supplementary materials


qm2044 scheme

Acta Cryst. (2012). E68, m62-m63    [ doi:10.1107/S1600536811053591 ]

(N-Ethyl-N-phenyldithiocarbamato-[kappa]S)triphenyltin(IV)

N. F. Kamaludin, I. Baba, N. Awang, M. I. Mohamed Tahir and E. R. T. Tiekink

Abstract top

The title compound, [Sn(C6H5)3(C9H10NS2)], has two independent molecules in the asymmetric unit and each features a tetrahedrally coordinated SnIV atom as the dithiocarbamate ligand coordinates in a monodentate fashion. As the non-coordinating thione S atom is proximate to the Sn atom [Sn...S(thione) = 3.1477 (6) and 2.9970 (5) Å for the independent molecules], distortions from the ideal geometry are evident [the widest angle being 120.48 (5)°]. The most notable feature of the crystal packing is the formation of C-H...[pi] interactions that lead to the formation of supramolecular layers parallel to (\overline{3}2\overline{1}).

Comment top

Potential applications as anti-cancer agents, anti-microbials and insecticides, and as convenient synthetic precursors for tin sulfide nanoparticles, characterize organotin dithiocarbamates (Tiekink, 2008). This background motivates our interest in this class of compound and led to the investigation of the title compound, (I). Recently, the structure of the n-butyl derivative was described (Kamaludin et al., 2011) and herein, we describe the analysis of (I).

There are two independent molecules in the asymmetric unit of (I): the molecular structures are shown in Fig. 1. Each molecule features Sn coordinated by the dithiocarbamate ligand and three ipso-C atoms of three benzene rings. The dithiocarbamate ligand coordinates essentially in a monodentate fashion, an assignment supported by the large disparity in the C—S bond distances, Table 1. The coordination geometry is based on a tetrahedron with the range of tetrahedral angles being 94.46 (5) to 120.48 (5)° for the Sn1-containing molecule and 95.28 (5) to 118.66 (5)° for the other. The wider angles are ascribed to the influence of the proximate thione-S atom [Sn1···S2 = 3.1477 (6) Å and Sn2···S4 = 2.9970 (5) Å]. The major differences between the independent molecules is highlighted in the overlay diagram, Fig. 2, showing that the chemically equivalent phenyl rings do not overlap significantly.

The crystal packing of (I) features C—H···π interactions involving the Sn- and N-phenyl rings as donors, and Sn-bound phenyl rings as acceptors, Table 2. The result is the formation of supramolecular layers parallel to (3 2 1), Fig. 3.

Related literature top

For a review on the applications and structural chemistry of tin dithiocarbamates, see: Tiekink (2008). For the recently reported n-butyl derivative, see: Kamaludin et al. (2011).

Experimental top

The title compound was prepared using an in situ method. A mixture of ethanol (50 ml) and N-ethylaniline (30 mM) was added to an ammonia solution (0.25%). The solution was stirred for half an hour at approximately 277 K. Carbon disulfide (30 mM) was added drop-wise and stirring was continued for another 6–8 h at 277 K. Triphenytin(IV) chloride (30 mM), dissolved in ethanol (20 ml), was added and stirring continued for a further 3 h. The white precipitate formed was filtered, washed with cold ethanol and dried in a vacuum desiccator. Recrystallization was from its ethanol:ethyl acetate (1:1) solution. Yield: 32%. M.pt. 381–382 K. Elemental analysis. Found (calculated) for C27H25NS2Sn: C, 59.19 (59.36); H 4.33 (4.61); N 2.52 (2.56); S 11.30 (11.74) %. IR (KBr): ν(C—H) 2986 m; ν(CN) 1478 m; ν(N—C) 1125 s; ν(CS) 997 s; ν(Sn—S) 357 s cm-1. 13C NMR (CDCl3): δ (CS2) 198.63 p.p.m..

Refinement top

Carbon-bound H-atoms were placed in calculated positions (C—H 0.95 to 0.99 Å) and were included in the refinement in the riding model approximation, with Uiso(H) set to 1.2 to 1.5Uequiv(C).

Computing details top

Data collection: CrysAlis PRO (Oxford Diffraction, 2010); cell refinement: CrysAlis PRO (Oxford Diffraction, 2010); data reduction: CrysAlis PRO (Oxford Diffraction, 2010); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997), DIAMOND (Brandenburg, 2006) and QMol (Gans & Shalloway, 2001); software used to prepare material for publication: publCIF (Westrip, 2010).

Figures top
[Figure 1] Fig. 1. The molecular structure of the two independent molecules comprising (I) showing the atom-labelling scheme and displacement ellipsoids at the 50% probability level.
[Figure 2] Fig. 2. An overlay diagram of the two independent molecules comprising (I) aligned so that the Sn—S—C planes are superimposed. The red image illustrates the molecule containing the Sn1 atom.
[Figure 3] Fig. 3. A view of the supramolecular layer parallel to [3 2 1] in (I) mediated by C—H···π interactions (purple dashed lines).
(N-Ethyl-N-phenyldithiocarbamato-κS)triphenyltin(IV) top
Crystal data top
[Sn(C6H5)3(C9H10NS2)]Z = 4
Mr = 546.29F(000) = 1104
Triclinic, P1Dx = 1.461 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 9.6973 (2) ÅCell parameters from 39367 reflections
b = 12.2804 (2) Åθ = 2–29°
c = 22.8523 (4) ŵ = 1.21 mm1
α = 90.588 (2)°T = 150 K
β = 101.573 (2)°Block, colourless
γ = 110.687 (2)°0.30 × 0.24 × 0.19 mm
V = 2484.39 (8) Å3
Data collection top
Oxford Diffraction Xcaliber Eos Gemini
diffractometer
10558 independent reflections
Radiation source: fine-focus sealed tube9633 reflections with I > 2σ(I)
graphiteRint = 0.038
Detector resolution: 16.1952 pixels mm-1θmax = 26.8°, θmin = 2.3°
ω scansh = 1212
Absorption correction: multi-scan
(CrysAlis PRO; Oxford Diffraction, 2010)
k = 1515
Tmin = 0.748, Tmax = 0.795l = 2828
62467 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)] = 0.022Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.055H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.0259P)2 + 1.489P]
where P = (Fo2 + 2Fc2)/3
10558 reflections(Δ/σ)max = 0.004
561 parametersΔρmax = 0.55 e Å3
0 restraintsΔρmin = 0.44 e Å3
Crystal data top
[Sn(C6H5)3(C9H10NS2)]γ = 110.687 (2)°
Mr = 546.29V = 2484.39 (8) Å3
Triclinic, P1Z = 4
a = 9.6973 (2) ÅMo Kα radiation
b = 12.2804 (2) ŵ = 1.21 mm1
c = 22.8523 (4) ÅT = 150 K
α = 90.588 (2)°0.30 × 0.24 × 0.19 mm
β = 101.573 (2)°
Data collection top
Oxford Diffraction Xcaliber Eos Gemini
diffractometer
10558 independent reflections
Absorption correction: multi-scan
(CrysAlis PRO; Oxford Diffraction, 2010)
9633 reflections with I > 2σ(I)
Tmin = 0.748, Tmax = 0.795Rint = 0.038
62467 measured reflectionsθmax = 26.8°
Refinement top
R[F2 > 2σ(F2)] = 0.022H-atom parameters constrained
wR(F2) = 0.055Δρmax = 0.55 e Å3
S = 1.00Δρmin = 0.44 e Å3
10558 reflectionsAbsolute structure: ?
561 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
Special details top

Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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
Sn10.425600 (14)0.868539 (11)0.613068 (5)0.02407 (4)
S10.25460 (6)0.77901 (4)0.51651 (2)0.02845 (10)
S20.39527 (6)0.61380 (5)0.57263 (2)0.03395 (11)
N10.2447 (2)0.58873 (15)0.45887 (7)0.0337 (4)
C10.2955 (2)0.65087 (17)0.51249 (8)0.0284 (4)
C20.2836 (3)0.4851 (2)0.44586 (11)0.0478 (6)
H2A0.38310.49440.47150.057*
H2B0.29230.48150.40350.057*
C30.1682 (3)0.3731 (2)0.45672 (13)0.0614 (8)
H3A0.16780.37230.49960.092*
H3B0.19310.30710.44390.092*
H3C0.06820.36630.43380.092*
C40.1517 (2)0.62092 (17)0.40950 (8)0.0314 (4)
C50.0031 (3)0.5806 (2)0.40371 (10)0.0386 (5)
H50.04820.53330.43240.046*
C60.0915 (3)0.6096 (2)0.35598 (11)0.0510 (6)
H60.19800.58230.35170.061*
C70.0259 (4)0.6780 (3)0.31455 (11)0.0610 (8)
H70.08710.69850.28190.073*
C80.1281 (4)0.7169 (2)0.32016 (11)0.0602 (8)
H80.17250.76360.29110.072*
C90.2197 (3)0.6885 (2)0.36788 (10)0.0440 (5)
H90.32600.71490.37170.053*
C100.6605 (2)0.89709 (18)0.62716 (8)0.0293 (4)
C110.7603 (2)0.9959 (2)0.60893 (10)0.0408 (5)
H110.72391.05070.58850.049*
C120.9148 (3)1.0149 (3)0.62057 (13)0.0574 (7)
H120.98281.08150.60720.069*
C130.9681 (3)0.9371 (3)0.65134 (14)0.0624 (8)
H131.07300.95030.65910.075*
C140.8709 (3)0.8402 (2)0.67092 (12)0.0517 (7)
H140.90860.78770.69290.062*
C150.7171 (2)0.8197 (2)0.65846 (9)0.0359 (5)
H150.64990.75210.67140.043*
C160.4002 (2)1.03524 (16)0.60391 (8)0.0271 (4)
C170.3810 (2)1.09529 (17)0.65201 (9)0.0332 (4)
H170.38291.06320.68970.040*
C180.3592 (3)1.20067 (19)0.64607 (10)0.0408 (5)
H180.34651.23990.67950.049*
C190.3559 (3)1.24854 (19)0.59177 (11)0.0421 (5)
H190.34121.32080.58770.051*
C200.3740 (3)1.1909 (2)0.54327 (10)0.0415 (5)
H200.37161.22350.50570.050*
C210.3956 (2)1.08579 (19)0.54950 (9)0.0350 (5)
H210.40771.04690.51580.042*
C220.3337 (2)0.80327 (17)0.68794 (8)0.0268 (4)
C230.1960 (2)0.7136 (2)0.68340 (10)0.0386 (5)
H230.14160.67160.64570.046*
C240.1371 (3)0.6849 (2)0.73484 (14)0.0581 (7)
H240.04230.62370.73210.070*
C250.2182 (4)0.7465 (3)0.78978 (12)0.0635 (8)
H250.17740.72820.82450.076*
C260.3555 (4)0.8328 (2)0.79434 (11)0.0593 (8)
H260.41170.87300.83220.071*
C270.4122 (3)0.8612 (2)0.74395 (9)0.0410 (5)
H270.50760.92210.74740.049*
Sn20.849644 (14)0.767651 (10)0.914470 (5)0.02217 (4)
S30.73045 (6)0.77465 (4)0.99945 (2)0.02867 (10)
S40.82367 (6)0.56918 (4)0.99206 (2)0.03252 (11)
N20.71753 (19)0.62538 (13)1.08192 (7)0.0289 (3)
C280.7555 (2)0.65068 (16)1.02941 (8)0.0257 (4)
C290.7378 (3)0.52486 (19)1.11280 (11)0.0483 (6)
H29A0.71940.46011.08260.058*
H29B0.66300.49701.13820.058*
C300.8959 (4)0.5582 (3)1.15146 (13)0.0726 (9)
H30A0.96960.57831.12580.109*
H30B0.90350.49211.17380.109*
H30C0.91680.62561.17970.109*
C310.6641 (2)0.69863 (16)1.11445 (8)0.0273 (4)
C320.7662 (2)0.79839 (17)1.14875 (9)0.0335 (4)
H320.87110.82171.14970.040*
C330.7126 (3)0.86425 (19)1.18188 (10)0.0409 (5)
H330.78110.93301.20590.049*
C340.5593 (3)0.8294 (2)1.17981 (10)0.0420 (5)
H340.52270.87471.20220.050*
C350.4607 (3)0.7303 (2)1.14582 (11)0.0440 (5)
H350.35570.70721.14470.053*
C360.5116 (2)0.66293 (19)1.11289 (10)0.0360 (5)
H360.44270.59341.08970.043*
C371.0884 (2)0.80657 (15)0.93488 (8)0.0225 (4)
C381.1777 (2)0.91710 (16)0.92315 (8)0.0251 (4)
H381.13140.97080.90840.030*
C391.3336 (2)0.95029 (17)0.93266 (8)0.0297 (4)
H391.39311.02610.92440.036*
C401.4021 (2)0.87260 (18)0.95422 (9)0.0313 (4)
H401.50860.89470.96050.038*
C411.3150 (2)0.76280 (18)0.96660 (9)0.0320 (4)
H411.36210.70990.98180.038*
C421.1587 (2)0.72925 (17)0.95689 (8)0.0284 (4)
H421.09970.65340.96530.034*
C430.8300 (2)0.92594 (16)0.88000 (8)0.0249 (4)
C440.8243 (2)1.01716 (18)0.91533 (9)0.0329 (4)
H440.82661.01010.95680.040*
C450.8153 (3)1.1176 (2)0.89075 (10)0.0413 (5)
H450.81091.17860.91540.050*
C460.8125 (2)1.12962 (18)0.83056 (9)0.0350 (5)
H460.80521.19830.81370.042*
C470.8206 (2)1.04148 (18)0.79481 (9)0.0330 (4)
H470.82051.04990.75350.040*
C480.8287 (2)0.94077 (17)0.81961 (8)0.0300 (4)
H480.83350.88030.79470.036*
C490.7240 (2)0.64207 (16)0.83962 (8)0.0285 (4)
C500.5873 (3)0.6435 (2)0.80722 (10)0.0440 (5)
H500.54360.69370.82150.053*
C510.5138 (3)0.5727 (2)0.75430 (12)0.0630 (8)
H510.41970.57410.73290.076*
C520.5760 (4)0.5013 (2)0.73294 (12)0.0695 (10)
H520.52610.45390.69630.083*
C530.7108 (4)0.4976 (2)0.76434 (13)0.0670 (9)
H530.75370.44740.74940.080*
C540.7849 (3)0.5676 (2)0.81818 (11)0.0456 (6)
H540.87720.56390.84010.055*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sn10.02483 (7)0.02598 (7)0.01999 (7)0.00680 (5)0.00633 (5)0.00045 (5)
S10.0337 (3)0.0290 (2)0.0217 (2)0.0118 (2)0.00338 (19)0.00109 (18)
S20.0372 (3)0.0334 (3)0.0284 (2)0.0131 (2)0.0004 (2)0.0015 (2)
N10.0406 (10)0.0317 (9)0.0273 (8)0.0143 (8)0.0021 (7)0.0043 (7)
C10.0275 (10)0.0282 (10)0.0256 (9)0.0054 (8)0.0061 (8)0.0005 (7)
C20.0574 (15)0.0529 (15)0.0401 (13)0.0336 (13)0.0016 (11)0.0077 (11)
C30.0743 (19)0.0410 (14)0.0637 (18)0.0265 (14)0.0058 (15)0.0103 (12)
C40.0423 (12)0.0292 (10)0.0209 (9)0.0136 (9)0.0017 (8)0.0057 (7)
C50.0437 (13)0.0378 (12)0.0331 (11)0.0155 (10)0.0043 (9)0.0046 (9)
C60.0518 (15)0.0561 (15)0.0439 (14)0.0285 (13)0.0079 (11)0.0133 (12)
C70.094 (2)0.0664 (18)0.0312 (13)0.0537 (18)0.0121 (14)0.0081 (12)
C80.105 (3)0.0555 (16)0.0303 (12)0.0382 (17)0.0208 (14)0.0141 (11)
C90.0528 (14)0.0423 (13)0.0371 (12)0.0143 (11)0.0156 (11)0.0035 (10)
C100.0262 (10)0.0353 (11)0.0235 (9)0.0072 (8)0.0067 (7)0.0044 (8)
C110.0342 (11)0.0423 (12)0.0364 (12)0.0015 (10)0.0102 (9)0.0028 (9)
C120.0339 (13)0.0641 (17)0.0583 (16)0.0058 (12)0.0190 (12)0.0106 (13)
C130.0251 (12)0.085 (2)0.0691 (18)0.0136 (13)0.0054 (12)0.0264 (16)
C140.0388 (13)0.0656 (17)0.0501 (14)0.0266 (13)0.0048 (11)0.0192 (12)
C150.0327 (11)0.0408 (12)0.0313 (11)0.0131 (9)0.0017 (8)0.0062 (9)
C160.0255 (9)0.0253 (9)0.0284 (10)0.0057 (8)0.0077 (8)0.0004 (7)
C170.0392 (11)0.0293 (10)0.0294 (10)0.0074 (9)0.0133 (9)0.0011 (8)
C180.0484 (13)0.0341 (11)0.0426 (12)0.0136 (10)0.0187 (10)0.0035 (9)
C190.0488 (13)0.0317 (11)0.0518 (14)0.0192 (10)0.0158 (11)0.0055 (10)
C200.0521 (14)0.0416 (12)0.0377 (12)0.0227 (11)0.0139 (10)0.0119 (10)
C210.0427 (12)0.0358 (11)0.0295 (10)0.0157 (10)0.0119 (9)0.0030 (8)
C220.0322 (10)0.0313 (10)0.0222 (9)0.0163 (8)0.0085 (8)0.0059 (7)
C230.0366 (12)0.0419 (12)0.0376 (12)0.0122 (10)0.0116 (9)0.0128 (9)
C240.0554 (16)0.0576 (16)0.075 (2)0.0238 (14)0.0380 (15)0.0376 (15)
C250.106 (3)0.0722 (19)0.0443 (15)0.0525 (19)0.0494 (17)0.0245 (14)
C260.105 (2)0.0549 (16)0.0273 (12)0.0363 (17)0.0212 (14)0.0058 (11)
C270.0556 (14)0.0401 (12)0.0254 (10)0.0173 (11)0.0050 (10)0.0002 (9)
Sn20.02496 (7)0.02192 (7)0.01935 (6)0.00797 (5)0.00520 (5)0.00102 (5)
S30.0357 (3)0.0334 (3)0.0260 (2)0.0199 (2)0.0129 (2)0.00964 (19)
S40.0459 (3)0.0260 (2)0.0315 (3)0.0154 (2)0.0169 (2)0.00464 (19)
N20.0399 (9)0.0213 (8)0.0287 (8)0.0100 (7)0.0164 (7)0.0061 (6)
C280.0257 (9)0.0238 (9)0.0252 (9)0.0054 (8)0.0066 (7)0.0018 (7)
C290.0849 (19)0.0261 (11)0.0492 (14)0.0252 (12)0.0386 (14)0.0172 (10)
C300.122 (3)0.0634 (19)0.0487 (16)0.059 (2)0.0063 (17)0.0182 (14)
C310.0375 (11)0.0254 (9)0.0216 (9)0.0116 (8)0.0119 (8)0.0063 (7)
C320.0340 (11)0.0281 (10)0.0365 (11)0.0086 (9)0.0081 (9)0.0031 (8)
C330.0569 (15)0.0311 (11)0.0318 (11)0.0141 (10)0.0072 (10)0.0033 (9)
C340.0608 (15)0.0445 (13)0.0341 (11)0.0281 (12)0.0233 (11)0.0073 (10)
C350.0404 (13)0.0488 (14)0.0498 (14)0.0173 (11)0.0231 (11)0.0099 (11)
C360.0363 (11)0.0335 (11)0.0346 (11)0.0063 (9)0.0113 (9)0.0027 (9)
C370.0259 (9)0.0247 (9)0.0173 (8)0.0100 (7)0.0042 (7)0.0011 (7)
C380.0295 (10)0.0253 (9)0.0210 (9)0.0117 (8)0.0031 (7)0.0005 (7)
C390.0287 (10)0.0296 (10)0.0259 (9)0.0052 (8)0.0050 (8)0.0004 (8)
C400.0258 (10)0.0387 (11)0.0267 (10)0.0117 (9)0.0002 (8)0.0069 (8)
C410.0349 (11)0.0341 (11)0.0290 (10)0.0190 (9)0.0002 (8)0.0031 (8)
C420.0346 (10)0.0243 (9)0.0272 (9)0.0123 (8)0.0054 (8)0.0007 (7)
C430.0243 (9)0.0270 (9)0.0234 (9)0.0101 (8)0.0038 (7)0.0019 (7)
C440.0471 (12)0.0356 (11)0.0222 (9)0.0210 (10)0.0098 (9)0.0026 (8)
C450.0644 (15)0.0368 (12)0.0362 (12)0.0303 (11)0.0188 (11)0.0054 (9)
C460.0422 (12)0.0311 (11)0.0366 (11)0.0179 (9)0.0105 (9)0.0110 (9)
C470.0391 (11)0.0333 (11)0.0224 (9)0.0100 (9)0.0034 (8)0.0052 (8)
C480.0391 (11)0.0259 (10)0.0228 (9)0.0090 (8)0.0071 (8)0.0003 (7)
C490.0334 (10)0.0222 (9)0.0230 (9)0.0011 (8)0.0072 (8)0.0007 (7)
C500.0428 (13)0.0346 (12)0.0420 (13)0.0060 (10)0.0040 (10)0.0021 (10)
C510.0662 (18)0.0442 (15)0.0438 (14)0.0060 (13)0.0172 (13)0.0028 (12)
C520.092 (2)0.0412 (15)0.0336 (13)0.0187 (15)0.0006 (14)0.0061 (11)
C530.095 (2)0.0418 (15)0.0559 (17)0.0058 (15)0.0331 (17)0.0173 (13)
C540.0497 (14)0.0393 (13)0.0450 (13)0.0111 (11)0.0139 (11)0.0103 (10)
Geometric parameters (Å, °) top
Sn1—C102.1339 (19)Sn2—C372.1413 (18)
Sn1—C162.1541 (19)Sn2—C432.1605 (19)
Sn1—C222.1210 (18)Sn2—C492.1379 (19)
Sn1—S12.4539 (5)Sn2—S32.4662 (5)
S1—C11.759 (2)S3—C281.7496 (19)
S2—C11.680 (2)S4—C281.6862 (19)
N1—C11.342 (2)N2—C281.333 (2)
N1—C41.448 (3)N2—C311.449 (2)
N1—C21.492 (3)N2—C291.481 (3)
C2—C31.496 (4)C29—C301.518 (4)
C2—H2A0.9900C29—H29A0.9900
C2—H2B0.9900C29—H29B0.9900
C3—H3A0.9800C30—H30A0.9800
C3—H3B0.9800C30—H30B0.9800
C3—H3C0.9800C30—H30C0.9800
C4—C91.382 (3)C31—C321.381 (3)
C4—C51.382 (3)C31—C361.379 (3)
C5—C61.379 (3)C32—C331.393 (3)
C5—H50.9500C32—H320.9500
C6—C71.374 (4)C33—C341.384 (3)
C6—H60.9500C33—H330.9500
C7—C81.376 (4)C34—C351.363 (3)
C7—H70.9500C34—H340.9500
C8—C91.391 (4)C35—C361.386 (3)
C8—H80.9500C35—H350.9500
C9—H90.9500C36—H360.9500
C10—C151.393 (3)C37—C381.391 (3)
C10—C111.388 (3)C37—C421.396 (3)
C11—C121.400 (3)C38—C391.389 (3)
C11—H110.9500C38—H380.9500
C12—C131.375 (4)C39—C401.386 (3)
C12—H120.9500C39—H390.9500
C13—C141.375 (4)C40—C411.382 (3)
C13—H130.9500C40—H400.9500
C14—C151.389 (3)C41—C421.392 (3)
C14—H140.9500C41—H410.9500
C15—H150.9500C42—H420.9500
C16—C171.396 (3)C43—C481.392 (3)
C16—C211.395 (3)C43—C441.398 (3)
C17—C181.387 (3)C44—C451.384 (3)
C17—H170.9500C44—H440.9500
C18—C191.378 (3)C45—C461.381 (3)
C18—H180.9500C45—H450.9500
C19—C201.382 (3)C46—C471.383 (3)
C19—H190.9500C46—H460.9500
C20—C211.384 (3)C47—C481.386 (3)
C20—H200.9500C47—H470.9500
C21—H210.9500C48—H480.9500
C22—C271.390 (3)C49—C501.389 (3)
C22—C231.382 (3)C49—C541.384 (3)
C23—C241.403 (3)C50—C511.386 (3)
C23—H230.9500C50—H500.9500
C24—C251.390 (4)C51—C521.362 (5)
C24—H240.9500C51—H510.9500
C25—C261.361 (4)C52—C531.376 (5)
C25—H250.9500C52—H520.9500
C26—C271.370 (3)C53—C541.398 (4)
C26—H260.9500C53—H530.9500
C27—H270.9500C54—H540.9500
C22—Sn1—C10112.49 (7)C49—Sn2—C37115.41 (7)
C22—Sn1—C16105.17 (7)C49—Sn2—C43101.51 (7)
C10—Sn1—C16108.02 (8)C37—Sn2—C43103.22 (7)
C22—Sn1—S1113.28 (6)C49—Sn2—S3118.66 (5)
C10—Sn1—S1120.48 (5)C37—Sn2—S3117.12 (5)
C16—Sn1—S194.46 (5)C43—Sn2—S395.28 (5)
C1—S1—Sn198.20 (7)C28—S3—Sn295.09 (6)
C1—N1—C4121.45 (17)C28—N2—C31122.39 (15)
C1—N1—C2122.48 (18)C28—N2—C29121.82 (16)
C4—N1—C2116.05 (16)C31—N2—C29115.65 (15)
N1—C1—S2123.77 (16)N2—C28—S4123.09 (14)
N1—C1—S1115.59 (15)N2—C28—S3116.67 (14)
S2—C1—S1120.63 (11)S4—C28—S3120.24 (11)
N1—C2—C3112.3 (2)N2—C29—C30111.3 (2)
N1—C2—H2A109.1N2—C29—H29A109.4
C3—C2—H2A109.1C30—C29—H29A109.4
N1—C2—H2B109.1N2—C29—H29B109.4
C3—C2—H2B109.1C30—C29—H29B109.4
H2A—C2—H2B107.9H29A—C29—H29B108.0
C2—C3—H3A109.5C29—C30—H30A109.5
C2—C3—H3B109.5C29—C30—H30B109.5
H3A—C3—H3B109.5H30A—C30—H30B109.5
C2—C3—H3C109.5C29—C30—H30C109.5
H3A—C3—H3C109.5H30A—C30—H30C109.5
H3B—C3—H3C109.5H30B—C30—H30C109.5
C9—C4—C5121.3 (2)C32—C31—C36121.41 (19)
C9—C4—N1119.0 (2)C32—C31—N2119.92 (18)
C5—C4—N1119.70 (19)C36—C31—N2118.56 (18)
C6—C5—C4119.5 (2)C31—C32—C33118.8 (2)
C6—C5—H5120.2C31—C32—H32120.6
C4—C5—H5120.2C33—C32—H32120.6
C7—C6—C5120.1 (3)C34—C33—C32119.9 (2)
C7—C6—H6120.0C34—C33—H33120.0
C5—C6—H6120.0C32—C33—H33120.0
C8—C7—C6120.2 (2)C35—C34—C33120.3 (2)
C8—C7—H7119.9C35—C34—H34119.9
C6—C7—H7119.9C33—C34—H34119.9
C7—C8—C9120.8 (3)C34—C35—C36120.8 (2)
C7—C8—H8119.6C34—C35—H35119.6
C9—C8—H8119.6C36—C35—H35119.6
C4—C9—C8118.2 (2)C31—C36—C35118.8 (2)
C4—C9—H9120.9C31—C36—H36120.6
C8—C9—H9120.9C35—C36—H36120.6
C15—C10—C11118.9 (2)C38—C37—C42118.60 (17)
C15—C10—Sn1119.93 (15)C38—C37—Sn2116.12 (13)
C11—C10—Sn1121.02 (16)C42—C37—Sn2125.26 (14)
C10—C11—C12120.0 (2)C39—C38—C37121.05 (17)
C10—C11—H11120.0C39—C38—H38119.5
C12—C11—H11120.0C37—C38—H38119.5
C13—C12—C11120.0 (3)C38—C39—C40119.83 (19)
C13—C12—H12120.0C38—C39—H39120.1
C11—C12—H12120.0C40—C39—H39120.1
C12—C13—C14120.6 (2)C41—C40—C39119.82 (19)
C12—C13—H13119.7C41—C40—H40120.1
C14—C13—H13119.7C39—C40—H40120.1
C13—C14—C15119.7 (3)C40—C41—C42120.42 (18)
C13—C14—H14120.2C40—C41—H41119.8
C15—C14—H14120.2C42—C41—H41119.8
C10—C15—C14120.8 (2)C41—C42—C37120.28 (18)
C10—C15—H15119.6C41—C42—H42119.9
C14—C15—H15119.6C37—C42—H42119.9
C17—C16—C21116.95 (18)C48—C43—C44117.55 (17)
C17—C16—Sn1121.01 (14)C48—C43—Sn2118.58 (13)
C21—C16—Sn1121.99 (14)C44—C43—Sn2123.82 (14)
C18—C17—C16121.53 (19)C45—C44—C43121.00 (18)
C18—C17—H17119.2C45—C44—H44119.5
C16—C17—H17119.2C43—C44—H44119.5
C19—C18—C17120.1 (2)C44—C45—C46120.29 (19)
C19—C18—H18120.0C44—C45—H45119.9
C17—C18—H18120.0C46—C45—H45119.9
C20—C19—C18119.7 (2)C47—C46—C45119.88 (19)
C20—C19—H19120.1C47—C46—H46120.1
C18—C19—H19120.1C45—C46—H46120.1
C19—C20—C21119.9 (2)C46—C47—C48119.56 (18)
C19—C20—H20120.1C46—C47—H47120.2
C21—C20—H20120.1C48—C47—H47120.2
C20—C21—C16121.82 (19)C43—C48—C47121.71 (18)
C20—C21—H21119.1C43—C48—H48119.1
C16—C21—H21119.1C47—C48—H48119.1
C27—C22—C23118.84 (19)C50—C49—C54118.5 (2)
C27—C22—Sn1117.20 (16)C50—C49—Sn2120.19 (16)
C23—C22—Sn1123.75 (15)C54—C49—Sn2120.84 (16)
C22—C23—C24119.6 (2)C51—C50—C49120.9 (3)
C22—C23—H23120.2C51—C50—H50119.5
C24—C23—H23120.2C49—C50—H50119.5
C25—C24—C23119.7 (3)C52—C51—C50120.1 (3)
C25—C24—H24120.2C52—C51—H51119.9
C23—C24—H24120.2C50—C51—H51119.9
C26—C25—C24120.6 (2)C51—C52—C53120.1 (2)
C26—C25—H25119.7C51—C52—H52119.9
C24—C25—H25119.7C53—C52—H52119.9
C25—C26—C27119.6 (3)C52—C53—C54120.2 (3)
C25—C26—H26120.2C52—C53—H53119.9
C27—C26—H26120.2C54—C53—H53119.9
C26—C27—C22121.7 (2)C53—C54—C49120.1 (3)
C26—C27—H27119.1C53—C54—H54120.0
C22—C27—H27119.1C49—C54—H54120.0
C22—Sn1—S1—C182.34 (8)C49—Sn2—S3—C2876.70 (9)
C10—Sn1—S1—C155.09 (9)C37—Sn2—S3—C2869.32 (8)
C16—Sn1—S1—C1169.04 (8)C43—Sn2—S3—C28177.10 (8)
C4—N1—C1—S2176.31 (16)C31—N2—C28—S4177.77 (15)
C2—N1—C1—S25.4 (3)C29—N2—C28—S42.3 (3)
C4—N1—C1—S15.0 (3)C31—N2—C28—S32.6 (3)
C2—N1—C1—S1173.26 (17)C29—N2—C28—S3178.10 (17)
Sn1—S1—C1—N1166.86 (14)Sn2—S3—C28—N2174.02 (14)
Sn1—S1—C1—S211.88 (12)Sn2—S3—C28—S46.32 (12)
C1—N1—C2—C392.9 (3)C28—N2—C29—C3086.3 (3)
C4—N1—C2—C388.7 (2)C31—N2—C29—C3089.5 (2)
C1—N1—C4—C995.5 (2)C28—N2—C31—C3280.5 (2)
C2—N1—C4—C982.9 (3)C29—N2—C31—C3295.2 (2)
C1—N1—C4—C586.6 (2)C28—N2—C31—C36103.0 (2)
C2—N1—C4—C595.0 (2)C29—N2—C31—C3681.2 (2)
C9—C4—C5—C60.9 (3)C36—C31—C32—C330.6 (3)
N1—C4—C5—C6178.75 (19)N2—C31—C32—C33176.94 (18)
C4—C5—C6—C70.0 (3)C31—C32—C33—C340.2 (3)
C5—C6—C7—C80.7 (4)C32—C33—C34—C350.5 (3)
C6—C7—C8—C90.5 (4)C33—C34—C35—C360.0 (4)
C5—C4—C9—C81.0 (3)C32—C31—C36—C351.1 (3)
N1—C4—C9—C8178.9 (2)N2—C31—C36—C35177.50 (19)
C7—C8—C9—C40.3 (4)C34—C35—C36—C310.8 (3)
C22—Sn1—C10—C1537.46 (17)C49—Sn2—C37—C38109.91 (13)
C16—Sn1—C10—C15153.09 (15)C43—Sn2—C37—C380.12 (14)
S1—Sn1—C10—C15100.26 (15)S3—Sn2—C37—C38102.97 (13)
C22—Sn1—C10—C11138.42 (16)C49—Sn2—C37—C4268.03 (17)
C16—Sn1—C10—C1122.79 (18)C43—Sn2—C37—C42177.83 (15)
S1—Sn1—C10—C1183.85 (16)S3—Sn2—C37—C4279.09 (15)
C15—C10—C11—C121.8 (3)C42—C37—C38—C390.4 (3)
Sn1—C10—C11—C12177.71 (17)Sn2—C37—C38—C39177.68 (14)
C10—C11—C12—C131.6 (4)C37—C38—C39—C400.1 (3)
C11—C12—C13—C140.0 (4)C38—C39—C40—C410.5 (3)
C12—C13—C14—C151.3 (4)C39—C40—C41—C420.7 (3)
C11—C10—C15—C140.5 (3)C40—C41—C42—C370.4 (3)
Sn1—C10—C15—C14176.47 (16)C38—C37—C42—C410.2 (3)
C13—C14—C15—C101.0 (3)Sn2—C37—C42—C41177.73 (14)
C22—Sn1—C16—C1720.76 (18)C49—Sn2—C43—C4835.27 (16)
C10—Sn1—C16—C1799.57 (17)C37—Sn2—C43—C4884.57 (16)
S1—Sn1—C16—C17136.35 (16)S3—Sn2—C43—C48155.95 (15)
C22—Sn1—C16—C21156.46 (16)C49—Sn2—C43—C44147.26 (17)
C10—Sn1—C16—C2183.20 (17)C37—Sn2—C43—C4492.89 (17)
S1—Sn1—C16—C2140.88 (17)S3—Sn2—C43—C4426.58 (17)
C21—C16—C17—C180.3 (3)C48—C43—C44—C451.0 (3)
Sn1—C16—C17—C18177.70 (17)Sn2—C43—C44—C45178.45 (17)
C16—C17—C18—C190.1 (3)C43—C44—C45—C460.3 (4)
C17—C18—C19—C200.2 (4)C44—C45—C46—C470.7 (4)
C18—C19—C20—C210.1 (4)C45—C46—C47—C481.1 (3)
C19—C20—C21—C160.1 (4)C44—C43—C48—C470.6 (3)
C17—C16—C21—C200.4 (3)Sn2—C43—C48—C47178.21 (16)
Sn1—C16—C21—C20177.70 (17)C46—C47—C48—C430.4 (3)
C10—Sn1—C22—C2748.80 (17)C37—Sn2—C49—C50153.78 (16)
C16—Sn1—C22—C2768.54 (17)C43—Sn2—C49—C5042.98 (18)
S1—Sn1—C22—C27170.33 (14)S3—Sn2—C49—C5059.63 (18)
C10—Sn1—C22—C23136.57 (17)C37—Sn2—C49—C5418.37 (19)
C16—Sn1—C22—C23106.10 (17)C43—Sn2—C49—C54129.18 (17)
S1—Sn1—C22—C234.30 (18)S3—Sn2—C49—C54128.22 (16)
C27—C22—C23—C241.5 (3)C54—C49—C50—C510.5 (3)
Sn1—C22—C23—C24173.10 (17)Sn2—C49—C50—C51171.82 (19)
C22—C23—C24—C250.3 (4)C49—C50—C51—C520.7 (4)
C23—C24—C25—C261.3 (4)C50—C51—C52—C531.1 (4)
C24—C25—C26—C271.8 (4)C51—C52—C53—C540.3 (4)
C25—C26—C27—C220.7 (4)C52—C53—C54—C491.0 (4)
C23—C22—C27—C261.0 (3)C50—C49—C54—C531.3 (3)
Sn1—C22—C27—C26173.95 (19)Sn2—C49—C54—C53170.94 (19)
Hydrogen-bond geometry (Å, °) top
Cg1, Cg2, and Cg3 are the centroids of the C16–C21, C37–C42 and C43–C48 benzene rings, respectively.
D—H···AD—HH···AD···AD—H···A
C9—H9···Cg1i0.952.723.630 (3)160
C25—H25···Cg2ii0.952.903.639 (3)135
C32—H32···Cg3iii0.952.923.824 (2)160
Symmetry codes: (i) −x+1, −y+2, −z+1; (ii) x−1, y, z; (iii) −x+2, −y+2, −z+2.
Table 1
Selected geometric parameters (Å)
top
Sn1—C102.1339 (19)Sn2—C372.1413 (18)
Sn1—C162.1541 (19)Sn2—C432.1605 (19)
Sn1—C222.1210 (18)Sn2—C492.1379 (19)
Sn1—S12.4539 (5)Sn2—S32.4662 (5)
S1—C11.759 (2)S3—C281.7496 (19)
S2—C11.680 (2)S4—C281.6862 (19)
Table 2
Hydrogen-bond geometry (Å, °)
top
Cg1, Cg2, and Cg3 are the centroids of the C16–C21, C37–C42 and C43–C48 benzene rings, respectively.
D—H···AD—HH···AD···AD—H···A
C9—H9···Cg1i0.952.723.630 (3)160
C25—H25···Cg2ii0.952.903.639 (3)135
C32—H32···Cg3iii0.952.923.824 (2)160
Symmetry codes: (i) −x+1, −y+2, −z+1; (ii) x−1, y, z; (iii) −x+2, −y+2, −z+2.
Acknowledgements top

The authors thank the Universiti Kebangsaan Malaysia (UKM-GUP-NBT-08–27-111), the Ministry of Higher Education (UKM-ST-06-FRGS0092–2010) and the Universiti Putra Malaysia for support.

references
References top

Brandenburg, K. (2006). DIAMOND. Crystal Impact GbR, Bonn, Germany.

Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.

Gans, J. & Shalloway, D. (2001). J. Mol. Graph. Model. 19, 557–559.

Kamaludin, N. F., Baba, I., Awang, N., Mohamed Tahir, M. I. & Tiekink, E. R. T. (2011). Acta Cryst. E67, m555–m556.

Oxford Diffraction (2010). CrysAlis PRO. Oxford Diffraction Ltd, Yarnton, Oxfordshire, England.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Tiekink, E. R. T. (2008). Appl. Organomet. Chem. 22, 533–550.

Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.