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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Aug 2;67(Pt 9):m1184. doi: 10.1107/S1600536811028510

Bis(η5-1-tert-butyl­inden­yl)nickel(II)

Heiko Bauer a, Yu Sun a, Helmut Sitzmann a,*
PMCID: PMC3200892  PMID: 22065650

Abstract

The title compound, [Ni(C13H15)2], shows a slightly distorted sandwich structure with two independent mol­ecules in the asymmetric unit. Both Ni atoms are located on crystallographic centres of inversion.

Related literature

For the synthetic procedure of the analogous indenylcobalt complex, see: Gou et al. (2007). For a description of the Cambridge Structural Database, see: Allen (2002). For the use of bis­(inden­yl)nickel(II) complexes as starting compounds for poly- and oligomerization catalysts, see: Xie et al. (2009); Fontaine & Zargarian et al. (2004). For the indenyl effect in SN1, SN2 and other reactions, see: Elschenbroich (2008); Rerek & Basolo (1984); Rerek et al. (1983), O’Connor & Casey (1987); Turaki et al. (1988); Caddy et al. (1978); Bönnemann (1985); Marder et al. (1988).graphic file with name e-67-m1184-scheme1.jpg

Experimental

Crystal data

  • [Ni(C13H15)2]

  • M r = 401.21

  • Triclinic, Inline graphic

  • a = 9.8116 (5) Å

  • b = 10.9631 (7) Å

  • c = 11.1658 (7) Å

  • α = 68.800 (6)°

  • β = 67.085 (5)°

  • γ = 85.212 (4)°

  • V = 1029.10 (11) Å3

  • Z = 2

  • Cu Kα radiation

  • μ = 1.38 mm−1

  • T = 150 K

  • 0.11 × 0.07 × 0.04 mm

Data collection

  • Oxford Diffraction Xcalibur Sapphire3 Gemini ultra diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) T min = 0.675, T max = 1.000

  • 8813 measured reflections

  • 3283 independent reflections

  • 2838 reflections with I > 2σ(I)

  • R int = 0.022

Refinement

  • R[F 2 > 2σ(F 2)] = 0.027

  • wR(F 2) = 0.075

  • S = 1.07

  • 3283 reflections

  • 253 parameters

  • H-atom parameters constrained

  • Δρmax = 0.24 e Å−3

  • Δρmin = −0.25 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2010); cell refinement: CrysAlis RED (Oxford Diffraction, 2010); data reduction: CrysAlis RED; program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SCHAKAL99 (Keller, 1999); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811028510/im2294sup1.cif

e-67-m1184-sup1.cif (24.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811028510/im2294Isup2.hkl

e-67-m1184-Isup2.hkl (157.7KB, hkl)

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

supplementary crystallographic information

Comment

The catalytic activity of indenylnickel(II) complexes has stimulated recent research activity. It is e.g. possible to oligomerize phenylsilane in the presence of a methylindenylnickel(II) phosphine complex (Fontaine & Zargarian, 2004). N-heterocyclic carbene complexes of indenylnickel(II) chloride have been shown to polymerize styrene (Xie et al., 2009). The starting compounds for these complexes are bis(indenyl)nickel(II) and bis(1-methylindenyl)nickel(II). With the well known indenyl effect (Elschenbroich, 2008) based on a slip-fold distortion of the indenyl ligand from η5 to η3 coordination, which greatly enhances the reactivity in SN1 and SN2 substitution reactions (Rerek & Basolo 1984, Rerek et al. 1983; O'Connor & Casey, 1987; Turaki et al., 1988) and other reactions, (Caddy et al., 1978; Bönnemann, 1985; Marder et al., 1988) the as yet unknown bis(η5-1-tert-butylindenyl)nickel(II) complex became interesting to us as a promising starting compound.

The title compound was synthesized from lithium 1-tert-butylindenide and nickel(II) bromide dimethoxyethane complex and crystallized as dark red prisms. In the structure shown here, the nickel atom is bound to the carbon atoms of the five-membered ring of the ligand by a distorted η5-coordination. The metal ion is positioned on a crystallographic centre of inversion and the two indenyl ligands are therefore arranged in a staggered coordination with a rotation angle of 180°. As known from similar complexes (Gou et al., 2007), the lengths of the five Ni—C bonds are split in two sets. The three shorter bond distances are 2.124 (1) Å, 1.994 (2) Å and 2.049 (2) Å, the two longer bond distances are 2.460 (2) Å and 2.505 (1) Å, which is even longer than for the Co complex (Gou et al., 2007). The distance between the nickel centre and the centroid of the five-membered ring is 1.7950 (8) Å. The folding angle of 4.28 (7)° shows a slightly smaller value than for unsubstituted indenyl complexes (Rerek et al., 1983). The two different bond length ranges are in accordance with the usual η2+η3-coordination of the indenyl ligand resulting from the reluctant participation of the benzene ring in the ligand-metal electron donation (Rerek et al., 1983). The bond between C1 and C10 is bending out 7.2 (1)° of the ring plane.

Experimental

To a stirred solution of 1-tert-butylindene (862 mg, 5.0 mmol) in diethyl ether (10 ml) a solution of n-BuLi (1.6 mol/l, 3.44 ml, 5.5 mmol) in hexane was added slowly at 0 °C. Stirring was continued for 19 h at room temperature, then the solvent was removed in vacuo. The resulting white precipitate was suspended in pentane, cooled overnight in a fridge, filtered and washed with pentane. The lithium 1-tert-butylindenide was suspended in THF (10 ml) and NiBr2 × dme (1.54 g, 5.0 mmol) was added. The mixture was stirred for 24 h at room temperature. The solvent was removed in vacuo and the residue extracted with pentane. The product was obtained as dark red prisms at -30 °C (323 mg, 16%).

Refinement

All hydrogen atoms were placed in calculated positions (C—H 0.95 or 0.98 Å) and refined by using a riding model, with Uiso(H)=1.2–1.5 Ueq of the parent atom.

Figures

Fig. 1.

Fig. 1.

View of the title compound showing thermal ellipsoids at the 50% probability level.

Fig. 2.

Fig. 2.

View of the title compound showing the folding angle of the indenyl ligand.

Crystal data

[Ni(C13H15)2] Z = 2
Mr = 401.21 F(000) = 428
Triclinic, P1 Dx = 1.295 Mg m3
Hall symbol: -P 1 Cu Kα radiation, λ = 1.54184 Å
a = 9.8116 (5) Å Cell parameters from 5554 reflections
b = 10.9631 (7) Å θ = 4.3–62.6°
c = 11.1658 (7) Å µ = 1.38 mm1
α = 68.800 (6)° T = 150 K
β = 67.085 (5)° Transparent prism, red
γ = 85.212 (4)° 0.11 × 0.07 × 0.04 mm
V = 1029.10 (11) Å3

Data collection

Oxford Diffraction Xcalibur Sapphire3 Gemini ultra diffractometer 3283 independent reflections
Radiation source: Enhance Ultra (Cu) X-ray Source 2838 reflections with I > 2σ(I)
mirror Rint = 0.022
Detector resolution: 16.1399 pixels mm-1 θmax = 62.6°, θmin = 4.3°
ω scans h = −9→11
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) k = −12→12
Tmin = 0.675, Tmax = 1.000 l = −12→12
8813 measured reflections

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)] = 0.027 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.075 H-atom parameters constrained
S = 1.07 w = 1/[σ2(Fo2) + (0.049P)2] where P = (Fo2 + 2Fc2)/3
3283 reflections (Δ/σ)max < 0.001
253 parameters Δρmax = 0.24 e Å3
0 restraints Δρmin = −0.25 e Å3

Special details

Experimental. CrysAlisPro, Oxford Diffraction Ltd., Version 1.171.33.66 (release 28-04-2010 CrysAlis171 .NET) (compiled Apr 28 2010,14:27:37) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
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)

x y z Uiso*/Ueq
C1 0.69298 (15) 0.98880 (15) 0.83091 (15) 0.0224 (3)
C2 0.66605 (16) 1.11686 (15) 0.83603 (16) 0.0253 (3)
H2 0.7279 1.1686 0.8495 0.030*
C3 0.53173 (17) 1.15413 (15) 0.81780 (16) 0.0262 (3)
H3 0.4779 1.2263 0.8348 0.031*
C4 0.49048 (16) 1.06274 (15) 0.76852 (15) 0.0246 (3)
C5 0.59070 (15) 0.96046 (14) 0.77499 (15) 0.0215 (3)
C6 0.57746 (17) 0.85971 (15) 0.73069 (16) 0.0265 (3)
H6 0.6427 0.7906 0.7348 0.032*
C7 0.46801 (18) 0.86187 (17) 0.68070 (17) 0.0334 (4)
H7 0.4605 0.7948 0.6481 0.040*
C8 0.36868 (18) 0.96052 (18) 0.67725 (18) 0.0360 (4)
H8 0.2937 0.9589 0.6438 0.043*
C9 0.37800 (17) 1.06062 (17) 0.72184 (17) 0.0325 (4)
H9 0.3091 1.1269 0.7208 0.039*
C10 0.83254 (16) 0.91731 (16) 0.83483 (17) 0.0273 (3)
C11 0.79792 (18) 0.76942 (17) 0.91908 (18) 0.0370 (4)
H11A 0.7370 0.7558 1.0169 0.056*
H11B 0.8908 0.7264 0.9126 0.056*
H11C 0.7439 0.7319 0.8815 0.056*
C12 0.93683 (17) 0.93709 (17) 0.68371 (17) 0.0325 (4)
H12A 0.8883 0.8985 0.6426 0.049*
H12B 1.0288 0.8943 0.6829 0.049*
H12C 0.9598 1.0311 0.6294 0.049*
C13 0.91121 (19) 0.9744 (2) 0.8992 (2) 0.0457 (5)
H13A 0.9415 1.0670 0.8421 0.069*
H13B 0.9990 0.9260 0.9029 0.069*
H13C 0.8435 0.9666 0.9937 0.069*
C14 1.06039 (15) 0.56135 (14) 0.63293 (15) 0.0207 (3)
C15 1.03662 (17) 0.66575 (14) 0.52347 (16) 0.0246 (3)
H15 1.1096 0.7312 0.4502 0.030*
C16 0.88655 (18) 0.65609 (16) 0.54168 (19) 0.0304 (4)
H16 0.8453 0.7033 0.4752 0.036*
C17 0.80661 (17) 0.56158 (16) 0.67958 (19) 0.0305 (4)
C18 0.91244 (16) 0.50176 (15) 0.73735 (16) 0.0247 (3)
C19 0.86545 (19) 0.40421 (17) 0.86990 (17) 0.0354 (4)
H19 0.9352 0.3626 0.9090 0.042*
C20 0.7145 (2) 0.3692 (2) 0.9435 (2) 0.0499 (6)
H20 0.6813 0.3043 1.0344 0.060*
C21 0.6116 (2) 0.4273 (2) 0.8868 (3) 0.0561 (7)
H21 0.5092 0.4011 0.9395 0.067*
C22 0.65523 (18) 0.5224 (2) 0.7551 (2) 0.0463 (5)
H22 0.5842 0.5607 0.7165 0.056*
C23 1.20379 (16) 0.54344 (15) 0.65758 (16) 0.0236 (3)
C24 1.18369 (17) 0.58486 (17) 0.78106 (17) 0.0300 (4)
H24A 1.1568 0.6761 0.7607 0.045*
H24B 1.2767 0.5767 0.7959 0.045*
H24C 1.1048 0.5281 0.8652 0.045*
C25 1.24681 (18) 0.40112 (16) 0.69020 (18) 0.0338 (4)
H25A 1.1628 0.3430 0.7666 0.051*
H25B 1.3318 0.3913 0.7176 0.051*
H25C 1.2734 0.3780 0.6073 0.051*
C26 1.33151 (17) 0.63006 (17) 0.52843 (18) 0.0339 (4)
H26A 1.3410 0.6090 0.4475 0.051*
H26B 1.4241 0.6140 0.5439 0.051*
H26C 1.3110 0.7225 0.5114 0.051*
Ni1 0.5000 1.0000 1.0000 0.02238 (12)
Ni2 1.0000 0.5000 0.5000 0.02285 (12)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0222 (7) 0.0248 (8) 0.0166 (8) −0.0013 (6) −0.0025 (6) −0.0083 (6)
C2 0.0280 (8) 0.0250 (8) 0.0182 (8) −0.0055 (6) −0.0017 (6) −0.0091 (6)
C3 0.0313 (8) 0.0201 (8) 0.0194 (8) 0.0025 (6) −0.0032 (6) −0.0057 (6)
C4 0.0264 (8) 0.0242 (8) 0.0156 (8) 0.0000 (6) −0.0033 (6) −0.0034 (6)
C5 0.0221 (7) 0.0226 (8) 0.0139 (7) −0.0017 (6) −0.0020 (6) −0.0049 (6)
C6 0.0305 (8) 0.0248 (8) 0.0207 (8) −0.0012 (6) −0.0053 (6) −0.0085 (6)
C7 0.0383 (9) 0.0367 (10) 0.0245 (9) −0.0108 (7) −0.0084 (7) −0.0113 (7)
C8 0.0307 (9) 0.0481 (11) 0.0264 (9) −0.0070 (8) −0.0129 (7) −0.0063 (8)
C9 0.0287 (8) 0.0371 (10) 0.0248 (9) 0.0035 (7) −0.0100 (7) −0.0044 (7)
C10 0.0227 (7) 0.0359 (9) 0.0235 (8) 0.0047 (6) −0.0064 (6) −0.0143 (7)
C11 0.0317 (8) 0.0390 (10) 0.0293 (9) 0.0106 (7) −0.0085 (7) −0.0053 (8)
C12 0.0258 (8) 0.0367 (10) 0.0273 (9) 0.0042 (7) −0.0020 (7) −0.0125 (7)
C13 0.0297 (9) 0.0751 (14) 0.0486 (12) 0.0102 (9) −0.0185 (8) −0.0381 (11)
C14 0.0223 (7) 0.0202 (7) 0.0206 (8) 0.0012 (6) −0.0063 (6) −0.0105 (6)
C15 0.0310 (8) 0.0179 (7) 0.0281 (9) 0.0035 (6) −0.0135 (7) −0.0100 (6)
C16 0.0349 (9) 0.0266 (8) 0.0450 (10) 0.0138 (7) −0.0253 (8) −0.0218 (8)
C17 0.0241 (8) 0.0349 (9) 0.0464 (11) 0.0071 (7) −0.0121 (7) −0.0326 (8)
C18 0.0237 (7) 0.0270 (8) 0.0253 (8) −0.0008 (6) −0.0032 (6) −0.0176 (7)
C19 0.0413 (9) 0.0367 (9) 0.0245 (9) −0.0125 (7) −0.0011 (7) −0.0163 (7)
C20 0.0506 (12) 0.0551 (12) 0.0342 (11) −0.0287 (10) 0.0123 (9) −0.0295 (10)
C21 0.0280 (9) 0.0732 (15) 0.0689 (16) −0.0203 (10) 0.0151 (10) −0.0591 (14)
C22 0.0226 (8) 0.0568 (12) 0.0778 (16) 0.0058 (8) −0.0102 (9) −0.0551 (13)
C23 0.0224 (7) 0.0282 (8) 0.0220 (8) 0.0026 (6) −0.0090 (6) −0.0106 (7)
C24 0.0292 (8) 0.0371 (9) 0.0284 (9) 0.0007 (7) −0.0121 (7) −0.0155 (7)
C25 0.0375 (9) 0.0353 (9) 0.0373 (10) 0.0131 (7) −0.0233 (8) −0.0152 (8)
C26 0.0237 (8) 0.0468 (11) 0.0299 (9) −0.0033 (7) −0.0077 (7) −0.0137 (8)
Ni1 0.02328 (19) 0.0207 (2) 0.0179 (2) 0.00272 (14) −0.00330 (15) −0.00650 (15)
Ni2 0.0256 (2) 0.0215 (2) 0.0289 (2) 0.00832 (14) −0.01484 (16) −0.01392 (16)

Geometric parameters (Å, °)

C1—C2 1.424 (2) C15—Ni2 2.0066 (15)
C1—C5 1.474 (2) C15—H15 0.9500
C1—C10 1.528 (2) C16—C17 1.449 (2)
C1—Ni1 2.1237 (14) C16—Ni2 2.0588 (15)
C2—C3 1.416 (2) C16—H16 0.9500
C2—Ni1 1.9942 (15) C17—C22 1.404 (2)
C2—H2 0.9500 C17—C18 1.424 (2)
C3—C4 1.453 (2) C17—Ni2 2.4247 (15)
C3—Ni1 2.0492 (15) C18—C19 1.397 (2)
C3—H3 0.9500 C18—Ni2 2.4543 (15)
C4—C9 1.397 (2) C19—C20 1.391 (3)
C4—C5 1.429 (2) C19—H19 0.9500
C4—Ni1 2.4604 (15) C20—C21 1.387 (3)
C5—C6 1.397 (2) C20—H20 0.9500
C5—Ni1 2.5048 (14) C21—C22 1.382 (3)
C6—C7 1.385 (2) C21—H21 0.9500
C6—H6 0.9500 C22—H22 0.9500
C7—C8 1.394 (3) C23—C25 1.531 (2)
C7—H7 0.9500 C23—C26 1.534 (2)
C8—C9 1.381 (3) C23—C24 1.540 (2)
C8—H8 0.9500 C24—H24A 0.9800
C9—H9 0.9500 C24—H24B 0.9800
C10—C13 1.530 (2) C24—H24C 0.9800
C10—C11 1.539 (2) C25—H25A 0.9800
C10—C12 1.539 (2) C25—H25B 0.9800
C11—H11A 0.9800 C25—H25C 0.9800
C11—H11B 0.9800 C26—H26A 0.9800
C11—H11C 0.9800 C26—H26B 0.9800
C12—H12A 0.9800 C26—H26C 0.9800
C12—H12B 0.9800 Ni1—C2i 1.9942 (15)
C12—H12C 0.9800 Ni1—C3i 2.0492 (15)
C13—H13A 0.9800 Ni1—C1i 2.1237 (14)
C13—H13B 0.9800 Ni1—C4i 2.4604 (15)
C13—H13C 0.9800 Ni1—C5i 2.5048 (14)
C14—C15 1.423 (2) Ni2—C15ii 2.0066 (15)
C14—C18 1.477 (2) Ni2—C16ii 2.0588 (15)
C14—C23 1.520 (2) Ni2—C14ii 2.1166 (14)
C14—Ni2 2.1166 (14) Ni2—C17ii 2.4247 (15)
C15—C16 1.413 (2) Ni2—C18ii 2.4543 (15)
C2—C1—C5 106.58 (13) C14—C23—C24 108.71 (12)
C2—C1—C10 125.06 (14) C25—C23—C24 109.00 (13)
C5—C1—C10 125.43 (13) C26—C23—C24 108.56 (13)
C2—C1—Ni1 64.95 (8) C23—C24—H24A 109.5
C5—C1—Ni1 86.25 (8) C23—C24—H24B 109.5
C10—C1—Ni1 128.67 (11) H24A—C24—H24B 109.5
C3—C2—C1 108.60 (13) C23—C24—H24C 109.5
C3—C2—Ni1 71.60 (9) H24A—C24—H24C 109.5
C1—C2—Ni1 74.74 (9) H24B—C24—H24C 109.5
C3—C2—H2 125.7 C23—C25—H25A 109.5
C1—C2—H2 125.7 C23—C25—H25B 109.5
Ni1—C2—H2 119.7 H25A—C25—H25B 109.5
C2—C3—C4 108.12 (13) C23—C25—H25C 109.5
C2—C3—Ni1 67.43 (9) H25A—C25—H25C 109.5
C4—C3—Ni1 87.54 (9) H25B—C25—H25C 109.5
C2—C3—H3 125.9 C23—C26—H26A 109.5
C4—C3—H3 125.9 C23—C26—H26B 109.5
Ni1—C3—H3 111.3 H26A—C26—H26B 109.5
C9—C4—C5 120.57 (14) C23—C26—H26C 109.5
C9—C4—C3 132.15 (14) H26A—C26—H26C 109.5
C5—C4—C3 107.27 (13) H26B—C26—H26C 109.5
C9—C4—Ni1 134.13 (11) C2—Ni1—C2i 180.0
C5—C4—Ni1 74.99 (8) C2—Ni1—C3 40.96 (6)
C3—C4—Ni1 56.32 (8) C2i—Ni1—C3 139.04 (6)
C6—C5—C4 119.25 (14) C2—Ni1—C3i 139.04 (6)
C6—C5—C1 133.14 (14) C2i—Ni1—C3i 40.96 (6)
C4—C5—C1 107.61 (13) C3—Ni1—C3i 180.00 (8)
C6—C5—Ni1 137.16 (11) C2—Ni1—C1i 139.68 (6)
C4—C5—Ni1 71.58 (8) C2i—Ni1—C1i 40.32 (6)
C1—C5—Ni1 57.78 (7) C3—Ni1—C1i 112.92 (6)
C7—C6—C5 119.14 (15) C3i—Ni1—C1i 67.08 (6)
C7—C6—H6 120.4 C2—Ni1—C1 40.32 (6)
C5—C6—H6 120.4 C2i—Ni1—C1 139.68 (6)
C6—C7—C8 121.33 (16) C3—Ni1—C1 67.08 (6)
C6—C7—H7 119.3 C3i—Ni1—C1 112.92 (6)
C8—C7—H7 119.3 C1i—Ni1—C1 180.000 (2)
C9—C8—C7 120.81 (15) C2—Ni1—C4 61.80 (6)
C9—C8—H8 119.6 C2i—Ni1—C4 118.20 (6)
C7—C8—H8 119.6 C3—Ni1—C4 36.15 (6)
C8—C9—C4 118.85 (15) C3i—Ni1—C4 143.85 (6)
C8—C9—H9 120.6 C1i—Ni1—C4 119.04 (5)
C4—C9—H9 120.6 C1—Ni1—C4 60.96 (5)
C1—C10—C13 110.58 (13) C2—Ni1—C4i 118.20 (6)
C1—C10—C11 112.17 (13) C2i—Ni1—C4i 61.80 (6)
C13—C10—C11 108.40 (15) C3—Ni1—C4i 143.85 (6)
C1—C10—C12 107.69 (13) C3i—Ni1—C4i 36.15 (6)
C13—C10—C12 108.98 (14) C1i—Ni1—C4i 60.96 (5)
C11—C10—C12 108.97 (14) C1—Ni1—C4i 119.04 (5)
C10—C11—H11A 109.5 C4—Ni1—C4i 180.0
C10—C11—H11B 109.5 C2—Ni1—C5i 119.05 (5)
H11A—C11—H11B 109.5 C2i—Ni1—C5i 60.95 (5)
C10—C11—H11C 109.5 C3—Ni1—C5i 119.72 (5)
H11A—C11—H11C 109.5 C3i—Ni1—C5i 60.28 (5)
H11B—C11—H11C 109.5 C1i—Ni1—C5i 35.97 (5)
C10—C12—H12A 109.5 C1—Ni1—C5i 144.03 (5)
C10—C12—H12B 109.5 C4—Ni1—C5i 146.56 (5)
H12A—C12—H12B 109.5 C4i—Ni1—C5i 33.44 (5)
C10—C12—H12C 109.5 C2—Ni1—C5 60.95 (5)
H12A—C12—H12C 109.5 C2i—Ni1—C5 119.05 (5)
H12B—C12—H12C 109.5 C3—Ni1—C5 60.28 (5)
C10—C13—H13A 109.5 C3i—Ni1—C5 119.72 (5)
C10—C13—H13B 109.5 C1i—Ni1—C5 144.03 (5)
H13A—C13—H13B 109.5 C1—Ni1—C5 35.97 (5)
C10—C13—H13C 109.5 C4—Ni1—C5 33.44 (5)
H13A—C13—H13C 109.5 C4i—Ni1—C5 146.56 (5)
H13B—C13—H13C 109.5 C5i—Ni1—C5 180.000 (1)
C15—C14—C18 106.70 (12) C15—Ni2—C15ii 180.00 (9)
C15—C14—C23 125.15 (13) C15—Ni2—C16 40.67 (6)
C18—C14—C23 125.70 (13) C15ii—Ni2—C16 139.33 (6)
C15—C14—Ni2 65.71 (8) C15—Ni2—C16ii 139.33 (6)
C18—C14—Ni2 84.13 (9) C15ii—Ni2—C16ii 40.67 (6)
C23—C14—Ni2 128.84 (10) C16—Ni2—C16ii 180.000 (1)
C16—C15—C14 108.81 (14) C15—Ni2—C14 40.25 (6)
C16—C15—Ni2 71.65 (9) C15ii—Ni2—C14 139.75 (6)
C14—C15—Ni2 74.04 (8) C16—Ni2—C14 67.03 (6)
C16—C15—H15 125.6 C16ii—Ni2—C14 112.97 (6)
C14—C15—H15 125.6 C15—Ni2—C14ii 139.75 (6)
Ni2—C15—H15 120.4 C15ii—Ni2—C14ii 40.25 (6)
C15—C16—C17 107.97 (14) C16—Ni2—C14ii 112.97 (6)
C15—C16—Ni2 67.68 (8) C16ii—Ni2—C14ii 67.03 (6)
C17—C16—Ni2 85.57 (9) C14—Ni2—C14ii 180.000 (1)
C15—C16—H16 126.0 C15—Ni2—C17 62.17 (6)
C17—C16—H16 126.0 C15ii—Ni2—C17 117.83 (6)
Ni2—C16—H16 112.9 C16—Ni2—C17 36.59 (6)
C22—C17—C18 120.18 (18) C16ii—Ni2—C17 143.41 (6)
C22—C17—C16 132.02 (17) C14—Ni2—C17 61.50 (5)
C18—C17—C16 107.78 (13) C14ii—Ni2—C17 118.50 (5)
C22—C17—Ni2 132.89 (11) C15—Ni2—C17ii 117.83 (6)
C18—C17—Ni2 74.18 (8) C15ii—Ni2—C17ii 62.17 (6)
C16—C17—Ni2 57.84 (8) C16—Ni2—C17ii 143.41 (6)
C19—C18—C17 119.91 (15) C16ii—Ni2—C17ii 36.59 (6)
C19—C18—C14 132.77 (15) C14—Ni2—C17ii 118.50 (5)
C17—C18—C14 107.31 (14) C14ii—Ni2—C17ii 61.50 (5)
C19—C18—Ni2 134.13 (11) C17—Ni2—C17ii 180.000 (1)
C17—C18—Ni2 71.90 (9) C15—Ni2—C18 61.93 (6)
C14—C18—Ni2 59.08 (7) C15ii—Ni2—C18 118.07 (6)
C20—C19—C18 118.66 (18) C16—Ni2—C18 61.16 (6)
C20—C19—H19 120.7 C16ii—Ni2—C18 118.84 (6)
C18—C19—H19 120.7 C14—Ni2—C18 36.79 (5)
C21—C20—C19 121.4 (2) C14ii—Ni2—C18 143.21 (5)
C21—C20—H20 119.3 C17—Ni2—C18 33.92 (5)
C19—C20—H20 119.3 C17ii—Ni2—C18 146.08 (6)
C22—C21—C20 121.16 (17) C15—Ni2—C18ii 118.07 (6)
C22—C21—H21 119.4 C15ii—Ni2—C18ii 61.93 (6)
C20—C21—H21 119.4 C16—Ni2—C18ii 118.84 (6)
C21—C22—C17 118.71 (19) C16ii—Ni2—C18ii 61.16 (6)
C21—C22—H22 120.6 C14—Ni2—C18ii 143.21 (5)
C17—C22—H22 120.6 C14ii—Ni2—C18ii 36.79 (5)
C14—C23—C25 112.06 (13) C17—Ni2—C18ii 146.08 (5)
C14—C23—C26 110.38 (13) C17ii—Ni2—C18ii 33.92 (5)
C25—C23—C26 108.07 (13) C18—Ni2—C18ii 180.000 (1)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IM2294).

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 datablock(s) I, global. DOI: 10.1107/S1600536811028510/im2294sup1.cif

e-67-m1184-sup1.cif (24.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811028510/im2294Isup2.hkl

e-67-m1184-Isup2.hkl (157.7KB, hkl)

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


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