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The crystal structure of the title compound, PbGeO3, shows a three-dimensional framework assembled by Pb6 and Ge6 structural building units. The Pb atom is coordinated by five O atoms in square-pyramidal coordination, while the Ge atom is tetra­hedrally coordinated by four O atoms.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806017697/fi2002sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806017697/fi2002Isup2.hkl
Contains datablock I

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](e-O) = 0.019 Å
  • R factor = 0.050
  • wR factor = 0.164
  • Data-to-parameter ratio = 13.4

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT031_ALERT_4_C Refined Extinction Parameter within Range ...... 2.75 Sigma PLAT062_ALERT_4_C Rescale T(min) & T(max) by ..................... 0.64 PLAT120_ALERT_1_C Reported SPGR R-3 Inconsistent with Explicit R-3R PLAT128_ALERT_4_C Non-standard setting of Space group R-3 .... R-3r PLAT144_ALERT_4_C su on alpha Small or Missing (x 10000) ..... 2 Deg. PLAT199_ALERT_1_C Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_C Check the Reported _diffrn_ambient_temperature . 293 K PLAT731_ALERT_1_C Bond Calc 3.6909(17), Rep 3.6910(8) ...... 2.12 su-Rat PB1 -PB1 1.555 5.665 PLAT731_ALERT_1_C Bond Calc 3.6909(18), Rep 3.6910(8) ...... 2.25 su-Rat PB1 -PB1 1.555 6.656
Alert level G ABSTM02_ALERT_3_G When printed, the submitted absorption T values will be replaced by the scaled T values. Since the ratio of scaled T's is identical to the ratio of reported T values, the scaling does not imply a change to the absorption corrections used in the study. Ratio of Tmax expected/reported 0.640 Tmax scaled 0.176 Tmin scaled 0.132 REFLT03_ALERT_1_G ALERT: Expected hkl max differ from CIF values From the CIF: _diffrn_reflns_theta_max 25.50 From the CIF: _reflns_number_total 628 From the CIF: _diffrn_reflns_limit_ max hkl 10. 7. 11. From the CIF: _diffrn_reflns_limit_ min hkl -10. -8. -11. TEST1: Expected hkl limits for theta max Calculated maximum hkl 11. 11. 11. Calculated minimum hkl -11. -11. -11.
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 9 ALERT level C = Check and explain 2 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 1 ALERT type 3 Indicator that the structure quality may be low 4 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Bruker, 2002); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997a); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997a); molecular graphics: SHELXTL (Sheldrick, 1997b); software used to prepare material for publication: SHELXTL.

(I) top
Crystal data top
GeO3PbDx = 6.373 Mg m3
Mr = 327.78Mo Kα radiation, λ = 0.71073 Å
Rhombohedral, R3Cell parameters from 2654 reflections
Hall symbol: -P 3*θ = 2.6–25.5°
a = 9.3282 (2) ŵ = 57.82 mm1
α = 113.4560 (2)°T = 293 K
V = 512.43 (2) Å3Block, colourless
Z = 60.04 × 0.03 × 0.03 mm
F(000) = 828
Data collection top
Bruker Apex2 CCD
diffractometer
628 independent reflections
Radiation source: fine-focus sealed tube553 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.047
ω scansθmax = 25.5°, θmin = 2.6°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
h = 1010
Tmin = 0.206, Tmax = 0.276k = 87
2654 measured reflectionsl = 1111
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.050 w = 1/[σ2(Fo2) + (0.1096P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.164(Δ/σ)max = 0.001
S = 1.21Δρmax = 4.40 e Å3
628 reflectionsΔρmin = 3.49 e Å3
47 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
18 restraintsExtinction coefficient: 0.0022 (8)
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
Pb10.71054 (12)0.01082 (12)0.17220 (12)0.0139 (5)
Ge11.2560 (3)0.5203 (3)0.6560 (3)0.0114 (7)
O11.033 (2)0.287 (2)0.540 (2)0.018 (3)
O21.478 (2)0.545 (2)0.777 (2)0.019 (3)
O30.684 (2)0.265 (2)0.152 (2)0.020 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pb10.0151 (6)0.0162 (6)0.0148 (6)0.0111 (5)0.0112 (5)0.0108 (5)
Ge10.0109 (12)0.0089 (11)0.0113 (12)0.0056 (10)0.0067 (10)0.0065 (10)
O10.019 (4)0.020 (5)0.015 (4)0.011 (3)0.013 (3)0.012 (3)
O20.019 (5)0.017 (4)0.021 (5)0.010 (3)0.012 (3)0.015 (4)
O30.017 (4)0.021 (5)0.021 (5)0.013 (3)0.016 (4)0.011 (3)
Geometric parameters (Å, º) top
Pb1—O1i2.270 (14)Ge1—O3v1.725 (15)
Pb1—O3ii2.416 (15)Ge1—O21.779 (15)
Pb1—O12.458 (14)Ge1—O2vi1.781 (15)
Pb1—O32.551 (16)O1—Pb1vii2.270 (14)
Pb1—O3iii2.590 (15)O2—Ge1viii1.781 (15)
Pb1—Pb1iv3.6910 (8)O3—Ge1v1.725 (15)
Pb1—Pb1ii3.6910 (8)O3—Pb1iv2.416 (15)
Ge1—O11.723 (14)O3—Pb1iii2.590 (15)
O1i—Pb1—O3ii78.6 (6)O3iii—Pb1—Pb1ii118.2 (3)
O1i—Pb1—O186.5 (5)Pb1iv—Pb1—Pb1ii118.066 (12)
O3ii—Pb1—O172.9 (5)O1—Ge1—O3v113.3 (7)
O1i—Pb1—O378.1 (5)O1—Ge1—O2111.9 (7)
O3ii—Pb1—O3153.4 (5)O3v—Ge1—O2106.0 (7)
O1—Pb1—O393.1 (5)O1—Ge1—O2vi107.6 (7)
O1i—Pb1—O3iii72.8 (5)O3v—Ge1—O2vi111.4 (7)
O3ii—Pb1—O3iii101.1 (6)O2—Ge1—O2vi106.6 (9)
O1—Pb1—O3iii159.3 (5)Ge1—O1—Pb1vii122.8 (7)
O3—Pb1—O3iii84.0 (5)Ge1—O1—Pb1128.1 (7)
O1i—Pb1—Pb1iv118.6 (4)Pb1vii—O1—Pb1108.6 (6)
O3ii—Pb1—Pb1iv161.0 (4)Ge1—O2—Ge1viii127.3 (8)
O1—Pb1—Pb1iv98.6 (3)Ge1v—O3—Pb1iv121.8 (7)
O3—Pb1—Pb1iv40.6 (3)Ge1v—O3—Pb1126.6 (8)
O3iii—Pb1—Pb1iv92.5 (3)Pb1iv—O3—Pb196.0 (5)
O1i—Pb1—Pb1ii121.4 (4)Ge1v—O3—Pb1iii110.9 (7)
O3ii—Pb1—Pb1ii43.4 (4)Pb1iv—O3—Pb1iii100.2 (5)
O1—Pb1—Pb1ii71.5 (4)Pb1—O3—Pb1iii96.0 (5)
O3—Pb1—Pb1ii153.0 (3)
Symmetry codes: (i) z, x1, y; (ii) y+1, z, x+1; (iii) x+1, y, z; (iv) z+1, x+1, y; (v) x+2, y+1, z+1; (vi) z+2, x+2, y+1; (vii) y+1, z, x; (viii) y+2, z+1, x+2.
 

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