Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270103011417/bc1018sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S0108270103011417/bc1018Isup2.hkl |
Cs[Mg(H2O)6](PO4) was formed by hydrothermal synthesis in the Cs3PO4–Mg(OH)2–H2O system (T = 280°C, P = 70 bar, t = 20 days, ratio Cs3PO4/Mg(OH)2 = 1:1) in 7 ml Cu tubes in a steel autoclave. Very small (<0.05 mm) colourless octahedral crystals often formed aggregates of 15–20 individuals. The presence of Cs, P and Mg atoms in the samples was confirmed by qualitative X-ray spectral analysis (CamScan 4DV and EDA Link AN 1000).
Data collection: Win-Xpose in X-AREA (Stoe & Cie, 2000); cell refinement: Win-Cell in X-AREA; data reduction: Win-Integrate in X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg, 1999).
Cs[Mg(H2O)6](PO4) | Mo Kα radiation, λ = 0.71073 Å |
Mr = 360.29 | Cell parameters from 2068 reflections |
Cubic, F43m | θ = 3.5–29.6° |
a = 10.0308 (14) Å | µ = 3.92 mm−1 |
V = 1009.3 (2) Å3 | T = 295 K |
Z = 4 | Octahedron, colourless |
F(000) = 696 | 0.04 × 0.04 × 0.04 mm |
Dx = 2.371 Mg m−3 |
Stoe IPDS-II diffractometer | 176 independent reflections |
Radiation source: fine-focus sealed tube | 163 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.028 |
Detector resolution: 150 pixels mm-1 | θmax = 29.7°, θmin = 3.5° |
ω scans | h = −13→13 |
Absorption correction: multi-scan XPREP in SHELXTL (Sheldrick, 1996) | k = −12→12 |
Tmin = 0.774, Tmax = 0.831 | l = −13→12 |
1751 measured reflections |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.017 | All H-atom parameters refined |
wR(F2) = 0.035 | w = 1/[σ2(Fo2) + (0.02P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.11 | (Δ/σ)max < 0.001 |
176 reflections | Δρmax = 0.19 e Å−3 |
14 parameters | Δρmin = −0.21 e Å−3 |
0 restraints | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: −0.04 (3) |
Cs[Mg(H2O)6](PO4) | Z = 4 |
Mr = 360.29 | Mo Kα radiation |
Cubic, F43m | µ = 3.92 mm−1 |
a = 10.0308 (14) Å | T = 295 K |
V = 1009.3 (2) Å3 | 0.04 × 0.04 × 0.04 mm |
Stoe IPDS-II diffractometer | 176 independent reflections |
Absorption correction: multi-scan XPREP in SHELXTL (Sheldrick, 1996) | 163 reflections with I > 2σ(I) |
Tmin = 0.774, Tmax = 0.831 | Rint = 0.028 |
1751 measured reflections |
R[F2 > 2σ(F2)] = 0.017 | All H-atom parameters refined |
wR(F2) = 0.035 | Δρmax = 0.19 e Å−3 |
S = 1.11 | Δρmin = −0.21 e Å−3 |
176 reflections | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
14 parameters | Absolute structure parameter: −0.04 (3) |
0 restraints |
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. |
x | y | z | Uiso*/Ueq | ||
Cs | 0.7500 | 0.7500 | 0.7500 | 0.0560 (2) | |
Mg | 0.0000 | 0.0000 | 0.0000 | 0.0307 (5) | |
P | 0.2500 | 0.2500 | 0.2500 | 0.0279 (3) | |
O2 | 0.2059 (3) | 0.0000 | 0.0000 | 0.0565 (8) | |
O1 | 0.33857 (17) | 0.33857 (17) | 0.33857 (17) | 0.0346 (6) | |
H | 0.252 (5) | 0.047 (2) | 0.047 (2) | 0.052 (8)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cs | 0.0560 (2) | 0.0560 (2) | 0.0560 (2) | 0.000 | 0.000 | 0.000 |
Mg | 0.0307 (5) | 0.0307 (5) | 0.0307 (5) | 0.000 | 0.000 | 0.000 |
P | 0.0279 (3) | 0.0279 (3) | 0.0279 (3) | 0.000 | 0.000 | 0.000 |
O2 | 0.0335 (12) | 0.0679 (12) | 0.0679 (12) | 0.000 | 0.000 | −0.0360 (18) |
O1 | 0.0346 (6) | 0.0346 (6) | 0.0346 (6) | −0.0032 (6) | −0.0032 (6) | −0.0032 (6) |
Cs—O2i | 3.5740 (6) | Mg—O2xv | 2.065 (3) |
Cs—O2ii | 3.5740 (6) | Mg—O2xvi | 2.065 (3) |
Cs—O2iii | 3.5740 (6) | Mg—O2xvii | 2.065 (3) |
Cs—O2iv | 3.5740 (6) | Mg—Csxviii | 4.3435 (6) |
Cs—O2v | 3.5740 (6) | Mg—Csxix | 4.3435 (6) |
Cs—O2vi | 3.5740 (6) | Mg—Csxx | 4.3435 (6) |
Cs—O2vii | 3.5739 (6) | Mg—Csxxi | 4.3435 (6) |
Cs—O2viii | 3.5739 (6) | P—O1 | 1.539 (3) |
Cs—O2ix | 3.5740 (6) | P—O1xxii | 1.539 (3) |
Cs—O2x | 3.5739 (6) | P—O1xxiii | 1.539 (3) |
Cs—O2xi | 3.5739 (6) | P—O1xxiv | 1.539 (3) |
Cs—O2xii | 3.5740 (6) | O2—Csxix | 3.5740 (6) |
Mg—O2 | 2.065 (3) | O2—Csxx | 3.5740 (6) |
Mg—O2xiii | 2.065 (3) | O2—H | 0.82 (4) |
Mg—O2xiv | 2.065 (3) | ||
O2i—Cs—O2ii | 48.23 (8) | O2viii—Cs—O2xii | 119.494 (6) |
O2i—Cs—O2iii | 48.23 (8) | O2ix—Cs—O2xii | 165.77 (9) |
O2ii—Cs—O2iii | 48.23 (8) | O2x—Cs—O2xii | 71.43 (7) |
O2i—Cs—O2iv | 165.77 (9) | O2xi—Cs—O2xii | 119.494 (6) |
O2ii—Cs—O2iv | 119.494 (6) | O2—Mg—O2xiii | 90.0 |
O2iii—Cs—O2iv | 119.494 (6) | O2—Mg—O2xiv | 90.0 |
O2i—Cs—O2v | 119.494 (6) | O2xiii—Mg—O2xiv | 180.0 |
O2ii—Cs—O2v | 165.77 (9) | O2—Mg—O2xv | 90.0 |
O2iii—Cs—O2v | 119.494 (6) | O2xiii—Mg—O2xv | 90.0 |
O2iv—Cs—O2v | 71.43 (7) | O2xiv—Mg—O2xv | 90.0 |
O2i—Cs—O2vi | 119.494 (6) | O2—Mg—O2xvi | 90.0 |
O2ii—Cs—O2vi | 119.494 (6) | O2xiii—Mg—O2xvi | 90.0 |
O2iii—Cs—O2vi | 165.77 (9) | O2xiv—Mg—O2xvi | 90.0 |
O2iv—Cs—O2vi | 71.43 (7) | O2xv—Mg—O2xvi | 180.0 |
O2v—Cs—O2vi | 71.43 (7) | O2—Mg—O2xvii | 180.0 |
O2i—Cs—O2vii | 90.879 (11) | O2xiii—Mg—O2xvii | 90.0 |
O2ii—Cs—O2vii | 119.494 (6) | O2xiv—Mg—O2xvii | 90.0 |
O2iii—Cs—O2vii | 71.43 (7) | O2xv—Mg—O2xvii | 90.0 |
O2iv—Cs—O2vii | 90.879 (11) | O2xvi—Mg—O2xvii | 90.0 |
O2v—Cs—O2vii | 48.23 (8) | O2—Mg—Csxviii | 125.3 |
O2vi—Cs—O2vii | 119.494 (6) | O2xiii—Mg—Csxviii | 54.7 |
O2i—Cs—O2viii | 90.879 (12) | O2xiv—Mg—Csxviii | 125.3 |
O2ii—Cs—O2viii | 71.43 (7) | O2xv—Mg—Csxviii | 54.7 |
O2iii—Cs—O2viii | 119.494 (6) | O2xvi—Mg—Csxviii | 125.3 |
O2iv—Cs—O2viii | 90.879 (11) | O2xvii—Mg—Csxviii | 54.7 |
O2v—Cs—O2viii | 119.494 (6) | O2—Mg—Csxix | 54.7 |
O2vi—Cs—O2viii | 48.23 (8) | O2xiii—Mg—Csxix | 54.7 |
O2vii—Cs—O2viii | 165.77 (9) | O2xiv—Mg—Csxix | 125.3 |
O2i—Cs—O2ix | 119.494 (6) | O2xv—Mg—Csxix | 125.3 |
O2ii—Cs—O2ix | 71.43 (7) | O2xvi—Mg—Csxix | 54.7 |
O2iii—Cs—O2ix | 90.879 (11) | O2xvii—Mg—Csxix | 125.3 |
O2iv—Cs—O2ix | 48.23 (8) | Csxviii—Mg—Csxix | 109.5 |
O2v—Cs—O2ix | 119.494 (7) | O2—Mg—Csxx | 54.7 |
O2vi—Cs—O2ix | 90.879 (11) | O2xiii—Mg—Csxx | 125.3 |
O2vii—Cs—O2ix | 119.494 (7) | O2xiv—Mg—Csxx | 54.7 |
O2viii—Cs—O2ix | 71.43 (7) | O2xv—Mg—Csxx | 54.736 (1) |
O2i—Cs—O2x | 71.43 (7) | O2xvi—Mg—Csxx | 125.3 |
O2ii—Cs—O2x | 90.879 (12) | O2xvii—Mg—Csxx | 125.3 |
O2iii—Cs—O2x | 119.494 (6) | Csxviii—Mg—Csxx | 109.5 |
O2iv—Cs—O2x | 119.494 (6) | Csxix—Mg—Csxx | 109.471 (1) |
O2v—Cs—O2x | 90.879 (11) | O2—Mg—Csxxi | 125.3 |
O2vi—Cs—O2x | 48.23 (8) | O2xiii—Mg—Csxxi | 125.3 |
O2vii—Cs—O2x | 119.494 (6) | O2xiv—Mg—Csxxi | 54.7 |
O2viii—Cs—O2x | 48.23 (8) | O2xv—Mg—Csxxi | 125.3 |
O2ix—Cs—O2x | 119.494 (6) | O2xvi—Mg—Csxxi | 54.7 |
O2i—Cs—O2xi | 119.494 (6) | O2xvii—Mg—Csxxi | 54.736 (1) |
O2ii—Cs—O2xi | 90.879 (11) | Csxviii—Mg—Csxxi | 109.5 |
O2iii—Cs—O2xi | 71.43 (7) | Csxix—Mg—Csxxi | 109.471 (1) |
O2iv—Cs—O2xi | 48.23 (8) | Csxx—Mg—Csxxi | 109.5 |
O2v—Cs—O2xi | 90.879 (12) | O1—P—O1xxii | 109.471 (1) |
O2vi—Cs—O2xi | 119.494 (6) | O1—P—O1xxiii | 109.5 |
O2vii—Cs—O2xi | 71.43 (7) | O1xxii—P—O1xxiii | 109.5 |
O2viii—Cs—O2xi | 119.494 (6) | O1—P—O1xxiv | 109.5 |
O2ix—Cs—O2xi | 48.23 (8) | O1xxii—P—O1xxiv | 109.471 (1) |
O2x—Cs—O2xi | 165.77 (9) | O1xxiii—P—O1xxiv | 109.5 |
O2i—Cs—O2xii | 71.43 (7) | Mg—O2—Csxix | 97.12 (4) |
O2ii—Cs—O2xii | 119.494 (6) | Mg—O2—Csxx | 97.12 (4) |
O2iii—Cs—O2xii | 90.879 (11) | Csxix—O2—Csxx | 165.77 (9) |
O2iv—Cs—O2xii | 119.494 (7) | Mg—O2—H | 125 (3) |
O2v—Cs—O2xii | 48.23 (8) | Csxix—O2—H | 85.9 (3) |
O2vi—Cs—O2xii | 90.879 (11) | Csxx—O2—H | 85.9 (3) |
O2vii—Cs—O2xii | 48.23 (8) | Hxxv—O2—H | 110.46 (2) |
Symmetry codes: (i) −y+1, z+1, −x+1; (ii) z+1, −x+1, −y+1; (iii) −x+1, −y+1, z+1; (iv) −y+1/2, z+1/2, −x+1; (v) z+1/2, −x+1, −y+1/2; (vi) −x+1, −y+1/2, z+1/2; (vii) y+1/2, z+1, x+1/2; (viii) y+1, z+1/2, x+1/2; (ix) x+1/2, y+1/2, z+1; (x) z+1, x+1/2, y+1/2; (xi) z+1/2, x+1/2, y+1; (xii) x+1/2, y+1, z+1/2; (xiii) −y, z, −x; (xiv) y, z, x; (xv) z, −x, −y; (xvi) z, x, y; (xvii) −x, −y, z; (xviii) x−1, y−1, z−1; (xix) x−1/2, y−1/2, z−1; (xx) x−1/2, y−1, z−1/2; (xxi) x−1, y−1/2, z−1/2; (xxii) x, −y+1/2, −z+1/2; (xxiii) −x+1/2, y, −z+1/2; (xxiv) −x+1/2, −y+1/2, z; (xxv) x, −y, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H···O1xxii | 0.82 (4) | 1.83 (3) | 2.649 (2) | 173 (5) |
Symmetry code: (xxii) x, −y+1/2, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | Cs[Mg(H2O)6](PO4) |
Mr | 360.29 |
Crystal system, space group | Cubic, F43m |
Temperature (K) | 295 |
a (Å) | 10.0308 (14) |
V (Å3) | 1009.3 (2) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 3.92 |
Crystal size (mm) | 0.04 × 0.04 × 0.04 |
Data collection | |
Diffractometer | Stoe IPDS-II diffractometer |
Absorption correction | Multi-scan XPREP in SHELXTL (Sheldrick, 1996) |
Tmin, Tmax | 0.774, 0.831 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 1751, 176, 163 |
Rint | 0.028 |
(sin θ/λ)max (Å−1) | 0.696 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.017, 0.035, 1.11 |
No. of reflections | 176 |
No. of parameters | 14 |
H-atom treatment | All H-atom parameters refined |
Δρmax, Δρmin (e Å−3) | 0.19, −0.21 |
Absolute structure | Flack H D (1983), Acta Cryst. A39, 876-881 |
Absolute structure parameter | −0.04 (3) |
Computer programs: Win-Xpose in X-AREA (Stoe & Cie, 2000), Win-Cell in X-AREA, Win-Integrate in X-AREA, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), DIAMOND (Brandenburg, 1999).
Cs—O2i | 3.5740 (6) | P—O1 | 1.539 (3) |
Mg—O2 | 2.065 (3) | O2—H | 0.82 (4) |
Mg—O2—H | 125 (3) | Hii—O2—H | 110.46 (2) |
Symmetry codes: (i) −y+1, z+1, −x+1; (ii) x, −y, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H···O1iii | 0.82 (4) | 1.83 (3) | 2.649 (2) | 173 (5) |
Symmetry code: (iii) x, −y+1/2, −z+1/2. |
In the course of investigations of magnesium phosphate minerals, such as bakchisaraitsevite, Na2(Mg4.5Fe0.5)[PO4]4·7H2O (Yakubovich et al., 2000), and their synthetic relatives, we have studied the products of soft hydrothermal syntheses in the Cs3PO4–Mg(OH)2–H2O system and found crystals of a new polymorph of Cs[Mg(H2O)6](PO4). Its structure has been determined by single-crystal X-ray diffraction. A hexagonal form was already known for this compound (Ferrari et al., 1955), but a cubic structure was deduced from powder diffraction data for the As analogue, Cs[Mg(H2O)6](AsO4).
Our crystal of Cs[Mg(H2O)6](PO4) belongs to the cubic F-43m space group. According to the high site symmetry (−43m) of the 4 d position, the Mg2+ ions occupy regular octahedra formed by the O2 atoms, with Mg—O distances of 2.065 (3) Å (Fig. 1). H atoms were localized and refined on the 48t h position, resulting in a sensible geometry for the aqua ligands.
Regular PO4 tetrahedra are connected `face-to-face' to four neighbouring [Mg(H2O)6]2+ cations by three strong hydrogen bonds [O2···O1 = 2.649 (2) Å and O2—H···O1 173 (5)°; Figs. 1 and 2, and Table 1]. Conversely, the octahedral cations are tetrahedrally surrounded by four anions. Thus, a sphalerite-like three-dimensional framework is formed, with [Mg(H2O)6]2+ and [PO4]3− complexes in the positions of the Zn2+ and S2− ions. The Cs+ cations center the volume and the edges of the cubic unit cell (Fig. 2). They are in the center of a cuboctahedron of 12 H2O-ligands from four [Mg(H2O)6]2+ cations. If the contacts of the Cs+ anions to these ligands are included, the O2 atoms are in an approximate trigonal-pyramidal environment. The two cations and the phosphate anion form cubic F-centered sublattices with shifted origins in 0,0,0 (Mg), 1/4,1/4,1/4 (P) and 3/4,3/4,3/4 (Cs), respectively. Thus, this simple cubic structure can also be derived from a rock-salt type '{Cs(PO4)}2−' structure, with [Mg(H2O)6]2+ cations in every second center of the Cs4(PO4)4 sub-cubes. This structure corresponds to that proposed for the arsenate analogue, Cs[Mg(H2O)6](AsO4), on the basis of powder data (Ferrari et al., 1955). The larger atomic radius of As compared with P is consistent with the enlargement of the unit-cell volume by about 6% with respect to the phosphate. For the latter, these authors found a hexagonal form [space group P63mc; a = 6.939 (2) Å and c = 11.896 (2) Å]. The volume per formula unit in the cubic polymorph [252.3 (1) Å3] is slightly larger (1.7%) than that of the hexagonal form (248.0 Å3), pointing to metastability of the cubic form.
The differences between the two structural forms can be described in terms of different sequences of close-packed layers of the Cs+, [Mg(H2O)6]2+ and PO43− components.
In the cubic form, each sublattice is arranged along the [111] direction in a cubic close packing (CCP), as indicated in Fig. 3(a) by the ABC (PO4), bca ([Mg(H2O)6]) and γαβ (Cs) sequences. In addition, the sequence of these alternating layers is also of the CCP-type (Abγ Bcα Caβ). In the hexagonal form, the [Mg(H2O)6]2+ and Cs+ cations form hexagonal close-packed sequences (bcb and γβγ) along the c axis. The phosphate anions are aligned along c but with alternating orientation (AA'A; Fig. 3 b).
A similar pseudohexagonal unit cell can be identified in the orthorhombic structures (space group Pmn21) of two analogues of the title compound, viz. the mineral struvite, (NH4)Mg(H2O)6[PO4], which seems to form as a result of bacterial attack on organic material (Whitaker & Jefferey, 1970; Dickens & Brown, 1972; Abbona et al., 1986; Ferraris et al., 1986), and a synthetic phase, KMg(H2O)6[PO4] (Mathew & Schröder, 1979). According to Dickens & Brown (1972), the {h0l} reflections of struvite show pseudohexagonal symmetry. As shown in Fig. 3c, layers of [PO4] tetrahedra are now stacked in a hexagonal primitive sequence (AAA). In contrast to the Cs compound, mixed layers of [Mg(H2O)6]2+ and ammonium cations follow so that, together with the phosphate anions, a cubic sequence results (AbcAbc).
The different packings in these related compounds correlate with significant differences in the hydrogen bonding networks. In the cubic Cs compound, the [Mg(H2O)6]2+ cations are tetrahedrally surrounded by four phosphate anions with four `face-to-face' triple hydrogen bonds. Although no H-atom positions are reported for the hexagonal form, it can be concluded from the O···O distances that the [Mg(H2O)6]2+ cations are surrounded by six PO4 anions in a trigonal-prismatic arrangement and are connected by three `edge-to-corner' and three `corner-to-edge' hydrogen bonds. A similar trigonal prismatic coordination is found in the struvite structure, which is connected by two `face-to-face', one `edge-to-edge' and three `corner-to-corner' hydrogen bonds. In addition, an O—H···N hydrogen bond links? one of the aqua ligands to the ammonium cation.