supplementary materials


Acta Cryst. (2009). E65, i58    [ doi:10.1107/S1600536809025434 ]

CsMgPO4

N. Yu. Strutynska, I. V. Zatovsky, V. N. Baumer and N. S. Slobodyanik

Abstract top

Caesium magnesium orthophosphate is built up from MgO4 and PO4 tetrahedra (both with . m. symmetry) linked together by corners, forming a three-dimensional framework. The Cs atoms have .m. site symmetry and are located in hexagonal channels running along the a- and b-axis directions.

Comment top

Double phosphates AIBIIPO4 (AI = alkali metal; BII = Ca, Sr, Ba, Zn, Cd, Pb) exhibit important properties such as ferroelectric and nonlinear optical behaviour (Blum et al., 1984; Elouadi et al., 1984; Sawada et al., 2003). Among some orthophosphates containing Cs and divalent metals, several polymorphs have been found. For instance, CsZnPO4 occurs in a monoclinic (space group P21/a) and two orthorhombic types (space groups Pna21 and Pnma) (Blum et al., 1986). In contrast, CsMnPO4 occurs in only one type (space group Pna21) (Yakubovich et al., 1990). CsMgPO4, reported here, is isotypic with the Pnma form of CsZnPO4.

Except for O2 (8d), all atoms are in special positions (4c) (Fig. 1). Each MgO4 tetrahedron is linked with four PO4 tetrahedra via common vertices, resulting in a three-dimensional framework with two types of hexagonal channels, filled by Cs atoms, along the a and b directions (Fig. 2). With a cut-off distance of 3.7 Å, the Cs atoms are 11-coordinate. In general, the principles of crystal structure building are equivalent to those in CsMIIPO4 (MII = Mn, Zn) (Yakubovich et al., 1990; Blum et al., 1986) and CsLi0.5Al0.5PO4 (Zapirov et al., 2008).

Related literature top

For the properties of double phosphates AIBIIPO4 (AI = alkali metal; BII = Ca, Sr, Ba, Zn, Cd, Pb) such as ferroelectric and non-linearoptical behaviour, see: Blum et al. (1984); Elouadi et al. (1984); Sawada et al. (2003). Several polymorphs have been found among orthophosphates containing Cs and divalent metals, see: Blum et al. (1986) for CsZnPO4. In contrast, CsMnPO4 occurs in only one type, see: Yakubovich et al. (1990). The title compound is isotypic with the Pnma form of CsZnPO4. For related structures, see: Yakubovich et al., 1990); Blum et al., 1986); Zaripov et al. (2008).

Experimental top

In the course of investigating the Cs2O–MgO–Bi2O3–P2O5 system, the starting components CsPO3 (3.0 g), MgO (0.113 g) and Bi2O3 (0.652 g) were finely ground and melted in a platinum crucible at 1273 K. The melt was kept at this temperature over 2 h to reach homogeneity and then cooled at a rate of 30 K h-1 to 993 K. After the melt was cooled to room temperature and treated with a small amount of deionized water, colorless needle-shaped crystals were isolated. X-ray powder diffraction showed that CsMgPO4 is the only crystalline product.

Refinement top

The deepest hole and the highest peak are 0.67 Å and 0.65 Å, respectively, from Cs1.

Computing details top

Data collection: CrysAlis CCD (Oxford Diffraction, 2006); cell refinement: CrysAlis CCD (Oxford Diffraction, 2006); data reduction: CrysAlis RED (Oxford Diffraction, 2006); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 1999); software used to prepare material for publication: WinGX (Farrugia, 1999) and enCIFer (Allen et al., 2004).

Figures top
[Figure 1] Fig. 1. View of CsMgPO4 with displacement ellipsoids at the 50% probability level.
[Figure 2] Fig. 2. Formation of hexagonal channels along a and b directions in CsMgPO4 (PO4, pink; MgO4, yellow; Cs, blue).
Caesium magnesium orthophosphate top
Crystal data top
CsMgPO4F000 = 456
Mr = 252.19Dx = 3.516 Mg m3
Orthorhombic, PnmaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2nCell parameters from 8753 reflections
a = 8.9327 (2) Åθ = 3.1–35.0º
b = 5.5277 (2) ŵ = 8.13 mm1
c = 9.6487 (3) ÅT = 293 K
V = 476.43 (3) Å3Prism, colorless
Z = 40.12 × 0.10 × 0.08 mm
Data collection top
Oxford Diffraction Xcalibur-3
diffractometer
1137 independent reflections
Radiation source: fine-focus sealed tube874 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.027
T = 293 Kθmax = 35.0º
φ and ω scansθmin = 3.1º
Absorption correction: multi-scan
(Blessing, 1995)
h = 14→14
Tmin = 0.413, Tmax = 0.503k = 8→8
8753 measured reflectionsl = 15→15
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: full  w = 1/[σ2(Fo2) + (0.0265P)2]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.021(Δ/σ)max = 0.018
wR(F2) = 0.047Δρmax = 1.23 e Å3
S = 1.00Δρmin = 1.02 e Å3
1137 reflectionsExtinction correction: SHELXL97 (Sheldrick, 2008)
41 parametersExtinction coefficient: 0.0211 (4)
Primary atom site location: structure-invariant direct methods
Crystal data top
CsMgPO4V = 476.43 (3) Å3
Mr = 252.19Z = 4
Orthorhombic, PnmaMo Kα
a = 8.9327 (2) ŵ = 8.13 mm1
b = 5.5277 (2) ÅT = 293 K
c = 9.6487 (3) Å0.12 × 0.10 × 0.08 mm
Data collection top
Oxford Diffraction Xcalibur-3
diffractometer
1137 independent reflections
Absorption correction: multi-scan
(Blessing, 1995)
874 reflections with I > 2σ(I)
Tmin = 0.413, Tmax = 0.503Rint = 0.027
8753 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.02141 parameters
wR(F2) = 0.047Δρmax = 1.23 e Å3
S = 1.00Δρmin = 1.02 e Å3
1137 reflections
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cs10.497176 (11)0.250.703332 (10)0.02472 (2)
Mg10.32166 (5)0.250.08109 (5)0.01434 (11)
P10.20302 (4)0.250.41474 (4)0.01345 (7)
O10.26034 (19)0.250.26799 (13)0.0590 (6)
O20.26291 (11)0.02604 (13)0.48850 (9)0.0328 (2)
O30.03356 (14)0.250.41501 (19)0.0345 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cs10.02161 (4)0.02632 (5)0.02623 (4)00.00031 (4)0
Mg10.01301 (19)0.0133 (2)0.0168 (2)00.00166 (17)0
P10.01272 (13)0.01259 (14)0.01505 (14)00.00207 (12)0
O10.0594 (11)0.1014 (17)0.0162 (7)00.0121 (7)0
O20.0239 (4)0.0190 (4)0.0555 (6)0.0002 (3)0.0016 (4)0.0156 (4)
O30.0121 (4)0.0286 (6)0.0629 (10)00.0003 (6)0
Geometric parameters (Å, °) top
Cs1—O23.1951 (9)Mg1—Cs1xiii4.1402 (4)
Cs1—O2i3.1951 (9)P1—O11.5056 (13)
Cs1—O2ii3.2166 (9)P1—O31.5138 (13)
Cs1—O2iii3.2166 (9)P1—O2i1.5249 (8)
Cs1—O3iv3.4476 (11)P1—O21.5249 (8)
Cs1—O3v3.4476 (11)P1—Cs1ix3.8727 (3)
Cs1—O1vi3.5224 (11)P1—Cs1xiii3.8727 (3)
Cs1—O1ii3.5224 (11)P1—Cs1vi4.0136 (3)
Cs1—O1v3.6496 (11)P1—Cs1ii4.0136 (3)
Cs1—O1iv3.6496 (11)P1—Cs1xiv4.1184 (4)
Cs1—O3vii3.6968 (18)O1—Cs1vi3.5224 (11)
Cs1—Mg1vi3.8189 (4)O1—Cs1ii3.5224 (11)
Mg1—O11.8847 (13)O1—Cs1ix3.6496 (11)
Mg1—O3viii1.8932 (13)O1—Cs1xiii3.6496 (11)
Mg1—O2ix1.9228 (8)O2—Mg1v1.9228 (8)
Mg1—O2x1.9228 (8)O2—Cs1ii3.2166 (9)
Mg1—Cs1vi3.8189 (4)O3—Mg1xii1.8932 (13)
Mg1—Cs1ii3.8189 (4)O3—Cs1ix3.4476 (11)
Mg1—Cs1xi3.9678 (5)O3—Cs1xiii3.4476 (11)
Mg1—Cs1xii3.9916 (5)O3—Cs1xiv3.6968 (18)
Mg1—Cs1ix4.1402 (4)
O2—Cs1—O2i45.59 (3)O1—Mg1—Cs1ix61.80 (3)
O2—Cs1—O2ii83.06 (3)O3viii—Mg1—Cs1ix133.01 (2)
O2i—Cs1—O2ii104.291 (19)O2ix—Mg1—Cs1ix48.11 (3)
O2—Cs1—O2iii104.291 (19)O2x—Mg1—Cs1ix113.07 (3)
O2i—Cs1—O2iii83.06 (3)Cs1vi—Mg1—Cs1ix128.277 (13)
O2ii—Cs1—O2iii56.64 (3)Cs1ii—Mg1—Cs1ix69.709 (5)
O2—Cs1—O3iv130.00 (3)Cs1xi—Mg1—Cs1ix122.243 (9)
O2i—Cs1—O3iv91.24 (3)Cs1xii—Mg1—Cs1ix72.323 (7)
O2ii—Cs1—O3iv140.73 (3)O1—Mg1—Cs1xiii61.80 (3)
O2iii—Cs1—O3iv90.78 (3)O3viii—Mg1—Cs1xiii133.01 (2)
O2—Cs1—O3v91.24 (3)O2ix—Mg1—Cs1xiii113.07 (3)
O2i—Cs1—O3v130.00 (3)O2x—Mg1—Cs1xiii48.11 (3)
O2ii—Cs1—O3v90.78 (3)Cs1vi—Mg1—Cs1xiii69.709 (5)
O2iii—Cs1—O3v140.73 (3)Cs1ii—Mg1—Cs1xiii128.277 (14)
O3iv—Cs1—O3v106.58 (5)Cs1xi—Mg1—Cs1xiii122.243 (9)
O2—Cs1—O1vi139.27 (2)Cs1xii—Mg1—Cs1xiii72.323 (7)
O2i—Cs1—O1vi98.61 (3)Cs1ix—Mg1—Cs1xiii83.758 (9)
O2ii—Cs1—O1vi90.44 (3)O1—P1—O3109.98 (10)
O2iii—Cs1—O1vi42.55 (2)O1—P1—O2i108.64 (5)
O3iv—Cs1—O1vi51.20 (3)O3—P1—O2i110.49 (5)
O3v—Cs1—O1vi129.16 (3)O1—P1—O2108.64 (5)
O2—Cs1—O1ii98.61 (3)O3—P1—O2110.49 (5)
O2i—Cs1—O1ii139.27 (2)O2i—P1—O2108.56 (7)
O2ii—Cs1—O1ii42.55 (2)O1—P1—Cs1116.78 (7)
O2iii—Cs1—O1ii90.44 (3)O3—P1—Cs1133.24 (7)
O3iv—Cs1—O1ii129.16 (3)O2i—P1—Cs154.54 (3)
O3v—Cs1—O1ii51.20 (3)O2—P1—Cs154.54 (3)
O1vi—Cs1—O1ii103.38 (4)O1—P1—Cs1ix70.23 (4)
O2—Cs1—O1v53.46 (2)O3—P1—Cs1ix62.56 (4)
O2i—Cs1—O1v89.52 (3)O2i—P1—Cs1ix170.83 (4)
O2ii—Cs1—O1v99.15 (2)O2—P1—Cs1ix80.12 (3)
O2iii—Cs1—O1v151.35 (2)Cs1—P1—Cs1ix134.428 (4)
O3iv—Cs1—O1v117.11 (3)O1—P1—Cs1xiii70.23 (4)
O3v—Cs1—O1v40.66 (3)O3—P1—Cs1xiii62.56 (4)
O1vi—Cs1—O1v165.554 (5)O2i—P1—Cs1xiii80.12 (3)
O1ii—Cs1—O1v77.288 (3)O2—P1—Cs1xiii170.83 (4)
O2—Cs1—O1iv89.52 (3)Cs1—P1—Cs1xiii134.428 (4)
O2i—Cs1—O1iv53.46 (2)Cs1ix—P1—Cs1xiii91.069 (8)
O2ii—Cs1—O1iv151.35 (2)O1—P1—Cs1vi60.41 (4)
O2iii—Cs1—O1iv99.15 (2)O3—P1—Cs1vi131.89 (3)
O3iv—Cs1—O1iv40.66 (3)O2i—P1—Cs1vi48.65 (4)
O3v—Cs1—O1iv117.11 (3)O2—P1—Cs1vi117.22 (4)
O1vi—Cs1—O1iv77.288 (3)Cs1—P1—Cs1vi75.434 (6)
O1ii—Cs1—O1iv165.554 (5)Cs1ix—P1—Cs1vi130.546 (10)
O1v—Cs1—O1iv98.45 (4)Cs1xiii—P1—Cs1vi70.558 (4)
O2—Cs1—O3vii134.74 (2)O1—P1—Cs1ii60.41 (4)
O2i—Cs1—O3vii134.74 (2)O3—P1—Cs1ii131.89 (3)
O2ii—Cs1—O3vii120.97 (2)O2i—P1—Cs1ii117.22 (4)
O2iii—Cs1—O3vii120.97 (2)O2—P1—Cs1ii48.65 (4)
O3iv—Cs1—O3vii54.33 (3)Cs1—P1—Cs1ii75.434 (6)
O3v—Cs1—O3vii54.33 (3)Cs1ix—P1—Cs1ii70.558 (4)
O1vi—Cs1—O3vii82.40 (2)Cs1xiii—P1—Cs1ii130.546 (10)
O1ii—Cs1—O3vii82.40 (2)Cs1vi—P1—Cs1ii87.043 (8)
O1v—Cs1—O3vii83.40 (2)O1—P1—Cs1xiv173.36 (7)
O1iv—Cs1—O3vii83.40 (2)O3—P1—Cs1xiv63.38 (7)
O2—Cs1—Mg1vi155.689 (15)O2i—P1—Cs1xiv74.87 (4)
O2i—Cs1—Mg1vi110.517 (14)O2—P1—Cs1xiv74.87 (4)
O2ii—Cs1—Mg1vi111.987 (18)Cs1—P1—Cs1xiv69.857 (6)
O2iii—Cs1—Mg1vi71.807 (16)Cs1ix—P1—Cs1xiv105.375 (7)
O3iv—Cs1—Mg1vi29.64 (2)Cs1xiii—P1—Cs1xiv105.375 (7)
O3v—Cs1—Mg1vi106.93 (3)Cs1vi—P1—Cs1xiv123.498 (7)
O1vi—Cs1—Mg1vi29.40 (2)Cs1ii—P1—Cs1xiv123.498 (7)
O1ii—Cs1—Mg1vi105.34 (2)P1—O1—Mg1177.02 (12)
O1v—Cs1—Mg1vi136.22 (2)P1—O1—Cs1vi97.77 (4)
O1iv—Cs1—Mg1vi68.03 (2)Mg1—O1—Cs1vi84.06 (4)
O3vii—Cs1—Mg1vi54.563 (11)P1—O1—Cs1ii97.77 (4)
O1—Mg1—O3viii105.76 (8)Mg1—O1—Cs1ii84.06 (4)
O1—Mg1—O2ix109.29 (4)Cs1vi—O1—Cs1ii103.38 (4)
O3viii—Mg1—O2ix113.71 (4)P1—O1—Cs1ix86.93 (5)
O1—Mg1—O2x109.29 (4)Mg1—O1—Cs1ix91.12 (4)
O3viii—Mg1—O2x113.71 (4)Cs1vi—O1—Cs1ix174.41 (4)
O2ix—Mg1—O2x105.04 (6)Cs1ii—O1—Cs1ix78.860 (3)
O1—Mg1—Cs1vi66.55 (3)P1—O1—Cs1xiii86.93 (5)
O3viii—Mg1—Cs1vi64.25 (3)Mg1—O1—Cs1xiii91.12 (4)
O2ix—Mg1—Cs1vi173.66 (3)Cs1vi—O1—Cs1xiii78.860 (3)
O2x—Mg1—Cs1vi81.10 (3)Cs1ii—O1—Cs1xiii174.41 (4)
O1—Mg1—Cs1ii66.55 (3)Cs1ix—O1—Cs1xiii98.45 (4)
O3viii—Mg1—Cs1ii64.25 (3)P1—O2—Mg1v136.32 (7)
O2ix—Mg1—Cs1ii81.10 (3)P1—O2—Cs1102.59 (4)
O2x—Mg1—Cs1ii173.66 (3)Mg1v—O2—Cs1105.27 (4)
Cs1vi—Mg1—Cs1ii92.725 (11)P1—O2—Cs1ii110.51 (4)
O1—Mg1—Cs1xi173.62 (6)Mg1v—O2—Cs1ii98.78 (3)
O3viii—Mg1—Cs1xi67.86 (6)Cs1—O2—Cs1ii96.94 (3)
O2ix—Mg1—Cs1xi74.24 (3)P1—O3—Mg1xii178.96 (13)
O2x—Mg1—Cs1xi74.24 (3)P1—O3—Cs1ix94.51 (5)
Cs1vi—Mg1—Cs1xi109.444 (9)Mg1xii—O3—Cs1ix86.11 (4)
Cs1ii—Mg1—Cs1xi109.444 (9)P1—O3—Cs1xiii94.51 (5)
O1—Mg1—Cs1xii116.54 (5)Mg1xii—O3—Cs1xiii86.11 (4)
O3viii—Mg1—Cs1xii137.70 (6)Cs1ix—O3—Cs1xiii106.58 (5)
O2ix—Mg1—Cs1xii52.79 (3)P1—O3—Cs1xiv95.14 (8)
O2x—Mg1—Cs1xii52.79 (3)Mg1xii—O3—Cs1xiv83.82 (6)
Cs1vi—Mg1—Cs1xii133.015 (6)Cs1ix—O3—Cs1xiv125.67 (3)
Cs1ii—Mg1—Cs1xii133.015 (6)Cs1xiii—O3—Cs1xiv125.67 (3)
Cs1xi—Mg1—Cs1xii69.840 (9)
Symmetry codes: (i) x, −y+1/2, z; (ii) −x+1, −y, −z+1; (iii) −x+1, y+1/2, −z+1; (iv) −x+1/2, −y+1, z+1/2; (v) −x+1/2, −y, z+1/2; (vi) −x+1, −y+1, −z+1; (vii) x+1/2, y, −z+3/2; (viii) x+1/2, y, −z+1/2; (ix) −x+1/2, −y, z−1/2; (x) −x+1/2, y+1/2, z−1/2; (xi) x, y, z−1; (xii) x−1/2, y, −z+1/2; (xiii) −x+1/2, −y+1, z−1/2; (xiv) x−1/2, y, −z+3/2.
Table 1
Selected geometric parameters (Å)
top
Cs1—O23.1951 (9)Mg1—O11.8847 (13)
Cs1—O2i3.2166 (9)Mg1—O3iv1.8932 (13)
Cs1—O3ii3.4476 (11)Mg1—O2v1.9228 (8)
Cs1—O1i3.5224 (11)P1—O11.5056 (13)
Cs1—O1ii3.6496 (11)P1—O31.5138 (13)
Cs1—O3iii3.6968 (18)P1—O21.5249 (8)
Symmetry codes: (i) −x+1, −y, −z+1; (ii) −x+1/2, −y+1, z+1/2; (iii) x+1/2, y, −z+3/2; (iv) x+1/2, y, −z+1/2; (v) −x+1/2, −y, z−1/2.
Acknowledgements top

The authors acknowledge the ICDD for financial support (grant No. 03–02).

references
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