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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Sep 19;68(Pt 10):m1277–m1278. doi: 10.1107/S1600536812037270

catena-Poly[[[iodidocopper(I)]-{μ-N-[(pyridin-2-yl-κN)methyl­idene]pyridin-3-amine-κ2 N 3:N 1}] acetonitrile hemisolvate]

Ali Mahmoudi a,*, Saeed Dehghanpour b, Mojtaba Babakhodaverdi a
PMCID: PMC3470156  PMID: 23125600

Abstract

In the asymmetric unit of the title polymeric complex, {[CuI(C11H9N3)]·0.5CH3CN}n, there are two CuI atoms, two N-[(pyridin-2-yl-κN)methyl­idene]pyridin-3-amine (PyPy) ligands and two I atoms. Both CuI atoms have a distorted tetra­hedral geometry, each being coordinated by one I atom, two N atoms of one PyPy ligand and one N atom from an adjacent PyPy ligand. In the crystal, infinite helical chains of [Cu2(PyPy)2]n are formed propagating along the b axis. These chains are linked via weak C—H⋯I hydrogen bonds and π–π stacking inter­actions [shortest centroid–centroid distance = 3.2727 (14) Å]. During the refinement, electron-density peaks were located that were believed to be highly disordered solvent mol­ecules (possibly acetonitrile). The SQUEEZE option in PLATON [Spek (2009). Acta Cryst. D65, 148–155] indicated there were solvent cavities with a total volume of 196 Å3 containing approximately 60 electrons per unit cell, which equated to one mol­ecule of acetonitrile per asymmetric unit.

Related literature  

For related structures and applications of coordination polymers, see: Moulton & Zaworotko (2001); Fei et al. (2000). For the synthesis of the title ligand, see: Dehghanpour et al. (2009). graphic file with name e-68-m1277-scheme1.jpg

Experimental  

Crystal data  

  • [CuI(C11H9N3)]·0.5C2H3N

  • M r = 394.18

  • Monoclinic, Inline graphic

  • a = 7.1800 (2) Å

  • b = 13.2303 (7) Å

  • c = 27.9383 (13) Å

  • β = 90.741 (3)°

  • V = 2653.7 (2) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 3.96 mm−1

  • T = 150 K

  • 0.17 × 0.12 × 0.10 mm

Data collection  

  • Nonius KappaCCD diffractometer

  • Absorption correction: multi-scan (SORTAV; Blessing, 1995) T min = 0.569, T max = 0.733

  • 19063 measured reflections

  • 4676 independent reflections

  • 2627 reflections with I > 2σ(I)

  • R int = 0.104

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.060

  • wR(F 2) = 0.178

  • S = 1.02

  • 4676 reflections

  • 289 parameters

  • H-atom parameters constrained

  • Δρmax = 1.39 e Å−3

  • Δρmin = −1.24 e Å−3

Data collection: COLLECT (Nonius, 2002); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN; program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812037270/su2480sup1.cif

e-68-m1277-sup1.cif (28.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812037270/su2480Isup2.hkl

e-68-m1277-Isup2.hkl (270.1KB, 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
C22—H22A⋯I1i 0.95 3.03 3.789 (12) 138
C20—H20A⋯I1ii 0.95 3.14 4.025 (12) 156
C17—H17A⋯I2iii 0.95 3.16 4.011 (11) 149

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic.

Acknowledgments

The authors are grateful to the Islamic Azad University, University Research Councils for partial support of this work. The crystal structure analysis was carried out by Dr A. J. Lough of the Department of Chemistry of the University of Toronto, Canada.

supplementary crystallographic information

Comment

In recent years, coordination polymers have received much attention due to their variety of architectures and the potential applications as functional materials (Moulton & Zaworotko, 2001). Early reports have shown that nitrogen heterocyclic ligands have been employed in the synthesis of many novel structures (Fei et al., 2000). Here, we report on the synthetic and crystal structure of a novel copper iodide complex based on the ligand pyridin-3-ylpyridin-2-ylmethyleneamine (PyPy).

The asymmetric unit of the title compound, Fig. 1, contains two CuI atoms, two pyridin-3-ylpyridin-2-ylmethyleneamine (Dehghanpour et al., 2009) ligands, and two I atoms, Each Cu+ atom is four-coordinated in a distorted tetrahedral configuration by two N atoms from one PyPy ligand, one N atom from an adjacent PyPy ligand and one I atom. Each PyPy ligand chelates the Cu atom (via N, N' atoms) and also bridges to another Cu atom (with N" atom), resulting in the formation of chains propagating along the b axis.

The two ligands in the asymmetric unit are nearly planar. In ligand A the interplanar angles between chelate ring (N2/C6/C7/N3) and pyridine ring (lN3/C7-C11) is 2.11 (3)°, while for ligand B [chelate ring N5/C17/C18/N6 and pyridine ring N6/C18-C22] the same angle is 5.82 (4)°. In ligand A the two pyridine rings (N1/C1-C5 and N3/C7-C11) are inclined to one another by 12.11 (4)°. In ligand B the two pyridine rings (N6/C18-C22 and N4/C12-5C16) are inclined to one another by 7.49 (3)°. However, the interplanar angle between two ligand mean planes (A and B) is 52.82 (1)°.

In the crystal, these chains interact viaπ–π interactions between adjacent, inversion replated PyPy ligands The shortest distance of 3.2727 (14) Å [C15-C19 ring, symmetry code: (iii) = -x + 3, -y - 1, -z + 1] is observed between two inversion related ligands. These chains are further connected through C—H···I interactions (Table 1 and Fig 2.).

Experimental

The title complex was prepared by the reaction of CuI (19.1 mg, 0.1 mmol) and pyridin-3-ylpyridin-2-ylmethyleneamine (18.3 mg, 0.1 mmol) in 20 ml of acetonitrile at room temperature. Crystals of the title compound, suitable for X-ray analysis, were obtained by slow evaporation of the solvent at rt.

Refinement

H atoms were placed in calculated positions and included in the refinement in a riding-motion approximation: C—H = 0.95 Å with Uiso(H)= 1.2Ueq(C). During the refinement of the structure, electron density peaks were located that were believed to be highly disordered solvent molecules (possibly acetonitrile). Attempts to model the solvent molecule were not successful. The SQUEEZE option in PLATON (Spek, A. L. (2009). Acta Cryst. D65, 148-155) indicated there were solvent cavities with a total volume of 196 Å3 containing approximately 60 electrons per unit cell. This was equated to one molecule of acetonitrile per asymmetric unit. The density, the F(000) value, the molecular weight and the formula are given taking into account the results obtained with the SQUEEZE option in PLATON.

Figures

Fig. 1.

Fig. 1.

A view of the molecular structure of the title complex, with atom numbering. Displacement ellipsoids are drawn at the 50% probability level [Symmetry codes: (ix) 5/2 - x, -1/2 + y, 1/2 - z; (x) x, -1 + y, z; (xiii) 5/2 - x, 1/2 + y, 1/2 - z].

Fig. 2.

Fig. 2.

A view of the π–π interactions and C—H···I hydrogen bonds (dotted lines) in the crystal structure of the title compound.

Crystal data

[CuI(C11H9N3)]·0.5C2H3N F(000) = 1512
Mr = 394.18 Dx = 1.973 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 19063 reflections
a = 7.1800 (2) Å θ = 2.5–25.0°
b = 13.2303 (7) Å µ = 3.96 mm1
c = 27.9383 (13) Å T = 150 K
β = 90.741 (3)° Block, brown
V = 2653.7 (2) Å3 0.17 × 0.12 × 0.10 mm
Z = 8

Data collection

Nonius KappaCCD diffractometer 4676 independent reflections
Radiation source: fine-focus sealed tube 2627 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.104
Detector resolution: 9 pixels mm-1 θmax = 25.0°, θmin = 2.7°
φ scans and ω scans with κ offsets h = −8→8
Absorption correction: multi-scan (SORTAV; Blessing, 1995) k = −15→15
Tmin = 0.569, Tmax = 0.733 l = −33→33
19063 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)] = 0.060 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.178 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0943P)2] where P = (Fo2 + 2Fc2)/3
4676 reflections (Δ/σ)max = 0.002
289 parameters Δρmax = 1.39 e Å3
0 restraints Δρmin = −1.24 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
I1 1.60988 (13) −0.00459 (7) 0.36787 (3) 0.0589 (3)
I2 0.61501 (9) −0.05499 (6) 0.10018 (2) 0.0389 (3)
Cu1 1.50363 (18) −0.17127 (11) 0.32943 (4) 0.0400 (4)
Cu2 0.97229 (16) −0.07450 (11) 0.10723 (4) 0.0365 (4)
N1 1.0526 (12) −0.0684 (7) 0.1767 (3) 0.039 (2)
N2 1.4312 (11) −0.1559 (6) 0.2576 (3) 0.032 (2)
N3 1.7228 (11) −0.2492 (7) 0.2989 (3) 0.039 (2)
N4 1.3514 (11) −0.2392 (7) 0.3785 (3) 0.036 (2)
N5 1.3643 (10) −0.4852 (7) 0.4384 (3) 0.029 (2)
N6 1.4522 (11) −0.6811 (7) 0.4423 (3) 0.037 (2)
C1 0.9411 (16) −0.0224 (9) 0.2091 (4) 0.042 (3)
H1A 0.8262 0.0063 0.1987 0.051*
C2 0.9913 (15) −0.0165 (9) 0.2567 (4) 0.044 (3)
H2A 0.9147 0.0176 0.2790 0.053*
C3 1.1567 (14) −0.0616 (8) 0.2713 (4) 0.038 (3)
H3A 1.1948 −0.0593 0.3040 0.045*
C4 1.2640 (14) −0.1092 (8) 0.2385 (4) 0.037 (3)
C5 1.2109 (13) −0.1129 (8) 0.1925 (3) 0.030 (2)
H5A 1.2867 −0.1478 0.1703 0.036*
C6 1.5589 (15) −0.1921 (8) 0.2304 (4) 0.036 (3)
H6A 1.5464 −0.1853 0.1966 0.043*
C7 1.7202 (14) −0.2428 (8) 0.2502 (3) 0.034 (3)
C8 1.8553 (15) −0.2858 (9) 0.2230 (4) 0.042 (3)
H8A 1.8478 −0.2806 0.1891 0.050*
C9 2.0017 (16) −0.3364 (9) 0.2440 (4) 0.044 (3)
H9A 2.0955 −0.3666 0.2250 0.053*
C10 2.0096 (15) −0.3424 (9) 0.2930 (4) 0.049 (3)
H10A 2.1101 −0.3757 0.3088 0.059*
C11 1.8675 (14) −0.2987 (9) 0.3186 (4) 0.045 (3)
H11A 1.8725 −0.3041 0.3525 0.054*
C12 1.2362 (14) −0.1885 (9) 0.4062 (4) 0.040 (3)
H12A 1.2122 −0.1196 0.3988 0.049*
C13 1.1467 (14) −0.2310 (9) 0.4462 (4) 0.045 (3)
H13A 1.0588 −0.1928 0.4638 0.054*
C14 1.1884 (13) −0.3277 (9) 0.4593 (4) 0.040 (3)
H14A 1.1356 −0.3570 0.4870 0.048*
C15 1.3101 (13) −0.3826 (9) 0.4310 (3) 0.033 (3)
C16 1.3879 (12) −0.3373 (8) 0.3914 (3) 0.031 (3)
H16A 1.4704 −0.3758 0.3724 0.037*
C17 1.2990 (12) −0.5374 (8) 0.4725 (4) 0.033 (3)
H17A 1.2150 −0.5068 0.4941 0.040*
C18 1.3492 (14) −0.6418 (8) 0.4791 (4) 0.035 (3)
C19 1.3045 (14) −0.6992 (9) 0.5186 (4) 0.042 (3)
H19A 1.2341 −0.6695 0.5435 0.051*
C20 1.3595 (14) −0.7977 (10) 0.5228 (4) 0.043 (3)
H20A 1.3260 −0.8378 0.5496 0.052*
C21 1.4685 (16) −0.8371 (9) 0.4854 (4) 0.050 (3)
H21A 1.5134 −0.9045 0.4872 0.060*
C22 1.5098 (16) −0.7777 (9) 0.4462 (4) 0.049 (3)
H22A 1.5814 −0.8060 0.4212 0.058*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
I1 0.0911 (7) 0.0473 (6) 0.0383 (5) −0.0199 (5) −0.0001 (4) −0.0023 (4)
I2 0.0311 (4) 0.0564 (6) 0.0292 (4) 0.0023 (3) −0.0015 (3) 0.0035 (4)
Cu1 0.0506 (8) 0.0436 (9) 0.0259 (7) 0.0010 (6) 0.0002 (6) 0.0026 (6)
Cu2 0.0346 (7) 0.0508 (10) 0.0241 (7) 0.0002 (6) 0.0001 (5) 0.0010 (6)
N1 0.048 (6) 0.047 (6) 0.023 (5) 0.004 (5) −0.001 (4) −0.002 (4)
N2 0.037 (5) 0.034 (6) 0.024 (5) 0.001 (4) −0.005 (4) 0.007 (4)
N3 0.031 (5) 0.039 (6) 0.046 (6) −0.005 (4) −0.009 (4) 0.003 (5)
N4 0.033 (5) 0.040 (6) 0.034 (5) 0.006 (4) 0.000 (4) −0.012 (5)
N5 0.029 (4) 0.041 (6) 0.019 (4) 0.004 (4) −0.005 (3) −0.003 (4)
N6 0.035 (5) 0.036 (6) 0.038 (5) −0.010 (4) −0.007 (4) −0.008 (5)
C1 0.051 (7) 0.046 (8) 0.030 (6) 0.006 (6) 0.004 (5) −0.003 (5)
C2 0.044 (7) 0.065 (9) 0.024 (6) 0.006 (6) 0.004 (5) 0.001 (6)
C3 0.047 (7) 0.037 (7) 0.029 (6) 0.013 (5) −0.009 (5) 0.005 (5)
C4 0.036 (6) 0.037 (7) 0.037 (7) 0.005 (5) −0.003 (5) 0.000 (6)
C5 0.030 (6) 0.036 (7) 0.025 (6) 0.000 (5) −0.004 (4) −0.003 (5)
C6 0.055 (7) 0.034 (7) 0.019 (5) −0.003 (5) −0.001 (5) 0.002 (5)
C7 0.042 (6) 0.038 (7) 0.022 (6) −0.005 (5) −0.004 (5) −0.001 (5)
C8 0.044 (7) 0.047 (8) 0.034 (6) −0.009 (6) 0.005 (5) −0.007 (6)
C9 0.049 (7) 0.037 (7) 0.046 (8) 0.003 (6) −0.017 (6) −0.014 (6)
C10 0.040 (7) 0.052 (9) 0.054 (8) 0.018 (6) −0.004 (6) −0.007 (7)
C11 0.040 (7) 0.048 (8) 0.045 (7) −0.006 (6) −0.004 (5) 0.005 (6)
C12 0.037 (6) 0.031 (7) 0.053 (8) 0.006 (5) −0.008 (5) −0.005 (6)
C13 0.031 (6) 0.043 (8) 0.061 (8) −0.003 (5) 0.008 (5) −0.007 (6)
C14 0.036 (6) 0.047 (8) 0.037 (6) −0.005 (5) 0.006 (5) −0.009 (6)
C15 0.028 (5) 0.047 (8) 0.025 (6) −0.001 (5) −0.008 (4) 0.002 (5)
C16 0.025 (5) 0.039 (7) 0.030 (6) −0.011 (5) −0.005 (4) −0.008 (5)
C17 0.020 (5) 0.048 (8) 0.031 (6) −0.005 (5) −0.006 (4) 0.013 (5)
C18 0.038 (6) 0.038 (7) 0.028 (6) −0.008 (5) −0.014 (5) 0.000 (5)
C19 0.042 (6) 0.055 (9) 0.030 (6) −0.010 (6) 0.004 (5) 0.011 (6)
C20 0.043 (7) 0.052 (9) 0.035 (7) −0.006 (6) −0.008 (5) 0.008 (6)
C21 0.062 (8) 0.033 (8) 0.054 (8) −0.008 (6) −0.019 (6) −0.002 (6)
C22 0.068 (8) 0.038 (8) 0.040 (7) −0.010 (6) 0.004 (6) −0.008 (6)

Geometric parameters (Å, º)

I1—Cu1 2.5645 (16) C5—H5A 0.9500
I2—Cu2 2.5832 (14) C6—C7 1.443 (14)
Cu1—N4 1.980 (9) C6—H6A 0.9500
Cu1—N3 2.074 (9) C7—C8 1.365 (14)
Cu1—N2 2.078 (8) C8—C9 1.372 (15)
Cu2—N1 2.018 (8) C8—H8A 0.9500
Cu2—N6i 2.053 (9) C9—C10 1.371 (15)
Cu2—N5i 2.107 (8) C9—H9A 0.9500
N1—C5 1.350 (12) C10—C11 1.382 (14)
N1—C1 1.361 (13) C10—H10A 0.9500
N2—C6 1.291 (12) C11—H11A 0.9500
N2—C4 1.445 (12) C12—C13 1.415 (15)
N3—C11 1.341 (13) C12—H12A 0.9500
N3—C7 1.362 (12) C13—C14 1.362 (15)
N4—C12 1.323 (12) C13—H13A 0.9500
N4—C16 1.372 (13) C14—C15 1.390 (14)
N5—C17 1.270 (12) C14—H14A 0.9500
N5—C15 1.426 (13) C15—C16 1.381 (13)
N5—Cu2ii 2.107 (8) C16—H16A 0.9500
N6—C22 1.347 (14) C17—C18 1.439 (15)
N6—C18 1.376 (13) C17—H17A 0.9500
N6—Cu2ii 2.053 (9) C18—C19 1.382 (14)
C1—C2 1.376 (14) C19—C20 1.366 (16)
C1—H1A 0.9500 C19—H19A 0.9500
C2—C3 1.386 (14) C20—C21 1.413 (15)
C2—H2A 0.9500 C20—H20A 0.9500
C3—C4 1.358 (14) C21—C22 1.382 (16)
C3—H3A 0.9500 C21—H21A 0.9500
C4—C5 1.339 (13) C22—H22A 0.9500
N4—Cu1—N3 119.2 (4) N3—C7—C8 122.0 (10)
N4—Cu1—N2 125.5 (3) N3—C7—C6 114.4 (9)
N3—Cu1—N2 80.4 (3) C8—C7—C6 123.5 (10)
N4—Cu1—I1 105.3 (3) C7—C8—C9 120.7 (11)
N3—Cu1—I1 112.1 (2) C7—C8—H8A 119.6
N2—Cu1—I1 112.9 (2) C9—C8—H8A 119.6
N1—Cu2—N6i 126.9 (3) C10—C9—C8 118.5 (11)
N1—Cu2—N5i 113.9 (3) C10—C9—H9A 120.8
N6i—Cu2—N5i 79.8 (3) C8—C9—H9A 120.8
N1—Cu2—I2 109.9 (2) C9—C10—C11 118.2 (11)
N6i—Cu2—I2 106.7 (2) C9—C10—H10A 120.9
N5i—Cu2—I2 117.3 (2) C11—C10—H10A 120.9
C5—N1—C1 118.5 (9) N3—C11—C10 124.3 (11)
C5—N1—Cu2 121.7 (7) N3—C11—H11A 117.8
C1—N1—Cu2 119.7 (7) C10—C11—H11A 117.8
C6—N2—C4 122.4 (9) N4—C12—C13 123.7 (11)
C6—N2—Cu1 111.2 (7) N4—C12—H12A 118.2
C4—N2—Cu1 126.4 (6) C13—C12—H12A 118.2
C11—N3—C7 116.3 (9) C14—C13—C12 119.0 (10)
C11—N3—Cu1 131.4 (8) C14—C13—H13A 120.5
C7—N3—Cu1 112.3 (7) C12—C13—H13A 120.5
C12—N4—C16 116.4 (9) C13—C14—C15 118.5 (10)
C12—N4—Cu1 122.0 (8) C13—C14—H14A 120.8
C16—N4—Cu1 120.5 (6) C15—C14—H14A 120.8
C17—N5—C15 121.6 (9) C16—C15—C14 119.4 (11)
C17—N5—Cu2ii 111.3 (7) C16—C15—N5 114.6 (9)
C15—N5—Cu2ii 126.8 (6) C14—C15—N5 125.9 (9)
C22—N6—C18 117.7 (9) N4—C16—C15 122.9 (9)
C22—N6—Cu2ii 128.6 (7) N4—C16—H16A 118.5
C18—N6—Cu2ii 113.1 (7) C15—C16—H16A 118.5
N1—C1—C2 121.3 (10) N5—C17—C18 121.6 (10)
N1—C1—H1A 119.3 N5—C17—H17A 119.2
C2—C1—H1A 119.3 C18—C17—H17A 119.2
C1—C2—C3 118.2 (10) N6—C18—C19 121.5 (10)
C1—C2—H2A 120.9 N6—C18—C17 113.8 (9)
C3—C2—H2A 120.9 C19—C18—C17 124.7 (10)
C4—C3—C2 119.5 (10) C20—C19—C18 121.5 (11)
C4—C3—H3A 120.2 C20—C19—H19A 119.3
C2—C3—H3A 120.2 C18—C19—H19A 119.3
C5—C4—C3 120.5 (10) C19—C20—C21 116.8 (11)
C5—C4—N2 124.3 (9) C19—C20—H20A 121.6
C3—C4—N2 115.2 (9) C21—C20—H20A 121.6
C4—C5—N1 121.8 (9) C22—C21—C20 120.1 (11)
C4—C5—H5A 119.1 C22—C21—H21A 119.9
N1—C5—H5A 119.1 C20—C21—H21A 119.9
N2—C6—C7 121.3 (9) N6—C22—C21 122.4 (11)
N2—C6—H6A 119.4 N6—C22—H22A 118.8
C7—C6—H6A 119.4 C21—C22—H22A 118.8

Symmetry codes: (i) −x+5/2, y+1/2, −z+1/2; (ii) −x+5/2, y−1/2, −z+1/2.

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C22—H22A···I1iii 0.95 3.03 3.789 (12) 138
C20—H20A···I1iv 0.95 3.14 4.025 (12) 156
C17—H17A···I2v 0.95 3.16 4.011 (11) 149

Symmetry codes: (iii) x, y−1, z; (iv) −x+3, −y−1, −z+1; (v) x+1/2, −y−1/2, z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SU2480).

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/S1600536812037270/su2480sup1.cif

e-68-m1277-sup1.cif (28.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812037270/su2480Isup2.hkl

e-68-m1277-Isup2.hkl (270.1KB, hkl)

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


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