metal-organic compounds
Poly[bis(μ2-pyrimidine-κ2N:N′)bis(selenocyanato-κN)zinc]
aInstitut für Anorganische Chemie, Christian-Albrechts-Universität Kiel, Max-Eyth Strasse 2, D-24098 Kiel, Germany
*Correspondence e-mail: jboeckmann@ac.uni-kiel.de
The 2(C4H4N2)2]n, consists of one Zn2+ cation located on a special position with 2/m, one selenocyanate anion on a mirror plane and one pyrimidine ligand on a twofold rotation axis. The zinc cation is coordinated by six N atoms of four pyrimidine ligands and two N-bonded selenocyanate anions in mutually trans orientations within a slightly distorted octahedral coordination environment. The Zn atoms are μ-1,3-bridged via the pyrimidine ligands into a polymeric layer extending parallel to (100).
of the title compound, [Zn(NCSe)Related literature
For isotypic structures with different divalent transition metals and thiocyanate ligands, see: Bhosekar et al. (2010); Lloret et al. (1998, 1999); Wriedt et al. (2009); Wriedt & Näther (2010).
Experimental
Crystal data
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Refinement
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Data collection: X-AREA (Stoe & Cie, 2008); cell X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP in SHELXTL (Sheldrick, 2008) and DIAMOND (Brandenburg, 2011); software used to prepare material for publication: SHELXL97.
Supporting information
10.1107/S1600536811023129/wm2498sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811023129/wm2498Isup2.hkl
The title compound was prepared by the reaction of 74.35 mg Zn(NO3)2 (0.25 mmol), 64.8 mg KSeCN (0.45 mmol) and 78.8 µL pyrimidine (0.50 mmol) in 1.00 ml water at RT in a closed 3 ml snap cap vial. After one week colourless needles of the title compound were obtained.
All H atoms were located in difference map but were positioned with idealized geometry and were refined isotropically with Ueq(H) = 1.2 Ueq(C) of the parent atom using a riding model with C—H = 0.95 Å.
Data collection: X-AREA (Stoe & Cie, 2008); cell
X-AREA (Stoe & Cie, 2008); data reduction: X-AREA (Stoe & Cie, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP in SHELXTL (Sheldrick, 2008) and DIAMOND (Brandenburg, 2011); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).[Zn(NCSe)2(C4H4N2)2] | Z = 4 |
Mr = 435.51 | F(000) = 832 |
Orthorhombic, Cmca | Dx = 2.094 Mg m−3 |
Hall symbol: -C 2bc 2 | Mo Kα radiation, λ = 0.71073 Å |
a = 9.4025 (9) Å | µ = 7.04 mm−1 |
b = 16.7146 (10) Å | T = 200 K |
c = 8.7886 (5) Å | Needle, colourless |
V = 1381.21 (17) Å3 | 0.28 × 0.22 × 0.16 mm |
Stoe IPDS-1 diffractometer | 657 independent reflections |
Radiation source: fine-focus sealed tube | 638 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.055 |
ϕ scans | θmax = 25.5°, θmin = 3.4° |
Absorption correction: numerical (X-SHAPE and X-RED32; Stoe & Cie, 2008) | h = −11→11 |
Tmin = 0.165, Tmax = 0.321 | k = −19→17 |
4502 measured reflections | l = −9→10 |
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)] = 0.029 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.073 | H-atom parameters constrained |
S = 1.15 | w = 1/[σ2(Fo2) + (0.0424P)2 + 2.801P] where P = (Fo2 + 2Fc2)/3 |
657 reflections | (Δ/σ)max = 0.001 |
51 parameters | Δρmax = 0.40 e Å−3 |
0 restraints | Δρmin = −0.81 e Å−3 |
[Zn(NCSe)2(C4H4N2)2] | V = 1381.21 (17) Å3 |
Mr = 435.51 | Z = 4 |
Orthorhombic, Cmca | Mo Kα radiation |
a = 9.4025 (9) Å | µ = 7.04 mm−1 |
b = 16.7146 (10) Å | T = 200 K |
c = 8.7886 (5) Å | 0.28 × 0.22 × 0.16 mm |
Stoe IPDS-1 diffractometer | 657 independent reflections |
Absorption correction: numerical (X-SHAPE and X-RED32; Stoe & Cie, 2008) | 638 reflections with I > 2σ(I) |
Tmin = 0.165, Tmax = 0.321 | Rint = 0.055 |
4502 measured reflections |
R[F2 > 2σ(F2)] = 0.029 | 0 restraints |
wR(F2) = 0.073 | H-atom parameters constrained |
S = 1.15 | Δρmax = 0.40 e Å−3 |
657 reflections | Δρmin = −0.81 e Å−3 |
51 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 | ||
Zn1 | 0.0000 | 0.5000 | 0.5000 | 0.0172 (2) | |
N1 | 0.0000 | 0.40527 (19) | 0.6452 (4) | 0.0220 (7) | |
C1 | 0.0000 | 0.3787 (2) | 0.7666 (4) | 0.0164 (7) | |
Se1 | 0.0000 | 0.34051 (3) | 0.95337 (5) | 0.0329 (2) | |
N11 | 0.1681 (2) | 0.56159 (13) | 0.6471 (2) | 0.0191 (5) | |
C11 | 0.2500 | 0.5254 (2) | 0.7500 | 0.0190 (7) | |
H11 | 0.2500 | 0.4685 | 0.7500 | 0.023* | |
C12 | 0.1740 (3) | 0.64196 (17) | 0.6445 (3) | 0.0216 (6) | |
H12 | 0.1240 | 0.6699 | 0.5671 | 0.026* | |
C13 | 0.2500 | 0.6849 (2) | 0.7500 | 0.0227 (8) | |
H13 | 0.2500 | 0.7417 | 0.7500 | 0.027* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Zn1 | 0.0157 (3) | 0.0225 (4) | 0.0133 (4) | 0.000 | 0.000 | 0.0033 (2) |
N1 | 0.0240 (16) | 0.0238 (17) | 0.0182 (16) | 0.000 | 0.000 | 0.0017 (13) |
C1 | 0.0123 (15) | 0.0190 (17) | 0.0178 (18) | 0.000 | 0.000 | −0.0030 (14) |
Se1 | 0.0494 (4) | 0.0337 (3) | 0.0156 (3) | 0.000 | 0.000 | 0.00690 (16) |
N11 | 0.0147 (11) | 0.0240 (12) | 0.0186 (11) | −0.0001 (8) | −0.0012 (9) | 0.0001 (8) |
C11 | 0.0113 (15) | 0.0247 (19) | 0.0210 (18) | 0.000 | −0.0013 (14) | 0.000 |
C12 | 0.0186 (13) | 0.0262 (14) | 0.0198 (13) | 0.0001 (11) | −0.0012 (11) | 0.0026 (10) |
C13 | 0.0192 (19) | 0.0212 (19) | 0.028 (2) | 0.000 | −0.0011 (16) | 0.000 |
Zn1—N1i | 2.033 (3) | N11—C11 | 1.333 (3) |
Zn1—N1 | 2.033 (3) | N11—C12 | 1.345 (4) |
Zn1—N11 | 2.287 (2) | C11—N11iv | 1.333 (3) |
Zn1—N11i | 2.287 (2) | C11—H11 | 0.9500 |
Zn1—N11ii | 2.287 (2) | C12—C13 | 1.373 (3) |
Zn1—N11iii | 2.287 (2) | C12—H12 | 0.9500 |
N1—C1 | 1.156 (5) | C13—C12iv | 1.373 (3) |
C1—Se1 | 1.761 (4) | C13—H13 | 0.9500 |
N1i—Zn1—N1 | 180.00 (11) | C1—N1—Zn1 | 151.5 (3) |
N1i—Zn1—N11 | 90.23 (9) | N1—C1—Se1 | 178.6 (3) |
N1—Zn1—N11 | 89.77 (9) | C11—N11—C12 | 116.2 (2) |
N1i—Zn1—N11i | 89.77 (9) | C11—N11—Zn1 | 125.3 (2) |
N1—Zn1—N11i | 90.23 (9) | C12—N11—Zn1 | 117.95 (17) |
N11—Zn1—N11i | 180.0 | N11iv—C11—N11 | 126.0 (4) |
N1i—Zn1—N11ii | 90.23 (9) | N11iv—C11—H11 | 117.0 |
N1—Zn1—N11ii | 89.77 (9) | N11—C11—H11 | 117.0 |
N11—Zn1—N11ii | 87.46 (11) | N11—C12—C13 | 122.2 (3) |
N11i—Zn1—N11ii | 92.54 (11) | N11—C12—H12 | 118.9 |
N1i—Zn1—N11iii | 89.77 (9) | C13—C12—H12 | 118.9 |
N1—Zn1—N11iii | 90.23 (9) | C12—C13—C12iv | 117.0 (4) |
N11—Zn1—N11iii | 92.54 (11) | C12—C13—H13 | 121.5 |
N11i—Zn1—N11iii | 87.45 (11) | C12iv—C13—H13 | 121.5 |
N11ii—Zn1—N11iii | 180.0 |
Symmetry codes: (i) −x, −y+1, −z+1; (ii) −x, y, z; (iii) x, −y+1, −z+1; (iv) −x+1/2, y, −z+3/2. |
Experimental details
Crystal data | |
Chemical formula | [Zn(NCSe)2(C4H4N2)2] |
Mr | 435.51 |
Crystal system, space group | Orthorhombic, Cmca |
Temperature (K) | 200 |
a, b, c (Å) | 9.4025 (9), 16.7146 (10), 8.7886 (5) |
V (Å3) | 1381.21 (17) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 7.04 |
Crystal size (mm) | 0.28 × 0.22 × 0.16 |
Data collection | |
Diffractometer | Stoe IPDS1 diffractometer |
Absorption correction | Numerical (X-SHAPE and X-RED32; Stoe & Cie, 2008) |
Tmin, Tmax | 0.165, 0.321 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4502, 657, 638 |
Rint | 0.055 |
(sin θ/λ)max (Å−1) | 0.606 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.029, 0.073, 1.15 |
No. of reflections | 657 |
No. of parameters | 51 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.40, −0.81 |
Computer programs: X-AREA (Stoe & Cie, 2008), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), XP in SHELXTL (Sheldrick, 2008) and DIAMOND (Brandenburg, 2011).
Acknowledgements
We gratefully acknowledge financial support by the DFG (project number NA 720/3–1) and the State of Schleswig–Holstein. We thank Professor Dr Wolfgang Bensch for the opportunity to use his experimental facilities. Special thanks go to Inke Jess for her support of the single-crystal measurements.
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
The structure determination of the title compound was performed as part of a project on the synthesis of new coordination polymers based on transition metal thiocyanates and the investigations of their thermal degradation products (Bhosekar et al., 2010; Wriedt et al., 2009; Wriedt & Näther, 2010)). Within this project we have reacted zinc(II) nitrate with potassium selenocyanate and pyrimidine in water, which leads to a single phase formation of the title compound, poly[bis(selenocyanato-κN)-bis(µ2-pyrimidine-N,N')zinc].
The title compound is isotypic with its zinc, manganese(II), iron(II), cobalt(II) and nickel(II) thiocyanato coordination polymer analogues (Bhosekar et al., 2010; Lloret et al., 1998; Lloret et al., 1999; Wriedt et al., 2009; Wriedt & Näther, 2010). In the crystal structure the zinc atoms are surrounded by six N-atoms of four pyrimidine ligands and two N-bonded selenocyanato anions in mutually trans orientations in a slightly distorted octahedral geometry (Fig. 1). The pyrimidine ligands bridge the metal cations forming layers which extend along the ac plane (Fig. 2). These layers are stacked in the direction of the crystallographic b axis. The Zn—Zn intralayer separation amounts to 6.4352 (4) Å, whereas the shortest Zn—Zn interlayer separation is 9.4422 (5) Å.