research communications
1.67Zn1.67Fe1.33(PO4)3
of a sodium, zinc and iron(III)-based non-stoichiometric phosphate with an alluaudite-like structure: NaaLaboratoire de Chimie du Solide Appliquée, Faculté des Sciences, Université Mohammed V, Avenue Ibn Battouta, BP 1014, Rabat, Morocco
*Correspondence e-mail: j_khmiyas@yahoo.fr
The new title compound, disodium dizinc iron(III) tris(phosphate), Na1.67Zn1.67Fe1.33(PO4)3, which belongs to the alluaudite family, has been synthesized by solid-state reactions. In this structure, all atoms are in general positions except for four, which are located on special positions of the C2/c This structure is characterized by cation substitutional disorder at two sites, one situated on the special position 4e (2) and the other on the general position 8f. The 4e site is partially occupied by Na+ [0.332 (3)], whereas the 8f site is entirely filled by a mixture of Fe and Zn. The full-occupancy sodium and zinc atoms are located at the Wyckoff positions on the inversion center 4a (-1) and on the twofold rotation axis 4e, respectively. of the occupancy ratios, bond-valence analysis and the electrical neutrality requirement of the structure lead to the given composition for the title compound. The three-dimensional framework of this structure consists of kinked chains of edge-sharing octahedra stacked parallel to [10-1]. The chains are formed by a succession of trimers based on [ZnO6] octahedra and the mixed-cation FeIII/ZnII [(Fe/Zn)O6] octahedra [FeIII:ZnIII ratio 0.668 (3)/0.332 (3)]. Continuous chains are held together by PO4 phosphate groups, forming polyhedral sheets perpendicular to [010]. The stacked sheets delimit two types of tunnels parallel to the c axis in which the sodium cations are located. Each Na+ cation is coordinated by eight O atoms. The disorder of Na in the tunnel might presage ionic mobility for this material.
Keywords: crystal structure; transition-metal phosphates; solid-state reaction synthesis; alluaudite structure type; Na1.67Zn1.67Fe1.33(PO4)3.
CCDC reference: 1402019
1. Chemical context
Alkali transition-metal phosphates belonging to the alluaudite family constitute one of the most diverse and rich classes of minerals, and have been studied intensively over the last few years. Owing to their outstanding physico-chemical properties, these compounds have many potential applications in various fields, such as et al., 2005) and as promising cathodes for sodium-ion batteries through the presence of mobile cations located in the tunnels of the open three-dimensional framework (Huang et al., 2015). In their recent study, Huang et al. (2015) point out that the electrochemical performance is not only associated with morphology, but also with the electronic and crystalline structure.
(KacimiAccordingly, a large number of alluaudite phases with alkali cations in the tunnels have been reported. Nevertheless, the presence of alkali metals in the tunnels of synthetic alluaudite phases is frequently accompanied by cationic distributions that lead to non-stoichiometric compositions, such as: (Na0.38,Ca0.31)MgFe2(PO4)3 (Zid et al., 2005); NaFe3.67(PO4)3 (Korzenski et al., 1998); Cu1.35Fe3(PO4)3 (Warner et al., 1993); K0.53Mn2.37Fe1.24(PO4)3 (Hidouri & Ben Amara, 2011); Na1.79Mg1.79Fe1.21(PO4)3 (Hidouri et al., 2003); Na1.50Mn2.48Al0.85(PO4)3 (Hatert, 2006); Na1−xLixMnFe2(PO4)3 where x = 0, 0.25, 0.50, and 0.75 (Hermann et al., 2002). As part of our study on alluaudite-related phosphates (Bouraima et al., 2015; Assani et al., 2011), we report the synthesis and the of a new sodium, zinc and iron-based non-stoichiometric phosphate, namely Na1.67Zn1.67Fe1.33(PO4)3.
2. Structural commentary
The alluaudite structure of the title compound crystallizes in the monoclinic C2/c, with Z = 4. The principal building units of the are represented in Fig. 1. of the occupancy fractions, bond-valence analysis based on the formula proposed by Brown & Altermatt (1985) and the required electrical neutrality of the structure lead to the formula Na1.67Zn1.67Fe1.33(PO4)3 for the title compound. The mixed Fe1 and Zn1 atoms are located at the general position 8f with Fe3+/Zn2+ occupancy fractions of 0.668 (3)/0.332 (3), and form a highly distorted [(Fe1/Zn1)O6] octahedral group, with Fe3+/Zn2+—O bond lengths ranging from 1.951 (1) to 2.209 (1)Å. The Zn2 atom is surrounded by six oxygen atoms, building a slightly distorted octahedron with an average Zn2—O bond length of 2.153 (1) Å.
The 6] octahedra leading to the formation of [(Fe1,Zn1)2O10] dimers that are connected by a common edge to [Zn2O6] octahedra, as shown in Fig. 2. These chains are linked by PO4 tetrahedral groups, forming a stack of sheets perpendicular to [010] and alternating with sodium layers, as shown in Fig. 3, which reveal small tunnels along the [201] direction. The three-dimensional framework also encloses two types of large tunnels, in which the Na+ cations reside, as shown in Fig. 4. The site 4e centred on the first tunnel is partially occupied by Na1 [0.332 (3)], whereas Na2 occupies site 4a centred on the second tunnel. Each sodium atom is surrounded by eight oxygen atoms with Na1—O and Na2—O bond lengths in the ranges 2.448 (1)–2.908 (2) Å, and 2.324 (1)–2.901 (1) Å, respectively. The displacement ellipsoids of the partially occupied atom Na1 are rather larger than those of the rest of the atoms. Most probably this is due to the size of the channels, which allows atom Na1 to have more freedom. The disorder of Na in the tunnel may presage ionic mobility for this material.
of this phosphate compound consists of infinite kinked chains of two edge-sharing [Fe1/Zn1O3. Synthesis and crystallization
Single crystals of Na1.67Zn1.67Fe1.33(PO4)3 were synthesised by conventional solid-state reaction (Girolami et al., 1999). The nitrate-based sodium, zinc and iron precursors, in addition to the 85 wt% H3PO4 were taken in proportions corresponding to the molar ratio Na:Zn:Fe:P = 2:2:1:3. The resulting reaction mixture was ground in an agate mortar and progressively heated in a platinum crucible to the melting temperature of 1135 K. The melted product was cooled at a rate of 5 K/h. The product was obtained as transparent brown crystals corresponding to the title phosphate.
4. Refinement
Crystal data, data collection and structure . Refinements of the site-occupancy factors of the metal site 8f revealed the ratio of Fe1:Zn1 = 0.668 (3):0.332 (3), whereas the the occupancy fraction of Na1 was constrained to that of Zn1 in order to maintain electrical neutrality. The highest peak and the deepest hole in the final difference Fourier map are at 0.72 and 0.40 Å from O1 and Zn2, respectively.
details are summarized in Table 1Supporting information
CCDC reference: 1402019
10.1107/S2056989015009767/pk2551sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S2056989015009767/pk2551Isup2.hkl
Alkali transition-metal phosphates belonging to the alluaudite family constitute one of the most diverse and rich classes of minerals, and have been studied intensively over the last few years. Owing to their outstanding physico-chemical properties, these compounds have many potential applications in various fields, such as
(Kacimi et al., 2005) and as promising cathodes for sodium-ion batteries through the presence of mobile cations located in the tunnels of the open three-dimensional framework (Huang et al., 2015). In their recent study, Huang et al. (2015) point out that the electrochemical performance is not only associated with morphology, but also with electronic and crystalline structure.Accordingly, a large number of alluaudite phases with alkali cations in the tunnels have been reported. Nevertheless, the presence of alkali metals in the tunnels of synthetic alluaudite phases is frequently accompanied by cationic distributions that lead to non-stoichiometric compositions, such as: (Na0.38,Ca0.31)MgFe2(PO4)3 (Zid et al., 2005); NaFe3.67(PO4)3 (Korzenski et al., 1998); Cu1.35Fe3(PO4)3 (Warner et al., 1993); K0.53Mn2.37Fe1.24(PO4)3 (Hidouri & Ben Amara, 2011); Na1.79Mg1.79Fe1.21(PO4)3 (Hidouri et al., 2003); Na1.50Mn2.48Al0.85(PO4)3 (Hatert, 2006); Na1-xLixMnFe2(PO4)3 where x = 0, 0.25, 0.50, and 0.75 (Hermann et al., 2002). As part of our study on alluaudite-related phosphates (Bouraima et al., 2015; Assani et al., 2011), we report the synthesis and the
of a new sodium, zinc and iron-based non-stoichiometric phosphate, namely Na1.67Zn1.67Fe1.33(PO4)3.The alluaudite structure of the title compound crystallizes in the monoclinic
C2/c, with Z = 4. The principal building units of the are represented in Fig. 1. of the occupancy fractions, bond-valence analysis based on the formula proposed by Brown & Altermatt (1985) and the required electrical neutrality of the structure lead to the formula Na1.67Zn1.67Fe1.33(PO4)3 for the title compound. The mixed Fe1 and Zn1 atoms are located at the general position 8f with Fe3+/Zn2+ occupancy fractions of 0.668 (3)/0.332 (3), and form a highly distorted [(Fe1/Zn1)O6] octahedral group, with Fe3+/Zn2+—O bond lengths ranging from 1.951 (1) to 2.209 (1)Å. The Zn2 atom is surrounded by six oxygen atoms, building a slightly distorted octahedron with an average Zn2—O bond length of 2.153 (1) Å.The
of this phosphate compound consists of infinite kinked chains of two edge-sharing [Fe1/Zn1O6] octahedra leading to the formation of [(Fe1,Zn1)2O10] dimers that are connected by a common edge to [Zn2O6] octahedra, as shown in Fig. 2. These chains are linked by PO4 tetrahedral groups, forming a stack of sheets perpendicular to [010] and alternating with sodium layers, as shown in Fig. 3, which reveal small tunnels along the [201] direction. The three-dimensional framework also encloses two types of large tunnels, in which the Na+ cations reside, as shown in Fig. 4. The site 4e centred on the first tunnel is partially occupied by Na1 [0.332 (3)], whereas Na2 occupies site 4a centred on the second tunnel. Each sodium atom is surrounded by eight oxygen atoms with Na1—O and Na2—O bond lengths in the ranges 2.448 (1)–2.908 (2) Å, and 2.324 (1)–2.901 (1) Å, respectively. The displacement ellipsoids of the partially occupied atom Na1 are rather larger than those of the rest of the atoms. Most probably this is due to the size of the channels, which allows atom Na1 to have more freedom. The disorder of Na in the tunnel may presage ionic mobility for this material.Single crystals of Na1.67Zn1.67Fe1.33(PO4)3 were synthesised by conventional solid-state reaction (Girolami et al., 1999). The nitrate-based sodium, zinc and iron precursors, in addition to the 85 wt% H3PO4 were taken in proportions corresponding to the molar ratio Na:Zn:Fe:P = 2:2:1:3. The resulting reaction mixture was ground in an agate mortar and progressively heated in a platinum crucible to the melting temperature of 1135 K. The melted product was cooled at a rate of 5 K/h. The product was obtained as transparent gray [brown in CIF] crystals corresponding to the title phosphate.
Crystal data, data collection and structure
details are summarized in Table 1. Refinements of the site-occupancy factors of the metal site 8f revealed the ratio of Fe1:Zn1 = 0.668 (3):0.332 (3), whereas the the occupancy fraction of Na1 was constrained to that of Zn1 in order to maintain electrical neutrality. The highest peak and the deepest hole in the final difference Fourier map are at 0.72 and 0.40 Å from O1 and Zn2, respectively.Data collection: APEX2 (Bruker, 2009); cell
SAINT (Bruker, 2009); data reduction: SAINT (Bruker, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEPIII (Burnett & Johnson, 1996), ORTEP-3 for Windows Farrugia, 2012) and DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).Fig. 1. The principal building units in the structure of the title compound. Displacement ellipsoids are drawn at the 50% probability level. Symmetry codes:(i) x + 1/2, y + 1/2, z; (ii) -x + 3/2, y + 1/2, -z + 1/2; (iii) -x + 3/2, -y + 3/2, -z + 1; (iv) -x + 3/2, -y + 3/2, -z; (v) -x + 1, -y + 1, -z; (vi) -x + 1, y, -z + 1/2; (vii) x, -y + 1, z + 1/2; (viii) x - 1/2, -y + 3/2, z - 1/2; (ix) -x + 2, y, -z + 3/2; (x) -x + 2, -y + 1, -z + 1; (xi) x + 1/2, -y + 1/2, z + 1/2; (xii) -x + 3/2, -y + 1/2, -z + 1; (xiii) x, -y + 1, z - 1/2. | |
Fig. 2. A view along b axis of a sheet resulting from chains connected by vertices of PO4 tetrahedra. | |
Fig. 3. A stack of layers perpendicular to the b axis, showing small tunnels along the [201] direction. | |
Fig. 4. Polyhedral representation of Na1.67Zn1.67Fe1.33(PO4)3 showing tunnels running along the [001] direction. |
Na1.67Zn1.67Fe1.33(PO4)3 | F(000) = 977 |
Mr = 506.59 | Dx = 3.904 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -c 2yc | Cell parameters from 2101 reflections |
a = 11.7545 (4) Å | θ = 2.5–36.3° |
b = 12.5080 (4) Å | µ = 7.52 mm−1 |
c = 6.4014 (2) Å | T = 296 K |
β = 113.507 (1)° | Block, brown |
V = 863.06 (5) Å3 | 0.31 × 0.25 × 0.19 mm |
Z = 4 |
Bruker X8 APEX diffractometer | 2101 independent reflections |
Radiation source: fine-focus sealed tube | 1997 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.031 |
ϕ and ω scans | θmax = 36.3°, θmin = 2.5° |
Absorption correction: multi-scan (SADABS; Bruker, 2009) | h = −19→16 |
Tmin = 0.504, Tmax = 0.748 | k = −20→20 |
18880 measured reflections | l = −10→10 |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | w = 1/[σ2(Fo2) + (0.016P)2 + 1.8532P] where P = (Fo2 + 2Fc2)/3 |
R[F2 > 2σ(F2)] = 0.017 | (Δ/σ)max = 0.001 |
wR(F2) = 0.046 | Δρmax = 0.65 e Å−3 |
S = 1.19 | Δρmin = −1.20 e Å−3 |
2101 reflections | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
96 parameters | Extinction coefficient: 0.0027 (2) |
Na1.67Zn1.67Fe1.33(PO4)3 | V = 863.06 (5) Å3 |
Mr = 506.59 | Z = 4 |
Monoclinic, C2/c | Mo Kα radiation |
a = 11.7545 (4) Å | µ = 7.52 mm−1 |
b = 12.5080 (4) Å | T = 296 K |
c = 6.4014 (2) Å | 0.31 × 0.25 × 0.19 mm |
β = 113.507 (1)° |
Bruker X8 APEX diffractometer | 2101 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2009) | 1997 reflections with I > 2σ(I) |
Tmin = 0.504, Tmax = 0.748 | Rint = 0.031 |
18880 measured reflections |
R[F2 > 2σ(F2)] = 0.017 | 96 parameters |
wR(F2) = 0.046 | 0 restraints |
S = 1.19 | Δρmax = 0.65 e Å−3 |
2101 reflections | Δρmin = −1.20 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. Reflections were merged by SHELXL according to the crystal class for the calculation of statistics and refinement. _reflns_Friedel_fraction is defined as the number of unique Friedel pairs measured divided by the number that would be possible theoretically, ignoring centric projections and systematic absences. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Fe1 | 0.71738 (2) | 0.84648 (2) | 0.12925 (3) | 0.00552 (5) | 0.668 (3) |
Zn1 | 0.71738 (2) | 0.84648 (2) | 0.12925 (3) | 0.00552 (5) | 0.332 (3) |
Zn2 | 0.5000 | 0.73133 (2) | 0.2500 | 0.00966 (5) | |
P1 | 0.76212 (3) | 0.60983 (2) | 0.37448 (5) | 0.00388 (6) | |
P2 | 0.5000 | 0.28835 (3) | 0.2500 | 0.00330 (7) | |
Na1 | 1.0000 | 0.49141 (19) | 0.7500 | 0.0356 (7) | 0.664 (6) |
Na2 | 0.5000 | 0.5000 | 0.0000 | 0.01511 (18) | |
O1 | 0.83510 (9) | 0.66524 (7) | 0.60760 (15) | 0.00695 (15) | |
O2 | 0.77771 (9) | 0.67779 (8) | 0.18481 (15) | 0.00760 (15) | |
O6 | 0.45837 (8) | 0.21761 (8) | 0.03327 (15) | 0.00622 (15) | |
O3 | 0.62448 (9) | 0.60224 (8) | 0.32496 (16) | 0.00806 (16) | |
O5 | 0.39712 (9) | 0.36396 (8) | 0.24820 (16) | 0.00747 (16) | |
O4 | 0.82109 (10) | 0.49950 (8) | 0.38406 (18) | 0.01105 (17) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Fe1 | 0.00523 (7) | 0.00632 (7) | 0.00583 (7) | −0.00082 (5) | 0.00307 (5) | −0.00067 (5) |
Zn1 | 0.00523 (7) | 0.00632 (7) | 0.00583 (7) | −0.00082 (5) | 0.00307 (5) | −0.00067 (5) |
Zn2 | 0.01124 (10) | 0.00917 (10) | 0.01083 (10) | 0.000 | 0.00679 (8) | 0.000 |
P1 | 0.00555 (12) | 0.00355 (11) | 0.00280 (11) | −0.00051 (9) | 0.00192 (9) | −0.00023 (8) |
P2 | 0.00319 (15) | 0.00365 (15) | 0.00256 (15) | 0.000 | 0.00063 (12) | 0.000 |
Na1 | 0.0167 (8) | 0.0452 (13) | 0.0345 (11) | 0.000 | −0.0008 (7) | 0.000 |
Na2 | 0.0221 (4) | 0.0079 (3) | 0.0091 (3) | 0.0024 (3) | −0.0004 (3) | 0.0006 (3) |
O1 | 0.0098 (4) | 0.0072 (4) | 0.0035 (3) | −0.0020 (3) | 0.0022 (3) | −0.0015 (3) |
O2 | 0.0090 (4) | 0.0101 (4) | 0.0043 (3) | −0.0022 (3) | 0.0032 (3) | 0.0013 (3) |
O6 | 0.0057 (3) | 0.0081 (4) | 0.0044 (3) | −0.0004 (3) | 0.0015 (3) | −0.0024 (3) |
O3 | 0.0068 (4) | 0.0083 (4) | 0.0101 (4) | −0.0015 (3) | 0.0044 (3) | −0.0006 (3) |
O5 | 0.0055 (3) | 0.0064 (3) | 0.0092 (4) | 0.0012 (3) | 0.0016 (3) | −0.0029 (3) |
O4 | 0.0147 (4) | 0.0062 (4) | 0.0125 (4) | 0.0026 (3) | 0.0057 (3) | −0.0019 (3) |
Fe1—O5i | 1.9514 (10) | P2—O6 | 1.5510 (9) |
Fe1—O4ii | 1.9607 (10) | P2—O6vi | 1.5510 (9) |
Fe1—O1iii | 2.0170 (10) | Na1—O4ix | 2.4476 (11) |
Fe1—O2iv | 2.0567 (10) | Na1—O4 | 2.4476 (11) |
Fe1—O6v | 2.0684 (9) | Na1—O4x | 2.5713 (12) |
Fe1—O2 | 2.2091 (10) | Na1—O4vii | 2.5713 (12) |
Zn2—O3vi | 2.1019 (10) | Na1—O1 | 2.812 (2) |
Zn2—O3 | 2.1019 (10) | Na1—O1ix | 2.812 (2) |
Zn2—O6vii | 2.1549 (10) | Na1—O6xi | 2.908 (2) |
Zn2—O6v | 2.1549 (10) | Na1—O6xii | 2.908 (2) |
Zn2—O1iii | 2.2028 (9) | Na2—O5xiii | 2.3239 (9) |
Zn2—O1viii | 2.2028 (9) | Na2—O5vi | 2.3239 (9) |
P1—O3 | 1.5225 (10) | Na2—O3 | 2.3823 (9) |
P1—O4 | 1.5345 (10) | Na2—O3v | 2.3824 (9) |
P1—O2 | 1.5518 (10) | Na2—O3xiii | 2.5179 (10) |
P1—O1 | 1.5563 (9) | Na2—O3vi | 2.5179 (10) |
P2—O5 | 1.5317 (10) | Na2—O5v | 2.9008 (10) |
P2—O5vi | 1.5317 (10) | Na2—O5 | 2.9008 (10) |
O5i—Fe1—O4ii | 95.89 (4) | O4—Na1—O1 | 55.92 (4) |
O5i—Fe1—O1iii | 109.05 (4) | O4x—Na1—O1 | 114.04 (7) |
O4ii—Fe1—O1iii | 88.00 (4) | O4vii—Na1—O1 | 61.59 (4) |
O5i—Fe1—O2iv | 87.13 (4) | O4ix—Na1—O1ix | 55.92 (4) |
O4ii—Fe1—O2iv | 101.39 (4) | O4—Na1—O1ix | 119.76 (8) |
O1iii—Fe1—O2iv | 160.53 (4) | O4x—Na1—O1ix | 61.58 (4) |
O5i—Fe1—O6v | 161.52 (4) | O4vii—Na1—O1ix | 114.04 (7) |
O4ii—Fe1—O6v | 100.93 (4) | O1—Na1—O1ix | 78.70 (7) |
O1iii—Fe1—O6v | 79.35 (4) | O4ix—Na1—O6xi | 114.24 (8) |
O2iv—Fe1—O6v | 82.12 (4) | O4—Na1—O6xi | 70.35 (5) |
O5i—Fe1—O2 | 79.41 (4) | O4x—Na1—O6xi | 83.40 (5) |
O4ii—Fe1—O2 | 173.23 (4) | O4vii—Na1—O6xi | 101.22 (6) |
O1iii—Fe1—O2 | 88.95 (4) | O1—Na1—O6xi | 125.27 (3) |
O2iv—Fe1—O2 | 83.34 (4) | O1ix—Na1—O6xi | 144.38 (3) |
O6v—Fe1—O2 | 84.43 (4) | O4ix—Na1—O6xii | 70.35 (5) |
O3vi—Zn2—O3 | 79.62 (5) | O4—Na1—O6xii | 114.24 (8) |
O3vi—Zn2—O6vii | 92.79 (4) | O4x—Na1—O6xii | 101.22 (6) |
O3—Zn2—O6vii | 113.99 (4) | O4vii—Na1—O6xii | 83.40 (5) |
O3vi—Zn2—O6v | 113.99 (4) | O1—Na1—O6xii | 144.38 (3) |
O3—Zn2—O6v | 92.79 (4) | O1ix—Na1—O6xii | 125.27 (3) |
O6vii—Zn2—O6v | 145.51 (5) | O6xi—Na1—O6xii | 51.96 (5) |
O3vi—Zn2—O1iii | 164.40 (4) | O5xiii—Na2—O5vi | 180.00 (3) |
O3—Zn2—O1iii | 86.51 (4) | O5xiii—Na2—O3 | 100.43 (3) |
O6vii—Zn2—O1iii | 86.30 (4) | O5vi—Na2—O3 | 79.57 (3) |
O6v—Zn2—O1iii | 73.53 (3) | O5xiii—Na2—O3v | 79.57 (3) |
O3vi—Zn2—O1viii | 86.51 (4) | O5vi—Na2—O3v | 100.43 (3) |
O3—Zn2—O1viii | 164.40 (4) | O3—Na2—O3v | 180.0 |
O6vii—Zn2—O1viii | 73.53 (3) | O5xiii—Na2—O3xiii | 107.29 (3) |
O6v—Zn2—O1viii | 86.30 (4) | O5vi—Na2—O3xiii | 72.71 (3) |
O1iii—Zn2—O1viii | 108.06 (5) | O3—Na2—O3xiii | 113.43 (4) |
O3—P1—O4 | 112.20 (6) | O3v—Na2—O3xiii | 66.57 (4) |
O3—P1—O2 | 108.58 (5) | O5xiii—Na2—O3vi | 72.71 (3) |
O4—P1—O2 | 109.36 (6) | O5vi—Na2—O3vi | 107.29 (3) |
O3—P1—O1 | 111.16 (6) | O3—Na2—O3vi | 66.57 (4) |
O4—P1—O1 | 107.14 (6) | O3v—Na2—O3vi | 113.43 (4) |
O2—P1—O1 | 108.32 (5) | O3xiii—Na2—O3vi | 180.00 (3) |
O5—P2—O5vi | 103.73 (8) | O5xiii—Na2—O5v | 53.55 (4) |
O5—P2—O6 | 112.27 (5) | O5vi—Na2—O5v | 126.45 (4) |
O5vi—P2—O6 | 109.00 (5) | O3—Na2—O5v | 85.32 (3) |
O5—P2—O6vi | 109.00 (5) | O3v—Na2—O5v | 94.68 (3) |
O5vi—P2—O6vi | 112.28 (5) | O3xiii—Na2—O5v | 67.11 (3) |
O6—P2—O6vi | 110.43 (7) | O3vi—Na2—O5v | 112.89 (3) |
O4ix—Na1—O4 | 175.26 (12) | O5xiii—Na2—O5 | 126.45 (4) |
O4ix—Na1—O4x | 79.21 (3) | O5vi—Na2—O5 | 53.55 (4) |
O4—Na1—O4x | 100.58 (3) | O3—Na2—O5 | 94.68 (3) |
O4ix—Na1—O4vii | 100.58 (3) | O3v—Na2—O5 | 85.32 (3) |
O4—Na1—O4vii | 79.20 (3) | O3xiii—Na2—O5 | 112.89 (3) |
O4x—Na1—O4vii | 174.93 (11) | O3vi—Na2—O5 | 67.11 (3) |
O4ix—Na1—O1 | 119.76 (8) | O5v—Na2—O5 | 180.00 (3) |
Symmetry codes: (i) x+1/2, y+1/2, z; (ii) −x+3/2, y+1/2, −z+1/2; (iii) −x+3/2, −y+3/2, −z+1; (iv) −x+3/2, −y+3/2, −z; (v) −x+1, −y+1, −z; (vi) −x+1, y, −z+1/2; (vii) x, −y+1, z+1/2; (viii) x−1/2, −y+3/2, z−1/2; (ix) −x+2, y, −z+3/2; (x) −x+2, −y+1, −z+1; (xi) x+1/2, −y+1/2, z+1/2; (xii) −x+3/2, −y+1/2, −z+1; (xiii) x, −y+1, z−1/2. |
Experimental details
Crystal data | |
Chemical formula | Na1.67Zn1.67Fe1.33(PO4)3 |
Mr | 506.59 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 296 |
a, b, c (Å) | 11.7545 (4), 12.5080 (4), 6.4014 (2) |
β (°) | 113.507 (1) |
V (Å3) | 863.06 (5) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 7.52 |
Crystal size (mm) | 0.31 × 0.25 × 0.19 |
Data collection | |
Diffractometer | Bruker X8 APEX diffractometer |
Absorption correction | Multi-scan (SADABS; Bruker, 2009) |
Tmin, Tmax | 0.504, 0.748 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 18880, 2101, 1997 |
Rint | 0.031 |
(sin θ/λ)max (Å−1) | 0.833 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.017, 0.046, 1.19 |
No. of reflections | 2101 |
No. of parameters | 96 |
Δρmax, Δρmin (e Å−3) | 0.65, −1.20 |
Computer programs: APEX2 (Bruker, 2009), SAINT (Bruker, 2009), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEPIII (Burnett & Johnson, 1996), ORTEP-3 for Windows Farrugia, 2012) and DIAMOND (Brandenburg, 2006), publCIF (Westrip, 2010).
Acknowledgements
The authors thank the Unit of Support for Technical and Scientific Research (UATRS, CNRST) for the X-ray measurements and Mohammed V University, Rabat, Morocco, for the financial support.
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