 (4)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Na1 0.0144 (3) 0.0144 (3) 0.0144 (3) −0.0019 (3) −0.0019 (3) −0.0019 (3)
Ba1 0.0144 (3) 0.0144 (3) 0.0144 (3) −0.0019 (3) −0.0019 (3) −0.0019 (3)
Na2 0.0232 (4) 0.0232 (4) 0.0232 (4) 0.0016 (3) 0.0016 (3) 0.0016 (3)
Ba2 0.0232 (4) 0.0232 (4) 0.0232 (4) 0.0016 (3) 0.0016 (3) 0.0016 (3)
Fe1 0.0104 (2) 0.0104 (2) 0.0104 (2) 0.0001 (2) −0.0001 (2) −0.0001 (2)
Fe2 0.0101 (2) 0.0101 (2) 0.0101 (2) 0.0024 (2) 0.0024 (2) −0.0024 (2)
P 0.0066 (4) 0.0073 (4) 0.0064 (4) −0.0005 (3) −0.0028 (3) 0.0010 (3)
O1 0.045 (3) 0.0170 (19) 0.076 (4) 0.0191 (19) −0.015 (3) −0.015 (2)
O2 0.029 (2) 0.061 (3) 0.042 (3) 0.003 (2) −0.025 (2) −0.031 (2)
O3 0.0120 (16) 0.063 (3) 0.035 (2) −0.0091 (18) 0.0085 (16) −0.023 (2)
O4A 0.020 (4) 0.066 (5) 0.031 (3) 0.020 (3) 0.015 (3) 0.040 (3)
O4B 0.020 (4) 0.066 (5) 0.031 (3) 0.020 (3) 0.015 (3) 0.040 (3)

Geometric parameters (Å, °)

Na1—O1i 2.864 (12) Ba2—O3xiii 2.772 (5)
Na1—O1 2.864 (12) Ba2—O3xiv 2.772 (5)
Na1—O1ii 2.864 (12) Ba2—O2ii 2.952 (5)
Na1—O4Biii 2.86 (3) Ba2—O2 2.952 (5)
Na1—O4Biv 2.86 (3) Ba2—O2i 2.952 (5)
Na1—O4Bv 2.86 (3) Ba2—O4Avi 3.047 (7)
Na1—O4Avi 3.045 (17) Ba2—O4Avii 3.047 (7)
Na1—O4Avii 3.045 (17) Ba2—O4Aviii 3.047 (7)
Na1—O4Aviii 3.045 (17) Fe1—O2ii 1.979 (4)
Na1—O2ix 2.763 (17) Fe1—O2xv 1.979 (4)
Na1—O2x 2.763 (17) Fe1—O2xvi 1.979 (4)
Na1—O2xi 2.763 (17) Fe1—O3xiii 1.990 (4)
Ba1—O1i 2.753 (7) Fe1—O3 1.990 (4)
Ba1—O1 2.753 (7) Fe1—O3xvii 1.990 (4)
Ba1—O1ii 2.753 (7) Fe1—Ba1xviii 3.6878 (19)
Ba1—O4Biii 2.89 (3) Fe1—Ba2iv 3.7867 (6)
Ba1—O4Biv 2.89 (3) Fe1—Ba2xv 3.7867 (6)
Ba1—O4Bv 2.89 (3) Fe2—O4Bxix 1.946 (18)
Ba1—O4Avi 2.902 (10) Fe2—O4Bii 1.946 (18)
Ba1—O4Avii 2.902 (10) Fe2—O4Bxii 1.946 (18)
Ba1—O4Aviii 2.902 (10) Fe2—O1xx 1.984 (5)
Ba1—O2ix 2.950 (6) Fe2—O1xxi 1.984 (5)
Ba1—O2x 2.950 (6) Fe2—O1xxii 1.984 (5)
Ba1—O2xi 2.950 (6) Fe2—O4Axix 1.982 (7)
Na2—O3xii 2.604 (8) Fe2—O4Aii 1.982 (7)
Na2—O3xiii 2.604 (8) Fe2—O4Axii 1.982 (7)
Na2—O3xiv 2.604 (8) P—O4B 1.470 (18)
Na2—O2 3.004 (6) P—O1xxiii 1.493 (4)
Na2—O2i 3.004 (6) P—O2xxiii 1.506 (4)
Na2—O2ii 3.004 (6) P—O3 1.526 (4)
Ba2—O3xii 2.772 (5) P—O4A 1.541 (7)
O1i—Na1—O1 94.9 (5) O2ix—Ba1—O2xi 55.17 (13)
O1i—Na1—O1ii 94.9 (5) O2x—Ba1—O2xi 55.17 (13)
O1—Na1—O1ii 94.9 (5) O3xii—Na2—O3xiii 100.1 (3)
O1i—Na1—O4Biii 58.0 (4) O3xii—Na2—O3xiv 100.1 (3)
O1—Na1—O4Biii 79.6 (4) O3xiii—Na2—O3xiv 100.1 (3)
O1ii—Na1—O4Biii 151.3 (7) O3xii—Na2—O2 83.46 (16)
O1i—Na1—O4Biv 151.3 (7) O3xiii—Na2—O2 158.5 (4)
O1—Na1—O4Biv 58.0 (4) O3xiv—Na2—O2 58.53 (12)
O1ii—Na1—O4Biv 79.6 (4) O3xii—Na2—O2i 58.53 (12)
O4Biii—Na1—O4Biv 118.89 (19) O3xiii—Na2—O2i 83.46 (16)
O1i—Na1—O4Bv 79.6 (4) O3xiv—Na2—O2i 158.5 (4)
O1—Na1—O4Bv 151.3 (7) O2—Na2—O2i 115.68 (18)
O1ii—Na1—O4Bv 58.0 (4) O3xii—Na2—O2ii 158.5 (4)
O4Biii—Na1—O4Bv 118.89 (19) O3xiii—Na2—O2ii 58.53 (12)
O4Biv—Na1—O4Bv 118.89 (19) O3xiv—Na2—O2ii 83.46 (16)
O1i—Na1—O4Avi 46.9 (2) O2—Na2—O2ii 115.68 (18)
O1—Na1—O4Avi 107.0 (6) O2i—Na2—O2ii 115.68 (18)
O1ii—Na1—O4Avi 49.5 (3) O3xii—Ba2—O3xiii 92.09 (15)
O1i—Na1—O4Avii 49.5 (3) O3xii—Ba2—O3xiv 92.09 (15)
O1—Na1—O4Avii 46.9 (2) O3xiii—Ba2—O3xiv 92.09 (15)
O1ii—Na1—O4Avii 107.0 (6) O3xii—Ba2—O2ii 148.54 (14)
O1i—Na1—O4Aviii 107.0 (6) O3xiii—Ba2—O2ii 57.63 (12)
O1—Na1—O4Aviii 49.5 (3) O3xiv—Ba2—O2ii 81.64 (14)
O1ii—Na1—O4Aviii 46.9 (2) O3xii—Ba2—O2 81.64 (14)
O4Avi—Na1—O4Aviii 81.1 (5) O3xiii—Ba2—O2 148.54 (14)
O4Avii—Na1—O4Aviii 81.1 (5) O3xiv—Ba2—O2 57.63 (12)
O1i—Na1—O2ix 97.97 (19) O2ii—Ba2—O2 118.95 (3)
O1—Na1—O2ix 104.0 (2) O3xii—Ba2—O2i 57.63 (12)
O1ii—Na1—O2ix 156.0 (6) O3xiii—Ba2—O2i 81.64 (14)
O4Biv—Na1—O2ix 97.9 (6) O3xiv—Ba2—O2i 148.54 (14)
O4Bv—Na1—O2ix 104.6 (6) O2ii—Ba2—O2i 118.95 (3)
O4Avi—Na1—O2ix 134.2 (2) O2—Ba2—O2i 118.95 (3)
O4Avii—Na1—O2ix 96.81 (16) O3xii—Ba2—O4Avi 104.95 (16)
O4Aviii—Na1—O2ix 144.2 (3) O3xiii—Ba2—O4Avi 83.7 (2)
O1i—Na1—O2x 156.0 (6) O3xiv—Ba2—O4Avi 162.54 (16)
O1—Na1—O2x 97.97 (19) O2ii—Ba2—O4Avi 81.80 (17)
O1ii—Na1—O2x 104.0 (2) O2—Ba2—O4Avi 127.8 (2)
O4Biii—Na1—O2x 104.6 (6) O2i—Ba2—O4Avi 47.59 (16)
O4Biv—Na1—O2x 49.4 (4) O3xii—Ba2—O4Avii 83.7 (2)
O4Bv—Na1—O2x 97.9 (6) O3xiii—Ba2—O4Avii 162.54 (16)
O4Avi—Na1—O2x 144.2 (3) O3xiv—Ba2—O4Avii 104.95 (16)
O4Avii—Na1—O2x 134.2 (2) O2ii—Ba2—O4Avii 127.8 (2)
O4Aviii—Na1—O2x 96.81 (16) O2—Ba2—O4Avii 47.59 (16)
O2ix—Na1—O2x 59.2 (4) O2i—Ba2—O4Avii 81.80 (17)
O1i—Na1—O2xi 104.0 (2) O4Avi—Ba2—O4Avii 81.1 (3)
O1—Na1—O2xi 156.0 (6) O3xii—Ba2—O4Aviii 162.54 (17)
O1ii—Na1—O2xi 97.97 (19) O3xiii—Ba2—O4Aviii 104.95 (16)
O4Biii—Na1—O2xi 97.9 (6) O3xiv—Ba2—O4Aviii 83.7 (2)
O4Biv—Na1—O2xi 104.6 (6) O2ii—Ba2—O4Aviii 47.59 (16)
O4Avi—Na1—O2xi 96.81 (16) O2—Ba2—O4Aviii 81.80 (17)
O4Avii—Na1—O2xi 144.2 (3) O2i—Ba2—O4Aviii 127.8 (2)
O4Aviii—Na1—O2xi 134.2 (2) O4Avi—Ba2—O4Aviii 81.1 (3)
O2ix—Na1—O2xi 59.2 (4) O4Avii—Ba2—O4Aviii 81.1 (3)
O2x—Na1—O2xi 59.2 (4) O2ii—Fe1—O2xv 87.3 (2)
O1i—Ba1—O1 100.10 (14) O2ii—Fe1—O2xvi 87.3 (2)
O1i—Ba1—O1ii 100.10 (14) O2xv—Fe1—O2xvi 87.3 (2)
O1—Ba1—O1ii 100.10 (14) O2ii—Fe1—O3xiii 88.26 (18)
O1i—Ba1—O4Biii 58.8 (4) O2xv—Fe1—O3xiii 89.2 (2)
O1—Ba1—O4Biii 80.9 (4) O2xvi—Fe1—O3xiii 174.5 (2)
O1ii—Ba1—O4Biii 158.5 (4) O2ii—Fe1—O3 174.5 (2)
O1i—Ba1—O4Biv 158.5 (4) O2xv—Fe1—O3 88.26 (18)
O1—Ba1—O4Biv 58.8 (4) O2xvi—Fe1—O3 89.2 (2)
O1ii—Ba1—O4Biv 80.9 (4) O3xiii—Fe1—O3 95.0 (2)
O4Biii—Ba1—O4Biv 116.8 (2) O2ii—Fe1—O3xvii 89.2 (2)
O1i—Ba1—O4Bv 80.9 (4) O2xv—Fe1—O3xvii 174.5 (2)
O1—Ba1—O4Bv 158.5 (4) O2xvi—Fe1—O3xvii 88.26 (18)
O1ii—Ba1—O4Bv 58.8 (4) O3xiii—Fe1—O3xvii 95.0 (2)
O4Biii—Ba1—O4Bv 116.8 (2) O3—Fe1—O3xvii 95.0 (2)
O4Biv—Ba1—O4Bv 116.8 (2) O4Bxix—Fe2—O4Bii 80.8 (9)
O1i—Ba1—O4Avi 49.19 (16) O4Bxix—Fe2—O4Bxii 80.8 (9)
O1—Ba1—O4Avi 114.25 (19) O4Bii—Fe2—O4Bxii 80.8 (9)
O1ii—Ba1—O4Avi 51.94 (17) O4Bxix—Fe2—O1xx 169.5 (6)
O1i—Ba1—O4Avii 51.94 (17) O4Bii—Fe2—O1xx 89.8 (8)
O1—Ba1—O4Avii 49.19 (16) O4Bxii—Fe2—O1xx 93.0 (5)
O1ii—Ba1—O4Avii 114.25 (19) O4Bxix—Fe2—O1xxi 93.0 (5)
O1i—Ba1—O4Aviii 114.25 (19) O4Bii—Fe2—O1xxi 169.5 (6)
O1—Ba1—O4Aviii 51.94 (17) O4Bxii—Fe2—O1xxi 89.8 (8)
O1ii—Ba1—O4Aviii 49.19 (16) O1xx—Fe2—O1xxi 95.5 (3)
O4Avi—Ba1—O4Aviii 86.1 (2) O4Bxix—Fe2—O1xxii 89.8 (8)
O4Avii—Ba1—O4Aviii 86.1 (2) O4Bii—Fe2—O1xxii 93.0 (5)
O1i—Ba1—O2ix 96.20 (14) O4Bxii—Fe2—O1xxii 169.5 (6)
O1—Ba1—O2ix 102.04 (15) O1xx—Fe2—O1xxii 95.5 (3)
O1ii—Ba1—O2ix 149.64 (14) O1xxi—Fe2—O1xxii 95.5 (3)
O4Biii—Ba1—O2ix 47.5 (4) O1xx—Fe2—O4Axix 168.6 (3)
O4Biv—Ba1—O2ix 93.1 (4) O1xxi—Fe2—O4Axix 77.4 (3)
O4Bv—Ba1—O2ix 99.2 (4) O1xxii—Fe2—O4Axix 94.1 (3)
O4Avi—Ba1—O2ix 132.27 (18) O4Bxix—Fe2—O4Aii 78.2 (6)
O4Avii—Ba1—O2ix 95.97 (17) O4Bii—Fe2—O4Aii 15.9 (5)
O4Aviii—Ba1—O2ix 141.66 (18) O4Bxii—Fe2—O4Aii 95.9 (8)
O1i—Ba1—O2x 149.64 (14) O1xx—Fe2—O4Aii 94.1 (3)
O1—Ba1—O2x 96.20 (14) O1xxi—Fe2—O4Aii 168.6 (3)
O1ii—Ba1—O2x 102.04 (15) O1xxii—Fe2—O4Aii 77.4 (3)
O4Biii—Ba1—O2x 99.2 (4) O4Axix—Fe2—O4Aii 94.0 (3)
O4Biv—Ba1—O2x 47.5 (4) O1xx—Fe2—O4Axii 77.4 (3)
O4Bv—Ba1—O2x 93.1 (4) O1xxi—Fe2—O4Axii 94.1 (3)
O4Avi—Ba1—O2x 141.66 (18) O1xxii—Fe2—O4Axii 168.6 (3)
O4Avii—Ba1—O2x 132.27 (18) O4Axix—Fe2—O4Axii 94.0 (3)
O4Aviii—Ba1—O2x 95.97 (17) O4Aii—Fe2—O4Axii 94.0 (3)
O2ix—Ba1—O2x 55.17 (13) O4B—P—O1xxiii 119.9 (10)
O1i—Ba1—O2xi 102.04 (15) O4B—P—O2xxiii 104.3 (11)
O1—Ba1—O2xi 149.64 (14) O1xxiii—P—O2xxiii 112.9 (3)
O1ii—Ba1—O2xi 96.20 (14) O4B—P—O3 97.0 (6)
O4Biii—Ba1—O2xi 93.1 (4) O1xxiii—P—O3 112.2 (3)
O4Biv—Ba1—O2xi 99.2 (4) O2xxiii—P—O3 109.2 (3)
O4Bv—Ba1—O2xi 47.5 (4) O4B—P—O4A 20.6 (6)
O4Avi—Ba1—O2xi 95.97 (16) O1xxiii—P—O4A 102.0 (4)
O4Avii—Ba1—O2xi 141.66 (18) O2xxiii—P—O4A 105.3 (4)
O4Aviii—Ba1—O2xi 132.27 (18) O3—P—O4A 115.1 (3)

Symmetry codes: (i) y, z, x; (ii) z, x, y; (iii) y+1/2, −z+3/2, −x+1; (iv) −x+1, y+1/2, −z+3/2; (v) −z+3/2, −x+1, y+1/2; (vi) y, z, x+1; (vii) x+1, y, z; (viii) z, x+1, y; (ix) y+1/2, −z+3/2, −x+2; (x) −x+2, y+1/2, −z+3/2; (xi) −z+3/2, −x+2, y+1/2; (xii) −y+3/2, −z+1, x+1/2; (xiii) −z+1, x+1/2, −y+3/2; (xiv) x+1/2, −y+3/2, −z+1; (xv) x−1/2, −y+3/2, −z+1; (xvi) −y+1, z+1/2, −x+3/2; (xvii) y−1/2, −z+3/2, −x+1; (xviii) −x+3/2, −y+2, z−1/2; (xix) −x+1, y−1/2, −z+3/2; (xx) −z+3/2, −x+1, y−1/2; (xxi) −y+2, z−1/2, −x+3/2; (xxii) x, y−1, z; (xxiii) x−1, y, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BR2076).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808023040/br2076sup1.cif

e-64-00i51-sup1.cif (20.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808023040/br2076Isup2.hkl

e-64-00i51-Isup2.hkl (32.3KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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