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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Nov 23;67(Pt 12):i74. doi: 10.1107/S1600536811048227

The matlockite-type praseodymium(III) oxide bromide PrOBr

Pia Talmon-Gros a, Christian M Schurz a, Thomas Schleid a,*
PMCID: PMC3238581  PMID: 22199472

Abstract

The crystal structure of the praseodymium(III) oxide bromide, PrOBr, can be best described with layers of agglomerated square anti­prisms [PrO4Br4]9−. These slabs are stacked along the c axis and linked via two different secondary contacts between Pr3+ and Br. The Pr3+ cations occupy the Wyckoff site 2c with 4mm symmetry and carry four O2− anions as well as four primary Br anions, yielding a coordination number of 8. While the Br anions exhibit the same site symmetry as the Pr3+ cations, the oxide anions are located at the Wyckoff position 2a with site symmetry Inline graphic m2 and have four Pr3+ cations as neighbours, defining a tetra­hedron.

Related literature

For prototypic PbFCl (mineral name: matlockite), see: Nieuwenkamp & Bijvoet (1932) and for an early powder study, see: Mayer et al. (1965). For other PrOX structures, see: Baenziger et al. (1950) for X = F, Zachariasen (1949) for X = Cl, and Potapova et al. (1977) for X = I. For data used for a comparison of the unit-cell dimensions, see: Shannon (1976) for ionic radii and Biltz (1934) for volume increments. For a proper classification of primary and secondary contacts, see: MAPLE (Hoppe, 1975) and for the bond-valence method, see: Brown (2002). For a comparison of intended synthesis attempts, see: Mattausch & Simon (1996); Lulei (1998).

Experimental

Crystal data

  • PrOBr

  • M r = 236.82

  • Tetragonal, Inline graphic

  • a = 4.0671 (3) Å

  • c = 7.4669 (5) Å

  • V = 123.51 (2) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 35.52 mm−1

  • T = 293 K

  • 0.11 × 0.07 × 0.02 mm

Data collection

  • Bruker–Nonius KappaCCD diffractometer

  • Absorption correction: numerical (X-SHAPE; Stoe & Cie, 1999) T min = 0.049, T max = 0.535

  • 1621 measured reflections

  • 113 independent reflections

  • 111 reflections with I > 2σ(I)

  • R int = 0.082

Refinement

  • R[F 2 > 2σ(F 2)] = 0.026

  • wR(F 2) = 0.059

  • S = 1.20

  • 113 reflections

  • 10 parameters

  • Δρmax = 1.14 e Å−3

  • Δρmin = −2.52 e Å−3

Data collection: COLLECT (Nonius, 1998); cell refinement: SCALEPACK (Otwinowski & Minor, 1997); data reduction: SCALEPACK and DENZO (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811048227/fi2117sup1.cif

e-67-00i74-sup1.cif (13.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811048227/fi2117Isup2.hkl

e-67-00i74-Isup2.hkl (6.5KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Selected bond lengths (Å).

Pr—O 4Inline graphic 2.3496 (3)
Pr—Br 4Inline graphic 3.2457 (8)
Pr—Br 3.6083 (14)
Pr—Br 3.8586 (14)

Acknowledgments

This work was supported by the State of Baden-Württemberg (Stuttgart) and the German Research Foundation (DFG, Bonn) within the funding programme Open Access Publishing. We thank Dr Sabine Strobel for the data collection.

supplementary crystallographic information

Comment

With the exception of PrOF (Baenziger et al. 1950) all praseodymium(III) oxide halides of the general composition PrOX (X = Cl – I; Zachariasen 1949, Potapova et al. 1977) crystallize with the matlockite-type structure (Nieuwenkamp & Bijvoet, 1932). The tetragonal crystal structure of the here presented praseodymium(III) oxide bromide PrOBr can be best described with layers of agglomerated square antiprisms [PrO4Br4]9– (d(Pr3+–O2-) = 234.96 (4) pm, d(Pr3+–Br-) = 324.57 (8) pm, d(Pr3+···Br-) = 360.8 (1) and 385.9 (1) pm; Figure 1). These slabs are stacked along the c-axis and linked via two different secondary contacts between Pr3+ and Br- (Figure 2). According to the ionic radii (rCl = 180 pm, rBr = 195 pm, rI = 220 pm; Shannon, 1976) of the halide anions involved the expansion of the unit-cell dimensions occurs in quite an usual range, but the c-axes become significantly longer than the a-axes (a-axes: from 405.3 pm to 408.6 pm; c-axes: from 679.9 pm to 916.2 pm) along the Cl-–Br-–I- track. The lattice parameters of single crystalline PrOBr (a = 406.71 pm, c = 746.69 pm) fit almost perfectly with that from a previous powder diffraction study (a = 407.1 pm, c = 748.7 pm; Mayer et al. 1965). Differences in the molar volumes of the PbFCl-type praseodymium(III) oxide halides (Vm(PrOCl) = 33.6 cm3/mol, Vm(PrOBr) = 37.2 cm3/mol, Vm(PrOI) = 46.1 cm3/mol) correspond well with the differences of the molar volumes of the respective halide anions (Vm(Cl-) = 16.3 cm3/mol, Vm(Br-) = 19.2 cm3/mol, Vm(I-) = 24.5 cm3/mol; Biltz 1934). However, the Pr3+ cations occupy the Wyckoff site 2c (symmetry: 4mm) and bond four O2- anions as well as four+one+one Br- anions ending up with a total coordination number of 8+1+1 (Figure 1). While the Br- anions exhibit the same site symmetry as the Pr3+ cations, the oxide anions are located at Wyckoff position 2a with the site symmetry 4m2. Bond-Valence and MAPLE calculations support the interpretation of one important (d(Pr3+···Br-) = 360.8 (1) pm) and one less important secondary contact (d(Pr3+···Br-) = 385.9 (1) pm): The valency and ECoN for the first bond amounts to values of about 0.08 (with R0 = 267 pm, b = 37 pm; Brown, 2002) and 0.12 (Hoppe, 1975), but almost nil for the second one, since this next nearest contact to bromide has only very low influence on the effective coordination sphere of the Pr3+ cations (ECoN = 0.03).

Experimental

Pale green, transparent, plate-shaped single crystals of PrOBr were obtained as by-product from a mixture of 0.06 g Pr, 0.38 g PrBr3 and 0.01 g NaN3, along with 0.30 g NaBr added as a flux. The mixture was kept at 800 °C for 7 days in an evacuated, sealed fused-silica vessel designed to produce the praseodymium(III) nitride bromide Pr3NBr6 in analogy with La3NBr6 (Lulei, 1998) and Ce3NBr6 (Mattausch & Simon, 1996).

Refinement

The highest peak and the deepest hole in the final difference Fourier map are 95 pm and 84 pm apart from Pr.

Figures

Fig. 1.

Fig. 1.

View at the square antiprism [PrO4Br4]9– with two different Br- caps in matlockite-type PrOBr. Displacement ellipsoids are drawn at 90 % probability level. Symmetry codes: (i) -x+1, -y, -z; (ii) x-1, y, z; (iii) -x+1, -y+1, -z; (iv) -x+1, -y+1, -z+1; (v) -x, -y, -z+1; (vi) -x, -y+1, -z+1; (vii) -x+1, -y, -z+1; (viii) x, y, z-1.

Fig. 2.

Fig. 2.

Polyhedral representation of the matlockite-type PrOBr structure (dotted lines indicate the first of the two kinds of secondary contacts between Pr3+ and Br-).

Crystal data

PrBrO Dx = 6.368 Mg m3
Mr = 236.82 Mo Kα radiation, λ = 0.71069 Å
Tetragonal, P4/nmm Cell parameters from 3957 reflections
Hall symbol: -P 4a 2a θ = 0.4–27.9°
a = 4.0671 (3) Å µ = 35.52 mm1
c = 7.4669 (5) Å T = 293 K
V = 123.51 (2) Å3 Plate, pale green
Z = 2 0.11 × 0.07 × 0.02 mm
F(000) = 204

Data collection

Bruker–Nonius KappaCCD diffractometer 113 independent reflections
Radiation source: fine-focus sealed tube 111 reflections with I > 2σ(I)
graphite Rint = 0.082
ω and φ scans θmax = 27.9°, θmin = 5.5°
Absorption correction: numerical (X-SHAPE; Stoe & Cie, 1999) h = −5→5
Tmin = 0.049, Tmax = 0.535 k = −5→5
1621 measured reflections l = −9→9

Refinement

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)] = 0.026 w = 1/[σ2(Fo2) + (0.0378P)2] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.059 (Δ/σ)max < 0.001
S = 1.20 Δρmax = 1.14 e Å3
113 reflections Δρmin = −2.52 e Å3
10 parameters Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraints Extinction coefficient: 0.032 (5)

Special details

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 > 2sigma(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)

x y z Uiso*/Ueq
Pr 0.2500 0.2500 0.15763 (8) 0.0106 (4)
O 0.7500 0.2500 0.0000 0.0129 (13)
Br 0.2500 0.2500 0.64087 (17) 0.0153 (4)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Pr 0.0084 (4) 0.0084 (4) 0.0148 (6) 0.000 0.000 0.000
O 0.0114 (17) 0.0114 (17) 0.016 (3) 0.000 0.000 0.000
Br 0.0149 (5) 0.0149 (5) 0.0160 (7) 0.000 0.000 0.000

Geometric parameters (Å, °)

Pr—Oi 2.3496 (3) Pr—Pri 3.7165 (8)
Pr—Oii 2.3496 (3) Pr—Prx 3.7165 (8)
Pr—Oiii 2.3496 (3) Pr—Priii 3.7165 (8)
Pr—O 2.3496 (3) O—Pri 2.3496 (3)
Pr—Briv 3.2457 (8) O—Prxi 2.3496 (3)
Pr—Brv 3.2457 (8) O—Priii 2.3496 (3)
Pr—Brvi 3.2457 (8) Br—Priv 3.2457 (8)
Pr—Brvii 3.2457 (8) Br—Prv 3.2457 (8)
Pr—Br 3.6083 (14) Br—Prvii 3.2457 (8)
Pr—Brviii 3.8586 (14) Br—Prvi 3.2457 (8)
Pr—Prix 3.7165 (8)
Oi—Pr—Oii 75.466 (11) O—Pr—Pri 37.733 (6)
Oi—Pr—Oiii 119.87 (3) Briv—Pr—Pri 107.075 (12)
Oii—Pr—Oiii 75.466 (11) Brv—Pr—Pri 107.075 (12)
Oi—Pr—O 75.466 (11) Brvi—Pr—Pri 168.31 (4)
Oii—Pr—O 119.87 (3) Brvii—Pr—Pri 66.920 (18)
Oiii—Pr—O 75.466 (11) Prix—Pr—Pri 66.346 (15)
Oi—Pr—Briv 140.758 (5) Oi—Pr—Prx 98.99 (2)
Oii—Pr—Briv 140.758 (5) Oii—Pr—Prx 37.733 (6)
Oiii—Pr—Briv 71.938 (15) Oiii—Pr—Prx 37.733 (6)
O—Pr—Briv 71.938 (15) O—Pr—Prx 98.99 (2)
Oi—Pr—Brv 71.938 (15) Briv—Pr—Prx 107.075 (12)
Oii—Pr—Brv 71.938 (15) Brv—Pr—Prx 107.075 (12)
Oiii—Pr—Brv 140.758 (5) Brvi—Pr—Prx 66.920 (18)
O—Pr—Brv 140.758 (5) Brvii—Pr—Prx 168.31 (4)
Briv—Pr—Brv 124.77 (5) Prix—Pr—Prx 66.346 (15)
Oi—Pr—Brvi 140.758 (5) Pri—Pr—Prx 101.39 (3)
Oii—Pr—Brvi 71.938 (15) Oi—Pr—Priii 98.99 (2)
Oiii—Pr—Brvi 71.938 (15) Oii—Pr—Priii 98.99 (2)
O—Pr—Brvi 140.758 (5) Oiii—Pr—Priii 37.733 (6)
Briv—Pr—Brvi 77.59 (2) O—Pr—Priii 37.733 (6)
Brv—Pr—Brvi 77.59 (2) Briv—Pr—Priii 66.920 (19)
Oi—Pr—Brvii 71.938 (15) Brv—Pr—Priii 168.31 (4)
Oii—Pr—Brvii 140.758 (5) Brvi—Pr—Priii 107.075 (12)
Oiii—Pr—Brvii 140.758 (6) Brvii—Pr—Priii 107.075 (12)
O—Pr—Brvii 71.938 (15) Prix—Pr—Priii 101.39 (3)
Briv—Pr—Brvii 77.59 (2) Pri—Pr—Priii 66.346 (15)
Brv—Pr—Brvii 77.59 (2) Prx—Pr—Priii 66.346 (15)
Brvi—Pr—Brvii 124.77 (5) Pr—O—Pri 104.534 (11)
Oi—Pr—Prix 37.733 (6) Pr—O—Prxi 119.87 (3)
Oii—Pr—Prix 37.733 (6) Pri—O—Prxi 104.534 (11)
Oiii—Pr—Prix 98.99 (2) Pr—O—Priii 104.534 (11)
O—Pr—Prix 98.99 (2) Pri—O—Priii 119.87 (3)
Briv—Pr—Prix 168.31 (4) Prxi—O—Priii 104.534 (11)
Brv—Pr—Prix 66.920 (19) Priv—Br—Prv 124.77 (5)
Brvi—Pr—Prix 107.075 (12) Priv—Br—Prvii 77.59 (2)
Brvii—Pr—Prix 107.075 (12) Prv—Br—Prvii 77.59 (2)
Oi—Pr—Pri 37.733 (6) Priv—Br—Prvi 77.59 (2)
Oii—Pr—Pri 98.99 (2) Prv—Br—Prvi 77.59 (2)
Oiii—Pr—Pri 98.99 (2) Prvii—Br—Prvi 124.77 (5)

Symmetry codes: (i) −x+1, −y, −z; (ii) x−1, y, z; (iii) −x+1, −y+1, −z; (iv) −x+1, −y+1, −z+1; (v) −x, −y, −z+1; (vi) −x, −y+1, −z+1; (vii) −x+1, −y, −z+1; (viii) x, y, z−1; (ix) −x, −y, −z; (x) −x, −y+1, −z; (xi) x+1, y, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FI2117).

References

  1. Baenziger, N. C., Holden, J. R., Knudson, G. E. & Popov, A. I. (1950). Atti Accad. Lig. Sci. Lett. Genoa, 7, 44–52.
  2. Biltz, W. (1934). Raumchemie fester Stoffe Leipzig: Verlag von Leopold Voss.
  3. Brandenburg, K. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
  4. Brown, I. D. (2002). The Bond Valence Model Oxford University Press.
  5. Hoppe, R. (1975). Crystal Structure and Chemical Bonding in Inorganic Chemistry, edited by C. J. M. Rooymans & A. Rabenau. Amsterdam: North-Holland Publishing Company.
  6. Lulei, M. (1998). Inorg. Chem. 37, 777–781.
  7. Mattausch, Hj. & Simon, A. (1996). Z. Kristallogr. New. Cryst. Struct. 211, 397.
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  9. Nieuwenkamp, W. & Bijvoet, J. M. (1932). Z. Kristallogr. 81, 469–473.
  10. Nonius (1998). COLLECT Nonius BV, Delft, The Netherlands.
  11. Otwinowski, Z. & Minor, W. (1997). Methods in Enzymology, Vol. 276, Macromolecular Crystallography, Part A, edited by C. W. Carter Jr & R. M. Sweet, pp. 307–326. New York: Academic Press, USA.
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  13. Shannon, R. D. (1976). Acta Cryst. A32, 751–767.
  14. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  15. Stoe & Cie (1999). X-SHAPE Stoe & Cie, Darmstadt, Germany.
  16. Zachariasen, W. H. (1949). Acta Cryst. 2, 388–390.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811048227/fi2117sup1.cif

e-67-00i74-sup1.cif (13.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811048227/fi2117Isup2.hkl

e-67-00i74-Isup2.hkl (6.5KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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