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The crystal structure of the low-temperature (LT) modification of LaBO3 has been redetermined from single-crystal X-ray data; the resulting structure confirms the previous study [Abdullaev, Dzhafarov & Mamedov (1976). Azerbaidzhanskii Khim. Zh. pp. 117–120], but with improved precision. LT-LaBO3 crystallizes in space group Pnma and adopts the aragonite-type structure. Except for one O atom, which is situated on a general position, all other atoms (one La, one B and a second O atom) lie on mirror planes. The structure is composed of LaO9 polyhedra with an average La—O distance of 2.593 Å and trigonal BO3 groups with an average B—O distance of 1.373 Å. Slight anisotropies of the thermal vibrations of La and B atoms suggest that the electrostatic La...La and La...B inter­actions across the shared edges are weak.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806010142/wm2006sup1.cif
Contains datablocks General, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806010142/wm2006Isup2.hkl
Contains datablock I

Key indicators

  • Single-crystal X-ray study
  • T = 296 K
  • Mean [sigma](O-B)= 0.004 Å
  • R factor = 0.017
  • wR factor = 0.029
  • Data-to-parameter ratio = 12.7

checkCIF/PLATON results

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Computing details top

Data collection: WinAFC (Rigaku Corporation, 1999); cell refinement: WinAFC; data reduction: TEXSAN (Molecular Structure Corporation, 1999); program(s) used to solve structure: TEXSAN; program(s) used to refine structure: TEXSAN; molecular graphics: ATOMS (Dowty, 2000); software used to prepare material for publication: TEXSAN.

lanthanum orthoborate top
Crystal data top
LaBO3F(000) = 344
Mr = 197.71Dx = 5.299 Mg m3
Orthorhombic, PnmaMo Kα radiation, λ = 0.71069 Å
Hall symbol: -P 2ac 2nCell parameters from 50 reflections
a = 5.8744 (3) Åθ = 22.5–25.0°
b = 5.1087 (3) ŵ = 16.88 mm1
c = 8.2581 (5) ÅT = 296 K
V = 247.83 (2) Å3Irregular, colorless
Z = 40.06 × 0.05 × 0.04 mm
Data collection top
Rigaku AFC-7R
diffractometer
Rint = 0.030
ω–2θ scansθmax = 30.0°
Absorption correction: part of the refinement model (ΔF)
(Walker & Stuart, 1983)
h = 88
Tmin = 0.418, Tmax = 0.509k = 07
1591 measured reflectionsl = 1111
396 independent reflections3 standard reflections every 150 reflections
369 reflections with F2 > 2σ(F2) intensity decay: 0.6%
Refinement top
Refinement on F w = 1/[σ2(Fo) + 0.00014|Fo|2]
R[F2 > 2σ(F2)] = 0.017(Δ/σ)max = 0.001
wR(F2) = 0.029Δρmax = 1.24 e Å3
S = 1.98Δρmin = 0.98 e Å3
369 reflectionsExtinction correction: Zachariasen (1967) type 2 Gaussian isotropic
29 parametersExtinction coefficient: 0.056 (3)
Special details top

Refinement. Refinement using reflections with F2 > 2.0 σ(F2). The weighted R-factor (wR), goodness of fit (S) and R-factor (gt) are based on F, with F set to zero for negative F. The threshold expression of F2 > 2.0 σ(F2) is used only for calculating R-factor (gt).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
La0.24319 (3)0.25000.58449 (3)0.0062 (1)
B0.5822 (7)0.25000.2611 (5)0.0079 (10)
O10.0970 (5)0.25000.0729 (3)0.0097 (7)
O20.5863 (4)0.0182 (4)0.1769 (2)0.0092 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
La0.0062 (2)0.0062 (2)0.0063 (2)0.00000.00038 (6)0.0000
B0.007 (2)0.008 (2)0.009 (2)0.00000.000 (1)0.0000
O10.011 (1)0.012 (1)0.006 (1)0.00000.002 (1)0.0000
O20.0118 (9)0.0064 (9)0.0095 (9)0.0000 (8)0.0002 (7)0.0008 (8)
Geometric parameters (Å, º) top
La—O1i2.451 (3)B—O2i3.230 (4)
La—O1ii2.723 (1)B—O2x3.230 (4)
La—O1iii2.723 (1)B—Bi2.943 (6)
La—O2ii2.491 (2)B—Bv2.943 (6)
La—O2iv2.491 (2)O1—O1xiii3.045 (3)
La—O2v2.629 (2)O1—O1xiv3.045 (3)
La—O2vi2.629 (2)O1—O23.225 (3)
La—O2vii2.601 (2)O1—O2xii3.225 (3)
La—O2viii2.601 (2)O1—O2xv3.338 (3)
La—B3.331 (4)O1—O2xvi3.338 (3)
La—Bii3.508 (3)O1—O2v2.383 (3)
La—Bv3.007 (4)O1—O2vi2.383 (3)
La—Biii3.508 (3)O1—O2xvii3.705 (3)
La—Bix3.034 (2)O1—O2xviii3.705 (3)
La—Bvii3.034 (2)O1—O2xix3.097 (3)
B—O1x1.374 (5)O1—O2xx3.097 (3)
B—O13.247 (5)O2—O2xii2.368 (4)
B—O1xi3.400 (5)O2—O2x3.176 (2)
B—O21.373 (3)O2—O2vi3.176 (2)
B—O2xii1.373 (3)O2—O2xxi2.740 (4)
B—O2v3.186 (5)O2—O2xx3.098 (4)
B—O2vi3.186 (5)
O1i—La—O1ii71.88 (6)Lav—O1—Laxvii108.12 (6)
O1i—La—O1iii71.88 (6)Lav—O1—Laxxii108.12 (6)
O1i—La—O2ii145.20 (5)Lav—O1—O2v115.9 (1)
O1i—La—O2iv145.20 (5)Lav—O1—O2vi115.9 (1)
O1i—La—O2v82.06 (8)Lav—O1—Bv118.4 (2)
O1i—La—O2vi82.06 (8)Laxvii—O1—Laxxii139.4 (1)
O1i—La—O2vii94.31 (7)Laxvii—O1—O2v116.4 (1)
O1i—La—O2viii94.31 (7)Laxvii—O1—O2vi60.81 (5)
O1ii—La—O1iii139.4 (1)Laxvii—O1—Bv89.23 (10)
O1ii—La—O2ii76.28 (7)Laxxii—O1—O2v60.81 (5)
O1ii—La—O2iv142.61 (7)Laxxii—O1—O2vi116.4 (1)
O1ii—La—O2v120.96 (7)Laxxii—O1—Bv89.23 (10)
O1ii—La—O2vi70.69 (7)O2v—O1—O2vi59.6 (1)
O1ii—La—O2vii112.84 (7)Lai—O2—Laxvii105.58 (7)
O1ii—La—O2viii53.11 (7)Lai—O2—Laix136.43 (9)
O1iii—La—O2ii142.61 (7)Lai—O2—O1i118.62 (9)
O1iii—La—O2iv76.28 (7)Lai—O2—O2xii63.23 (4)
O1iii—La—O2v70.69 (7)Lai—O2—O2xxi116.77 (4)
O1iii—La—O2vi120.96 (7)Lai—O2—B91.9 (2)
O1iii—La—O2vii53.11 (7)Laxvii—O2—Laix103.98 (7)
O1iii—La—O2viii112.84 (7)Laxvii—O2—O1i124.0 (1)
O2ii—La—O2iv66.73 (9)Laxvii—O2—O2xii123.37 (5)
O2ii—La—O2v103.11 (4)Laxvii—O2—O2xxi56.63 (5)
O2ii—La—O2vi74.42 (7)Laxvii—O2—B128.0 (2)
O2ii—La—O2vii110.91 (5)Laix—O2—O1i66.08 (6)
O2ii—La—O2viii77.14 (5)Laix—O2—O2xii121.79 (4)
O2iv—La—O2v74.42 (7)Laix—O2—O2xxi58.21 (4)
O2iv—La—O2vi103.11 (4)Laix—O2—B94.4 (2)
O2iv—La—O2vii77.14 (5)O1i—O2—O2xii60.20 (6)
O2iv—La—O2viii110.91 (5)O1i—O2—O2xxi119.80 (6)
O2v—La—O2vi53.55 (9)O2xii—O2—O2xxi180.0
O2v—La—O2vii121.32 (2)O2xxi—O2—B149.6 (2)
O2v—La—O2viii173.98 (8)O1i—B—O2120.3 (2)
O2vi—La—O2vii173.98 (8)O1i—B—O2xii120.3 (2)
O2vi—La—O2viii121.32 (2)O2—B—O2xii119.1 (3)
O2vii—La—O2viii63.59 (9)
Symmetry codes: (i) x+1/2, y+1/2, z+1/2; (ii) x+1/2, y, z+1/2; (iii) x+1/2, y+1, z+1/2; (iv) x+1/2, y+1/2, z+1/2; (v) x1/2, y+1/2, z+1/2; (vi) x1/2, y, z+1/2; (vii) x+1, y+1/2, z+1; (viii) x+1, y, z+1; (ix) x+1, y1/2, z+1; (x) x+1/2, y, z+1/2; (xi) x+1, y, z; (xii) x, y+1/2, z; (xiii) x, y+1/2, z; (xiv) x, y1/2, z; (xv) x1, y, z; (xvi) x1, y+1/2, z; (xvii) x+1/2, y, z1/2; (xviii) x+1/2, y+1/2, z1/2; (xix) x+1, y+1/2, z; (xx) x+1, y, z; (xxi) x, y1/2, z; (xxii) x+1/2, y+1, z1/2.
 

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