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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Jun 13;64(Pt 7):m911. doi: 10.1107/S1600536808017121

catena-Poly[[[bis­(O,O′-diisobutyl dithio­phosphato-κ2 S,S′)nickel(II)]-μ-1,2-bis­(4-pyridylmethyl­ene)hydrazine-κ2 N:N′] toluene disolvate]

Erick Berdugo a, Edward R T Tiekink a,*
PMCID: PMC2961896  PMID: 21202772

Abstract

The polymeric title compound, {[Ni(C8H18O2PS2)2(C12H10N4)]·2C7H7}n, has a linear topology and features octa­hedrally coordinated Ni atoms with a trans-N2S4 donor set. The toluene solvent mol­ecules occupy channels defined by the three-dimensional stacking of the polymeric chains. The Ni atom is located at a centre of inversion and the bridging 1,2-bis­(4-pyridylmethyl­ene)hydrazine4-pyridine mol­ecule is also disposed about a centre of inversion. One isobutoxy group is disordered equally over two positions.

Related literature

For a related structure, see: Berdugo et al. (2007). For related literature, see: Lai et al. (2004); Chen et al. (2006); Tiekink (2006); Benson et al. (2007).graphic file with name e-64-0m911-scheme1.jpg

Experimental

Crystal data

  • [Ni(C8H18O2PS2)2(C12H10N4)]·2C7H7

  • M r = 935.85

  • Triclinic, Inline graphic

  • a = 8.7132 (15) Å

  • b = 12.089 (2) Å

  • c = 12.293 (2) Å

  • α = 82.662 (10)°

  • β = 86.528 (10)°

  • γ = 69.321 (6)°

  • V = 1201.4 (4) Å3

  • Z = 1

  • Mo Kα radiation

  • μ = 0.69 mm−1

  • T = 98 (2) K

  • 0.30 × 0.20 × 0.10 mm

Data collection

  • Rigaku AFC12K/SATURN724 diffractometer

  • Absorption correction: multi-scan (ABSCOR; Higashi, 1995) T min = 0.795, T max = 1 (expected range = 0.742–0.934)

  • 8239 measured reflections

  • 5457 independent reflections

  • 4980 reflections with I > 2σ(I)

  • R int = 0.033

Refinement

  • R[F 2 > 2σ(F 2)] = 0.054

  • wR(F 2) = 0.142

  • S = 1.08

  • 5457 reflections

  • 279 parameters

  • H-atom parameters constrained

  • Δρmax = 0.64 e Å−3

  • Δρmin = −0.78 e Å−3

Data collection: CrystalClear (Rigaku, 2005); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEPII (Johnson, 1976) and DIAMOND (Brandenburg, 2006); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808017121/ng2459sup1.cif

e-64-0m911-sup1.cif (26.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808017121/ng2459Isup2.hkl

e-64-0m911-Isup2.hkl (267.2KB, 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
C12—H12⋯S1i 0.95 2.76 3.694 (3) 169

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors gratefully thank the MBRS–RISE program (GM60655) for support and Cheminova is thanked for the gift of the dithiophosphate used in this study.

supplementary crystallographic information

Comment

Interest in examining structures related to the title compound (I), Fig. 1, relates in the main to attempts to control polymer formation and when formed topology (Lai et al., 2004; Chen et al. 2006; Tiekink, 2006; Benson et al., 2007 & Berdugo et al., 2007). A linear polymer is found in (I), Fig. 2, in which the Ni atom is located on a centre of inversion and the bridging 4-pyridinealdazine ligand is disposed about another centre of inversion. The Ni atom exists in a trans-N2S4 octahedral coordination geommetry. The polymers are aligned along the c-direction and form layers in the ac-plane that are stabilized by C—H···S contacts, Table 1. Layers stack along the b axis and define approximate squares with Ni···Ni edges 12.1 and 12.3 Å. Despite the fact that the isobutyl residues protrude into the resulting channels, the toluene molecules are accommodated in these as seen in Fig. 3.

Experimental

The title compound was prepared by refluxing equimolar amounts of the parent nickel dithiophosphate with 4-pyridinealdazine (Sigma-Aldrich) in toluene (30 ml) for 30 min following a literature procedure (Berdugo et al., 2007). Brown crystals of (I) were isolated by the slow evaporation (3 days) of this toluene solution. The crystals lost crystallinity with standing in air after a few minutes. IR (cm-1): v(C—O) 1126, v(P—O) 951, v(P—S)asymm 672, v(P—S)sym 593.

Refinement

The methyene-C5 and methine-C6 atoms of the O2—C5—C8 butyl group were disordered over two sites with s.o.f. = 0.5 (from anisotropic refinement); the O2, C7 and C8 atoms were localized in one site only. The H atoms were geometrically placed (C—H = 0.95–1.00 Å) and refined as riding with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C).

Figures

Fig. 1.

Fig. 1.

Coordination geometry of the Ni atom in (I) showing the crystallographic numbering scheme. Displacement ellipsoids are shown at the 70% probability level. Symmetry operation i: 1 - x, 1 - y, 1 - z & ii: 2 - x, 1 - y, 2 - z. Only one orientation of the disordered O2—C5—C8 butyl group is shown for clarity.

Fig. 2.

Fig. 2.

Polymer topology in (I). Colour code: Ni (orange), S (yellow), P (pink), O (red), N (blue), C (grey) & H (green).

Fig. 3.

Fig. 3.

A view of the crystal packing in (I) highlighting the channels occupied by the solvent toluene molecules (four shown in space filling mode). Colour code as for Fig. 2.

Crystal data

[Ni(C8H18O2PS2)2(C12H10N4)]·2C7H7 Z = 1
Mr = 935.85 F(000) = 496
Triclinic, P1 Dx = 1.294 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71070 Å
a = 8.7132 (15) Å Cell parameters from 4131 reflections
b = 12.089 (2) Å θ = 2.3–40.7°
c = 12.293 (2) Å µ = 0.69 mm1
α = 82.662 (10)° T = 98 K
β = 86.528 (10)° Prism, brown-orange
γ = 69.321 (6)° 0.30 × 0.20 × 0.10 mm
V = 1201.4 (4) Å3

Data collection

Rigaku AFC12K/SATURN724 diffractometer 5457 independent reflections
Radiation source: fine-focus sealed tube 4980 reflections with I > 2σ(I)
graphite Rint = 0.033
ω scans θmax = 27.5°, θmin = 2.3°
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) h = −11→11
Tmin = 0.795, Tmax = 1 k = −13→15
8239 measured reflections l = −15→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)] = 0.054 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.142 H-atom parameters constrained
S = 1.08 w = 1/[σ2(Fo2) + (0.064P)2 + 1.4047P] where P = (Fo2 + 2Fc2)/3
5457 reflections (Δ/σ)max < 0.001
279 parameters Δρmax = 0.64 e Å3
0 restraints Δρmin = −0.78 e Å3

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 Occ. (<1)
Ni 0.5000 0.5000 0.5000 0.02039 (14)
S1 0.38649 (8) 0.38353 (7) 0.64197 (5) 0.02552 (17)
S2 0.67986 (8) 0.29788 (6) 0.46088 (5) 0.02452 (16)
P1 0.55031 (9) 0.24313 (7) 0.58030 (6) 0.02530 (17)
O1 0.6644 (3) 0.15123 (18) 0.67162 (16) 0.0295 (4)
N1 0.6658 (3) 0.5003 (2) 0.61646 (17) 0.0205 (4)
N2 0.9368 (3) 0.5058 (2) 0.96412 (18) 0.0256 (5)
C1 0.7711 (4) 0.1916 (3) 0.7302 (2) 0.0309 (6)
H1A 0.7063 0.2423 0.7859 0.037*
H1B 0.8205 0.2396 0.6782 0.037*
C2 0.9051 (4) 0.0857 (3) 0.7856 (2) 0.0303 (6)
H2 0.9674 0.0343 0.7286 0.036*
C3 1.0219 (4) 0.1321 (3) 0.8386 (3) 0.0420 (8)
H3A 1.1097 0.0648 0.8754 0.063*
H3B 0.9610 0.1855 0.8923 0.063*
H3C 1.0695 0.1755 0.7818 0.063*
C4 0.8358 (5) 0.0118 (3) 0.8709 (3) 0.0399 (8)
H4A 0.9260 −0.0558 0.9049 0.060*
H4B 0.7624 −0.0175 0.8352 0.060*
H4C 0.7744 0.0613 0.9273 0.060*
O2 0.4688 (3) 0.1558 (2) 0.54352 (18) 0.0365 (5) 0.50
C5 0.3314 (8) 0.2219 (5) 0.4584 (5) 0.0237 (12) 0.50
H5A 0.2908 0.3076 0.4683 0.028* 0.50
H5B 0.3821 0.2143 0.3842 0.028* 0.50
C6 0.2185 (9) 0.1915 (8) 0.4606 (6) 0.0447 (17) 0.50
H6A 0.1330 0.2627 0.4881 0.054* 0.50
C7 0.1788 (5) 0.0918 (4) 0.5366 (3) 0.0565 (11) 0.50
H7A 0.0721 0.0903 0.5173 0.085* 0.50
H7B 0.1752 0.1075 0.6131 0.085* 0.50
H7C 0.2640 0.0148 0.5273 0.085* 0.50
C8 0.1386 (4) 0.1940 (3) 0.3445 (3) 0.0392 (7) 0.50
H8A 0.0449 0.1669 0.3574 0.059* 0.50
H8B 0.2210 0.1413 0.2985 0.059* 0.50
H8C 0.1017 0.2754 0.3073 0.059* 0.50
O32 0.4688 (3) 0.1558 (2) 0.54352 (18) 0.0365 (5) 0.50
C35 0.3937 (10) 0.1619 (8) 0.4454 (5) 0.0359 (15) 0.50
H35A 0.3574 0.2468 0.4149 0.043* 0.50
H35B 0.4830 0.1191 0.3961 0.043* 0.50
C36 0.2674 (7) 0.1257 (5) 0.4299 (5) 0.0216 (10) 0.50
H36A 0.3227 0.0475 0.4005 0.026* 0.50
C37 0.1788 (5) 0.0918 (4) 0.5366 (3) 0.0565 (11) 0.50
H37A 0.0915 0.0649 0.5169 0.085* 0.50
H37B 0.1312 0.1616 0.5767 0.085* 0.50
H37C 0.2582 0.0278 0.5830 0.085* 0.50
C38 0.1386 (4) 0.1940 (3) 0.3445 (3) 0.0392 (7) 0.50
H38A 0.0580 0.1546 0.3438 0.059* 0.50
H38B 0.1916 0.1960 0.2720 0.059* 0.50
H38C 0.0833 0.2755 0.3627 0.059* 0.50
C9 0.6097 (3) 0.5338 (2) 0.7157 (2) 0.0226 (5)
H9 0.4946 0.5601 0.7293 0.027*
C10 0.7099 (3) 0.5319 (2) 0.7990 (2) 0.0227 (5)
H10 0.6648 0.5576 0.8676 0.027*
C11 0.8794 (3) 0.4915 (2) 0.7802 (2) 0.0214 (5)
C12 0.9386 (3) 0.4578 (2) 0.6774 (2) 0.0224 (5)
H12 1.0532 0.4305 0.6617 0.027*
C13 0.8285 (3) 0.4644 (2) 0.5982 (2) 0.0225 (5)
H13 0.8699 0.4425 0.5278 0.027*
C14 0.9924 (3) 0.4844 (2) 0.8672 (2) 0.0236 (5)
H14 1.1066 0.4638 0.8516 0.028*
C15 0.5105 (4) 0.7783 (3) −0.0282 (3) 0.0331 (7)
C16 0.4464 (4) 0.6899 (3) 0.0108 (3) 0.0341 (7)
H16 0.4841 0.6424 0.0782 0.041*
C17 0.3289 (4) 0.6702 (3) −0.0467 (3) 0.0396 (7)
H17 0.2853 0.6104 −0.0182 0.048*
C18 0.2746 (4) 0.7376 (3) −0.1460 (3) 0.0412 (8)
H18 0.1939 0.7242 −0.1858 0.049*
C19 0.3388 (5) 0.8241 (3) −0.1867 (3) 0.0409 (8)
H19 0.3024 0.8700 −0.2550 0.049*
C20 0.4562 (4) 0.8450 (3) −0.1289 (3) 0.0374 (7)
H20 0.4995 0.9048 −0.1578 0.045*
C21 0.6361 (5) 0.8005 (3) 0.0363 (3) 0.0461 (8)
H21A 0.6290 0.7699 0.1134 0.069*
H21B 0.6150 0.8862 0.0304 0.069*
H21C 0.7460 0.7598 0.0069 0.069*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Ni 0.0115 (2) 0.0342 (3) 0.0152 (2) −0.00714 (19) −0.00478 (17) −0.00191 (18)
S1 0.0150 (3) 0.0399 (4) 0.0199 (3) −0.0084 (3) −0.0028 (2) 0.0008 (3)
S2 0.0158 (3) 0.0365 (4) 0.0203 (3) −0.0070 (3) −0.0042 (2) −0.0037 (3)
P1 0.0194 (3) 0.0345 (4) 0.0219 (3) −0.0092 (3) −0.0064 (3) −0.0007 (3)
O1 0.0293 (11) 0.0306 (10) 0.0278 (10) −0.0096 (9) −0.0100 (9) 0.0017 (8)
N1 0.0135 (10) 0.0313 (11) 0.0171 (10) −0.0078 (9) −0.0058 (8) −0.0010 (8)
N2 0.0194 (11) 0.0366 (12) 0.0227 (11) −0.0107 (10) −0.0096 (9) −0.0029 (9)
C1 0.0312 (15) 0.0320 (14) 0.0269 (14) −0.0061 (12) −0.0147 (12) −0.0020 (11)
C2 0.0295 (15) 0.0310 (14) 0.0238 (13) −0.0015 (12) −0.0073 (12) −0.0019 (11)
C3 0.0416 (19) 0.0414 (17) 0.0380 (17) −0.0051 (15) −0.0229 (15) −0.0037 (14)
C4 0.0437 (19) 0.0377 (16) 0.0264 (15) −0.0022 (14) −0.0030 (14) 0.0049 (13)
O2 0.0376 (12) 0.0486 (13) 0.0326 (11) −0.0256 (11) −0.0088 (10) −0.0040 (10)
C5 0.020 (3) 0.016 (2) 0.031 (3) −0.001 (2) −0.017 (2) 0.003 (2)
C6 0.032 (4) 0.058 (5) 0.043 (4) −0.019 (4) −0.015 (3) 0.015 (4)
C7 0.045 (2) 0.084 (3) 0.049 (2) −0.042 (2) −0.0094 (18) 0.022 (2)
C8 0.0304 (16) 0.0492 (18) 0.0411 (18) −0.0182 (15) −0.0093 (14) 0.0007 (15)
O32 0.0376 (12) 0.0486 (13) 0.0326 (11) −0.0256 (11) −0.0088 (10) −0.0040 (10)
C35 0.037 (4) 0.053 (5) 0.027 (3) −0.028 (4) −0.006 (3) 0.001 (3)
C36 0.024 (3) 0.016 (2) 0.027 (3) −0.007 (2) −0.001 (2) −0.008 (2)
C37 0.045 (2) 0.084 (3) 0.049 (2) −0.042 (2) −0.0094 (18) 0.022 (2)
C38 0.0304 (16) 0.0492 (18) 0.0411 (18) −0.0182 (15) −0.0093 (14) 0.0007 (15)
C9 0.0167 (12) 0.0315 (13) 0.0190 (12) −0.0071 (10) −0.0057 (10) −0.0022 (10)
C10 0.0190 (12) 0.0303 (13) 0.0192 (12) −0.0082 (10) −0.0061 (10) −0.0024 (10)
C11 0.0174 (12) 0.0281 (12) 0.0204 (12) −0.0098 (10) −0.0075 (10) 0.0000 (10)
C12 0.0135 (11) 0.0305 (13) 0.0231 (12) −0.0080 (10) −0.0041 (10) 0.0001 (10)
C13 0.0145 (12) 0.0324 (13) 0.0207 (12) −0.0080 (10) −0.0035 (10) −0.0019 (10)
C14 0.0188 (12) 0.0301 (13) 0.0239 (12) −0.0102 (10) −0.0075 (10) −0.0020 (10)
C15 0.0297 (15) 0.0316 (14) 0.0328 (16) −0.0039 (12) 0.0015 (13) −0.0061 (12)
C16 0.0316 (16) 0.0323 (14) 0.0305 (15) −0.0035 (12) 0.0062 (13) −0.0006 (12)
C17 0.0360 (17) 0.0420 (17) 0.0404 (18) −0.0140 (14) 0.0092 (14) −0.0067 (14)
C18 0.0318 (17) 0.0471 (18) 0.0415 (18) −0.0079 (15) 0.0004 (14) −0.0119 (15)
C19 0.0439 (19) 0.0386 (16) 0.0303 (16) −0.0030 (15) −0.0023 (14) −0.0010 (13)
C20 0.0431 (18) 0.0309 (15) 0.0340 (16) −0.0091 (14) 0.0030 (14) −0.0010 (13)
C21 0.046 (2) 0.0434 (18) 0.050 (2) −0.0162 (16) −0.0097 (17) −0.0032 (16)

Geometric parameters (Å, °)

Ni—N1 2.096 (2) C8—H8C 0.9800
Ni—N1i 2.096 (2) O32—C35 1.388 (7)
Ni—S1i 2.4806 (8) C35—C36 1.352 (8)
Ni—S1 2.4806 (8) C35—H35A 0.9900
Ni—S2 2.4823 (8) C35—H35B 0.9900
Ni—S2i 2.4823 (8) C36—C38 1.519 (6)
S1—P1 1.9949 (11) C36—C37 1.564 (7)
S2—P1 1.9864 (10) C36—H36A 1.0000
P1—O32 1.585 (2) C37—H37A 0.9800
P1—O2 1.585 (2) C37—H37B 0.9800
P1—O1 1.587 (2) C37—H37C 0.9800
O1—C1 1.453 (3) C38—H38A 0.9800
N1—C13 1.342 (3) C38—H38B 0.9800
N1—C9 1.344 (3) C38—H38C 0.9800
N2—C14 1.281 (4) C9—C10 1.379 (3)
N2—N2ii 1.410 (4) C9—H9 0.9500
C1—C2 1.511 (4) C10—C11 1.396 (4)
C1—H1A 0.9900 C10—H10 0.9500
C1—H1B 0.9900 C11—C12 1.391 (4)
C2—C4 1.525 (4) C11—C14 1.472 (3)
C2—C3 1.533 (4) C12—C13 1.384 (3)
C2—H2 1.0000 C12—H12 0.9500
C3—H3A 0.9800 C13—H13 0.9500
C3—H3B 0.9800 C14—H14 0.9500
C3—H3C 0.9800 C15—C16 1.393 (4)
C4—H4A 0.9800 C15—C20 1.398 (4)
C4—H4B 0.9800 C15—C21 1.505 (5)
C4—H4C 0.9800 C16—C17 1.381 (5)
O2—C5 1.558 (6) C16—H16 0.9500
C5—C6 1.164 (9) C17—C18 1.387 (5)
C5—H5A 0.9900 C17—H17 0.9500
C5—H5B 0.9900 C18—C19 1.380 (5)
C6—C7 1.553 (8) C18—H18 0.9500
C6—C8 1.617 (8) C19—C20 1.389 (5)
C6—H6A 1.0000 C19—H19 0.9500
C7—H7A 0.9800 C20—H20 0.9500
C7—H7B 0.9800 C21—H21A 0.9800
C7—H7C 0.9800 C21—H21B 0.9800
C8—H8A 0.9800 C21—H21C 0.9800
C8—H8B 0.9800
N1—Ni—N1i 180.0 H7B—C7—H7C 109.5
N1—Ni—S1i 91.71 (6) C6—C8—H8A 109.5
N1i—Ni—S1i 88.29 (6) C6—C8—H8B 109.5
N1—Ni—S1 88.29 (6) H8A—C8—H8B 109.5
N1i—Ni—S1 91.71 (6) C6—C8—H8C 109.5
S1i—Ni—S1 180.00 (3) H8A—C8—H8C 109.5
N1—Ni—S2 90.35 (6) H8B—C8—H8C 109.5
N1i—Ni—S2 89.65 (6) C35—O32—P1 129.0 (3)
S1i—Ni—S2 98.04 (3) C36—C35—O32 127.6 (6)
S1—Ni—S2 81.96 (3) C36—C35—H35A 105.4
N1—Ni—S2i 89.65 (6) O32—C35—H35A 105.4
N1i—Ni—S2i 90.35 (6) C36—C35—H35B 105.4
S1i—Ni—S2i 81.96 (3) O32—C35—H35B 105.4
S1—Ni—S2i 98.04 (3) H35A—C35—H35B 106.0
S2—Ni—S2i 180.0 C35—C36—C38 120.7 (5)
P1—S1—Ni 84.11 (3) C35—C36—C37 115.7 (5)
P1—S2—Ni 84.24 (3) C38—C36—C37 108.6 (4)
O32—P1—O2 0.00 (17) C35—C36—H36A 103.1
O32—P1—O1 96.75 (12) C38—C36—H36A 103.1
O2—P1—O1 96.75 (12) C37—C36—H36A 103.1
O32—P1—S2 113.02 (9) C36—C37—H37A 109.5
O2—P1—S2 113.02 (9) C36—C37—H37B 109.5
O1—P1—S2 111.99 (9) H37A—C37—H37B 109.5
O32—P1—S1 112.44 (10) C36—C37—H37C 109.5
O2—P1—S1 112.44 (10) H37A—C37—H37C 109.5
O1—P1—S1 112.53 (9) H37B—C37—H37C 109.5
S2—P1—S1 109.66 (5) C36—C38—H38A 109.5
C1—O1—P1 117.69 (18) C36—C38—H38B 109.5
C13—N1—C9 117.5 (2) H38A—C38—H38B 109.5
C13—N1—Ni 122.93 (18) C36—C38—H38C 109.5
C9—N1—Ni 119.51 (17) H38A—C38—H38C 109.5
C14—N2—N2ii 111.6 (3) H38B—C38—H38C 109.5
O1—C1—C2 109.9 (2) N1—C9—C10 123.6 (2)
O1—C1—H1A 109.7 N1—C9—H9 118.2
C2—C1—H1A 109.7 C10—C9—H9 118.2
O1—C1—H1B 109.7 C9—C10—C11 118.5 (2)
C2—C1—H1B 109.7 C9—C10—H10 120.8
H1A—C1—H1B 108.2 C11—C10—H10 120.8
C1—C2—C4 111.8 (3) C12—C11—C10 118.4 (2)
C1—C2—C3 108.0 (3) C12—C11—C14 120.9 (2)
C4—C2—C3 110.8 (3) C10—C11—C14 120.8 (2)
C1—C2—H2 108.7 C13—C12—C11 119.1 (2)
C4—C2—H2 108.7 C13—C12—H12 120.4
C3—C2—H2 108.7 C11—C12—H12 120.4
C2—C3—H3A 109.5 N1—C13—C12 122.9 (2)
C2—C3—H3B 109.5 N1—C13—H13 118.6
H3A—C3—H3B 109.5 C12—C13—H13 118.6
C2—C3—H3C 109.5 N2—C14—C11 119.9 (2)
H3A—C3—H3C 109.5 N2—C14—H14 120.0
H3B—C3—H3C 109.5 C11—C14—H14 120.0
C2—C4—H4A 109.5 C16—C15—C20 118.4 (3)
C2—C4—H4B 109.5 C16—C15—C21 120.7 (3)
H4A—C4—H4B 109.5 C20—C15—C21 120.9 (3)
C2—C4—H4C 109.5 C17—C16—C15 121.2 (3)
H4A—C4—H4C 109.5 C17—C16—H16 119.4
H4B—C4—H4C 109.5 C15—C16—H16 119.4
C5—O2—P1 111.3 (3) C16—C17—C18 120.0 (3)
C6—C5—O2 117.8 (6) C16—C17—H17 120.0
C6—C5—H5A 107.9 C18—C17—H17 120.0
O2—C5—H5A 107.9 C19—C18—C17 119.5 (3)
C6—C5—H5B 107.9 C19—C18—H18 120.2
O2—C5—H5B 107.9 C17—C18—H18 120.2
H5A—C5—H5B 107.2 C18—C19—C20 120.8 (3)
C5—C6—C7 130.3 (6) C18—C19—H19 119.6
C5—C6—C8 117.4 (6) C20—C19—H19 119.6
C7—C6—C8 104.4 (5) C19—C20—C15 120.1 (3)
C5—C6—H6A 99.3 C19—C20—H20 120.0
C7—C6—H6A 99.3 C15—C20—H20 120.0
C8—C6—H6A 99.3 C15—C21—H21A 109.5
C6—C7—H7A 109.5 C15—C21—H21B 109.5
C6—C7—H7B 109.5 H21A—C21—H21B 109.5
H7A—C7—H7B 109.5 C15—C21—H21C 109.5
C6—C7—H7C 109.5 H21A—C21—H21C 109.5
H7A—C7—H7C 109.5 H21B—C21—H21C 109.5
N1—Ni—S1—P1 −91.85 (7) O32—P1—O2—C5 0(43)
N1i—Ni—S1—P1 88.15 (7) O1—P1—O2—C5 174.5 (3)
S1i—Ni—S1—P1 114 (100) S2—P1—O2—C5 −68.1 (3)
S2—Ni—S1—P1 −1.26 (3) S1—P1—O2—C5 56.7 (3)
S2i—Ni—S1—P1 178.74 (3) P1—O2—C5—C6 −146.3 (7)
N1—Ni—S2—P1 89.49 (7) O2—C5—C6—C7 −0.2 (15)
N1i—Ni—S2—P1 −90.51 (7) O2—C5—C6—C8 −143.8 (5)
S1i—Ni—S2—P1 −178.74 (3) O2—P1—O32—C35 0(59)
S1—Ni—S2—P1 1.26 (3) O1—P1—O32—C35 −158.0 (5)
S2i—Ni—S2—P1 16 (100) S2—P1—O32—C35 −40.6 (5)
Ni—S2—P1—O32 124.67 (10) S1—P1—O32—C35 84.2 (5)
Ni—S2—P1—O2 124.67 (10) P1—O32—C35—C36 −147.9 (7)
Ni—S2—P1—O1 −127.32 (9) O32—C35—C36—C38 144.5 (7)
Ni—S2—P1—S1 −1.65 (4) O32—C35—C36—C37 10.4 (12)
Ni—S1—P1—O32 −124.99 (10) C13—N1—C9—C10 −0.6 (4)
Ni—S1—P1—O2 −124.99 (10) Ni—N1—C9—C10 177.1 (2)
Ni—S1—P1—O1 127.01 (9) N1—C9—C10—C11 −1.0 (4)
Ni—S1—P1—S2 1.65 (4) C9—C10—C11—C12 1.5 (4)
O32—P1—O1—C1 178.8 (2) C9—C10—C11—C14 −178.2 (2)
O2—P1—O1—C1 178.8 (2) C10—C11—C12—C13 −0.5 (4)
S2—P1—O1—C1 60.6 (2) C14—C11—C12—C13 179.2 (2)
S1—P1—O1—C1 −63.5 (2) C9—N1—C13—C12 1.7 (4)
N1i—Ni—N1—C13 83 (100) Ni—N1—C13—C12 −175.9 (2)
S1i—Ni—N1—C13 −52.9 (2) C11—C12—C13—N1 −1.1 (4)
S1—Ni—N1—C13 127.1 (2) N2ii—N2—C14—C11 179.8 (3)
S2—Ni—N1—C13 45.1 (2) C12—C11—C14—N2 −173.9 (3)
S2i—Ni—N1—C13 −134.9 (2) C10—C11—C14—N2 5.8 (4)
N1i—Ni—N1—C9 −95 (100) C20—C15—C16—C17 −1.6 (5)
S1i—Ni—N1—C9 129.46 (19) C21—C15—C16—C17 178.8 (3)
S1—Ni—N1—C9 −50.54 (19) C15—C16—C17—C18 1.0 (5)
S2—Ni—N1—C9 −132.48 (19) C16—C17—C18—C19 0.0 (5)
S2i—Ni—N1—C9 47.52 (19) C17—C18—C19—C20 −0.5 (5)
P1—O1—C1—C2 −162.1 (2) C18—C19—C20—C15 −0.1 (5)
O1—C1—C2—C4 −62.2 (3) C16—C15—C20—C19 1.1 (5)
O1—C1—C2—C3 175.6 (3) C21—C15—C20—C19 −179.3 (3)

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

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C12—H12···S1iii 0.95 2.76 3.694 (3) 169

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG2459).

References

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  2. Berdugo, E., Tiekink, E. R. T., Wardell, J. L. & Wardell, S. M. S. V. (2007). Acta Cryst. E63, m764–m766.
  3. Brandenburg, K. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
  4. Chen, D., Lai, C. S. & Tiekink, E. R. T. (2006). CrystEngComm, 8, 51–58.
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  10. Tiekink, E. R. T. (2006). CrystEngComm, 6, 104–118.

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/S1600536808017121/ng2459sup1.cif

e-64-0m911-sup1.cif (26.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808017121/ng2459Isup2.hkl

e-64-0m911-Isup2.hkl (267.2KB, hkl)

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


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