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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2007 Dec 18;64(Pt 1):m199. doi: 10.1107/S1600536807066287

Rhodamine 6G hexa­chlorido­stannate(IV) acetonitrile disolvate

Ramaiyer Venkatraman a, Lungile Sitole a, Frank R Fronczek b,*
PMCID: PMC2915129  PMID: 21200545

Abstract

In the title compound, bis({6-ethylamino-10-[2-(methoxycarbonyl)phenyl]-2,7-dimethylxanthen-3-ylidene}ethanaminium) hexachloridotin(IV) acetonitrile disolvate, (C27H29N2O3)2[SnCl6]·2C2H3N, the octa­hedral SnCl6 2− anion lies on an inversion center. The xanthene ring system is essentially planar, with an average deviation of 0.020 Å, and the substituent benzene ring forms a dihedral angle of 85.89 (2)° with it. The Sn—Cl distances are in the range 2.4237 (3)–2.4454 (3) Å. There are N—H⋯Cl hydrogen bonds between SnCl6 2− ions and rhodamine 6G cations as well as π–π stacking inter­actions between rhodamine 6G cations (inter­planar distance of 3.827 Å).

Related literature

For related literature, see: Bhagavthy et al. (1993); Fun et al. (1997); Herz (1974); Johnson & McGrane (1993); Liu et al. (1998); Nguyen & Meyer (1992); Wang et al. (1997). For the structure of the analogous ethyl ester as the chloride salt hydrate, see: Adhikesavalu et al. (2001).graphic file with name e-64-0m199-scheme1.jpg

Experimental

Crystal data

  • (C27H29N2O3)2[SnCl6]·2C2H3N

  • M r = 1272.54

  • Triclinic, Inline graphic

  • a = 9.7871 (10) Å

  • b = 11.7827 (11) Å

  • c = 13.2893 (12) Å

  • α = 80.583 (4)°

  • β = 77.309 (4)°

  • γ = 82.467 (4)°

  • V = 1467.7 (2) Å3

  • Z = 1

  • Mo Kα radiation

  • μ = 0.76 mm−1

  • T = 90.0 (5) K

  • 0.28 × 0.27 × 0.25 mm

Data collection

  • Nonius KappaCCD diffractometer with Oxford Cryostream

  • Absorption correction: multi-scan (DENZO and SCALEPACK; Otwinowski & Minor, 1997) T min = 0.815, T max = 0.832

  • 54250 measured reflections

  • 14412 independent reflections

  • 12969 reflections with I > 2σ(I)

  • R int = 0.024

Refinement

  • R[F 2 > 2σ(F 2)] = 0.029

  • wR(F 2) = 0.073

  • S = 1.03

  • 14412 reflections

  • 362 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.74 e Å−3

  • Δρmin = −1.24 e Å−3

Data collection: COLLECT (Nonius, 2000); cell refinement: DENZO and SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO and SCALEPACK; program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536807066287/pv2056sup1.cif

e-64-0m199-sup1.cif (26.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807066287/pv2056Isup2.hkl

e-64-0m199-Isup2.hkl (704.4KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1N⋯Cl2 0.81 (2) 2.61 (2) 3.3644 (10) 156 (2)
N2—H2N⋯Cl1i 0.86 (2) 2.75 (2) 3.5603 (10) 159 (2)

Symmetry code: (i) Inline graphic.

Acknowledgments

RV acknowledges support for supplies by the grant JSU RISE program (NIH grant No. 1RO25GM067122). The purchase of the diffractometer was made possible by grant No. LEQSF(1999–2000)-ENH-TR-13, administered by the Louisiana Board of Regents.

supplementary crystallographic information

Comment

The excellent photo-physical properties of rhodamines are well known (Herz, 1974; Johnson & McGrane, 1993; Nguyen & Meyer, 1992), and recently metal complexes of rhodamine 6 G have been reported by several authors (Bhagavthy et al., 1993; Fun et al., 1997; Wang et al., 1997; Liu et al., 1998). The aggregative properties of cationic species of the dye were observed to be dependent on the anionic environment created by the metal ions. We have synthesized a rhodamine 6 G derivative, 9-[2-methoxycarbonyl)phenyl]-3,6-bis(ethylamino)-2,7-dimethylxanthylium hexachlorotin(IV) diacetonitrile solvate, (I), the structure of which is presented in this paper.

The structure of (I) consists of discrete SnCl62- anions lying on inversion centers, rhodamine 6 G cations and acetonitrile solvent molecules (Fig. 1). The xanthene ring of the cation is planar within an average deviation of 0.020 Å (maximum deviation is 0.045 (1) Å for C4), and the phenyl ring forms a dihedral angle of 85.89 (2)° with it. The C—N distances N1—C24 and N2—C26 are normal for this type of single bond, whereas C3—N1 and C11—N2 are much shorter, showing partial double-bond character; details are in the Table. A similar trend is observed in the other rhodamine 6 G cations (Wang et al., 1997; Liu et al., 1998).

Both hydrogen bonding between cations and anions and π-π stacking interactions between rhodamine 6 G cations exist. Parallel rhodamine ions related by the inversion center have an interplanar distance of 3.827 Å (Fig. 2), and are slipped such that their O1—C13 bonds exactly overlap.

Experimental

Diphenyl tin dichloride (0.344 g, 1 mmol) was dissolved in 20 ml me thanol, and then 20 ml of methanol solution of rhodamine 6 G (0.479 g, 1 mmol) was added. The bright red solution was refluxed for 1 hr, whereafter red brown solid were obtained on cooling. Suitable size crystals were obtained by the recrystallization at room temperature from acetonitrile (yield ca 85%).

Refinement

H atoms were placed in idealized positions with C—H distances at 0.99, 0.98 and 0.95 Å for CH2, CH3 and aromatic CH groups, respectively using a riding model. Uiso for H was assigned as 1.2 times Ueq of the attached C atoms (1.5 for methyl); a torsional parameter was refined for each methyl group. The largest positive and negative residual density peaks were located within 1 Å of the Sn1 position.

Figures

Fig. 1.

Fig. 1.

Numbering scheme and ellipsoids at the 50% level. (i = 1 - x, -y, -z).

Fig. 2.

Fig. 2.

The unit cell, showing stacking of rhodamine cations and hydrogen bonding.

Crystal data

(C27H29N2O3)2[SnCl6]·2C2H3N Z = 1
Mr = 1272.54 F000 = 654
Triclinic, P1 Dx = 1.440 Mg m3
Hall symbol: -P 1 Mo Kα radiation λ = 0.71073 Å
a = 9.7871 (10) Å Cell parameters from 13141 reflections
b = 11.7827 (11) Å θ = 2.5–36.8º
c = 13.2893 (12) Å µ = 0.76 mm1
α = 80.583 (4)º T = 90.0 (5) K
β = 77.309 (4)º Fragment, red-orange
γ = 82.467 (4)º 0.28 × 0.27 × 0.25 mm
V = 1467.7 (2) Å3

Data collection

Nonius KappaCCD diffractometer with Oxford Cryostream 14412 independent reflections
Radiation source: fine-focus sealed tube 12969 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.024
T = 90.0(5) K θmax = 36.8º
ω scans with κ offsets θmin = 2.7º
Absorption correction: multi-scan(DENZO and SCALEPACK; Otwinowski & Minor, 1997) h = −16→16
Tmin = 0.815, Tmax = 0.832 k = −19→19
54250 measured reflections l = −22→21

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.029   w = 1/[σ2(Fo2) + (0.0303P)2 + 0.821P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.073 (Δ/σ)max < 0.001
S = 1.03 Δρmax = 0.74 e Å3
14412 reflections Δρmin = −1.24 e Å3
362 parameters Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0053 (5)
Secondary atom site location: difference Fourier map

Special details

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)

x y z Uiso*/Ueq
Sn1 0.5000 0.0000 0.0000 0.00926 (3)
Cl1 0.53900 (3) 0.04133 (2) 0.164917 (19) 0.01502 (5)
Cl2 0.51522 (3) 0.20275 (2) −0.07554 (2) 0.01362 (4)
Cl3 0.24802 (3) 0.04038 (2) 0.05732 (2) 0.01381 (4)
O1 0.40633 (8) 0.58975 (7) 0.38427 (6) 0.01354 (13)
O2 1.06811 (9) 0.46854 (8) 0.36352 (7) 0.01853 (15)
O3 0.83375 (10) 0.47563 (9) 0.39044 (9) 0.0272 (2)
N1 0.42673 (10) 0.33594 (9) 0.13842 (8) 0.01642 (17)
H1N 0.4731 (19) 0.3059 (16) 0.0897 (14) 0.020*
N2 0.35159 (10) 0.83221 (9) 0.64389 (7) 0.01542 (16)
H2N 0.3892 (19) 0.8743 (16) 0.6750 (14) 0.019*
C1 0.48174 (10) 0.54161 (9) 0.30004 (8) 0.01118 (15)
C2 0.41464 (10) 0.46614 (9) 0.26289 (8) 0.01275 (16)
H2 0.3206 0.4516 0.2948 0.015*
C3 0.48671 (11) 0.41085 (9) 0.17721 (8) 0.01291 (16)
C4 0.63032 (11) 0.43418 (9) 0.12992 (8) 0.01360 (16)
C5 0.69115 (11) 0.51151 (9) 0.16815 (8) 0.01310 (16)
H5 0.7846 0.5275 0.1359 0.016*
C6 0.62049 (10) 0.56913 (9) 0.25423 (8) 0.01122 (15)
C7 0.68061 (10) 0.64746 (8) 0.29612 (8) 0.01058 (15)
C8 0.60111 (10) 0.69685 (9) 0.38325 (8) 0.01108 (15)
C9 0.65144 (10) 0.77664 (9) 0.43315 (8) 0.01170 (15)
H9 0.7429 0.8005 0.4054 0.014*
C10 0.57244 (11) 0.82019 (9) 0.51976 (8) 0.01222 (15)
C11 0.43234 (11) 0.78594 (9) 0.56098 (8) 0.01258 (16)
C12 0.38037 (11) 0.70714 (9) 0.51364 (8) 0.01331 (16)
H12 0.2889 0.6832 0.5408 0.016*
C13 0.46414 (10) 0.66475 (9) 0.42693 (8) 0.01159 (15)
C14 0.70941 (13) 0.37222 (11) 0.04109 (10) 0.0197 (2)
H14A 0.8074 0.3907 0.0232 0.030*
H14B 0.6655 0.3969 −0.0195 0.030*
H14C 0.7069 0.2886 0.0616 0.030*
C15 0.62856 (12) 0.90417 (10) 0.57043 (9) 0.01553 (17)
H15A 0.7239 0.9186 0.5326 0.023*
H15B 0.6310 0.8716 0.6428 0.023*
H15C 0.5674 0.9770 0.5689 0.023*
C16 0.82316 (10) 0.68456 (8) 0.24669 (8) 0.01064 (15)
C17 0.94862 (10) 0.62467 (9) 0.27097 (8) 0.01147 (15)
C18 1.07793 (11) 0.66730 (9) 0.22341 (8) 0.01360 (16)
H18 1.1625 0.6273 0.2402 0.016*
C19 1.08333 (11) 0.76787 (9) 0.15174 (8) 0.01417 (17)
H19 1.1713 0.7963 0.1196 0.017*
C20 0.95942 (12) 0.82636 (10) 0.12744 (9) 0.01498 (17)
H20 0.9629 0.8948 0.0784 0.018*
C21 0.82987 (11) 0.78526 (9) 0.17463 (8) 0.01412 (17)
H21 0.7457 0.8260 0.1576 0.017*
C22 0.94161 (11) 0.51676 (9) 0.34679 (9) 0.01400 (17)
C23 1.06484 (13) 0.36159 (11) 0.43498 (10) 0.0211 (2)
H23A 0.9925 0.3717 0.4976 0.032*
H23B 1.1569 0.3406 0.4543 0.032*
H23C 1.0429 0.3000 0.4014 0.032*
C24 0.28833 (12) 0.29543 (10) 0.18084 (9) 0.01633 (18)
H24A 0.2628 0.3019 0.2562 0.020*
H24B 0.2931 0.2127 0.1733 0.020*
C25 0.17375 (14) 0.36257 (13) 0.12788 (12) 0.0258 (2)
H25A 0.1665 0.4443 0.1367 0.039*
H25B 0.0836 0.3314 0.1593 0.039*
H25C 0.1973 0.3554 0.0535 0.039*
C26 0.20472 (12) 0.81093 (11) 0.68565 (9) 0.0185 (2)
H26A 0.2000 0.7296 0.7190 0.022*
H26B 0.1527 0.8234 0.6281 0.022*
C27 0.13662 (13) 0.89136 (12) 0.76511 (10) 0.0232 (2)
H27A 0.1871 0.8779 0.8227 0.035*
H27B 0.0382 0.8763 0.7920 0.035*
H27C 0.1406 0.9718 0.7319 0.035*
N3 −0.01218 (17) 0.87440 (15) 0.42927 (13) 0.0429 (4)
C28 0.09893 (16) 0.88240 (12) 0.37996 (11) 0.0259 (2)
C29 0.23901 (15) 0.89178 (14) 0.31671 (11) 0.0267 (3)
H29A 0.2723 0.8203 0.2862 0.040*
H29B 0.3031 0.9042 0.3603 0.040*
H29C 0.2364 0.9571 0.2609 0.040*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Sn1 0.01002 (4) 0.00916 (4) 0.00947 (4) −0.00130 (3) −0.00229 (3) −0.00309 (3)
Cl1 0.01755 (10) 0.01736 (11) 0.01246 (10) −0.00091 (8) −0.00530 (8) −0.00629 (8)
Cl2 0.01605 (10) 0.01023 (9) 0.01489 (10) −0.00222 (7) −0.00319 (8) −0.00189 (7)
Cl3 0.01070 (9) 0.01542 (10) 0.01489 (10) −0.00084 (7) −0.00195 (7) −0.00214 (8)
O1 0.0112 (3) 0.0151 (3) 0.0155 (3) −0.0041 (2) 0.0009 (2) −0.0078 (3)
O2 0.0122 (3) 0.0194 (4) 0.0205 (4) 0.0012 (3) −0.0034 (3) 0.0050 (3)
O3 0.0140 (4) 0.0235 (4) 0.0401 (6) −0.0072 (3) −0.0080 (4) 0.0150 (4)
N1 0.0148 (4) 0.0163 (4) 0.0198 (4) −0.0041 (3) 0.0003 (3) −0.0103 (3)
N2 0.0155 (4) 0.0181 (4) 0.0135 (4) −0.0043 (3) 0.0004 (3) −0.0073 (3)
C1 0.0097 (3) 0.0108 (4) 0.0131 (4) −0.0009 (3) −0.0008 (3) −0.0041 (3)
C2 0.0104 (4) 0.0126 (4) 0.0162 (4) −0.0023 (3) −0.0012 (3) −0.0058 (3)
C3 0.0126 (4) 0.0116 (4) 0.0155 (4) −0.0019 (3) −0.0024 (3) −0.0047 (3)
C4 0.0120 (4) 0.0142 (4) 0.0150 (4) −0.0018 (3) −0.0005 (3) −0.0058 (3)
C5 0.0109 (4) 0.0143 (4) 0.0143 (4) −0.0017 (3) −0.0002 (3) −0.0054 (3)
C6 0.0094 (3) 0.0113 (4) 0.0132 (4) −0.0014 (3) −0.0015 (3) −0.0034 (3)
C7 0.0092 (3) 0.0106 (4) 0.0119 (4) −0.0011 (3) −0.0016 (3) −0.0022 (3)
C8 0.0106 (4) 0.0112 (4) 0.0118 (4) −0.0019 (3) −0.0017 (3) −0.0026 (3)
C9 0.0116 (4) 0.0114 (4) 0.0128 (4) −0.0022 (3) −0.0026 (3) −0.0026 (3)
C10 0.0133 (4) 0.0121 (4) 0.0123 (4) −0.0023 (3) −0.0031 (3) −0.0030 (3)
C11 0.0136 (4) 0.0126 (4) 0.0115 (4) −0.0019 (3) −0.0010 (3) −0.0032 (3)
C12 0.0129 (4) 0.0138 (4) 0.0135 (4) −0.0039 (3) 0.0007 (3) −0.0052 (3)
C13 0.0112 (4) 0.0115 (4) 0.0127 (4) −0.0025 (3) −0.0015 (3) −0.0038 (3)
C14 0.0171 (5) 0.0222 (5) 0.0207 (5) −0.0045 (4) 0.0030 (4) −0.0129 (4)
C15 0.0174 (4) 0.0168 (4) 0.0149 (4) −0.0039 (3) −0.0038 (3) −0.0067 (3)
C16 0.0095 (3) 0.0114 (4) 0.0114 (4) −0.0020 (3) −0.0014 (3) −0.0028 (3)
C17 0.0099 (4) 0.0109 (4) 0.0135 (4) −0.0015 (3) −0.0016 (3) −0.0020 (3)
C18 0.0097 (4) 0.0142 (4) 0.0168 (4) −0.0018 (3) −0.0015 (3) −0.0029 (3)
C19 0.0122 (4) 0.0149 (4) 0.0153 (4) −0.0037 (3) −0.0001 (3) −0.0034 (3)
C20 0.0152 (4) 0.0147 (4) 0.0144 (4) −0.0045 (3) −0.0019 (3) 0.0005 (3)
C21 0.0121 (4) 0.0140 (4) 0.0158 (4) −0.0018 (3) −0.0031 (3) −0.0002 (3)
C22 0.0124 (4) 0.0128 (4) 0.0167 (4) −0.0012 (3) −0.0042 (3) −0.0002 (3)
C23 0.0200 (5) 0.0197 (5) 0.0199 (5) 0.0023 (4) −0.0043 (4) 0.0049 (4)
C24 0.0158 (4) 0.0139 (4) 0.0206 (5) −0.0046 (3) −0.0018 (4) −0.0065 (4)
C25 0.0188 (5) 0.0259 (6) 0.0337 (7) −0.0029 (4) −0.0078 (5) −0.0030 (5)
C26 0.0152 (4) 0.0217 (5) 0.0186 (5) −0.0044 (4) 0.0023 (4) −0.0088 (4)
C27 0.0178 (5) 0.0290 (6) 0.0230 (5) −0.0010 (4) 0.0017 (4) −0.0134 (5)
N3 0.0356 (7) 0.0410 (8) 0.0433 (8) −0.0075 (6) 0.0048 (6) 0.0053 (7)
C28 0.0311 (6) 0.0223 (6) 0.0233 (6) −0.0063 (5) −0.0045 (5) 0.0009 (4)
C29 0.0252 (6) 0.0370 (7) 0.0190 (5) −0.0098 (5) −0.0050 (4) −0.0010 (5)

Geometric parameters (Å, °)

Sn1—Cl3 2.4237 (3) C14—H14A 0.9800
Sn1—Cl3i 2.4237 (3) C14—H14B 0.9800
Sn1—Cl1i 2.4396 (3) C14—H14C 0.9800
Sn1—Cl1 2.4396 (3) C15—H15A 0.9800
Sn1—Cl2i 2.4454 (3) C15—H15B 0.9800
Sn1—Cl2 2.4454 (3) C15—H15C 0.9800
O1—C1 1.3618 (12) C16—C21 1.3966 (15)
O1—C13 1.3632 (12) C16—C17 1.4080 (14)
O2—C22 1.3417 (13) C17—C18 1.4017 (14)
O2—C23 1.4479 (15) C17—C22 1.4865 (15)
O3—C22 1.2078 (14) C18—C19 1.3925 (15)
N1—C3 1.3443 (13) C18—H18 0.9500
N1—C24 1.4583 (15) C19—C20 1.3893 (16)
N1—H1N 0.81 (2) C19—H19 0.9500
N2—C11 1.3553 (13) C20—C21 1.3955 (15)
N2—C26 1.4613 (15) C20—H20 0.9500
N2—H2N 0.86 (2) C21—H21 0.9500
C1—C2 1.3802 (14) C23—H23A 0.9800
C1—C6 1.4169 (14) C23—H23B 0.9800
C2—C3 1.4099 (14) C23—H23C 0.9800
C2—H2 0.9500 C24—C25 1.5201 (18)
C3—C4 1.4500 (15) C24—H24A 0.9900
C4—C5 1.3673 (14) C24—H24B 0.9900
C4—C14 1.5027 (15) C25—H25A 0.9800
C5—C6 1.4252 (14) C25—H25B 0.9800
C5—H5 0.9500 C25—H25C 0.9800
C6—C7 1.4008 (14) C26—C27 1.5198 (16)
C7—C8 1.4109 (14) C26—H26A 0.9900
C7—C16 1.4941 (14) C26—H26B 0.9900
C8—C13 1.4128 (14) C27—H27A 0.9800
C8—C9 1.4266 (14) C27—H27B 0.9800
C9—C10 1.3727 (14) C27—H27C 0.9800
C9—H9 0.9500 N3—C28 1.146 (2)
C10—C11 1.4442 (15) C28—C29 1.450 (2)
C10—C15 1.5024 (14) C29—H29A 0.9800
C11—C12 1.4043 (14) C29—H29B 0.9800
C12—C13 1.3839 (14) C29—H29C 0.9800
C12—H12 0.9500
Cl3—Sn1—Cl3i 180.0 H14A—C14—H14C 109.5
Cl3—Sn1—Cl1i 89.363 (10) H14B—C14—H14C 109.5
Cl3i—Sn1—Cl1i 90.638 (10) C10—C15—H15A 109.5
Cl3—Sn1—Cl1 90.638 (10) C10—C15—H15B 109.5
Cl3i—Sn1—Cl1 89.362 (10) H15A—C15—H15B 109.5
Cl1i—Sn1—Cl1 180.0 C10—C15—H15C 109.5
Cl3—Sn1—Cl2i 90.291 (10) H15A—C15—H15C 109.5
Cl3i—Sn1—Cl2i 89.709 (10) H15B—C15—H15C 109.5
Cl1i—Sn1—Cl2i 90.829 (10) C21—C16—C17 119.27 (9)
Cl1—Sn1—Cl2i 89.170 (10) C21—C16—C7 117.43 (9)
Cl3—Sn1—Cl2 89.709 (10) C17—C16—C7 123.29 (9)
Cl3i—Sn1—Cl2 90.290 (10) C18—C17—C16 119.71 (9)
Cl1i—Sn1—Cl2 89.171 (11) C18—C17—C22 121.02 (9)
Cl1—Sn1—Cl2 90.830 (10) C16—C17—C22 119.27 (9)
Cl2i—Sn1—Cl2 180.0 C19—C18—C17 120.52 (10)
C1—O1—C13 120.30 (8) C19—C18—H18 119.7
C22—O2—C23 114.57 (9) C17—C18—H18 119.7
C3—N1—C24 126.24 (9) C20—C19—C18 119.63 (10)
C3—N1—H1N 118.0 (13) C20—C19—H19 120.2
C24—N1—H1N 115.6 (13) C18—C19—H19 120.2
C11—N2—C26 123.53 (9) C19—C20—C21 120.47 (10)
C11—N2—H2N 118.5 (12) C19—C20—H20 119.8
C26—N2—H2N 118.0 (12) C21—C20—H20 119.8
O1—C1—C2 116.05 (9) C20—C21—C16 120.40 (10)
O1—C1—C6 121.03 (9) C20—C21—H21 119.8
C2—C1—C6 122.93 (9) C16—C21—H21 119.8
C1—C2—C3 119.50 (9) O3—C22—O2 122.39 (10)
C1—C2—H2 120.3 O3—C22—C17 124.24 (10)
C3—C2—H2 120.3 O2—C22—C17 113.37 (9)
N1—C3—C2 121.95 (10) O2—C23—H23A 109.5
N1—C3—C4 118.77 (9) O2—C23—H23B 109.5
C2—C3—C4 119.29 (9) H23A—C23—H23B 109.5
C5—C4—C3 119.00 (9) O2—C23—H23C 109.5
C5—C4—C14 121.49 (10) H23A—C23—H23C 109.5
C3—C4—C14 119.51 (9) H23B—C23—H23C 109.5
C4—C5—C6 122.88 (9) N1—C24—C25 113.19 (10)
C4—C5—H5 118.6 N1—C24—H24A 108.9
C6—C5—H5 118.6 C25—C24—H24A 108.9
C7—C6—C1 119.38 (9) N1—C24—H24B 108.9
C7—C6—C5 124.23 (9) C25—C24—H24B 108.9
C1—C6—C5 116.38 (9) H24A—C24—H24B 107.8
C6—C7—C8 118.96 (9) C24—C25—H25A 109.5
C6—C7—C16 121.31 (9) C24—C25—H25B 109.5
C8—C7—C16 119.63 (9) H25A—C25—H25B 109.5
C7—C8—C13 119.28 (9) C24—C25—H25C 109.5
C7—C8—C9 124.03 (9) H25A—C25—H25C 109.5
C13—C8—C9 116.67 (9) H25B—C25—H25C 109.5
C10—C9—C8 122.33 (9) N2—C26—C27 110.50 (10)
C10—C9—H9 118.8 N2—C26—H26A 109.5
C8—C9—H9 118.8 C27—C26—H26A 109.5
C9—C10—C11 119.04 (9) N2—C26—H26B 109.5
C9—C10—C15 121.00 (9) C27—C26—H26B 109.5
C11—C10—C15 119.95 (9) H26A—C26—H26B 108.1
N2—C11—C12 120.82 (10) C26—C27—H27A 109.5
N2—C11—C10 119.37 (9) C26—C27—H27B 109.5
C12—C11—C10 119.80 (9) H27A—C27—H27B 109.5
C13—C12—C11 119.16 (9) C26—C27—H27C 109.5
C13—C12—H12 120.4 H27A—C27—H27C 109.5
C11—C12—H12 120.4 H27B—C27—H27C 109.5
O1—C13—C12 115.99 (9) N3—C28—C29 179.32 (18)
O1—C13—C8 121.03 (9) C28—C29—H29A 109.5
C12—C13—C8 122.98 (9) C28—C29—H29B 109.5
C4—C14—H14A 109.5 H29A—C29—H29B 109.5
C4—C14—H14B 109.5 C28—C29—H29C 109.5
H14A—C14—H14B 109.5 H29A—C29—H29C 109.5
C4—C14—H14C 109.5 H29B—C29—H29C 109.5
C13—O1—C1—C2 179.54 (9) C9—C10—C11—C12 1.40 (15)
C13—O1—C1—C6 −0.75 (15) C15—C10—C11—C12 −179.79 (10)
O1—C1—C2—C3 −178.69 (9) N2—C11—C12—C13 177.80 (10)
C6—C1—C2—C3 1.61 (16) C10—C11—C12—C13 −0.92 (16)
C24—N1—C3—C2 −4.43 (18) C1—O1—C13—C12 −178.66 (9)
C24—N1—C3—C4 174.88 (11) C1—O1—C13—C8 1.91 (15)
C1—C2—C3—N1 179.50 (10) C11—C12—C13—O1 −179.22 (9)
C1—C2—C3—C4 0.18 (16) C11—C12—C13—C8 0.19 (16)
N1—C3—C4—C5 179.10 (11) C7—C8—C13—O1 −2.03 (15)
C2—C3—C4—C5 −1.56 (16) C9—C8—C13—O1 179.45 (9)
N1—C3—C4—C14 −1.55 (16) C7—C8—C13—C12 178.58 (10)
C2—C3—C4—C14 177.78 (11) C9—C8—C13—C12 0.06 (15)
C3—C4—C5—C6 1.23 (17) C6—C7—C16—C21 93.07 (12)
C14—C4—C5—C6 −178.10 (11) C8—C7—C16—C21 −83.31 (12)
O1—C1—C6—C7 −0.26 (15) C6—C7—C16—C17 −88.32 (13)
C2—C1—C6—C7 179.42 (10) C8—C7—C16—C17 95.30 (12)
O1—C1—C6—C5 178.39 (9) C21—C16—C17—C18 0.58 (15)
C2—C1—C6—C5 −1.93 (15) C7—C16—C17—C18 −178.01 (9)
C4—C5—C6—C7 179.04 (10) C21—C16—C17—C22 −179.32 (9)
C4—C5—C6—C1 0.46 (16) C7—C16—C17—C22 2.09 (15)
C1—C6—C7—C8 0.11 (15) C16—C17—C18—C19 −0.52 (15)
C5—C6—C7—C8 −178.42 (10) C22—C17—C18—C19 179.38 (10)
C1—C6—C7—C16 −176.29 (9) C17—C18—C19—C20 0.11 (16)
C5—C6—C7—C16 5.18 (16) C18—C19—C20—C21 0.25 (16)
C6—C7—C8—C13 1.00 (15) C19—C20—C21—C16 −0.19 (16)
C16—C7—C8—C13 177.46 (9) C17—C16—C21—C20 −0.23 (15)
C6—C7—C8—C9 179.40 (10) C7—C16—C21—C20 178.44 (10)
C16—C7—C8—C9 −4.14 (15) C23—O2—C22—O3 2.09 (17)
C7—C8—C9—C10 −177.98 (10) C23—O2—C22—C17 −178.43 (10)
C13—C8—C9—C10 0.46 (15) C18—C17—C22—O3 179.92 (12)
C8—C9—C10—C11 −1.18 (15) C16—C17—C22—O3 −0.18 (17)
C8—C9—C10—C15 −179.97 (10) C18—C17—C22—O2 0.46 (15)
C26—N2—C11—C12 −4.18 (17) C16—C17—C22—O2 −179.64 (9)
C26—N2—C11—C10 174.54 (10) C3—N1—C24—C25 96.39 (14)
C9—C10—C11—N2 −177.33 (10) C11—N2—C26—C27 −169.80 (11)
C15—C10—C11—N2 1.48 (15)

Symmetry codes: (i) −x+1, −y, −z.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1N···Cl2 0.81 (2) 2.61 (2) 3.3644 (10) 156 (2)
N2—H2N···Cl1ii 0.86 (2) 2.75 (2) 3.5603 (10) 159 (2)

Symmetry codes: (ii) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PV2056).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536807066287/pv2056sup1.cif

e-64-0m199-sup1.cif (26.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807066287/pv2056Isup2.hkl

e-64-0m199-Isup2.hkl (704.4KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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