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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Sep 14;67(Pt 10):m1389. doi: 10.1107/S1600536811036555

catena-Poly[[(triphenyl­phosphane)copper(I)]-di-μ-iodido-[(triphenyl­phosphane)copper(I)]-μ-{1,2-bis­[1-(pyridin-4-yl)ethyl­idene]hydrazine}]

Hoong-Kun Fun a,*,, Wan-Sin Loh a,§, Goutam K Patra b, Anindita Mukherjee b, Pankaj K Pal b
PMCID: PMC3201507  PMID: 22058699

Abstract

In the title coordination polymer, [Cu2I2(C14H14N4)(C18H15P)2]n, the CuI atom is coordinated by two I atoms, one P atom and one N atom in a fairly regular tetra­hedral arrangement. A crystallographic inversion centre generates a Cu2I2 diamond with a Cu–Cu separation of 3.0120 (5) Å. The complete N,N′-(1-pyridin-4-yl-ethethyl­idene)-hydrazine mol­ecule is also generated by inversion symmetry, and this bridging ligand leads to [011] polymeric chains in the crystal structure.

Related literature

For background to copper(I) iodide and triphenyl­phosphine networks, see: Siedel & Stang (2002); Fujita et al. (2005); Banerjee et al. (2008); Zhou et al. (2006); Yam & Lo (1999). For the stability of the temperature controller used in the data collection, see: Cosier & Glazer (1986).graphic file with name e-67-m1389-scheme1.jpg

Experimental

Crystal data

  • [Cu2I2(C14H14N4)(C18H15P)2]

  • M r = 1143.72

  • Triclinic, Inline graphic

  • a = 9.2788 (4) Å

  • b = 11.4322 (5) Å

  • c = 12.4204 (5) Å

  • α = 74.566 (2)°

  • β = 76.690 (2)°

  • γ = 72.067 (2)°

  • V = 1192.41 (9) Å3

  • Z = 1

  • Mo Kα radiation

  • μ = 2.29 mm−1

  • T = 100 K

  • 0.36 × 0.23 × 0.15 mm

Data collection

  • Bruker SMART APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2009) T min = 0.494, T max = 0.724

  • 33229 measured reflections

  • 8881 independent reflections

  • 7865 reflections with I > 2σ(I)

  • R int = 0.041

Refinement

  • R[F 2 > 2σ(F 2)] = 0.032

  • wR(F 2) = 0.086

  • S = 1.05

  • 8881 reflections

  • 272 parameters

  • H-atom parameters constrained

  • Δρmax = 2.34 e Å−3

  • Δρmin = −1.81 e Å−3

Data collection: APEX2 (Bruker, 2009); cell refinement: SAINT (Bruker, 2009); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811036555/hb6379sup1.cif

e-67-m1389-sup1.cif (23.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811036555/hb6379Isup2.hkl

e-67-m1389-Isup2.hkl (434.4KB, hkl)

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

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

Cu1—I1i 2.6417 (3)
Cu1—I1 2.6781 (3)
Cu1—N1 2.0586 (15)
Cu1—P1 2.2278 (5)
Cu1i—I1—Cu1 68.967 (9)

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors thank Universiti Sains Malaysia (USM) for the Research University Grant (1001/PFIZIK/811160). WSL also thanks the Malaysian Government and USM for the award of a research fellowship.

supplementary crystallographic information

Comment

Copper(I) iodides are interesting building blocks for the formation of extended solid-state coordination architectures (Siedel et al., 2002; Fujita et al., 2005; Banerjee et al., 2008). Copper(I) complexes with PPh3 as a co-ligand are of rising importance owing to their diverse structures and photophysical and chemical properties (Zhou et al., 2006; Yam & Lo, 1999).

The asymmetric unit of the title polymeric compound (Fig. 1) contains one CuI cation, one iodine anion, one triphenylphosphane unit and one N,N'-(1-pyridin-4-yl-ethethylidene)-hydrazine unit. The other half being generated by an inversion center (symmetry code: -x + 2, -y, -z). Each CuI cation is tetracoordinated by one nitrogen, one phosphorus and two iodine atoms. The Cu–I distances are 2.6417 (3) and 2.6781 (3) Å. In the crystal (Fig. 2 & Fig. 3), the nitrogen atoms are bridged together, leading to the formation of polymeric chains along the [011].

Experimental

The N,N'-bis-(1-pyridin-4-yl-ethethylidene)-hydrazine component was prepared in good yield as a yellow solid by condensing hydrazine hydrate with 4-acetylpyridine in anhydrous methanol in 1:2 molar ratio. The Cu(I) complex was prepared in the following way: to a solution of PPh3 (0.262 g, 1 mmol) in CH3CN (50 ml), CuI (0.19 g, 1 mmol) was added. The reaction mixture was stirred for about 1 h to obtain a white turbid solution. Then N,N'-bis-(1-pyridin-4-yl-ethethylidene)-hydrazine (0.238 g, 1 mmol) in 20 ml CHCl3 was added with constant stirring at room temperature to give a clear yellowish solution. Orange–red block-shaped crystals were obtained by slow evaporation of the solution after 2 days. Yield: 0.45 g (70%).

Refinement

All H atoms were positioned geometrically and refined using a riding model with Uiso(H) = 1.2 Ueq(C) [C–H = 0.95–0.98 Å].

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, showing 50% probability displacement ellipsoids.

Fig. 2.

Fig. 2.

The polymeric chain of the title compound with 50% probability ellipsoids for non H atoms, showing the coordination environment for the N atoms.

Fig. 3.

Fig. 3.

The crystal packing of the title compound, viewed along the a axis.

Crystal data

[Cu2I2(C14H14N4)(C18H15P)2] Z = 1
Mr = 1143.72 F(000) = 566
Triclinic, P1 Dx = 1.593 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 9.2788 (4) Å Cell parameters from 9948 reflections
b = 11.4322 (5) Å θ = 2.3–34.9°
c = 12.4204 (5) Å µ = 2.29 mm1
α = 74.566 (2)° T = 100 K
β = 76.690 (2)° Block, orange
γ = 72.067 (2)° 0.36 × 0.23 × 0.15 mm
V = 1192.41 (9) Å3

Data collection

Bruker SMART APEXII CCD diffractometer 8881 independent reflections
Radiation source: fine-focus sealed tube 7865 reflections with I > 2σ(I)
graphite Rint = 0.041
φ and ω scans θmax = 33.0°, θmin = 1.7°
Absorption correction: multi-scan (SADABS; Bruker, 2009) h = −14→14
Tmin = 0.494, Tmax = 0.724 k = −17→16
33229 measured reflections l = −18→19

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)] = 0.032 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.086 H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0516P)2 + 0.4005P] where P = (Fo2 + 2Fc2)/3
8881 reflections (Δ/σ)max = 0.002
272 parameters Δρmax = 2.34 e Å3
0 restraints Δρmin = −1.81 e Å3

Special details

Experimental. The crystal was placed in the cold stream of an Oxford Cryosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1) K.
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
I1 0.855859 (12) −0.132037 (10) 0.055940 (9) 0.01592 (4)
Cu1 0.86308 (2) 0.10732 (2) 0.023918 (18) 0.01484 (5)
P1 0.75620 (5) 0.16954 (4) 0.18626 (4) 0.01378 (8)
N1 0.74367 (17) 0.19616 (15) −0.10892 (13) 0.0163 (3)
N2 0.53664 (18) 0.47410 (16) −0.45218 (13) 0.0191 (3)
C1 0.7889 (2) 0.28666 (19) −0.19227 (16) 0.0201 (3)
H1A 0.8756 0.3112 −0.1869 0.024*
C2 0.7158 (2) 0.34564 (19) −0.28518 (16) 0.0203 (3)
H2A 0.7511 0.4099 −0.3412 0.024*
C3 0.5898 (2) 0.31012 (17) −0.29597 (15) 0.0160 (3)
C4 0.5405 (2) 0.21851 (19) −0.20863 (16) 0.0201 (3)
H4A 0.4539 0.1924 −0.2115 0.024*
C5 0.6193 (2) 0.16582 (19) −0.11742 (16) 0.0196 (3)
H5A 0.5828 0.1049 −0.0578 0.024*
C6 0.5135 (2) 0.36689 (18) −0.39770 (15) 0.0171 (3)
C7 0.4228 (3) 0.2953 (2) −0.42808 (18) 0.0248 (4)
H7A 0.3972 0.3349 −0.5040 0.037*
H7B 0.3280 0.2960 −0.3732 0.037*
H7C 0.4839 0.2082 −0.4269 0.037*
C8 0.79470 (19) 0.30849 (17) 0.20650 (15) 0.0153 (3)
C9 0.8041 (2) 0.32434 (19) 0.31231 (16) 0.0187 (3)
H9A 0.7892 0.2611 0.3780 0.022*
C10 0.8351 (2) 0.4324 (2) 0.32155 (18) 0.0227 (4)
H10A 0.8428 0.4422 0.3935 0.027*
C11 0.8550 (2) 0.52586 (19) 0.22673 (19) 0.0236 (4)
H11A 0.8755 0.5997 0.2338 0.028*
C12 0.8450 (3) 0.5120 (2) 0.12104 (18) 0.0247 (4)
H12A 0.8580 0.5762 0.0559 0.030*
C13 0.8158 (2) 0.40299 (19) 0.11159 (17) 0.0223 (4)
H13A 0.8102 0.3929 0.0393 0.027*
C14 0.8022 (2) 0.05253 (17) 0.31409 (15) 0.0152 (3)
C15 0.6953 (2) 0.0328 (2) 0.41092 (18) 0.0290 (5)
H15A 0.5914 0.0808 0.4125 0.035*
C16 0.7404 (3) −0.0575 (3) 0.5063 (2) 0.0391 (6)
H16A 0.6667 −0.0713 0.5721 0.047*
C17 0.8924 (3) −0.1270 (2) 0.5051 (2) 0.0321 (5)
H17A 0.9229 −0.1884 0.5699 0.038*
C18 0.9990 (3) −0.1063 (2) 0.4092 (2) 0.0332 (5)
H18A 1.1036 −0.1523 0.4087 0.040*
C19 0.9544 (2) −0.0186 (2) 0.31328 (17) 0.0250 (4)
H19A 1.0279 −0.0070 0.2468 0.030*
C20 0.5469 (2) 0.21052 (18) 0.20193 (16) 0.0173 (3)
C21 0.4819 (2) 0.1214 (2) 0.18810 (17) 0.0201 (3)
H21A 0.5455 0.0406 0.1792 0.024*
C22 0.3255 (2) 0.1495 (2) 0.18721 (17) 0.0220 (4)
H22A 0.2825 0.0876 0.1788 0.026*
C23 0.2321 (2) 0.2676 (2) 0.1986 (2) 0.0267 (4)
H23A 0.1256 0.2879 0.1957 0.032*
C24 0.2950 (3) 0.3556 (2) 0.2141 (3) 0.0363 (6)
H24A 0.2308 0.4362 0.2232 0.044*
C25 0.4523 (2) 0.3274 (2) 0.2166 (2) 0.0296 (5)
H25A 0.4942 0.3882 0.2284 0.036*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
I1 0.01722 (6) 0.01009 (6) 0.01945 (6) −0.00324 (4) −0.00483 (4) −0.00023 (4)
Cu1 0.01887 (10) 0.01192 (11) 0.01240 (10) −0.00298 (8) −0.00424 (7) −0.00015 (7)
P1 0.01561 (18) 0.0109 (2) 0.01386 (19) −0.00234 (14) −0.00335 (14) −0.00154 (15)
N1 0.0198 (6) 0.0119 (7) 0.0153 (7) −0.0020 (5) −0.0060 (5) 0.0005 (5)
N2 0.0205 (7) 0.0176 (8) 0.0159 (7) −0.0021 (6) −0.0077 (5) 0.0028 (6)
C1 0.0239 (8) 0.0159 (9) 0.0201 (8) −0.0071 (7) −0.0094 (7) 0.0042 (6)
C2 0.0240 (8) 0.0167 (9) 0.0193 (8) −0.0065 (7) −0.0098 (7) 0.0046 (6)
C3 0.0175 (7) 0.0127 (8) 0.0154 (7) −0.0002 (6) −0.0054 (6) −0.0008 (6)
C4 0.0209 (8) 0.0187 (9) 0.0196 (8) −0.0063 (6) −0.0074 (6) 0.0025 (6)
C5 0.0218 (8) 0.0185 (9) 0.0161 (8) −0.0064 (6) −0.0062 (6) 0.0046 (6)
C6 0.0185 (7) 0.0150 (8) 0.0150 (7) 0.0000 (6) −0.0052 (6) −0.0014 (6)
C7 0.0348 (10) 0.0171 (9) 0.0245 (9) −0.0056 (8) −0.0146 (8) −0.0007 (7)
C8 0.0148 (7) 0.0115 (8) 0.0182 (8) −0.0022 (5) −0.0028 (6) −0.0021 (6)
C9 0.0206 (8) 0.0159 (8) 0.0197 (8) −0.0047 (6) −0.0033 (6) −0.0039 (6)
C10 0.0264 (9) 0.0198 (9) 0.0238 (9) −0.0062 (7) −0.0032 (7) −0.0085 (7)
C11 0.0234 (8) 0.0136 (9) 0.0329 (11) −0.0046 (7) 0.0000 (7) −0.0074 (7)
C12 0.0319 (10) 0.0144 (9) 0.0253 (10) −0.0067 (7) −0.0020 (8) −0.0013 (7)
C13 0.0293 (9) 0.0154 (9) 0.0201 (9) −0.0050 (7) −0.0054 (7) −0.0002 (7)
C14 0.0186 (7) 0.0125 (8) 0.0141 (7) −0.0040 (6) −0.0038 (6) −0.0011 (6)
C15 0.0210 (8) 0.0424 (14) 0.0192 (9) −0.0099 (8) −0.0056 (7) 0.0044 (8)
C16 0.0348 (11) 0.0576 (18) 0.0215 (10) −0.0234 (12) −0.0088 (9) 0.0141 (10)
C17 0.0445 (12) 0.0253 (11) 0.0257 (10) −0.0109 (9) −0.0178 (9) 0.0083 (8)
C18 0.0364 (11) 0.0292 (12) 0.0237 (10) 0.0098 (9) −0.0124 (9) −0.0035 (8)
C19 0.0234 (8) 0.0260 (11) 0.0171 (8) 0.0041 (7) −0.0038 (7) −0.0022 (7)
C20 0.0173 (7) 0.0158 (8) 0.0176 (8) −0.0017 (6) −0.0047 (6) −0.0033 (6)
C21 0.0189 (7) 0.0213 (9) 0.0210 (9) −0.0047 (6) −0.0026 (6) −0.0072 (7)
C22 0.0192 (8) 0.0273 (10) 0.0228 (9) −0.0084 (7) −0.0035 (7) −0.0080 (7)
C23 0.0179 (8) 0.0292 (11) 0.0329 (11) −0.0035 (7) −0.0089 (7) −0.0057 (8)
C24 0.0201 (9) 0.0222 (11) 0.0659 (18) 0.0019 (8) −0.0124 (10) −0.0121 (11)
C25 0.0197 (8) 0.0194 (10) 0.0517 (14) −0.0007 (7) −0.0104 (9) −0.0120 (9)

Geometric parameters (Å, °)

Cu1—I1i 2.6417 (3) C10—C11 1.383 (3)
Cu1—I1 2.6781 (3) C10—H10A 0.9500
Cu1—N1 2.0586 (15) C11—C12 1.390 (3)
Cu1—P1 2.2278 (5) C11—H11A 0.9500
Cu1—I1i 2.6417 (3) C12—C13 1.393 (3)
Cu1—Cu1i 3.0120 (5) C12—H12A 0.9500
P1—C8 1.8214 (19) C13—H13A 0.9500
P1—C14 1.8228 (18) C14—C15 1.387 (3)
P1—C20 1.8288 (18) C14—C19 1.396 (3)
N1—C5 1.336 (2) C15—C16 1.398 (3)
N1—C1 1.348 (2) C15—H15A 0.9500
N2—C6 1.288 (2) C16—C17 1.389 (4)
N2—N2ii 1.405 (3) C16—H16A 0.9500
C1—C2 1.383 (2) C17—C18 1.380 (4)
C1—H1A 0.9500 C17—H17A 0.9500
C2—C3 1.394 (3) C18—C19 1.390 (3)
C2—H2A 0.9500 C18—H18A 0.9500
C3—C4 1.395 (3) C19—H19A 0.9500
C3—C6 1.487 (2) C20—C25 1.386 (3)
C4—C5 1.388 (2) C20—C21 1.396 (3)
C4—H4A 0.9500 C21—C22 1.389 (3)
C5—H5A 0.9500 C21—H21A 0.9500
C6—C7 1.503 (3) C22—C23 1.385 (3)
C7—H7A 0.9800 C22—H22A 0.9500
C7—H7B 0.9800 C23—C24 1.381 (3)
C7—H7C 0.9800 C23—H23A 0.9500
C8—C13 1.393 (3) C24—C25 1.401 (3)
C8—C9 1.399 (3) C24—H24A 0.9500
C9—C10 1.390 (3) C25—H25A 0.9500
C9—H9A 0.9500
Cu1i—I1—Cu1 68.967 (9) C8—C9—H9A 119.9
N1—Cu1—P1 115.34 (5) C11—C10—C9 120.45 (19)
N1—Cu1—I1i 104.66 (5) C11—C10—H10A 119.8
P1—Cu1—I1i 115.133 (15) C9—C10—H10A 119.8
N1—Cu1—I1 102.74 (5) C10—C11—C12 120.15 (19)
P1—Cu1—I1 107.279 (15) C10—C11—H11A 119.9
I1i—Cu1—I1 111.033 (9) C12—C11—H11A 119.9
N1—Cu1—Cu1i 114.71 (5) C11—C12—C13 119.39 (19)
P1—Cu1—Cu1i 129.538 (16) C11—C12—H12A 120.3
I1i—Cu1—Cu1i 56.087 (8) C13—C12—H12A 120.3
I1—Cu1—Cu1i 54.946 (8) C12—C13—C8 121.04 (19)
C8—P1—C14 103.50 (8) C12—C13—H13A 119.5
C8—P1—C20 103.58 (8) C8—C13—H13A 119.5
C14—P1—C20 104.71 (8) C15—C14—C19 119.24 (17)
C8—P1—Cu1 117.67 (6) C15—C14—P1 123.60 (14)
C14—P1—Cu1 115.48 (6) C19—C14—P1 117.15 (14)
C20—P1—Cu1 110.48 (6) C14—C15—C16 120.1 (2)
C5—N1—C1 116.93 (15) C14—C15—H15A 120.0
C5—N1—Cu1 121.74 (12) C16—C15—H15A 120.0
C1—N1—Cu1 121.32 (12) C17—C16—C15 120.3 (2)
C6—N2—N2ii 113.4 (2) C17—C16—H16A 119.9
N1—C1—C2 123.36 (18) C15—C16—H16A 119.9
N1—C1—H1A 118.3 C18—C17—C16 119.6 (2)
C2—C1—H1A 118.3 C18—C17—H17A 120.2
C1—C2—C3 119.49 (17) C16—C17—H17A 120.2
C1—C2—H2A 120.3 C17—C18—C19 120.4 (2)
C3—C2—H2A 120.3 C17—C18—H18A 119.8
C2—C3—C4 117.29 (16) C19—C18—H18A 119.8
C2—C3—C6 120.86 (17) C18—C19—C14 120.3 (2)
C4—C3—C6 121.85 (17) C18—C19—H19A 119.8
C5—C4—C3 119.33 (17) C14—C19—H19A 119.8
C5—C4—H4A 120.3 C25—C20—C21 118.99 (17)
C3—C4—H4A 120.3 C25—C20—P1 123.81 (16)
N1—C5—C4 123.53 (17) C21—C20—P1 116.96 (14)
N1—C5—H5A 118.2 C22—C21—C20 120.79 (19)
C4—C5—H5A 118.2 C22—C21—H21A 119.6
N2—C6—C3 114.47 (17) C20—C21—H21A 119.6
N2—C6—C7 126.95 (17) C23—C22—C21 120.06 (19)
C3—C6—C7 118.56 (17) C23—C22—H22A 120.0
C6—C7—H7A 109.5 C21—C22—H22A 120.0
C6—C7—H7B 109.5 C24—C23—C22 119.50 (18)
H7A—C7—H7B 109.5 C24—C23—H23A 120.2
C6—C7—H7C 109.5 C22—C23—H23A 120.2
H7A—C7—H7C 109.5 C23—C24—C25 120.7 (2)
H7B—C7—H7C 109.5 C23—C24—H24A 119.6
C13—C8—C9 118.83 (18) C25—C24—H24A 119.6
C13—C8—P1 118.03 (14) C20—C25—C24 119.9 (2)
C9—C8—P1 123.14 (14) C20—C25—H25A 120.1
C10—C9—C8 120.13 (18) C24—C25—H25A 120.1
C10—C9—H9A 119.9
Cu1i—I1—Cu1—N1 111.41 (5) Cu1—P1—C8—C13 32.33 (16)
Cu1i—I1—Cu1—P1 −126.595 (17) C14—P1—C8—C9 −18.90 (17)
Cu1i—I1—Cu1—I1i 0.0 C20—P1—C8—C9 90.17 (16)
N1—Cu1—P1—C8 −84.49 (8) Cu1—P1—C8—C9 −147.61 (13)
I1i—Cu1—P1—C8 37.63 (6) C13—C8—C9—C10 −0.5 (3)
I1—Cu1—P1—C8 161.76 (6) P1—C8—C9—C10 179.45 (15)
Cu1i—Cu1—P1—C8 103.30 (6) C8—C9—C10—C11 0.9 (3)
N1—Cu1—P1—C14 152.70 (8) C9—C10—C11—C12 −0.4 (3)
I1i—Cu1—P1—C14 −85.18 (7) C10—C11—C12—C13 −0.4 (3)
I1—Cu1—P1—C14 38.95 (7) C11—C12—C13—C8 0.8 (3)
Cu1i—Cu1—P1—C14 −19.51 (7) C9—C8—C13—C12 −0.3 (3)
N1—Cu1—P1—C20 34.12 (9) P1—C8—C13—C12 179.73 (16)
I1i—Cu1—P1—C20 156.24 (7) C8—P1—C14—C15 91.61 (19)
I1—Cu1—P1—C20 −79.63 (7) C20—P1—C14—C15 −16.6 (2)
Cu1i—Cu1—P1—C20 −138.08 (7) Cu1—P1—C14—C15 −138.34 (17)
P1—Cu1—N1—C5 −77.61 (16) C8—P1—C14—C19 −87.26 (17)
I1i—Cu1—N1—C5 154.82 (14) C20—P1—C14—C19 164.52 (16)
I1—Cu1—N1—C5 38.75 (16) Cu1—P1—C14—C19 42.79 (18)
Cu1i—Cu1—N1—C5 95.78 (15) C19—C14—C15—C16 −0.1 (4)
P1—Cu1—N1—C1 103.31 (15) P1—C14—C15—C16 −178.9 (2)
I1i—Cu1—N1—C1 −24.26 (16) C14—C15—C16—C17 0.7 (4)
I1—Cu1—N1—C1 −140.33 (15) C15—C16—C17—C18 0.1 (4)
Cu1i—Cu1—N1—C1 −83.30 (16) C16—C17—C18—C19 −1.5 (4)
C5—N1—C1—C2 −1.6 (3) C17—C18—C19—C14 2.1 (4)
Cu1—N1—C1—C2 177.55 (16) C15—C14—C19—C18 −1.3 (3)
N1—C1—C2—C3 −1.0 (3) P1—C14—C19—C18 177.6 (2)
C1—C2—C3—C4 2.3 (3) C8—P1—C20—C25 4.4 (2)
C1—C2—C3—C6 −176.79 (18) C14—P1—C20—C25 112.59 (19)
C2—C3—C4—C5 −1.2 (3) Cu1—P1—C20—C25 −122.45 (18)
C6—C3—C4—C5 177.88 (19) C8—P1—C20—C21 178.64 (15)
C1—N1—C5—C4 2.8 (3) C14—P1—C20—C21 −73.20 (16)
Cu1—N1—C5—C4 −176.36 (16) Cu1—P1—C20—C21 51.76 (16)
C3—C4—C5—N1 −1.4 (3) C25—C20—C21—C22 1.0 (3)
N2ii—N2—C6—C3 −179.94 (18) P1—C20—C21—C22 −173.48 (16)
N2ii—N2—C6—C7 1.5 (3) C20—C21—C22—C23 0.9 (3)
C2—C3—C6—N2 −21.8 (3) C21—C22—C23—C24 −1.9 (3)
C4—C3—C6—N2 159.10 (19) C22—C23—C24—C25 1.0 (4)
C2—C3—C6—C7 156.82 (19) C21—C20—C25—C24 −1.9 (3)
C4—C3—C6—C7 −22.2 (3) P1—C20—C25—C24 172.2 (2)
C14—P1—C8—C13 161.04 (15) C23—C24—C25—C20 0.9 (4)
C20—P1—C8—C13 −89.89 (16)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB6379).

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) global, I. DOI: 10.1107/S1600536811036555/hb6379sup1.cif

e-67-m1389-sup1.cif (23.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811036555/hb6379Isup2.hkl

e-67-m1389-Isup2.hkl (434.4KB, hkl)

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


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