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In the title mononuclear lead silanethiol­ates, [Pb(C12H27O3SSi)2(C10H8N2)], (I), and [Pb(C12H27O3SSi)2(C24H16N2)]·0.5C6H6, (II), the Pb atom shows a distorted square-pyramidal coordination with a PbON2S2 core in which one S atom lies in an axial position. Inter­molecular π–π and C—H...π inter­actions stabilize the structures. The benzene solvent mol­ecule in (II) lies on an inversion centre.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270107029629/bg3039sup1.cif
Contains datablocks I, II, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270107029629/bg3039Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270107029629/bg3039IIsup3.hkl
Contains datablock II

CCDC references: 659106; 659107

Comment top

The present study is a continuation of our investigation of silanethiolate complexes of various metals (see, for example, Kloskowska et al., 2006). The compounds often show interesting structural features and are potential precursors for the generation of structurized metal sulfides (Tran et al., 2000). Only three structures containing an Si–S–Pb sequence can be found in the Cambrigde Structural Database (CSD; Version 5.28, May 2007 update; Allen, 2002). The dimeric lead tri-tert-butoxysilanetiolate, in the form of the diglyme solvate, was obtained by reaction of silanethiol with PbO (Wojnowski et al., 1986). Another complex, Pb{SSi(OC4H9)3}2N2C12H8, (ortho-phenanthroline)bis(tri-tert-butoxysilanethiolato)lead(II), mononuclear and heteroleptic, was obtained about ten years later by incorporation of a chelating N-ligand (Peters et al., 1997). Finally, a metallorganic compound, namely a plumbolane (2,2,3,3-tetramethyl-5,5-diphenyl-1,4,2,3,5-dithiadisilaplumbolane), was reported (Herzog & Rheinwald, 2002). Several attempts to obtain and characterize heteroleptic silanethiolates with PPh3 or simple heteroaromatic nitrogen bases as additional ligands have failed so far. Here, we present the syntheses and structures of two mononuclear complexes, namely (2,2'-bipyridine)bis(tri-tert-butoxysilanethiolato)lead(II), (I), and (4,7-diphenyl-1,10-phenanthroline)bis(tri-tert-butoxysilanethiolato)lead(II) benzene hemisolvate, (II). To our knowledge, no lead complexes with this latter heterocyclic ligand have been structurally characterized by X-ray diffraction to date.

Both compounds show a distorted square-pyramidal coordination of the Pb atoms. The impact of the `inert pair effect' on the structure is clearly manifested. The base plane contains N, N, S and O atoms, whereas the second S atom, found in the apical position, belongs to the O,S-chelating tri-tert-butoxysilanethiolate ligand. A widening of the valence angles at the S atoms by ca 4° in the silanethiolate ligands not involved in chelation is observed in both structures (Tables 1 and 2). It is worth noting the influence of the steric effect of the S-atom lone pairs on the coordination of sulfur. In (I), the Pb—N bond lengths differ, although the difference is small. This is not the case in (II), where Pb—N2 is about 0.2 Å longer than Pb—N1. The Si—S bond lengths are shorter and Pb—S distinctly longer compared with the respective bonds in the plumbolane (Si—S ca 2.14 and Pb—S ca 2.50 Å). This probably indicates a partially ionic character of the metal–ligand bonds in (I) and (II) (Baranowska et al., 2006). The Si2—O4 bond length is slightly longer than the other Si—O bonds in (I), due to chelation; this effect was noted previously by Jesionka et al. (2005). In (II), the situation is complicated by disorder.

In structure (I), the aromatic 2,2'-bipyridine rings of two neighbouring molecules are linked by a ππ interaction. Even if such an arrangement of heterocyclic rings is not possible in complex (II), due to the non-planar character of 4,7-diphenyl-1,10-phenanthroline, it is possible between the phenyl substituents of the heteroaromatic base. In addition to this, some C—H···π interactions complete the packing interaction scheme (Table 3).

The large dihedral angles between the phenanthroline residue and its phenyl substituents C37–C42 and C43–C48 [49.5 (2)° and 51.1 (2)°, respectively] indicate that π electrons in the phenanthroline group are not coupled with the phenyl substituents; the same behaviour (shown in Fig. 3, with data extracted from the CSD) has been observed in all 43 complexes of the 4,7-diphenyl-1,10-phenanthroline ligand known so far (for example, Brandi-Blanco et al., 2005).

The benzene solvate molecule in (II) sits on the inversion centre at (1/2, 1/2, 1/2), filling voids within the structure. Its linkage to the main frame is by way of a C—H···π interaction (final entry in Table 3).

Related literature top

For related literature, see: Allen (2002); Baranowska et al. (2006); Brandi-Blanco, Choquesillo-Lazarte, Gonzalez-Perez, Castineiras & Niclos-Gutierrez (2005); Herzog & Rheinwald (2002); Jesionka et al. (2005); Kloskowska et al. (2006); Perrin & Armarego (1988); Peters et al. (1997); Sheldrick (1997); Tran et al. (2000); Wojnowski et al. (1986).

Experimental top

All manipulations were carried out under an atmosphere of nitrogen using standard Schlenk techniques. The solvents were purified and dried by standard methods (Perrin & Armarego, 1988).

Compound (I) was prepared by the addition of [{(tBuO)3SiS}2Pb}2 (0.3 g, 0.20 mmol) (Wojnowski et al., 1986) dissolved in hexane–pentane (40:60 v/v) (25 ml) to a solution of 2,2'-bipyridine (130 mg, 0.83 mmol) in hexane–pentane (40:60 v/v) (5 ml). The mixture was shaken for a few minutes and subsequently left at ca 273 K for 15 h. The solid material was then filtered off, and the solution was concentrated to half its initial volume and left for crystallization at ca 273 K. After a week, good quality crystals of (I) (m.p. 433 K) were obtained in moderate yields (ca 50%, not optimized) with consistent elemental analyses for C, H, S and N.

Solid [{(tBuO)3SiS}2Pb}2 (0.3 g, 0.20 mmol) (Wojnowski et al., 1986) and 4,7-diphenyl-1,10-phenanthroline (bathophenanthroline) (250 mg, 0.40 mmol) were added to hexane (20 ml). The mixture was shaken for 10 min and subsequently left at ca 273 K for 5 h. The solid material was filtered off, and the solution was concentrated to form a raw product. Recrystallization from hexane–benzene (1:1 v/v) solution was carried out at ca 273 K. After a month, crystals of (II) (m.p. 440 K) separated (yield ca 40%, not optimized). Elemental analyses for C, H, S and N were consistent with the assumed formula.

Refinement top

All H atoms were refined as riding on their parent C atoms, with methyl C—H = 0.98 Å, methylene C—H = 0.99 Å and aromatic C—H = 0.95 Å, and with Uiso(H) = 1.2Ueq(C) for aromatic CH, 1.3Ueq(C) for CH2 groups and 1.5Ueq(C) for methyl groups. In the case of (II), elucidation of structure from diffraction data required special treatment. Two butoxy groups starting from O4 and O6 were refined as disordered over two positions with occupancies 0.714 (12) and 0.286 (12). Atoms C5–C8 and C10–C12 were refined with ISOR/SIMU instructions (SHELXL97; Sheldrick, 1997) simulating isotropic behaviour because of non-acceptable parameters of their ellipsoids. The highest electron-density peaks are located 0.78 Å from atom Pb1 in (I) and 0.86 Å from Pb1 in (II).

Computing details top

Data collection: CrysAlis CCD (Oxford Diffraction, 2006) for (I); KM4 System (Gałdecki, Kowalski et al., 1996) for (II). Cell refinement: CrysAlis RED (Oxford Diffraction, 2006) for (I); KM4 System for (II). Data reduction: CrysAlis RED for (I); DATAPROC (Gałdecki, Kowalski & Uszyński, 1996) for (II). For both compounds, program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: Mercury (Version 1.5; Macrae et al., 2006); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing the atom-numbering scheme and with displacement ellipsoids drawn at the 25% probability level. H atoms have been omitted.
[Figure 2] Fig. 2. The molecular structure of (II), showing the atom-numbering scheme and with displacement ellipsoids drawn at the 25% probability level. H atoms and the solvent benzene molecule have been omitted. Only the major part of the disordered group is shown.
[Figure 3] Fig. 3. Histogram of phenyl–heterocycle dihedral angles in 4,7-diphenyl-1,10-phenanthroline complexes currently (May 2007) deposited in the CSD.
(I) (2,2'-Bipyridine)bis(tri-tert-butoxysilanethiolato-κS)lead(II) top
Crystal data top
[Pb(C12H27O3SSi)2(C10H8N2)]Z = 2
Mr = 922.35F(000) = 940
Triclinic, P1Dx = 1.429 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 9.4053 (4) ÅCell parameters from 15949 reflections
b = 13.8617 (7) Åθ = 2.3–32.5°
c = 18.0405 (9) ŵ = 4.13 mm1
α = 107.361 (5)°T = 120 K
β = 99.069 (4)°Prism, colourless
γ = 101.086 (4)°0.49 × 0.13 × 0.09 mm
V = 2144.1 (2) Å3
Data collection top
Oxford Diffraction KM4 CCD
diffractometer
10174 independent reflections
Graphite monochromator9037 reflections with I > 2σ(I)
Detector resolution: 8.1883 pixels mm-1Rint = 0.030
0.75° ω scansθmax = 28°, θmin = 2.3°
Absorption correction: multi-scan
(CrysAlis RED; Oxford Diffraction, 2006)
h = 1212
Tmin = 0.503, Tmax = 0.695k = 1418
17997 measured reflectionsl = 2318
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)] = 0.040Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.099H-atom parameters constrained
S = 1.16 w = 1/[σ2(Fo2) + (0.050P)2 + 3.7754P]
where P = (Fo2 + 2Fc2)/3
10174 reflections(Δ/σ)max = 0.002
442 parametersΔρmax = 2.11 e Å3
0 restraintsΔρmin = 1.55 e Å3
Crystal data top
[Pb(C12H27O3SSi)2(C10H8N2)]γ = 101.086 (4)°
Mr = 922.35V = 2144.1 (2) Å3
Triclinic, P1Z = 2
a = 9.4053 (4) ÅMo Kα radiation
b = 13.8617 (7) ŵ = 4.13 mm1
c = 18.0405 (9) ÅT = 120 K
α = 107.361 (5)°0.49 × 0.13 × 0.09 mm
β = 99.069 (4)°
Data collection top
Oxford Diffraction KM4 CCD
diffractometer
10174 independent reflections
Absorption correction: multi-scan
(CrysAlis RED; Oxford Diffraction, 2006)
9037 reflections with I > 2σ(I)
Tmin = 0.503, Tmax = 0.695Rint = 0.030
17997 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0400 restraints
wR(F2) = 0.099H-atom parameters constrained
S = 1.16Δρmax = 2.11 e Å3
10174 reflectionsΔρmin = 1.55 e Å3
442 parameters
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. 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 > σ(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) top
xyzUiso*/Ueq
Pb10.315870 (19)0.972615 (13)0.206568 (9)0.02625 (6)
S10.01803 (14)0.91949 (10)0.19134 (8)0.0342 (2)
S20.28288 (14)1.14875 (9)0.18240 (6)0.0299 (2)
Si10.00171 (13)0.77880 (9)0.21186 (7)0.0238 (2)
Si20.38698 (13)1.24362 (9)0.29961 (7)0.0231 (2)
N10.2652 (6)0.8609 (3)0.0558 (2)0.0401 (10)
N20.5408 (5)0.9858 (4)0.1287 (2)0.0363 (9)
O10.1723 (3)0.7674 (2)0.22923 (19)0.0273 (6)
O20.0772 (4)0.7708 (3)0.28461 (19)0.0311 (7)
O30.0904 (3)0.6755 (3)0.13643 (19)0.0312 (7)
O40.4343 (3)1.1630 (2)0.34381 (18)0.0267 (6)
O50.2863 (3)1.3133 (2)0.34597 (19)0.0271 (6)
O60.5413 (3)1.3290 (2)0.31002 (19)0.0272 (6)
C10.2332 (5)0.6806 (4)0.2312 (3)0.0350 (10)
C20.1487 (7)0.6154 (5)0.2721 (5)0.064 (2)
H2A0.14840.660.32560.095*
H2B0.19710.560.27630.095*
H2C0.0460.5840.24080.095*
C30.2293 (7)0.6161 (5)0.1457 (4)0.0567 (17)
H3A0.12560.58520.11580.085*
H3B0.27940.56040.14610.085*
H3C0.28040.66130.12020.085*
C40.3942 (6)0.7295 (4)0.2785 (4)0.0423 (12)
H4A0.44820.76960.25060.063*
H4B0.4420.67420.28370.063*
H4C0.39570.77610.33170.063*
C50.0705 (6)0.8459 (4)0.3610 (3)0.0390 (11)
C60.1202 (9)0.7819 (6)0.4114 (4)0.0631 (19)
H6A0.2210.73740.38560.095*
H6B0.120.82880.46430.095*
H6C0.05180.73810.41710.095*
C70.1737 (6)0.9150 (5)0.3502 (4)0.0492 (14)
H7A0.13990.95430.31650.074*
H7B0.17280.96390.40240.074*
H7C0.27520.87150.32480.074*
C80.0906 (6)0.9113 (4)0.3989 (3)0.0423 (12)
H8A0.15550.86490.40320.063*
H8B0.09590.95940.45210.063*
H8C0.12320.95140.36540.063*
C90.2435 (5)0.6393 (4)0.0924 (3)0.0364 (11)
C100.3431 (7)0.6953 (8)0.1359 (5)0.079 (3)
H10A0.33730.68530.18780.119*
H10B0.44590.66720.10440.119*
H10C0.31120.770.14420.119*
C110.2871 (7)0.5221 (6)0.0779 (5)0.0629 (18)
H11A0.21740.48880.0510.094*
H11B0.38820.49160.04430.094*
H11C0.28370.51050.12910.094*
C120.2483 (7)0.6560 (5)0.0125 (4)0.0530 (15)
H12A0.2110.73050.02150.079*
H12B0.35110.63140.01920.079*
H12C0.18590.61670.01630.079*
C130.5357 (5)1.1818 (4)0.4188 (3)0.0275 (9)
C140.5280 (7)1.2801 (5)0.4819 (3)0.0435 (12)
H14A0.5581.34040.4650.065*
H14B0.59511.290.53250.065*
H14C0.42581.27350.48910.065*
C150.6912 (6)1.1897 (5)0.4041 (4)0.0438 (13)
H15A0.69411.12380.36520.066*
H15B0.76241.20380.45430.066*
H15C0.71761.24670.38310.066*
C160.4873 (7)1.0871 (4)0.4433 (3)0.0447 (13)
H16A0.38391.07930.44850.067*
H16B0.55161.09650.49460.067*
H16C0.49511.02440.40260.067*
C170.1334 (5)1.2939 (4)0.3517 (3)0.0305 (9)
C180.1303 (6)1.3742 (5)0.4301 (4)0.0465 (13)
H18A0.191.36230.47470.07*
H18B0.02741.36710.4360.07*
H18C0.17161.44470.43010.07*
C190.0417 (6)1.3097 (5)0.2811 (4)0.0489 (14)
H19A0.06881.38370.28610.073*
H19B0.06431.28840.28020.073*
H19C0.06151.26740.23150.073*
C200.0795 (6)1.1844 (4)0.3536 (3)0.0364 (11)
H20A0.08191.13320.30310.055*
H20B0.02261.17390.3610.055*
H20C0.14451.17540.39780.055*
C210.5669 (5)1.4307 (4)0.3021 (3)0.0300 (9)
C220.4719 (6)1.4256 (4)0.2237 (3)0.0394 (11)
H22A0.49521.37530.17910.059*
H22B0.49311.49480.21810.059*
H22C0.36641.40350.22340.059*
C230.5338 (6)1.5094 (4)0.3722 (3)0.0377 (11)
H23A0.42641.49340.36890.057*
H23B0.56771.580.37060.057*
H23C0.5861.50550.42230.057*
C240.7317 (6)1.4614 (5)0.3030 (4)0.0466 (14)
H24A0.79091.46330.35350.07*
H24B0.75681.53060.29770.07*
H24C0.75351.41010.25850.07*
C250.6736 (7)1.0520 (5)0.1650 (4)0.0494 (14)
H250.68521.10080.21670.059*
C260.7945 (7)1.0530 (6)0.1311 (5)0.062 (2)
H260.8881.10040.15950.075*
C270.7788 (8)0.9849 (7)0.0559 (5)0.062 (2)
H270.86070.98460.03120.075*
C280.6433 (8)0.9174 (6)0.0173 (4)0.0552 (18)
H280.62940.870.03530.066*
C290.5243 (6)0.9182 (4)0.0554 (3)0.0391 (12)
C300.3745 (7)0.8479 (4)0.0169 (3)0.0386 (12)
C310.1265 (9)0.8020 (6)0.0194 (3)0.064 (2)
H310.04950.81240.04690.076*
C320.0890 (11)0.7272 (6)0.0557 (4)0.077 (3)
H320.01120.68840.07980.092*
C330.2009 (12)0.7110 (6)0.0941 (4)0.078 (3)
H330.18040.65830.1450.094*
C340.3431 (10)0.7715 (6)0.0584 (4)0.064 (2)
H340.4210.76130.08530.077*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pb10.03536 (9)0.02262 (9)0.02095 (8)0.00824 (6)0.00767 (6)0.00648 (6)
S10.0363 (6)0.0318 (6)0.0379 (6)0.0131 (5)0.0056 (5)0.0155 (5)
S20.0440 (6)0.0237 (5)0.0202 (5)0.0095 (5)0.0041 (4)0.0059 (4)
Si10.0219 (5)0.0243 (6)0.0222 (5)0.0052 (4)0.0038 (4)0.0046 (4)
Si20.0263 (5)0.0212 (5)0.0219 (5)0.0089 (4)0.0058 (4)0.0053 (4)
N10.066 (3)0.027 (2)0.0226 (19)0.001 (2)0.0158 (19)0.0062 (16)
N20.042 (2)0.042 (2)0.029 (2)0.0157 (19)0.0116 (18)0.0128 (18)
O10.0209 (14)0.0253 (15)0.0356 (17)0.0064 (12)0.0057 (12)0.0102 (13)
O20.0321 (16)0.0285 (16)0.0252 (15)0.0015 (13)0.0073 (13)0.0019 (13)
O30.0241 (15)0.0329 (17)0.0255 (15)0.0047 (13)0.0025 (12)0.0030 (13)
O40.0308 (15)0.0238 (15)0.0239 (15)0.0079 (12)0.0049 (12)0.0061 (12)
O50.0239 (14)0.0247 (15)0.0295 (16)0.0091 (12)0.0072 (12)0.0022 (12)
O60.0266 (15)0.0234 (15)0.0326 (16)0.0090 (12)0.0086 (13)0.0083 (13)
C10.030 (2)0.024 (2)0.051 (3)0.0109 (18)0.005 (2)0.012 (2)
C20.046 (3)0.053 (4)0.114 (6)0.016 (3)0.020 (4)0.057 (4)
C30.045 (3)0.044 (3)0.062 (4)0.021 (3)0.002 (3)0.010 (3)
C40.029 (2)0.041 (3)0.054 (3)0.013 (2)0.000 (2)0.014 (3)
C50.038 (3)0.040 (3)0.028 (2)0.003 (2)0.011 (2)0.002 (2)
C60.086 (5)0.059 (4)0.038 (3)0.003 (4)0.036 (3)0.011 (3)
C70.040 (3)0.047 (3)0.047 (3)0.010 (2)0.018 (2)0.007 (3)
C80.044 (3)0.044 (3)0.023 (2)0.001 (2)0.004 (2)0.003 (2)
C90.025 (2)0.039 (3)0.033 (2)0.0010 (19)0.0005 (18)0.004 (2)
C100.032 (3)0.112 (7)0.064 (5)0.023 (4)0.001 (3)0.011 (4)
C110.045 (3)0.058 (4)0.075 (5)0.009 (3)0.003 (3)0.030 (4)
C120.054 (3)0.052 (4)0.043 (3)0.004 (3)0.005 (3)0.015 (3)
C130.026 (2)0.033 (2)0.025 (2)0.0094 (18)0.0045 (16)0.0105 (18)
C140.051 (3)0.049 (3)0.027 (2)0.021 (3)0.003 (2)0.007 (2)
C150.033 (3)0.061 (4)0.048 (3)0.021 (2)0.014 (2)0.026 (3)
C160.050 (3)0.042 (3)0.039 (3)0.003 (2)0.001 (2)0.022 (2)
C170.023 (2)0.033 (2)0.034 (2)0.0120 (18)0.0090 (18)0.0057 (19)
C180.035 (3)0.046 (3)0.050 (3)0.014 (2)0.019 (2)0.003 (3)
C190.035 (3)0.053 (3)0.060 (4)0.022 (3)0.000 (3)0.021 (3)
C200.033 (2)0.034 (3)0.042 (3)0.010 (2)0.016 (2)0.007 (2)
C210.031 (2)0.025 (2)0.037 (2)0.0104 (18)0.0132 (19)0.0096 (19)
C220.051 (3)0.031 (3)0.040 (3)0.019 (2)0.011 (2)0.013 (2)
C230.040 (3)0.023 (2)0.044 (3)0.0040 (19)0.013 (2)0.002 (2)
C240.034 (3)0.041 (3)0.077 (4)0.015 (2)0.027 (3)0.027 (3)
C250.045 (3)0.056 (4)0.053 (3)0.013 (3)0.013 (3)0.026 (3)
C260.043 (3)0.084 (5)0.092 (5)0.029 (3)0.025 (3)0.064 (5)
C270.056 (4)0.105 (6)0.075 (5)0.057 (4)0.041 (4)0.066 (5)
C280.082 (5)0.082 (5)0.048 (3)0.066 (4)0.045 (3)0.045 (3)
C290.058 (3)0.047 (3)0.037 (3)0.038 (3)0.024 (2)0.027 (2)
C300.071 (4)0.031 (2)0.024 (2)0.030 (3)0.017 (2)0.0102 (19)
C310.083 (5)0.059 (4)0.028 (3)0.021 (4)0.015 (3)0.008 (3)
C320.116 (7)0.053 (4)0.031 (3)0.025 (4)0.008 (4)0.005 (3)
C330.148 (8)0.043 (4)0.027 (3)0.026 (5)0.006 (4)0.005 (3)
C340.108 (6)0.060 (4)0.032 (3)0.050 (4)0.017 (3)0.009 (3)
Geometric parameters (Å, º) top
Pb1—N12.610 (4)C12—H12B0.98
Pb1—S22.6705 (11)C12—H12C0.98
Pb1—S12.7034 (13)C13—C141.515 (7)
Pb1—N22.725 (4)C13—C151.517 (6)
S1—Si12.0730 (17)C13—C161.518 (7)
S2—Si22.0861 (16)C14—H14A0.98
Si1—O31.625 (3)C14—H14B0.98
Si1—O21.627 (3)C14—H14C0.98
Si1—O11.633 (3)C15—H15A0.98
Si2—O51.628 (3)C15—H15B0.98
Si2—O61.632 (3)C15—H15C0.98
Si2—O41.641 (3)C16—H16A0.98
N1—C311.342 (8)C16—H16B0.98
N1—C301.344 (7)C16—H16C0.98
N2—C251.332 (8)C17—C201.517 (7)
N2—C291.338 (7)C17—C191.519 (7)
O1—C11.436 (5)C17—C181.525 (7)
O2—C51.442 (6)C18—H18A0.98
O3—C91.442 (5)C18—H18B0.98
O4—C131.448 (5)C18—H18C0.98
O5—C171.437 (5)C19—H19A0.98
O6—C211.437 (5)C19—H19B0.98
C1—C21.517 (8)C19—H19C0.98
C1—C31.526 (8)C20—H20A0.98
C1—C41.528 (7)C20—H20B0.98
C2—H2A0.98C20—H20C0.98
C2—H2B0.98C21—C241.522 (7)
C2—H2C0.98C21—C221.524 (7)
C3—H3A0.98C21—C231.524 (7)
C3—H3B0.98C22—H22A0.98
C3—H3C0.98C22—H22B0.98
C4—H4A0.98C22—H22C0.98
C4—H4B0.98C23—H23A0.98
C4—H4C0.98C23—H23B0.98
C5—C61.513 (8)C23—H23C0.98
C5—C71.519 (8)C24—H24A0.98
C5—C81.536 (7)C24—H24B0.98
C6—H6A0.98C24—H24C0.98
C6—H6B0.98C25—C261.373 (9)
C6—H6C0.98C25—H250.95
C7—H7A0.98C26—C271.367 (11)
C7—H7B0.98C26—H260.95
C7—H7C0.98C27—C281.363 (11)
C8—H8A0.98C27—H270.95
C8—H8B0.98C28—C291.403 (7)
C8—H8C0.98C28—H280.95
C9—C101.498 (9)C29—C301.475 (9)
C9—C121.522 (8)C30—C341.397 (8)
C9—C111.528 (9)C31—C321.380 (9)
C10—H10A0.98C31—H310.95
C10—H10B0.98C32—C331.366 (13)
C10—H10C0.98C32—H320.95
C11—H11A0.98C33—C341.372 (12)
C11—H11B0.98C33—H330.95
C11—H11C0.98C34—H340.95
C12—H12A0.98
N1—Pb1—S295.78 (10)H12B—C12—H12C109.5
N1—Pb1—S186.96 (11)O4—C13—C14111.0 (4)
S2—Pb1—S187.14 (4)O4—C13—C15107.9 (4)
N1—Pb1—N260.74 (14)C14—C13—C15111.3 (5)
S2—Pb1—N285.70 (9)O4—C13—C16106.2 (4)
S1—Pb1—N2145.90 (9)C14—C13—C16110.3 (4)
Si1—S1—Pb197.90 (5)C15—C13—C16110.0 (4)
Si2—S2—Pb194.17 (5)C13—C14—H14A109.5
O3—Si1—O2104.71 (17)C13—C14—H14B109.5
O3—Si1—O1105.72 (17)H14A—C14—H14B109.5
O2—Si1—O1111.48 (18)C13—C14—H14C109.5
O3—Si1—S1115.27 (14)H14A—C14—H14C109.5
O2—Si1—S1114.26 (14)H14B—C14—H14C109.5
O1—Si1—S1105.21 (13)C13—C15—H15A109.5
O5—Si2—O6103.97 (17)C13—C15—H15B109.5
O5—Si2—O4112.24 (17)H15A—C15—H15B109.5
O6—Si2—O4105.83 (17)C13—C15—H15C109.5
O5—Si2—S2114.68 (13)H15A—C15—H15C109.5
O6—Si2—S2115.23 (13)H15B—C15—H15C109.5
O4—Si2—S2104.75 (13)C13—C16—H16A109.5
C31—N1—C30118.5 (5)C13—C16—H16B109.5
C31—N1—Pb1117.9 (4)H16A—C16—H16B109.5
C30—N1—Pb1122.9 (4)C13—C16—H16C109.5
C25—N2—C29118.3 (5)H16A—C16—H16C109.5
C25—N2—Pb1121.2 (4)H16B—C16—H16C109.5
C29—N2—Pb1120.1 (4)O5—C17—C20110.4 (4)
C1—O1—Si1132.5 (3)O5—C17—C19108.2 (4)
C5—O2—Si1132.4 (3)C20—C17—C19111.5 (4)
C9—O3—Si1133.3 (3)O5—C17—C18105.8 (4)
C13—O4—Si2131.4 (3)C20—C17—C18109.8 (4)
C17—O5—Si2134.8 (3)C19—C17—C18111.0 (4)
C21—O6—Si2131.0 (3)C17—C18—H18A109.5
O1—C1—C2111.2 (4)C17—C18—H18B109.5
O1—C1—C3108.2 (4)H18A—C18—H18B109.5
C2—C1—C3111.6 (5)C17—C18—H18C109.5
O1—C1—C4105.1 (4)H18A—C18—H18C109.5
C2—C1—C4110.4 (5)H18B—C18—H18C109.5
C3—C1—C4110.1 (5)C17—C19—H19A109.5
C1—C2—H2A109.5C17—C19—H19B109.5
C1—C2—H2B109.5H19A—C19—H19B109.5
H2A—C2—H2B109.5C17—C19—H19C109.5
C1—C2—H2C109.5H19A—C19—H19C109.5
H2A—C2—H2C109.5H19B—C19—H19C109.5
H2B—C2—H2C109.5C17—C20—H20A109.5
C1—C3—H3A109.5C17—C20—H20B109.5
C1—C3—H3B109.5H20A—C20—H20B109.5
H3A—C3—H3B109.5C17—C20—H20C109.5
C1—C3—H3C109.5H20A—C20—H20C109.5
H3A—C3—H3C109.5H20B—C20—H20C109.5
H3B—C3—H3C109.5O6—C21—C24105.3 (4)
C1—C4—H4A109.5O6—C21—C22110.3 (4)
C1—C4—H4B109.5C24—C21—C22110.6 (4)
H4A—C4—H4B109.5O6—C21—C23110.7 (4)
C1—C4—H4C109.5C24—C21—C23109.4 (4)
H4A—C4—H4C109.5C22—C21—C23110.4 (4)
H4B—C4—H4C109.5C21—C22—H22A109.5
O2—C5—C6105.4 (4)C21—C22—H22B109.5
O2—C5—C7109.5 (4)H22A—C22—H22B109.5
C6—C5—C7111.4 (5)C21—C22—H22C109.5
O2—C5—C8109.6 (4)H22A—C22—H22C109.5
C6—C5—C8109.7 (5)H22B—C22—H22C109.5
C7—C5—C8111.0 (5)C21—C23—H23A109.5
C5—C6—H6A109.5C21—C23—H23B109.5
C5—C6—H6B109.5H23A—C23—H23B109.5
H6A—C6—H6B109.5C21—C23—H23C109.5
C5—C6—H6C109.5H23A—C23—H23C109.5
H6A—C6—H6C109.5H23B—C23—H23C109.5
H6B—C6—H6C109.5C21—C24—H24A109.5
C5—C7—H7A109.5C21—C24—H24B109.5
C5—C7—H7B109.5H24A—C24—H24B109.5
H7A—C7—H7B109.5C21—C24—H24C109.5
C5—C7—H7C109.5H24A—C24—H24C109.5
H7A—C7—H7C109.5H24B—C24—H24C109.5
H7B—C7—H7C109.5N2—C25—C26123.0 (7)
C5—C8—H8A109.5N2—C25—H25118.5
C5—C8—H8B109.5C26—C25—H25118.5
H8A—C8—H8B109.5C27—C26—C25119.2 (7)
C5—C8—H8C109.5C27—C26—H26120.4
H8A—C8—H8C109.5C25—C26—H26120.4
H8B—C8—H8C109.5C28—C27—C26118.7 (6)
O3—C9—C10112.4 (4)C28—C27—H27120.6
O3—C9—C12107.5 (4)C26—C27—H27120.6
C10—C9—C12110.2 (6)C27—C28—C29119.6 (6)
O3—C9—C11105.5 (4)C27—C28—H28120.2
C10—C9—C11112.1 (6)C29—C28—H28120.2
C12—C9—C11108.9 (5)N2—C29—C28121.0 (6)
C9—C10—H10A109.5N2—C29—C30116.4 (4)
C9—C10—H10B109.5C28—C29—C30122.5 (5)
H10A—C10—H10B109.5N1—C30—C34119.8 (6)
C9—C10—H10C109.5N1—C30—C29117.9 (4)
H10A—C10—H10C109.5C34—C30—C29122.3 (6)
H10B—C10—H10C109.5N1—C31—C32123.9 (7)
C9—C11—H11A109.5N1—C31—H31118
C9—C11—H11B109.5C32—C31—H31118
H11A—C11—H11B109.5C33—C32—C31117.7 (8)
C9—C11—H11C109.5C33—C32—H32121.2
H11A—C11—H11C109.5C31—C32—H32121.2
H11B—C11—H11C109.5C32—C33—C34119.3 (6)
C9—C12—H12A109.5C32—C33—H33120.4
C9—C12—H12B109.5C34—C33—H33120.4
H12A—C12—H12B109.5C33—C34—C30120.7 (7)
C9—C12—H12C109.5C33—C34—H34119.6
H12A—C12—H12C109.5C30—C34—H34119.6
(II) (4,7-diphenyl-1,10-phenanthroline-κ2N,N')bis(tri-tert- butoxysilanethiolato-κS)lead(II) benzene hemisolvate top
Crystal data top
[Pb(C12H27O3SSi)2(C24H16N2)]·0.5C6H6Z = 2
Mr = 1137.6F(000) = 1166
Triclinic, P1Dx = 1.332 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 10.204 (2) ÅCell parameters from 49 reflections
b = 13.359 (3) Åθ = 4.4–37.9°
c = 21.109 (4) ŵ = 3.13 mm1
α = 84.57 (3)°T = 293 K
β = 83.05 (3)°Fragment, colourless
γ = 85.29 (3)°0.6 × 0.41 × 0.32 mm
V = 2836.2 (10) Å3
Data collection top
Oxford Diffraction KM4 single-point
diffractometer
Rint = 0.053
Graphite monochromatorθmax = 25.1°, θmin = 2.0°
ω/2θ scansh = 1212
Absorption correction: ψ scan
(North et al., 1968)
k = 015
Tmin = 0.198, Tmax = 0.359l = 2525
10564 measured reflections3 standard reflections every 200 reflections
10091 independent reflections intensity decay: 5.7%
7445 reflections with I > 2σ(I)
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)] = 0.037Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.118H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.0755P)2 + 0.8361P]
where P = (Fo2 + 2Fc2)/3
10091 reflections(Δ/σ)max = 0.012
648 parametersΔρmax = 0.84 e Å3
115 restraintsΔρmin = 0.80 e Å3
Crystal data top
[Pb(C12H27O3SSi)2(C24H16N2)]·0.5C6H6γ = 85.29 (3)°
Mr = 1137.6V = 2836.2 (10) Å3
Triclinic, P1Z = 2
a = 10.204 (2) ÅMo Kα radiation
b = 13.359 (3) ŵ = 3.13 mm1
c = 21.109 (4) ÅT = 293 K
α = 84.57 (3)°0.6 × 0.41 × 0.32 mm
β = 83.05 (3)°
Data collection top
Oxford Diffraction KM4 single-point
diffractometer
7445 reflections with I > 2σ(I)
Absorption correction: ψ scan
(North et al., 1968)
Rint = 0.053
Tmin = 0.198, Tmax = 0.3593 standard reflections every 200 reflections
10564 measured reflections intensity decay: 5.7%
10091 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.037115 restraints
wR(F2) = 0.118H-atom parameters constrained
S = 1.00Δρmax = 0.84 e Å3
10091 reflectionsΔρmin = 0.80 e Å3
648 parameters
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. 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 > σ(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) top
xyzUiso*/UeqOcc. (<1)
Pb10.33407 (2)0.624570 (17)0.207892 (10)0.05504 (10)
S10.07168 (17)0.65601 (13)0.20030 (8)0.0664 (4)
S20.28104 (17)0.48929 (12)0.30476 (7)0.0603 (4)
Si10.07247 (18)0.78656 (13)0.13868 (8)0.0589 (4)
Si20.32274 (17)0.36772 (13)0.24981 (8)0.0574 (4)
N10.3153 (4)0.7586 (3)0.2904 (2)0.0505 (11)
N20.5493 (5)0.6455 (4)0.2751 (2)0.0561 (12)
O10.0039 (5)0.8831 (3)0.1714 (2)0.0785 (13)
O20.2258 (5)0.8121 (3)0.1248 (2)0.0756 (13)
O30.0049 (6)0.7809 (4)0.0747 (2)0.0884 (16)
O40.2112 (6)0.2873 (5)0.2580 (4)0.075 (3)0.714 (12)
O4A0.1832 (15)0.3474 (12)0.2182 (7)0.060 (5)0.286 (12)
O50.3735 (7)0.4132 (4)0.1791 (2)0.1005 (19)
O60.4562 (8)0.2995 (5)0.2684 (3)0.075 (2)0.714 (12)
O6A0.3651 (17)0.2626 (11)0.2801 (7)0.058 (5)0.286 (12)
C10.1407 (7)0.9126 (5)0.1908 (4)0.0732 (18)
C20.1736 (11)1.0098 (8)0.1509 (6)0.135 (4)
H2A0.11621.05990.15830.203*
H2B0.26391.03310.16280.203*
H2C0.16140.9980.10630.203*
C30.1460 (10)0.9335 (9)0.2593 (5)0.125 (4)
H3A0.13550.87110.28540.188*
H3B0.22980.96770.27270.188*
H3C0.07610.97520.2640.188*
C40.2308 (9)0.8325 (8)0.1856 (6)0.123 (4)
H4A0.23250.82240.14130.185*
H4B0.31840.85260.20420.185*
H4C0.19960.77080.20790.185*
C50.2970 (10)0.8963 (7)0.0946 (5)0.130 (3)
C60.2290 (13)0.9512 (10)0.0435 (7)0.173 (4)
H6A0.21080.9050.0140.259*
H6B0.28421.00120.02120.259*
H6C0.14740.98350.06160.259*
C70.3147 (14)0.9637 (10)0.1435 (7)0.167 (4)
H7A0.23120.99820.15710.25*
H7B0.37661.01220.12590.25*
H7C0.34770.92490.17960.25*
C80.4268 (12)0.8549 (9)0.0679 (7)0.163 (4)
H8A0.46530.80990.09990.245*
H8B0.48330.90890.05450.245*
H8C0.41710.81890.03170.245*
C90.0034 (16)0.7085 (9)0.0302 (6)0.148 (3)
C100.1072 (14)0.6363 (9)0.0603 (6)0.156 (4)
H10A0.08390.60740.10120.234*
H10B0.11040.58360.03280.234*
H10C0.19240.67260.06590.234*
C110.0533 (16)0.7651 (10)0.0259 (6)0.178 (4)
H11A0.09480.72060.04920.267*
H11B0.0190.79370.05310.267*
H11C0.11670.81810.01230.267*
C120.1286 (16)0.6468 (11)0.0191 (7)0.177 (4)
H12A0.19960.69090.01430.265*
H12B0.1310.61250.0190.265*
H12C0.13830.59830.05510.265*
C130.0688 (10)0.2966 (9)0.2583 (6)0.073 (4)0.714 (12)
C140.011 (2)0.322 (3)0.3244 (11)0.105 (7)0.714 (12)
H14A0.04040.26990.35540.157*0.714 (12)
H14B0.08360.32590.32710.157*0.714 (12)
H14C0.04030.38520.33280.157*0.714 (12)
C150.0270 (18)0.3763 (10)0.2073 (8)0.118 (5)0.714 (12)
H15A0.06770.38190.20910.177*0.714 (12)
H15B0.06510.35760.16590.177*0.714 (12)
H15C0.05730.43990.21470.177*0.714 (12)
C160.038 (3)0.1925 (14)0.2461 (17)0.125 (8)0.714 (12)
H16A0.0630.18220.20170.188*0.714 (12)
H16B0.0550.18520.25660.188*0.714 (12)
H16C0.08670.14340.27210.188*0.714 (12)
C13A0.061 (3)0.301 (4)0.242 (2)0.094*0.286 (12)
C14A0.009 (9)0.326 (8)0.308 (3)0.13 (3)*0.286 (12)
H14D0.07410.30410.33680.194*0.286 (12)
H14E0.07060.2930.32190.194*0.286 (12)
H14F0.00950.39790.30870.194*0.286 (12)
C15A0.046 (4)0.357 (3)0.206 (2)0.109 (13)*0.286 (12)
H15D0.01230.4150.18150.164*0.286 (12)
H15E0.11880.37820.23680.164*0.286 (12)
H15F0.07690.31330.17860.164*0.286 (12)
C16A0.072 (8)0.193 (4)0.228 (4)0.13 (3)*0.286 (12)
H16D0.14670.15830.24660.194*0.286 (12)
H16E0.08350.18770.18270.194*0.286 (12)
H16F0.00720.16180.24660.194*0.286 (12)
C170.4378 (13)0.3740 (7)0.1216 (4)0.122 (2)
C180.4178 (16)0.2628 (8)0.1216 (6)0.180 (7)
H18A0.44740.22710.15950.27*
H18B0.46770.23680.08440.27*
H18C0.32550.25410.12090.27*
C190.3683 (15)0.4361 (10)0.0697 (5)0.158 (5)
H19A0.27790.41920.07290.238*
H19B0.41240.42190.02840.238*
H19C0.37060.50650.0750.238*
C200.5773 (13)0.3980 (14)0.1128 (8)0.212 (8)
H20A0.58230.46840.11740.318*
H20B0.61660.38290.07080.318*
H20C0.6240.35860.14450.318*
C210.483 (2)0.225 (2)0.3135 (11)0.081 (6)0.714 (12)
C220.6318 (15)0.2252 (17)0.3231 (11)0.158 (9)0.714 (12)
H22A0.68470.2240.28230.237*0.714 (12)
H22B0.65670.16690.35040.237*0.714 (12)
H22C0.64560.28510.34250.237*0.714 (12)
C230.460 (4)0.118 (2)0.2970 (17)0.148 (13)0.714 (12)
H23A0.36630.11180.29710.222*0.714 (12)
H23B0.49320.06840.32840.222*0.714 (12)
H23C0.50420.10590.25540.222*0.714 (12)
C240.413 (2)0.241 (2)0.3810 (10)0.118 (11)0.714 (12)
H24A0.41760.31010.38970.178*0.714 (12)
H24B0.45490.19730.41230.178*0.714 (12)
H24C0.32150.22680.38310.178*0.714 (12)
C21A0.482 (7)0.215 (7)0.328 (4)0.081 (6)0.286 (12)
C22A0.594 (3)0.284 (3)0.301 (3)0.14 (2)0.286 (12)
H22D0.55630.34890.28670.211*0.286 (12)
H22E0.64550.25420.2650.211*0.286 (12)
H22F0.64990.28990.33330.211*0.286 (12)
C23A0.495 (9)0.121 (4)0.300 (4)0.14 (3)0.286 (12)
H23D0.41560.08660.31230.216*0.286 (12)
H23E0.5690.08080.31480.216*0.286 (12)
H23F0.50840.13330.25430.216*0.286 (12)
C24A0.406 (4)0.239 (3)0.383 (2)0.09 (2)0.286 (12)
H24D0.44740.28750.40270.138*0.286 (12)
H24E0.39560.17920.41170.138*0.286 (12)
H24F0.320.26670.37280.138*0.286 (12)
C250.2044 (6)0.8160 (5)0.2972 (3)0.0630 (16)
H250.14310.81320.26830.076*
C260.1741 (6)0.8814 (5)0.3459 (3)0.0609 (15)
H260.09330.91930.34920.073*
C270.2609 (5)0.8895 (4)0.3877 (3)0.0520 (13)
C280.3854 (6)0.8341 (4)0.3795 (3)0.0503 (13)
C290.4902 (6)0.8444 (4)0.4168 (3)0.0582 (15)
H290.47940.89220.44660.07*
C300.6032 (6)0.7872 (4)0.4099 (3)0.0569 (14)
H300.66880.79570.43550.068*
C310.6269 (5)0.7132 (4)0.3646 (3)0.0497 (13)
C320.7427 (5)0.6478 (4)0.3586 (3)0.0526 (13)
C330.7595 (6)0.5880 (5)0.3085 (3)0.0625 (16)
H330.83730.54740.3010.075*
C340.6618 (6)0.5883 (5)0.2698 (3)0.0655 (17)
H340.67520.54510.23720.079*
C350.5322 (5)0.7075 (4)0.3219 (3)0.0486 (13)
C360.4078 (5)0.7684 (4)0.3303 (3)0.0491 (13)
C370.2233 (5)0.9516 (5)0.4425 (3)0.0568 (15)
C380.1652 (7)1.0482 (5)0.4335 (4)0.0755 (19)
H380.15221.07520.39230.091*
C390.1264 (9)1.1052 (7)0.4844 (7)0.110 (4)
H390.08931.17060.47720.132*
C400.1419 (9)1.0664 (10)0.5447 (7)0.121 (4)
H400.11471.10550.57870.145*
C410.1959 (9)0.9725 (10)0.5563 (4)0.120 (4)
H410.2060.94620.5980.144*
C420.2375 (7)0.9138 (7)0.5038 (4)0.085 (2)
H420.2750.84850.51140.102*
C430.8411 (5)0.6423 (4)0.4056 (3)0.0527 (13)
C440.9746 (6)0.6484 (5)0.3836 (3)0.0658 (16)
H441.00280.65660.33990.079*
C451.0638 (6)0.6420 (6)0.4279 (4)0.0757 (19)
H451.15320.64680.41380.091*
C461.0243 (7)0.6290 (5)0.4920 (4)0.0695 (18)
H461.08630.62530.52110.083*
C470.8927 (7)0.6213 (5)0.5134 (4)0.0681 (17)
H470.8650.61150.5570.082*
C480.8026 (6)0.6283 (4)0.4697 (3)0.0565 (14)
H480.71330.62340.48410.068*
C490.5828 (9)0.4255 (7)0.4748 (6)0.108 (3)
H490.63910.37410.45760.13*
C500.5042 (11)0.4871 (9)0.4366 (4)0.101 (3)
H500.50810.47810.39320.121*
C510.4223 (9)0.5599 (9)0.4620 (6)0.105 (3)
H510.36840.60090.43630.126*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pb10.06311 (16)0.05643 (14)0.04580 (13)0.00725 (10)0.00336 (9)0.00667 (9)
S10.0665 (10)0.0688 (10)0.0648 (10)0.0138 (8)0.0156 (8)0.0070 (8)
S20.0787 (11)0.0571 (8)0.0458 (8)0.0072 (7)0.0051 (7)0.0076 (6)
Si10.0687 (11)0.0573 (9)0.0529 (9)0.0052 (8)0.0146 (8)0.0053 (7)
Si20.0587 (10)0.0553 (9)0.0571 (10)0.0040 (7)0.0009 (8)0.0086 (7)
N10.047 (3)0.056 (3)0.049 (3)0.002 (2)0.010 (2)0.006 (2)
N20.053 (3)0.059 (3)0.056 (3)0.004 (2)0.000 (2)0.014 (2)
O10.075 (3)0.068 (3)0.095 (4)0.006 (2)0.007 (3)0.023 (3)
O20.070 (3)0.070 (3)0.082 (3)0.010 (2)0.001 (2)0.012 (2)
O30.133 (5)0.073 (3)0.067 (3)0.000 (3)0.045 (3)0.009 (2)
O40.066 (4)0.056 (4)0.105 (6)0.010 (3)0.013 (4)0.015 (4)
O4A0.067 (10)0.059 (10)0.058 (10)0.011 (8)0.010 (7)0.011 (8)
O50.171 (6)0.069 (3)0.057 (3)0.017 (3)0.018 (3)0.016 (2)
O60.063 (5)0.069 (4)0.088 (5)0.002 (4)0.006 (4)0.003 (4)
O6A0.053 (11)0.046 (8)0.071 (10)0.007 (7)0.003 (7)0.003 (7)
C10.069 (5)0.069 (4)0.081 (5)0.006 (3)0.014 (4)0.008 (3)
C20.131 (9)0.121 (8)0.142 (10)0.031 (7)0.021 (7)0.021 (7)
C30.102 (7)0.179 (11)0.093 (7)0.011 (7)0.008 (5)0.026 (7)
C40.077 (6)0.116 (8)0.182 (11)0.020 (5)0.005 (6)0.039 (7)
C50.124 (6)0.096 (6)0.157 (8)0.037 (5)0.017 (6)0.031 (5)
C60.167 (9)0.146 (8)0.190 (9)0.044 (7)0.007 (8)0.074 (7)
C70.183 (9)0.123 (7)0.194 (10)0.070 (7)0.013 (8)0.005 (7)
C80.131 (7)0.137 (8)0.202 (9)0.028 (6)0.047 (7)0.023 (7)
C90.224 (9)0.133 (7)0.108 (6)0.005 (6)0.084 (6)0.045 (5)
C100.219 (10)0.138 (8)0.133 (8)0.032 (7)0.071 (8)0.041 (6)
C110.273 (11)0.168 (9)0.113 (7)0.014 (8)0.097 (7)0.025 (6)
C120.228 (11)0.164 (9)0.151 (8)0.006 (8)0.033 (8)0.080 (7)
C130.063 (6)0.065 (6)0.099 (11)0.018 (5)0.024 (6)0.023 (6)
C140.069 (9)0.162 (19)0.085 (10)0.023 (8)0.006 (8)0.013 (11)
C150.134 (14)0.091 (9)0.138 (13)0.023 (9)0.058 (11)0.010 (8)
C160.101 (14)0.082 (10)0.20 (3)0.023 (8)0.019 (16)0.052 (12)
C170.190.096 (6)0.070 (5)0.013 (7)0.042 (6)0.030 (5)
C180.301 (19)0.103 (8)0.126 (9)0.013 (9)0.057 (10)0.063 (7)
C190.226 (15)0.177 (12)0.073 (7)0.026 (11)0.002 (8)0.028 (7)
C200.125 (11)0.31 (2)0.195 (16)0.028 (12)0.056 (10)0.099 (15)
C210.0910.070 (9)0.077 (15)0.012 (5)0.019 (8)0.014 (11)
C220.072 (10)0.170 (19)0.21 (2)0.042 (11)0.008 (11)0.025 (16)
C230.18 (3)0.088 (16)0.17 (2)0.016 (14)0.023 (19)0.044 (16)
C240.121 (19)0.13 (2)0.107 (18)0.013 (15)0.051 (13)0.010 (15)
C21A0.0910.070 (9)0.077 (15)0.012 (5)0.019 (8)0.014 (11)
C22A0.036 (18)0.10 (3)0.28 (6)0.011 (16)0.04 (3)0.03 (3)
C23A0.12 (4)0.05 (3)0.24 (8)0.02 (2)0.00 (4)0.03 (3)
C24A0.08 (3)0.06 (2)0.11 (4)0.003 (19)0.08 (3)0.01 (2)
C250.053 (4)0.071 (4)0.067 (4)0.004 (3)0.018 (3)0.011 (3)
C260.051 (3)0.062 (4)0.070 (4)0.009 (3)0.009 (3)0.017 (3)
C270.046 (3)0.047 (3)0.064 (4)0.001 (2)0.008 (3)0.012 (3)
C280.049 (3)0.043 (3)0.060 (3)0.000 (2)0.006 (3)0.010 (2)
C290.049 (3)0.059 (3)0.071 (4)0.001 (3)0.012 (3)0.027 (3)
C300.047 (3)0.061 (3)0.067 (4)0.006 (3)0.012 (3)0.020 (3)
C310.039 (3)0.053 (3)0.056 (3)0.008 (2)0.000 (2)0.004 (2)
C320.042 (3)0.052 (3)0.063 (4)0.008 (2)0.004 (3)0.007 (3)
C330.045 (3)0.067 (4)0.074 (4)0.004 (3)0.002 (3)0.017 (3)
C340.065 (4)0.070 (4)0.063 (4)0.002 (3)0.001 (3)0.024 (3)
C350.043 (3)0.045 (3)0.057 (3)0.007 (2)0.002 (2)0.006 (2)
C360.043 (3)0.042 (3)0.063 (3)0.006 (2)0.005 (3)0.006 (2)
C370.041 (3)0.066 (4)0.067 (4)0.004 (3)0.005 (3)0.025 (3)
C380.066 (4)0.057 (4)0.104 (6)0.005 (3)0.003 (4)0.024 (4)
C390.073 (5)0.074 (5)0.187 (11)0.018 (4)0.026 (7)0.068 (7)
C400.064 (5)0.160 (11)0.151 (10)0.027 (6)0.026 (6)0.103 (9)
C410.073 (5)0.212 (12)0.085 (6)0.013 (7)0.013 (4)0.082 (7)
C420.065 (4)0.117 (6)0.076 (5)0.016 (4)0.013 (4)0.035 (4)
C430.042 (3)0.047 (3)0.068 (4)0.000 (2)0.004 (3)0.005 (3)
C440.044 (3)0.081 (4)0.070 (4)0.001 (3)0.001 (3)0.003 (3)
C450.039 (3)0.092 (5)0.094 (6)0.001 (3)0.009 (3)0.001 (4)
C460.064 (4)0.066 (4)0.081 (5)0.004 (3)0.023 (4)0.006 (3)
C470.071 (4)0.056 (4)0.077 (4)0.001 (3)0.009 (4)0.008 (3)
C480.048 (3)0.062 (3)0.057 (4)0.008 (3)0.005 (3)0.006 (3)
C490.080 (6)0.093 (6)0.148 (10)0.026 (5)0.005 (6)0.018 (6)
C500.093 (7)0.135 (8)0.082 (6)0.059 (6)0.023 (5)0.022 (6)
C510.069 (5)0.130 (8)0.115 (8)0.041 (6)0.040 (5)0.057 (7)
Geometric parameters (Å, º) top
Pb1—N12.594 (5)C17—C201.471 (17)
Pb1—S22.6331 (18)C17—C181.515 (14)
Pb1—S12.6976 (18)C17—C191.521 (16)
Pb1—N22.801 (5)C18—H18A0.96
S1—Si12.075 (2)C18—H18B0.96
S2—Si22.071 (2)C18—H18C0.96
Si1—O31.599 (5)C19—H19A0.96
Si1—O21.615 (5)C19—H19B0.96
Si1—O11.619 (5)C19—H19C0.96
Si2—O6A1.538 (13)C20—H20A0.96
Si2—O51.600 (5)C20—H20B0.96
Si2—O41.611 (7)C20—H20C0.96
Si2—O61.642 (7)C21—C241.55 (2)
Si2—O4A1.696 (15)C21—C231.55 (2)
N1—C251.315 (7)C21—C221.55 (2)
N1—C361.361 (7)C22—H22A0.96
N2—C341.326 (8)C22—H22B0.96
N2—C351.333 (7)C22—H22C0.96
O1—C11.439 (8)C23—H23A0.96
O2—C51.444 (10)C23—H23B0.96
O3—C91.425 (11)C23—H23C0.96
O4—C131.448 (11)C24—H24A0.96
O4A—C13A1.45 (2)C24—H24B0.96
O5—C171.431 (9)C24—H24C0.96
O6—C211.35 (3)C21A—C24A1.36 (6)
O6A—C21A1.70 (10)C21A—C23A1.42 (7)
C1—C41.487 (11)C21A—C22A1.55 (7)
C1—C31.494 (11)C22A—H22D0.96
C1—C21.516 (11)C22A—H22E0.96
C2—H2A0.96C22A—H22F0.96
C2—H2B0.96C23A—H23D0.96
C2—H2C0.96C23A—H23E0.96
C3—H3A0.96C23A—H23F0.96
C3—H3B0.96C24A—H24D0.96
C3—H3C0.96C24A—H24E0.96
C4—H4A0.96C24A—H24F0.96
C4—H4B0.96C25—C261.401 (9)
C4—H4C0.96C25—H250.93
C5—C61.460 (12)C26—C271.341 (8)
C5—C81.461 (11)C26—H260.93
C5—C71.470 (12)C27—C281.417 (8)
C6—H6A0.96C27—C371.482 (8)
C6—H6B0.96C28—C361.408 (8)
C6—H6C0.96C28—C291.426 (8)
C7—H7A0.96C29—C301.330 (8)
C7—H7B0.96C29—H290.93
C7—H7C0.96C30—C311.426 (8)
C8—H8A0.96C30—H300.93
C8—H8B0.96C31—C351.410 (8)
C8—H8C0.96C31—C321.411 (8)
C9—C111.466 (15)C32—C331.370 (8)
C9—C121.525 (18)C32—C431.488 (8)
C9—C101.532 (18)C33—C341.363 (9)
C10—H10A0.96C33—H330.93
C10—H10B0.96C34—H340.93
C10—H10C0.96C35—C361.452 (7)
C11—H11A0.96C37—C421.364 (10)
C11—H11B0.96C37—C381.381 (9)
C11—H11C0.96C38—C391.376 (12)
C12—H12A0.96C38—H380.93
C12—H12B0.96C39—C401.351 (15)
C12—H12C0.96C39—H390.93
C13—C141.503 (13)C40—C411.341 (15)
C13—C161.503 (11)C40—H400.93
C13—C151.515 (12)C41—C421.421 (11)
C14—H14A0.96C41—H410.93
C14—H14B0.96C42—H420.93
C14—H14C0.96C43—C481.361 (8)
C15—H15A0.96C43—C441.392 (8)
C15—H15B0.96C44—C451.374 (9)
C15—H15C0.96C44—H440.93
C16—H16A0.96C45—C461.363 (10)
C16—H16B0.96C45—H450.93
C16—H16C0.96C46—C471.372 (10)
C13A—C14A1.501 (17)C46—H460.93
C13A—C16A1.501 (17)C47—C481.371 (9)
C13A—C15A1.506 (17)C47—H470.93
C14A—H14D0.96C48—H480.93
C14A—H14E0.96C49—C51i1.359 (15)
C14A—H14F0.96C49—C501.377 (13)
C15A—H15D0.96C49—H490.93
C15A—H15E0.96C50—C511.338 (14)
C15A—H15F0.96C50—H500.93
C16A—H16D0.96C51—C49i1.359 (15)
C16A—H16E0.96C51—H510.93
C16A—H16F0.96
N1—Pb1—S287.77 (11)H16D—C16A—H16E109.5
N1—Pb1—S189.44 (11)C13A—C16A—H16F109.5
S2—Pb1—S188.41 (6)H16D—C16A—H16F109.5
N1—Pb1—N260.42 (14)H16E—C16A—H16F109.5
S2—Pb1—N281.17 (11)O5—C17—C20109.3 (10)
S1—Pb1—N2148.25 (10)O5—C17—C18110.9 (8)
Si1—S1—Pb199.04 (9)C20—C17—C18114.3 (12)
Si2—S2—Pb194.28 (8)O5—C17—C19102.8 (9)
O3—Si1—O2113.1 (3)C20—C17—C19107.8 (11)
O3—Si1—O1104.8 (3)C18—C17—C19111.2 (11)
O2—Si1—O1105.4 (3)C17—C18—H18A109.5
O3—Si1—S1115.2 (2)C17—C18—H18B109.5
O2—Si1—S1105.16 (19)H18A—C18—H18B109.5
O1—Si1—S1113.0 (2)C17—C18—H18C109.5
O6A—Si2—O5125.4 (6)H18A—C18—H18C109.5
O6A—Si2—O464.9 (7)H18B—C18—H18C109.5
O5—Si2—O4118.4 (4)C17—C19—H19A109.5
O5—Si2—O6100.4 (4)C17—C19—H19B109.5
O4—Si2—O6103.5 (4)H19A—C19—H19B109.5
O6A—Si2—O4A102.8 (8)C17—C19—H19C109.5
O5—Si2—O4A85.2 (6)H19A—C19—H19C109.5
O6—Si2—O4A136.1 (6)H19B—C19—H19C109.5
O6A—Si2—S2121.1 (6)C17—C20—H20A109.5
O5—Si2—S2106.3 (2)C17—C20—H20B109.5
O4—Si2—S2115.4 (3)H20A—C20—H20B109.5
O6—Si2—S2111.7 (3)C17—C20—H20C109.5
O4A—Si2—S2108.1 (5)H20A—C20—H20C109.5
C25—N1—C36117.9 (5)H20B—C20—H20C109.5
C25—N1—Pb1117.4 (4)O6—C21—C24114 (2)
C36—N1—Pb1124.5 (3)O6—C21—C23115 (2)
C34—N2—C35116.8 (5)C24—C21—C23108.7 (19)
C34—N2—Pb1124.4 (4)O6—C21—C22107.9 (16)
C35—N2—Pb1118.2 (4)C24—C21—C22102.6 (17)
C1—O1—Si1134.3 (4)C23—C21—C22108 (3)
C5—O2—Si1135.9 (5)C21—C22—H22A109.5
C9—O3—Si1137.5 (6)C21—C22—H22B109.5
C13—O4—Si2133.6 (7)H22A—C22—H22B109.5
C13A—O4A—Si2136 (2)C21—C22—H22C109.5
C17—O5—Si2136.2 (6)H22A—C22—H22C109.5
C21—O6—Si2135.5 (11)H22B—C22—H22C109.5
Si2—O6A—C21A136 (3)C21—C23—H23A109.5
O1—C1—C4113.0 (6)C21—C23—H23B109.5
O1—C1—C3105.1 (6)H23A—C23—H23B109.5
C4—C1—C3109.3 (8)C21—C23—H23C109.5
O1—C1—C2106.5 (7)H23A—C23—H23C109.5
C4—C1—C2113.2 (8)H23B—C23—H23C109.5
C3—C1—C2109.3 (8)C21—C24—H24A109.5
C1—C2—H2A109.5C21—C24—H24B109.5
C1—C2—H2B109.5H24A—C24—H24B109.5
H2A—C2—H2B109.5C21—C24—H24C109.5
C1—C2—H2C109.5H24A—C24—H24C109.5
H2A—C2—H2C109.5H24B—C24—H24C109.5
H2B—C2—H2C109.5C24A—C21A—C23A128 (7)
C1—C3—H3A109.5C24A—C21A—C22A118 (5)
C1—C3—H3B109.5C23A—C21A—C22A112 (5)
H3A—C3—H3B109.5C24A—C21A—O6A94 (5)
C1—C3—H3C109.5C23A—C21A—O6A92 (6)
H3A—C3—H3C109.5C22A—C21A—O6A99 (6)
H3B—C3—H3C109.5C21A—C22A—H22D109.5
C1—C4—H4A109.5C21A—C22A—H22E109.5
C1—C4—H4B109.5H22D—C22A—H22E109.5
H4A—C4—H4B109.5C21A—C22A—H22F109.5
C1—C4—H4C109.5H22D—C22A—H22F109.5
H4A—C4—H4C109.5H22E—C22A—H22F109.5
H4B—C4—H4C109.5C21A—C23A—H23D109.5
O2—C5—C6112.0 (9)C21A—C23A—H23E109.5
O2—C5—C8106.9 (8)H23D—C23A—H23E109.5
C6—C5—C8109.5 (11)C21A—C23A—H23F109.5
O2—C5—C7108.9 (9)H23D—C23A—H23F109.5
C6—C5—C7110.4 (11)H23E—C23A—H23F109.5
C8—C5—C7109.0 (11)C21A—C24A—H24D109.5
C5—C6—H6A109.5C21A—C24A—H24E109.5
C5—C6—H6B109.5H24D—C24A—H24E109.5
H6A—C6—H6B109.5C21A—C24A—H24F109.5
C5—C6—H6C109.5H24D—C24A—H24F109.5
H6A—C6—H6C109.5H24E—C24A—H24F109.5
H6B—C6—H6C109.5N1—C25—C26123.2 (6)
C5—C7—H7A109.5N1—C25—H25118.4
C5—C7—H7B109.5C26—C25—H25118.4
H7A—C7—H7B109.5C27—C26—C25120.3 (5)
C5—C7—H7C109.5C27—C26—H26119.8
H7A—C7—H7C109.5C25—C26—H26119.8
H7B—C7—H7C109.5C26—C27—C28118.4 (5)
C5—C8—H8A109.5C26—C27—C37120.0 (5)
C5—C8—H8B109.5C28—C27—C37121.6 (5)
H8A—C8—H8B109.5C36—C28—C27118.0 (5)
C5—C8—H8C109.5C36—C28—C29118.5 (5)
H8A—C8—H8C109.5C27—C28—C29123.4 (5)
H8B—C8—H8C109.5C30—C29—C28121.5 (5)
O3—C9—C11105.9 (10)C30—C29—H29119.2
O3—C9—C12110.1 (10)C28—C29—H29119.2
C11—C9—C12117.1 (13)C29—C30—C31122.2 (5)
O3—C9—C10107.5 (11)C29—C30—H30118.9
C11—C9—C10108.2 (12)C31—C30—H30118.9
C12—C9—C10107.7 (12)C35—C31—C32118.1 (5)
C9—C10—H10A109.5C35—C31—C30118.5 (5)
C9—C10—H10B109.5C32—C31—C30123.4 (5)
H10A—C10—H10B109.5C33—C32—C31117.3 (5)
C9—C10—H10C109.5C33—C32—C43121.3 (5)
H10A—C10—H10C109.5C31—C32—C43121.3 (5)
H10B—C10—H10C109.5C34—C33—C32119.8 (6)
C9—C11—H11A109.5C34—C33—H33120.1
C9—C11—H11B109.5C32—C33—H33120.1
H11A—C11—H11B109.5N2—C34—C33124.9 (6)
C9—C11—H11C109.5N2—C34—H34117.6
H11A—C11—H11C109.5C33—C34—H34117.6
H11B—C11—H11C109.5N2—C35—C31123.0 (5)
C9—C12—H12A109.5N2—C35—C36118.0 (5)
C9—C12—H12B109.5C31—C35—C36119.0 (5)
H12A—C12—H12B109.5N1—C36—C28122.0 (5)
C9—C12—H12C109.5N1—C36—C35118.2 (5)
H12A—C12—H12C109.5C28—C36—C35119.7 (5)
H12B—C12—H12C109.5C42—C37—C38117.6 (6)
O4—C13—C14106.8 (11)C42—C37—C27121.5 (6)
O4—C13—C16102.9 (12)C38—C37—C27120.8 (6)
C14—C13—C16111.0 (19)C39—C38—C37121.2 (9)
O4—C13—C15111.1 (10)C39—C38—H38119.4
C14—C13—C15111.8 (17)C37—C38—H38119.4
C16—C13—C15112.7 (16)C40—C39—C38120.2 (10)
C13—C14—H14A109.5C40—C39—H39119.9
C13—C14—H14B109.5C38—C39—H39119.9
H14A—C14—H14B109.5C41—C40—C39121.1 (9)
C13—C14—H14C109.5C41—C40—H40119.5
H14A—C14—H14C109.5C39—C40—H40119.5
H14B—C14—H14C109.5C40—C41—C42118.9 (10)
C13—C15—H15A109.5C40—C41—H41120.6
C13—C15—H15B109.5C42—C41—H41120.6
H15A—C15—H15B109.5C37—C42—C41121.0 (8)
C13—C15—H15C109.5C37—C42—H42119.5
H15A—C15—H15C109.5C41—C42—H42119.5
H15B—C15—H15C109.5C48—C43—C44119.8 (6)
C13—C16—H16A109.5C48—C43—C32120.8 (5)
C13—C16—H16B109.5C44—C43—C32119.4 (6)
H16A—C16—H16B109.5C45—C44—C43118.3 (6)
C13—C16—H16C109.5C45—C44—H44120.8
H16A—C16—H16C109.5C43—C44—H44120.8
H16B—C16—H16C109.5C46—C45—C44121.6 (6)
O4A—C13A—C14A113 (5)C46—C45—H45119.2
O4A—C13A—C16A110 (4)C44—C45—H45119.2
C14A—C13A—C16A118 (6)C45—C46—C47119.8 (7)
O4A—C13A—C15A107 (3)C45—C46—H46120.1
C14A—C13A—C15A99 (5)C47—C46—H46120.1
C16A—C13A—C15A109 (5)C48—C47—C46119.2 (7)
C13A—C14A—H14D109.5C48—C47—H47120.4
C13A—C14A—H14E109.5C46—C47—H47120.4
H14D—C14A—H14E109.5C43—C48—C47121.3 (6)
C13A—C14A—H14F109.5C43—C48—H48119.3
H14D—C14A—H14F109.5C47—C48—H48119.3
H14E—C14A—H14F109.5C51i—C49—C50119.6 (10)
C13A—C15A—H15D109.5C51i—C49—H49120.2
C13A—C15A—H15E109.5C50—C49—H49120.2
H15D—C15A—H15E109.5C51—C50—C49119.7 (10)
C13A—C15A—H15F109.5C51—C50—H50120.2
H15D—C15A—H15F109.5C49—C50—H50120.2
H15E—C15A—H15F109.5C50—C51—C49i120.7 (9)
C13A—C16A—H16D109.5C50—C51—H51119.7
C13A—C16A—H16E109.4C49i—C51—H51119.7
Symmetry code: (i) x+1, y+1, z+1.

Experimental details

(I)(II)
Crystal data
Chemical formula[Pb(C12H27O3SSi)2(C10H8N2)][Pb(C12H27O3SSi)2(C24H16N2)]·0.5C6H6
Mr922.351137.6
Crystal system, space groupTriclinic, P1Triclinic, P1
Temperature (K)120293
a, b, c (Å)9.4053 (4), 13.8617 (7), 18.0405 (9)10.204 (2), 13.359 (3), 21.109 (4)
α, β, γ (°)107.361 (5), 99.069 (4), 101.086 (4)84.57 (3), 83.05 (3), 85.29 (3)
V3)2144.1 (2)2836.2 (10)
Z22
Radiation typeMo KαMo Kα
µ (mm1)4.133.13
Crystal size (mm)0.49 × 0.13 × 0.090.6 × 0.41 × 0.32
Data collection
DiffractometerOxford Diffraction KM4 CCD
diffractometer
Oxford Diffraction KM4 single-point
diffractometer
Absorption correctionMulti-scan
(CrysAlis RED; Oxford Diffraction, 2006)
ψ scan
(North et al., 1968)
Tmin, Tmax0.503, 0.6950.198, 0.359
No. of measured, independent and
observed [I > 2σ(I)] reflections
17997, 10174, 9037 10564, 10091, 7445
Rint0.0300.053
(sin θ/λ)max1)0.6610.597
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.040, 0.099, 1.16 0.037, 0.118, 1.00
No. of reflections1017410091
No. of parameters442648
No. of restraints0115
H-atom treatmentH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)2.11, 1.550.84, 0.80

Computer programs: CrysAlis CCD (Oxford Diffraction, 2006), KM4 System (Gałdecki, Kowalski et al., 1996), CrysAlis RED (Oxford Diffraction, 2006), KM4 System, CrysAlis RED, DATAPROC (Gałdecki, Kowalski & Uszyński, 1996), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), Mercury (Version 1.5; Macrae et al., 2006), WinGX (Farrugia, 1999).

Selected geometric parameters (Å, º) for (I) top
Pb1—N12.610 (4)Si1—O31.625 (3)
Pb1—S22.6705 (11)Si1—O21.627 (3)
Pb1—S12.7034 (13)Si1—O11.633 (3)
Pb1—N22.725 (4)Si2—O51.628 (3)
S1—Si12.0730 (17)Si2—O61.632 (3)
S2—Si22.0861 (16)Si2—O41.641 (3)
N1—Pb1—S295.78 (10)S2—Pb1—N285.70 (9)
N1—Pb1—S186.96 (11)S1—Pb1—N2145.90 (9)
S2—Pb1—S187.14 (4)Si1—S1—Pb197.90 (5)
N1—Pb1—N260.74 (14)Si2—S2—Pb194.17 (5)
Selected geometric parameters (Å, º) for (II) top
Pb1—N12.594 (5)Pb1—N22.801 (5)
Pb1—S22.6331 (18)S1—Si12.075 (2)
Pb1—S12.6976 (18)S2—Si22.071 (2)
N1—Pb1—S287.77 (11)S2—Pb1—N281.17 (11)
N1—Pb1—S189.44 (11)S1—Pb1—N2148.25 (10)
S2—Pb1—S188.41 (6)Si1—S1—Pb199.04 (9)
N1—Pb1—N260.42 (14)Si2—S2—Pb194.28 (8)
ππ and C—H···π contacts (Å, °) for (I) and (II) top
CompoundGroup 1/Group 2DA (°)DCC/DCH (Å)τ (°)
(I)Cg1/Cg2i5.63.797 (4)24, 31
(II)Cg3/Cg3ii0.03.717 (5)17.1
(II)C51—H51/Cg42.9813.6
(II)C48—H48/Cg52.816.6
DA is the dihedral angle between planes. DCC is the length of the CC (centroid-to-centroid) vector in ππ. DCH is the length of the CH (centroid to H) vector in C—H···π. τ is the angle(s) subtended by the plane normal(s) to CC or CH.

Cg1 is the centroid of the ring N1/C30–C34, Cg2 of the ring N2/C25–C9, Cg3 of the ring C37–C42, Cg4 of the ring C28–C31/C35–C36 and Cg5 of the ring C49–C51/(C49–C51)iii

Symmetry codes: (i) 1-x, 2-y, -z; (ii) -x, 2-y, 1-z; (iii) 1-x, 1-y, 1-z.
 

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