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Acta Crystallographica Section E: Crystallographic Communications logoLink to Acta Crystallographica Section E: Crystallographic Communications
. 2023 Mar 15;79(Pt 4):328–330. doi: 10.1107/S2056989023002293

Garnet-type Na3Te2(FeO4)3

Felix Eder a, Matthias Weil a,*
Editor: S Parkinb
PMCID: PMC10088310  PMID: 37057020

The garnet-type crystal structure of Na3Te2(FeO4)3 shows high similarities with its isotypic analogues Na3Te2[(Fe0.5Al0.5)O4]3 and Na3Te2(GaO4)3.

Keywords: crystal structure, garnet, oxidotellurate(VI), isotypism, structural similarity

Abstract

Na3Te2(FeO4)3 or Na3Te2Fe3O12, tris­odium ditellurium(VI) triiron(III) dodeca­oxide, was obtained in the form of single-crystals under hydro­thermal conditions. Na3Te2(FeO4)3 adopts the garnet structure type in space group Ia Inline graphic d and comprises one Na (multiplicity 24, Wyckoff letter c, site symmetry 2.22), one Te (16 a, . Inline graphic .), one Fe (24 d, Inline graphic ..) and one O atom (96 h, 1) in the asymmetric unit. The three-dimensional framework structure is built of [TeO6] octa­hedra and [FeO4] tetra­hedra by vertex-sharing. The larger Na+ cations are situated in the inter­stices of the framework and are eightfold coordinated in the form of a distorted dodeca­hedron. Qu­anti­tative structural comparisons with isotypic Na3Te2[(Fe0.5Al0.5)O4]3 and Na3Te2(GaO4)3 show a high degree of similarity between the three crystal structures.

1. Chemical context

Layered oxidotellurates(VI) comprising an alkali metal (or ammonium) and a transition metal M, such as (NH4)4(VO2)2Te2O8(OH)2·2H2O (Nagarathinam et al., 2022), Li2Ni2TeO6 (Grundish et al., 2019), Na3Ni1.5TeO6 (Grundish et al., 2020) or K2 M 2TeO6 (M = Ni, Mg, Zn, Co, Cu; Masese et al., 2018) are considered to be promising battery materials. In the quest for new representatives of this group of materials comprising K and FeIII, we obtained a phase under hydro­thermal conditions with a supposed composition of K12FeIII 6TeVI 4O27·3H2O. However, this phase is not layered but crystallizes in a cubic framework structure with positionally disordered crystal water mol­ecules [Z = 4, space group I Inline graphic 3d, a = 14.7307 (12) Å at room temperature; Eder & Weil, 2023], which is closely related to the phase K12+6x Fe6Te4–x O27 [x = 0.222 (4), Z = 4, space group I Inline graphic 3d, a = 14.7440 (10) Å at 100 K; Albrecht et al., 2021]. With the intention of synthesizing the possible Na-analogue Na12FeIII 6TeVI 4O27·3H2O, we obtained garnet-type Na3Te2(FeO4)3 instead, and report here its crystal structure and qu­anti­tative comparisons with related crystal structures.

2. Structural commentary

The garnet supergroup has the general formula {X 3}[Y 2](Z 3)φ 12 and includes all phases, which crystallize isostructurally with garnet, regardless of the type of elements present at the four atomic sites (Grew et al., 2013). The crystal structure of garnet comprises a three-dimensional framework built of [ 6] octa­hedra and (Zφ4) tetra­hedra in which each octa­hedron is joined to six others through vertex-sharing tetra­hedra. In turn, each tetra­hedron shares its vertices with four octa­hedra, so that the composition of the framework is Y 2 Z 3 φ 12. Larger X atoms occupy positions in the inter­stices of the framework and are eightfold coordinated in the form of a distorted dodeca­hedron (Wells, 1975). In a crystal–chemical sense, the final composition can therefore be expressed as {X 3}[8do][Y 2][6o](Z 3 [4t]12, or as {X 3}[8do][Y 2][6o](Z [4t] φ 4)3. In the title compound, Na takes the X position (multiplicity 24, Wyckoff letter c, site symmetry 2.22), Te the Y position (16 a, . Inline graphic .), Fe the Z position (24 d, Inline graphic ..) and O the φ position (96 h, 1). The crystal structure of Na3Te2(FeO4)3 is displayed in Fig. 1. Bond-valence sums (Brown, 2002) for all atoms were computed with the parameters of Brese & O’Keeffe (1991). The values (in valence units) of 1.19 for Na, 6.00 for Te, 2.98 for Fe and 2.04 for O are in very good agreement with the expected values of 1, 6, 3 and 2, respectively.

Figure 1.

Figure 1

Projection of the garnet-type crystal structure of Na3Te2(FeO4)3 along [0 Inline graphic 0]. Displacement ellipsoids are drawn at the 90% probability level. [TeO6] octa­hedra (red) and (FeO4) tetra­hedra (blue) are given in the polyhedral representation, Na atoms as green ellipsoids and O atoms as white ellipsoids.

The garnet supergroup includes several chemical classes, which is also reflected by the high number of phases that adopt the garnet structure type. A search in the ICSD (version 2022-1; Zagorac et al., 2019), using the garnet structure type in space group Ia Inline graphic d and with Si on the Z position as search field revealed about 420 entries, and with atoms other than Si on the Z position about 350 entries. With Te on the Y position, only five phases were found, including the mineral yafsoanite [ideally Ca3Te2(ZnO4)3, Jarosch & Zemann, 1989; Mills et al., 2010], the Li-conducting Nd3(Te2–x Sb x )(Li3+x O4)3 (x = 0.05, 0.10) (O’Callaghan et al., 2008), Na3Te2[(Fe0.5Al0.5)O4]3 (Wedel & Sugiyama, 1999) and Na3Te2(GaO4)3 (Frau et al., 2008). The latter two phases comprise Na on the X position and, with respect to the title compound, therefore are the chemically most related compounds. A comparison of relevant bond lengths in the three garnets, together with structural similarity parameters, as revealed by the program compstru (de la Flor et al., 2016) available at the Bilbao Crystallographic Server (Aroyo et al., 2006), is given in Table 1. The cations occupying the Z site apparently influence the two Na—O bond lengths in the crystal structures, although the ionic radii (Shannon, 1976) of Z do not directly correlate with this behaviour. The title compound with Z = Fe (ionic radius 0.49 Å) has the longest Na—O bonds, followed by the mixed-occupied compound with Z = (Fe,Al) (averaged ionic radius 0.44 Å) and the compound with Z = Ga (ionic radius 0.47 Å). On the other hand, the Te—O bond lengths in the three garnet structures are virtually identical.

Table 1. Selected bond lengths (Å) in related garnet-type Na3Te2(ZO4)3 oxidotellurates(VI) and their structure similarity parameters relative to Na3Te2(FeO4)3 .

  Na3Te2(FeO4)3 Na3Te2[(Al,Fe)O4]3 Na3Te2(GaO4)3
Na1—O1 (4×) 2.4208 (10) 2.396 (3) 2.3907 (17)
Na1—O1 (4×) 2.6226 (10) 2.597 (3) 2.5609 (17)
Te1—O1 (6×) 1.9169 (9) 1.914 (2) 1.9124 (17)
M1—O1 (4×) 1.8680 (9) 1.829 (2) 1.8405 (16)
       
Degree of lattice distortion, S   0.0064 0.0079
Atomic displacement of O1 a (Å)   0.0205 0.0322
Measure of similarity, Δ   0.001 0.002

Note: (a) The three other atomic sites do not show a displacement due to their site symmetries.

An X-ray powder diffraction pattern of Na3Te2(FeO4)3 has been deposited with the ICDD (PDF 00-048-0300; Gates-Rector & Blanton, 2019) without giving atomic coordinates for the O-atom site or displacement parameters for the atoms. The corresponding unit-cell parameter a = 12.5257 (1) Å determined from room-temperature powder X-ray measurement data is in very good agreement with the one from single-crystal data (Table 2). In the context of investigating the magnetic ordering of FeIII on the Z sites, neutron powder data recorded at room temperature were also reported for Na3Te2(FeO4)3 (Plakhtii et al., 1977).

Table 2. Experimental details.

Crystal data
Chemical formula Na3Te2Fe3O12
M r 683.72
Crystal system, space group Cubic, I a Inline graphic d
Temperature (K) 296
a (Å) 12.5276 (9)
V3) 1966.1 (4)
Z 8
Radiation type Mo Kα
μ (mm−1) 10.39
Crystal size (mm) 0.06 × 0.06 × 0.06
 
Data collection
Diffractometer Bruker APEXII CCD
Absorption correction Multi-scan (SADABS; Krause et al., 2015)
T min, T max 0.677, 0.748
No. of measured, independent and observed [I > 2σ(I)] reflections 42303, 569, 446
R int 0.060
(sin θ/λ)max−1) 0.934
 
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S 0.017, 0.041, 1.16
No. of reflections 569
No. of parameters 18
Δρmax, Δρmin (e Å−3) 1.25, −0.68

Computer programs: APEX3 and SAINT (Bruker, 2016), SHELXT (Sheldrick, 2015a ), SHELXL (Sheldrick, 2015b ), ATOMS for Windows (Dowty, 2006) and publCIF (Westrip, 2010).

3. Synthesis and crystallization

The solid educts Fe(NO3)3·9H2O, TeO2, H6TeO6 and NaOH were weighed in the molar ratios 2:1:2:15 and placed into a Teflon container (inner volume ca 5 ml). The container was filled to about 2/3 of its volume with water, closed with a Teflon lid and embedded into a steel autoclave. The hydro­thermal experiment was conducted at 473 K for five days. The solid product was filtered off, washed with water and ethanol and dried in air. It consisted of light-brown microcrystalline material and a few amber-coloured cuboid crystals of Na3Te2(FeO4)3, as well as a very few small yellowish platy crystals of an unknown phase. Preliminary single-crystal measurements of the latter indicated a unit cell with hexa­gonal metrics (a = 5.252, c = 15.724 Å) and obvious twinning, which has precluded a structure solution so far. Similar metrics were found for Na2GeTeO6 (Woodward et al., 1998). The powder X-ray diffraction pattern of the bulk revealed Na3Te2(FeO4)3 as a side product and the unknown phase (assuming a close relation with Na2GeTeO6) as the main phase, in an approximate mass ratio of 0.15:0.85.

4. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S2056989023002293/pk2684sup1.cif

e-79-00328-sup1.cif (1.3MB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989023002293/pk2684Isup2.hkl

e-79-00328-Isup2.hkl (54.8KB, hkl)

CCDC reference: 2247314

Additional supporting information: crystallographic information; 3D view; checkCIF report

Acknowledgments

We thank Ruben do Carmo for assistance during preparative studies. The X-ray centre of TU Wien is acknowledged for providing access to the single-crystal and powder X-ray diffractometers.

supplementary crystallographic information

Crystal data

Na3Te2Fe3O12 Mo Kα radiation, λ = 0.71073 Å
Mr = 683.72 Cell parameters from 6128 reflections
Cubic, Ia3d θ = 4.0–41.1°
a = 12.5276 (9) Å µ = 10.39 mm1
V = 1966.1 (4) Å3 T = 296 K
Z = 8 Cube, amber
F(000) = 2488 0.06 × 0.06 × 0.06 mm
Dx = 4.620 Mg m3

Data collection

Bruker APEXII CCD diffractometer 446 reflections with I > 2σ(I)
ω– and φ–scans Rint = 0.060
Absorption correction: multi-scan (SADABS; Krause et al., 2015) θmax = 41.6°, θmin = 4.0°
Tmin = 0.677, Tmax = 0.748 h = −23→23
42303 measured reflections k = −23→23
569 independent reflections l = −23→23

Refinement

Refinement on F2 0 restraints
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0169P)2 + 1.9053P] where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.017 (Δ/σ)max < 0.001
wR(F2) = 0.041 Δρmax = 1.25 e Å3
S = 1.16 Δρmin = −0.68 e Å3
569 reflections Extinction correction: SHELXL-2019/2 (Sheldrick 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
18 parameters Extinction coefficient: 0.00158 (6)

Special details

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

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

x y z Uiso*/Ueq
Na1 0.250000 0.375000 0.500000 0.01227 (18)
Te1 0.500000 0.500000 0.500000 0.00480 (5)
Fe1 0.250000 0.625000 0.500000 0.00637 (7)
O1 0.35650 (7) 0.53021 (8) 0.45633 (8) 0.00976 (16)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Na1 0.0150 (3) 0.0068 (4) 0.0150 (3) 0.000 0.0012 (4) 0.000
Te1 0.00480 (5) 0.00480 (5) 0.00480 (5) 0.00038 (3) 0.00038 (3) 0.00038 (3)
Fe1 0.00652 (9) 0.00605 (14) 0.00652 (9) 0.000 0.000 0.000
O1 0.0068 (4) 0.0106 (4) 0.0119 (4) 0.0023 (3) −0.0013 (3) −0.0006 (3)

Geometric parameters (Å, º)

Na1—O1i 2.4208 (10) Te1—O1viii 1.9169 (9)
Na1—O1ii 2.4208 (10) Te1—O1ix 1.9169 (9)
Na1—O1iii 2.4208 (10) Te1—O1x 1.9169 (9)
Na1—O1 2.4208 (10) Te1—O1vii 1.9169 (9)
Na1—O1iv 2.6226 (10) Te1—O1xi 1.9169 (9)
Na1—O1v 2.6226 (10) Fe1—O1xii 1.8680 (9)
Na1—O1vi 2.6226 (10) Fe1—O1ii 1.8680 (9)
Na1—O1vii 2.6226 (10) Fe1—O1xiii 1.8680 (9)
Te1—O1 1.9169 (9) Fe1—O1 1.8680 (9)
O1i—Na1—O1ii 153.42 (4) O1—Te1—O1viii 91.50 (4)
O1i—Na1—O1iii 73.12 (4) O1—Te1—O1ix 88.50 (4)
O1ii—Na1—O1iii 113.33 (4) O1viii—Te1—O1ix 180.0
O1i—Na1—O1 113.33 (4) O1—Te1—O1x 91.50 (4)
O1ii—Na1—O1 73.12 (4) O1viii—Te1—O1x 88.50 (4)
O1iii—Na1—O1 153.42 (4) O1ix—Te1—O1x 91.50 (4)
O1i—Na1—O1iv 125.56 (2) O1—Te1—O1vii 88.50 (4)
O1ii—Na1—O1iv 77.63 (3) O1viii—Te1—O1vii 91.50 (4)
O1iii—Na1—O1iv 63.92 (4) O1ix—Te1—O1vii 88.50 (4)
O1—Na1—O1iv 94.14 (3) O1x—Te1—O1vii 180.0
O1i—Na1—O1v 94.14 (3) O1—Te1—O1xi 180.0
O1ii—Na1—O1v 63.92 (4) O1viii—Te1—O1xi 88.50 (4)
O1iii—Na1—O1v 77.63 (3) O1ix—Te1—O1xi 91.50 (4)
O1—Na1—O1v 125.56 (2) O1x—Te1—O1xi 88.50 (4)
O1iv—Na1—O1v 106.99 (4) O1vii—Te1—O1xi 91.50 (4)
O1i—Na1—O1vi 63.92 (4) O1xii—Fe1—O1ii 113.83 (3)
O1ii—Na1—O1vi 94.14 (3) O1xii—Fe1—O1xiii 101.06 (6)
O1iii—Na1—O1vi 125.56 (2) O1ii—Fe1—O1xiii 113.83 (3)
O1—Na1—O1vi 77.63 (3) O1xii—Fe1—O1 113.83 (3)
O1iv—Na1—O1vi 169.86 (4) O1ii—Fe1—O1 101.06 (6)
O1v—Na1—O1vi 73.94 (4) O1xiii—Fe1—O1 113.83 (3)
O1i—Na1—O1vii 77.63 (3) Fe1—O1—Te1 135.38 (5)
O1ii—Na1—O1vii 125.56 (2) Fe1—O1—Na1 92.91 (4)
O1iii—Na1—O1vii 94.14 (3) Te1—O1—Na1 107.08 (4)
O1—Na1—O1vii 63.92 (4) Fe1—O1—Na1ix 116.33 (4)
O1iv—Na1—O1vii 73.94 (4) Te1—O1—Na1ix 99.78 (4)
O1v—Na1—O1vii 169.86 (4) Na1—O1—Na1ix 98.95 (3)
O1vi—Na1—O1vii 106.99 (4)

Symmetry codes: (i) −z+3/4, −y+3/4, −x+3/4; (ii) −x+1/2, y, −z+1; (iii) z−1/4, −y+3/4, x+1/4; (iv) y−1/4, −x+3/4, z+1/4; (v) −z+1/2, x, −y+1; (vi) −y+3/4, −x+3/4, −z+3/4; (vii) z, x, y; (viii) −y+1, −z+1, −x+1; (ix) y, z, x; (x) −z+1, −x+1, −y+1; (xi) −x+1, −y+1, −z+1; (xii) −z+3/4, −y+5/4, x+1/4; (xiii) z−1/4, −y+5/4, −x+3/4.

Funding Statement

The authors acknowledge TU Wien Bibliothek for financial support through its Open Access Funding Programme.

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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 datablock(s) I, global. DOI: 10.1107/S2056989023002293/pk2684sup1.cif

e-79-00328-sup1.cif (1.3MB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989023002293/pk2684Isup2.hkl

e-79-00328-Isup2.hkl (54.8KB, hkl)

CCDC reference: 2247314

Additional supporting information: crystallographic information; 3D view; checkCIF report


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