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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Feb 16;67(Pt 3):m339. doi: 10.1107/S1600536811004971

1-(4-Cyano­benz­yl)-3,5-dimethyl­pyridinium bis­(benzene-1,2-dithiol­ato)nickelate(III)

Yan-Jie Dong a, Xue-Jun Kong a,*
PMCID: PMC3051972  PMID: 21522268

Abstract

The asymmetric unit of the title compound, (C15H15N2)[Ni(C6H4S2)2], contains half each of two independent centrosymmetric anions and a single cation in a general position. The NiIII ions are coordinated by four S atoms in a square-planar geometry. The anions exhibit two packing modes, viz. stacked along the a axis in a face-to-face fashion with an alternate arrangement of anions and cations, and stacked in a side-by-side fashion, forming ribbons parallel to (011).

Related literature

For general background to mol­ecular-based magnetic materials, see: Jones (1997 ▶); Akutagawa et al. (2009 ▶). For the role played by the size and shape of the counter-cations in determining the ground-state properties of the resulting materials, see: Ren et al. (2003 ▶). For related structures, see: Sellmann et al. (1991 ▶); Xie et al. (2002 ▶, 2003 ▶); Ren et al. (2002 ▶).graphic file with name e-67-0m339-scheme1.jpg

Experimental

Crystal data

  • (C15H15N2)[Ni(C6H4S2)2]

  • M r = 562.42

  • Triclinic, Inline graphic

  • a = 7.1517 (7) Å

  • b = 12.8190 (13) Å

  • c = 15.3294 (16) Å

  • α = 69.774 (1)°

  • β = 77.740 (1)°

  • γ = 87.721 (1)°

  • V = 1287.8 (2) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 1.10 mm−1

  • T = 296 K

  • 0.36 × 0.30 × 0.28 mm

Data collection

  • Bruker SMART APEX CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2000 ▶) T min = 0.694, T max = 0.749

  • 6530 measured reflections

  • 4530 independent reflections

  • 3728 reflections with I > 2σ(I)

  • R int = 0.042

Refinement

  • R[F 2 > 2σ(F 2)] = 0.036

  • wR(F 2) = 0.098

  • S = 1.02

  • 4530 reflections

  • 312 parameters

  • H-atom parameters constrained

  • Δρmax = 0.25 e Å−3

  • Δρmin = −0.39 e Å−3

Data collection: SMART (Bruker, 2000 ▶); cell refinement: SAINT (Bruker, 2000 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811004971/rz2554sup1.cif

e-67-0m339-sup1.cif (23.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811004971/rz2554Isup2.hkl

e-67-0m339-Isup2.hkl (221.9KB, hkl)

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

Acknowledgments

This work was supported by the National Natural Science Foundation of China (No. 20971004), the Key Project of Chinese Ministry of Education (No. 210102) and the Natural Science Foundation of Anhui Province (No. 11040606M45).

supplementary crystallographic information

Comment

Molecular solids with particular functionality are continuously paid much attention by chemists and physicists in the field of materials science (Jones, 1997). The preparation of new molecular based spin-bearing systems, among others, has been pursued from the viewpoint of materials/physical organic chemistry to develop novel molecular-based magnetic materials (Akutagawa et al., 2009). In our previous research using benzylpyridinium derivatives ([RBzPy]+) as the counter-cation of [M(mnt)2]- (where M = Ni, Pd and Pt and mnt2- = maleodinitriledithiolate), a series of ion-pair compounds with segregated columnar stacks of cations and anions has been prepared (Ren et al., 2002; Ren et al., 2003; Xie et al., 2002). The quasi one-dimensional magnetic nature of these compounds was attributed to intermolecular orbital interactions within the anionic columns. As an extension of our work on this series of complexes, we report here the crystal structure of the title compound, (I).

The asymmetric unit of (I) contains half each of two independent centrosymmetric [Ni(C6H4S2)2]- anions and one (C15H15N2)+ cation. In the anions, the nickel(III) ions are coordinated by four S atoms in a square-planar geometry; the Ni—S bonds and S—Ni—S angles are in agreement with the corresponding values found in analogous complexes (Sellmann et al., 1991; Xie et al., 2003). The centrosymmetric [Ni(C6H4S2)2]- anions are almost planar. The dihedral angle between the two benzene rings of the cation is 86.49 (6)°. In the crystal structure, the packing of the two anions is different (Fig. 2). The Ni1-containing anions stack in a side-by-side fashion, forming one-dimensional ribbons parallel to (011); the shortest distance between the adjacent nickel(III) ions is 7.152 (6) Å. The Ni2-containing anions stack in a face-to-face fashion along the a axis with an alternating arrangement of [Ni(C6H4S2)2]- anions and [C15H15N2]+ cations such that the pyridine ring of the cation lies above the benzene ring of the anion. The shortest distance between adjacent nickel(III) ions is also 7.152 (6) Å. A Ni···Ni distance of 8.155 (9)Å is found between adjacent Ni1-containing and Ni2-containing anions.

Experimental

Benzene-1,2-dithiol (142 mg, 1.0 mmol) was added to a solution of sodium metal (46 mg, 2.0 mmol) in absolute ethanol (25 ml), under a nitrogen atmosphere at room temperature. A solution of NiCl2.6H2O (120 mg, 0.5 mmol) in ethanol (25 ml) was added, resulting in the mixture turning a muddy red-brown colour. Following this, [CNBzPy(CH3)2]Br (304 mg, 1.0 mmol) was added and the mixture allowed to stand with stirring for 1 h, and then stirred for an additional 24 h in air. The colour of the mixture gradually turned green, indicating oxidation from a dianionic species to the more stable monoanionic form. The precipitate was washed with absolute ethanol and diethyl ether and then dried. The crude product was recrystallized twice from dichloromethane to give the title compound (yield 198 mg, 54%).

Refinement

All H atoms were placed in calculated positions and refined using a riding model, with C–H = 0.93–0.97 Å, and with Uiso(H) = 1.2 Ueq(C) or 1.5 Ueq(C) for methyl H atoms.

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I) with the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level. Symmetry codes: (A) 1-x, 1-y, 1-z; (B) 1-x, 2-y, -z.

Fig. 2.

Fig. 2.

Packing diagram of (I) viewed along the a axis.

Crystal data

(C15H15N2)[Ni(C6H4S2)2] Z = 2
Mr = 562.42 F(000) = 582
Triclinic, P1 Dx = 1.450 Mg m−3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 7.1517 (7) Å Cell parameters from 3577 reflections
b = 12.8190 (13) Å θ = 2.6–27.0°
c = 15.3294 (16) Å µ = 1.10 mm−1
α = 69.774 (1)° T = 296 K
β = 77.740 (1)° Block, dark green
γ = 87.721 (1)° 0.36 × 0.30 × 0.28 mm
V = 1287.8 (2) Å3

Data collection

Bruker SMART APEX CCD area-detector diffractometer 4530 independent reflections
Radiation source: sealed tube 3728 reflections with I > 2σ(I)
graphite Rint = 0.042
φ and ω scans θmax = 25.1°, θmin = 1.5°
Absorption correction: multi-scan (SADABS; Bruker, 2000) h = −8→8
Tmin = 0.694, Tmax = 0.749 k = −12→15
6530 measured reflections l = −18→15

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.036 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.098 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0581P)2] where P = (Fo2 + 2Fc2)/3
4530 reflections (Δ/σ)max = 0.001
312 parameters Δρmax = 0.25 e Å−3
0 restraints Δρmin = −0.39 e Å−3

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
Ni1 0.5000 0.5000 0.5000 0.05051 (14)
Ni2 0.5000 1.0000 0.0000 0.06279 (16)
S1 0.38833 (9) 0.43210 (6) 0.41084 (5) 0.06354 (19)
S2 0.78410 (8) 0.44650 (5) 0.45826 (4) 0.05774 (17)
S3 0.52163 (10) 0.85288 (5) 0.11833 (6) 0.0751 (2)
S4 0.44027 (9) 1.09946 (6) 0.09034 (6) 0.0758 (2)
C1 0.5817 (3) 0.3696 (2) 0.36074 (16) 0.0563 (6)
C2 0.5622 (4) 0.3134 (2) 0.29922 (18) 0.0710 (7)
H2 0.4429 0.3068 0.2862 0.085*
C3 0.7171 (4) 0.2681 (3) 0.2582 (2) 0.0800 (8)
H3 0.7024 0.2306 0.2177 0.096*
C4 0.8974 (4) 0.2777 (2) 0.2765 (2) 0.0779 (8)
H4 1.0026 0.2472 0.2480 0.093*
C5 0.9189 (4) 0.3322 (2) 0.33656 (18) 0.0674 (7)
H5 1.0394 0.3392 0.3482 0.081*
C6 0.7616 (3) 0.37727 (19) 0.38061 (15) 0.0544 (5)
C7 0.4721 (4) 0.8937 (2) 0.2174 (2) 0.0750 (8)
C8 0.4671 (4) 0.8185 (3) 0.3089 (3) 0.0933 (10)
H8 0.4884 0.7438 0.3178 0.112*
C9 0.4315 (5) 0.8526 (4) 0.3851 (3) 0.1155 (14)
H9 0.4298 0.8014 0.4456 0.139*
C10 0.3978 (5) 0.9626 (5) 0.3733 (3) 0.1139 (14)
H10 0.3753 0.9851 0.4261 0.137*
C11 0.3969 (4) 1.0402 (3) 0.2847 (3) 0.0971 (10)
H11 0.3712 1.1140 0.2779 0.116*
C12 0.4356 (3) 1.0061 (2) 0.2045 (2) 0.0734 (7)
C13 0.7251 (6) 0.5985 (3) −0.0472 (2) 0.0964 (10)
C14 0.8167 (5) 0.6096 (2) 0.0246 (2) 0.0708 (7)
C15 1.0079 (5) 0.6423 (2) 0.0003 (2) 0.0809 (8)
H15 1.0773 0.6544 −0.0612 0.097*
C16 1.0958 (4) 0.6572 (2) 0.06717 (19) 0.0723 (7)
H16 1.2245 0.6796 0.0505 0.087*
C17 0.9938 (4) 0.63901 (18) 0.15919 (17) 0.0571 (6)
C18 0.8028 (4) 0.60457 (19) 0.18304 (18) 0.0614 (6)
H18 0.7338 0.5916 0.2447 0.074*
C19 0.7138 (4) 0.5892 (2) 0.1172 (2) 0.0713 (7)
H19 0.5858 0.5654 0.1343 0.086*
C20 1.0872 (4) 0.65782 (19) 0.23205 (18) 0.0632 (6)
H20A 1.0577 0.5944 0.2906 0.076*
H20B 1.2250 0.6635 0.2093 0.076*
C21 0.9853 (4) 0.7593 (2) 0.34242 (17) 0.0622 (6)
H21 0.9952 0.6936 0.3918 0.075*
C22 0.9338 (4) 0.8545 (2) 0.36168 (17) 0.0648 (7)
C23 0.9208 (3) 0.9501 (2) 0.28705 (17) 0.0597 (6)
H23 0.8853 1.0150 0.2995 0.072*
C24 0.9592 (3) 0.95288 (18) 0.19364 (15) 0.0512 (5)
C25 1.0102 (3) 0.85467 (18) 0.17933 (15) 0.0509 (5)
H25 1.0374 0.8532 0.1177 0.061*
C26 0.8910 (5) 0.8506 (3) 0.46412 (19) 0.0950 (10)
H26A 0.8574 0.9231 0.4661 0.142*
H26B 1.0023 0.8277 0.4907 0.142*
H26C 0.7864 0.7985 0.5004 0.142*
C27 0.9439 (3) 1.0558 (2) 0.11151 (17) 0.0617 (6)
H27A 1.0669 1.0761 0.0692 0.093*
H27B 0.9012 1.1153 0.1346 0.093*
H27C 0.8536 1.0422 0.0781 0.093*
N1 0.6563 (6) 0.5905 (3) −0.1048 (2) 0.1353 (14)
N2 1.0217 (3) 0.76078 (14) 0.25195 (12) 0.0528 (5)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Ni1 0.0451 (2) 0.0580 (3) 0.0509 (2) −0.00616 (18) −0.01511 (17) −0.01801 (19)
Ni2 0.0386 (2) 0.0489 (3) 0.0962 (4) 0.00137 (17) −0.0198 (2) −0.0160 (2)
S1 0.0478 (3) 0.0842 (4) 0.0722 (4) −0.0036 (3) −0.0202 (3) −0.0387 (3)
S2 0.0473 (3) 0.0721 (4) 0.0593 (3) −0.0029 (3) −0.0192 (3) −0.0244 (3)
S3 0.0622 (4) 0.0528 (4) 0.1011 (5) 0.0018 (3) −0.0223 (4) −0.0121 (3)
S4 0.0527 (4) 0.0594 (4) 0.1193 (6) 0.0036 (3) −0.0267 (4) −0.0308 (4)
C1 0.0559 (14) 0.0622 (14) 0.0501 (12) −0.0090 (11) −0.0119 (10) −0.0171 (11)
C2 0.0641 (16) 0.0864 (18) 0.0730 (16) −0.0116 (14) −0.0170 (13) −0.0376 (15)
C3 0.083 (2) 0.090 (2) 0.0773 (18) −0.0109 (16) −0.0060 (15) −0.0465 (16)
C4 0.0702 (18) 0.088 (2) 0.0779 (18) 0.0033 (15) −0.0050 (14) −0.0381 (16)
C5 0.0548 (15) 0.0792 (18) 0.0669 (15) 0.0004 (12) −0.0127 (12) −0.0235 (14)
C6 0.0538 (13) 0.0553 (13) 0.0505 (12) −0.0052 (10) −0.0133 (10) −0.0118 (10)
C7 0.0439 (14) 0.0775 (19) 0.095 (2) −0.0151 (12) −0.0167 (13) −0.0157 (16)
C8 0.0681 (19) 0.099 (2) 0.095 (2) −0.0250 (17) −0.0201 (17) −0.006 (2)
C9 0.082 (2) 0.150 (4) 0.098 (3) −0.045 (3) −0.019 (2) −0.018 (3)
C10 0.077 (2) 0.165 (4) 0.102 (3) −0.036 (3) −0.007 (2) −0.052 (3)
C11 0.0607 (18) 0.113 (3) 0.129 (3) −0.0204 (17) −0.0139 (19) −0.057 (3)
C12 0.0415 (13) 0.0823 (19) 0.096 (2) −0.0117 (12) −0.0158 (13) −0.0276 (16)
C13 0.131 (3) 0.077 (2) 0.090 (2) 0.0043 (19) −0.047 (2) −0.0267 (18)
C14 0.095 (2) 0.0486 (14) 0.0756 (17) 0.0042 (13) −0.0351 (16) −0.0201 (13)
C15 0.113 (3) 0.0626 (17) 0.0636 (16) −0.0043 (16) −0.0130 (16) −0.0199 (13)
C16 0.0724 (18) 0.0616 (16) 0.0770 (18) −0.0079 (13) −0.0066 (14) −0.0209 (14)
C17 0.0669 (15) 0.0398 (12) 0.0625 (14) 0.0040 (10) −0.0202 (12) −0.0113 (10)
C18 0.0655 (15) 0.0529 (14) 0.0629 (14) 0.0007 (11) −0.0178 (12) −0.0137 (11)
C19 0.0727 (17) 0.0596 (15) 0.0846 (19) −0.0003 (13) −0.0283 (15) −0.0213 (14)
C20 0.0626 (15) 0.0515 (14) 0.0749 (16) 0.0057 (11) −0.0262 (13) −0.0145 (12)
C21 0.0633 (15) 0.0659 (16) 0.0537 (14) −0.0124 (12) −0.0227 (11) −0.0084 (12)
C22 0.0615 (15) 0.0786 (18) 0.0563 (14) −0.0147 (13) −0.0149 (12) −0.0226 (14)
C23 0.0522 (14) 0.0626 (15) 0.0682 (15) −0.0056 (11) −0.0131 (11) −0.0265 (13)
C24 0.0393 (11) 0.0540 (13) 0.0609 (13) −0.0056 (9) −0.0159 (10) −0.0168 (11)
C25 0.0479 (12) 0.0544 (13) 0.0508 (12) −0.0033 (10) −0.0187 (10) −0.0132 (10)
C26 0.114 (3) 0.114 (3) 0.0588 (16) −0.019 (2) −0.0142 (16) −0.0323 (17)
C27 0.0556 (14) 0.0527 (13) 0.0729 (15) 0.0009 (10) −0.0198 (12) −0.0130 (12)
N1 0.186 (4) 0.134 (3) 0.112 (2) −0.004 (3) −0.083 (3) −0.044 (2)
N2 0.0505 (11) 0.0507 (11) 0.0562 (11) −0.0044 (8) −0.0207 (9) −0.0109 (9)

Geometric parameters (Å, °)

Ni1—S1 2.1459 (6) C13—C14 1.443 (4)
Ni1—S1i 2.1459 (6) C14—C15 1.380 (4)
Ni1—S2 2.1560 (6) C14—C19 1.392 (4)
Ni1—S2i 2.1560 (6) C15—C16 1.379 (4)
Ni2—S3ii 2.1451 (7) C15—H15 0.9300
Ni2—S3 2.1451 (7) C16—C17 1.388 (4)
Ni2—S4ii 2.1569 (8) C16—H16 0.9300
Ni2—S4 2.1569 (8) C17—C18 1.385 (3)
S1—C1 1.741 (3) C17—C20 1.506 (3)
S2—C6 1.747 (2) C18—C19 1.372 (3)
S3—C7 1.735 (3) C18—H18 0.9300
S4—C12 1.739 (3) C19—H19 0.9300
C1—C6 1.399 (3) C20—N2 1.491 (3)
C1—C2 1.400 (3) C20—H20A 0.9700
C2—C3 1.366 (4) C20—H20B 0.9700
C2—H2 0.9300 C21—N2 1.349 (3)
C3—C4 1.395 (4) C21—C22 1.370 (4)
C3—H3 0.9300 C21—H21 0.9300
C4—C5 1.368 (4) C22—C23 1.373 (4)
C4—H4 0.9300 C22—C26 1.518 (4)
C5—C6 1.397 (4) C23—C24 1.388 (3)
C5—H5 0.9300 C23—H23 0.9300
C7—C8 1.395 (4) C24—C25 1.374 (3)
C7—C12 1.407 (4) C24—C27 1.496 (3)
C8—C9 1.356 (5) C25—N2 1.341 (3)
C8—H8 0.9300 C25—H25 0.9300
C9—C10 1.377 (6) C26—H26A 0.9600
C9—H9 0.9300 C26—H26B 0.9600
C10—C11 1.379 (5) C26—H26C 0.9600
C10—H10 0.9300 C27—H27A 0.9600
C11—C12 1.414 (4) C27—H27B 0.9600
C11—H11 0.9300 C27—H27C 0.9600
C13—N1 1.133 (4)
S1—Ni1—S1i 180.00 (3) C15—C14—C13 119.2 (3)
S1—Ni1—S2 92.04 (2) C19—C14—C13 120.8 (3)
S1i—Ni1—S2 87.97 (2) C16—C15—C14 119.9 (3)
S1—Ni1—S2i 87.97 (2) C16—C15—H15 120.0
S1i—Ni1—S2i 92.03 (2) C14—C15—H15 120.0
S2—Ni1—S2i 180.0 C15—C16—C17 120.5 (3)
S3ii—Ni2—S3 180.00 (4) C15—C16—H16 119.8
S3ii—Ni2—S4ii 91.75 (3) C17—C16—H16 119.8
S3—Ni2—S4ii 88.25 (3) C18—C17—C16 119.0 (2)
S3ii—Ni2—S4 88.25 (3) C18—C17—C20 120.1 (2)
S3—Ni2—S4 91.75 (3) C16—C17—C20 120.9 (2)
S4ii—Ni2—S4 180.00 (2) C19—C18—C17 121.1 (2)
C1—S1—Ni1 104.89 (8) C19—C18—H18 119.5
C6—S2—Ni1 104.81 (8) C17—C18—H18 119.5
C7—S3—Ni2 105.49 (11) C18—C19—C14 119.5 (3)
C12—S4—Ni2 104.82 (11) C18—C19—H19 120.3
C6—C1—C2 119.0 (2) C14—C19—H19 120.3
C6—C1—S1 119.51 (18) N2—C20—C17 112.08 (18)
C2—C1—S1 121.47 (19) N2—C20—H20A 109.2
C3—C2—C1 120.5 (3) C17—C20—H20A 109.2
C3—C2—H2 119.7 N2—C20—H20B 109.2
C1—C2—H2 119.7 C17—C20—H20B 109.2
C2—C3—C4 120.5 (3) H20A—C20—H20B 107.9
C2—C3—H3 119.8 N2—C21—C22 120.2 (2)
C4—C3—H3 119.8 N2—C21—H21 119.9
C5—C4—C3 119.7 (3) C22—C21—H21 119.9
C5—C4—H4 120.1 C21—C22—C23 118.4 (2)
C3—C4—H4 120.1 C21—C22—C26 119.2 (3)
C4—C5—C6 120.7 (2) C23—C22—C26 122.3 (3)
C4—C5—H5 119.7 C22—C23—C24 122.0 (2)
C6—C5—H5 119.7 C22—C23—H23 119.0
C5—C6—C1 119.5 (2) C24—C23—H23 119.0
C5—C6—S2 121.75 (19) C25—C24—C23 116.6 (2)
C1—C6—S2 118.69 (19) C25—C24—C27 120.6 (2)
C8—C7—C12 119.3 (3) C23—C24—C27 122.8 (2)
C8—C7—S3 122.0 (3) N2—C25—C24 121.7 (2)
C12—C7—S3 118.7 (2) N2—C25—H25 119.1
C9—C8—C7 121.0 (4) C24—C25—H25 119.1
C9—C8—H8 119.5 C22—C26—H26A 109.5
C7—C8—H8 119.5 C22—C26—H26B 109.5
C8—C9—C10 120.2 (4) H26A—C26—H26B 109.5
C8—C9—H9 119.9 C22—C26—H26C 109.5
C10—C9—H9 119.9 H26A—C26—H26C 109.5
C9—C10—C11 121.3 (4) H26B—C26—H26C 109.5
C9—C10—H10 119.4 C24—C27—H27A 109.5
C11—C10—H10 119.4 C24—C27—H27B 109.5
C10—C11—C12 119.1 (4) H27A—C27—H27B 109.5
C10—C11—H11 120.4 C24—C27—H27C 109.5
C12—C11—H11 120.4 H27A—C27—H27C 109.5
C7—C12—C11 119.0 (3) H27B—C27—H27C 109.5
C7—C12—S4 119.2 (2) C25—N2—C21 121.1 (2)
C11—C12—S4 121.8 (3) C25—N2—C20 119.51 (19)
N1—C13—C14 178.7 (4) C21—N2—C20 119.3 (2)
C15—C14—C19 120.0 (2)
S2—Ni1—S1—C1 2.24 (8) C8—C7—C12—S4 −179.55 (19)
S2i—Ni1—S1—C1 −177.76 (8) S3—C7—C12—S4 0.3 (3)
S1—Ni1—S2—C6 −1.49 (8) C10—C11—C12—C7 0.6 (4)
S1i—Ni1—S2—C6 178.51 (8) C10—C11—C12—S4 −179.1 (2)
S4ii—Ni2—S3—C7 −177.93 (9) Ni2—S4—C12—C7 1.4 (2)
S4—Ni2—S3—C7 2.07 (9) Ni2—S4—C12—C11 −179.0 (2)
S3ii—Ni2—S4—C12 178.07 (8) C19—C14—C15—C16 −1.4 (4)
S3—Ni2—S4—C12 −1.93 (8) C13—C14—C15—C16 177.7 (3)
Ni1—S1—C1—C6 −2.8 (2) C14—C15—C16—C17 0.3 (4)
Ni1—S1—C1—C2 178.49 (18) C15—C16—C17—C18 0.7 (4)
C6—C1—C2—C3 −0.9 (4) C15—C16—C17—C20 −178.4 (2)
S1—C1—C2—C3 177.8 (2) C16—C17—C18—C19 −0.5 (4)
C1—C2—C3—C4 −0.4 (4) C20—C17—C18—C19 178.6 (2)
C2—C3—C4—C5 0.5 (5) C17—C18—C19—C14 −0.6 (4)
C3—C4—C5—C6 0.7 (4) C15—C14—C19—C18 1.5 (4)
C4—C5—C6—C1 −2.0 (4) C13—C14—C19—C18 −177.5 (3)
C4—C5—C6—S2 179.6 (2) C18—C17—C20—N2 −72.8 (3)
C2—C1—C6—C5 2.1 (3) C16—C17—C20—N2 106.3 (3)
S1—C1—C6—C5 −176.67 (18) N2—C21—C22—C23 −0.1 (3)
C2—C1—C6—S2 −179.45 (18) N2—C21—C22—C26 179.2 (2)
S1—C1—C6—S2 1.8 (3) C21—C22—C23—C24 −0.3 (3)
Ni1—S2—C6—C5 178.62 (18) C26—C22—C23—C24 −179.7 (2)
Ni1—S2—C6—C1 0.16 (19) C22—C23—C24—C25 0.3 (3)
Ni2—S3—C7—C8 178.04 (19) C22—C23—C24—C27 179.3 (2)
Ni2—S3—C7—C12 −1.8 (2) C23—C24—C25—N2 0.2 (3)
C12—C7—C8—C9 −1.4 (4) C27—C24—C25—N2 −178.85 (19)
S3—C7—C8—C9 178.8 (2) C24—C25—N2—C21 −0.7 (3)
C7—C8—C9—C10 0.6 (5) C24—C25—N2—C20 −177.0 (2)
C8—C9—C10—C11 0.8 (6) C22—C21—N2—C25 0.6 (3)
C9—C10—C11—C12 −1.4 (5) C22—C21—N2—C20 176.9 (2)
C8—C7—C12—C11 0.8 (4) C17—C20—N2—C25 −44.8 (3)
S3—C7—C12—C11 −179.4 (2) C17—C20—N2—C21 138.9 (2)

Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+1, −y+2, −z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RZ2554).

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 I, global. DOI: 10.1107/S1600536811004971/rz2554sup1.cif

e-67-0m339-sup1.cif (23.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811004971/rz2554Isup2.hkl

e-67-0m339-Isup2.hkl (221.9KB, hkl)

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


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