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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 May 12;68(Pt 6):m756–m757. doi: 10.1107/S1600536812020843

Di-μ-iodido-bis­[(dimethyl 2,2′-biquinoline-4,4′-dicarboxyl­ate-κ2 N,N′)copper(I)]

Radosław Starosta a,*, Urszula K Komarnicka a, Justyna Nagaj a, Kamila Stokowa-Sołtys a, Aleksandra Bykowska a
PMCID: PMC3379095  PMID: 22719316

Abstract

In the centrosymmetric dinuclear title complex, [Cu2I2(C22H16N2O4)2], the CuI atom is coordinated in a distorted tetra­hedral geometry by an N,N′-bidentate dimethyl 2,2′-biquinoline-4,4′-dicarboxyl­ate ligand and two symmetry-related I atoms, which act as bridges to a symmetry-related CuI atom. The distance between the CuI atoms within the dinuclear unit is 2.6723 (11) Å.

Related literature  

Copper(I) complexes are a subject of high inter­est and have been extensively studied during the past two decades because of their diversified photo-physical properties (Lavie-Cambot et al., 2008; Vorontsov et al., 2009; Hashimoto et al., 2011). The title complex is similar to other copper(I) complexes with halides and aromatic diimines: [Cu2I2(1,10-phenanthroline)2] and Cu2 X 2(2,9-dimethyl-1,10-phenanthroline)2], where X = I, Br, Cl (Healy et al., 1985); [Cu2 X 2(1,10-phenanthroline)2], where X = Cl and I (Yu et al., 2004); [Cu2 X 2(NN)2], where X = Br, I and NN = bidentate imino nitroxides (Oshio et al., 1996); [Cu2Cl2(dihexsyl-2,2′-biquinoline-4,4′-dicarboxyl­ate)2] [Cu2Cl2(2,2′-biquinoline-4,4′-dicarb­oxy­lic acid)2] (Vatsadze et al., 2010). For the preparation of the dimethyl-2,2′-biquinoline-4,4′-dicarboxyl­ate ligand, see: Pucci et al. (2011) and of the P(CH2N(CH2CH2)2O)3 phosphane ligand, see: Starosta et al. (2010).graphic file with name e-68-0m756-scheme1.jpg

Experimental  

Crystal data  

  • [Cu2I2(C22H16N2O4)2]

  • M r = 1125.62

  • Triclinic, Inline graphic

  • a = 8.792 (3) Å

  • b = 9.157 (3) Å

  • c = 12.865 (4) Å

  • α = 96.59 (3)°

  • β = 102.49 (3)°

  • γ = 103.51 (3)°

  • V = 968.2 (5) Å3

  • Z = 1

  • Mo Kα radiation

  • μ = 2.76 mm−1

  • T = 100 K

  • 0.15 × 0.10 × 0.10 mm

Data collection  

  • Kuma KM-4-CCD κ-geometry diffractometer

  • Absorption correction: analytical [CrysAlis RED (Oxford Diffraction, 2006), based on expressions derived by Clark & Reid (1995)] T min = 0.466, T max = 0.912

  • 15308 measured reflections

  • 5471 independent reflections

  • 4606 reflections with I > 2σ(I)

  • R int = 0.028

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.027

  • wR(F 2) = 0.065

  • S = 1.02

  • 5471 reflections

  • 273 parameters

  • H-atom parameters constrained

  • Δρmax = 0.89 e Å−3

  • Δρmin = −1.16 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2006); cell refinement: CrysAlis RED (Oxford Diffraction, 2006); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2006); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812020843/kp2406sup1.cif

e-68-0m756-sup1.cif (23.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812020843/kp2406Isup2.hkl

e-68-0m756-Isup2.hkl (267.9KB, hkl)

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

Table 1. Selected bond lengths (Å).

Cu1—N1A 2.088 (2)
Cu1—N1B 2.092 (2)
Cu1—I1 2.5473 (10)
Cu1—I1i 2.6996 (9)

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors are grateful to Dr Miłosz Siczek for the crystal measurements and help with the preparation of this manuscript.

supplementary crystallographic information

Comment

The asymmetric unit of the studied bis((µ-iodo)-(dimethyl-2,2'-biquinoline-4,4'-dicarboxylate))-di-copper(I) complex consist of the [(dimethyl-2,2'-biquinoline-4,4'-dicarboxylate)Cu(I)] moiety (Fig. 1, Table 1). CuI atoms are bridged by two iodide ions forming the planar rhombic Cu2(µ-I)2 core. Additionally coordinated by the imine nitrogen atoms of the dimethyl-2,2'-biquinoline-4,4'-dicarboxylate ligand, each CuI atom reveals a distorted tetrahedral geometry. Connected quinoline rings of the coordinated molecule of dimethyl-2,2'-biquinoline-4,4'-dicarboxylate are not coplanar, the angle between their planes is 5.40 (7)°.

Experimental

Crystals of the title complex were grown in the mixture of dichloromethane and acetone in an attempt to obtain crystals of [Cu(I)(dimethyl-2,2'-biquinoline-4,4'-dicarboxylate) P(CH2N(CH2CH2)2O)3] complex. CuI was purchased from Aldrich. Dimethyl-2,2'-biquinoline-4,4'- dicarboxylate ligand was prepared from 2,2'-biquinoline-4,4'-dicarboxylic acid (Aldrich) according to the literature method (Pucci et al., 2011). P(CH2N(CH2CH2)2O)3 phosphane ligand was synthesized as described previously (Starosta et al., 2010).

Refinement

All hydrogen atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the complex showing the atom-labelling scheme and displacement ellipsoids at the 50% probability (symmmetry code used: -x + 1, -y, -z + 1).

Crystal data

[Cu2I2(C22H16N2O4)2] Z = 1
Mr = 1125.62 F(000) = 552
Triclinic, P1 Dx = 1.930 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 8.792 (3) Å Cell parameters from 11359 reflections
b = 9.157 (3) Å θ = 2.9–36.8°
c = 12.865 (4) Å µ = 2.76 mm1
α = 96.59 (3)° T = 100 K
β = 102.49 (3)° Plate, orange
γ = 103.51 (3)° 0.15 × 0.10 × 0.10 mm
V = 968.2 (5) Å3

Data collection

Kuma KM-4-CCD κ-geometry diffractometer 5471 independent reflections
Radiation source: fine-focus sealed tube 4606 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.028
ω scans θmax = 30.0°, θmin = 2.9°
Absorption correction: analytical [CrysAlis RED (Oxford Diffraction, 2006), based on expressions derived by Clark & Reid (1995)] h = −10→12
Tmin = 0.466, Tmax = 0.912 k = −12→11
15308 measured reflections l = −17→17

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) = 0.065 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.040P)2] where P = (Fo2 + 2Fc2)/3
5471 reflections (Δ/σ)max = 0.001
273 parameters Δρmax = 0.89 e Å3
0 restraints Δρmin = −1.16 e Å3

Special details

Experimental. Absorption correction: CrysAlis RED, (Oxford Diffraction, 2006). Analytical numeric absorption correction using a multifaceted crystal model based on expressions derived by R.C. Clark & J.S. Reid. (Clark, R. C. & Reid, J. S., 1995)
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
Cu1 0.34262 (3) −0.02511 (3) 0.49564 (2) 0.01649 (7)
I1 0.495174 (17) 0.240323 (17) 0.478225 (12) 0.01826 (5)
N1A 0.1380 (2) −0.1629 (2) 0.38141 (15) 0.0142 (3)
C2A 0.0293 (3) −0.2436 (3) 0.42433 (18) 0.0153 (4)
C3A −0.0976 (3) −0.3688 (3) 0.36264 (18) 0.0172 (4)
H3A −0.1715 −0.4265 0.3963 0.021*
C4A −0.1132 (3) −0.4064 (3) 0.25341 (18) 0.0165 (4)
C5A −0.0028 (3) −0.3491 (3) 0.09277 (18) 0.0191 (4)
H5A −0.0859 −0.4295 0.0451 0.023*
C6A 0.1133 (3) −0.2621 (3) 0.05366 (19) 0.0204 (5)
H6A 0.1111 −0.2840 −0.0207 0.024*
C7A 0.2367 (3) −0.1399 (3) 0.12198 (19) 0.0200 (5)
H7A 0.3155 −0.0795 0.0932 0.024*
C8A 0.2426 (3) −0.1086 (3) 0.22991 (19) 0.0178 (4)
H8A 0.3256 −0.0265 0.2759 0.021*
C9A 0.1252 (3) −0.1986 (2) 0.27237 (18) 0.0150 (4)
C10A −0.0005 (3) −0.3205 (3) 0.20414 (18) 0.0158 (4)
C11A −0.2508 (3) −0.5363 (3) 0.18690 (19) 0.0190 (4)
O11A −0.3182 (2) −0.5417 (2) 0.09388 (14) 0.0281 (4)
O12A −0.28999 (19) −0.64555 (19) 0.24393 (14) 0.0212 (3)
C12A −0.4228 (3) −0.7757 (3) 0.1849 (2) 0.0245 (5)
H12D −0.5155 −0.7399 0.1519 0.037*
H12E −0.4536 −0.8435 0.2349 0.037*
H12F −0.3887 −0.8313 0.1283 0.037*
N1B 0.1763 (2) −0.0732 (2) 0.58953 (15) 0.0144 (3)
C2B 0.0491 (2) −0.1915 (3) 0.54192 (17) 0.0140 (4)
C3B −0.0588 (3) −0.2629 (3) 0.59879 (18) 0.0154 (4)
H3B −0.1447 −0.3501 0.5632 0.019*
C4B −0.0395 (3) −0.2061 (3) 0.70607 (18) 0.0155 (4)
C5B 0.1212 (3) −0.0045 (3) 0.86815 (18) 0.0169 (4)
H5B 0.0512 −0.0429 0.9113 0.020*
C6B 0.2517 (3) 0.1184 (3) 0.91204 (18) 0.0193 (4)
H6B 0.2709 0.1642 0.9854 0.023*
C7B 0.3583 (3) 0.1782 (3) 0.85011 (19) 0.0188 (4)
H7B 0.4489 0.2630 0.8821 0.023*
C8B 0.3309 (3) 0.1139 (3) 0.74412 (18) 0.0176 (4)
H8B 0.4023 0.1548 0.7025 0.021*
C9B 0.1967 (3) −0.0135 (3) 0.69604 (18) 0.0153 (4)
C10B 0.0894 (3) −0.0752 (2) 0.75828 (17) 0.0145 (4)
C11B −0.1583 (3) −0.2831 (3) 0.76375 (18) 0.0163 (4)
O11B −0.1970 (2) −0.2197 (2) 0.83756 (14) 0.0220 (4)
O12B −0.2166 (2) −0.43175 (19) 0.72286 (14) 0.0210 (3)
C12B −0.3430 (3) −0.5141 (3) 0.7667 (2) 0.0241 (5)
H12A −0.3126 −0.4851 0.8456 0.036*
H12B −0.3575 −0.6240 0.7470 0.036*
H12C −0.4443 −0.4890 0.7371 0.036*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cu1 0.01350 (13) 0.01802 (14) 0.01445 (13) −0.00091 (10) 0.00308 (10) 0.00031 (10)
I1 0.01682 (7) 0.01604 (7) 0.01965 (8) 0.00169 (5) 0.00320 (5) 0.00222 (5)
N1A 0.0140 (8) 0.0151 (9) 0.0116 (8) 0.0030 (7) 0.0011 (7) 0.0007 (7)
C2A 0.0139 (9) 0.0167 (10) 0.0136 (10) 0.0032 (8) 0.0028 (8) −0.0001 (8)
C3A 0.0139 (10) 0.0188 (11) 0.0161 (10) 0.0003 (8) 0.0029 (8) 0.0020 (8)
C4A 0.0170 (10) 0.0145 (10) 0.0150 (10) 0.0019 (8) 0.0020 (8) −0.0011 (8)
C5A 0.0216 (11) 0.0190 (11) 0.0140 (10) 0.0038 (9) 0.0028 (8) −0.0011 (8)
C6A 0.0274 (12) 0.0200 (11) 0.0122 (10) 0.0059 (9) 0.0039 (9) −0.0006 (8)
C7A 0.0227 (11) 0.0205 (11) 0.0170 (10) 0.0040 (9) 0.0063 (9) 0.0051 (9)
C8A 0.0173 (10) 0.0180 (11) 0.0160 (10) 0.0026 (8) 0.0023 (8) 0.0027 (8)
C9A 0.0145 (9) 0.0146 (10) 0.0142 (10) 0.0028 (8) 0.0018 (8) 0.0016 (8)
C10A 0.0150 (10) 0.0160 (10) 0.0140 (10) 0.0031 (8) 0.0009 (8) −0.0001 (8)
C11A 0.0157 (10) 0.0198 (11) 0.0186 (11) 0.0011 (8) 0.0053 (8) −0.0024 (9)
O11A 0.0260 (9) 0.0315 (10) 0.0161 (8) −0.0037 (8) −0.0016 (7) −0.0013 (7)
O12A 0.0164 (8) 0.0178 (8) 0.0224 (8) −0.0030 (6) 0.0000 (6) 0.0000 (7)
C12A 0.0162 (11) 0.0184 (11) 0.0312 (13) −0.0030 (9) 0.0012 (10) −0.0017 (10)
N1B 0.0129 (8) 0.0160 (9) 0.0123 (8) 0.0013 (7) 0.0024 (7) 0.0008 (7)
C2B 0.0121 (9) 0.0148 (10) 0.0124 (9) 0.0012 (7) 0.0013 (7) 0.0002 (8)
C3B 0.0118 (9) 0.0170 (10) 0.0151 (10) 0.0016 (8) 0.0012 (8) 0.0016 (8)
C4B 0.0129 (9) 0.0173 (10) 0.0158 (10) 0.0034 (8) 0.0039 (8) 0.0021 (8)
C5B 0.0176 (10) 0.0192 (11) 0.0138 (10) 0.0056 (8) 0.0036 (8) 0.0022 (8)
C6B 0.0220 (11) 0.0211 (11) 0.0124 (10) 0.0053 (9) 0.0024 (8) −0.0020 (8)
C7B 0.0175 (10) 0.0162 (10) 0.0180 (10) 0.0004 (8) 0.0018 (8) −0.0021 (8)
C8B 0.0167 (10) 0.0181 (11) 0.0157 (10) 0.0007 (8) 0.0047 (8) 0.0005 (8)
C9B 0.0141 (9) 0.0168 (10) 0.0142 (10) 0.0042 (8) 0.0023 (8) 0.0011 (8)
C10B 0.0142 (9) 0.0157 (10) 0.0135 (10) 0.0042 (8) 0.0030 (8) 0.0021 (8)
C11B 0.0145 (9) 0.0182 (10) 0.0149 (10) 0.0035 (8) 0.0017 (8) 0.0036 (8)
O11B 0.0212 (8) 0.0233 (9) 0.0191 (8) 0.0007 (7) 0.0085 (7) −0.0016 (7)
O12B 0.0214 (8) 0.0167 (8) 0.0250 (9) 0.0013 (6) 0.0110 (7) 0.0025 (7)
C12B 0.0244 (12) 0.0179 (11) 0.0299 (13) 0.0001 (9) 0.0132 (10) 0.0042 (10)

Geometric parameters (Å, º)

Cu1—N1A 2.088 (2) C12A—H12D 0.9800
Cu1—N1B 2.092 (2) C12A—H12E 0.9800
Cu1—I1 2.5473 (10) C12A—H12F 0.9800
Cu1—I1i 2.6996 (9) N1B—C2B 1.336 (3)
Cu1—Cu1i 2.6723 (11) N1B—C9B 1.373 (3)
I1—Cu1i 2.6997 (9) C2B—C3B 1.408 (3)
N1A—C2A 1.325 (3) C3B—C4B 1.377 (3)
N1A—C9A 1.377 (3) C3B—H3B 0.9500
C2A—C3A 1.414 (3) C4B—C10B 1.422 (3)
C2A—C2B 1.493 (3) C4B—C11B 1.500 (3)
C3A—C4A 1.377 (3) C5B—C6B 1.368 (3)
C3A—H3A 0.9500 C5B—C10B 1.425 (3)
C4A—C10A 1.423 (3) C5B—H5B 0.9500
C4A—C11A 1.502 (3) C6B—C7B 1.413 (3)
C5A—C6A 1.366 (3) C6B—H6B 0.9500
C5A—C10A 1.421 (3) C7B—C8B 1.368 (3)
C5A—H5A 0.9500 C7B—H7B 0.9500
C6A—C7A 1.412 (3) C8B—C9B 1.419 (3)
C6A—H6A 0.9500 C8B—H8B 0.9500
C7A—C8A 1.372 (3) C9B—C10B 1.426 (3)
C7A—H7A 0.9500 C11B—O11B 1.208 (3)
C8A—C9A 1.412 (3) C11B—O12B 1.336 (3)
C8A—H8A 0.9500 O12B—C12B 1.448 (3)
C9A—C10A 1.420 (3) C12B—H12A 0.9800
C11A—O11A 1.205 (3) C12B—H12B 0.9800
C11A—O12A 1.332 (3) C12B—H12C 0.9800
O12A—C12A 1.455 (3)
N1A—Cu1—N1B 78.10 (8) O12A—C12A—H12F 109.5
N1A—Cu1—I1 124.55 (6) H12D—C12A—H12F 109.5
N1B—Cu1—I1 125.61 (6) H12E—C12A—H12F 109.5
N1A—Cu1—I1i 96.95 (6) C2B—N1B—C9B 118.65 (19)
N1B—Cu1—I1i 103.46 (6) C2B—N1B—Cu1 113.28 (14)
I1—Cu1—I1i 118.85 (3) C9B—N1B—Cu1 127.25 (15)
Cu1—I1—Cu1i 61.15 (3) N1B—C2B—C3B 122.3 (2)
C2A—N1A—C9A 119.28 (19) N1B—C2B—C2A 115.52 (19)
C2A—N1A—Cu1 113.75 (15) C3B—C2B—C2A 122.14 (19)
C9A—N1A—Cu1 125.41 (15) C4B—C3B—C2B 119.9 (2)
N1A—C2A—C3A 122.3 (2) C4B—C3B—H3B 120.1
N1A—C2A—C2B 115.21 (19) C2B—C3B—H3B 120.1
C3A—C2A—C2B 122.5 (2) C3B—C4B—C10B 119.5 (2)
C4A—C3A—C2A 119.4 (2) C3B—C4B—C11B 118.5 (2)
C4A—C3A—H3A 120.3 C10B—C4B—C11B 121.9 (2)
C2A—C3A—H3A 120.3 C6B—C5B—C10B 120.6 (2)
C3A—C4A—C10A 119.8 (2) C6B—C5B—H5B 119.7
C3A—C4A—C11A 119.7 (2) C10B—C5B—H5B 119.7
C10A—C4A—C11A 120.5 (2) C5B—C6B—C7B 121.1 (2)
C6A—C5A—C10A 120.6 (2) C5B—C6B—H6B 119.4
C6A—C5A—H5A 119.7 C7B—C6B—H6B 119.4
C10A—C5A—H5A 119.7 C8B—C7B—C6B 119.9 (2)
C5A—C6A—C7A 121.1 (2) C8B—C7B—H7B 120.0
C5A—C6A—H6A 119.5 C6B—C7B—H7B 120.0
C7A—C6A—H6A 119.5 C7B—C8B—C9B 120.4 (2)
C8A—C7A—C6A 120.0 (2) C7B—C8B—H8B 119.8
C8A—C7A—H7A 120.0 C9B—C8B—H8B 119.8
C6A—C7A—H7A 120.0 N1B—C9B—C8B 117.5 (2)
C7A—C8A—C9A 119.8 (2) N1B—C9B—C10B 122.5 (2)
C7A—C8A—H8A 120.1 C8B—C9B—C10B 120.0 (2)
C9A—C8A—H8A 120.1 C4B—C10B—C5B 125.0 (2)
N1A—C9A—C8A 117.3 (2) C4B—C10B—C9B 117.0 (2)
N1A—C9A—C10A 122.1 (2) C5B—C10B—C9B 118.0 (2)
C8A—C9A—C10A 120.6 (2) O11B—C11B—O12B 124.0 (2)
C9A—C10A—C5A 117.9 (2) O11B—C11B—C4B 124.8 (2)
C9A—C10A—C4A 117.1 (2) O12B—C11B—C4B 111.19 (19)
C5A—C10A—C4A 125.0 (2) C11B—O12B—C12B 115.55 (18)
O11A—C11A—O12A 123.9 (2) O12B—C12B—H12A 109.5
O11A—C11A—C4A 124.7 (2) O12B—C12B—H12B 109.5
O12A—C11A—C4A 111.4 (2) H12A—C12B—H12B 109.5
C11A—O12A—C12A 114.73 (19) O12B—C12B—H12C 109.5
O12A—C12A—H12D 109.5 H12A—C12B—H12C 109.5
O12A—C12A—H12E 109.5 H12B—C12B—H12C 109.5
H12D—C12A—H12E 109.5
N1A—Cu1—I1—Cu1i −123.16 (7) I1—Cu1—N1B—C2B 140.88 (14)
N1B—Cu1—I1—Cu1i 136.17 (7) I1i—Cu1—N1B—C2B −77.71 (15)
I1i—Cu1—I1—Cu1i 0.0 N1A—Cu1—N1B—C9B −173.9 (2)
N1B—Cu1—N1A—C2A −17.89 (15) I1—Cu1—N1B—C9B −49.7 (2)
I1—Cu1—N1A—C2A −143.16 (14) I1i—Cu1—N1B—C9B 91.69 (18)
I1i—Cu1—N1A—C2A 84.46 (15) C9B—N1B—C2B—C3B −4.1 (3)
N1B—Cu1—N1A—C9A 176.59 (19) Cu1—N1B—C2B—C3B 166.34 (17)
I1—Cu1—N1A—C9A 51.33 (19) C9B—N1B—C2B—C2A 176.24 (19)
I1i—Cu1—N1A—C9A −81.05 (18) Cu1—N1B—C2B—C2A −13.4 (2)
C9A—N1A—C2A—C3A 1.9 (3) N1A—C2A—C2B—N1B −1.9 (3)
Cu1—N1A—C2A—C3A −164.62 (17) C3A—C2A—C2B—N1B 179.0 (2)
C9A—N1A—C2A—C2B −177.27 (19) N1A—C2A—C2B—C3B 178.4 (2)
Cu1—N1A—C2A—C2B 16.2 (2) C3A—C2A—C2B—C3B −0.7 (3)
N1A—C2A—C3A—C4A −2.1 (3) N1B—C2B—C3B—C4B 3.3 (3)
C2B—C2A—C3A—C4A 177.0 (2) C2A—C2B—C3B—C4B −177.0 (2)
C2A—C3A—C4A—C10A 0.9 (3) C2B—C3B—C4B—C10B 0.2 (3)
C2A—C3A—C4A—C11A −178.1 (2) C2B—C3B—C4B—C11B 178.9 (2)
C10A—C5A—C6A—C7A −1.2 (4) C10B—C5B—C6B—C7B −0.1 (4)
C5A—C6A—C7A—C8A 1.0 (4) C5B—C6B—C7B—C8B 0.6 (4)
C6A—C7A—C8A—C9A 0.0 (3) C6B—C7B—C8B—C9B −0.5 (4)
C2A—N1A—C9A—C8A 179.3 (2) C2B—N1B—C9B—C8B −178.8 (2)
Cu1—N1A—C9A—C8A −15.9 (3) Cu1—N1B—C9B—C8B 12.3 (3)
C2A—N1A—C9A—C10A −0.5 (3) C2B—N1B—C9B—C10B 1.5 (3)
Cu1—N1A—C9A—C10A 164.31 (16) Cu1—N1B—C9B—C10B −167.44 (16)
C7A—C8A—C9A—N1A 179.4 (2) C7B—C8B—C9B—N1B −179.7 (2)
C7A—C8A—C9A—C10A −0.8 (3) C7B—C8B—C9B—C10B 0.0 (3)
N1A—C9A—C10A—C5A −179.6 (2) C3B—C4B—C10B—C5B 179.2 (2)
C8A—C9A—C10A—C5A 0.6 (3) C11B—C4B—C10B—C5B 0.6 (3)
N1A—C9A—C10A—C4A −0.6 (3) C3B—C4B—C10B—C9B −2.6 (3)
C8A—C9A—C10A—C4A 179.5 (2) C11B—C4B—C10B—C9B 178.8 (2)
C6A—C5A—C10A—C9A 0.4 (3) C6B—C5B—C10B—C4B 177.8 (2)
C6A—C5A—C10A—C4A −178.5 (2) C6B—C5B—C10B—C9B −0.4 (3)
C3A—C4A—C10A—C9A 0.4 (3) N1B—C9B—C10B—C4B 1.8 (3)
C11A—C4A—C10A—C9A 179.4 (2) C8B—C9B—C10B—C4B −177.9 (2)
C3A—C4A—C10A—C5A 179.3 (2) N1B—C9B—C10B—C5B −179.8 (2)
C11A—C4A—C10A—C5A −1.7 (3) C8B—C9B—C10B—C5B 0.4 (3)
C3A—C4A—C11A—O11A 146.9 (3) C3B—C4B—C11B—O11B −149.8 (2)
C10A—C4A—C11A—O11A −32.1 (4) C10B—C4B—C11B—O11B 28.8 (3)
C3A—C4A—C11A—O12A −32.9 (3) C3B—C4B—C11B—O12B 30.2 (3)
C10A—C4A—C11A—O12A 148.1 (2) C10B—C4B—C11B—O12B −151.2 (2)
O11A—C11A—O12A—C12A 0.2 (3) O11B—C11B—O12B—C12B 5.1 (3)
C4A—C11A—O12A—C12A 179.96 (18) C4B—C11B—O12B—C12B −174.87 (19)
N1A—Cu1—N1B—C2B 16.69 (15)

Symmetry code: (i) −x+1, −y, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: KP2406).

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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/S1600536812020843/kp2406sup1.cif

e-68-0m756-sup1.cif (23.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812020843/kp2406Isup2.hkl

e-68-0m756-Isup2.hkl (267.9KB, hkl)

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


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