Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807031716/tk2172sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807031716/tk2172Isup2.hkl |
CCDC reference: 657519
Key indicators
- Single-crystal X-ray study
- T = 295 K
- Mean (C-C) = 0.013 Å
- R factor = 0.055
- wR factor = 0.129
- Data-to-parameter ratio = 13.4
checkCIF/PLATON results
No syntax errors found
Alert level A PLAT027_ALERT_3_A _diffrn_reflns_theta_full (too) Low ............ 24.60 Deg.
Author Response: Data was collected to 25.0 degrees. No data was observed between 24.6 and 25.00 degrees. |
Alert level C THETM01_ALERT_3_C The value of sine(theta_max)/wavelength is less than 0.590 Calculated sin(theta_max)/wavelength = 0.5857 PLAT023_ALERT_3_C Resolution (too) Low [sin(th)/Lambda < 0.6]..... 24.60 Deg. PLAT180_ALERT_3_C Check Cell Rounding: # of Values Ending with 0 = 3 PLAT341_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang ... 13
Alert level G PLAT794_ALERT_5_G Check Predicted Bond Valency for Zn (2) 1.89
1 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 4 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 5 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check
A solution of quinoxaline (1.4 g, 10 mmol) in absolute ethanol (10 ml) was added to a solution of ZnBr2 (2.3 g, 10 mmol) in absolute ethanol (10 ml) yielding a pale-orange solution. The flask was wrapped in aluminium foil and allowed to evaporate under a slow flow of argon. After 12 h, light-brown crystals of (I) were collected, washed with cold ethanol and allowed to air dry yielding 1.62 g (67%). IR (KBr, cm-1): 1504 s, 1466m, 1383w, 1360 s, 1215m, 1147m, 1131m, 1046 s, 965 s,876m, 772 s, 766 s.
We are interested in the study of low-dimensional coordination polymers and their magnetic properties. Our previous work on two copper(II) complexes of quinoxaline (quinox) showed that Cu(quinox)X2 complexes (X = Cl, Br) form structural and magnetic ladders. The rungs of the ladder are formed by bridging halide ions and the rails formed by bridging quinoxaline molecules (Lindroos and Lumme, 1990; Landee et al., 2003). A diamagnetic analogue of these materials would be useful for related experiments and we previously prepared the chloride analogue of (I) (Markowitz et al., 2006). It resulted in a tetrahedral complex which was not a suitable analogue so the bromo complex was prepared and is reported here. Reaction of ZnBr2 with quinoxaline gave Zn(quinox)Br2, even in the presence of excess ZnBr2.
The ZnII complex (I, Fig. 1) is a distorted tetrahedron with a mean angle at Zn of 120.6 (2)° (Turnbull et al., 2005). The Br1—Zn—Br2 and N1—Zn1—N11 angles are both expanded and correspond with the chloride complex, unlike the pyridine and quinoline analogues (Markowitz et al. 2006 and references therein). The two quinoxaline ligands are nearly planar. The mean deviation from planarity for the N1 containing quinoxaline is 0.013 (12) Å and the angle between the normals to the two component rings is 1.0 (1)°; the comparable values for the N11 ring are 0.019 (17) Å and 1.4 (1)°; both are identical with the chloride complex, within experimental error. The bond lengths and angles within the quinoxaline rings are the same within experimental error and agree with those values seen in chloride analogue and similar mono-coordinated complexes such as [Cu(quinox)2(H2O)3](ClO4)2 (Lumme et al., 1988) and [Cu(quinox)2(C2N3)2] (Luo et al., 2004).
Complex (I) packs in the lattice such that π-stacking is observed between inversion related quinoxaline rings, generating layers parallel to the bc-plane. The ring overlap occurs between both the nitrogen-containing rings and the non-nitrogen containing rings. The interplanar distance between the stacked N1-rings is 3.30 (1)Å and the displacement angle (defined as the angle between the mean plane of the ring and the line connecting the ring centroids) is 19.1 (1)° while the values for the carbocyclic rings containing C6 are 3.41 (1)Å and 13.9 (1)°, respectively. For the stacked N11 rings the distance is 3.25 (2)Å with a displacement angle of 19.3 (1)° while the carbocyclic C16 rings are separated by 3.51 (1) Å and 6.0 (1)°. Both show that the carbocyclic rings are slightly further apart, but show greater overlap compared to the heterocyclic rings.
For related literature, see: Landee et al. (2003); Lindroos & Lumme (1990); Lumme et al. (1988); Luo et al. (2004); Markowitz et al. (2006); Turnbull et al. (2005).
Data collection: XSCANS (Siemens, 1992); cell refinement: XSCANS; data reduction: SHELXTL (Siemens, 1990); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Fig. 1. Molecular structure of (I), showing atom labelling scheme and 50% atom displacement ellipsoids. |
[ZnBr2(C8H6N2)2] | Z = 2 |
Mr = 485.49 | F(000) = 472 |
Triclinic, P1 | Dx = 1.911 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 8.2527 (11) Å | Cell parameters from 31 reflections |
b = 8.6670 (9) Å | θ = 3.3–15.6° |
c = 12.4651 (17) Å | µ = 6.19 mm−1 |
α = 80.067 (13)° | T = 295 K |
β = 86.260 (12)° | Parallelpiped, colourless |
γ = 73.94 (1)° | 0.2 × 0.15 × 0.12 mm |
V = 843.80 (18) Å3 |
Bruker P4 diffractometer | 1703 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.082 |
Graphite monochromator | θmax = 24.6°, θmin = 2.5° |
ω scans | h = −9→1 |
Absorption correction: ψ scan (SHELXTL; Siemens, 1990) | k = −10→9 |
Tmin = 0.363, Tmax = 0.476 | l = −14→14 |
3382 measured reflections | 3 standard reflections every 97 reflections |
2781 independent reflections | intensity decay: 2.1% |
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)] = 0.055 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.129 | H-atom parameters constrained |
S = 1.01 | w = 1/[σ2(Fo2) + (0.0507P)2 + 0.6175P] where P = (Fo2 + 2Fc2)/3 |
2781 reflections | (Δ/σ)max < 0.001 |
208 parameters | Δρmax = 0.68 e Å−3 |
0 restraints | Δρmin = −0.53 e Å−3 |
[ZnBr2(C8H6N2)2] | γ = 73.94 (1)° |
Mr = 485.49 | V = 843.80 (18) Å3 |
Triclinic, P1 | Z = 2 |
a = 8.2527 (11) Å | Mo Kα radiation |
b = 8.6670 (9) Å | µ = 6.19 mm−1 |
c = 12.4651 (17) Å | T = 295 K |
α = 80.067 (13)° | 0.2 × 0.15 × 0.12 mm |
β = 86.260 (12)° |
Bruker P4 diffractometer | 1703 reflections with I > 2σ(I) |
Absorption correction: ψ scan (SHELXTL; Siemens, 1990) | Rint = 0.082 |
Tmin = 0.363, Tmax = 0.476 | 3 standard reflections every 97 reflections |
3382 measured reflections | intensity decay: 2.1% |
2781 independent reflections |
R[F2 > 2σ(F2)] = 0.055 | 0 restraints |
wR(F2) = 0.129 | H-atom parameters constrained |
S = 1.01 | Δρmax = 0.68 e Å−3 |
2781 reflections | Δρmin = −0.53 e Å−3 |
208 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 | ||
Zn | 0.34064 (11) | 0.66777 (11) | 0.75037 (8) | 0.0414 (3) | |
Br1 | 0.48802 (12) | 0.39624 (11) | 0.73519 (9) | 0.0618 (3) | |
Br2 | 0.48360 (11) | 0.86374 (11) | 0.76689 (8) | 0.0560 (3) | |
N1 | 0.2157 (8) | 0.7537 (7) | 0.6045 (5) | 0.0396 (16) | |
C2 | 0.2853 (11) | 0.8412 (10) | 0.5272 (7) | 0.048 (2) | |
H2A | 0.3835 | 0.8650 | 0.5427 | 0.058* | |
C3 | 0.2186 (13) | 0.8992 (11) | 0.4236 (8) | 0.057 (2) | |
H3A | 0.2736 | 0.9606 | 0.3733 | 0.068* | |
N4 | 0.0816 (11) | 0.8707 (9) | 0.3944 (6) | 0.058 (2) | |
C5 | 0.0051 (11) | 0.7813 (10) | 0.4701 (8) | 0.049 (2) | |
C6 | −0.1435 (11) | 0.7466 (12) | 0.4439 (8) | 0.057 (3) | |
H6A | −0.1895 | 0.7856 | 0.3751 | 0.069* | |
C7 | −0.2190 (12) | 0.6551 (12) | 0.5204 (9) | 0.060 (3) | |
H7A | −0.3178 | 0.6336 | 0.5035 | 0.072* | |
C8 | −0.1515 (11) | 0.5936 (11) | 0.6230 (8) | 0.056 (2) | |
H8A | −0.2055 | 0.5305 | 0.6728 | 0.067* | |
C9 | −0.0086 (10) | 0.6229 (10) | 0.6527 (7) | 0.047 (2) | |
H9A | 0.0359 | 0.5801 | 0.7215 | 0.057* | |
C10 | 0.0702 (9) | 0.7198 (9) | 0.5763 (7) | 0.038 (2) | |
N11 | 0.2023 (8) | 0.6495 (8) | 0.8954 (5) | 0.0393 (16) | |
C12 | 0.2657 (11) | 0.5273 (11) | 0.9726 (8) | 0.051 (2) | |
H12A | 0.3641 | 0.4501 | 0.9577 | 0.061* | |
C13 | 0.1906 (13) | 0.5087 (12) | 1.0769 (8) | 0.060 (3) | |
H13A | 0.2438 | 0.4226 | 1.1294 | 0.071* | |
N14 | 0.0498 (11) | 0.6075 (10) | 1.1023 (6) | 0.059 (2) | |
C15 | −0.0207 (11) | 0.7367 (10) | 1.0254 (7) | 0.046 (2) | |
C16 | −0.1749 (11) | 0.8485 (12) | 1.0501 (8) | 0.054 (2) | |
H16A | −0.2280 | 0.8339 | 1.1178 | 0.065* | |
C17 | −0.2415 (12) | 0.9746 (12) | 0.9740 (8) | 0.057 (2) | |
H17A | −0.3427 | 1.0474 | 0.9899 | 0.068* | |
C18 | −0.1666 (11) | 1.0026 (11) | 0.8715 (7) | 0.051 (2) | |
H18A | −0.2165 | 1.0938 | 0.8216 | 0.062* | |
C19 | −0.0202 (10) | 0.8964 (10) | 0.8445 (7) | 0.044 (2) | |
H19A | 0.0291 | 0.9138 | 0.7759 | 0.052* | |
C20 | 0.0556 (9) | 0.7603 (9) | 0.9212 (6) | 0.0368 (19) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Zn | 0.0367 (6) | 0.0398 (6) | 0.0459 (7) | −0.0105 (4) | −0.0020 (5) | −0.0017 (5) |
Br1 | 0.0525 (6) | 0.0409 (5) | 0.0840 (8) | −0.0006 (4) | −0.0017 (5) | −0.0081 (5) |
Br2 | 0.0524 (6) | 0.0567 (6) | 0.0657 (7) | −0.0249 (5) | 0.0031 (5) | −0.0132 (5) |
N1 | 0.031 (4) | 0.035 (4) | 0.046 (4) | −0.003 (3) | 0.003 (3) | 0.001 (3) |
C2 | 0.044 (5) | 0.045 (5) | 0.051 (6) | −0.011 (4) | 0.013 (4) | −0.001 (5) |
C3 | 0.072 (7) | 0.054 (6) | 0.042 (6) | −0.021 (5) | 0.014 (5) | 0.001 (5) |
N4 | 0.084 (6) | 0.043 (4) | 0.040 (5) | −0.010 (4) | −0.001 (4) | −0.001 (4) |
C5 | 0.052 (5) | 0.040 (5) | 0.050 (6) | 0.000 (4) | −0.006 (5) | −0.014 (5) |
C6 | 0.047 (6) | 0.066 (6) | 0.055 (7) | 0.000 (5) | −0.013 (5) | −0.020 (5) |
C7 | 0.043 (5) | 0.061 (6) | 0.080 (8) | −0.008 (5) | −0.010 (5) | −0.030 (6) |
C8 | 0.052 (6) | 0.067 (6) | 0.053 (7) | −0.021 (5) | 0.006 (5) | −0.017 (5) |
C9 | 0.047 (5) | 0.051 (5) | 0.046 (6) | −0.014 (4) | 0.002 (4) | −0.011 (4) |
C10 | 0.032 (5) | 0.034 (4) | 0.044 (6) | 0.000 (4) | 0.001 (4) | −0.010 (4) |
N11 | 0.036 (4) | 0.041 (4) | 0.040 (4) | −0.014 (3) | −0.007 (3) | 0.006 (3) |
C12 | 0.044 (5) | 0.050 (5) | 0.057 (7) | −0.013 (4) | −0.011 (5) | −0.002 (5) |
C13 | 0.068 (7) | 0.060 (6) | 0.050 (7) | −0.027 (6) | −0.018 (5) | 0.017 (5) |
N14 | 0.068 (6) | 0.066 (5) | 0.047 (5) | −0.031 (5) | −0.004 (4) | 0.002 (4) |
C15 | 0.051 (5) | 0.051 (5) | 0.040 (5) | −0.023 (5) | −0.011 (4) | −0.001 (4) |
C16 | 0.054 (6) | 0.069 (6) | 0.044 (6) | −0.023 (5) | 0.009 (5) | −0.012 (5) |
C17 | 0.049 (5) | 0.065 (6) | 0.060 (7) | −0.009 (5) | −0.002 (5) | −0.031 (6) |
C18 | 0.054 (6) | 0.055 (6) | 0.043 (6) | −0.004 (5) | −0.010 (5) | −0.016 (5) |
C19 | 0.041 (5) | 0.045 (5) | 0.044 (5) | −0.015 (4) | 0.001 (4) | 0.002 (4) |
C20 | 0.030 (4) | 0.046 (5) | 0.035 (5) | −0.018 (4) | −0.003 (4) | 0.002 (4) |
Zn—N1 | 2.068 (7) | C9—C10 | 1.406 (11) |
Zn—N11 | 2.080 (6) | C9—H9A | 0.9300 |
Zn—Br2 | 2.3623 (12) | N11—C12 | 1.315 (10) |
Zn—Br1 | 2.3650 (13) | N11—C20 | 1.380 (10) |
N1—C2 | 1.323 (10) | C12—C13 | 1.406 (13) |
N1—C10 | 1.392 (9) | C12—H12A | 0.9300 |
C2—C3 | 1.391 (13) | C13—N14 | 1.296 (12) |
C2—H2A | 0.9300 | C13—H13A | 0.9300 |
C3—N4 | 1.308 (11) | N14—C15 | 1.361 (11) |
C3—H3A | 0.9300 | C15—C20 | 1.414 (11) |
N4—C5 | 1.353 (11) | C15—C16 | 1.422 (12) |
C5—C6 | 1.412 (12) | C16—C17 | 1.333 (13) |
C5—C10 | 1.421 (12) | C16—H16A | 0.9300 |
C6—C7 | 1.364 (13) | C17—C18 | 1.395 (12) |
C6—H6A | 0.9300 | C17—H17A | 0.9300 |
C7—C8 | 1.386 (13) | C18—C19 | 1.363 (11) |
C7—H7A | 0.9300 | C18—H18A | 0.9300 |
C8—C9 | 1.360 (11) | C19—C20 | 1.406 (11) |
C8—H8A | 0.9300 | C19—H19A | 0.9300 |
N1—Zn—N11 | 119.5 (2) | N1—C10—C9 | 119.6 (7) |
N1—Zn—Br2 | 104.56 (18) | N1—C10—C5 | 119.4 (7) |
N11—Zn—Br2 | 103.95 (18) | C9—C10—C5 | 121.0 (8) |
N1—Zn—Br1 | 103.70 (18) | C12—N11—C20 | 116.5 (7) |
N11—Zn—Br1 | 104.58 (18) | C12—N11—Zn | 117.3 (6) |
Br2—Zn—Br1 | 121.69 (5) | C20—N11—Zn | 125.9 (5) |
C2—N1—C10 | 116.0 (7) | N11—C12—C13 | 122.7 (9) |
C2—N1—Zn | 117.5 (6) | N11—C12—H12A | 118.7 |
C10—N1—Zn | 126.4 (5) | C13—C12—H12A | 118.7 |
N1—C2—C3 | 123.2 (9) | N14—C13—C12 | 122.2 (9) |
N1—C2—H2A | 118.4 | N14—C13—H13A | 118.9 |
C3—C2—H2A | 118.4 | C12—C13—H13A | 118.9 |
N4—C3—C2 | 122.6 (8) | C13—N14—C15 | 117.5 (8) |
N4—C3—H3A | 118.7 | N14—C15—C20 | 121.1 (8) |
C2—C3—H3A | 118.7 | N14—C15—C16 | 119.3 (9) |
C3—N4—C5 | 116.9 (8) | C20—C15—C16 | 119.6 (8) |
N4—C5—C6 | 119.8 (9) | C17—C16—C15 | 118.4 (8) |
N4—C5—C10 | 122.0 (8) | C17—C16—H16A | 120.8 |
C6—C5—C10 | 118.3 (8) | C15—C16—H16A | 120.8 |
C7—C6—C5 | 119.4 (9) | C16—C17—C18 | 123.1 (9) |
C7—C6—H6A | 120.3 | C16—C17—H17A | 118.4 |
C5—C6—H6A | 120.3 | C18—C17—H17A | 118.4 |
C6—C7—C8 | 121.4 (9) | C19—C18—C17 | 120.0 (9) |
C6—C7—H7A | 119.3 | C19—C18—H18A | 120.0 |
C8—C7—H7A | 119.3 | C17—C18—H18A | 120.0 |
C9—C8—C7 | 121.8 (9) | C18—C19—C20 | 119.6 (8) |
C9—C8—H8A | 119.1 | C18—C19—H19A | 120.2 |
C7—C8—H8A | 119.1 | C20—C19—H19A | 120.2 |
C8—C9—C10 | 118.2 (9) | N11—C20—C19 | 120.7 (7) |
C8—C9—H9A | 120.9 | N11—C20—C15 | 119.9 (7) |
C10—C9—H9A | 120.9 | C19—C20—C15 | 119.4 (8) |
N11—Zn—N1—C2 | 145.7 (6) | N1—Zn—N11—C12 | 145.1 (6) |
Br2—Zn—N1—C2 | 30.0 (6) | Br2—Zn—N11—C12 | −98.9 (6) |
Br1—Zn—N1—C2 | −98.5 (6) | Br1—Zn—N11—C12 | 29.7 (6) |
N11—Zn—N1—C10 | −38.9 (7) | N1—Zn—N11—C20 | −39.9 (7) |
Br2—Zn—N1—C10 | −154.6 (5) | Br2—Zn—N11—C20 | 76.2 (6) |
Br1—Zn—N1—C10 | 76.9 (6) | Br1—Zn—N11—C20 | −155.2 (6) |
C10—N1—C2—C3 | 0.8 (11) | C20—N11—C12—C13 | −0.4 (11) |
Zn—N1—C2—C3 | 176.7 (7) | Zn—N11—C12—C13 | 175.1 (6) |
N1—C2—C3—N4 | −0.4 (14) | N11—C12—C13—N14 | 2.9 (14) |
C2—C3—N4—C5 | 0.2 (13) | C12—C13—N14—C15 | −3.1 (13) |
C3—N4—C5—C6 | 179.8 (8) | C13—N14—C15—C20 | 1.1 (12) |
C3—N4—C5—C10 | −0.4 (12) | C13—N14—C15—C16 | −179.7 (8) |
N4—C5—C6—C7 | 179.5 (9) | N14—C15—C16—C17 | 179.7 (8) |
C10—C5—C6—C7 | −0.3 (12) | C20—C15—C16—C17 | −1.1 (13) |
C5—C6—C7—C8 | −0.9 (14) | C15—C16—C17—C18 | −0.4 (14) |
C6—C7—C8—C9 | 0.8 (14) | C16—C17—C18—C19 | 1.5 (14) |
C7—C8—C9—C10 | 0.6 (13) | C17—C18—C19—C20 | −1.0 (12) |
C2—N1—C10—C9 | 177.9 (8) | C12—N11—C20—C19 | 179.0 (7) |
Zn—N1—C10—C9 | 2.4 (10) | Zn—N11—C20—C19 | 3.9 (10) |
C2—N1—C10—C5 | −1.0 (10) | C12—N11—C20—C15 | −1.6 (10) |
Zn—N1—C10—C5 | −176.5 (5) | Zn—N11—C20—C15 | −176.7 (5) |
C8—C9—C10—N1 | 179.3 (7) | C18—C19—C20—N11 | 178.9 (7) |
C8—C9—C10—C5 | −1.9 (12) | C18—C19—C20—C15 | −0.5 (11) |
N4—C5—C10—N1 | 0.8 (12) | N14—C15—C20—N11 | 1.3 (12) |
C6—C5—C10—N1 | −179.4 (7) | C16—C15—C20—N11 | −177.9 (7) |
N4—C5—C10—C9 | −178.1 (7) | N14—C15—C20—C19 | −179.3 (7) |
C6—C5—C10—C9 | 1.8 (11) | C16—C15—C20—C19 | 1.5 (12) |
Experimental details
Crystal data | |
Chemical formula | [ZnBr2(C8H6N2)2] |
Mr | 485.49 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 295 |
a, b, c (Å) | 8.2527 (11), 8.6670 (9), 12.4651 (17) |
α, β, γ (°) | 80.067 (13), 86.260 (12), 73.94 (1) |
V (Å3) | 843.80 (18) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 6.19 |
Crystal size (mm) | 0.2 × 0.15 × 0.12 |
Data collection | |
Diffractometer | Bruker P4 |
Absorption correction | ψ scan (SHELXTL; Siemens, 1990) |
Tmin, Tmax | 0.363, 0.476 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3382, 2781, 1703 |
Rint | 0.082 |
(sin θ/λ)max (Å−1) | 0.586 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.055, 0.129, 1.01 |
No. of reflections | 2781 |
No. of parameters | 208 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.68, −0.53 |
Computer programs: XSCANS (Siemens, 1992), XSCANS, SHELXTL (Siemens, 1990), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL.
We are interested in the study of low-dimensional coordination polymers and their magnetic properties. Our previous work on two copper(II) complexes of quinoxaline (quinox) showed that Cu(quinox)X2 complexes (X = Cl, Br) form structural and magnetic ladders. The rungs of the ladder are formed by bridging halide ions and the rails formed by bridging quinoxaline molecules (Lindroos and Lumme, 1990; Landee et al., 2003). A diamagnetic analogue of these materials would be useful for related experiments and we previously prepared the chloride analogue of (I) (Markowitz et al., 2006). It resulted in a tetrahedral complex which was not a suitable analogue so the bromo complex was prepared and is reported here. Reaction of ZnBr2 with quinoxaline gave Zn(quinox)Br2, even in the presence of excess ZnBr2.
The ZnII complex (I, Fig. 1) is a distorted tetrahedron with a mean angle at Zn of 120.6 (2)° (Turnbull et al., 2005). The Br1—Zn—Br2 and N1—Zn1—N11 angles are both expanded and correspond with the chloride complex, unlike the pyridine and quinoline analogues (Markowitz et al. 2006 and references therein). The two quinoxaline ligands are nearly planar. The mean deviation from planarity for the N1 containing quinoxaline is 0.013 (12) Å and the angle between the normals to the two component rings is 1.0 (1)°; the comparable values for the N11 ring are 0.019 (17) Å and 1.4 (1)°; both are identical with the chloride complex, within experimental error. The bond lengths and angles within the quinoxaline rings are the same within experimental error and agree with those values seen in chloride analogue and similar mono-coordinated complexes such as [Cu(quinox)2(H2O)3](ClO4)2 (Lumme et al., 1988) and [Cu(quinox)2(C2N3)2] (Luo et al., 2004).
Complex (I) packs in the lattice such that π-stacking is observed between inversion related quinoxaline rings, generating layers parallel to the bc-plane. The ring overlap occurs between both the nitrogen-containing rings and the non-nitrogen containing rings. The interplanar distance between the stacked N1-rings is 3.30 (1)Å and the displacement angle (defined as the angle between the mean plane of the ring and the line connecting the ring centroids) is 19.1 (1)° while the values for the carbocyclic rings containing C6 are 3.41 (1)Å and 13.9 (1)°, respectively. For the stacked N11 rings the distance is 3.25 (2)Å with a displacement angle of 19.3 (1)° while the carbocyclic C16 rings are separated by 3.51 (1) Å and 6.0 (1)°. Both show that the carbocyclic rings are slightly further apart, but show greater overlap compared to the heterocyclic rings.