metal-organic compounds
Bis(4-amino-1-hexylpyridinium) bis(1,2-dicyanoethene-1,2-dithiolato)cuprate(II)
aDepartment of Applied Chemistry, College of Science, Nanjing University of Technology, No.5 Xinmofan Road, Nanjing, Nanjing 210009, People's Republic of China
*Correspondence e-mail: liuqi198721@163.com
The complete complex anion in the title salt, (C11H19N2)2[Cu(C4N2S2)2], has 2/m symmetry while the complete cation is generated by mirror symmetry with the non-H atoms of the alkyl chain lying on the plane. A square-planar geometry based on an S4 donor set is found in the anion; the Cu—S distance is 2.2663 (5) Å. In the crystal, intermolecular N—H⋯N hydrogen bonds link the ions into layers in the bc plane comprising alternating rows of cations and anions.
Related literature
For square-planar M[dithiolene]2 complexes acting as magnetic materials or showing nonlinear optical properties, see: Cassoux et al. (1991); Robertson & Cronin (2002).
Experimental
Crystal data
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Refinement
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Data collection: SMART (Siemens, 1996); cell SAINT (Siemens, 1996); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.
Supporting information
10.1107/S1600536811021611/tk2752sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811021611/tk2752Isup2.hkl
Disodium maleonitriledithiolate (468 mg, 2.5 mmol) and cupric nitrate trihydrate (302 mg, 1.25 mmol) were mixed under stirring in water (20 mL) at room temperature. Subsequently, a solution of 1-hexyl-4-aminopyridinium iodide (765 mg, 2.5 mmol) in water (10 mL) was added to the mixture. The brown precipitate that formed immediately was filtered off and washed with water. The crude product was recrystallized from acetone (20 mL) to give brown crystals. The crystals suitable for X-ray diffraction measurements were obtained by diffusing diethyl ether into the solution of the salt in acetone for 6 days.
The C-bound H atoms were geometrically placed (C—H = 0.93 or 0.96 Å) and refined as riding with Uiso(H) = 1.2-1.5Ueq(C). The N-bound H atom was refined freely.
Data collection: SMART (Siemens, 1996); cell
SAINT (Siemens, 1996); data reduction: SAINT (Siemens, 1996); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).(C11H19N2)2[Cu(C4N2S2)2] | F(000) = 734 |
Mr = 702.51 | Dx = 1.348 Mg m−3 |
Monoclinic, C2/m | Melting point = 430–432 K |
Hall symbol: -C 2y | Mo Kα radiation, λ = 0.71073 Å |
a = 13.3648 (9) Å | Cell parameters from 2059 reflections |
b = 10.0768 (4) Å | θ = 3.1–29.2° |
c = 13.8550 (8) Å | µ = 0.91 mm−1 |
β = 111.902 (8)° | T = 293 K |
V = 1731.24 (17) Å3 | Block, brown |
Z = 2 | 0.3 × 0.2 × 0.1 mm |
Siemens SMART CCD area-detector diffractometer | 1805 independent reflections |
Radiation source: fine-focus sealed tube | 1299 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.019 |
ϕ and ω scans | θmax = 26.0°, θmin = 3.1° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −12→16 |
Tmin = 0.939, Tmax = 1.000 | k = −11→12 |
4194 measured reflections | l = −17→16 |
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)] = 0.031 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.074 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.92 | w = 1/[σ2(Fo2) + (0.0411P)2] where P = (Fo2 + 2Fc2)/3 |
1805 reflections | (Δ/σ)max < 0.001 |
117 parameters | Δρmax = 0.22 e Å−3 |
0 restraints | Δρmin = −0.17 e Å−3 |
(C11H19N2)2[Cu(C4N2S2)2] | V = 1731.24 (17) Å3 |
Mr = 702.51 | Z = 2 |
Monoclinic, C2/m | Mo Kα radiation |
a = 13.3648 (9) Å | µ = 0.91 mm−1 |
b = 10.0768 (4) Å | T = 293 K |
c = 13.8550 (8) Å | 0.3 × 0.2 × 0.1 mm |
β = 111.902 (8)° |
Siemens SMART CCD area-detector diffractometer | 1805 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 1299 reflections with I > 2σ(I) |
Tmin = 0.939, Tmax = 1.000 | Rint = 0.019 |
4194 measured reflections |
R[F2 > 2σ(F2)] = 0.031 | 0 restraints |
wR(F2) = 0.074 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.92 | Δρmax = 0.22 e Å−3 |
1805 reflections | Δρmin = −0.17 e Å−3 |
117 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Cu1 | 0.0000 | 0.5000 | 0.0000 | 0.04510 (17) | |
S1 | 0.04362 (5) | 0.66007 (5) | 0.12376 (4) | 0.0623 (2) | |
N1 | 0.12555 (15) | 0.7075 (2) | 0.40284 (14) | 0.0721 (6) | |
N2 | 0.3513 (2) | 0.5000 | 0.5099 (2) | 0.0615 (8) | |
N3 | 0.39247 (19) | 0.5000 | 0.23171 (18) | 0.0536 (6) | |
C1 | 0.07750 (14) | 0.56692 (18) | 0.23653 (14) | 0.0445 (4) | |
C2 | 0.10516 (16) | 0.6424 (2) | 0.33068 (15) | 0.0507 (5) | |
C3 | 0.3637 (2) | 0.5000 | 0.4193 (2) | 0.0472 (7) | |
C4 | 0.37096 (16) | 0.38155 (19) | 0.36957 (15) | 0.0544 (5) | |
H4A | 0.3666 | 0.3005 | 0.3998 | 0.065* | |
C5 | 0.38435 (18) | 0.3850 (2) | 0.27783 (17) | 0.0586 (6) | |
H5A | 0.3881 | 0.3054 | 0.2454 | 0.070* | |
C6 | 0.4079 (3) | 0.5000 | 0.1312 (2) | 0.0678 (9) | |
H6A | 0.4487 | 0.4229 | 0.1280 | 0.081* | |
C7 | 0.3047 (3) | 0.5000 | 0.0398 (3) | 0.0810 (10) | |
H7A | 0.2635 | 0.4226 | 0.0414 | 0.097* | |
C8 | 0.3282 (3) | 0.5000 | −0.0612 (3) | 0.0819 (11) | |
H8A | 0.3740 | 0.4117 | −0.0657 | 0.098* | |
C9 | 0.2314 (3) | 0.5000 | −0.1571 (3) | 0.0917 (12) | |
H9A | 0.1892 | 0.4230 | −0.1569 | 0.110* | |
C10 | 0.2529 (4) | 0.5000 | −0.2572 (3) | 0.0930 (12) | |
H10A | 0.2950 | 0.4229 | −0.2577 | 0.112* | |
C11 | 0.1534 (3) | 0.5000 | −0.3517 (3) | 0.0931 (12) | |
H11A | 0.1716 | 0.5000 | −0.4125 | 0.140* | |
H11B | 0.1119 | 0.4222 | −0.3519 | 0.140* | |
H2A | 0.3461 (18) | 0.432 (2) | 0.5381 (16) | 0.075 (8)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cu1 | 0.0613 (3) | 0.0335 (3) | 0.0420 (3) | 0.000 | 0.0211 (2) | 0.000 |
S1 | 0.1042 (5) | 0.0323 (3) | 0.0463 (3) | 0.0005 (3) | 0.0235 (3) | 0.0001 (2) |
N1 | 0.0822 (14) | 0.0679 (13) | 0.0574 (11) | 0.0058 (11) | 0.0159 (10) | −0.0184 (10) |
N2 | 0.076 (2) | 0.0505 (19) | 0.0559 (16) | 0.000 | 0.0218 (15) | 0.000 |
N3 | 0.0594 (15) | 0.0435 (14) | 0.0669 (15) | 0.000 | 0.0340 (13) | 0.000 |
C1 | 0.0492 (11) | 0.0407 (10) | 0.0423 (10) | 0.0004 (9) | 0.0155 (9) | −0.0020 (8) |
C2 | 0.0538 (13) | 0.0454 (11) | 0.0486 (11) | 0.0054 (10) | 0.0143 (10) | 0.0004 (10) |
C3 | 0.0386 (16) | 0.0423 (17) | 0.0544 (17) | 0.000 | 0.0100 (14) | 0.000 |
C4 | 0.0649 (14) | 0.0343 (11) | 0.0652 (14) | 0.0001 (10) | 0.0257 (12) | 0.0042 (10) |
C5 | 0.0692 (15) | 0.0352 (11) | 0.0769 (15) | 0.0012 (10) | 0.0338 (13) | −0.0054 (11) |
C6 | 0.080 (2) | 0.058 (2) | 0.083 (2) | 0.000 | 0.051 (2) | 0.000 |
C7 | 0.090 (3) | 0.096 (3) | 0.070 (2) | 0.000 | 0.045 (2) | 0.000 |
C8 | 0.092 (3) | 0.087 (3) | 0.079 (2) | 0.000 | 0.046 (2) | 0.000 |
C9 | 0.108 (3) | 0.096 (3) | 0.084 (3) | 0.000 | 0.051 (3) | 0.000 |
C10 | 0.114 (3) | 0.099 (3) | 0.080 (3) | 0.000 | 0.053 (3) | 0.000 |
C11 | 0.122 (3) | 0.073 (3) | 0.097 (3) | 0.000 | 0.055 (3) | 0.000 |
Cu1—S1i | 2.2663 (5) | C4—C5 | 1.349 (3) |
Cu1—S1 | 2.2663 (5) | C4—H4A | 0.9300 |
Cu1—S1ii | 2.2663 (5) | C5—H5A | 0.9300 |
Cu1—S1iii | 2.2663 (5) | C6—C7 | 1.483 (4) |
S1—C1 | 1.7319 (19) | C6—H6A | 0.9600 |
N1—C2 | 1.141 (2) | C7—C8 | 1.545 (4) |
N2—C3 | 1.327 (4) | C7—H7A | 0.9600 |
N2—H2A | 0.80 (2) | C8—C9 | 1.468 (5) |
N3—C5 | 1.347 (2) | C8—H8A | 1.0943 |
N3—C5iii | 1.347 (2) | C9—C10 | 1.519 (4) |
N3—C6 | 1.482 (3) | C9—H9A | 0.9601 |
C1—C1iii | 1.349 (4) | C10—C11 | 1.478 (5) |
C1—C2 | 1.434 (3) | C10—H10A | 0.9600 |
C3—C4 | 1.399 (2) | C11—H11A | 0.9600 |
C3—C4iii | 1.399 (2) | C11—H11B | 0.9600 |
S1i—Cu1—S1 | 180.00 (2) | N3—C5—C4 | 122.1 (2) |
S1i—Cu1—S1ii | 90.75 (3) | N3—C5—H5A | 118.9 |
S1—Cu1—S1ii | 89.25 (3) | C4—C5—H5A | 118.9 |
S1i—Cu1—S1iii | 89.25 (3) | N3—C6—C7 | 113.0 (2) |
S1—Cu1—S1iii | 90.75 (3) | N3—C6—H6A | 108.9 |
S1ii—Cu1—S1iii | 180.00 (3) | C7—C6—H6A | 108.9 |
C1—S1—Cu1 | 101.76 (6) | C6—C7—C8 | 109.6 (3) |
C3—N2—H2A | 121.7 (17) | C6—C7—H7A | 109.8 |
C5—N3—C5iii | 118.7 (2) | C8—C7—H7A | 109.5 |
C5—N3—C6 | 120.65 (12) | C9—C8—C7 | 114.3 (3) |
C5iii—N3—C6 | 120.65 (12) | C9—C8—H8A | 105.7 |
C1iii—C1—C2 | 122.02 (11) | C7—C8—H8A | 111.0 |
C1iii—C1—S1 | 122.82 (6) | C8—C9—C10 | 115.0 (3) |
C2—C1—S1 | 115.16 (14) | C8—C9—H9A | 108.5 |
N1—C2—C1 | 176.9 (2) | C10—C9—H9A | 108.3 |
N2—C3—C4 | 121.46 (13) | C11—C10—C9 | 113.2 (3) |
N2—C3—C4iii | 121.46 (13) | C11—C10—H10A | 109.3 |
C4—C3—C4iii | 117.1 (3) | C9—C10—H10A | 108.5 |
C5—C4—C3 | 120.0 (2) | C10—C11—H11A | 109.8 |
C5—C4—H4A | 120.0 | C10—C11—H11B | 109.3 |
C3—C4—H4A | 120.0 | H11A—C11—H11B | 109.5 |
Symmetry codes: (i) −x, −y+1, −z; (ii) −x, y, −z; (iii) x, −y+1, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···N1iv | 0.81 (2) | 2.39 (2) | 3.157 (2) | 160 (2) |
Symmetry code: (iv) −x+1/2, y−1/2, −z+1. |
Experimental details
Crystal data | |
Chemical formula | (C11H19N2)2[Cu(C4N2S2)2] |
Mr | 702.51 |
Crystal system, space group | Monoclinic, C2/m |
Temperature (K) | 293 |
a, b, c (Å) | 13.3648 (9), 10.0768 (4), 13.8550 (8) |
β (°) | 111.902 (8) |
V (Å3) | 1731.24 (17) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.91 |
Crystal size (mm) | 0.3 × 0.2 × 0.1 |
Data collection | |
Diffractometer | Siemens SMART CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.939, 1.000 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4194, 1805, 1299 |
Rint | 0.019 |
(sin θ/λ)max (Å−1) | 0.617 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.031, 0.074, 0.92 |
No. of reflections | 1805 |
No. of parameters | 117 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.22, −0.17 |
Computer programs: SMART (Siemens, 1996), SAINT (Siemens, 1996), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···N1i | 0.81 (2) | 2.39 (2) | 3.157 (2) | 160 (2) |
Symmetry code: (i) −x+1/2, y−1/2, −z+1. |
Acknowledgements
The authors thank the Science and Technology Department of Jiangsu Province, People's Republic of China, for support.
References
Cassoux, P., Valade, L., Kobayashi, H., Kobayashi, A., Clark, R. A. & Underhill, A. E. (1991). Coord. Chem. Rev. 110, 115–160. CrossRef CAS Web of Science Google Scholar
Robertson, N. & Cronin, L. (2002). Coord. Chem. Rev. 227, 93–127. Web of Science CrossRef CAS Google Scholar
Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Siemens (1996). SMART and SAINT. Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA. Google Scholar
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Square-planar M[dithiolene]2 complexes have attracted extensive interest in the areas of conducting and magnetic materials, dyes, non-linear optics and catalysis (Robertson et al., 2002; Cassoux et al., 1991). Herein, we report the crystal structure of the title compound, Fig.1.
The [Cu(mnt)2]2- dianion is located about a site of symmetry 2/m. The 1-hexyl-4-aminopyridinium cation lies on a mirror plane whereby the non-H atoms of the alkyl chain lie on the plane which bisects the 1,4 atoms of the benzene ring.
In the crystal structure, intermolecular N—H···N hydrogen bonds (Table 1) link the cations and anions to form a layer in the bc plane comprising alternating cations and anions.