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CeAsO4 was synthesized by the high-temperature solid-state reaction between CeO2, K2CO3 and (NH4)H2AsO4. The compound is isostructural with compounds of the monazite structure type. The structure is built up from CeO8 bis-disphenoids and AsO4 tetrahedra, joined by corners and edges.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802018664/br6063sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802018664/br6063Isup2.hkl
Contains datablock I

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](As-O) = 0.007 Å
  • R factor = 0.031
  • wR factor = 0.082
  • Data-to-parameter ratio = 12.7

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry

General Notes

ABSTM_02 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 0.925 Tmax scaled 0.490 Tmin scaled 0.203

Computing details top

Data collection: CAD-4 EXPRESS (Duisenberg, 1992; Macíček & Yordanov, 1992); cell refinement: CAD-4 EXPRESS; data reduction: MolEN (Fair, 1990); program(s) used to solve structure: SHELXS86 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg, 1998); software used to prepare material for publication: SHELXL97.

cerium arsenate top
Crystal data top
CeAsO4F(000) = 492
Mr = 279.03Dx = 5.663 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71069 Å
Hall symbol: -P 2ynCell parameters from 25 reflections
a = 6.975 (1) Åθ = 2.8–28.0°
b = 7.177 (1) ŵ = 23.77 mm1
c = 6.759 (2) ÅT = 293 K
β = 104.69 (1)°Parallelepiped, colorless
V = 327.29 (12) Å30.1 × 0.06 × 0.03 mm
Z = 4
Data collection top
Enraf-Nonius CAD-4
diffractometer
681 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.024
Graphite monochromatorθmax = 27.0°, θmin = 3.8°
ω/2θ scansh = 88
Absorption correction: ψ scan
(North et al. 1968)
k = 99
Tmin = 0.22, Tmax = 0.53l = 80
1478 measured reflections2 standard reflections every 120 min
712 independent reflections intensity decay: 0.4%
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)] = 0.031 w = 1/[σ2(Fo2) + (0.0592P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.082(Δ/σ)max = 0.03
S = 1.24Δρmax = 1.97 e Å3
712 reflectionsΔρmin = 3.18 e Å3
56 parametersExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 1263 (56)
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
Ce0.21913 (8)0.15370 (8)0.40111 (8)0.0203 (4)
As0.19637 (17)0.16297 (13)0.88645 (15)0.0197 (4)
O10.1098 (12)0.3406 (8)0.0013 (12)0.0257 (16)
O20.0155 (10)0.1083 (10)0.6742 (10)0.0256 (13)
O30.2457 (10)0.0040 (10)0.0691 (9)0.0246 (14)
O40.3808 (10)0.2171 (11)0.7766 (10)0.0255 (13)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ce0.0203 (5)0.0195 (6)0.0212 (5)0.00000 (14)0.0051 (3)0.00056 (15)
As0.0199 (7)0.0196 (7)0.0197 (7)0.0002 (3)0.0053 (5)0.0001 (3)
O10.028 (4)0.023 (4)0.030 (4)0.000 (2)0.012 (3)0.004 (2)
O20.023 (3)0.026 (3)0.026 (3)0.001 (3)0.003 (3)0.002 (3)
O30.031 (3)0.018 (3)0.024 (3)0.000 (3)0.007 (3)0.002 (2)
O40.026 (3)0.027 (3)0.026 (3)0.001 (3)0.011 (3)0.002 (3)
Geometric parameters (Å, º) top
Ce—O2i2.460 (7)Ce—O22.619 (7)
Ce—O3ii2.472 (7)Ce—O1v2.636 (8)
Ce—O4iii2.476 (7)As—O1vi1.683 (6)
Ce—O42.543 (7)As—O41.685 (7)
Ce—O1iv2.551 (7)As—O3vi1.692 (7)
Ce—O32.562 (6)As—O21.699 (7)
O1vi—As—O4115.6 (4)O1vi—As—O2106.7 (4)
O1vi—As—O3vi103.3 (3)O4—As—O299.7 (3)
O4—As—O3vi116.6 (3)O3vi—As—O2115.0 (4)
Symmetry codes: (i) x, y, z+1; (ii) x+1/2, y+1/2, z+1/2; (iii) x1/2, y+1/2, z1/2; (iv) x+1/2, y1/2, z+1/2; (v) x+1/2, y+1/2, z+1/2; (vi) x, y, z+1.
 

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