


Supporting information
![]() | Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536810016363/wm2342sup1.cif |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S1600536810016363/wm2342Isup2.hkl |
Key indicators
- Single-crystal X-ray study
- T = 296 K
- Mean
(Lu-O) = 0.003 Å
- R factor = 0.020
- wR factor = 0.038
- Data-to-parameter ratio = 17.5
checkCIF/PLATON results
No syntax errors found
Alert level C PLAT910_ALERT_3_C Missing # of FCF Reflections Below Th(Min) ..... 1 PLAT915_ALERT_3_C Low Friedel Pair Coverage ...................... 75.77 Perc. PLAT041_ALERT_1_C Calc. and Reported SumFormula Strings Differ ? PLAT042_ALERT_1_C Calc. and Reported MoietyFormula Strings Differ ? PLAT045_ALERT_1_C Calculated and Reported Z Differ by ............ 0.50 Ratio PLAT950_ALERT_1_C Reported and Calculated Hmax Values Differ by .. 4
Alert level G REFLT03_ALERT_1_G ALERT: Expected hkl max differ from CIF values From the CIF: _diffrn_reflns_theta_max 30.41 From the CIF: _reflns_number_total 717 From the CIF: _diffrn_reflns_limit_ max hkl 11. 20. 9. From the CIF: _diffrn_reflns_limit_ min hkl -16. -6. -19. TEST1: Expected hkl limits for theta max Calculated maximum hkl 20. 20. 20. Calculated minimum hkl -20. -20. -20. REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 30.41 From the CIF: _reflns_number_total 717 Count of symmetry unique reflns 444 Completeness (_total/calc) 161.49% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 273 Fraction of Friedel pairs measured 0.615 Are heavy atom types Z>Si present yes PLAT180_ALERT_4_G Check Cell Rounding: # of Values Ending with 0 = 3 PLAT792_ALERT_1_G The Model has Chirality at P (Verify) .... S PLAT850_ALERT_4_G Check Flack Parameter Exact Value 0.00 and su .. 0.01
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 6 ALERT level C = Check and explain 5 ALERT level G = General alerts; check 6 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 3 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check
Single crystals of the title compound were obtained by solid state reaction while attempting to synthesized a long chain polyphosphate by reacting Lu2O3 with (NH4)H2PO4 and Rb2CO3 in an alumina boat. A mixture of these reagents in the molar ratio 27 : 85.5 : 8.7 was used for the synthesis. The mixture was successively heated at 473 K for 24 hours, then at 573 K for 24 additional hours and finally at 813 K for 24 hours. Then the sample was cooled down to 683 K at the rate of 3 K h-1 and maintained at this temperature for 36 hours. Finally, the sample was cooled down to room temperature by shutting the muffle furnace off. Single crystals were extracted from the batch by washing with hot water and filtering. The crystals were dried at 353 K in an oven. A translucent octahedral crystal of the title compound was selected for the structure refinement.
The highest residual peak in the final difference Fourier map was located 0.87 Å from atom Lu and the deepest hole was located 0.99 Å from atom Lu.
The title compound is the third polymorph of composition Lu(PO3)3 besides the monoclinic form described by Höppe & Sedlmaier (2007) and Yuan et al. (2008) and the trigonal form more recently reported by Bejaoui et al. (2008). The title compound is also the less dense polymorph with a calculated density of 3.451 Mg.m3 versus 3.587 Mg.m3 for the trigonal and 3.708 Mg.m3 for the monoclinic form and is probably the highest temperature form. This cyclotetraphosphate belongs to a structural type (cubic, with space group I43d) known since 1927 through the archetype Al4(P4O12)3 determined by Hendricks & Wyckoff (1927). Then Pauling & Sherman (1937) gave the first description of the structure and reported roughly estimated atomic coordinates deduced from geometrical considerations. Since this time only five members of this family, viz. Cr4III(P4O12)3 (Rémy & Boullé, 1964), Ti4III(P4O12)3 (Liebau & Williams, 1964), Fe4III(P4O12)3 (d'Yvoire et al., 1962), Sc4III(P4O12)3 (Bagieu-Beucher, 1976; Mezentseva et al.,1977 and Smolin et al., 1978) and Yb4III(P4O12)3 (Chudinova, 1979), have been identified. Corresponding unit cell parameters are listed in Durif (1995). Among these isotypic compounds only the structure of the Sc4(P4O12)3 cyclotetraphosphate has almost simultaneously been refined from single-crystal data by Bagieu-Beucher & Guittel (1978) and Smolin et al. (1978). Their refinements confirmed the description of Pauling & Sherman (1937) according to which all the crystallographically independent atoms except the AIII element (.3. symmetry) are in general positions. The structure is built of four-membered phosphate ring anions (P4O12)4- (Fig. 1), isolated from each other and further linked by LuO6 octahedra by sharing corners. Each LuO6 octahedron is linked to six (P4O12)4- rings (Fig. 2a) while each (P4O12)4- ring is linked to eight LuO6 octahedra (Fig. 2b) through oxygen atoms with shorter P—O distances (1.464 (4) and 1.481 (4) Å). The (P4O12)4- ring anions are located around the 12a Wyckoff positions of space group I43d and exhibit 4 symmetry. Comparison of the (P4O12)4- ring anions in both Sc4(P4O12)3 and Lu4(P4O12)3 structures shows these two ring anions being geometrically quite identical with alternating upward- and downward-pointing tetrahedra and P—O—P angles of 137.1° and 136.9 (2)°, respectively. The P—O distances in the PO4 groups are identical within their e.s.d.. The four bridging oxygen atoms of these ring anions are located at the apices of a flattened tetrahedron with characteristic angles of 148.22° and 94.30° for Sc and 147.95° and 94.37° for the Lu cyclotetraphosphate. The LuO6 octahedron is very slightly distorted along a threefold axis, resulting in two sets of Lu—O distances equal to 2.182 (3) and 2.185 (4) Å, respectively.
The title compound belongs to a structural type discovered a long time ago through the Al4(P4O12)3 member, the structure of which was first investigated by Hendricks & Wyckoff (1927) and then described by Pauling & Sherman (1937). Since then, five isotypic compounds have been characterized: Cr4(P4O12)3 (Rémy & Boullé, 1964); Ti4(P4O12)3 (Liebau & Williams, 1964); Fe4(P4O12)3 (d'Yvoire et al., 1962); Sc4(P4O12)3 (Bagieu-Beucher, 1976; Mezentseva et al., 1977; Bagieu-Beucher & Guitel, 1978; Smolin et al. 1978) and Yb4(P4O12)3 (Chudinova, 1979). For a review of the crystal chemistry of cyclotetraphosphates, see: Durif (1995). For other polymorphs of composition Lu(PO3)3, see: Höppe & Sedlmaier (2007); Yuan et al. (2008); Bejaoui et al. (2008).
Data collection: APEX2 (Bruker, 2008); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT (Bruker, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: CaRine (Boudias & Monceau, 1998) and ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).
Lu4(P4O12)3 | Dx = 3.451 Mg m−3 |
Mr = 1647.52 | Mo Kα radiation, λ = 0.71073 Å |
Cubic, I43d | Cell parameters from 1548 reflections |
Hall symbol: I -4bd 2c 3 | θ = 3.4–30.3° |
a = 14.6920 (6) Å | µ = 13.08 mm−1 |
V = 3171.3 (2) Å3 | T = 296 K |
Z = 4 | Truncated octahedron, colourless |
F(000) = 3008 | 0.18 × 0.10 × 0.08 mm |
Bruker APEXII CCD diffractometer | 717 independent reflections |
Radiation source: fine-focus sealed tube | 659 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.034 |
Detector resolution: 8.3333 pixels mm-1 | θmax = 30.4°, θmin = 3.9° |
φ and ω scans | h = −16→11 |
Absorption correction: multi-scan (SADABS; Bruker, 2008) | k = −6→20 |
Tmin = 0.534, Tmax = 0.746 | l = −19→9 |
3088 measured reflections |
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)] = 0.020 | w = 1/[σ2(Fo2) + (0.0088P)2] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.038 | (Δ/σ)max < 0.001 |
S = 1.03 | Δρmax = 0.90 e Å−3 |
717 reflections | Δρmin = −0.67 e Å−3 |
41 parameters | Absolute structure: Flack (1983), 272 Friedel pairs |
0 restraints | Absolute structure parameter: 0.000 (15) |
0 constraints |
Lu4(P4O12)3 | Z = 4 |
Mr = 1647.52 | Mo Kα radiation |
Cubic, I43d | µ = 13.08 mm−1 |
a = 14.6920 (6) Å | T = 296 K |
V = 3171.3 (2) Å3 | 0.18 × 0.10 × 0.08 mm |
Bruker APEXII CCD diffractometer | 717 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2008) | 659 reflections with I > 2σ(I) |
Tmin = 0.534, Tmax = 0.746 | Rint = 0.034 |
3088 measured reflections |
R[F2 > 2σ(F2)] = 0.020 | 0 restraints |
wR(F2) = 0.038 | Δρmax = 0.90 e Å−3 |
S = 1.03 | Δρmin = −0.67 e Å−3 |
717 reflections | Absolute structure: Flack (1983), 272 Friedel pairs |
41 parameters | Absolute structure parameter: 0.000 (15) |
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. |
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 | ||
Lu | 0.896610 (13) | 0.396610 (13) | 0.103390 (13) | 0.00602 (8) | |
P | 0.95737 (9) | 0.37294 (9) | 0.33447 (9) | 0.0077 (2) | |
O1 | 1.0613 (2) | 0.3432 (2) | 0.3430 (2) | 0.0128 (7) | |
O2 | 1.0325 (2) | 0.3642 (3) | 0.0522 (2) | 0.0188 (8) | |
O3 | 0.9295 (2) | 0.3498 (3) | 0.2404 (2) | 0.0142 (7) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Lu | 0.00602 (8) | 0.00602 (8) | 0.00602 (8) | 0.00039 (8) | −0.00039 (8) | −0.00039 (8) |
P | 0.0097 (5) | 0.0051 (6) | 0.0082 (6) | 0.0017 (5) | −0.0008 (5) | 0.0015 (4) |
O1 | 0.0113 (15) | 0.0146 (18) | 0.0123 (17) | 0.0007 (15) | −0.0025 (14) | 0.0054 (17) |
O2 | 0.0103 (17) | 0.024 (2) | 0.022 (2) | 0.0016 (18) | 0.0015 (16) | −0.0014 (18) |
O3 | 0.0202 (19) | 0.0141 (19) | 0.0084 (16) | 0.0012 (16) | −0.0050 (15) | 0.0023 (16) |
Lu—O3i | 2.182 (3) | P—O2iii | 1.464 (4) |
Lu—O3ii | 2.182 (3) | P—O3 | 1.481 (4) |
Lu—O3 | 2.182 (3) | P—O1iv | 1.583 (3) |
Lu—O2i | 2.185 (4) | P—O1 | 1.594 (3) |
Lu—O2ii | 2.185 (4) | O1—Pv | 1.583 (3) |
Lu—O2 | 2.185 (4) | O2—Pvi | 1.464 (4) |
O3i—Lu—O3ii | 89.06 (14) | O3—Lu—O2 | 92.64 (13) |
O3i—Lu—O3 | 89.06 (14) | O2i—Lu—O2 | 87.72 (15) |
O3ii—Lu—O3 | 89.06 (14) | O2ii—Lu—O2 | 87.72 (15) |
O3i—Lu—O2i | 92.64 (13) | O2iii—P—O3 | 118.0 (2) |
O3ii—Lu—O2i | 178.26 (14) | O2iii—P—O1iv | 107.3 (2) |
O3—Lu—O2i | 90.59 (14) | O3—P—O1iv | 111.5 (2) |
O3i—Lu—O2ii | 90.59 (14) | O2iii—P—O1 | 109.2 (2) |
O3ii—Lu—O2ii | 92.64 (13) | O3—P—O1 | 106.0 (2) |
O3—Lu—O2ii | 178.26 (14) | O1iv—P—O1 | 103.9 (2) |
O2i—Lu—O2ii | 87.72 (15) | Pv—O1—P | 136.9 (2) |
O3i—Lu—O2 | 178.26 (14) | Pvi—O2—Lu | 164.9 (2) |
O3ii—Lu—O2 | 90.59 (14) | P—O3—Lu | 148.2 (2) |
Symmetry codes: (i) −z+1, x−1/2, −y+1/2; (ii) y+1/2, −z+1/2, −x+1; (iii) −z+1, −x+3/2, y; (iv) −y+5/4, x−3/4, −z+3/4; (v) y+3/4, −x+5/4, −z+3/4; (vi) −y+3/2, z, −x+1. |
Experimental details
Crystal data | |
Chemical formula | Lu4(P4O12)3 |
Mr | 1647.52 |
Crystal system, space group | Cubic, I43d |
Temperature (K) | 296 |
a (Å) | 14.6920 (6) |
V (Å3) | 3171.3 (2) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 13.08 |
Crystal size (mm) | 0.18 × 0.10 × 0.08 |
Data collection | |
Diffractometer | Bruker APEXII CCD |
Absorption correction | Multi-scan (SADABS; Bruker, 2008) |
Tmin, Tmax | 0.534, 0.746 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3088, 717, 659 |
Rint | 0.034 |
(sin θ/λ)max (Å−1) | 0.712 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.020, 0.038, 1.03 |
No. of reflections | 717 |
No. of parameters | 41 |
Δρmax, Δρmin (e Å−3) | 0.90, −0.67 |
Absolute structure | Flack (1983), 272 Friedel pairs |
Absolute structure parameter | 0.000 (15) |
Computer programs: APEX2 (Bruker, 2008), SAINT (Bruker, 2008), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), CaRine (Boudias & Monceau, 1998) and ORTEP-3 (Farrugia, 1997), SHELXTL (Sheldrick, 2008).
Lu—O3i | 2.182 (3) | Lu—O2 | 2.185 (4) |
Lu—O3ii | 2.182 (3) | P—O2iii | 1.464 (4) |
Lu—O3 | 2.182 (3) | P—O3 | 1.481 (4) |
Lu—O2i | 2.185 (4) | P—O1iv | 1.583 (3) |
Lu—O2ii | 2.185 (4) | P—O1 | 1.594 (3) |
Symmetry codes: (i) −z+1, x−1/2, −y+1/2; (ii) y+1/2, −z+1/2, −x+1; (iii) −z+1, −x+3/2, y; (iv) −y+5/4, x−3/4, −z+3/4. |
The title compound is the third polymorph of composition Lu(PO3)3 besides the monoclinic form described by Höppe & Sedlmaier (2007) and Yuan et al. (2008) and the trigonal form more recently reported by Bejaoui et al. (2008). The title compound is also the less dense polymorph with a calculated density of 3.451 Mg.m3 versus 3.587 Mg.m3 for the trigonal and 3.708 Mg.m3 for the monoclinic form and is probably the highest temperature form. This cyclotetraphosphate belongs to a structural type (cubic, with space group I43d) known since 1927 through the archetype Al4(P4O12)3 determined by Hendricks & Wyckoff (1927). Then Pauling & Sherman (1937) gave the first description of the structure and reported roughly estimated atomic coordinates deduced from geometrical considerations. Since this time only five members of this family, viz. Cr4III(P4O12)3 (Rémy & Boullé, 1964), Ti4III(P4O12)3 (Liebau & Williams, 1964), Fe4III(P4O12)3 (d'Yvoire et al., 1962), Sc4III(P4O12)3 (Bagieu-Beucher, 1976; Mezentseva et al.,1977 and Smolin et al., 1978) and Yb4III(P4O12)3 (Chudinova, 1979), have been identified. Corresponding unit cell parameters are listed in Durif (1995). Among these isotypic compounds only the structure of the Sc4(P4O12)3 cyclotetraphosphate has almost simultaneously been refined from single-crystal data by Bagieu-Beucher & Guittel (1978) and Smolin et al. (1978). Their refinements confirmed the description of Pauling & Sherman (1937) according to which all the crystallographically independent atoms except the AIII element (.3. symmetry) are in general positions. The structure is built of four-membered phosphate ring anions (P4O12)4- (Fig. 1), isolated from each other and further linked by LuO6 octahedra by sharing corners. Each LuO6 octahedron is linked to six (P4O12)4- rings (Fig. 2a) while each (P4O12)4- ring is linked to eight LuO6 octahedra (Fig. 2b) through oxygen atoms with shorter P—O distances (1.464 (4) and 1.481 (4) Å). The (P4O12)4- ring anions are located around the 12a Wyckoff positions of space group I43d and exhibit 4 symmetry. Comparison of the (P4O12)4- ring anions in both Sc4(P4O12)3 and Lu4(P4O12)3 structures shows these two ring anions being geometrically quite identical with alternating upward- and downward-pointing tetrahedra and P—O—P angles of 137.1° and 136.9 (2)°, respectively. The P—O distances in the PO4 groups are identical within their e.s.d.. The four bridging oxygen atoms of these ring anions are located at the apices of a flattened tetrahedron with characteristic angles of 148.22° and 94.30° for Sc and 147.95° and 94.37° for the Lu cyclotetraphosphate. The LuO6 octahedron is very slightly distorted along a threefold axis, resulting in two sets of Lu—O distances equal to 2.182 (3) and 2.185 (4) Å, respectively.