inorganic compounds
Dilead(II) oxyhydroxide bromide
aDepartment of Physics, Shizuoka University, Shizuoka 422-8529, Japan, and bInstitute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba, 277-8581, Japan
*Correspondence e-mail: [email protected]
The of the title compound, Pb2O(OH)Br, has been determined by single-crystal X-ray diffraction. The compound crystallizes in the tetragonal space group P42/mcm. The structure consists of [PbO4Br4] square antiprisms, which form square layers in the ab plane and are stacked alternately along the c-axis direction. The hydroxide site is assigned on the basis of bond-valence-sum calculations.
Keywords: crystal structure; Pb(II); oxyhydroxide; bromide; square antiprismatic coordination.
CCDC reference: 2578647
Structure description
Lead oxyhalides comprise a diverse family of compounds with a variety of crystal structures. Among them, Pb2O(OH)Cl (Turner et al., 2015
), Pb2O(OH)I (Siidra et al., 2013
), and Pb3O2(OH)Br (Krivovichev & Burns, 2001
) are oxide–hydroxide halides related to the title compound. In this work, we report the crystal structure of Pb2O(OH)Br determined by single-crystal X-ray diffraction.
The title compound crystallizes in the tetragonal space group P42/mcm. We note that the crystal structure of Pb2O(OH)Br is different from the ones of Pb2O(OH)Cl (space group Pnma) and Pb2O(OH)I (space group C2/m). The asymmetric unit contains one Pb site, three O sites (O1, O2 and O3), and one Br site. The divalent Pb cation is coordinated in a square-antiprismatic mode by four O and four Br atoms (Fig. 1
and Table 1
). The O4 and Br4 squares are parallel, rotated by 45° relative to each other, with the Br4 square having an edge length approximately √2 times that of the O4 square. The face-sharing square antiprisms form square layers in the ab plane (Fig. 2
). These layers with opposite orientations are alternately stacked along the c axis. Consequently, a Br square layer and an O square layer are formed alternately along the c axis with 45° relative rotation. The Br atom is surrounded by eight Pb cations in a distorted cubic arrangement, while each of the O atoms is surrounded by four Pb cations in a distorted tetrahedral mode (Fig. 3
).
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| | Figure 1 (a) Coordination environment of the Pb atom. Displacement ellipsoids are drawn at the 50% probability level; (b) the [PbBr4O4] coordination polyhedron viewed along the c axis. [Symmetry codes: (i) x, y − 1, z; (ii) −x + 1, −y + 1, −z; (iii) −x, −y + 1, −z; (iv) y, −x, −z + |
| Figure 2 The crystal structure of Pb2O(OH)Br with polyhedral representation. (a) Perspective view, projections along (b) the a and (c) the c axes. |
| | Figure 3 Coordination environments of the (a) Br and (b) O atoms. Ellipsoids are drawn at the 50% probability level. [Symmetry codes: (ii) −x + 1, −y + 1, −z; (iii) −x, −y + 1, −z; (iv) y, −x, −z + |
Charge neutrality requires the presence of one H atom per formula unit, although the H atom could not be located from difference Fourier maps owing to the presence of the heavy Pb atom. Bond-valence-sum (BVS) calculations (Brown, 2002
; Brese & O'Keeffe, 1991
) were therefore carried out to identify the hydroxide site (Table 2
). Consistent with the longest Pb—O3 bond length, O3 exhibits the lowest BVS value, supporting its assignment as the hydroxide site. We note that the O2 site cannot be assigned as the hydroxide site because its multiplicity is twice that of the O1 and O3 sites. The off-centered coordination around the Pb2+ cation reflects the stereochemical activity of its 6s2 electron lone pair.
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Synthesis and crystallization
Single crystals of Pb2O(OH)Br were obtained serendipitously during attempts to synthesize the Br analogues of diaboleite, Pb2CuCl2(OH)4, and cumengeite, Pb21Cu20Cl42(OH)40·6H2O, (Alun Humphreys et al., 1980
) under hydrothermal conditions. Pb wire (0.6 g, Nilaco), CuBr2 (0.2 g, FUJIFILM Wako), and 5 wt% aqueous ammonia (8 ml) were placed in a polymer-lined stainless-steel autoclave and heated at 533 K for 24 h. Yellow, plate-like crystals grew on the surface of the Pb wire, and a suitable crystal was selected for the single-crystal X-ray diffraction measurements.
Refinement
Details of data collection and structure are given in Table 3
. The largest residual electron-density peaks are located within 0.9 Å of the Pb atom and are attributed to Fourier termination errors associated with the heavy Pb atom.
|
Structural data
CCDC reference: 2578647
contains datablock I. DOI: https://doi.org/10.1107/S241431462600790X/wm4254sup1.cif
Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S241431462600790X/wm4254Isup2.hkl
| Pb2O(OH)Br | Dx = 8.019 Mg m−3 |
| Mr = 526.29 | Mo Kα radiation, λ = 0.71073 Å |
| Tetragonal, P42/mcm | Cell parameters from 2463 reflections |
| a = 5.8161 (3) Å | θ = 3.1–34.3° |
| c = 12.8870 (13) Å | µ = 86.13 mm−1 |
| V = 435.93 (6) Å3 | T = 296 K |
| Z = 4 | Plate, yellow |
| F(000) = 860 | 0.10 × 0.08 × 0.01 mm |
| XtaLAB AFC11 (RCD3): quarter-chi single diffractometer | 705 independent reflections |
| Radiation source: Rotating-anode X-ray tube, Rigaku (Mo) X-ray Source | 460 reflections with I > 2σ(I) |
| Mirror monochromator | Rint = 0.062 |
| Detector resolution: 10.0000 pixels mm-1 | θmax = 38.8°, θmin = 3.2° |
| ω scans | h = −8→10 |
| Absorption correction: multi-scan (CrysAlisPro; Rigaku OD, 2023) | k = −10→10 |
| Tmin = 0.542, Tmax = 1.000 | l = −22→18 |
| 9139 measured reflections |
| Refinement on F2 | 0 restraints |
| Least-squares matrix: full | Primary atom site location: dual |
| R[F2 > 2σ(F2)] = 0.044 | H-atom parameters not defined |
| wR(F2) = 0.131 | w = 1/[σ2(Fo2) + (0.0369P)2 + 26.4764P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.12 | (Δ/σ)max < 0.001 |
| 705 reflections | Δρmax = 6.55 e Å−3 |
| 18 parameters | Δρmin = −4.22 e Å−3 |
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. |
| x | y | z | Uiso*/Ueq | ||
| Pb | 0.26668 (8) | 0.26668 (8) | 0.15022 (4) | 0.01991 (19) | |
| Br | 0.2582 (3) | 0.7418 (3) | 0.000000 | 0.0233 (4) | |
| O1 | 0.500000 | 0.500000 | 0.250000 | 0.018 (7) | |
| O2 | 0.000000 | 0.500000 | 0.250000 | 0.023 (8) | |
| O3H | 0.000000 | 0.000000 | 0.250000 | 0.020 (7) |
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Pb | 0.0215 (2) | 0.0215 (2) | 0.0168 (3) | −0.0095 (3) | −0.00071 (12) | −0.00071 (12) |
| Br | 0.0204 (6) | 0.0204 (6) | 0.0290 (11) | 0.0022 (15) | 0.000 | 0.000 |
| O1 | 0.020 (10) | 0.020 (10) | 0.015 (16) | 0.000 | 0.000 | 0.000 |
| O2 | 0.016 (10) | 0.024 (12) | 0.03 (2) | 0.000 | 0.000 | 0.000 |
| O3H | 0.022 (11) | 0.022 (11) | 0.017 (17) | 0.000 | 0.000 | 0.000 |
| Pb—Bri | 3.3741 (15) | Pb—O1 | 2.3101 (6) |
| Pb—Br | 3.3741 (15) | Pb—O2iv | 2.4291 (3) |
| Pb—Brii | 3.6154 (15) | Pb—O2 | 2.4291 (3) |
| Pb—Briii | 3.6154 (15) | Pb—O3H | 2.5426 (6) |
| Br—Pb—Bri | 72.22 (6) | Pb—O1—Pbix | 58.337 (6) |
| Briii—Pb—Brii | 71.96 (6) | Pbxiv—O1—Pbxvii | 94.056 (3) |
| Br—Pb—Briii | 72.039 (8) | Pbxv—O1—Pbviii | 94.056 (4) |
| Bri—Pb—Brii | 72.039 (8) | Pb—O2—Pbxi | 100.64 (3) |
| Br—Pb—Brii | 112.590 (16) | Pbxviii—O2—Pbxix | 51.065 (2) |
| Bri—Pb—Briii | 112.590 (16) | Pbxviii—O2—Pbxx | 92.740 (7) |
| O1—Pb—Br | 81.191 (16) | Pbviii—O2—Pbiv | 143.039 (7) |
| O1—Pb—Bri | 81.191 (16) | Pbxvi—O2—Pbviii | 92.740 (7) |
| O1—Pb—Brii | 143.33 (3) | Pbix—O2—Pbxx | 55.085 (16) |
| O1—Pb—Briii | 143.33 (3) | Pbxv—O2—Pbiv | 63.525 (18) |
| O1—Pb—O2 | 75.655 (14) | Pb—O2—Pbxv | 112.08 (3) |
| O1—Pb—O2iv | 75.655 (14) | Pbxi—O2—Pbviii | 55.085 (16) |
| O1—Pb—O3H | 115.80 (2) | Pbxviii—O2—Pbviii | 118.901 (6) |
| O2—Pb—Briii | 75.63 (3) | Pb—O2—Pbxx | 148.277 (12) |
| O2iv—Pb—Brii | 75.63 (3) | Pbxi—O2—Pbxv | 116.07 (2) |
| O2iv—Pb—Br | 146.59 (3) | Pbxix—O2—Pbxx | 143.039 (7) |
| O2—Pb—Bri | 146.59 (3) | Pbxi—O2—Pbiv | 99.647 (17) |
| O2—Pb—Brii | 138.29 (3) | Pbv—O2—Pbiv | 92.740 (7) |
| O2iv—Pb—Briii | 138.29 (3) | Pb—O2—Pbix | 116.07 (2) |
| O2—Pb—Br | 80.62 (3) | Pbxxi—O2—Pbxix | 92.740 (7) |
| O2iv—Pb—Bri | 80.62 (3) | Pb—O2—Pbviii | 99.647 (17) |
| O2iv—Pb—O2 | 115.67 (2) | Pbix—O2—Pbviii | 63.525 (19) |
| O2—Pb—O3H | 71.552 (14) | Pbxi—O2—Pbix | 112.08 (3) |
| O2iv—Pb—O3H | 71.552 (14) | Pbxxi—O2—Pbviii | 95.585 (7) |
| O3H—Pb—Brii | 75.368 (15) | Pbxix—O2—Pbviii | 149.527 (14) |
| O3H—Pb—Briii | 75.368 (15) | Pbxv—O2—Pbxx | 99.647 (17) |
| O3H—Pb—Br | 141.34 (3) | Pbxv—O2—Pbix | 100.64 (3) |
| O3H—Pb—Bri | 141.34 (3) | Pbv—O2—Pbxx | 95.585 (8) |
| Pbv—Br—Pbvi | 124.37 (4) | Pbxxi—O2—Pbxx | 51.065 (2) |
| Pbi—Br—Pbvii | 72.180 (8) | Pb—O2—Pbiv | 55.085 (16) |
| Pbviii—Br—Pbix | 74.70 (4) | Pb—O2—Pbxviii | 106.011 (17) |
| Pb—Br—Pbvi | 124.37 (4) | Pbxviii—O2—Pbiv | 95.585 (7) |
| Pbx—Br—Pbix | 107.961 (8) | Pbxvi—O2—Pbiv | 51.065 (2) |
| Pbiii—Br—Pbvi | 58.241 (14) | Pbxix—O2—Pbiv | 48.630 (9) |
| Pbx—Br—Pbvii | 112.591 (17) | Pbxi—O2—Pbxviii | 153.350 (11) |
| Pbix—Br—Pbvi | 122.98 (3) | Pbxi—O2—Pbv | 53.030 (17) |
| Pb—Br—Pbviii | 112.590 (16) | Pbv—O2—Pbxix | 118.901 (6) |
| Pbv—Br—Pbxi | 54.357 (14) | Pbxv—O2—Pbv | 153.350 (11) |
| Pbi—Br—Pbix | 176.910 (14) | Pbxv—O2—Pbxviii | 53.030 (17) |
| Pb—Br—Pbxi | 54.357 (14) | Pbix—O2—Pbv | 106.011 (17) |
| Pbviii—Br—Pbiii | 108.04 (6) | Pbxv—O2—Pbviii | 148.277 (12) |
| Pbx—Br—Pbviii | 176.910 (15) | Pbxviii—O2—Pbv | 147.940 (14) |
| Pb—Br—Pbvii | 176.910 (15) | Pbix—O2—Pbxviii | 55.377 (19) |
| Pbv—Br—Pbviii | 72.179 (8) | Pbxvi—O2—Pbv | 47.339 (10) |
| Pbi—Br—Pbviii | 107.961 (8) | Pbv—O2—Pbviii | 51.065 (2) |
| Pbiii—Br—Pbvii | 74.70 (4) | Pb—O2—Pbxxi | 153.350 (11) |
| Pbix—Br—Pbxi | 58.241 (14) | Pb—O2—Pbxvi | 53.029 (17) |
| Pbx—Br—Pbxi | 124.37 (4) | Pbxi—O2—Pbxxi | 106.011 (17) |
| Pbvii—Br—Pbix | 108.04 (6) | Pbxi—O2—Pbxx | 63.525 (19) |
| Pbv—Br—Pbiii | 176.910 (15) | Pbxv—O2—Pbxxi | 55.377 (19) |
| Pbx—Br—Pbvi | 54.357 (14) | Pbxi—O2—Pbxvi | 55.377 (19) |
| Pbi—Br—Pbxi | 124.37 (4) | Pbix—O2—Pbxxi | 53.030 (17) |
| Pbi—Br—Pbvi | 54.357 (14) | Pbxvi—O2—Pbxx | 118.901 (6) |
| Pb—Br—Pbiii | 107.961 (8) | Pbxviii—O2—Pbxxi | 47.339 (9) |
| Pbviii—Br—Pbvi | 122.98 (3) | Pbxv—O2—Pbxvi | 106.011 (17) |
| Pbiii—Br—Pbxi | 122.98 (3) | Pbxvi—O2—Pbxxi | 147.940 (14) |
| Pbx—Br—Pbv | 107.78 (6) | Pbviii—O2—Pbxx | 48.630 (8) |
| Pbv—Br—Pbix | 112.591 (17) | Pbv—O2—Pbxxi | 146.116 (7) |
| Pbx—Br—Pbi | 69.33 (4) | Pbix—O2—Pbxvi | 153.350 (11) |
| Pbv—Br—Pbvii | 107.961 (8) | Pb—O2—Pbxix | 63.525 (19) |
| Pbv—Br—Pbi | 70.02 (4) | Pbix—O2—Pbiv | 148.277 (12) |
| Pbi—Br—Pbiii | 112.591 (17) | Pbxi—O2—Pbxix | 148.277 (12) |
| Pbx—Br—Pb | 70.02 (4) | Pbxviii—O2—Pbxvi | 146.116 (7) |
| Pb—Br—Pbix | 72.179 (8) | Pbxv—O2—Pbxix | 55.085 (16) |
| Pbv—Br—Pb | 69.33 (4) | Pbxxi—O2—Pbiv | 118.901 (6) |
| Pbx—Br—Pbiii | 72.180 (8) | Pbix—O2—Pbxix | 99.647 (17) |
| Pbi—Br—Pb | 107.78 (6) | Pb—O2—Pbv | 55.377 (19) |
| Pbviii—Br—Pbvii | 64.75 (3) | Pbxvi—O2—Pbxix | 95.585 (7) |
| Pbvi—Br—Pbxi | 178.24 (6) | Pbxx—O2—Pbiv | 149.527 (14) |
| Pbiii—Br—Pbix | 64.75 (3) | Pb—O3H—Pbxix | 119.24 (3) |
| Pbviii—Br—Pbxi | 58.241 (14) | Pbix—O3H—Pbxvii | 121.353 (13) |
| Pbvii—Br—Pbvi | 58.241 (14) | Pbxvi—O3H—Pbix | 94.262 (4) |
| Pbvii—Br—Pbxi | 122.98 (3) | Pbxviii—O3H—Pbxvii | 148.360 (14) |
| Pb—O1—Pbv | 112.35 (3) | Pbxi—O3H—Pbxviii | 94.262 (4) |
| Pbiv—O1—Pbviii | 147.401 (13) | Pbiv—O3H—Pbix | 152.875 (9) |
| Pbxii—O1—Pbxiii | 94.056 (4) | Pbxv—O3H—Pbxvii | 152.875 (9) |
| Pbxiii—O1—Pbviii | 116.547 (13) | Pb—O3H—Pbxv | 104.820 (12) |
| Pbxiv—O1—Pbxv | 149.152 (13) | Pbxix—O3H—Pbxviii | 60.734 (7) |
| Pbxi—O1—Pbxiii | 148.721 (10) | Pbxvi—O3H—Pbxviii | 141.606 (14) |
| Pbxvi—O1—Pbviii | 148.721 (10) | Pb—O3H—Pbix | 60.734 (7) |
| Pb—O1—Pbxvi | 108.051 (15) | Pbxix—O3H—Pbxv | 104.820 (12) |
| Pbv—O1—Pbxv | 148.721 (10) | Pbii—O3H—Pbix | 148.360 (14) |
| Pbxii—O1—Pbxv | 116.547 (13) | Pbxix—O3H—Pbxvii | 102.305 (10) |
| Pb—O1—Pbxiii | 103.228 (10) | Pbxxii—O3H—Pbxvii | 94.262 (4) |
| Pbv—O1—Pbxvi | 108.051 (15) | Pb—O3H—Pbiv | 104.820 (12) |
| Pbxvii—O1—Pbxiii | 53.957 (13) | Pbxxiii—O3H—Pbii | 94.262 (4) |
| Pbv—O1—Pbviii | 58.337 (6) | Pb—O3H—Pbxviii | 102.305 (10) |
| Pbix—O1—Pbviii | 53.957 (13) | Pbiv—O3H—Pbxviii | 152.875 (9) |
| Pb—O1—Pbxi | 108.051 (15) | Pbxix—O3H—Pbiv | 104.820 (12) |
| Pbiv—O1—Pbxvii | 45.493 (14) | Pbxxiii—O3H—Pbxviii | 50.571 (15) |
| Pb—O1—Pbxv | 56.043 (19) | Pbii—O3H—Pbxviii | 121.353 (13) |
| Pbxi—O1—Pbxv | 58.337 (6) | Pbxv—O3H—Pbix | 52.101 (18) |
| Pbv—O1—Pbxi | 108.051 (15) | Pbxv—O3H—Pbiv | 119.24 (3) |
| Pbiv—O1—Pbxv | 53.957 (13) | Pbxxii—O3H—Pbix | 141.606 (14) |
| Pbxvii—O1—Pbxv | 94.056 (4) | Pbxxiii—O3H—Pbix | 94.262 (4) |
| Pbxvi—O1—Pbxiii | 56.044 (19) | Pb—O3H—Pbxvii | 60.734 (7) |
| Pbxvi—O1—Pbxi | 112.35 (3) | Pb—O3H—Pbxvi | 52.101 (18) |
| Pbix—O1—Pbxiii | 149.152 (13) | Pbxvi—O3H—Pbxvii | 50.571 (15) |
| Pbiv—O1—Pbxiii | 94.056 (4) | Pbxi—O3H—Pbxvii | 94.262 (4) |
| Pb—O1—Pbviii | 103.228 (10) | Pbii—O3H—Pbxvii | 48.014 (14) |
| Pb—O1—Pbxii | 148.721 (10) | Pbxix—O3H—Pbxvi | 152.875 (9) |
| Pbxii—O1—Pbviii | 45.493 (14) | Pbxix—O3H—Pbxxii | 52.101 (18) |
| Pbxiv—O1—Pbviii | 94.056 (4) | Pbxxii—O3H—Pbii | 50.571 (15) |
| Pbxi—O1—Pbxvii | 148.721 (10) | Pbxv—O3H—Pbxxii | 102.305 (10) |
| Pbv—O1—Pbxii | 56.044 (19) | Pbxv—O3H—Pbxvi | 102.305 (10) |
| Pbv—O1—Pbix | 103.228 (10) | Pbiv—O3H—Pbxxii | 60.734 (7) |
| Pbix—O1—Pbxvii | 116.547 (13) | Pbxv—O3H—Pbxviii | 52.101 (18) |
| Pbxvi—O1—Pbix | 148.721 (10) | Pbxvi—O3H—Pbxxii | 121.353 (13) |
| Pbxvi—O1—Pbxii | 103.228 (10) | Pbiv—O3H—Pbxvi | 60.734 (7) |
| Pbxi—O1—Pbix | 56.044 (19) | Pbxi—O3H—Pbxxii | 148.360 (14) |
| Pbxvi—O1—Pbxv | 103.228 (10) | Pbxxii—O3H—Pbxviii | 94.262 (4) |
| Pbxii—O1—Pbix | 94.056 (3) | Pb—O3H—Pbxxiii | 152.876 (9) |
| Pbxi—O1—Pbxii | 58.337 (6) | Pb—O3H—Pbxi | 52.101 (18) |
| Pbxiv—O1—Pbix | 147.401 (13) | Pbxix—O3H—Pbxxiii | 52.101 (18) |
| Pbix—O1—Pbxv | 45.493 (14) | Pbxix—O3H—Pbix | 102.305 (10) |
| Pb—O1—Pbiv | 56.043 (19) | Pbxv—O3H—Pbxxiii | 60.734 (7) |
| Pb—O1—Pbxiv | 148.721 (10) | Pbxix—O3H—Pbxi | 152.875 (9) |
| Pbv—O1—Pbiv | 148.721 (10) | Pbiv—O3H—Pbxxiii | 102.305 (10) |
| Pbv—O1—Pbxiii | 58.337 (6) | Pbxi—O3H—Pbix | 50.571 (15) |
| Pbxvi—O1—Pbiv | 58.337 (6) | Pbxvi—O3H—Pbxxiii | 148.360 (14) |
| Pbv—O1—Pbxiv | 56.044 (19) | Pbxv—O3H—Pbxi | 60.734 (7) |
| Pbxi—O1—Pbiv | 103.228 (10) | Pbxi—O3H—Pbxxiii | 121.353 (13) |
| Pbxiv—O1—Pbxiii | 45.493 (14) | Pbxviii—O3H—Pbix | 48.014 (14) |
| Pbxii—O1—Pbiv | 149.152 (13) | Pbxxii—O3H—Pbxxiii | 48.014 (14) |
| Pbxvi—O1—Pbxiv | 58.337 (6) | Pbiv—O3H—Pbxi | 102.305 (10) |
| Pbxiv—O1—Pbiv | 116.547 (13) | Pb—O3H—Pbii | 102.305 (10) |
| Pbxv—O1—Pbxiii | 147.401 (13) | Pbiv—O3H—Pbxvii | 52.101 (18) |
| Pbix—O1—Pbiv | 94.056 (4) | Pbxix—O3H—Pbii | 60.734 (7) |
| Pbxi—O1—Pbxiv | 103.228 (10) | Pbxvi—O3H—Pbxi | 48.014 (14) |
| Pb—O1—Pbxvii | 58.337 (6) | Pbxv—O3H—Pbii | 152.875 (9) |
| Pbxi—O1—Pbviii | 56.044 (19) | Pbxxiii—O3H—Pbxvii | 141.606 (14) |
| Pbv—O1—Pbxvii | 103.228 (10) | Pbiv—O3H—Pbii | 52.101 (18) |
| Pbxii—O1—Pbxiv | 53.957 (13) | Pb—O3H—Pbxxii | 152.876 (9) |
| Pbxvi—O1—Pbxvii | 56.044 (19) | Pbxvi—O3H—Pbii | 94.262 (4) |
| Pbxvii—O1—Pbviii | 149.152 (13) | Pbxi—O3H—Pbii | 141.606 (14) |
| Pbxii—O1—Pbxvii | 147.401 (13) |
| Symmetry codes: (i) −x+1, −y+1, −z; (ii) x, y−1, z; (iii) −x, −y+1, −z; (iv) y, −x, −z+1/2; (v) −x+1, −y+1, z; (vi) y, −x+1, z−1/2; (vii) x, y+1, −z; (viii) x, y+1, z; (ix) −x, −y+1, z; (x) x, y, −z; (xi) y, −x+1, −z+1/2; (xii) −y+1, x+1, −z+1/2; (xiii) x+1, y, z; (xiv) y+1, −x+1, −z+1/2; (xv) −y, x, −z+1/2; (xvi) −y+1, x, −z+1/2; (xvii) −x+1, −y, z; (xviii) x−1, y, z; (xix) −x, −y, z; (xx) −y, x+1, −z+1/2; (xxi) y−1, −x+1, −z+1/2; (xxii) −y, x−1, −z+1/2; (xxiii) y−1, −x, −z+1/2. |
| Pb (8 o) | m | 2.16 |
| Br (4 j) | mm2 | 0.84 |
| O1 (2 d) | 42m | 2.34 |
| O2 (4 e) | 222 | 1.70 |
| O3H (2 b) | 42m | 1.25 |
Acknowledgements
The XRD experiments were performed as joint research at the Institute for Solid State Physics, University of Tokyo and at the Molecular Structure Analysis Section, Shizuoka Instrumental Analysis Center, Shizuoka University.
Funding information
Funding for this research was provided by: Japan Society for the Promotion of Science.
References
Alun Humphreys, D., Thomas, J. H., Williams, P. A. & Symes, R. F. (1980). Miner. Mag. 43, 901–904. CrossRef Google Scholar
Brese, N. E. & O'Keeffe, M. (1991). Acta Cryst. B47, 192–197. CrossRef CAS Web of Science IUCr Journals Google Scholar
Brown, I. D. (2002). The Chemical Bond in Inorganic Chemistry: The Bond Valence Model. Oxford University Press. Google Scholar
Dolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339–341. Web of Science CrossRef CAS IUCr Journals Google Scholar
Krivovichev, S. V. & Burns, P. C. (2001). Solid State Sci. 3, 455–459. CrossRef CAS Google Scholar
Momma, K. & Izumi, F. (2011). J. Appl. Cryst. 44, 1272–1276. Web of Science CrossRef CAS IUCr Journals Google Scholar
Rigaku OD (2023). CrysAlis PRO. Rigaku Oxford Diffraction, Yarnton, England. Google Scholar
Sheldrick, G. M. (2015a). Acta Cryst. A71, 3–8. Web of Science CrossRef IUCr Journals Google Scholar
Sheldrick, G. M. (2015b). Acta Cryst. C71, 3–8. Web of Science CrossRef IUCr Journals Google Scholar
Siidra, O. I., Zenko, D. Y., Suknotova, A. N. & Krivovichev, S. V. (2013). Miner. Mag. 77, 3239–3248. CrossRef CAS Google Scholar
Turner, R. W., Siidra, O. I., Rumsey, M. S., Polekhovsky, Y. S., Kretser, Y. L., Krivovichev, S. V., Spratt, J. & Stanley, C. J. (2015). Miner. Mag. 79, 1203–1211. CrossRef Google Scholar
Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925. Web of Science CrossRef CAS IUCr Journals Google Scholar
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