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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Mar 26;67(Pt 4):m501. doi: 10.1107/S1600536811010555

[1,2-Bis­(diisopropyl­phosphan­yl)ethane-κ2 P,P′]dichloridonickel(II)–9H-carbazole (1/2)

Farah Cañavera-Buelvas a, Marcos Flores-Alamo a, Juventino J García a,*
PMCID: PMC3100014  PMID: 21754008

Abstract

In the title compound, [NiCl2(C14H32P2)]·2C12H9N, the neutral [Ni(dppe)Cl2] complex [dppe is 1,2-bis­(diisopropyl­phosphan­yl)ethane] consists of a tetracoordinated Ni2+ cation and has a crystallographic twofold axis passing through the metal atom and the mid-point of the CH2—CH2 bond of the dppe ligand. The metal atom shows slight tetra­hedral distortion from an ideal square-planar coordination geometry, as reflected in the dihedral angle between NiCl2 and NiP2 planes of 15.32 (2)°. The 9H-carbazole ring system is essentially planar (r.m.s. deviation = 0.022 Å). In the crystal packing, there are two symmetry-related 9H-carbazole mol­ecules between two adjacent NiII complexes, with an angle between the carbazole mean planes of ca 77°.

Related literature

For the use of nickel complexes of the type [Ni(dppe)Cl2] as starting materials and precursors in metal-mediated and catalytic systems, respectively, see: Vicic & Jones (1997); Arévalo & García (2010). For details of tetra­hedral distortion and motifs, see: Angulo et al. (2003); Dahlenburg & Kurth (2001); Etter et al. (1990).graphic file with name e-67-0m501-scheme1.jpg

Experimental

Crystal data

  • [NiCl2(C14H32P2)]·2C12H9N

  • M r = 726.35

  • Monoclinic, Inline graphic

  • a = 22.5830 (5) Å

  • b = 8.4374 (2) Å

  • c = 18.9630 (5) Å

  • β = 101.544 (2)°

  • V = 3540.15 (15) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.82 mm−1

  • T = 122 K

  • 0.42 × 0.16 × 0.02 mm

Data collection

  • Oxford Diffraction Xcalibur Atlas Gemini diffractometer

  • Absorption correction: analytical [CrysAlis PRO (Oxford Diffraction, 2009); based on expressions derived by Clark & Reid (1995)] T min = 0.851, T max = 0.987

  • 12792 measured reflections

  • 3484 independent reflections

  • 2908 reflections with I > 2σ(I)

  • R int = 0.027

Refinement

  • R[F 2 > 2σ(F 2)] = 0.026

  • wR(F 2) = 0.065

  • S = 1.05

  • 3484 reflections

  • 211 parameters

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

  • Δρmax = 0.62 e Å−3

  • Δρmin = −0.26 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2009); cell refinement: CrysAlis RED (Oxford Diffraction, 2009); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811010555/bh2344sup1.cif

e-67-0m501-sup1.cif (19.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811010555/bh2344Isup2.hkl

e-67-0m501-Isup2.hkl (167.5KB, hkl)

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

Table 1. Selected geometric parameters (Å, °).

Ni1—Cl1 2.2221 (4)
Ni1—P1 2.1581 (5)
P1i—Ni1—P1 88.61 (3)
P1i—Ni1—Cl1i 168.757 (16)
P1i—Ni1—Cl1 89.797 (16)
Cl1i—Ni1—Cl1 93.87 (2)

Symmetry code: (i) Inline graphic.

Acknowledgments

We thank PAPIIT-DGAPA-UNAM (IN-201010) and CONACYT (080606) for their financial support of this work and DGAPA-UNAM for a postdoctoral grant to FCB. We also thank Dr A. Arévalo for technical assistance.

supplementary crystallographic information

Comment

The nickel complexes of the type [Ni(dppe)Cl2] are useful starting materials for the preparation of catalysts and catalytic precursors, for an interesting series of active catalyst in a wide variety of stoichiometric (Vicic & Jones, 1997) and catalytic systems (Arévalo & García, 2010). The synthesis of the current complex [Ni (dppe)Cl2](carbazole)2 (see Scheme) can be envisaged as the preparation of a model compound relevant to hydrodenitrogenation and N—H activation process.

In the asymmetric unit, the tetracoordinated [Ni(dppe)Cl2] complex has a 2-fold axis passing through the metal and the centre of the methylene—methylene bond (Fig. 1). The metal center shows slight tetrahedral distortion from ideal square-planar coordination geometry, with the angle between the normals to the planes defined by the two cis-Cl–Ni–Cl and cis-P–Ni–P fragments [15.32 (2)°] being larger than the limiting value of 0° for square-planar coordination. Additionally, the metal ion is situated 0.1144 (1) Å above the Cl1/P1/Cl1i/P1i plane [symmetry code: (i) -x, y, 1/2 - z]. These deviations from planarity, which can safely be attributed to some steric congestion by intermolecular contacts between the metallic complex and the 9H-carbazole molecules (Fig. 2), are somewhat larger than the distortion from ideal square-planar coordination geometry observed for related [Ni(dcpe)Cl2] (Angulo et al., 2003) and [(1S,2S)-C5H8{P(C6H11)2}2NiCl2] (Dahlenburg & Kurth, 2001) complexes, where the NiCl2/NiP2 dihedral angles are 3.96 and 5.37°, respectively. The Ni–P bond lengths in the title compound are equal, by symmetry. Probably as a consequence of the steric bulk of the 9H-carbazole molecules, the Ni–Cl distance, 2.2221 (4) Å, tends to be slightly longer than those in the analogues nickel complexes.

In the crystal packing, there are two 9H-carbazole molecules between two adjacent nickel complexes, with an angle between the carbazole mean planes of ca. 77°. There are two types of intermolecular contacts: one of the van der Waals type N—H···Cl [2.65 (2) Å] is formed from N1 donor atom of the 9H-carbazole to Cl1 chloride atom acceptor of the metallic complex; and other of the type C—H···N [2.645 (1) Å] involving C19 in the dppe ligand and N1 in 9H-carbazole. These van der Waals interactions lead to infinite ribbons based on R12(5) motifs (Etter et al., 1990), as illustrated in Fig. 2.

Experimental

A THF solution of [Ni(dppe)H]2 (Vicic & Jones, 1997) (0.100 g, 0.15 mmol) was added with 9H-carbazole (0. 261 g, 1.56 mmol) and heated to 80 °C for 10 h. After this time, the solution changed from wine red color to brown. The solvent was eliminated under reduced pressure and the resulting solid dissolved in dichloromethane (DCM). Slow evaporation at room temperature of DCM afforded crystals suitable for X-ray diffraction. NMR: 31P{1H} (acetone-d6,121.32 MHz, 25 °C): d 57.2. NMR 1H (acetone-d6, 300 MHz, 25 °C): d 8.13 (d, JH—H=7.8, 1H), d 7.54 (d, JH—H=7.8, 1H), d 7.39 (dd, JH—H=7.8, JH—H=7.2, 1H), d 7.18 (dd, JH—H=7.2, JH—H=7.8, 1H), d 2.5 (m, CH, 2H), d 1.7 (m, CH2, 2H), d 1.35 (m, CH3, 12H). Elemental analysis (calc.): C 62.9 (62.83), H 6.90 (6.93), N 3.82% (3.85%).

Refinement

H atom bonded to N atom was located in a difference and was refined with free coordinates and Uiso(H) = 1.2Ueq(N). H atoms attached to C atoms were placed in geometrically idealized positions, and refined as riding on their parent atoms, with C—H distances fixed to 0.95 (aromatic CH), 0.98 (methyl CH3), 0.99 (methylene CH2) and 1.00 Å (methine CH), and with Uiso = 1.2–1.5 Ueq(C).

Figures

Fig. 1.

Fig. 1.

The molecular structure for the title compound. Displacement ellipsoids are draw at the 50% probability level and H atoms are shown as circles of arbitrary size. Symmetry code for i labeled atoms: -x, y, -z + 1/2.

Fig. 2.

Fig. 2.

Intermolecular van der Waals contacts (dashed lines) in the crystal structure, forming infinite ribbons including R12(5) motifs.

Crystal data

[NiCl2(C14H32P2)]·2C12H9N F(000) = 1536
Mr = 726.35 Dx = 1.363 Mg m3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2yc Cell parameters from 7654 reflections
a = 22.5830 (5) Å θ = 3.3–26.0°
b = 8.4374 (2) Å µ = 0.82 mm1
c = 18.9630 (5) Å T = 122 K
β = 101.544 (2)° Prism, orange
V = 3540.15 (15) Å3 0.42 × 0.16 × 0.02 mm
Z = 4

Data collection

Oxford Diffraction Xcalibur Atlas Gemini diffractometer 3484 independent reflections
Radiation source: fine-focus sealed tube 2908 reflections with I > 2σ(I)
graphite Rint = 0.027
Detector resolution: 10.4685 pixels mm-1 θmax = 26.1°, θmin = 3.5°
ω scans h = −27→27
Absorption correction: analytical [CrysAlis PRO (Oxford Diffraction, 2009); based on expressions derived by Clark & Reid (1995)] k = −10→10
Tmin = 0.851, Tmax = 0.987 l = −18→23
12792 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)] = 0.026 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.065 H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0343P)2 + 0.7966P] where P = (Fo2 + 2Fc2)/3
3484 reflections (Δ/σ)max = 0.001
211 parameters Δρmax = 0.62 e Å3
0 restraints Δρmin = −0.25 e Å3
0 constraints

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
C1 0.13521 (7) 0.51654 (19) 0.17978 (9) 0.0162 (4)
C2 0.10421 (8) 0.4878 (2) 0.10949 (9) 0.0208 (4)
H2 0.0704 0.4185 0.0998 0.025*
C3 0.12477 (8) 0.5644 (2) 0.05455 (10) 0.0237 (4)
H3 0.1046 0.5469 0.0062 0.028*
C4 0.17440 (8) 0.6668 (2) 0.06818 (10) 0.0231 (4)
H4 0.1873 0.7177 0.0291 0.028*
C5 0.20488 (8) 0.6947 (2) 0.13744 (10) 0.0207 (4)
H5 0.2385 0.7648 0.1464 0.025*
C6 0.18570 (7) 0.61860 (19) 0.19446 (9) 0.0163 (4)
C7 0.20640 (7) 0.61872 (19) 0.27183 (9) 0.0164 (4)
C8 0.25374 (8) 0.6941 (2) 0.31818 (10) 0.0218 (4)
H8 0.2812 0.7597 0.2996 0.026*
C9 0.26007 (8) 0.6719 (2) 0.39150 (10) 0.0251 (4)
H9 0.2922 0.7226 0.4235 0.03*
C10 0.21966 (8) 0.5759 (2) 0.41916 (10) 0.0236 (4)
H10 0.2246 0.5635 0.4698 0.028*
C11 0.17264 (8) 0.4985 (2) 0.37428 (9) 0.0195 (4)
H11 0.1453 0.4334 0.3933 0.023*
C12 0.16687 (7) 0.51933 (19) 0.30049 (9) 0.0164 (4)
C13 0.12297 (7) 0.9420 (2) 0.35115 (9) 0.0193 (4)
H13 0.1382 0.8312 0.361 0.023*
C14 0.14981 (8) 1.0047 (2) 0.28869 (10) 0.0247 (4)
H14A 0.136 1.1137 0.2776 0.037*
H14B 0.1366 0.9377 0.2463 0.037*
H14C 0.194 1.0031 0.3022 0.037*
C15 0.14581 (8) 1.0381 (2) 0.41930 (10) 0.0247 (4)
H15A 0.19 1.0448 0.428 0.037*
H15B 0.1335 0.9862 0.4603 0.037*
H15C 0.1286 1.145 0.4134 0.037*
C16 0.01068 (8) 0.9163 (2) 0.40785 (9) 0.0213 (4)
H16 0.0272 1.0094 0.4381 0.026*
C17 0.03308 (9) 0.7674 (2) 0.45155 (11) 0.0316 (5)
H17A 0.0223 0.7741 0.499 0.047*
H17B 0.0771 0.7595 0.4573 0.047*
H17C 0.0141 0.6734 0.4262 0.047*
C18 −0.05797 (8) 0.9302 (2) 0.39410 (10) 0.0268 (4)
H18A −0.0761 0.8401 0.3649 0.04*
H18B −0.0705 1.0292 0.3684 0.04*
H18C −0.0714 0.9301 0.4401 0.04*
C19 0.02934 (8) 0.7388 (2) 0.27707 (10) 0.0251 (4)
H19A 0.0633 0.7196 0.2523 0.03*
H19B 0.029 0.6525 0.3124 0.03*
Cl1 −0.025597 (18) 1.29303 (5) 0.16367 (2) 0.01865 (11)
N1 0.12485 (7) 0.45582 (17) 0.24411 (8) 0.0174 (3)
Ni1 0 1.11320 (3) 0.25 0.01164 (9)
P1 0.039792 (19) 0.93016 (5) 0.32401 (2) 0.01575 (11)
H1N 0.0953 (9) 0.405 (2) 0.2501 (10) 0.019*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0171 (8) 0.0132 (8) 0.0203 (9) 0.0045 (7) 0.0080 (7) 0.0006 (7)
C2 0.0194 (9) 0.0193 (9) 0.0239 (10) −0.0008 (7) 0.0046 (8) −0.0053 (7)
C3 0.0245 (10) 0.0283 (10) 0.0183 (10) 0.0045 (8) 0.0045 (8) −0.0027 (8)
C4 0.0257 (10) 0.0252 (9) 0.0214 (10) 0.0059 (8) 0.0114 (8) 0.0056 (8)
C5 0.0188 (9) 0.0181 (9) 0.0272 (10) 0.0014 (7) 0.0091 (8) 0.0037 (8)
C6 0.0143 (8) 0.0140 (8) 0.0214 (9) 0.0033 (7) 0.0060 (7) 0.0007 (7)
C7 0.0149 (8) 0.0147 (8) 0.0205 (9) 0.0027 (7) 0.0054 (7) 0.0006 (7)
C8 0.0184 (9) 0.0204 (9) 0.0274 (10) −0.0012 (8) 0.0061 (8) 0.0000 (8)
C9 0.0198 (9) 0.0280 (10) 0.0248 (10) 0.0000 (8) −0.0016 (8) −0.0049 (8)
C10 0.0268 (10) 0.0265 (10) 0.0169 (9) 0.0076 (8) 0.0029 (8) 0.0026 (7)
C11 0.0221 (9) 0.0161 (9) 0.0222 (10) 0.0029 (7) 0.0089 (8) 0.0036 (7)
C12 0.0172 (8) 0.0127 (8) 0.0198 (9) 0.0039 (7) 0.0047 (7) −0.0006 (7)
C13 0.0157 (8) 0.0182 (9) 0.0218 (9) 0.0040 (7) −0.0020 (7) 0.0012 (7)
C14 0.0183 (9) 0.0281 (10) 0.0274 (10) 0.0031 (8) 0.0037 (8) 0.0027 (8)
C15 0.0173 (9) 0.0268 (10) 0.0270 (10) −0.0005 (8) −0.0027 (8) −0.0019 (8)
C16 0.0212 (9) 0.0252 (10) 0.0165 (9) −0.0046 (8) 0.0013 (7) 0.0039 (7)
C17 0.0337 (11) 0.0314 (11) 0.0278 (11) −0.0026 (9) 0.0016 (9) 0.0124 (9)
C18 0.0220 (9) 0.0363 (11) 0.0219 (10) −0.0054 (8) 0.0042 (8) 0.0041 (8)
C19 0.0311 (10) 0.0137 (8) 0.0276 (10) 0.0010 (8) −0.0014 (8) −0.0001 (8)
Cl1 0.0204 (2) 0.0144 (2) 0.0208 (2) 0.00193 (16) 0.00338 (17) 0.00393 (16)
N1 0.0162 (7) 0.0158 (7) 0.0218 (8) −0.0033 (6) 0.0074 (6) −0.0011 (6)
Ni1 0.01075 (15) 0.00869 (15) 0.01507 (16) 0 0.00161 (11) 0
P1 0.0167 (2) 0.0120 (2) 0.0169 (2) −0.00081 (17) −0.00073 (17) 0.00090 (17)

Geometric parameters (Å, °)

C1—N1 1.386 (2) C13—H13 1
C1—C2 1.397 (2) C14—H14A 0.98
C1—C6 1.411 (2) C14—H14B 0.98
C2—C3 1.383 (3) C14—H14C 0.98
C2—H2 0.95 C15—H15A 0.98
C3—C4 1.398 (3) C15—H15B 0.98
C3—H3 0.95 C15—H15C 0.98
C4—C5 1.376 (2) C16—C18 1.524 (2)
C4—H4 0.95 C16—C17 1.534 (2)
C5—C6 1.399 (2) C16—P1 1.8418 (18)
C5—H5 0.95 C16—H16 1
C6—C7 1.448 (2) C17—H17A 0.98
C7—C8 1.394 (2) C17—H17B 0.98
C7—C12 1.411 (2) C17—H17C 0.98
C8—C9 1.382 (3) C18—H18A 0.98
C8—H8 0.95 C18—H18B 0.98
C9—C10 1.399 (3) C18—H18C 0.98
C9—H9 0.95 C19—C19i 1.505 (3)
C10—C11 1.384 (2) C19—P1 1.8362 (18)
C10—H10 0.95 C19—H19A 0.99
C11—C12 1.390 (2) C19—H19B 0.99
C11—H11 0.95 Ni1—Cl1 2.2221 (4)
C12—N1 1.387 (2) N1—H1N 0.821 (19)
C13—C15 1.525 (2) Ni1—P1i 2.1581 (5)
C13—C14 1.529 (3) Ni1—P1 2.1581 (5)
C13—P1 1.8482 (17) Ni1—Cl1i 2.2221 (4)
N1—C1—C2 129.44 (16) H14B—C14—H14C 109.5
N1—C1—C6 108.91 (15) C13—C15—H15A 109.5
C2—C1—C6 121.65 (16) C13—C15—H15B 109.5
C3—C2—C1 117.26 (16) H15A—C15—H15B 109.5
C3—C2—H2 121.4 C13—C15—H15C 109.5
C1—C2—H2 121.4 H15A—C15—H15C 109.5
C2—C3—C4 121.82 (17) H15B—C15—H15C 109.5
C2—C3—H3 119.1 C18—C16—C17 111.69 (15)
C4—C3—H3 119.1 C18—C16—P1 111.96 (12)
C5—C4—C3 120.79 (17) C17—C16—P1 112.49 (13)
C5—C4—H4 119.6 C18—C16—H16 106.8
C3—C4—H4 119.6 C17—C16—H16 106.8
C4—C5—C6 119.09 (17) P1—C16—H16 106.8
C4—C5—H5 120.5 C16—C17—H17A 109.5
C6—C5—H5 120.5 C16—C17—H17B 109.5
C5—C6—C1 119.38 (16) H17A—C17—H17B 109.5
C5—C6—C7 134.09 (16) C16—C17—H17C 109.5
C1—C6—C7 106.53 (14) H17A—C17—H17C 109.5
C8—C7—C12 119.53 (16) H17B—C17—H17C 109.5
C8—C7—C6 133.67 (16) C16—C18—H18A 109.5
C12—C7—C6 106.80 (14) C16—C18—H18B 109.5
C9—C8—C7 118.98 (16) H18A—C18—H18B 109.5
C9—C8—H8 120.5 C16—C18—H18C 109.5
C7—C8—H8 120.5 H18A—C18—H18C 109.5
C8—C9—C10 120.79 (17) H18B—C18—H18C 109.5
C8—C9—H9 119.6 C19i—C19—P1 109.93 (8)
C10—C9—H9 119.6 C19i—C19—H19A 109.7
C11—C10—C9 121.37 (17) P1—C19—H19A 109.7
C11—C10—H10 119.3 C19i—C19—H19B 109.7
C9—C10—H10 119.3 P1—C19—H19B 109.7
C10—C11—C12 117.70 (16) H19A—C19—H19B 108.2
C10—C11—H11 121.1 C1—N1—C12 109.01 (14)
C12—C11—H11 121.1 C1—N1—H1N 126.9 (13)
N1—C12—C11 129.69 (15) C12—N1—H1N 123.1 (13)
N1—C12—C7 108.71 (14) P1i—Ni1—P1 88.61 (3)
C11—C12—C7 121.60 (16) P1i—Ni1—Cl1i 168.757 (16)
C15—C13—C14 110.67 (15) P1—Ni1—Cl1i 89.797 (16)
C15—C13—P1 114.66 (12) P1i—Ni1—Cl1 89.797 (16)
C14—C13—P1 109.96 (12) P1—Ni1—Cl1 168.758 (16)
C15—C13—H13 107.1 Cl1i—Ni1—Cl1 93.87 (2)
C14—C13—H13 107.1 C19—P1—C16 109.21 (9)
P1—C13—H13 107.1 C19—P1—C13 101.97 (8)
C13—C14—H14A 109.5 C16—P1—C13 106.35 (8)
C13—C14—H14B 109.5 C19—P1—Ni1 108.52 (6)
H14A—C14—H14B 109.5 C16—P1—Ni1 115.65 (6)
C13—C14—H14C 109.5 C13—P1—Ni1 114.22 (6)
H14A—C14—H14C 109.5
N1—C1—C2—C3 −179.52 (17) C6—C1—N1—C12 1.32 (18)
C6—C1—C2—C3 −0.4 (3) C11—C12—N1—C1 177.09 (17)
C1—C2—C3—C4 −0.1 (3) C7—C12—N1—C1 −2.04 (18)
C2—C3—C4—C5 0.2 (3) C19i—C19—P1—C16 93.81 (18)
C3—C4—C5—C6 0.3 (3) C19i—C19—P1—C13 −153.95 (17)
C4—C5—C6—C1 −0.7 (2) C19i—C19—P1—Ni1 −33.06 (19)
C4—C5—C6—C7 179.56 (17) C18—C16—P1—C19 −79.07 (14)
N1—C1—C6—C5 −179.89 (15) C17—C16—P1—C19 47.67 (15)
C2—C1—C6—C5 0.8 (2) C18—C16—P1—C13 171.60 (13)
N1—C1—C6—C7 −0.11 (18) C17—C16—P1—C13 −61.66 (14)
C2—C1—C6—C7 −179.40 (15) C18—C16—P1—Ni1 43.64 (14)
C5—C6—C7—C8 −0.7 (3) C17—C16—P1—Ni1 170.38 (11)
C1—C6—C7—C8 179.53 (18) C15—C13—P1—C19 −151.39 (13)
C5—C6—C7—C12 178.62 (18) C14—C13—P1—C19 83.17 (14)
C1—C6—C7—C12 −1.10 (18) C15—C13—P1—C16 −37.02 (15)
C12—C7—C8—C9 −1.3 (2) C14—C13—P1—C16 −162.46 (12)
C6—C7—C8—C9 178.01 (17) C15—C13—P1—Ni1 91.77 (13)
C7—C8—C9—C10 −0.2 (3) C14—C13—P1—Ni1 −33.67 (14)
C8—C9—C10—C11 0.8 (3) P1i—Ni1—P1—C19 10.07 (6)
C9—C10—C11—C12 0.0 (3) Cl1i—Ni1—P1—C19 178.94 (7)
C10—C11—C12—N1 179.44 (16) Cl1—Ni1—P1—C19 −71.87 (12)
C10—C11—C12—C7 −1.5 (2) P1i—Ni1—P1—C16 −113.00 (7)
C8—C7—C12—N1 −178.60 (15) Cl1i—Ni1—P1—C16 55.87 (6)
C6—C7—C12—N1 1.93 (18) Cl1—Ni1—P1—C16 165.06 (10)
C8—C7—C12—C11 2.2 (2) P1i—Ni1—P1—C13 123.06 (7)
C6—C7—C12—C11 −177.29 (15) Cl1i—Ni1—P1—C13 −68.07 (6)
C2—C1—N1—C12 −179.46 (16) Cl1—Ni1—P1—C13 41.12 (12)

Symmetry codes: (i) −x, y, −z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BH2344).

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/S1600536811010555/bh2344sup1.cif

e-67-0m501-sup1.cif (19.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811010555/bh2344Isup2.hkl

e-67-0m501-Isup2.hkl (167.5KB, hkl)

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


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