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Organolead compounds are of inter­est mainly as catalysts and organolead halides have proved to be very efficient materials for solar cells. Two organolead(IV) di­methyl­arsinates, namely catena-poly[[tri­phenyl­lead(IV)]-μ-chlorido-[tri­phenyl­lead(IV)]-μ-di­methyl­arsinato-κ2O:O′], [Pb2(C6H5)6(C2H6AsO2)Cl]n or [(Ph3Pb)2Cl(O2AsMe2)], (1), and poly[chlorido­(μ3-di­methyl­arsinato-κ3O:O,O′:O′)di­phenyl­lead(IV)], [Pb(C6H5)2(C2H6AsO2)Cl]n or [(Ph2ClPb)(O2AsMe2)], (2), together with the tri­phenyl­lead(IV) di­phenyl­phosphinate catena-poly[[tri­phenyl­lead(IV)]-μ-di­phenyl­phosphinato-κ2O:O′], [Pb(C6H5)3(C12H10O2P)]n or [(Ph3Pb)(O2PPh2)], (3), have been synthesized and characterized by single-crystal X-ray diffraction, IR spectroscopy and mass spectrometry. In (1), a chain structure was found with alternating chloride and Pb—O—As—O—Pb arsinate bridges between five-coordinate PbIV atoms. In (2), bidentate and chelate-like bonded di­methyl­arsinate ligands form double chains with heptacoordinated PbIV atoms. In (3), a pentacoordinated PbIV atom is connected by Pb—O—P—O—Pb phosphinate bridges to form a linear chain. Obviously, the steric demand of the phenyl ligands at PbIV reduces the possibility of inter­connections via polydentate ligands to one dimension only. Thus, no metal–organic frameworks (MOF) are formed but instead various chain structures are observed.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229618004850/uk3151sup1.cif
Contains datablocks 1, 2, 3, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229618004850/uk3151Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229618004850/uk3151IIsup3.hkl
Contains datablock II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229618004850/uk3151IIIsup4.hkl
Contains datablock III

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2053229618004850/uk3151sup5.pdf
Geometrical, Raman, IR and MS data

CCDC references: 1497176; 1497175; 1497174

Computing details top

For all structures, data collection: X-AREA (Stoe & Cie, 2013); cell refinement: X-AREA (Stoe & Cie, 2013); data reduction: X-AREA (Stoe & Cie, 2013). Program(s) used to solve structure: SHELXS97 (Sheldrick, 2008) for (1), (3); SIR2011 (Burla et al., 2012) for (2). Program(s) used to refine structure: SHELXL2013 (Sheldrick, 2015) for (1), (3); SHELXL97 (Sheldrick, 2008) for (2). For all structures, molecular graphics: DIAMOND (Brandenburg, 2016).

catena-Poly[[triphenyllead(IV)]-µ-chlorido-[triphenyllead(IV)]-µ-dimethylarsinato-κ2O:O'] (1) top
Crystal data top
[Pb2(C6H5)6(C2H6AsO2)Cl]Dx = 1.955 Mg m3
Mr = 1049.42Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 9292 reflections
a = 19.0566 (8) Åθ = 2.0–26.1°
b = 15.5255 (10) ŵ = 10.46 mm1
c = 24.0975 (14) ÅT = 153 K
V = 7129.6 (7) Å3Block, colourless
Z = 80.16 × 0.12 × 0.09 mm
F(000) = 3952
Data collection top
Stoe IPDS 2
diffractometer
6273 independent reflections
Radiation source: fine-focus sealed tube4712 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.076
Detector resolution: 6.7 pixels mm-1θmax = 25.0°, θmin = 1.9°
ω scansh = 2022
Absorption correction: gaussian
(Coppens et al., 1965)
k = 1818
Tmin = 0.383, Tmax = 0.585l = 2528
41656 measured reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.040H-atom parameters constrained
wR(F2) = 0.079 w = 1/[σ2(Fo2) + (0.036P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
6273 reflectionsΔρmax = 2.64 e Å3
325 parametersΔρmin = 1.31 e Å3
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. All phenyl rings were refined as idealized rigid groups (AFIX 66)

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pb10.21533 (2)0.25344 (2)0.08898 (2)0.02170 (8)
Pb20.24676 (2)0.33066 (2)0.31934 (2)0.02138 (8)
As10.19577 (4)0.12320 (5)0.03722 (4)0.02216 (19)
Cl10.24679 (12)0.29385 (13)0.19868 (8)0.0268 (4)
O10.2518 (3)0.1413 (4)0.0892 (2)0.0285 (13)
O20.1834 (3)0.2131 (3)0.0004 (3)0.0273 (13)
C10.3288 (2)0.2547 (4)0.0685 (2)0.030 (2)
C20.3801 (3)0.2420 (4)0.10865 (18)0.0283 (19)
H20.36690.23140.14610.034*
C30.4507 (2)0.2448 (4)0.0941 (2)0.039 (2)
H30.48570.23610.12160.047*
C40.4699 (2)0.2602 (4)0.0394 (3)0.041 (3)
H40.51810.26210.02940.049*
C50.4186 (3)0.2730 (4)0.0008 (2)0.043 (3)
H50.43180.28360.03820.052*
C60.3481 (3)0.2702 (4)0.0137 (2)0.035 (2)
H60.31300.27890.01370.042*
C70.1587 (3)0.1393 (3)0.1192 (3)0.0243 (19)
C80.1921 (2)0.0757 (3)0.1500 (3)0.033 (2)
H80.23880.08430.16250.040*
C90.1570 (3)0.0003 (3)0.1626 (3)0.040 (3)
H90.17990.04380.18370.048*
C100.0886 (3)0.0128 (3)0.1443 (3)0.045 (3)
H100.06470.06480.15290.054*
C110.0552 (3)0.0508 (4)0.1135 (3)0.047 (3)
H110.00840.04230.10100.057*
C120.0902 (3)0.1269 (3)0.1009 (3)0.035 (2)
H120.06740.17030.07980.042*
C130.1551 (3)0.3738 (3)0.0779 (2)0.0219 (18)
C140.1211 (3)0.3876 (3)0.0277 (2)0.0252 (19)
H140.12370.34560.00090.030*
C150.0832 (3)0.4630 (3)0.01919 (19)0.029 (2)
H150.06000.47240.01520.035*
C160.0793 (3)0.5246 (3)0.0610 (2)0.031 (2)
H160.05340.57610.05510.038*
C170.1133 (3)0.5108 (3)0.1112 (2)0.032 (2)
H170.11070.55280.13980.039*
C180.1512 (3)0.4354 (3)0.11970 (18)0.027 (2)
H180.17440.42600.15400.033*
C190.1776 (3)0.2159 (3)0.3269 (2)0.0244 (19)
C200.1786 (3)0.1660 (4)0.3748 (2)0.035 (2)
H200.20850.18130.40470.042*
C210.1357 (3)0.0938 (3)0.3789 (2)0.037 (2)
H210.13640.05980.41160.044*
C220.0919 (3)0.0715 (3)0.3351 (3)0.036 (2)
H220.06260.02220.33790.043*
C230.0909 (3)0.1214 (4)0.2872 (2)0.035 (2)
H230.06100.10610.25720.042*
C240.1338 (3)0.1936 (3)0.2831 (2)0.030 (2)
H240.13310.22760.25030.036*
C250.36245 (19)0.3285 (4)0.3184 (2)0.0241 (18)
C260.3991 (3)0.3391 (4)0.36779 (18)0.0277 (19)
H260.37430.34880.40140.033*
C270.4719 (3)0.3355 (4)0.3680 (2)0.034 (2)
H270.49700.34280.40180.041*
C280.50821 (19)0.3213 (4)0.3188 (2)0.032 (2)
H280.55800.31890.31900.038*
C290.4716 (3)0.3107 (4)0.2694 (2)0.032 (2)
H290.49640.30100.23580.039*
C300.3987 (3)0.3143 (4)0.26917 (18)0.0255 (19)
H300.37370.30700.23540.031*
C310.1862 (3)0.4447 (3)0.2943 (3)0.0227 (18)
C320.1144 (3)0.4337 (3)0.2871 (3)0.031 (2)
H320.09360.37900.29370.037*
C330.0730 (2)0.5026 (3)0.2703 (3)0.031 (2)
H330.02390.49510.26540.037*
C340.1034 (3)0.5826 (3)0.2607 (3)0.034 (2)
H340.07510.62970.24920.040*
C350.1752 (3)0.5937 (3)0.2679 (3)0.035 (2)
H350.19600.64840.26130.042*
C360.2166 (2)0.5247 (3)0.2847 (3)0.031 (2)
H360.26570.53230.28970.037*
C370.2334 (5)0.0304 (6)0.0061 (4)0.038 (2)
H37A0.20190.01820.03720.046*
H37B0.27970.04670.02030.046*
H37C0.23780.02100.01720.046*
C380.1081 (5)0.0862 (7)0.0660 (4)0.038 (2)
H38A0.07540.07580.03530.045*
H38B0.11460.03280.08710.045*
H38C0.08890.13080.09050.045*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pb10.02607 (15)0.01689 (13)0.02215 (16)0.00096 (13)0.00054 (14)0.00002 (14)
Pb20.02182 (15)0.02003 (14)0.02229 (16)0.00047 (13)0.00117 (15)0.00149 (12)
As10.0255 (4)0.0188 (4)0.0222 (5)0.0005 (3)0.0000 (4)0.0010 (3)
Cl10.0306 (11)0.0259 (9)0.0239 (11)0.0011 (9)0.0014 (10)0.0007 (8)
O10.028 (3)0.036 (3)0.023 (3)0.001 (3)0.002 (3)0.001 (2)
O20.039 (3)0.019 (3)0.024 (3)0.003 (3)0.000 (3)0.005 (2)
C10.038 (5)0.016 (4)0.036 (5)0.000 (4)0.003 (4)0.009 (4)
C20.026 (4)0.027 (4)0.031 (5)0.002 (4)0.001 (4)0.002 (4)
C30.025 (5)0.036 (5)0.057 (7)0.000 (4)0.006 (4)0.014 (5)
C40.031 (5)0.032 (5)0.060 (8)0.006 (4)0.013 (5)0.021 (5)
C50.046 (6)0.040 (6)0.044 (7)0.013 (5)0.012 (5)0.007 (5)
C60.037 (5)0.034 (6)0.034 (6)0.006 (4)0.005 (4)0.001 (4)
C70.027 (5)0.020 (4)0.025 (5)0.003 (3)0.008 (4)0.003 (3)
C80.032 (5)0.021 (4)0.047 (6)0.002 (4)0.006 (4)0.001 (4)
C90.053 (7)0.025 (5)0.043 (7)0.003 (4)0.005 (5)0.012 (4)
C100.049 (7)0.031 (5)0.056 (8)0.019 (5)0.005 (6)0.005 (5)
C110.036 (6)0.043 (6)0.063 (8)0.018 (5)0.005 (5)0.005 (5)
C120.034 (5)0.031 (5)0.040 (6)0.003 (4)0.006 (5)0.007 (4)
C130.023 (4)0.019 (4)0.024 (5)0.000 (3)0.004 (4)0.001 (3)
C140.020 (4)0.024 (4)0.031 (5)0.004 (3)0.001 (4)0.005 (4)
C150.027 (5)0.032 (5)0.029 (6)0.008 (4)0.000 (4)0.003 (4)
C160.028 (5)0.028 (5)0.038 (6)0.010 (4)0.006 (4)0.000 (4)
C170.036 (6)0.027 (5)0.033 (6)0.001 (4)0.002 (5)0.003 (4)
C180.026 (5)0.031 (5)0.025 (5)0.002 (4)0.006 (4)0.001 (4)
C190.020 (4)0.023 (4)0.030 (6)0.002 (3)0.001 (4)0.008 (4)
C200.048 (6)0.033 (5)0.024 (5)0.007 (5)0.001 (4)0.003 (4)
C210.059 (7)0.024 (5)0.028 (6)0.015 (4)0.009 (5)0.003 (4)
C220.036 (5)0.024 (5)0.047 (7)0.009 (4)0.012 (5)0.000 (4)
C230.027 (5)0.031 (5)0.046 (7)0.011 (4)0.008 (4)0.008 (4)
C240.028 (5)0.030 (5)0.032 (6)0.000 (4)0.003 (4)0.005 (4)
C250.035 (5)0.016 (4)0.022 (5)0.003 (3)0.004 (4)0.003 (3)
C260.027 (5)0.029 (5)0.027 (5)0.001 (4)0.001 (4)0.001 (4)
C270.029 (5)0.039 (5)0.034 (6)0.002 (4)0.009 (4)0.004 (4)
C280.022 (4)0.034 (5)0.040 (6)0.000 (4)0.001 (4)0.005 (4)
C290.031 (5)0.033 (5)0.032 (6)0.008 (4)0.007 (4)0.001 (4)
C300.027 (5)0.022 (4)0.027 (5)0.003 (3)0.001 (4)0.001 (4)
C310.026 (5)0.019 (4)0.023 (5)0.005 (3)0.004 (4)0.001 (3)
C320.032 (5)0.021 (5)0.038 (6)0.006 (4)0.000 (4)0.001 (4)
C330.028 (5)0.031 (5)0.034 (6)0.000 (4)0.001 (4)0.002 (4)
C340.036 (5)0.022 (4)0.042 (6)0.009 (4)0.008 (4)0.001 (4)
C350.034 (5)0.017 (4)0.054 (7)0.003 (4)0.003 (5)0.005 (4)
C360.024 (5)0.032 (5)0.038 (6)0.001 (4)0.003 (4)0.004 (4)
C370.040 (6)0.041 (5)0.033 (6)0.008 (4)0.004 (4)0.012 (4)
C380.036 (6)0.043 (6)0.035 (6)0.004 (5)0.004 (4)0.011 (5)
Geometric parameters (Å, º) top
Pb1—C72.199 (4)C16—H160.9500
Pb1—C132.210 (4)C17—C181.3900
Pb1—C12.219 (4)C17—H170.9500
Pb1—O22.323 (6)C18—H180.9500
Pb1—Cl12.782 (2)C19—C201.3900
Pb2—C312.198 (4)C19—C241.3900
Pb2—C252.205 (4)C20—C211.3900
Pb2—C192.224 (4)C20—H200.9500
Pb2—O1i2.248 (6)C21—C221.3900
Pb2—Cl12.963 (2)C21—H210.9500
As1—O11.670 (6)C22—C231.3900
As1—O21.672 (5)C22—H220.9500
As1—C381.898 (10)C23—C241.3900
As1—C371.918 (9)C23—H230.9500
O1—Pb2ii2.248 (6)C24—H240.9500
C1—C21.3900C25—C261.3900
C1—C61.3900C25—C301.3900
C2—C31.3900C26—C271.3900
C2—H20.9500C26—H260.9500
C3—C41.3900C27—C281.3900
C3—H30.9500C27—H270.9500
C4—C51.3900C28—C291.3900
C4—H40.9500C28—H280.9500
C5—C61.3900C29—C301.3900
C5—H50.9500C29—H290.9500
C6—H60.9500C30—H300.9500
C7—C81.3900C31—C321.3900
C7—C121.3900C31—C361.3900
C8—C91.3900C32—C331.3900
C8—H80.9500C32—H320.9500
C9—C101.3900C33—C341.3900
C9—H90.9500C33—H330.9500
C10—C111.3900C34—C351.3900
C10—H100.9500C34—H340.9500
C11—C121.3900C35—C361.3900
C11—H110.9500C35—H350.9500
C12—H120.9500C36—H360.9500
C13—C141.3900C37—H37A0.9800
C13—C181.3900C37—H37B0.9800
C14—C151.3900C37—H37C0.9800
C14—H140.9500C38—H38A0.9800
C15—C161.3900C38—H38B0.9800
C15—H150.9500C38—H38C0.9800
C16—C171.3900
C7—Pb1—C13117.8 (2)C17—C16—H16120.0
C7—Pb1—C1124.0 (2)C15—C16—H16120.0
C13—Pb1—C1118.2 (2)C18—C17—C16120.0
C7—Pb1—O287.8 (2)C18—C17—H17120.0
C13—Pb1—O288.86 (19)C16—C17—H17120.0
C1—Pb1—O292.9 (2)C17—C18—C13120.0
C7—Pb1—Cl188.44 (17)C17—C18—H18120.0
C13—Pb1—Cl192.05 (14)C13—C18—H18120.0
C1—Pb1—Cl189.98 (15)C20—C19—C24120.0
O2—Pb1—Cl1176.11 (16)C20—C19—Pb2120.4 (3)
C31—Pb2—C25122.3 (2)C24—C19—Pb2119.6 (3)
C31—Pb2—C19110.9 (2)C19—C20—C21120.0
C25—Pb2—C19125.5 (2)C19—C20—H20120.0
C31—Pb2—O1i97.8 (2)C21—C20—H20120.0
C25—Pb2—O1i88.3 (2)C20—C21—C22120.0
C19—Pb2—O1i95.7 (2)C20—C21—H21120.0
C31—Pb2—Cl183.49 (18)C22—C21—H21120.0
C25—Pb2—Cl189.22 (14)C23—C22—C21120.0
C19—Pb2—Cl185.75 (15)C23—C22—H22120.0
O1i—Pb2—Cl1177.54 (17)C21—C22—H22120.0
O1—As1—O2110.4 (3)C22—C23—C24120.0
O1—As1—C38109.9 (4)C22—C23—H23120.0
O2—As1—C38108.9 (4)C24—C23—H23120.0
O1—As1—C37107.2 (4)C23—C24—C19120.0
O2—As1—C37113.0 (4)C23—C24—H24120.0
C38—As1—C37107.5 (5)C19—C24—H24120.0
Pb1—Cl1—Pb2167.35 (9)C26—C25—C30120.0
As1—O1—Pb2ii137.8 (4)C26—C25—Pb2119.4 (3)
As1—O2—Pb1132.9 (3)C30—C25—Pb2120.6 (3)
C2—C1—C6120.0C27—C26—C25120.0
C2—C1—Pb1121.9 (3)C27—C26—H26120.0
C6—C1—Pb1118.1 (3)C25—C26—H26120.0
C3—C2—C1120.0C28—C27—C26120.0
C3—C2—H2120.0C28—C27—H27120.0
C1—C2—H2120.0C26—C27—H27120.0
C2—C3—C4120.0C27—C28—C29120.0
C2—C3—H3120.0C27—C28—H28120.0
C4—C3—H3120.0C29—C28—H28120.0
C5—C4—C3120.0C30—C29—C28120.0
C5—C4—H4120.0C30—C29—H29120.0
C3—C4—H4120.0C28—C29—H29120.0
C6—C5—C4120.0C29—C30—C25120.0
C6—C5—H5120.0C29—C30—H30120.0
C4—C5—H5120.0C25—C30—H30120.0
C5—C6—C1120.0C32—C31—C36120.0
C5—C6—H6120.0C32—C31—Pb2116.9 (3)
C1—C6—H6120.0C36—C31—Pb2123.1 (3)
C8—C7—C12120.0C31—C32—C33120.0
C8—C7—Pb1121.6 (3)C31—C32—H32120.0
C12—C7—Pb1117.9 (3)C33—C32—H32120.0
C9—C8—C7120.0C32—C33—C34120.0
C9—C8—H8120.0C32—C33—H33120.0
C7—C8—H8120.0C34—C33—H33120.0
C8—C9—C10120.0C35—C34—C33120.0
C8—C9—H9120.0C35—C34—H34120.0
C10—C9—H9120.0C33—C34—H34120.0
C11—C10—C9120.0C34—C35—C36120.0
C11—C10—H10120.0C34—C35—H35120.0
C9—C10—H10120.0C36—C35—H35120.0
C12—C11—C10120.0C35—C36—C31120.0
C12—C11—H11120.0C35—C36—H36120.0
C10—C11—H11120.0C31—C36—H36120.0
C11—C12—C7120.0As1—C37—H37A109.5
C11—C12—H12120.0As1—C37—H37B109.5
C7—C12—H12120.0H37A—C37—H37B109.5
C14—C13—C18120.0As1—C37—H37C109.5
C14—C13—Pb1118.5 (3)H37A—C37—H37C109.5
C18—C13—Pb1121.5 (3)H37B—C37—H37C109.5
C13—C14—C15120.0As1—C38—H38A109.5
C13—C14—H14120.0As1—C38—H38B109.5
C15—C14—H14120.0H38A—C38—H38B109.5
C16—C15—C14120.0As1—C38—H38C109.5
C16—C15—H15120.0H38A—C38—H38C109.5
C14—C15—H15120.0H38B—C38—H38C109.5
C17—C16—C15120.0
Symmetry codes: (i) x, y+1/2, z+1/2; (ii) x, y+1/2, z1/2.
Poly[chlorido(µ3-dimethylarsinato-κ3O:O,O':O')diphenyllead(IV)] (2) top
Crystal data top
[Pb(C6H5)2(C2H6AsO2)Cl]F(000) = 992
Mr = 533.83Dx = 2.375 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 7.3822 (3) ÅCell parameters from 14717 reflections
b = 19.9500 (7) Åθ = 2.0–27.2°
c = 10.2878 (4) ŵ = 13.67 mm1
β = 99.763 (3)°T = 100 K
V = 1493.19 (10) Å3Needle, colourless
Z = 40.26 × 0.03 × 0.03 mm
Data collection top
Stoe IPDS/2T
diffractometer
2934 independent reflections
Radiation source: fine-focus sealed tube2116 reflections with I > 2σ(I)
Detector resolution: 6.7 pixels mm-1Rint = 0.094
ω–scansθmax = 26.0°, θmin = 2.3°
Absorption correction: gaussian
(Coppens et al., 1965)
h = 99
Tmin = 0.183, Tmax = 0.727k = 2424
21245 measured reflectionsl = 1212
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.032H-atom parameters constrained
wR(F2) = 0.067 w = 1/[σ2(Fo2) + (0.030P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.96(Δ/σ)max < 0.001
2934 reflectionsΔρmax = 1.60 e Å3
173 parametersΔρmin = 1.43 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.00158 (14)
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pb10.72935 (3)0.01889 (2)0.39198 (3)0.02132 (11)
Cl10.6838 (2)0.06690 (10)0.14258 (19)0.0276 (4)
As10.80432 (8)0.02385 (4)0.71823 (7)0.02082 (17)
O10.9474 (6)0.0265 (3)0.6067 (5)0.0233 (11)
O20.6000 (6)0.0103 (3)0.6226 (5)0.0254 (12)
C10.7357 (9)0.1241 (3)0.4576 (7)0.0196 (15)
C20.6534 (9)0.1432 (4)0.5607 (8)0.0256 (17)
H20.59200.11120.60610.031*
C30.6607 (10)0.2101 (4)0.5982 (9)0.0303 (19)
H30.60470.22410.67030.036*
C40.7498 (10)0.2567 (4)0.5307 (8)0.0295 (19)
H40.75600.30230.55740.035*
C50.8295 (10)0.2366 (4)0.4244 (9)0.0294 (18)
H50.88860.26870.37770.035*
C60.8233 (10)0.1696 (4)0.3858 (8)0.0245 (17)
H60.87700.15530.31290.029*
C70.7202 (9)0.0825 (4)0.3123 (8)0.0220 (16)
C80.6264 (9)0.0917 (4)0.1841 (8)0.0233 (16)
H80.56360.05540.13650.028*
C90.6262 (10)0.1551 (4)0.1269 (9)0.0288 (18)
H90.56570.16190.03880.035*
C100.7132 (10)0.2074 (4)0.1978 (9)0.032 (2)
H100.71150.25060.15870.038*
C110.8025 (10)0.1982 (4)0.3244 (10)0.034 (2)
H110.86210.23520.37200.041*
C120.8073 (10)0.1359 (4)0.3841 (9)0.0269 (18)
H120.86880.12980.47210.032*
C130.8766 (10)0.0463 (4)0.8386 (9)0.032 (2)
H13A0.99640.03570.89160.048*
H13B0.78520.05160.89670.048*
H13C0.88580.08810.79010.048*
C140.8019 (10)0.1056 (5)0.8132 (9)0.0326 (19)
H14A0.92220.11260.86840.049*
H14B0.77510.14290.75090.049*
H14C0.70710.10340.86920.049*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pb10.01614 (13)0.02184 (15)0.02556 (16)0.00021 (13)0.00230 (9)0.00146 (16)
Cl10.0293 (9)0.0273 (10)0.0250 (10)0.0023 (8)0.0017 (8)0.0001 (8)
As10.0145 (3)0.0260 (4)0.0216 (4)0.0001 (3)0.0019 (3)0.0008 (4)
O10.013 (2)0.031 (3)0.025 (3)0.002 (2)0.0040 (18)0.005 (3)
O20.009 (2)0.031 (3)0.034 (3)0.001 (2)0.0024 (19)0.003 (3)
C10.022 (3)0.014 (3)0.022 (4)0.001 (3)0.000 (3)0.010 (3)
C20.018 (3)0.023 (4)0.035 (5)0.004 (3)0.004 (3)0.009 (4)
C30.021 (4)0.035 (5)0.035 (5)0.003 (3)0.002 (3)0.005 (4)
C40.025 (4)0.023 (4)0.037 (5)0.003 (3)0.004 (3)0.007 (4)
C50.027 (4)0.028 (4)0.033 (5)0.000 (3)0.003 (3)0.003 (4)
C60.025 (4)0.023 (4)0.025 (4)0.003 (3)0.001 (3)0.003 (3)
C70.017 (3)0.015 (4)0.032 (5)0.002 (3)0.002 (3)0.000 (3)
C80.024 (3)0.025 (4)0.022 (4)0.005 (3)0.006 (3)0.003 (3)
C90.025 (4)0.030 (4)0.031 (5)0.005 (3)0.003 (3)0.002 (4)
C100.025 (4)0.025 (4)0.044 (5)0.001 (3)0.000 (4)0.011 (4)
C110.024 (4)0.024 (4)0.051 (6)0.004 (3)0.000 (4)0.005 (4)
C120.019 (3)0.031 (4)0.029 (5)0.002 (3)0.003 (3)0.001 (4)
C130.018 (3)0.038 (5)0.041 (5)0.007 (3)0.006 (3)0.001 (4)
C140.023 (4)0.038 (5)0.037 (5)0.000 (3)0.007 (3)0.002 (4)
Geometric parameters (Å, º) top
Pb1—C72.180 (7)C5—C61.392 (11)
Pb1—C12.202 (7)C5—H50.9500
Pb1—O1i2.389 (4)C6—H60.9500
Pb1—O2ii2.416 (4)C7—C121.390 (11)
Pb1—O12.662 (5)C7—C81.394 (11)
Pb1—Cl12.706 (2)C8—C91.394 (11)
As1—O21.678 (4)C8—H80.9500
As1—O11.687 (5)C9—C101.370 (12)
As1—C131.885 (9)C9—H90.9500
As1—C141.902 (9)C10—C111.368 (12)
O1—Pb1i2.389 (4)C10—H100.9500
O2—Pb1ii2.416 (4)C11—C121.385 (11)
C1—C21.363 (11)C11—H110.9500
C1—C61.396 (11)C12—H120.9500
C2—C31.389 (11)C13—H13A0.9800
C2—H20.9500C13—H13B0.9800
C3—C41.390 (12)C13—H13C0.9800
C3—H30.9500C14—H14A0.9800
C4—C51.386 (12)C14—H14B0.9800
C4—H40.9500C14—H14C0.9800
C7—Pb1—C1175.8 (3)C4—C5—C6120.3 (8)
C7—Pb1—O1i91.6 (2)C4—C5—H5119.8
C1—Pb1—O1i88.2 (2)C6—C5—H5119.8
C7—Pb1—O2ii86.8 (2)C5—C6—C1118.0 (7)
C1—Pb1—O2ii93.2 (2)C5—C6—H6121.0
O1i—Pb1—O2ii176.80 (18)C1—C6—H6121.0
C7—Pb1—O188.4 (2)C12—C7—C8120.9 (7)
C1—Pb1—O195.3 (2)C12—C7—Pb1122.0 (6)
O1i—Pb1—O163.51 (19)C8—C7—Pb1117.2 (5)
O2ii—Pb1—O1119.20 (16)C7—C8—C9118.9 (7)
C7—Pb1—Cl188.9 (2)C7—C8—H8120.5
C1—Pb1—Cl186.9 (2)C9—C8—H8120.5
O1i—Pb1—Cl186.92 (13)C10—C9—C8120.0 (8)
O2ii—Pb1—Cl190.25 (13)C10—C9—H9120.0
O1—Pb1—Cl1150.20 (10)C8—C9—H9120.0
O2—As1—O1102.1 (2)C11—C10—C9120.7 (8)
O2—As1—C13113.1 (3)C11—C10—H10119.6
O1—As1—C13109.3 (3)C9—C10—H10119.6
O2—As1—C14110.7 (3)C10—C11—C12121.0 (8)
O1—As1—C14112.6 (3)C10—C11—H11119.5
C13—As1—C14109.0 (4)C12—C11—H11119.5
As1—O1—Pb1i137.2 (3)C11—C12—C7118.5 (8)
As1—O1—Pb1101.16 (19)C11—C12—H12120.7
Pb1i—O1—Pb1116.49 (19)C7—C12—H12120.7
As1—O2—Pb1ii145.1 (3)As1—C13—H13A109.5
C2—C1—C6122.5 (7)As1—C13—H13B109.5
C2—C1—Pb1121.0 (6)H13A—C13—H13B109.5
C6—C1—Pb1116.5 (5)As1—C13—H13C109.5
C1—C2—C3118.9 (8)H13A—C13—H13C109.5
C1—C2—H2120.5H13B—C13—H13C109.5
C3—C2—H2120.5As1—C14—H14A109.5
C2—C3—C4120.2 (8)As1—C14—H14B109.5
C2—C3—H3119.9H14A—C14—H14B109.5
C4—C3—H3119.9As1—C14—H14C109.5
C5—C4—C3120.1 (8)H14A—C14—H14C109.5
C5—C4—H4120.0H14B—C14—H14C109.5
C3—C4—H4120.0
Symmetry codes: (i) x+2, y, z+1; (ii) x+1, y, z+1.
catena-Poly[[triphenyllead(IV)]-µ-diphenylphosphinato-κ2O:O'] (3) top
Crystal data top
[Pb(C6H5)3(C12H10O2P)]F(000) = 1272
Mr = 655.66Dx = 1.740 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 13.8277 (8) ÅCell parameters from 22205 reflections
b = 12.6242 (6) Åθ = 1.9–27.1°
c = 14.4713 (8) ŵ = 6.83 mm1
β = 97.717 (5)°T = 100 K
V = 2503.3 (2) Å3Needle, colourless
Z = 40.11 × 0.04 × 0.02 mm
Data collection top
Stoe IPDS/2T
diffractometer
5316 independent reflections
Radiation source: fine-focus sealed tube3301 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.095
Detector resolution: 6.7 pixels mm-1θmax = 26.9°, θmin = 1.9°
ω scansh = 1717
Absorption correction: gaussian
(Coppens et al., 1965)
k = 1515
Tmin = 0.376, Tmax = 0.917l = 1818
18698 measured reflections
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)] = 0.045Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.101H-atom parameters constrained
S = 0.91 w = 1/[σ2(Fo2) + (0.040P)2]
where P = (Fo2 + 2Fc2)/3
5316 reflections(Δ/σ)max = 0.001
223 parametersΔρmax = 2.58 e Å3
2 restraintsΔρmin = 2.17 e Å3
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. All phenyl rings refined using geometrical constraints (AFIX 66). Rotationally Disordered phenyl ring (C13—C18) refined with equal anisotropic displacement parameters for neighboring atoms. The occupations of both orientations were set 50:50% since refinement confirmed this ratio within the 3\s limit.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Pb10.22665 (2)0.84365 (2)0.19550 (2)0.03541 (10)
P10.15953 (16)0.60620 (16)0.31759 (15)0.0343 (5)
O10.1699 (4)0.6709 (4)0.2329 (4)0.0392 (13)
O20.2323 (4)0.5195 (4)0.3428 (4)0.0399 (14)
C10.2631 (4)0.7809 (4)0.0635 (3)0.038 (2)
C20.2790 (4)0.8476 (3)0.0093 (3)0.0361 (18)
H20.27000.92190.00390.043*
C30.3081 (4)0.8058 (4)0.0901 (3)0.043 (2)
H30.31890.85150.13980.052*
C40.3213 (4)0.6972 (4)0.0980 (3)0.049 (2)
H40.34110.66860.15320.059*
C50.3054 (4)0.6304 (3)0.0252 (4)0.050 (2)
H50.31440.55620.03060.060*
C60.2763 (4)0.6722 (4)0.0556 (3)0.042 (2)
H60.26550.62660.10540.050*
C70.3428 (4)0.8381 (4)0.3127 (3)0.0362 (18)
C80.4179 (5)0.7649 (5)0.3124 (4)0.060 (3)
H80.41770.71720.26160.072*
C90.4932 (4)0.7617 (5)0.3863 (5)0.075 (4)
H90.54460.71170.38600.090*
C100.4935 (4)0.8316 (6)0.4605 (4)0.062 (3)
H100.54510.82940.51100.074*
C110.4185 (4)0.9047 (5)0.4609 (3)0.052 (3)
H110.41870.95250.51160.062*
C120.3431 (4)0.9080 (4)0.3870 (4)0.039 (2)
H120.29180.95800.38730.046*
C13A0.0824 (5)0.9098 (10)0.2076 (9)0.039 (2)*0.5
C14A0.0753 (5)0.9735 (10)0.2848 (8)0.044 (3)*0.5
H14A0.13010.98190.33140.053*0.5
C15A0.0118 (7)1.0250 (9)0.2937 (7)0.044 (3)*0.5
H15A0.01661.06860.34640.053*0.5
C16A0.0919 (5)1.0127 (9)0.2255 (8)0.041 (3)*0.5
H16A0.15151.04790.23160.049*0.5
C17A0.0849 (6)0.9490 (9)0.1484 (7)0.044 (3)*0.5
H17A0.13960.94060.10170.053*0.5
C18A0.0022 (7)0.8975 (9)0.1394 (7)0.047 (3)*0.5
H18A0.00700.85400.08670.057*0.5
C13B0.0852 (5)0.9165 (10)0.1989 (9)0.039 (2)*0.5
C14B0.0516 (7)0.9464 (10)0.2814 (7)0.044 (3)*0.5
H14B0.08940.93130.33970.053*0.5
C15B0.0374 (7)0.9983 (9)0.2786 (6)0.044 (3)*0.5
H15B0.06041.01870.33500.053*0.5
C16B0.0927 (5)1.0204 (9)0.1934 (8)0.041 (3)*0.5
H16B0.15351.05590.19150.049*0.5
C17B0.0591 (7)0.9906 (9)0.1109 (6)0.044 (3)*0.5
H17B0.09691.00570.05260.053*0.5
C18B0.0299 (7)0.9387 (9)0.1137 (7)0.047 (3)*0.5
H18B0.05290.91830.05730.057*0.5
C190.0383 (3)0.5496 (4)0.3019 (4)0.0343 (18)
C200.0121 (4)0.4842 (4)0.3718 (3)0.039 (2)
H200.05560.47470.42790.047*
C210.0776 (4)0.4328 (4)0.3597 (4)0.050 (2)
H210.09540.38820.40740.060*
C220.1411 (3)0.4467 (5)0.2776 (4)0.051 (2)
H220.20240.41160.26940.061*
C230.1150 (4)0.5120 (5)0.2077 (3)0.052 (3)
H230.15840.52150.15170.063*
C240.0253 (4)0.5635 (4)0.2199 (3)0.043 (2)
H240.00740.60810.17210.051*
C250.1655 (4)0.6902 (4)0.4197 (3)0.036 (2)
C260.2498 (3)0.6920 (4)0.4838 (4)0.043 (2)
H260.30420.64950.47400.052*
C270.2547 (3)0.7561 (5)0.5624 (3)0.043 (2)
H270.31240.75740.60620.052*
C280.1752 (4)0.8184 (4)0.5768 (3)0.047 (2)
H280.17850.86220.63050.056*
C290.0908 (4)0.8165 (4)0.5127 (4)0.066 (3)
H290.03650.85910.52260.080*
C300.0860 (3)0.7524 (4)0.4341 (4)0.056 (3)
H300.02830.75110.39030.067*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pb10.04572 (18)0.02277 (13)0.03683 (16)0.00280 (18)0.00222 (11)0.00012 (17)
P10.0372 (12)0.0240 (10)0.0412 (12)0.0009 (9)0.0034 (10)0.0032 (9)
O10.049 (3)0.024 (3)0.047 (3)0.002 (3)0.017 (3)0.007 (3)
O20.043 (3)0.020 (3)0.056 (4)0.002 (2)0.002 (3)0.000 (3)
C10.042 (5)0.025 (4)0.045 (5)0.002 (4)0.004 (4)0.002 (4)
C20.039 (4)0.028 (4)0.040 (4)0.005 (4)0.002 (3)0.005 (4)
C30.046 (5)0.042 (5)0.041 (5)0.004 (4)0.005 (4)0.010 (4)
C40.046 (5)0.051 (5)0.048 (5)0.003 (5)0.000 (4)0.014 (5)
C50.055 (6)0.033 (5)0.063 (6)0.007 (4)0.012 (5)0.010 (4)
C60.058 (5)0.031 (5)0.038 (4)0.003 (4)0.012 (4)0.001 (4)
C70.040 (4)0.030 (4)0.035 (4)0.003 (4)0.005 (3)0.004 (4)
C80.063 (7)0.062 (6)0.055 (6)0.034 (5)0.010 (5)0.000 (5)
C90.064 (7)0.091 (9)0.066 (7)0.040 (7)0.003 (6)0.019 (7)
C100.047 (6)0.083 (8)0.052 (6)0.009 (6)0.007 (5)0.021 (6)
C110.048 (6)0.063 (6)0.041 (5)0.008 (5)0.006 (4)0.005 (5)
C120.033 (5)0.039 (5)0.042 (5)0.004 (4)0.002 (4)0.010 (4)
C190.039 (5)0.028 (4)0.036 (4)0.003 (4)0.004 (4)0.001 (3)
C200.042 (5)0.032 (4)0.044 (5)0.004 (4)0.006 (4)0.002 (4)
C210.058 (6)0.034 (5)0.056 (6)0.008 (4)0.005 (5)0.004 (4)
C220.038 (5)0.048 (6)0.067 (6)0.009 (4)0.008 (5)0.018 (5)
C230.044 (6)0.062 (6)0.050 (6)0.003 (5)0.001 (4)0.012 (5)
C240.041 (5)0.044 (5)0.043 (5)0.006 (4)0.006 (4)0.001 (4)
C250.040 (5)0.028 (4)0.038 (4)0.004 (3)0.007 (4)0.005 (3)
C260.041 (5)0.050 (5)0.038 (5)0.002 (4)0.002 (4)0.007 (4)
C270.043 (5)0.049 (5)0.035 (5)0.006 (4)0.002 (4)0.005 (4)
C280.055 (6)0.036 (5)0.046 (5)0.002 (4)0.003 (4)0.010 (4)
C290.060 (6)0.048 (6)0.085 (8)0.020 (5)0.014 (6)0.023 (5)
C300.056 (6)0.027 (4)0.078 (7)0.006 (4)0.011 (5)0.015 (5)
Geometric parameters (Å, º) top
Pb1—C72.175 (4)C16A—C17A1.3900
Pb1—C13B2.168 (4)C16A—H16A0.9500
Pb1—C13A2.192 (4)C17A—C18A1.3900
Pb1—C12.189 (4)C17A—H17A0.9500
Pb1—O2i2.375 (5)C18A—H18A0.9500
Pb1—O12.404 (5)C13B—C14B1.3900
P1—O11.496 (6)C13B—C18B1.3900
P1—O21.499 (5)C14B—C15B1.3900
P1—C191.809 (4)C14B—H14B0.9500
P1—C251.811 (4)C15B—C16B1.3900
O2—Pb1ii2.375 (5)C15B—H15B0.9500
C1—C21.3900C16B—C17B1.3900
C1—C61.3900C16B—H16B0.9500
C2—C31.3900C17B—C18B1.3900
C2—H20.9500C17B—H17B0.9500
C3—C41.3900C18B—H18B0.9500
C3—H30.9500C19—C201.3900
C4—C51.3900C19—C241.3900
C4—H40.9500C20—C211.3900
C5—C61.3900C20—H200.9500
C5—H50.9500C21—C221.3900
C6—H60.9500C21—H210.9500
C7—C81.3900C22—C231.3900
C7—C121.3900C22—H220.9500
C8—C91.3900C23—C241.3900
C8—H80.9500C23—H230.9500
C9—C101.3900C24—H240.9500
C9—H90.9500C25—C261.3900
C10—C111.3900C25—C301.3900
C10—H100.9500C26—C271.3900
C11—C121.3900C26—H260.9500
C11—H110.9500C27—C281.3900
C12—H120.9500C27—H270.9500
C13A—C14A1.3900C28—C291.3900
C13A—C18A1.3900C28—H280.9500
C14A—C15A1.3900C29—C301.3900
C14A—H14A0.9500C29—H290.9500
C15A—C16A1.3900C30—H300.9500
C15A—H15A0.9500
C7—Pb1—C13B124.7 (4)C16A—C15A—H15A120.0
C7—Pb1—C13A122.3 (4)C14A—C15A—H15A120.0
C7—Pb1—C1115.9 (2)C15A—C16A—C17A120.0
C13B—Pb1—C1119.2 (4)C15A—C16A—H16A120.0
C13A—Pb1—C1121.8 (4)C17A—C16A—H16A120.0
C7—Pb1—O2i92.2 (2)C18A—C17A—C16A120.0
C13B—Pb1—O2i81.6 (4)C18A—C17A—H17A120.0
C13A—Pb1—O2i84.9 (4)C16A—C17A—H17A120.0
C1—Pb1—O2i92.54 (19)C17A—C18A—C13A120.0
C7—Pb1—O191.4 (2)C17A—C18A—H18A120.0
C13B—Pb1—O193.3 (4)C13A—C18A—H18A120.0
C13A—Pb1—O190.0 (4)C14B—C13B—C18B120.0
C1—Pb1—O189.31 (18)C14B—C13B—Pb1122.8 (6)
O2i—Pb1—O1174.82 (18)C18B—C13B—Pb1117.1 (6)
O1—P1—O2117.6 (4)C15B—C14B—C13B120.0
O1—P1—C19107.6 (3)C15B—C14B—H14B120.0
O2—P1—C19108.8 (3)C13B—C14B—H14B120.0
O1—P1—C25110.5 (3)C14B—C15B—C16B120.0
O2—P1—C25105.9 (3)C14B—C15B—H15B120.0
C19—P1—C25105.9 (3)C16B—C15B—H15B120.0
P1—O1—Pb1138.6 (3)C15B—C16B—C17B120.0
P1—O2—Pb1ii143.1 (3)C15B—C16B—H16B120.0
C2—C1—C6120.0C17B—C16B—H16B120.0
C2—C1—Pb1121.4 (3)C16B—C17B—C18B120.0
C6—C1—Pb1118.5 (3)C16B—C17B—H17B120.0
C1—C2—C3120.0C18B—C17B—H17B120.0
C1—C2—H2120.0C17B—C18B—C13B120.0
C3—C2—H2120.0C17B—C18B—H18B120.0
C4—C3—C2120.0C13B—C18B—H18B120.0
C4—C3—H3120.0C20—C19—C24120.0
C2—C3—H3120.0C20—C19—P1118.1 (3)
C5—C4—C3120.0C24—C19—P1121.8 (3)
C5—C4—H4120.0C21—C20—C19120.0
C3—C4—H4120.0C21—C20—H20120.0
C4—C5—C6120.0C19—C20—H20120.0
C4—C5—H5120.0C22—C21—C20120.0
C6—C5—H5120.0C22—C21—H21120.0
C5—C6—C1120.0C20—C21—H21120.0
C5—C6—H6120.0C23—C22—C21120.0
C1—C6—H6120.0C23—C22—H22120.0
C8—C7—C12120.0C21—C22—H22120.0
C8—C7—Pb1119.5 (3)C22—C23—C24120.0
C12—C7—Pb1120.5 (3)C22—C23—H23120.0
C7—C8—C9120.0C24—C23—H23120.0
C7—C8—H8120.0C23—C24—C19120.0
C9—C8—H8120.0C23—C24—H24120.0
C8—C9—C10120.0C19—C24—H24120.0
C8—C9—H9120.0C26—C25—C30120.0
C10—C9—H9120.0C26—C25—P1119.8 (3)
C11—C10—C9120.0C30—C25—P1120.2 (3)
C11—C10—H10120.0C25—C26—C27120.0
C9—C10—H10120.0C25—C26—H26120.0
C10—C11—C12120.0C27—C26—H26120.0
C10—C11—H11120.0C28—C27—C26120.0
C12—C11—H11120.0C28—C27—H27120.0
C11—C12—C7120.0C26—C27—H27120.0
C11—C12—H12120.0C29—C28—C27120.0
C7—C12—H12120.0C29—C28—H28120.0
C14A—C13A—C18A120.0C27—C28—H28120.0
C14A—C13A—Pb1116.6 (6)C30—C29—C28120.0
C18A—C13A—Pb1123.2 (6)C30—C29—H29120.0
C13A—C14A—C15A120.0C28—C29—H29120.0
C13A—C14A—H14A120.0C29—C30—C25120.0
C15A—C14A—H14A120.0C29—C30—H30120.0
C16A—C15A—C14A120.0C25—C30—H30120.0
Symmetry codes: (i) x+1/2, y+1/2, z+1/2; (ii) x+1/2, y1/2, z+1/2.
 

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