Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805038237/ci6658sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536805038237/ci6658Isup2.hkl |
CCDC reference: 293853
Data collection: CAD-4 Software (Enraf–Nonius, 1989); cell refinement: CAD-4 Software; data reduction: local programs; program(s) used to solve structure: SHELXS86 (Sheldrick, 1986); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 in WinGX (Farrugia, 1999); software used to prepare material for publication: SHELXL97.
[Zn(CH3O3S)2] | F(000) = 512 |
Mr = 255.56 | Dx = 2.360 Mg m−3 |
Monoclinic, Cc | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: C -2yc | Cell parameters from 25 reflections |
a = 8.332 (5) Å | θ = 9–12° |
b = 10.797 (10) Å | µ = 3.97 mm−1 |
c = 8.939 (2) Å | T = 295 K |
β = 116.56 (3)° | Prism, colourless |
V = 719.3 (8) Å3 | 0.12 × 0.10 × 0.10 mm |
Z = 4 |
Enraf-Nonius CAD-4 diffractometer | Rint = 0.000 |
Radiation source: fine-focus sealed tube, Enraf-Nonius X-ray Generator | θmax = 25.3°, θmin = 3.3° |
Graphite monochromator | h = −10→8 |
ω scan | k = 0→12 |
653 measured reflections | l = 0→10 |
653 independent reflections | 3 standard reflections every 10800 min |
652 reflections with I > 2σ(I) | intensity decay: 5.0% |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.028 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.074 | w = 1/[σ2(Fo2) + (0.0173P)2 + 8.9338P] where P = (Fo2 + 2Fc2)/3 |
S = 1.15 | (Δ/σ)max = 0.013 |
653 reflections | Δρmax = 0.67 e Å−3 |
108 parameters | Δρmin = −0.79 e Å−3 |
4 restraints | Absolute structure: Flack (1983) |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.02 (3) |
Experimental. Several crystals have been tested, all showing extreme mosaicity and heavily broadened, multiple peaks in the ω axis. Eventually, a (nearly) single-crystal specimen was found, which allowed a satisfactory unit cell determination, although with far from ideal e.s.d.'s. Of the several data collections performed with increasing ω scan width, the best results, reported hereafter, were obtained by the omega scan method with a rather unconventional scan angle of Δω=6.0 + 0.35tanθ°, 150 s per reflection (see the caption of Figure 3 for a further comment). Data collection performed with an Enraf–Nonius CAD-4 four-circle diffractometer equipped with a scintillation counter, sealed X-ray tube with Mo Kα radiation, graphite monochromator. Lattice parameters obtained by the indexing and least-squares refinement procedures of the setting angles of 25 strong reflections randomly distributed in the 9<θ<12° range. No absorption correction was applied. Powder diffraction data (Cu Kα radiation) were collected on the bulk sample, in order to test sample purity, crystal mosaicity and to confirm the unit cell proposed above. The relevant comments are reported in the caption to Fig.3. |
Geometry. All e.s.d.'s 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. |
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 | 0.00150 (9) | 0.14440 (7) | 0.55754 (9) | 0.02306 (17) | |
S1 | 0.0926 (2) | 0.34050 (17) | 0.8285 (2) | 0.0264 (4) | |
S2 | 0.2006 (2) | 0.02396 (17) | 0.3735 (2) | 0.0259 (4) | |
O1 | 0.1286 (7) | 0.3027 (5) | 0.6808 (6) | 0.0276 (12) | |
O2 | 0.2496 (6) | 0.2991 (5) | 0.9910 (6) | 0.0284 (12) | |
O3 | 0.3197 (6) | 0.5296 (5) | 0.9125 (6) | 0.0323 (14) | |
C1 | 0.1364 (9) | 0.5070 (8) | 0.8371 (11) | 0.034 (2) | |
H1A | 0.0827 | 0.5408 | 0.7246 | 0.040* | |
H1B | 0.0821 | 0.5479 | 0.8999 | 0.040* | |
O4 | 0.2039 (6) | 0.0495 (5) | 0.5419 (6) | 0.0307 (13) | |
O5 | 0.0352 (7) | −0.0570 (5) | 0.2720 (6) | 0.0281 (12) | |
O6 | −0.0117 (6) | 0.2178 (5) | 0.3204 (6) | 0.0302 (13) | |
C2 | 0.1220 (11) | 0.1736 (7) | 0.2768 (10) | 0.0343 (18) | |
H2A | 0.2213 | 0.2316 | 0.3147 | 0.041* | |
H2B | 0.0727 | 0.1662 | 0.1562 | 0.041* | |
H3 | 0.336 (3) | 0.518 (9) | 0.829 (2) | 0.07 (4)* | |
H6 | −0.113 (3) | 0.207 (7) | 0.244 (5) | 0.04 (3)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Zn | 0.0225 (3) | 0.0221 (3) | 0.0231 (3) | 0.0007 (4) | 0.0089 (2) | 0.0005 (4) |
S1 | 0.0196 (7) | 0.0254 (9) | 0.0325 (9) | −0.0014 (7) | 0.0101 (6) | −0.0049 (7) |
S2 | 0.0218 (7) | 0.0280 (9) | 0.0272 (8) | −0.0009 (7) | 0.0105 (6) | −0.0051 (7) |
O1 | 0.029 (2) | 0.025 (2) | 0.026 (2) | −0.005 (2) | 0.0094 (19) | −0.008 (2) |
O2 | 0.028 (2) | 0.029 (3) | 0.026 (2) | −0.004 (2) | 0.0103 (19) | −0.001 (2) |
O3 | 0.029 (3) | 0.031 (3) | 0.036 (3) | −0.003 (2) | 0.013 (2) | −0.003 (2) |
C1 | 0.024 (4) | 0.022 (3) | 0.047 (4) | 0.005 (3) | 0.009 (3) | −0.001 (3) |
O4 | 0.026 (2) | 0.036 (3) | 0.028 (2) | 0.001 (2) | 0.010 (2) | −0.007 (2) |
O5 | 0.027 (2) | 0.031 (3) | 0.025 (2) | −0.008 (2) | 0.0104 (19) | −0.006 (2) |
O6 | 0.028 (2) | 0.025 (3) | 0.037 (3) | 0.000 (2) | 0.015 (2) | 0.004 (2) |
C2 | 0.039 (4) | 0.028 (4) | 0.043 (4) | −0.003 (3) | 0.025 (3) | −0.001 (3) |
Zn—O2i | 2.004 (5) | O2—Zniii | 2.004 (5) |
Zn—O4 | 2.031 (5) | O3—C1 | 1.388 (9) |
Zn—O5ii | 2.040 (5) | O3—Zniii | 2.398 (6) |
Zn—O1 | 2.053 (5) | O3—H3 | 0.821 (11) |
Zn—O6 | 2.219 (5) | C1—H1A | 0.9700 |
Zn—O3i | 2.398 (6) | C1—H1B | 0.9700 |
S1—O2 | 1.524 (5) | O5—Zniv | 2.040 (5) |
S1—O1 | 1.535 (6) | O6—C2 | 1.418 (10) |
S1—C1 | 1.829 (9) | O6—H6 | 0.820 (10) |
S2—O4 | 1.518 (5) | C2—H2A | 0.9700 |
S2—O5 | 1.539 (5) | C2—H2B | 0.9700 |
S2—C2 | 1.812 (8) | ||
O2i—Zn—O4 | 157.7 (2) | S1—O2—Zniii | 122.2 (3) |
O2i—Zn—O5ii | 96.0 (2) | C1—O3—Zniii | 114.6 (5) |
O4—Zn—O5ii | 93.5 (2) | C1—O3—H3 | 97 (2) |
O2i—Zn—O1 | 97.3 (2) | Zniii—O3—H3 | 93 (5) |
O4—Zn—O1 | 102.3 (2) | O3—C1—S1 | 110.4 (5) |
O5ii—Zn—O1 | 93.4 (2) | O3—C1—H1A | 109.6 |
O2i—Zn—O6 | 90.6 (2) | S1—C1—H1A | 109.6 |
O4—Zn—O6 | 78.6 (2) | O3—C1—H1B | 109.6 |
O5ii—Zn—O6 | 171.8 (2) | S1—C1—H1B | 109.6 |
O1—Zn—O6 | 90.5 (2) | H1A—C1—H1B | 108.1 |
O2i—Zn—O3i | 75.7 (2) | S2—O4—Zn | 120.8 (3) |
O4—Zn—O3i | 84.9 (2) | S2—O5—Zniv | 121.9 (3) |
O5ii—Zn—O3i | 86.2 (2) | C2—O6—Zn | 115.7 (4) |
O1—Zn—O3i | 172.9 (2) | C2—O6—H6 | 111 (4) |
O6—Zn—O3i | 90.79 (19) | Zn—O6—H6 | 110 (5) |
O2—S1—O1 | 109.1 (3) | O6—C2—S2 | 109.2 (5) |
O2—S1—C1 | 100.3 (3) | O6—C2—H2A | 109.8 |
O1—S1—C1 | 100.6 (4) | S2—C2—H2A | 109.8 |
O4—S2—O5 | 107.6 (3) | O6—C2—H2B | 109.8 |
O4—S2—C2 | 98.9 (4) | S2—C2—H2B | 109.8 |
O5—S2—C2 | 100.8 (3) | H2A—C2—H2B | 108.3 |
S1—O1—Zn | 115.5 (3) |
Symmetry codes: (i) x−1/2, −y+1/2, z−1/2; (ii) x, −y, z+1/2; (iii) x+1/2, −y+1/2, z+1/2; (iv) x, −y, z−1/2. |