inorganic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Journal logoIUCrDATA
ISSN: 2414-3146

Dilead(II) oxyhydroxide bromide

crossmark logo

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]

Edited by M. Weil, Vienna University of Technology, Austria (Received 17 July 2026; accepted 1 August 2026; online 7 August 2026)

The crystal structure 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.

3D view (loading...)
[Scheme 3D1]

Structure description

Lead oxyhalides comprise a diverse family of compounds with a variety of crystal structures. Among them, Pb2O(OH)Cl (Turner et al., 2015View full citation), Pb2O(OH)I (Siidra et al., 2013View full citation), and Pb3O2(OH)Br (Krivovichev & Burns, 2001View full citation) 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[link] and Table 1[link]). 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[link]). 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[link]).

Table 1
Selected bond lengths (Å)

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)
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation.
[Figure 1]
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 + Mathematical equation.]
[Figure 2]
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]
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 + Mathematical equation; (v) −x + 1, −y + 1, z; (vi) y, −x + 1, z − Mathematical equation; (vii) x, y + 1, −z; (viii) x, y + 1, z; (ix) −x, −y + 1, z; (x) x, y, −z; (xi) y, −x + 1, −z + Mathematical equation; (xv) −y, x, −z + Mathematical equation; (xvi) −y + 1, x, −z + Mathematical equation; (xvii) −x + 1, −y, z; (xix) −x, −y, 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, 2002View full citation; Brese & O'Keeffe, 1991View full citation) were therefore carried out to identify the hydroxide site (Table 2[link]). 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.

Table 2
Atomic sites (multiplicity and Wyckoff letter), site symmetries, and bond-valence sums (in valence units)

Pb (8 o) m 2.16
Br (4 j) mm2 0.84
O1 (2 d) Mathematical equation2m 2.34
O2 (4 e) 222 1.70
O3H (2 b) Mathematical equation2m 1.25

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., 1980View full citation) 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 refinement are given in Table 3[link]. 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.

Table 3
Experimental details

Crystal data
Chemical formula Pb2O(OH)Br
Mr 526.29
Crystal system, space group Tetragonal, P42/mcm
Temperature (K) 296
a, c (Å) 5.8161 (3), 12.8870 (13)
V3) 435.93 (6)
Z 4
Radiation type Mo Kα
μ (mm−1) 86.13
Crystal size (mm) 0.10 × 0.08 × 0.01
 
Data collection
Diffractometer XtaLAB AFC11 (RCD3): quarter-chi single
Absorption correction Multi-scan (CrysAlis PRO; Rigaku OD, 2023View full citation)
Tmin, Tmax 0.542, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections 9139, 705, 460
Rint 0.062
(sin θ/λ)max−1) 0.882
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.044, 0.131, 1.12
No. of reflections 705
No. of parameters 18
H-atom treatment H-atom parameters not defined
Δρmax, Δρmin (e Å−3) 6.55, −4.22
Computer programs: CrysAlis PRO (Rigaku OD, 2023View full citation), SHELXT (Sheldrick, 2015aView full citation), SHELXL (Sheldrick, 2015bView full citation), VESTA (Momma & Izumi, 2011View full citation), OLEX2 (Dolomanov et al., 2009View full citation) and publCIF (Westrip, 2010View full citation).

Structural data


Computing details top

Dilead(II) oxyhydroxide bromide top
Crystal data top
Pb2O(OH)BrDx = 8.019 Mg m3
Mr = 526.29Mo Kα radiation, λ = 0.71073 Å
Tetragonal, P42/mcmCell parameters from 2463 reflections
a = 5.8161 (3) Åθ = 3.1–34.3°
c = 12.8870 (13) ŵ = 86.13 mm1
V = 435.93 (6) Å3T = 296 K
Z = 4Plate, yellow
F(000) = 8600.10 × 0.08 × 0.01 mm
Data collection top
XtaLAB AFC11 (RCD3): quarter-chi single
diffractometer
705 independent reflections
Radiation source: Rotating-anode X-ray tube, Rigaku (Mo) X-ray Source460 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.062
Detector resolution: 10.0000 pixels mm-1θmax = 38.8°, θmin = 3.2°
ω scansh = 810
Absorption correction: multi-scan
(CrysAlisPro; Rigaku OD, 2023)
k = 1010
Tmin = 0.542, Tmax = 1.000l = 2218
9139 measured reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullPrimary atom site location: dual
R[F2 > 2σ(F2)] = 0.044H-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 reflectionsΔρmax = 6.55 e Å3
18 parametersΔρmin = 4.22 e Å3
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pb0.26668 (8)0.26668 (8)0.15022 (4)0.01991 (19)
Br0.2582 (3)0.7418 (3)0.0000000.0233 (4)
O10.5000000.5000000.2500000.018 (7)
O20.0000000.5000000.2500000.023 (8)
O3H0.0000000.0000000.2500000.020 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pb0.0215 (2)0.0215 (2)0.0168 (3)0.0095 (3)0.00071 (12)0.00071 (12)
Br0.0204 (6)0.0204 (6)0.0290 (11)0.0022 (15)0.0000.000
O10.020 (10)0.020 (10)0.015 (16)0.0000.0000.000
O20.016 (10)0.024 (12)0.03 (2)0.0000.0000.000
O3H0.022 (11)0.022 (11)0.017 (17)0.0000.0000.000
Geometric parameters (Å, º) top
Pb—Bri3.3741 (15)Pb—O12.3101 (6)
Pb—Br3.3741 (15)Pb—O2iv2.4291 (3)
Pb—Brii3.6154 (15)Pb—O22.4291 (3)
Pb—Briii3.6154 (15)Pb—O3H2.5426 (6)
Br—Pb—Bri72.22 (6)Pb—O1—Pbix58.337 (6)
Briii—Pb—Brii71.96 (6)Pbxiv—O1—Pbxvii94.056 (3)
Br—Pb—Briii72.039 (8)Pbxv—O1—Pbviii94.056 (4)
Bri—Pb—Brii72.039 (8)Pb—O2—Pbxi100.64 (3)
Br—Pb—Brii112.590 (16)Pbxviii—O2—Pbxix51.065 (2)
Bri—Pb—Briii112.590 (16)Pbxviii—O2—Pbxx92.740 (7)
O1—Pb—Br81.191 (16)Pbviii—O2—Pbiv143.039 (7)
O1—Pb—Bri81.191 (16)Pbxvi—O2—Pbviii92.740 (7)
O1—Pb—Brii143.33 (3)Pbix—O2—Pbxx55.085 (16)
O1—Pb—Briii143.33 (3)Pbxv—O2—Pbiv63.525 (18)
O1—Pb—O275.655 (14)Pb—O2—Pbxv112.08 (3)
O1—Pb—O2iv75.655 (14)Pbxi—O2—Pbviii55.085 (16)
O1—Pb—O3H115.80 (2)Pbxviii—O2—Pbviii118.901 (6)
O2—Pb—Briii75.63 (3)Pb—O2—Pbxx148.277 (12)
O2iv—Pb—Brii75.63 (3)Pbxi—O2—Pbxv116.07 (2)
O2iv—Pb—Br146.59 (3)Pbxix—O2—Pbxx143.039 (7)
O2—Pb—Bri146.59 (3)Pbxi—O2—Pbiv99.647 (17)
O2—Pb—Brii138.29 (3)Pbv—O2—Pbiv92.740 (7)
O2iv—Pb—Briii138.29 (3)Pb—O2—Pbix116.07 (2)
O2—Pb—Br80.62 (3)Pbxxi—O2—Pbxix92.740 (7)
O2iv—Pb—Bri80.62 (3)Pb—O2—Pbviii99.647 (17)
O2iv—Pb—O2115.67 (2)Pbix—O2—Pbviii63.525 (19)
O2—Pb—O3H71.552 (14)Pbxi—O2—Pbix112.08 (3)
O2iv—Pb—O3H71.552 (14)Pbxxi—O2—Pbviii95.585 (7)
O3H—Pb—Brii75.368 (15)Pbxix—O2—Pbviii149.527 (14)
O3H—Pb—Briii75.368 (15)Pbxv—O2—Pbxx99.647 (17)
O3H—Pb—Br141.34 (3)Pbxv—O2—Pbix100.64 (3)
O3H—Pb—Bri141.34 (3)Pbv—O2—Pbxx95.585 (8)
Pbv—Br—Pbvi124.37 (4)Pbxxi—O2—Pbxx51.065 (2)
Pbi—Br—Pbvii72.180 (8)Pb—O2—Pbiv55.085 (16)
Pbviii—Br—Pbix74.70 (4)Pb—O2—Pbxviii106.011 (17)
Pb—Br—Pbvi124.37 (4)Pbxviii—O2—Pbiv95.585 (7)
Pbx—Br—Pbix107.961 (8)Pbxvi—O2—Pbiv51.065 (2)
Pbiii—Br—Pbvi58.241 (14)Pbxix—O2—Pbiv48.630 (9)
Pbx—Br—Pbvii112.591 (17)Pbxi—O2—Pbxviii153.350 (11)
Pbix—Br—Pbvi122.98 (3)Pbxi—O2—Pbv53.030 (17)
Pb—Br—Pbviii112.590 (16)Pbv—O2—Pbxix118.901 (6)
Pbv—Br—Pbxi54.357 (14)Pbxv—O2—Pbv153.350 (11)
Pbi—Br—Pbix176.910 (14)Pbxv—O2—Pbxviii53.030 (17)
Pb—Br—Pbxi54.357 (14)Pbix—O2—Pbv106.011 (17)
Pbviii—Br—Pbiii108.04 (6)Pbxv—O2—Pbviii148.277 (12)
Pbx—Br—Pbviii176.910 (15)Pbxviii—O2—Pbv147.940 (14)
Pb—Br—Pbvii176.910 (15)Pbix—O2—Pbxviii55.377 (19)
Pbv—Br—Pbviii72.179 (8)Pbxvi—O2—Pbv47.339 (10)
Pbi—Br—Pbviii107.961 (8)Pbv—O2—Pbviii51.065 (2)
Pbiii—Br—Pbvii74.70 (4)Pb—O2—Pbxxi153.350 (11)
Pbix—Br—Pbxi58.241 (14)Pb—O2—Pbxvi53.029 (17)
Pbx—Br—Pbxi124.37 (4)Pbxi—O2—Pbxxi106.011 (17)
Pbvii—Br—Pbix108.04 (6)Pbxi—O2—Pbxx63.525 (19)
Pbv—Br—Pbiii176.910 (15)Pbxv—O2—Pbxxi55.377 (19)
Pbx—Br—Pbvi54.357 (14)Pbxi—O2—Pbxvi55.377 (19)
Pbi—Br—Pbxi124.37 (4)Pbix—O2—Pbxxi53.030 (17)
Pbi—Br—Pbvi54.357 (14)Pbxvi—O2—Pbxx118.901 (6)
Pb—Br—Pbiii107.961 (8)Pbxviii—O2—Pbxxi47.339 (9)
Pbviii—Br—Pbvi122.98 (3)Pbxv—O2—Pbxvi106.011 (17)
Pbiii—Br—Pbxi122.98 (3)Pbxvi—O2—Pbxxi147.940 (14)
Pbx—Br—Pbv107.78 (6)Pbviii—O2—Pbxx48.630 (8)
Pbv—Br—Pbix112.591 (17)Pbv—O2—Pbxxi146.116 (7)
Pbx—Br—Pbi69.33 (4)Pbix—O2—Pbxvi153.350 (11)
Pbv—Br—Pbvii107.961 (8)Pb—O2—Pbxix63.525 (19)
Pbv—Br—Pbi70.02 (4)Pbix—O2—Pbiv148.277 (12)
Pbi—Br—Pbiii112.591 (17)Pbxi—O2—Pbxix148.277 (12)
Pbx—Br—Pb70.02 (4)Pbxviii—O2—Pbxvi146.116 (7)
Pb—Br—Pbix72.179 (8)Pbxv—O2—Pbxix55.085 (16)
Pbv—Br—Pb69.33 (4)Pbxxi—O2—Pbiv118.901 (6)
Pbx—Br—Pbiii72.180 (8)Pbix—O2—Pbxix99.647 (17)
Pbi—Br—Pb107.78 (6)Pb—O2—Pbv55.377 (19)
Pbviii—Br—Pbvii64.75 (3)Pbxvi—O2—Pbxix95.585 (7)
Pbvi—Br—Pbxi178.24 (6)Pbxx—O2—Pbiv149.527 (14)
Pbiii—Br—Pbix64.75 (3)Pb—O3H—Pbxix119.24 (3)
Pbviii—Br—Pbxi58.241 (14)Pbix—O3H—Pbxvii121.353 (13)
Pbvii—Br—Pbvi58.241 (14)Pbxvi—O3H—Pbix94.262 (4)
Pbvii—Br—Pbxi122.98 (3)Pbxviii—O3H—Pbxvii148.360 (14)
Pb—O1—Pbv112.35 (3)Pbxi—O3H—Pbxviii94.262 (4)
Pbiv—O1—Pbviii147.401 (13)Pbiv—O3H—Pbix152.875 (9)
Pbxii—O1—Pbxiii94.056 (4)Pbxv—O3H—Pbxvii152.875 (9)
Pbxiii—O1—Pbviii116.547 (13)Pb—O3H—Pbxv104.820 (12)
Pbxiv—O1—Pbxv149.152 (13)Pbxix—O3H—Pbxviii60.734 (7)
Pbxi—O1—Pbxiii148.721 (10)Pbxvi—O3H—Pbxviii141.606 (14)
Pbxvi—O1—Pbviii148.721 (10)Pb—O3H—Pbix60.734 (7)
Pb—O1—Pbxvi108.051 (15)Pbxix—O3H—Pbxv104.820 (12)
Pbv—O1—Pbxv148.721 (10)Pbii—O3H—Pbix148.360 (14)
Pbxii—O1—Pbxv116.547 (13)Pbxix—O3H—Pbxvii102.305 (10)
Pb—O1—Pbxiii103.228 (10)Pbxxii—O3H—Pbxvii94.262 (4)
Pbv—O1—Pbxvi108.051 (15)Pb—O3H—Pbiv104.820 (12)
Pbxvii—O1—Pbxiii53.957 (13)Pbxxiii—O3H—Pbii94.262 (4)
Pbv—O1—Pbviii58.337 (6)Pb—O3H—Pbxviii102.305 (10)
Pbix—O1—Pbviii53.957 (13)Pbiv—O3H—Pbxviii152.875 (9)
Pb—O1—Pbxi108.051 (15)Pbxix—O3H—Pbiv104.820 (12)
Pbiv—O1—Pbxvii45.493 (14)Pbxxiii—O3H—Pbxviii50.571 (15)
Pb—O1—Pbxv56.043 (19)Pbii—O3H—Pbxviii121.353 (13)
Pbxi—O1—Pbxv58.337 (6)Pbxv—O3H—Pbix52.101 (18)
Pbv—O1—Pbxi108.051 (15)Pbxv—O3H—Pbiv119.24 (3)
Pbiv—O1—Pbxv53.957 (13)Pbxxii—O3H—Pbix141.606 (14)
Pbxvii—O1—Pbxv94.056 (4)Pbxxiii—O3H—Pbix94.262 (4)
Pbxvi—O1—Pbxiii56.044 (19)Pb—O3H—Pbxvii60.734 (7)
Pbxvi—O1—Pbxi112.35 (3)Pb—O3H—Pbxvi52.101 (18)
Pbix—O1—Pbxiii149.152 (13)Pbxvi—O3H—Pbxvii50.571 (15)
Pbiv—O1—Pbxiii94.056 (4)Pbxi—O3H—Pbxvii94.262 (4)
Pb—O1—Pbviii103.228 (10)Pbii—O3H—Pbxvii48.014 (14)
Pb—O1—Pbxii148.721 (10)Pbxix—O3H—Pbxvi152.875 (9)
Pbxii—O1—Pbviii45.493 (14)Pbxix—O3H—Pbxxii52.101 (18)
Pbxiv—O1—Pbviii94.056 (4)Pbxxii—O3H—Pbii50.571 (15)
Pbxi—O1—Pbxvii148.721 (10)Pbxv—O3H—Pbxxii102.305 (10)
Pbv—O1—Pbxii56.044 (19)Pbxv—O3H—Pbxvi102.305 (10)
Pbv—O1—Pbix103.228 (10)Pbiv—O3H—Pbxxii60.734 (7)
Pbix—O1—Pbxvii116.547 (13)Pbxv—O3H—Pbxviii52.101 (18)
Pbxvi—O1—Pbix148.721 (10)Pbxvi—O3H—Pbxxii121.353 (13)
Pbxvi—O1—Pbxii103.228 (10)Pbiv—O3H—Pbxvi60.734 (7)
Pbxi—O1—Pbix56.044 (19)Pbxi—O3H—Pbxxii148.360 (14)
Pbxvi—O1—Pbxv103.228 (10)Pbxxii—O3H—Pbxviii94.262 (4)
Pbxii—O1—Pbix94.056 (3)Pb—O3H—Pbxxiii152.876 (9)
Pbxi—O1—Pbxii58.337 (6)Pb—O3H—Pbxi52.101 (18)
Pbxiv—O1—Pbix147.401 (13)Pbxix—O3H—Pbxxiii52.101 (18)
Pbix—O1—Pbxv45.493 (14)Pbxix—O3H—Pbix102.305 (10)
Pb—O1—Pbiv56.043 (19)Pbxv—O3H—Pbxxiii60.734 (7)
Pb—O1—Pbxiv148.721 (10)Pbxix—O3H—Pbxi152.875 (9)
Pbv—O1—Pbiv148.721 (10)Pbiv—O3H—Pbxxiii102.305 (10)
Pbv—O1—Pbxiii58.337 (6)Pbxi—O3H—Pbix50.571 (15)
Pbxvi—O1—Pbiv58.337 (6)Pbxvi—O3H—Pbxxiii148.360 (14)
Pbv—O1—Pbxiv56.044 (19)Pbxv—O3H—Pbxi60.734 (7)
Pbxi—O1—Pbiv103.228 (10)Pbxi—O3H—Pbxxiii121.353 (13)
Pbxiv—O1—Pbxiii45.493 (14)Pbxviii—O3H—Pbix48.014 (14)
Pbxii—O1—Pbiv149.152 (13)Pbxxii—O3H—Pbxxiii48.014 (14)
Pbxvi—O1—Pbxiv58.337 (6)Pbiv—O3H—Pbxi102.305 (10)
Pbxiv—O1—Pbiv116.547 (13)Pb—O3H—Pbii102.305 (10)
Pbxv—O1—Pbxiii147.401 (13)Pbiv—O3H—Pbxvii52.101 (18)
Pbix—O1—Pbiv94.056 (4)Pbxix—O3H—Pbii60.734 (7)
Pbxi—O1—Pbxiv103.228 (10)Pbxvi—O3H—Pbxi48.014 (14)
Pb—O1—Pbxvii58.337 (6)Pbxv—O3H—Pbii152.875 (9)
Pbxi—O1—Pbviii56.044 (19)Pbxxiii—O3H—Pbxvii141.606 (14)
Pbv—O1—Pbxvii103.228 (10)Pbiv—O3H—Pbii52.101 (18)
Pbxii—O1—Pbxiv53.957 (13)Pb—O3H—Pbxxii152.876 (9)
Pbxvi—O1—Pbxvii56.044 (19)Pbxvi—O3H—Pbii94.262 (4)
Pbxvii—O1—Pbviii149.152 (13)Pbxi—O3H—Pbii141.606 (14)
Pbxii—O1—Pbxvii147.401 (13)
Symmetry codes: (i) x+1, y+1, z; (ii) x, y1, z; (iii) x, y+1, z; (iv) y, x, z+1/2; (v) x+1, y+1, z; (vi) y, x+1, z1/2; (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) x1, y, z; (xix) x, y, z; (xx) y, x+1, z+1/2; (xxi) y1, x+1, z+1/2; (xxii) y, x1, z+1/2; (xxiii) y1, x, z+1/2.
Atomic sites (multiplicity and Wyckoff letter), site symmetries, and bond-valence sums (in valence units) top
Pb (8 o)m2.16
Br (4 j)mm20.84
O1 (2 d)42m2.34
O2 (4 e)2221.70
O3H (2 b)42m1.25
 

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

Return to citationAlun Humphreys, D., Thomas, J. H., Williams, P. A. & Symes, R. F. (1980). Miner. Mag. 43, 901–904.  CrossRef Google Scholar
Return to citationBrese, N. E. & O'Keeffe, M. (1991). Acta Cryst. B47, 192–197.  CrossRef CAS Web of Science IUCr Journals Google Scholar
Return to citationBrown, I. D. (2002). The Chemical Bond in Inorganic Chemistry: The Bond Valence Model. Oxford University Press.  Google Scholar
Return to citationDolomanov, 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
Return to citationKrivovichev, S. V. & Burns, P. C. (2001). Solid State Sci. 3, 455–459.  CrossRef CAS Google Scholar
Return to citationMomma, K. & Izumi, F. (2011). J. Appl. Cryst. 44, 1272–1276.  Web of Science CrossRef CAS IUCr Journals Google Scholar
Return to citationRigaku OD (2023). CrysAlis PRO. Rigaku Oxford Diffraction, Yarnton, England.  Google Scholar
Return to citationSheldrick, G. M. (2015a). Acta Cryst. A71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationSheldrick, G. M. (2015b). Acta Cryst. C71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationSiidra, O. I., Zenko, D. Y., Suknotova, A. N. & Krivovichev, S. V. (2013). Miner. Mag. 77, 3239–3248.  CrossRef CAS Google Scholar
Return to citationTurner, 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
Return to citationWestrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.  Web of Science CrossRef CAS IUCr Journals Google Scholar

This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.

Journal logoIUCrDATA
ISSN: 2414-3146