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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Dec 18;67(Pt 1):i2. doi: 10.1107/S1600536810052451

Silver indium diphosphate, AgInP2O7

Hafid Zouihri a,*,‡, Mohamed Saadi a, Boujemaa Jaber b, Lehcen El Ammari a
PMCID: PMC3050398  PMID: 21522510

Abstract

Polycrystalline material of the title compound, AgInP2O7, was synthesized by traditional high-temperature solid-state methods and single crystals were grown from the melt of a mixture of AgInP2O7 and B2O3 as flux in a platinium crucible. The structure consists of InO6 octa­hedra, which are corner-shared to PO4 tetra­hedra into a three-dimensional network with hexa­gonal channels running parallel to the c axis. The silver cation, located in the channel, is bonded to seven O atoms of the [InP2O7] framework with Ag–O distances ranging from 2.370 (2) to 3.015 (2) Å. The P2O7 diphosphate anion is characterized by a P—O—P angle of 137.27 (9) and a nearly eclipsed conformation. AgInP2O7 is isotypic with the M IFeP2O7 (M I = Na, K, Rb, Cs and Ag) diphosphate family.

Related literature

For properties of M IFeP2O7 (M I = Na, K, Rb, Cs and Ag) diphosphates, see: Terebilenko et al. (2010 ▶); Hizhnyi et al. (2008 ▶); Whangbo et al. (2004 ▶); Vitins et al. (2000 ▶). For isotypic structures, see: Belkouch et al. (1995 ▶); Gabelica-Robert et al. (1982 ▶); Moya-Pizarro et al. (1984 ▶); Mercader et al. (1990 ▶).

Experimental

Crystal data

  • AgInP2O7

  • M r = 396.63

  • Monoclinic, Inline graphic

  • a = 7.4867 (3) Å

  • b = 8.2620 (3) Å

  • c = 9.8383 (5) Å

  • β = 112.038 (2)°

  • V = 564.09 (4) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 8.11 mm−1

  • T = 296 K

  • 0.08 × 0.06 × 0.05 mm

Data collection

  • Bruker X8 APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1999 ▶) T min = 0.563, T max = 0.667

  • 21692 measured reflections

  • 3730 independent reflections

  • 3245 reflections with I > 2σ(I)

  • R int = 0.035

Refinement

  • R[F 2 > 2σ(F 2)] = 0.021

  • wR(F 2) = 0.048

  • S = 1.03

  • 3730 reflections

  • 101 parameters

  • Δρmax = 1.62 e Å−3

  • Δρmin = −2.04 e Å−3

Data collection: APEX2 (Bruker, 2005 ▶); cell refinement: SAINT (Bruker, 2005 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810052451/br2154sup1.cif

e-67-000i2-sup1.cif (14.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810052451/br2154Isup2.hkl

e-67-000i2-Isup2.hkl (179.2KB, hkl)

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

Acknowledgments

The authors thank the Unit of Support for Technical and Scientific Research (UATRS, CNRST) for the X-ray data collection.

supplementary crystallographic information

Comment

The diphosphates AIMIIIP2O7 (AI = Li, Na, K, Rb, Cs and Ag; MIII = Al, Ga, Cr, Fe, In, Y) are extensively studied for their electrical and optical properties and for its perspective application as magnetic materials (Terebilenko et al. (2010); Hizhnyi et al. (2008); Whangbo et al. (2004); Vitins et al. (2000)). The crystal structures of most of these compounds are known except a few cases in which the crystal growth is difficult. In this context, the present paper reports on the determination of AgInP2O7 crystal structure from X-ray diffraction single-crystal data.

The structure of this phosphate is characterized by a three-dimensional network built up from indum octahedra linked to diphosphate groups by a corner-sharing. Each InO6 octahedra is surrounded by six PO4 tetrahedra belonging to five different P2O7 groups (see Fig.1 and Fig.2). As a result of these blocks, assemblage three-dimensional-framework is formed with hexagonal channels, where silver cations reside. Although, the coordination sphere of Ag+ cations is composed of seven O2- anions in an irregular geometry, located at Ag–O distances between 2.370 (2) and 3.015 (2) Å (see Fig.2). Furthermore, the diphosphate group contains two distorted PO4 tetrahedra sharing one corner and display a nearly eclipsed conformation. The P–O bond-lengths range between 1.492 (2) Å for terminal P1–O1 and 1.606 (2) Å for the bridging P2–O7 bond. Therefore, a P1–O7–P2 angle of 137.27 (9) ° is wider than 133.6 (3)° and 132.9 (3) ° reported for both AgFeP2O7 and NaFeP2O7 respectively (Belkouch et al. (1995); Gabelica-Robert et al. (1982); Moya-Pizarro et al. (1984); Mercader et al. (1990)).

Silver indium diphosphate (pyrophosphate) is isostructural to AIFeP2O7 (AI = Na, K, Rb, Cs and Ag) diphosphates family and is categorized as a dichromate type.

Experimental

AgInP2O7 in the form of single crystals was prepared by stoichiometric reaction of AgNO3, (NH4)2HPO4 and In2O3 in B2O3 flux. The mixture was heated at 773 K under ambiante atmosphere for 6 h and 973 K for 2 h with intermediate grindings to ensure complete reaction. Subsequent melting at 1323 K followed by slow cooling to room temperature at a rate of 12°K h-1 resulted in colourless crystals of the title compound.

Refinement

The highest and deepest hole residual peak in the final difference Fourier map are located at 0.49 Å and 0.58 Å, respectively from Ag1 atom. The not significants bonds and angles were removed from the CIF file.

Figures

Fig. 1.

Fig. 1.

Partial plot of AgInP2O7 crystal structure shawing plyhedra linkage. Displacement ellipsoids are drawn at the 50% probability level. Symmetry codes: (i) -x + 1, y - 1/2, -z + 1/2; (ii) -x, y - 1/2, -z + 1/2; (iii) -x + 1, -y + 1, -z + 1; (iv) x, -y + 3/2, z - 1/2; (v) x - 1, y, z; (vi) x - 1, -y + 3/2, z - 1/2; (vii) -x, -y + 1, -z + 1.

Fig. 2.

Fig. 2.

Perspective view along [101] of the AgInP2O7 framework structure shawing tunnel where silver cations are located.

Crystal data

AgInP2O7 F(000) = 728
Mr = 396.63 Dx = 4.670 Mg m−3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 317 reflections
a = 7.4867 (3) Å θ = 2.5–30.2°
b = 8.2620 (3) Å µ = 8.11 mm−1
c = 9.8383 (5) Å T = 296 K
β = 112.038 (2)° Block, colourless
V = 564.09 (4) Å3 0.08 × 0.06 × 0.05 mm
Z = 4

Data collection

Bruker X8 APEXII CCD area-detector diffractometer 3730 independent reflections
Radiation source: fine-focus sealed tube 3245 reflections with I > 2σ(I)
graphite Rint = 0.035
ω and φ scans θmax = 41.0°, θmin = 2.9°
Absorption correction: multi-scan (SADABS; Sheldrick, 1999) h = −13→13
Tmin = 0.563, Tmax = 0.667 k = −15→15
21692 measured reflections l = −18→18

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.021 w = 1/[σ2(Fo2) + (0.017P)2 + 0.9979P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.048 (Δ/σ)max = 0.001
S = 1.03 Δρmax = 1.62 e Å−3
3730 reflections Δρmin = −2.04 e Å−3
101 parameters Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraints Extinction coefficient: 0.0171 (4)

Special details

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

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

x y z Uiso*/Ueq
In1 0.242354 (15) 0.495357 (12) 0.247622 (11) 0.00618 (3)
Ag1 −0.20911 (3) 0.52697 (2) 0.30478 (2) 0.02442 (4)
P1 0.57689 (6) 0.74758 (5) 0.46083 (4) 0.00600 (6)
P2 0.17589 (6) 0.78735 (5) 0.45174 (4) 0.00656 (6)
O1 0.6810 (2) 0.86792 (17) 0.40464 (15) 0.0141 (2)
O2 0.6836 (2) 0.71622 (16) 0.62241 (14) 0.0136 (2)
O3 0.52473 (17) 0.59259 (15) 0.36935 (14) 0.01027 (19)
O4 0.04427 (18) 0.91166 (17) 0.35059 (15) 0.0123 (2)
O5 0.1917 (2) 0.79561 (16) 0.60976 (14) 0.0126 (2)
O6 0.13231 (18) 0.61348 (15) 0.39564 (14) 0.01054 (19)
O7 0.37868 (18) 0.83601 (16) 0.44239 (16) 0.0128 (2)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
In1 0.00656 (4) 0.00614 (4) 0.00593 (4) −0.00024 (3) 0.00244 (3) −0.00045 (3)
Ag1 0.01913 (7) 0.02720 (8) 0.03341 (9) −0.00235 (6) 0.01725 (7) −0.01071 (7)
P1 0.00574 (14) 0.00643 (14) 0.00582 (14) −0.00025 (11) 0.00217 (11) 0.00044 (11)
P2 0.00588 (14) 0.00706 (14) 0.00644 (14) 0.00073 (11) 0.00195 (11) −0.00090 (12)
O1 0.0185 (6) 0.0141 (5) 0.0133 (5) −0.0053 (4) 0.0104 (5) 0.0012 (4)
O2 0.0195 (6) 0.0098 (5) 0.0070 (4) −0.0006 (4) −0.0001 (4) 0.0018 (4)
O3 0.0072 (4) 0.0099 (5) 0.0130 (5) −0.0012 (3) 0.0030 (4) −0.0040 (4)
O4 0.0084 (5) 0.0135 (5) 0.0135 (5) 0.0034 (4) 0.0023 (4) 0.0041 (4)
O5 0.0211 (6) 0.0099 (5) 0.0072 (4) −0.0009 (4) 0.0058 (4) −0.0023 (4)
O6 0.0116 (5) 0.0097 (5) 0.0123 (5) −0.0019 (4) 0.0067 (4) −0.0039 (4)
O7 0.0078 (5) 0.0100 (5) 0.0217 (6) 0.0010 (4) 0.0069 (4) −0.0020 (4)

Geometric parameters (Å, °)

In1—O1i 2.0799 (13) Ag1—O5vii 2.7829 (14)
In1—O4ii 2.1120 (12) Ag1—O6vii 3.0153 (14)
In1—O2iii 2.1133 (13) P1—O1 1.4919 (13)
In1—O5iv 2.1401 (13) P1—O2 1.5097 (13)
In1—O3 2.1562 (12) P1—O3 1.5292 (13)
In1—O6 2.1569 (12) P1—O7 1.6021 (13)
Ag1—O3v 2.3703 (12) P2—O4 1.5101 (13)
Ag1—O6 2.4757 (13) P2—O5 1.5158 (13)
Ag1—O4ii 2.4865 (14) P2—O6 1.5295 (13)
Ag1—O2vi 2.6991 (14) P2—O7 1.6062 (13)
Ag1—O7ii 2.7744 (15)
O1i—In1—O4ii 90.70 (6) O3v—Ag1—O5vii 94.99 (4)
O1i—In1—O2iii 86.35 (6) O6—Ag1—O5vii 104.03 (4)
O4ii—In1—O2iii 89.82 (6) O4ii—Ag1—O5vii 80.85 (4)
O1i—In1—O5iv 89.04 (5) O2vi—Ag1—O5vii 157.25 (4)
O4ii—In1—O5iv 93.79 (5) O7ii—Ag1—O5vii 71.00 (4)
O2iii—In1—O5iv 174.18 (6) O3v—Ag1—O6vii 72.37 (4)
O1i—In1—O3 96.36 (5) O6—Ag1—O6vii 88.04 (4)
O4ii—In1—O3 172.86 (5) O4ii—Ag1—O6vii 119.79 (4)
O2iii—In1—O3 89.55 (5) O2vi—Ag1—O6vii 148.46 (4)
O5iv—In1—O3 87.43 (5) O7ii—Ag1—O6vii 119.64 (4)
O1i—In1—O6 173.56 (5) O5vii—Ag1—O6vii 50.65 (4)
O4ii—In1—O6 82.94 (5) O1—P1—O2 111.17 (8)
O2iii—In1—O6 92.62 (5) O1—P1—O3 113.17 (8)
O5iv—In1—O6 92.35 (5) O2—P1—O3 113.16 (8)
O3—In1—O6 89.98 (5) O1—P1—O7 104.17 (8)
O3v—Ag1—O6 134.04 (4) O2—P1—O7 107.40 (8)
O3v—Ag1—O4ii 155.99 (4) O3—P1—O7 107.10 (7)
O6—Ag1—O4ii 69.47 (4) O4—P2—O5 115.20 (8)
O3v—Ag1—O2vi 85.86 (5) O4—P2—O6 113.76 (8)
O6—Ag1—O2vi 91.29 (4) O5—P2—O6 109.65 (8)
O4ii—Ag1—O2vi 89.15 (5) O4—P2—O7 100.90 (8)
O3v—Ag1—O7ii 102.17 (4) O5—P2—O7 109.63 (8)
O6—Ag1—O7ii 123.47 (4) O6—P2—O7 107.01 (7)
O4ii—Ag1—O7ii 54.04 (4) P1—O7—P2 137.27 (9)
O2vi—Ag1—O7ii 86.57 (4)

Symmetry codes: (i) −x+1, y−1/2, −z+1/2; (ii) −x, y−1/2, −z+1/2; (iii) −x+1, −y+1, −z+1; (iv) x, −y+3/2, z−1/2; (v) x−1, y, z; (vi) x−1, −y+3/2, z−1/2; (vii) −x, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BR2154).

References

  1. Belkouch, J., Monceaux, L. & Courtine, P. (1995). Mater. Res. Bull. 30, 149–160.
  2. Bruker (2005). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  3. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  4. Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837–838.
  5. Gabelica-Robert, M., Goreaud, M., Labbe, Ph. & Raveau, B. (1982). J. Solid State Chem. 45, 389–395.
  6. Hizhnyi, Y. A., Oliynyk, A., Gomenyuk, O., Nedilko, S. G., Nagornyi, P., Bojko, R. & Bojko, V. (2008). Opt. Mater. 30, 687–689.
  7. Mercader, R. C., Terminiello, L., Long, G. J., Reichel, D. G., Dickhaus, K., Zysler, R., Sanchez, R. & Tovar, M. (1990). Phys. Rev. B Condens. Matter, 42, 25–32. [DOI] [PubMed]
  8. Moya-Pizarro, T., Salmon, R., Fournes, S. L., Le Flem, G., Wanklyn, B. S. & Hagenmuller, P. (1984). J. Solid State Chem. 53, 387–397.
  9. Sheldrick, G. M. (1999). SADABS University of Göttingen, Germany.
  10. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  11. Terebilenko, K. V., Kirichok, A. A., Baumer, V. N., Sereduk, M., Slobodyanik, N. S. & Gütlich, P. (2010). J. Solid State Chem. 183, 1473–1476.
  12. Vitins, G., Kanepe, Z., Vitins, A., Ronis, J., Dindune, A. & Lusis, A. (2000). J. Solid State Electochem. 4, 146–152.
  13. Whangbo, M.-H., Dai, D. & Koo, H.-J. (2004). Dalton Trans. pp. 3019–3025. [DOI] [PubMed]

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/S1600536810052451/br2154sup1.cif

e-67-000i2-sup1.cif (14.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810052451/br2154Isup2.hkl

e-67-000i2-Isup2.hkl (179.2KB, hkl)

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


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