Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805020192/lh6460sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536805020192/lh6460Isup2.hkl |
CCDC reference: 282533
Key indicators
- Single-crystal X-ray study
- T = 220 K
- Mean (C-C)= 0.002 Å
- R factor = 0.036
- wR factor = 0.107
- Data-to-parameter ratio = 16.0
checkCIF/PLATON results
No syntax errors found No errors found in this datablock
Data collection: SMART (Bruker, 1999); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: UdMX (local program; Author and date?).
C14H14S2 | F(000) = 260 |
Mr = 246.37 | Dx = 1.325 Mg m−3 |
Monoclinic, P21/c | Cu Kα radiation, λ = 1.54178 Å |
Hall symbol: -P 2ybc | Cell parameters from 4189 reflections |
a = 5.8654 (1) Å | θ = 3.2–72.7° |
b = 7.5638 (1) Å | µ = 3.63 mm−1 |
c = 14.0472 (2) Å | T = 220 K |
β = 97.600 (1)° | Needle-like, colorless |
V = 617.73 (2) Å3 | 0.32 × 0.06 × 0.05 mm |
Z = 2 |
Bruker SMART 2000 area-detector diffractometer | 1184 independent reflections |
Radiation source: X-ray sealed tube | 1099 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.026 |
Detector resolution: 5.5 pixels mm-1 | θmax = 72.7°, θmin = 6.4° |
ω scans | h = −5→6 |
Absorption correction: multi-scan (SADABS; Sheldrick,1996) | k = −9→9 |
Tmin = 0.375, Tmax = 0.825 | l = −17→16 |
5018 measured reflections |
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)] = 0.036 | H-atom parameters constrained |
wR(F2) = 0.107 | w = 1/[σ2(Fo2) + (0.0794P)2 + 0.1086P] where P = (Fo2 + 2Fc2)/3 |
S = 1.03 | (Δ/σ)max < 0.001 |
1184 reflections | Δρmax = 0.23 e Å−3 |
74 parameters | Δρmin = −0.23 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.018 (2) |
Experimental. X-ray crystallographic data for I were collected from a single-crystal sample, which was mounted on a loop fiber. Data were collected using a Bruker Platform diffractometer, equipped with a Bruker SMART 2 K Charged-Coupled Device (CCD) Area Detector using the program SMART and normal focus sealed tube source graphite monochromated Cu—Kα radiation. The crystal-to-detector distance was 4.908 cm, and the data collection was carried out in 512 x 512 pixel mode, utilizing 4 x 4 pixel binning. The initial unit-cell parameters were determined by a least-squares fit of the angular setting of strong reflections, collected by a 9.0 degree scan in 30 frames over four different parts of the reciprocal space (120 frames total). One complete sphere of data was collected, to better than 0.8 Å resolution. Upon completion of the data collection, the first 101 frames were recollected in order to improve the decay correction analysis. |
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 | ||
S1 | 0.66983 (6) | 0.07504 (6) | 0.41416 (3) | 0.0399 (2) | |
C1 | 0.7328 (3) | 0.05351 (17) | 0.29514 (11) | 0.0307 (4) | |
C4 | 0.7900 (3) | 0.0336 (2) | 0.10185 (12) | 0.0453 (4) | |
H4 | 0.8092 | 0.0265 | 0.0366 | 0.054* | |
C6 | 0.9244 (3) | −0.0306 (2) | 0.26748 (11) | 0.0374 (4) | |
H6 | 1.0358 | −0.0806 | 0.3140 | 0.045* | |
C5 | 0.9501 (3) | −0.0404 (2) | 0.17069 (12) | 0.0417 (4) | |
H5 | 1.0788 | −0.0985 | 0.1520 | 0.050* | |
C2 | 0.5714 (3) | 0.1287 (2) | 0.22523 (12) | 0.0403 (4) | |
H2 | 0.4421 | 0.1866 | 0.2433 | 0.048* | |
C3 | 0.6005 (3) | 0.1185 (2) | 0.12942 (13) | 0.0477 (5) | |
H3 | 0.4908 | 0.1697 | 0.0826 | 0.057* | |
C7 | 0.8901 (3) | −0.0522 (2) | 0.48666 (12) | 0.0375 (4) | |
H7A | 0.8315 | −0.0905 | 0.5455 | 0.045* | |
H7B | 0.9244 | −0.1582 | 0.4511 | 0.045* |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0319 (3) | 0.0569 (3) | 0.0319 (3) | 0.00648 (14) | 0.00862 (18) | 0.00177 (14) |
C1 | 0.0303 (8) | 0.0315 (7) | 0.0304 (7) | −0.0021 (5) | 0.0041 (6) | 0.0009 (5) |
C4 | 0.0596 (11) | 0.0477 (9) | 0.0287 (8) | −0.0031 (8) | 0.0067 (7) | −0.0018 (7) |
C6 | 0.0368 (9) | 0.0417 (8) | 0.0335 (8) | 0.0068 (6) | 0.0038 (6) | 0.0025 (6) |
C5 | 0.0472 (10) | 0.0416 (8) | 0.0385 (9) | 0.0053 (7) | 0.0138 (7) | −0.0027 (6) |
C2 | 0.0349 (9) | 0.0446 (9) | 0.0406 (9) | 0.0056 (6) | 0.0015 (6) | 0.0020 (7) |
C3 | 0.0496 (11) | 0.0540 (10) | 0.0369 (9) | 0.0046 (8) | −0.0044 (7) | 0.0062 (7) |
C7 | 0.0354 (9) | 0.0461 (8) | 0.0317 (7) | −0.0028 (6) | 0.0072 (6) | 0.0070 (6) |
S1—C1 | 1.7667 (15) | C6—H6 | 0.94 |
S1—C7 | 1.8123 (16) | C5—H5 | 0.94 |
C1—C6 | 1.391 (2) | C2—C3 | 1.381 (2) |
C1—C2 | 1.392 (2) | C2—H2 | 0.94 |
C4—C5 | 1.375 (2) | C3—H3 | 0.94 |
C4—C3 | 1.383 (3) | C7—C7i | 1.515 (3) |
C4—H4 | 0.94 | C7—H7A | 0.98 |
C6—C5 | 1.390 (2) | C7—H7B | 0.98 |
C1—S1—C7 | 105.08 (7) | C3—C2—C1 | 120.32 (16) |
C6—C1—C2 | 119.27 (15) | C3—C2—H2 | 119.8 |
C6—C1—S1 | 125.75 (12) | C1—C2—H2 | 119.8 |
C2—C1—S1 | 114.98 (12) | C2—C3—C4 | 120.41 (16) |
C5—C4—C3 | 119.46 (16) | C2—C3—H3 | 119.8 |
C5—C4—H4 | 120.3 | C4—C3—H3 | 119.8 |
C3—C4—H4 | 120.3 | C7i—C7—S1 | 112.48 (14) |
C5—C6—C1 | 119.60 (14) | C7i—C7—H7A | 109.1 |
C5—C6—H6 | 120.2 | S1—C7—H7A | 109.1 |
C1—C6—H6 | 120.2 | C7i—C7—H7B | 109.1 |
C4—C5—C6 | 120.94 (16) | S1—C7—H7B | 109.1 |
C4—C5—H5 | 119.5 | H7A—C7—H7B | 107.8 |
C6—C5—H5 | 119.5 | ||
C7—S1—C1—C6 | −5.28 (15) | C6—C1—C2—C3 | 0.5 (2) |
C7—S1—C1—C2 | 174.47 (12) | S1—C1—C2—C3 | −179.25 (13) |
C2—C1—C6—C5 | −0.9 (2) | C1—C2—C3—C4 | 0.0 (3) |
S1—C1—C6—C5 | 178.87 (12) | C5—C4—C3—C2 | −0.2 (3) |
C3—C4—C5—C6 | −0.2 (3) | C1—S1—C7—C7i | 83.90 (17) |
C1—C6—C5—C4 | 0.7 (3) |
Symmetry code: (i) −x+2, −y, −z+1. |