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Compound 6,6′-([1]benzothieno[3,2-b][1]benzothio­phene-2,7-diyl)bis­(butan-1-ol) (BTBT-C4OH) displays a continuous type 0 first-order isosymmetric phase transition at 200 K which is accompanied by a continuous change of the thermal expansion along the b axis from positive to negative. The equivalent isotropic atomic displacement parameters for all non-hydrogen atoms as well as all the eigenvalues of the anisotropic atomic displacement tensor show discontinuous behavior at the phase transition. The eigenvalues of the translational tensor in a rigid-body description of the molecule are all discontinuous at the phase transition, but the librational eigenvalues are discontinuous only in their temperature derivative. BTBT-C4OH displays a similar type of quasi-supercritical phase transition as bis(hydroxyhexyl)[1]benzothieno[3,2-b][1]benzothiophene (BTBT-C6OH), despite the difference in molecular packing and the very large difference in thermal expansion magnitudes.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520620007702/bm5126sup1.cif
Contains datablocks global, I, A110, A120, A130, A140, A150, A160, A170, A180, A190, A200, A210, A220, A230, A240, A250, A260, A270, A280, A290, A300

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520620007702/bm5126Isup2.hkl
Contains datablock I

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520620007702/bm5126sup3.pdf
Tables S1 and S2. Figures S1-S14

CCDC references: 2008258; 2012245; 2012246; 2012247; 2012248; 2012249; 2012250; 2012251; 2012252; 2012253; 2012254; 2012255; 2012256; 2012257; 2012258; 2012259; 2012260; 2012261; 2012262; 2012263; 2012264

Computing details top

Data collection: Local Elettra software for A110, A120, A130, A140, A150, A160, A170, A180, A190, A200, A210, A220, A230, A240, A250, A260, A270, A280, A290, A300. Cell refinement: XDS (Kabsch, 2010) for A110, A120, A130, A140, A150, A160, A170, A180, A190, A200, A210, A220, A230, A240, A250, A260, A270, A280, A290, A300. Data reduction: XDS (Kabsch, 2010)) for A110, A120, A130, A140, A150, A160, A170, A180, A190, A200, A210, A220, A230, A240, A250, A260, A270, A280, A290, A300. Program(s) used to solve structure: Superflip (Palatinus and Chapuis, 2007 for A110, A120, A130, A140, A150, A160, A170, A180, A190, A200, A210, A220, A230, A240, A250, A260, A270, A280, A290, A300. Program(s) used to refine structure: SHELXL2018/3 (Sheldrick, 2018) for A110, A120, A130, A140, A150, A160, A170, A180, A190, A200, A210, A220, A230, A240, A250, A260, A270, A280, A290, A300.

(I) top
Crystal data top
C22H24O2S2β = 106.988 (3)°
Mr = 384.56V = 935.24 (5) Å3
Monoclinic, p121/c1Z = 2.0
Hall symbol: -p 2ybcDx = 1.365 Mg m3
a = 13.4387 (4) ŵ = 0.25 mm1
b = 5.09342 (10) ÅStick, colourless
c = 14.2867 (4) Å0.5 × 0.2 × 0.1 mm
Data collection top
2897 independent reflectionsk =
2897 reflections with F > 0 & F/u(F) > 3.0 & |F_calc| > 103l =
h =
Refinement top
Least-squares matrix: full72 constraints
R[F2 > 2σ(F2)] = 0.030Hydrogen site location: HAR
wR(F2) = 0.029Only H-atom coordinates refined
S = 2.58Weighting scheme based on measured s.u.'s w = 1/σ(F)
2897 reflections(Δ/σ)max = 0.001
154 parametersΔρmax = 0.42 e Å3
0 restraintsΔρmin = 0.19 e Å3
Special details top

Refinement. . If constraints were applied they are defined by zero eigenvalues of the least-squares hessian, see the value of _refine_ls_SVD_threshold

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.647325 (17)0.32314 (4)0.537855 (15)0.02239 (12)
C20.64910 (7)0.55467 (16)0.62878 (6)0.0202 (4)
C30.55405 (6)0.69162 (16)0.61177 (6)0.0193 (4)
C40.48065 (6)0.59765 (16)0.52316 (6)0.0198 (4)
C50.54449 (7)0.88766 (17)0.67753 (6)0.0232 (4)
H50.4723 (8)0.9956 (19)0.6653 (7)0.027903 (1)*
C60.62900 (7)0.94065 (17)0.75831 (6)0.0233 (4)
H60.6228 (8)1.103 (2)0.8096 (7)0.028603 (1)*
C70.72378 (7)0.80264 (17)0.77628 (6)0.0215 (4)
C80.73354 (7)0.60776 (18)0.71101 (6)0.0226 (4)
H80.8023 (7)0.5077 (19)0.7252 (7)0.027314 (1)*
C90.81196 (7)0.86099 (18)0.86716 (6)0.0235 (4)
H9A0.8045 (8)1.0589 (19)0.8937 (7)0.028860 (1)*
H9B0.8864 (8)0.8645 (18)0.8516 (7)0.028860 (1)*
C100.81803 (8)0.66231 (18)0.94848 (6)0.0250 (5)
H10A0.8320 (8)0.470 (2)0.9206 (8)0.030570 (1)*
H10B0.7439 (8)0.6643 (19)0.9611 (7)0.030570 (1)*
C110.90223 (7)0.72552 (17)1.04372 (6)0.0228 (4)
H11A0.9774 (8)0.7461 (19)1.0320 (7)0.027961 (1)*
H11B0.8864 (8)0.9071 (19)1.0714 (7)0.027961 (1)*
C120.91161 (7)0.51262 (18)1.11944 (6)0.0244 (4)
H12A0.8398 (7)0.4893 (19)1.1358 (7)0.030085 (1)*
H12B0.9294 (7)0.3234 (19)1.0913 (7)0.030085 (1)*
O130.99092 (5)0.57593 (13)1.20706 (4)0.0276 (3)
H131.0025 (10)0.419 (3)1.2490 (9)0.041965 (1)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.02104 (10)0.02602 (13)0.01892 (12)0.00299 (8)0.00397 (8)0.00490 (9)
C20.0214 (4)0.0227 (4)0.0160 (4)0.0002 (3)0.0049 (3)0.0020 (3)
C30.0208 (4)0.0211 (4)0.0164 (4)0.0006 (3)0.0061 (3)0.0024 (3)
C40.0203 (4)0.0221 (4)0.0170 (4)0.0009 (3)0.0058 (3)0.0030 (3)
C50.0242 (4)0.0255 (4)0.0191 (4)0.0008 (3)0.0051 (3)0.0053 (3)
C60.0260 (4)0.0248 (4)0.0182 (4)0.0014 (3)0.0048 (3)0.0045 (3)
C70.0242 (4)0.0239 (4)0.0148 (4)0.0037 (3)0.0031 (3)0.0015 (3)
C80.0209 (4)0.0262 (4)0.0191 (4)0.0003 (3)0.0032 (3)0.0029 (3)
C90.0263 (4)0.0243 (4)0.0172 (4)0.0054 (3)0.0020 (3)0.0006 (3)
C100.0318 (5)0.0212 (4)0.0178 (4)0.0050 (4)0.0005 (3)0.0006 (3)
C110.0288 (4)0.0195 (4)0.0169 (4)0.0032 (3)0.0016 (3)0.0018 (3)
C120.0309 (5)0.0210 (4)0.0183 (4)0.0014 (3)0.0024 (4)0.0005 (3)
O130.0329 (4)0.0267 (4)0.0187 (3)0.0008 (3)0.0006 (3)0.0015 (3)
Geometric parameters (Å, º) top
S1—C21.7495 (8)C11—C121.5107 (12)
O13—C121.4238 (10)C5—H51.084 (10)
O13—H130.985 (13)C6—H61.124 (10)
C2—C31.4128 (11)C8—H81.022 (9)
C2—C81.4007 (11)C9—H9A1.092 (10)
C3—C41.4405 (11)C9—H9B1.086 (10)
C3—C51.4024 (11)C10—H10A1.095 (10)
C5—C61.3887 (11)C10—H10B1.064 (10)
C6—C71.4112 (12)C11—H11A1.077 (10)
C7—C81.3940 (12)C11—H11B1.052 (9)
C7—C91.5097 (12)C12—H12A1.063 (10)
C9—C101.5249 (12)C12—H12B1.097 (10)
C10—C111.5283 (12)
S1—C2—C3112.93 (6)C6—C5—H5120.8 (5)
S1—C2—C8125.79 (7)C7—C6—H6118.9 (5)
O13—C12—C11110.57 (7)C7—C8—H8118.6 (5)
O13—C12—H12A109.1 (5)C7—C9—H9A110.6 (5)
O13—C12—H12B109.5 (5)C7—C9—H9B111.4 (5)
C12—O13—H13107.2 (7)C9—C10—H10A107.1 (5)
C2—C3—C4109.85 (7)C9—C10—H10B106.2 (5)
C2—C3—C5119.44 (7)C10—C9—H9A109.8 (5)
C2—C8—C7119.14 (8)C10—C9—H9B108.6 (5)
C3—C2—C8121.28 (7)C10—C11—H11A111.5 (5)
C3—C5—C6118.84 (8)C10—C11—H11B110.0 (5)
C4—C3—C5130.70 (8)C11—C10—H10A110.6 (5)
C5—C6—C7122.00 (8)C11—C10—H10B109.5 (5)
C6—C7—C8119.29 (8)C11—C12—H12A110.2 (5)
C6—C7—C9119.89 (8)C11—C12—H12B110.4 (5)
C7—C9—C10112.23 (7)C12—C11—H11A107.2 (5)
C8—C7—C9120.79 (8)C12—C11—H11B110.2 (5)
C9—C10—C11113.54 (7)H9A—C9—H9B103.8 (7)
C10—C11—C12111.81 (7)H10A—C10—H10B109.8 (7)
C2—C8—H8122.3 (5)H11A—C11—H11B106.0 (7)
C3—C5—H5120.4 (5)H12A—C12—H12B107.0 (7)
C5—C6—H6119.1 (5)
(A110) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.377 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.438 (3) ÅCell parameters from 7090 reflections
b = 5.061 (1) Åθ = 2.5–25.0°
c = 14.262 (1) ŵ = 0.29 mm1
β = 106.973 (15)°T = 110 K
V = 927.7 (3) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.025
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8303 measured reflectionsh = 1919
2748 independent reflectionsk = 66
2488 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.039H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.109 w = 1/[σ2(Fo2) + (0.0546P)2 + 0.561P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max = 0.001
2748 reflectionsΔρmax = 0.95 e Å3
121 parametersΔρmin = 0.43 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.003 (2)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64732 (2)0.32338 (7)0.53732 (2)0.02323 (12)
C20.64913 (10)0.5558 (3)0.62860 (9)0.0208 (2)
C30.55401 (10)0.6922 (3)0.61188 (9)0.0205 (2)
C40.48088 (10)0.5974 (3)0.52338 (9)0.0205 (2)
C50.54471 (10)0.8887 (3)0.67775 (9)0.0237 (3)
H50.4815530.9841690.6673870.028*
C60.62896 (10)0.9416 (3)0.75822 (9)0.0244 (3)
H60.6227421.0751830.8029840.029*
C70.72359 (10)0.8039 (3)0.77586 (9)0.0221 (3)
C80.73353 (10)0.6092 (3)0.71059 (9)0.0230 (3)
H80.7967540.5136680.7215220.028*
C90.81195 (11)0.8624 (3)0.86665 (9)0.0237 (3)
H9A0.8024761.0414430.8906830.028*
H9B0.8783100.8610980.8496680.028*
C100.81829 (12)0.6625 (3)0.94811 (10)0.0253 (3)
H10A0.8325700.4855710.9253320.030*
H10B0.7499980.6544040.9612930.030*
C110.90210 (11)0.7273 (3)1.04344 (9)0.0229 (3)
H11A0.9697110.7501401.0297690.027*
H11B0.8846400.8961441.0699770.027*
C120.91190 (11)0.5125 (3)1.11888 (9)0.0249 (3)
H12A0.8446400.4898091.1332430.030*
H12B0.9296050.3432301.0928030.030*
O130.99097 (8)0.5794 (2)1.20678 (7)0.0272 (2)
H131.0010 (12)0.456 (4)1.2441 (12)0.041*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.02192 (17)0.02674 (19)0.02021 (17)0.00306 (11)0.00485 (12)0.00497 (11)
C20.0238 (6)0.0218 (6)0.0179 (5)0.0002 (4)0.0076 (4)0.0009 (4)
C30.0230 (5)0.0217 (6)0.0179 (5)0.0015 (4)0.0075 (4)0.0011 (4)
C40.0210 (5)0.0229 (6)0.0183 (5)0.0003 (4)0.0067 (4)0.0012 (4)
C50.0257 (6)0.0255 (6)0.0205 (5)0.0006 (5)0.0074 (5)0.0039 (5)
C60.0293 (6)0.0247 (6)0.0195 (5)0.0028 (5)0.0076 (5)0.0039 (5)
C70.0254 (6)0.0238 (6)0.0166 (5)0.0049 (5)0.0053 (4)0.0003 (4)
C80.0231 (6)0.0258 (6)0.0197 (5)0.0005 (5)0.0055 (4)0.0012 (5)
C90.0270 (6)0.0236 (6)0.0182 (5)0.0054 (5)0.0030 (4)0.0007 (4)
C100.0323 (7)0.0206 (6)0.0192 (5)0.0051 (5)0.0017 (5)0.0003 (4)
C110.0292 (6)0.0192 (6)0.0180 (5)0.0032 (5)0.0034 (4)0.0009 (4)
C120.0318 (6)0.0212 (6)0.0187 (5)0.0024 (5)0.0025 (5)0.0007 (5)
O130.0334 (5)0.0247 (5)0.0187 (4)0.0013 (4)0.0001 (4)0.0003 (4)
Geometric parameters (Å, º) top
S1—C4i1.7342 (13)C9—C101.5241 (19)
S1—C21.7496 (13)C9—H9A0.9900
C2—C81.3972 (17)C9—H9B0.9900
C2—C31.4104 (18)C10—C111.5267 (18)
C3—C51.3983 (18)C10—H10A0.9900
C3—C41.4369 (17)C10—H10B0.9900
C4—C4i1.372 (2)C11—C121.5083 (19)
C5—C61.3828 (18)C11—H11A0.9900
C5—H50.9500C11—H11B0.9900
C6—C71.4069 (19)C12—O131.4274 (16)
C6—H60.9500C12—H12A0.9900
C7—C81.3887 (19)C12—H12B0.9900
C7—C91.5088 (18)O13—H130.81 (2)
C8—H80.9500
C4i—S1—C290.69 (6)C10—C9—H9A109.2
C8—C2—C3121.41 (12)C7—C9—H9B109.2
C8—C2—S1125.75 (10)C10—C9—H9B109.2
C3—C2—S1112.84 (9)H9A—C9—H9B107.9
C5—C3—C2119.26 (12)C9—C10—C11113.49 (11)
C5—C3—C4130.94 (12)C9—C10—H10A108.9
C2—C3—C4109.80 (11)C11—C10—H10A108.9
C4i—C4—C3114.20 (14)C9—C10—H10B108.9
C4i—C4—S1i112.46 (13)C11—C10—H10B108.9
C3—C4—S1i133.34 (10)H10A—C10—H10B107.7
C6—C5—C3118.90 (12)C12—C11—C10111.61 (11)
C6—C5—H5120.5C12—C11—H11A109.3
C3—C5—H5120.5C10—C11—H11A109.3
C5—C6—C7122.05 (12)C12—C11—H11B109.3
C5—C6—H6119.0C10—C11—H11B109.3
C7—C6—H6119.0H11A—C11—H11B108.0
C8—C7—C6119.37 (12)O13—C12—C11110.06 (11)
C8—C7—C9120.59 (12)O13—C12—H12A109.6
C6—C7—C9120.01 (12)C11—C12—H12A109.6
C7—C8—C2119.00 (12)O13—C12—H12B109.6
C7—C8—H8120.5C11—C12—H12B109.6
C2—C8—H8120.5H12A—C12—H12B108.2
C7—C9—C10112.26 (11)C12—O13—H13109.5
C7—C9—H9A109.2
C4i—S1—C2—C8179.45 (12)C3—C5—C6—C70.1 (2)
C4i—S1—C2—C30.70 (10)C5—C6—C7—C80.3 (2)
C8—C2—C3—C51.29 (19)C5—C6—C7—C9177.82 (12)
S1—C2—C3—C5178.57 (10)C6—C7—C8—C20.3 (2)
C8—C2—C3—C4179.51 (12)C9—C7—C8—C2178.37 (12)
S1—C2—C3—C40.64 (14)C3—C2—C8—C71.1 (2)
C5—C3—C4—C4i178.88 (15)S1—C2—C8—C7178.76 (10)
C2—C3—C4—C4i0.20 (19)C8—C7—C9—C1079.29 (16)
C5—C3—C4—S1i1.5 (2)C6—C7—C9—C1098.78 (15)
C2—C3—C4—S1i179.39 (11)C7—C9—C10—C11175.92 (12)
C2—C3—C5—C60.7 (2)C9—C10—C11—C12175.02 (12)
C4—C3—C5—C6179.71 (13)C10—C11—C12—O13179.86 (11)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.812.022.7942 (9)160
C6—H6···S1iii0.953.304.0922 (13)142
C9—H9A···S1iii0.993.434.0609 (15)124
C10—H10B···S1iii0.993.313.9212 (16)122
C10—H10B···S1iv0.993.133.8276 (15)129
C11—H11B···S1iii0.993.404.0897 (16)129
C12—H12A···S1iv0.993.053.8037 (16)134
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A120) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.374 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.450 (3) ÅCell parameters from 6962 reflections
b = 5.063 (1) Åθ = 2.3–24.3°
c = 14.270 (1) ŵ = 0.29 mm1
β = 107.026 (15)°T = 120 K
V = 929.2 (3) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.023
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8199 measured reflectionsh = 1919
2739 independent reflectionsk = 66
2497 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.039H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.111 w = 1/[σ2(Fo2) + (0.0565P)2 + 0.4952P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max = 0.001
2739 reflectionsΔρmax = 0.93 e Å3
121 parametersΔρmin = 0.45 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.003 (3)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64721 (2)0.32336 (7)0.53739 (2)0.02441 (12)
C20.64899 (10)0.5559 (3)0.62858 (9)0.0218 (2)
C30.55402 (10)0.6920 (3)0.61191 (9)0.0216 (2)
C40.48089 (9)0.5974 (3)0.52340 (9)0.0216 (2)
C50.54474 (10)0.8884 (3)0.67769 (9)0.0250 (3)
H50.4816310.9839030.6672350.030*
C60.62895 (10)0.9413 (3)0.75828 (9)0.0255 (3)
H60.6227171.0745940.8030940.031*
C70.72360 (10)0.8037 (3)0.77586 (9)0.0233 (3)
C80.73341 (10)0.6090 (3)0.71070 (9)0.0241 (3)
H80.7965400.5132740.7217080.029*
C90.81190 (11)0.8620 (3)0.86678 (9)0.0249 (3)
H9A0.8024371.0409620.8907850.030*
H9B0.8782360.8607070.8498810.030*
C100.81827 (12)0.6623 (3)0.94816 (10)0.0265 (3)
H10A0.8325270.4854990.9254230.032*
H10B0.7500290.6543140.9613010.032*
C110.90204 (11)0.7272 (3)1.04349 (9)0.0241 (3)
H11A0.9696030.7498381.0298670.029*
H11B0.8846250.8960391.0699540.029*
C120.91182 (11)0.5128 (3)1.11892 (9)0.0262 (3)
H12A0.8446200.4904031.1332630.031*
H12B0.9294130.3434931.0928820.031*
O130.99087 (8)0.5794 (2)1.20676 (7)0.0286 (2)
H131.0000 (12)0.457 (4)1.2444 (12)0.043*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.02290 (17)0.0281 (2)0.02137 (17)0.00317 (11)0.00508 (12)0.00530 (11)
C20.0246 (6)0.0229 (6)0.0187 (5)0.0005 (4)0.0078 (4)0.0010 (4)
C30.0244 (5)0.0225 (6)0.0188 (5)0.0015 (4)0.0078 (4)0.0009 (4)
C40.0217 (5)0.0240 (6)0.0195 (5)0.0005 (4)0.0068 (4)0.0008 (4)
C50.0273 (6)0.0266 (6)0.0214 (6)0.0006 (5)0.0077 (5)0.0041 (5)
C60.0305 (6)0.0260 (6)0.0204 (5)0.0028 (5)0.0079 (5)0.0037 (5)
C70.0267 (6)0.0251 (6)0.0175 (5)0.0051 (5)0.0055 (4)0.0002 (4)
C80.0241 (6)0.0270 (6)0.0207 (5)0.0006 (5)0.0056 (4)0.0014 (5)
C90.0285 (6)0.0250 (6)0.0188 (5)0.0058 (5)0.0033 (4)0.0007 (4)
C100.0338 (7)0.0213 (6)0.0204 (5)0.0056 (5)0.0016 (5)0.0001 (4)
C110.0304 (6)0.0204 (6)0.0189 (5)0.0034 (5)0.0032 (5)0.0010 (4)
C120.0330 (6)0.0225 (6)0.0195 (5)0.0025 (5)0.0021 (5)0.0004 (5)
O130.0351 (5)0.0259 (5)0.0196 (4)0.0011 (4)0.0001 (4)0.0006 (4)
Geometric parameters (Å, º) top
S1—C4i1.7340 (13)C9—C101.5231 (19)
S1—C21.7497 (13)C9—H9A0.9900
C2—C81.3985 (17)C9—H9B0.9900
C2—C31.4090 (18)C10—C111.5265 (18)
C3—C51.3977 (18)C10—H10A0.9900
C3—C41.4368 (17)C10—H10B0.9900
C4—C4i1.373 (2)C11—C121.5072 (19)
C5—C61.3837 (18)C11—H11A0.9900
C5—H50.9500C11—H11B0.9900
C6—C71.408 (2)C12—O131.4265 (15)
C6—H60.9500C12—H12A0.9900
C7—C81.3876 (19)C12—H12B0.9900
C7—C91.5095 (18)O13—H130.80 (2)
C8—H80.9500
C4i—S1—C290.67 (6)C10—C9—H9A109.1
C8—C2—C3121.39 (12)C7—C9—H9B109.1
C8—C2—S1125.70 (10)C10—C9—H9B109.1
C3—C2—S1112.91 (9)H9A—C9—H9B107.9
C5—C3—C2119.30 (12)C9—C10—C11113.50 (11)
C5—C3—C4130.89 (12)C9—C10—H10A108.9
C2—C3—C4109.80 (11)C11—C10—H10A108.9
C4i—C4—C3114.18 (14)C9—C10—H10B108.9
C4i—C4—S1i112.43 (13)C11—C10—H10B108.9
C3—C4—S1i133.39 (10)H10A—C10—H10B107.7
C6—C5—C3118.93 (13)C12—C11—C10111.64 (11)
C6—C5—H5120.5C12—C11—H11A109.3
C3—C5—H5120.5C10—C11—H11A109.3
C5—C6—C7121.97 (12)C12—C11—H11B109.3
C5—C6—H6119.0C10—C11—H11B109.3
C7—C6—H6119.0H11A—C11—H11B108.0
C8—C7—C6119.39 (12)O13—C12—C11110.12 (11)
C8—C7—C9120.63 (13)O13—C12—H12A109.6
C6—C7—C9119.95 (12)C11—C12—H12A109.6
C7—C8—C2119.01 (12)O13—C12—H12B109.6
C7—C8—H8120.5C11—C12—H12B109.6
C2—C8—H8120.5H12A—C12—H12B108.2
C7—C9—C10112.34 (11)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.39 (12)C3—C5—C6—C70.1 (2)
C4i—S1—C2—C30.62 (10)C5—C6—C7—C80.1 (2)
C8—C2—C3—C51.43 (19)C5—C6—C7—C9177.79 (12)
S1—C2—C3—C5178.56 (10)C6—C7—C8—C20.5 (2)
C8—C2—C3—C4179.46 (12)C9—C7—C8—C2178.35 (12)
S1—C2—C3—C40.55 (14)C3—C2—C8—C71.3 (2)
C5—C3—C4—C4i178.82 (15)S1—C2—C8—C7178.73 (10)
C2—C3—C4—C4i0.15 (19)C8—C7—C9—C1079.19 (16)
C5—C3—C4—S1i1.6 (2)C6—C7—C9—C1098.66 (15)
C2—C3—C4—S1i179.45 (11)C7—C9—C10—C11175.94 (12)
C2—C3—C5—C60.8 (2)C9—C10—C11—C12175.06 (12)
C4—C3—C5—C6179.71 (13)C10—C11—C12—O13179.82 (12)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.802.032.7954 (9)160
C6—H6···S1iii0.953.304.0951 (13)142
C9—H9A···S1iii0.993.434.0657 (15)124
C10—H10B···S1iii0.993.313.9257 (17)122
C10—H10B···S1iv0.993.133.8312 (15)129
C11—H11B···S1iii0.993.404.0937 (16)129
C12—H12A···S1iv0.993.053.8068 (16)134
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A130) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.373 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.462 (2) ÅCell parameters from 6972 reflections
b = 5.064 (1) Åθ = 2.5–24.8°
c = 14.278 (1) ŵ = 0.29 mm1
β = 107.080 (14)°T = 130 K
V = 930.4 (2) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.023
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8277 measured reflectionsh = 1919
2748 independent reflectionsk = 67
2496 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.038H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.110 w = 1/[σ2(Fo2) + (0.0566P)2 + 0.4659P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max = 0.001
2748 reflectionsΔρmax = 0.91 e Å3
121 parametersΔρmin = 0.40 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.003 (3)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64710 (2)0.32342 (7)0.53747 (2)0.02573 (12)
C20.64890 (10)0.5559 (3)0.62866 (9)0.0228 (2)
C30.55395 (10)0.6919 (3)0.61190 (9)0.0225 (2)
C40.48091 (9)0.5975 (3)0.52342 (9)0.0227 (2)
C50.54472 (10)0.8881 (3)0.67773 (9)0.0262 (3)
H50.4816350.9834730.6673350.031*
C60.62893 (10)0.9410 (3)0.75825 (9)0.0267 (3)
H60.6227601.0744410.8029760.032*
C70.72350 (10)0.8033 (3)0.77597 (9)0.0245 (3)
C80.73327 (10)0.6088 (3)0.71080 (9)0.0253 (3)
H80.7963370.5129990.7218260.030*
C90.81171 (11)0.8618 (3)0.86675 (9)0.0263 (3)
H9A0.8022111.0407540.8907040.032*
H9B0.8779680.8605990.8498750.032*
C100.81821 (12)0.6623 (3)0.94819 (10)0.0280 (3)
H10A0.7500340.6541910.9613210.034*
H10B0.8324540.4854430.9254900.034*
C110.90197 (11)0.7272 (3)1.04349 (9)0.0254 (3)
H11A0.9694740.7498581.0299050.030*
H11B0.8845750.8959951.0699500.030*
C120.91174 (11)0.5127 (3)1.11885 (9)0.0275 (3)
H12A0.8445890.4902381.1331430.033*
H12B0.9293370.3434531.0928330.033*
O130.99080 (8)0.5795 (2)1.20673 (7)0.0302 (2)
H131.0001 (12)0.457 (4)1.2443 (12)0.045*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.02391 (17)0.0298 (2)0.02238 (17)0.00335 (11)0.00504 (12)0.00564 (11)
C20.0257 (5)0.0242 (6)0.0191 (5)0.0005 (4)0.0075 (4)0.0009 (4)
C30.0251 (5)0.0238 (6)0.0195 (5)0.0015 (4)0.0080 (4)0.0010 (4)
C40.0229 (5)0.0255 (6)0.0200 (5)0.0004 (4)0.0068 (4)0.0010 (4)
C50.0280 (6)0.0282 (6)0.0225 (5)0.0006 (5)0.0075 (5)0.0043 (5)
C60.0317 (6)0.0268 (6)0.0216 (5)0.0031 (5)0.0078 (5)0.0041 (5)
C70.0277 (6)0.0263 (6)0.0185 (5)0.0055 (5)0.0052 (4)0.0001 (4)
C80.0254 (6)0.0281 (6)0.0215 (5)0.0010 (5)0.0057 (4)0.0016 (5)
C90.0297 (6)0.0260 (6)0.0204 (5)0.0065 (5)0.0032 (4)0.0010 (4)
C100.0359 (7)0.0224 (6)0.0211 (5)0.0060 (5)0.0013 (5)0.0003 (4)
C110.0318 (6)0.0219 (6)0.0197 (5)0.0038 (5)0.0032 (5)0.0012 (4)
C120.0345 (6)0.0234 (6)0.0207 (5)0.0025 (5)0.0022 (5)0.0008 (5)
O130.0370 (5)0.0272 (5)0.0206 (4)0.0012 (4)0.0005 (4)0.0003 (4)
Geometric parameters (Å, º) top
S1—C4i1.7337 (13)C9—C101.5235 (18)
S1—C21.7503 (13)C9—H9A0.9900
C2—C81.3981 (17)C9—H9B0.9900
C2—C31.4090 (18)C10—C111.5264 (18)
C3—C51.3982 (17)C10—H10A0.9900
C3—C41.4358 (17)C10—H10B0.9900
C4—C4i1.375 (2)C11—C121.5075 (18)
C5—C61.3831 (18)C11—H11A0.9900
C5—H50.9500C11—H11B0.9900
C6—C71.4079 (19)C12—O131.4273 (15)
C6—H60.9500C12—H12A0.9900
C7—C81.3874 (18)C12—H12B0.9900
C7—C91.5079 (18)O13—H130.80 (2)
C8—H80.9500
C4i—S1—C290.70 (6)C10—C9—H9A109.1
C8—C2—C3121.45 (12)C7—C9—H9B109.1
C8—C2—S1125.68 (10)C10—C9—H9B109.1
C3—C2—S1112.87 (9)H9A—C9—H9B107.9
C5—C3—C2119.23 (12)C11—C10—C9113.53 (11)
C5—C3—C4130.91 (12)C11—C10—H10A108.9
C2—C3—C4109.85 (11)C9—C10—H10A108.9
C4i—C4—C3114.19 (14)C11—C10—H10B108.9
C4i—C4—S1i112.38 (12)C9—C10—H10B108.9
C3—C4—S1i133.43 (10)H10A—C10—H10B107.7
C6—C5—C3118.91 (12)C12—C11—C10111.58 (11)
C6—C5—H5120.5C12—C11—H11A109.3
C3—C5—H5120.5C10—C11—H11A109.3
C5—C6—C7122.05 (12)C12—C11—H11B109.3
C5—C6—H6119.0C10—C11—H11B109.3
C7—C6—H6119.0H11A—C11—H11B108.0
C8—C7—C6119.33 (12)O13—C12—C11110.05 (11)
C8—C7—C9120.68 (12)O13—C12—H12A109.7
C6—C7—C9119.96 (12)C11—C12—H12A109.7
C7—C8—C2119.01 (12)O13—C12—H12B109.7
C7—C8—H8120.5C11—C12—H12B109.7
C2—C8—H8120.5H12A—C12—H12B108.2
C7—C9—C10112.33 (11)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.34 (12)C3—C5—C6—C70.1 (2)
C4i—S1—C2—C30.60 (10)C5—C6—C7—C80.2 (2)
C8—C2—C3—C51.46 (19)C5—C6—C7—C9177.81 (12)
S1—C2—C3—C5178.59 (10)C6—C7—C8—C20.45 (19)
C8—C2—C3—C4179.45 (12)C9—C7—C8—C2178.48 (12)
S1—C2—C3—C40.50 (14)C3—C2—C8—C71.3 (2)
C5—C3—C4—C4i178.87 (15)S1—C2—C8—C7178.76 (10)
C2—C3—C4—C4i0.09 (19)C8—C7—C9—C1079.25 (16)
C5—C3—C4—S1i1.6 (2)C6—C7—C9—C1098.77 (15)
C2—C3—C4—S1i179.45 (11)C7—C9—C10—C11175.96 (12)
C2—C3—C5—C60.8 (2)C9—C10—C11—C12175.06 (12)
C4—C3—C5—C6179.62 (13)C10—C11—C12—O13179.84 (12)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.802.032.7963 (9)160
C6—H6···S1iii0.953.314.0993 (13)142
C9—H9A···S1iii0.993.434.0700 (15)124
C10—H10A···S1iii0.993.313.9292 (16)122
C10—H10A···S1iv0.993.143.8346 (15)129
C11—H11B···S1iii0.993.404.0968 (15)129
C12—H12A···S1iv0.993.053.8088 (15)134
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A140) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.371 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.473 (2) ÅCell parameters from 6963 reflections
b = 5.066 (1) Åθ = 2.4–26.0°
c = 14.286 (1) ŵ = 0.29 mm1
β = 107.137 (14)°T = 140 K
V = 931.8 (2) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.024
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8296 measured reflectionsh = 1919
2749 independent reflectionsk = 67
2484 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.039H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.109 w = 1/[σ2(Fo2) + (0.0541P)2 + 0.465P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max = 0.001
2749 reflectionsΔρmax = 0.91 e Å3
121 parametersΔρmin = 0.37 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.004 (2)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64700 (2)0.32344 (7)0.53754 (2)0.02705 (12)
C20.64886 (10)0.5556 (3)0.62875 (9)0.0239 (2)
C30.55395 (10)0.6918 (3)0.61189 (9)0.0235 (2)
C40.48091 (9)0.5972 (3)0.52336 (9)0.0235 (2)
C50.54474 (11)0.8876 (3)0.67773 (9)0.0274 (3)
H50.4816780.9828180.6673590.033*
C60.62892 (11)0.9404 (3)0.75822 (9)0.0281 (3)
H60.6227781.0737350.8029550.034*
C70.72340 (10)0.8029 (3)0.77594 (9)0.0257 (3)
C80.73318 (10)0.6089 (3)0.71079 (9)0.0264 (3)
H80.7962920.5134850.7217690.032*
C90.81155 (11)0.8615 (3)0.86684 (9)0.0276 (3)
H9A0.8020191.0404290.8907260.033*
H9B0.8777980.8603960.8500580.033*
C100.81808 (12)0.6622 (3)0.94826 (10)0.0295 (3)
H10A0.7499710.6543160.9613790.035*
H10B0.8322420.4854080.9255850.035*
C110.90186 (11)0.7270 (3)1.04354 (9)0.0267 (3)
H11A0.9693060.7493981.0299620.032*
H11B0.8845660.8958161.0699480.032*
C120.91168 (11)0.5130 (3)1.11892 (9)0.0289 (3)
H12A0.8445830.4907461.1331990.035*
H12B0.9291810.3436941.0929550.035*
O130.99072 (8)0.5796 (2)1.20674 (7)0.0319 (2)
H131.0002 (13)0.457 (4)1.2441 (13)0.048*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.02489 (17)0.0314 (2)0.02349 (17)0.00360 (11)0.00509 (12)0.00586 (11)
C20.0270 (6)0.0253 (6)0.0202 (5)0.0005 (5)0.0080 (4)0.0010 (4)
C30.0262 (6)0.0252 (6)0.0199 (5)0.0014 (4)0.0079 (4)0.0008 (4)
C40.0237 (5)0.0264 (6)0.0208 (5)0.0004 (4)0.0071 (4)0.0013 (4)
C50.0291 (6)0.0295 (6)0.0238 (6)0.0004 (5)0.0080 (5)0.0046 (5)
C60.0337 (6)0.0285 (6)0.0221 (5)0.0031 (5)0.0083 (5)0.0045 (5)
C70.0289 (6)0.0278 (6)0.0192 (5)0.0061 (5)0.0054 (4)0.0002 (4)
C80.0261 (6)0.0297 (6)0.0225 (5)0.0012 (5)0.0057 (4)0.0014 (5)
C90.0312 (6)0.0276 (6)0.0210 (5)0.0067 (5)0.0030 (5)0.0010 (5)
C100.0375 (7)0.0237 (6)0.0223 (6)0.0061 (5)0.0010 (5)0.0004 (4)
C110.0329 (6)0.0231 (6)0.0209 (5)0.0039 (5)0.0031 (5)0.0016 (4)
C120.0365 (7)0.0249 (6)0.0211 (5)0.0029 (5)0.0019 (5)0.0008 (5)
O130.0388 (5)0.0289 (5)0.0218 (4)0.0014 (4)0.0009 (4)0.0001 (4)
Geometric parameters (Å, º) top
S1—C4i1.7333 (13)C9—C101.5233 (19)
S1—C21.7501 (13)C9—H9A0.9900
C2—C81.3972 (17)C9—H9B0.9900
C2—C31.4099 (18)C10—C111.5260 (18)
C3—C51.3973 (18)C10—H10A0.9900
C3—C41.4366 (17)C10—H10B0.9900
C4—C4i1.372 (2)C11—C121.5062 (19)
C5—C61.3826 (18)C11—H11A0.9900
C5—H50.9500C11—H11B0.9900
C6—C71.407 (2)C12—O131.4265 (16)
C6—H60.9500C12—H12A0.9900
C7—C81.3865 (19)C12—H12B0.9900
C7—C91.5086 (18)O13—H130.80 (2)
C8—H80.9500
C4i—S1—C290.68 (6)C10—C9—H9A109.1
C8—C2—C3121.41 (12)C7—C9—H9B109.1
C8—C2—S1125.74 (10)C10—C9—H9B109.1
C3—C2—S1112.85 (9)H9A—C9—H9B107.9
C5—C3—C2119.22 (12)C11—C10—C9113.56 (11)
C5—C3—C4130.97 (12)C11—C10—H10A108.9
C2—C3—C4109.80 (11)C9—C10—H10A108.9
C4i—C4—C3114.20 (14)C11—C10—H10B108.9
C4i—C4—S1i112.46 (13)C9—C10—H10B108.9
C3—C4—S1i133.34 (10)H10A—C10—H10B107.7
C6—C5—C3118.92 (13)C12—C11—C10111.65 (11)
C6—C5—H5120.5C12—C11—H11A109.3
C3—C5—H5120.5C10—C11—H11A109.3
C5—C6—C7122.05 (12)C12—C11—H11B109.3
C5—C6—H6119.0C10—C11—H11B109.3
C7—C6—H6119.0H11A—C11—H11B108.0
C8—C7—C6119.35 (12)O13—C12—C11110.12 (11)
C8—C7—C9120.73 (13)O13—C12—H12A109.6
C6—C7—C9119.90 (12)C11—C12—H12A109.6
C7—C8—C2119.04 (12)O13—C12—H12B109.6
C7—C8—H8120.5C11—C12—H12B109.6
C2—C8—H8120.5H12A—C12—H12B108.2
C7—C9—C10112.36 (11)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.52 (13)C3—C5—C6—C70.1 (2)
C4i—S1—C2—C30.65 (10)C5—C6—C7—C80.3 (2)
C8—C2—C3—C51.2 (2)C5—C6—C7—C9177.79 (13)
S1—C2—C3—C5178.64 (10)C6—C7—C8—C20.3 (2)
C8—C2—C3—C4179.54 (12)C9—C7—C8—C2178.35 (12)
S1—C2—C3—C40.62 (14)C3—C2—C8—C71.0 (2)
C5—C3—C4—C4i178.91 (15)S1—C2—C8—C7178.78 (10)
C2—C3—C4—C4i0.24 (19)C8—C7—C9—C1079.32 (17)
C5—C3—C4—S1i1.4 (2)C6—C7—C9—C1098.72 (16)
C2—C3—C4—S1i179.44 (11)C7—C9—C10—C11176.06 (12)
C2—C3—C5—C60.6 (2)C9—C10—C11—C12175.08 (12)
C4—C3—C5—C6179.68 (13)C10—C11—C12—O13179.84 (12)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.802.032.7972 (10)160
C6—H6···S1iii0.953.314.1037 (13)142
C9—H9A···S1iii0.993.444.0738 (16)124
C10—H10A···S1iii0.993.323.9321 (17)122
C10—H10A···S1iv0.993.143.8373 (15)129
C11—H11B···S1iii0.993.414.1003 (16)129
C12—H12A···S1iv0.993.063.8117 (15)134
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A150) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.369 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.484 (2) ÅCell parameters from 6940 reflections
b = 5.068 (1) Åθ = 2.4–24.9°
c = 14.294 (1) ŵ = 0.29 mm1
β = 107.194 (12)°T = 150 K
V = 933.2 (2) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.023
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8300 measured reflectionsh = 1919
2741 independent reflectionsk = 67
2472 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.039H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.111 w = 1/[σ2(Fo2) + (0.0552P)2 + 0.473P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max = 0.001
2741 reflectionsΔρmax = 0.87 e Å3
121 parametersΔρmin = 0.38 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.004 (3)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64689 (2)0.32342 (7)0.53763 (2)0.02843 (12)
C20.64878 (10)0.5555 (3)0.62876 (9)0.0249 (2)
C30.55399 (10)0.6915 (3)0.61196 (9)0.0246 (2)
C40.48093 (10)0.5971 (3)0.52333 (9)0.0246 (2)
C50.54480 (11)0.8872 (3)0.67774 (10)0.0287 (3)
H50.4817610.9824100.6673080.034*
C60.62893 (11)0.9401 (3)0.75826 (9)0.0293 (3)
H60.6228041.0733440.8029800.035*
C70.72333 (11)0.8026 (3)0.77600 (9)0.0269 (3)
C80.73313 (10)0.6085 (3)0.71084 (10)0.0277 (3)
H80.7961860.5130390.7218560.033*
C90.81154 (11)0.8612 (3)0.86693 (10)0.0292 (3)
H9A0.8020901.0400470.8907900.035*
H9B0.8777270.8598260.8501820.035*
C100.81806 (12)0.6623 (3)0.94825 (10)0.0308 (3)
H10A0.7499960.6545880.9613320.037*
H10B0.8321250.4854860.9255990.037*
C110.90190 (11)0.7269 (3)1.04359 (9)0.0280 (3)
H11A0.9693100.7489521.0300620.034*
H11B0.8847250.8958151.0699440.034*
C120.91162 (12)0.5132 (3)1.11898 (10)0.0304 (3)
H12A0.8445450.4912661.1331780.037*
H12B0.9290440.3438711.0930850.037*
O130.99058 (9)0.5797 (2)1.20677 (7)0.0336 (2)
H131.0001 (13)0.455 (4)1.2448 (13)0.050*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.02608 (18)0.0330 (2)0.02467 (18)0.00379 (12)0.00520 (12)0.00617 (12)
C20.0280 (6)0.0263 (6)0.0211 (5)0.0006 (5)0.0082 (4)0.0011 (4)
C30.0266 (6)0.0267 (6)0.0211 (5)0.0016 (4)0.0081 (4)0.0009 (4)
C40.0246 (5)0.0276 (6)0.0217 (5)0.0002 (5)0.0072 (4)0.0013 (5)
C50.0307 (6)0.0310 (7)0.0246 (6)0.0007 (5)0.0083 (5)0.0049 (5)
C60.0347 (7)0.0297 (7)0.0232 (6)0.0029 (5)0.0083 (5)0.0045 (5)
C70.0304 (6)0.0290 (7)0.0200 (5)0.0061 (5)0.0055 (5)0.0000 (4)
C80.0272 (6)0.0308 (7)0.0241 (6)0.0013 (5)0.0060 (5)0.0017 (5)
C90.0331 (6)0.0289 (7)0.0222 (5)0.0073 (5)0.0030 (5)0.0009 (5)
C100.0387 (7)0.0250 (6)0.0233 (6)0.0067 (5)0.0008 (5)0.0005 (5)
C110.0343 (6)0.0241 (6)0.0223 (5)0.0041 (5)0.0030 (5)0.0017 (5)
C120.0385 (7)0.0257 (6)0.0225 (6)0.0028 (5)0.0019 (5)0.0008 (5)
O130.0407 (6)0.0306 (5)0.0227 (4)0.0015 (4)0.0011 (4)0.0001 (4)
Geometric parameters (Å, º) top
S1—C4i1.7332 (13)C9—C101.5214 (19)
S1—C21.7495 (13)C9—H9A0.9900
C2—C81.3976 (18)C9—H9B0.9900
C2—C31.4090 (18)C10—C111.5269 (18)
C3—C51.3971 (18)C10—H10A0.9900
C3—C41.4375 (17)C10—H10B0.9900
C4—C4i1.372 (3)C11—C121.5059 (19)
C5—C61.3826 (18)C11—H11A0.9900
C5—H50.9500C11—H11B0.9900
C6—C71.407 (2)C12—O131.4254 (16)
C6—H60.9500C12—H12A0.9900
C7—C81.3879 (19)C12—H12B0.9900
C7—C91.5093 (18)O13—H130.82 (2)
C8—H80.9500
C4i—S1—C290.66 (6)C10—C9—H9A109.1
C8—C2—C3121.41 (12)C7—C9—H9B109.1
C8—C2—S1125.68 (10)C10—C9—H9B109.1
C3—C2—S1112.91 (9)H9A—C9—H9B107.9
C5—C3—C2119.28 (12)C11—C10—C9113.59 (11)
C5—C3—C4130.95 (12)C11—C10—H10A108.8
C2—C3—C4109.76 (11)C9—C10—H10A108.8
C4i—C4—C3114.18 (14)C11—C10—H10B108.8
C4i—C4—S1i112.48 (13)C9—C10—H10B108.8
C3—C4—S1i133.34 (10)H10A—C10—H10B107.7
C6—C5—C3118.93 (13)C12—C11—C10111.68 (11)
C6—C5—H5120.5C12—C11—H11A109.3
C3—C5—H5120.5C10—C11—H11A109.3
C5—C6—C7122.01 (13)C12—C11—H11B109.3
C5—C6—H6119.0C10—C11—H11B109.3
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.39 (12)O13—C12—C11110.15 (12)
C8—C7—C9120.67 (13)O13—C12—H12A109.6
C6—C7—C9119.91 (12)C11—C12—H12A109.6
C7—C8—C2118.97 (13)O13—C12—H12B109.6
C7—C8—H8120.5C11—C12—H12B109.6
C2—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.37 (11)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.50 (13)C3—C5—C6—C70.1 (2)
C4i—S1—C2—C30.58 (10)C5—C6—C7—C80.3 (2)
C8—C2—C3—C51.3 (2)C5—C6—C7—C9177.80 (13)
S1—C2—C3—C5178.64 (10)C6—C7—C8—C20.3 (2)
C8—C2—C3—C4179.54 (12)C9—C7—C8—C2178.39 (12)
S1—C2—C3—C40.54 (14)C3—C2—C8—C71.1 (2)
C5—C3—C4—C4i178.87 (15)S1—C2—C8—C7178.80 (10)
C2—C3—C4—C4i0.2 (2)C8—C7—C9—C1079.38 (17)
C5—C3—C4—S1i1.5 (2)C6—C7—C9—C1098.67 (16)
C2—C3—C4—S1i179.49 (11)C7—C9—C10—C11176.06 (13)
C2—C3—C5—C60.7 (2)C9—C10—C11—C12175.13 (13)
C4—C3—C5—C6179.63 (14)C10—C11—C12—O13179.88 (12)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.822.022.7977 (10)160
C6—H6···S1iii0.953.314.1072 (14)142
C9—H9A···S1iii0.993.444.0793 (16)124
C10—H10A···S1iii0.993.323.9365 (17)122
C10—H10A···S1iv0.993.143.8421 (16)129
C11—H11B···S1iii0.993.414.1051 (16)129
C12—H12A···S1iv0.993.063.8146 (16)134
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A160) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.366 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.496 (3) ÅCell parameters from 7083 reflections
b = 5.070 (1) Åθ = 2.4–25.5°
c = 14.303 (1) ŵ = 0.29 mm1
β = 107.255 (14)°T = 160 K
V = 934.6 (3) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.021
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8282 measured reflectionsh = 1919
2741 independent reflectionsk = 67
2463 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.040H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.116 w = 1/[σ2(Fo2) + (0.0604P)2 + 0.3814P]
where P = (Fo2 + 2Fc2)/3
S = 1.09(Δ/σ)max = 0.001
2741 reflectionsΔρmax = 0.83 e Å3
121 parametersΔρmin = 0.43 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.006 (3)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64677 (2)0.32349 (7)0.53772 (2)0.02997 (13)
C20.64870 (10)0.5553 (3)0.62887 (9)0.0263 (3)
C30.55388 (10)0.6914 (3)0.61197 (9)0.0259 (3)
C40.48095 (10)0.5971 (3)0.52328 (9)0.0260 (3)
C50.54481 (11)0.8869 (3)0.67770 (10)0.0305 (3)
H50.4818580.9822380.6672420.037*
C60.62899 (11)0.9394 (3)0.75829 (10)0.0309 (3)
H60.6229011.0724550.8030350.037*
C70.72326 (11)0.8021 (3)0.77607 (9)0.0286 (3)
C80.73296 (11)0.6081 (3)0.71098 (10)0.0293 (3)
H80.7959580.5126290.7220600.035*
C90.81147 (11)0.8606 (3)0.86704 (10)0.0308 (3)
H9A0.8020771.0395030.8908430.037*
H9B0.8776150.8590900.8503630.037*
C100.81792 (12)0.6620 (3)0.94833 (10)0.0326 (3)
H10A0.7499010.6544490.9613420.039*
H10B0.8319590.4851760.9257550.039*
C110.90174 (11)0.7268 (3)1.04363 (9)0.0297 (3)
H11A0.9690860.7489441.0301310.036*
H11B0.8845530.8956861.0699250.036*
C120.91156 (12)0.5135 (3)1.11897 (10)0.0322 (3)
H12A0.8445440.4916271.1331390.039*
H12B0.9289190.3442501.0930840.039*
O130.99050 (9)0.5796 (2)1.20678 (7)0.0355 (3)
H130.9989 (13)0.459 (4)1.2443 (13)0.053*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.02736 (18)0.0348 (2)0.02615 (18)0.00399 (12)0.00544 (12)0.00640 (12)
C20.0288 (6)0.0282 (6)0.0224 (5)0.0007 (5)0.0083 (4)0.0013 (4)
C30.0288 (6)0.0275 (6)0.0222 (5)0.0015 (4)0.0088 (4)0.0013 (4)
C40.0264 (5)0.0290 (6)0.0227 (5)0.0003 (5)0.0077 (4)0.0010 (5)
C50.0322 (6)0.0326 (7)0.0266 (6)0.0009 (5)0.0087 (5)0.0055 (5)
C60.0366 (7)0.0313 (7)0.0245 (6)0.0033 (5)0.0085 (5)0.0050 (5)
C70.0324 (6)0.0307 (7)0.0213 (5)0.0064 (5)0.0058 (5)0.0003 (5)
C80.0285 (6)0.0329 (7)0.0252 (6)0.0013 (5)0.0060 (5)0.0013 (5)
C90.0343 (7)0.0308 (7)0.0238 (6)0.0078 (5)0.0031 (5)0.0010 (5)
C100.0407 (7)0.0267 (7)0.0245 (6)0.0072 (5)0.0008 (5)0.0010 (5)
C110.0364 (6)0.0255 (6)0.0233 (6)0.0041 (5)0.0030 (5)0.0018 (5)
C120.0402 (7)0.0272 (6)0.0244 (6)0.0030 (5)0.0021 (5)0.0009 (5)
O130.0425 (6)0.0322 (6)0.0247 (5)0.0017 (4)0.0012 (4)0.0001 (4)
Geometric parameters (Å, º) top
S1—C4i1.7327 (14)C9—C101.521 (2)
S1—C21.7495 (13)C9—H9A0.9900
C2—C81.3971 (18)C9—H9B0.9900
C2—C31.4102 (18)C10—C111.5267 (19)
C3—C51.3964 (18)C10—H10A0.9900
C3—C41.4372 (17)C10—H10B0.9900
C4—C4i1.371 (3)C11—C121.5044 (19)
C5—C61.3833 (18)C11—H11A0.9900
C5—H50.9500C11—H11B0.9900
C6—C71.406 (2)C12—O131.4251 (16)
C6—H60.9500C12—H12A0.9900
C7—C81.3869 (19)C12—H12B0.9900
C7—C91.5097 (18)O13—H130.80 (2)
C8—H80.9500
C4i—S1—C290.68 (6)C10—C9—H9A109.1
C8—C2—C3121.41 (12)C7—C9—H9B109.1
C8—C2—S1125.72 (11)C10—C9—H9B109.1
C3—C2—S1112.87 (10)H9A—C9—H9B107.9
C5—C3—C2119.23 (12)C11—C10—C9113.53 (12)
C5—C3—C4131.02 (12)C11—C10—H10A108.9
C2—C3—C4109.74 (11)C9—C10—H10A108.9
C4i—C4—C3114.21 (14)C11—C10—H10B108.9
C4i—C4—S1i112.50 (13)C9—C10—H10B108.9
C3—C4—S1i133.30 (10)H10A—C10—H10B107.7
C6—C5—C3118.90 (13)C12—C11—C10111.67 (12)
C6—C5—H5120.5C12—C11—H11A109.3
C3—C5—H5120.5C10—C11—H11A109.3
C5—C6—C7122.07 (13)C12—C11—H11B109.3
C5—C6—H6119.0C10—C11—H11B109.3
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.36 (12)O13—C12—C11110.26 (12)
C8—C7—C9120.70 (13)O13—C12—H12A109.6
C6—C7—C9119.91 (13)C11—C12—H12A109.6
C7—C8—C2119.01 (13)O13—C12—H12B109.6
C7—C8—H8120.5C11—C12—H12B109.6
C2—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.35 (11)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.49 (13)C3—C5—C6—C70.0 (2)
C4i—S1—C2—C30.60 (11)C5—C6—C7—C80.2 (2)
C8—C2—C3—C51.3 (2)C5—C6—C7—C9177.86 (13)
S1—C2—C3—C5178.58 (11)C6—C7—C8—C20.4 (2)
C8—C2—C3—C4179.57 (12)C9—C7—C8—C2178.44 (12)
S1—C2—C3—C40.51 (14)C3—C2—C8—C71.2 (2)
C5—C3—C4—C4i178.84 (15)S1—C2—C8—C7178.74 (11)
C2—C3—C4—C4i0.1 (2)C8—C7—C9—C1079.43 (17)
C5—C3—C4—S1i1.6 (2)C6—C7—C9—C1098.61 (16)
C2—C3—C4—S1i179.45 (11)C7—C9—C10—C11176.05 (13)
C2—C3—C5—C60.7 (2)C9—C10—C11—C12175.07 (13)
C4—C3—C5—C6179.59 (14)C10—C11—C12—O13179.84 (12)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.802.042.7986 (10)159
C6—H6···S1iii0.953.324.1118 (14)142
C9—H9A···S1iii0.993.454.0847 (17)124
C10—H10A···S1iii0.993.323.9404 (18)122
C10—H10A···S1iv0.993.153.8446 (16)129
C11—H11B···S1iii0.993.414.1078 (17)129
C12—H12A···S1iv0.993.063.8180 (17)134
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A170) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.364 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.508 (3) ÅCell parameters from 6920 reflections
b = 5.073 (1) Åθ = 2.4–24.3°
c = 14.312 (1) ŵ = 0.29 mm1
β = 107.316 (13)°T = 170 K
V = 936.3 (3) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.023
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8289 measured reflectionsh = 1919
2751 independent reflectionsk = 67
2471 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.040H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.117 w = 1/[σ2(Fo2) + (0.0605P)2 + 0.3871P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max = 0.001
2751 reflectionsΔρmax = 0.80 e Å3
121 parametersΔρmin = 0.41 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.005 (3)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64665 (3)0.32349 (8)0.53781 (2)0.03141 (13)
C20.64861 (10)0.5552 (3)0.62891 (9)0.0274 (3)
C30.55389 (10)0.6911 (3)0.61197 (9)0.0270 (3)
C40.48100 (10)0.5970 (3)0.52330 (9)0.0273 (3)
C50.54484 (11)0.8864 (3)0.67777 (10)0.0319 (3)
H50.4818880.9814280.6673260.038*
C60.62888 (11)0.9391 (3)0.75830 (10)0.0325 (3)
H60.6228021.0721710.8029570.039*
C70.72317 (11)0.8017 (3)0.77618 (9)0.0299 (3)
C80.73277 (11)0.6080 (3)0.71100 (10)0.0308 (3)
H80.7957310.5125200.7220820.037*
C90.81135 (12)0.8603 (3)0.86708 (10)0.0324 (3)
H9A0.8019911.0390860.8908310.039*
H9B0.8774220.8586370.8504260.039*
C100.81785 (13)0.6618 (3)0.94840 (10)0.0342 (3)
H10A0.7499050.6544340.9614030.041*
H10B0.8318240.4850710.9258660.041*
C110.90164 (12)0.7266 (3)1.04360 (9)0.0311 (3)
H11A0.9689260.7484641.0301130.037*
H11B0.8845480.8954761.0698300.037*
C120.91148 (12)0.5136 (3)1.11901 (10)0.0336 (3)
H12A0.8445140.4919001.1331260.040*
H12B0.9287810.3443421.0931890.040*
O130.99036 (9)0.5796 (2)1.20677 (7)0.0373 (3)
H130.9998 (13)0.456 (4)1.2447 (13)0.056*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.02865 (18)0.0365 (2)0.02729 (18)0.00422 (12)0.00559 (13)0.00672 (12)
C20.0298 (6)0.0292 (6)0.0233 (5)0.0008 (5)0.0083 (4)0.0012 (5)
C30.0295 (6)0.0290 (6)0.0231 (5)0.0017 (5)0.0089 (4)0.0013 (4)
C40.0278 (5)0.0306 (6)0.0239 (5)0.0003 (5)0.0081 (4)0.0012 (5)
C50.0339 (6)0.0342 (7)0.0275 (6)0.0007 (5)0.0090 (5)0.0054 (5)
C60.0388 (7)0.0330 (7)0.0255 (6)0.0036 (5)0.0092 (5)0.0054 (5)
C70.0338 (6)0.0324 (7)0.0218 (5)0.0068 (5)0.0057 (5)0.0002 (5)
C80.0301 (6)0.0339 (7)0.0268 (6)0.0017 (5)0.0061 (5)0.0018 (5)
C90.0362 (7)0.0325 (7)0.0245 (6)0.0083 (5)0.0029 (5)0.0010 (5)
C100.0430 (8)0.0280 (7)0.0255 (6)0.0077 (5)0.0007 (5)0.0009 (5)
C110.0381 (7)0.0268 (6)0.0243 (6)0.0046 (5)0.0029 (5)0.0021 (5)
C120.0422 (7)0.0280 (7)0.0254 (6)0.0031 (5)0.0020 (5)0.0009 (5)
O130.0445 (6)0.0337 (6)0.0258 (5)0.0016 (4)0.0017 (4)0.0001 (4)
Geometric parameters (Å, º) top
S1—C4i1.7330 (14)C9—C101.521 (2)
S1—C21.7499 (13)C9—H9A0.9900
C2—C81.3962 (18)C9—H9B0.9900
C2—C31.4095 (19)C10—C111.5255 (19)
C3—C51.3968 (18)C10—H10A0.9900
C3—C41.4368 (17)C10—H10B0.9900
C4—C4i1.371 (3)C11—C121.505 (2)
C5—C61.3819 (19)C11—H11A0.9900
C5—H50.9500C11—H11B0.9900
C6—C71.407 (2)C12—O131.4242 (16)
C6—H60.9500C12—H12A0.9900
C7—C81.388 (2)C12—H12B0.9900
C7—C91.5090 (18)O13—H130.82 (2)
C8—H80.9500
C4i—S1—C290.67 (6)C10—C9—H9A109.1
C8—C2—C3121.41 (12)C7—C9—H9B109.1
C8—C2—S1125.71 (11)C10—C9—H9B109.1
C3—C2—S1112.88 (10)H9A—C9—H9B107.9
C5—C3—C2119.21 (12)C11—C10—C9113.54 (12)
C5—C3—C4131.05 (13)C11—C10—H10A108.9
C2—C3—C4109.73 (11)C9—C10—H10A108.9
C4i—C4—C3114.26 (15)C11—C10—H10B108.9
C4i—C4—S1i112.45 (13)C9—C10—H10B108.9
C3—C4—S1i133.29 (10)H10A—C10—H10B107.7
C6—C5—C3118.98 (13)C12—C11—C10111.70 (12)
C6—C5—H5120.5C12—C11—H11A109.3
C3—C5—H5120.5C10—C11—H11A109.3
C5—C6—C7122.03 (13)C12—C11—H11B109.3
C5—C6—H6119.0C10—C11—H11B109.3
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.30 (12)O13—C12—C11110.31 (12)
C8—C7—C9120.75 (13)O13—C12—H12A109.6
C6—C7—C9119.93 (13)C11—C12—H12A109.6
C7—C8—C2119.07 (13)O13—C12—H12B109.6
C7—C8—H8120.5C11—C12—H12B109.6
C2—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.36 (12)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.49 (13)C3—C5—C6—C70.2 (2)
C4i—S1—C2—C30.55 (11)C5—C6—C7—C80.3 (2)
C8—C2—C3—C51.3 (2)C5—C6—C7—C9177.86 (13)
S1—C2—C3—C5178.67 (11)C6—C7—C8—C20.3 (2)
C8—C2—C3—C4179.55 (12)C9—C7—C8—C2178.50 (13)
S1—C2—C3—C40.49 (15)C3—C2—C8—C71.2 (2)
C5—C3—C4—C4i178.88 (16)S1—C2—C8—C7178.81 (11)
C2—C3—C4—C4i0.1 (2)C8—C7—C9—C1079.53 (18)
C5—C3—C4—S1i1.5 (2)C6—C7—C9—C1098.62 (17)
C2—C3—C4—S1i179.52 (11)C7—C9—C10—C11176.07 (13)
C2—C3—C5—C60.6 (2)C9—C10—C11—C12175.10 (13)
C4—C3—C5—C6179.57 (14)C10—C11—C12—O13179.87 (13)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.822.022.8002 (10)160
C6—H6···S1iii0.953.324.1158 (14)142
C9—H9A···S1iii0.993.464.0902 (17)124
C10—H10A···S1iii0.993.333.9450 (18)122
C10—H10A···S1iv0.993.153.8482 (16)129
C11—H11B···S1iii0.993.424.1123 (17)129
C12—H12A···S1iv0.993.063.8207 (17)134
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A180) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.361 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.521 (3) ÅCell parameters from 6914 reflections
b = 5.076 (1) Åθ = 2.4–24.7°
c = 14.322 (1) ŵ = 0.29 mm1
β = 107.384 (14)°T = 180 K
V = 938.1 (3) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.022
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8298 measured reflectionsh = 1919
2758 independent reflectionsk = 67
2465 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.042H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.119 w = 1/[σ2(Fo2) + (0.0603P)2 + 0.4239P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max = 0.001
2758 reflectionsΔρmax = 0.81 e Å3
121 parametersΔρmin = 0.45 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.006 (3)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64652 (3)0.32353 (8)0.53791 (2)0.03306 (13)
C20.64847 (11)0.5551 (3)0.62900 (9)0.0288 (3)
C30.55387 (11)0.6910 (3)0.61195 (10)0.0283 (3)
C40.48101 (10)0.5969 (3)0.52329 (9)0.0285 (3)
C50.54489 (12)0.8858 (3)0.67780 (10)0.0333 (3)
H50.4819350.9805430.6674100.040*
C60.62893 (12)0.9386 (3)0.75832 (10)0.0339 (3)
H60.6228841.0717490.8029150.041*
C70.72307 (11)0.8014 (3)0.77625 (10)0.0312 (3)
C80.73270 (11)0.6078 (3)0.71110 (10)0.0321 (3)
H80.7956430.5125700.7221820.038*
C90.81118 (12)0.8599 (3)0.86713 (10)0.0342 (3)
H9A0.8018841.0386820.8908170.041*
H9B0.8772070.8580890.8505490.041*
C100.81772 (13)0.6620 (3)0.94844 (11)0.0358 (3)
H10A0.7498250.6548680.9613820.043*
H10B0.8315660.4852560.9259300.043*
C110.90150 (12)0.7263 (3)1.04369 (10)0.0326 (3)
H11A0.9687450.7479661.0302750.039*
H11B0.8845130.8951141.0699200.039*
C120.91131 (12)0.5136 (3)1.11905 (10)0.0351 (3)
H12A0.8444150.4919871.1331450.042*
H12B0.9285580.3442961.0932850.042*
O130.99025 (9)0.5798 (2)1.20678 (8)0.0393 (3)
H130.9996 (14)0.458 (4)1.2441 (14)0.059*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.02995 (19)0.0385 (2)0.02873 (19)0.00444 (13)0.00576 (13)0.00705 (13)
C20.0315 (6)0.0309 (7)0.0245 (5)0.0008 (5)0.0090 (5)0.0013 (5)
C30.0308 (6)0.0302 (7)0.0244 (6)0.0017 (5)0.0091 (5)0.0014 (5)
C40.0291 (6)0.0317 (7)0.0246 (5)0.0001 (5)0.0081 (5)0.0013 (5)
C50.0347 (7)0.0358 (7)0.0291 (6)0.0006 (5)0.0089 (5)0.0058 (5)
C60.0399 (7)0.0345 (7)0.0270 (6)0.0036 (6)0.0092 (5)0.0057 (5)
C70.0353 (7)0.0330 (7)0.0235 (6)0.0071 (5)0.0060 (5)0.0003 (5)
C80.0312 (6)0.0357 (7)0.0277 (6)0.0013 (5)0.0064 (5)0.0013 (5)
C90.0380 (7)0.0342 (7)0.0259 (6)0.0086 (6)0.0027 (5)0.0009 (5)
C100.0448 (8)0.0292 (7)0.0267 (6)0.0078 (6)0.0006 (5)0.0007 (5)
C110.0397 (7)0.0275 (7)0.0259 (6)0.0053 (5)0.0027 (5)0.0021 (5)
C120.0437 (8)0.0293 (7)0.0267 (6)0.0032 (6)0.0018 (5)0.0010 (5)
O130.0466 (6)0.0358 (6)0.0269 (5)0.0019 (5)0.0020 (4)0.0003 (4)
Geometric parameters (Å, º) top
S1—C4i1.7325 (14)C9—C101.520 (2)
S1—C21.7505 (14)C9—H9A0.9900
C2—C81.3968 (19)C9—H9B0.9900
C2—C31.4088 (19)C10—C111.5255 (19)
C3—C51.3965 (19)C10—H10A0.9900
C3—C41.4364 (18)C10—H10B0.9900
C4—C4i1.372 (3)C11—C121.504 (2)
C5—C61.3819 (19)C11—H11A0.9900
C5—H50.9500C11—H11B0.9900
C6—C71.406 (2)C12—O131.4246 (17)
C6—H60.9500C12—H12A0.9900
C7—C81.388 (2)C12—H12B0.9900
C7—C91.5084 (19)O13—H130.80 (3)
C8—H80.9500
C4i—S1—C290.67 (7)C10—C9—H9A109.1
C8—C2—C3121.46 (13)C7—C9—H9B109.1
C8—C2—S1125.66 (11)C10—C9—H9B109.1
C3—C2—S1112.88 (10)H9A—C9—H9B107.9
C5—C3—C2119.15 (12)C11—C10—C9113.67 (12)
C5—C3—C4131.09 (13)C11—C10—H10A108.8
C2—C3—C4109.75 (12)C9—C10—H10A108.8
C4i—C4—C3114.25 (15)C11—C10—H10B108.8
C4i—C4—S1i112.44 (14)C9—C10—H10B108.8
C3—C4—S1i133.30 (11)H10A—C10—H10B107.7
C6—C5—C3119.03 (14)C12—C11—C10111.78 (12)
C6—C5—H5120.5C12—C11—H11A109.3
C3—C5—H5120.5C10—C11—H11A109.3
C5—C6—C7122.02 (13)C12—C11—H11B109.3
C5—C6—H6119.0C10—C11—H11B109.3
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.33 (13)O13—C12—C11110.23 (12)
C8—C7—C9120.72 (14)O13—C12—H12A109.6
C6—C7—C9119.93 (13)C11—C12—H12A109.6
C7—C8—C2119.00 (14)O13—C12—H12B109.6
C7—C8—H8120.5C11—C12—H12B109.6
C2—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.41 (12)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.57 (14)C3—C5—C6—C70.3 (2)
C4i—S1—C2—C30.58 (11)C5—C6—C7—C80.4 (2)
C8—C2—C3—C51.1 (2)C5—C6—C7—C9177.80 (14)
S1—C2—C3—C5178.74 (11)C6—C7—C8—C20.3 (2)
C8—C2—C3—C4179.59 (13)C9—C7—C8—C2178.45 (13)
S1—C2—C3—C40.55 (15)C3—C2—C8—C71.0 (2)
C5—C3—C4—C4i178.97 (16)S1—C2—C8—C7178.81 (11)
C2—C3—C4—C4i0.2 (2)C8—C7—C9—C1079.61 (19)
C5—C3—C4—S1i1.3 (3)C6—C7—C9—C1098.56 (17)
C2—C3—C4—S1i179.51 (12)C7—C9—C10—C11176.11 (14)
C2—C3—C5—C60.4 (2)C9—C10—C11—C12175.07 (14)
C4—C3—C5—C6179.55 (14)C10—C11—C12—O13179.88 (13)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.802.042.8015 (10)160
C6—H6···S1iii0.953.334.1206 (14)142
C9—H9A···S1iii0.993.464.0958 (18)124
C10—H10A···S1iii0.993.333.9486 (19)122
C10—H10A···S1iv0.993.163.8532 (17)129
C11—H11B···S1iii0.993.424.1164 (18)129
C12—H12A···S1iv0.993.073.8224 (18)134
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A190) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.359 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.535 (3) ÅCell parameters from 7082 reflections
b = 5.078 (1) Åθ = 2.3–24.6°
c = 14.332 (1) ŵ = 0.29 mm1
β = 107.455 (15)°T = 190 K
V = 939.7 (3) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.022
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8316 measured reflectionsh = 1919
2767 independent reflectionsk = 67
2452 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.043H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.124 w = 1/[σ2(Fo2) + (0.0645P)2 + 0.3676P]
where P = (Fo2 + 2Fc2)/3
S = 1.09(Δ/σ)max = 0.001
2767 reflectionsΔρmax = 0.80 e Å3
121 parametersΔρmin = 0.50 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.007 (3)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64639 (3)0.32366 (8)0.53801 (3)0.03487 (14)
C20.64839 (11)0.5549 (3)0.62917 (10)0.0303 (3)
C30.55377 (11)0.6905 (3)0.61193 (10)0.0298 (3)
C40.48105 (11)0.5970 (3)0.52324 (10)0.0300 (3)
C50.54489 (12)0.8852 (3)0.67774 (11)0.0352 (3)
H50.4819660.9798590.6673040.042*
C60.62890 (12)0.9383 (3)0.75827 (10)0.0360 (3)
H60.6228661.0716330.8027440.043*
C70.72297 (12)0.8011 (3)0.77638 (10)0.0329 (3)
C80.73256 (11)0.6077 (3)0.71111 (11)0.0340 (3)
H80.7955040.5128240.7221100.041*
C90.81105 (13)0.8594 (3)0.86716 (11)0.0360 (3)
H9A0.8018781.0382570.8907500.043*
H9B0.8769800.8572330.8505800.043*
C100.81767 (14)0.6618 (3)0.94866 (11)0.0377 (3)
H10A0.7498650.6549520.9616230.045*
H10B0.8314170.4849390.9262740.045*
C110.90139 (12)0.7262 (3)1.04369 (10)0.0344 (3)
H11A0.9685580.7475321.0302650.041*
H11B0.8845210.8951871.0698120.041*
C120.91118 (13)0.5138 (3)1.11914 (11)0.0371 (3)
H12A0.8443480.4926101.1332190.045*
H12B0.9282840.3444121.0934550.045*
O130.99007 (10)0.5798 (2)1.20674 (8)0.0415 (3)
H130.9994 (14)0.457 (4)1.2444 (14)0.062*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0315 (2)0.0406 (2)0.0304 (2)0.00461 (13)0.00597 (14)0.00738 (13)
C20.0327 (6)0.0327 (7)0.0257 (6)0.0008 (5)0.0091 (5)0.0013 (5)
C30.0323 (6)0.0321 (7)0.0256 (6)0.0021 (5)0.0095 (5)0.0013 (5)
C40.0306 (6)0.0334 (7)0.0260 (6)0.0004 (5)0.0084 (5)0.0016 (5)
C50.0375 (7)0.0377 (7)0.0302 (6)0.0005 (6)0.0097 (5)0.0060 (6)
C60.0422 (8)0.0367 (8)0.0283 (6)0.0038 (6)0.0095 (6)0.0058 (5)
C70.0370 (7)0.0347 (7)0.0249 (6)0.0069 (5)0.0064 (5)0.0003 (5)
C80.0328 (6)0.0379 (7)0.0294 (6)0.0015 (5)0.0066 (5)0.0016 (5)
C90.0402 (7)0.0358 (7)0.0273 (6)0.0089 (6)0.0032 (5)0.0013 (5)
C100.0469 (8)0.0310 (7)0.0279 (6)0.0080 (6)0.0002 (6)0.0006 (5)
C110.0419 (7)0.0293 (7)0.0270 (6)0.0052 (6)0.0026 (5)0.0023 (5)
C120.0461 (8)0.0305 (7)0.0285 (6)0.0035 (6)0.0017 (5)0.0010 (5)
O130.0492 (6)0.0374 (6)0.0286 (5)0.0017 (5)0.0021 (4)0.0004 (4)
Geometric parameters (Å, º) top
S1—C4i1.7321 (15)C9—C101.522 (2)
S1—C21.7509 (14)C9—H9A0.9900
C2—C81.3951 (19)C9—H9B0.9900
C2—C31.409 (2)C10—C111.523 (2)
C3—C51.3961 (19)C10—H10A0.9900
C3—C41.4350 (18)C10—H10B0.9900
C4—C4i1.372 (3)C11—C121.505 (2)
C5—C61.382 (2)C11—H11A0.9900
C5—H50.9500C11—H11B0.9900
C6—C71.406 (2)C12—O131.4228 (17)
C6—H60.9500C12—H12A0.9900
C7—C81.389 (2)C12—H12B0.9900
C7—C91.507 (2)O13—H130.81 (3)
C8—H80.9500
C4i—S1—C290.71 (7)C10—C9—H9A109.1
C8—C2—C3121.56 (13)C7—C9—H9B109.1
C8—C2—S1125.67 (11)C10—C9—H9B109.1
C3—C2—S1112.77 (10)H9A—C9—H9B107.8
C5—C3—C2119.04 (13)C11—C10—C9113.67 (12)
C5—C3—C4131.11 (13)C11—C10—H10A108.8
C2—C3—C4109.84 (12)C9—C10—H10A108.8
C4i—C4—C3114.25 (16)C11—C10—H10B108.8
C4i—C4—S1i112.42 (14)C9—C10—H10B108.8
C3—C4—S1i133.33 (11)H10A—C10—H10B107.7
C6—C5—C3119.11 (14)C12—C11—C10111.73 (12)
C6—C5—H5120.4C12—C11—H11A109.3
C3—C5—H5120.4C10—C11—H11A109.3
C5—C6—C7122.02 (14)C12—C11—H11B109.3
C5—C6—H6119.0C10—C11—H11B109.3
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.24 (13)O13—C12—C11110.27 (13)
C8—C7—C9120.72 (14)O13—C12—H12A109.6
C6—C7—C9120.02 (14)C11—C12—H12A109.6
C7—C8—C2119.03 (14)O13—C12—H12B109.6
C7—C8—H8120.5C11—C12—H12B109.6
C2—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.49 (12)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.68 (14)C3—C5—C6—C70.4 (2)
C4i—S1—C2—C30.61 (11)C5—C6—C7—C80.6 (2)
C8—C2—C3—C51.1 (2)C5—C6—C7—C9177.76 (14)
S1—C2—C3—C5178.65 (11)C6—C7—C8—C20.0 (2)
C8—C2—C3—C4179.81 (13)C9—C7—C8—C2178.39 (13)
S1—C2—C3—C40.48 (16)C3—C2—C8—C70.9 (2)
C5—C3—C4—C4i178.96 (17)S1—C2—C8—C7178.82 (11)
C2—C3—C4—C4i0.0 (2)C8—C7—C9—C1079.83 (19)
C5—C3—C4—S1i1.6 (3)C6—C7—C9—C1098.52 (18)
C2—C3—C4—S1i179.42 (12)C7—C9—C10—C11176.09 (14)
C2—C3—C5—C60.4 (2)C9—C10—C11—C12175.08 (14)
C4—C3—C5—C6179.33 (15)C10—C11—C12—O13179.87 (14)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.812.032.8029 (10)160
C6—H6···S1iii0.953.334.1257 (15)142
C9—H9A···S1iii0.993.474.1021 (18)124
C10—H10A···S1iii0.993.333.9523 (19)123
C10—H10A···S1iv0.993.163.8563 (18)129
C11—H11B···S1iii0.993.434.1201 (19)129
C12—H12A···S1iv0.993.073.8253 (18)134
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A200) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.357 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.550 (2) ÅCell parameters from 7071 reflections
b = 5.078 (1) Åθ = 2.4–24.3°
c = 14.344 (2) ŵ = 0.29 mm1
β = 107.529 (17)°T = 200 K
V = 941.1 (2) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.023
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8206 measured reflectionsh = 1919
2773 independent reflectionsk = 67
2418 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.048H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.137 w = 1/[σ2(Fo2) + (0.0697P)2 + 0.4379P]
where P = (Fo2 + 2Fc2)/3
S = 1.10(Δ/σ)max = 0.001
2773 reflectionsΔρmax = 0.82 e Å3
121 parametersΔρmin = 0.64 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.012 (4)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64631 (3)0.32361 (9)0.53812 (3)0.03699 (15)
C20.64831 (12)0.5547 (3)0.62921 (11)0.0323 (3)
C30.55386 (12)0.6903 (3)0.61199 (11)0.0318 (3)
C40.48109 (12)0.5967 (3)0.52328 (11)0.0317 (3)
C50.54478 (13)0.8847 (4)0.67768 (12)0.0371 (3)
H50.4818790.9792810.6671960.044*
C60.62884 (14)0.9374 (4)0.75828 (11)0.0380 (4)
H60.6227851.0703260.8028500.046*
C70.72288 (13)0.8008 (3)0.77638 (11)0.0349 (3)
C80.73246 (13)0.6072 (4)0.71127 (11)0.0359 (3)
H80.7953060.5119470.7224050.043*
C90.81104 (14)0.8590 (4)0.86728 (12)0.0384 (4)
H9A0.8019901.0379690.8908190.046*
H9B0.8769280.8564580.8508090.046*
C100.81746 (15)0.6621 (3)0.94849 (12)0.0398 (4)
H10A0.7496760.6556270.9613050.048*
H10B0.8310730.4851350.9261350.048*
C110.90124 (14)0.7262 (3)1.04373 (11)0.0366 (3)
H11A0.9683590.7476261.0304110.044*
H11B0.8843960.8950811.0698840.044*
C120.91109 (15)0.5137 (3)1.11908 (12)0.0395 (4)
H12A0.8443170.4923351.1330710.047*
H12B0.9282510.3444361.0934300.047*
O130.98997 (11)0.5800 (3)1.20676 (9)0.0441 (3)
H130.9985 (15)0.458 (5)1.2451 (16)0.066*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0339 (2)0.0427 (3)0.0319 (2)0.00472 (15)0.00612 (15)0.00774 (15)
C20.0351 (7)0.0351 (8)0.0268 (6)0.0008 (6)0.0096 (5)0.0013 (5)
C30.0350 (7)0.0342 (8)0.0265 (6)0.0019 (6)0.0096 (5)0.0014 (5)
C40.0332 (7)0.0342 (8)0.0272 (6)0.0000 (6)0.0084 (5)0.0018 (5)
C50.0398 (8)0.0387 (8)0.0320 (7)0.0008 (6)0.0097 (6)0.0061 (6)
C60.0446 (9)0.0391 (9)0.0293 (7)0.0044 (7)0.0096 (6)0.0066 (6)
C70.0401 (8)0.0367 (8)0.0254 (6)0.0076 (6)0.0063 (6)0.0003 (5)
C80.0357 (7)0.0398 (8)0.0300 (7)0.0021 (6)0.0066 (6)0.0019 (6)
C90.0437 (8)0.0381 (8)0.0285 (7)0.0096 (7)0.0036 (6)0.0010 (6)
C100.0495 (9)0.0330 (8)0.0297 (7)0.0086 (7)0.0008 (6)0.0007 (6)
C110.0448 (8)0.0308 (7)0.0283 (7)0.0054 (6)0.0022 (6)0.0021 (6)
C120.0497 (9)0.0324 (8)0.0294 (7)0.0036 (7)0.0014 (6)0.0007 (6)
O130.0526 (7)0.0397 (7)0.0301 (6)0.0023 (6)0.0023 (5)0.0004 (5)
Geometric parameters (Å, º) top
S1—C4i1.7330 (16)C9—C101.517 (2)
S1—C21.7503 (16)C9—H9A0.9900
C2—C81.396 (2)C9—H9B0.9900
C2—C31.408 (2)C10—C111.525 (2)
C3—C51.395 (2)C10—H10A0.9900
C3—C41.436 (2)C10—H10B0.9900
C4—C4i1.371 (3)C11—C121.504 (2)
C5—C61.383 (2)C11—H11A0.9900
C5—H50.9500C11—H11B0.9900
C6—C71.405 (3)C12—O131.4239 (19)
C6—H60.9500C12—H12A0.9900
C7—C81.389 (2)C12—H12B0.9900
C7—C91.509 (2)O13—H130.81 (3)
C8—H80.9500
C4i—S1—C290.68 (7)C10—C9—H9A109.1
C8—C2—C3121.54 (15)C7—C9—H9B109.1
C8—C2—S1125.63 (13)C10—C9—H9B109.1
C3—C2—S1112.83 (11)H9A—C9—H9B107.8
C5—C3—C2119.20 (14)C11—C10—C9113.71 (14)
C5—C3—C4130.99 (15)C11—C10—H10A108.8
C2—C3—C4109.81 (14)C9—C10—H10A108.8
C4i—C4—C3114.28 (18)C11—C10—H10B108.8
C4i—C4—S1i112.39 (15)C9—C10—H10B108.8
C3—C4—S1i133.33 (12)H10A—C10—H10B107.7
C6—C5—C3118.92 (16)C12—C11—C10111.81 (14)
C6—C5—H5120.5C12—C11—H11A109.3
C3—C5—H5120.5C10—C11—H11A109.3
C5—C6—C7122.12 (15)C12—C11—H11B109.3
C5—C6—H6118.9C10—C11—H11B109.3
C7—C6—H6118.9H11A—C11—H11B107.9
C8—C7—C6119.26 (15)O13—C12—C11110.22 (14)
C8—C7—C9120.65 (16)O13—C12—H12A109.6
C6—C7—C9120.07 (15)C11—C12—H12A109.6
C7—C8—C2118.95 (16)O13—C12—H12B109.6
C7—C8—H8120.5C11—C12—H12B109.6
C2—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.44 (14)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.66 (16)C3—C5—C6—C70.3 (3)
C4i—S1—C2—C30.57 (13)C5—C6—C7—C80.3 (3)
C8—C2—C3—C51.1 (2)C5—C6—C7—C9177.81 (16)
S1—C2—C3—C5178.72 (13)C6—C7—C8—C20.3 (2)
C8—C2—C3—C4179.69 (15)C9—C7—C8—C2178.46 (15)
S1—C2—C3—C40.53 (17)C3—C2—C8—C71.0 (2)
C5—C3—C4—C4i178.94 (18)S1—C2—C8—C7178.72 (13)
C2—C3—C4—C4i0.2 (2)C8—C7—C9—C1079.8 (2)
C5—C3—C4—S1i1.4 (3)C6—C7—C9—C1098.3 (2)
C2—C3—C4—S1i179.51 (13)C7—C9—C10—C11176.08 (16)
C2—C3—C5—C60.4 (2)C9—C10—C11—C12174.94 (16)
C4—C3—C5—C6179.45 (16)C10—C11—C12—O13179.91 (16)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.812.032.8029 (10)159
C6—H6···S1iii0.953.344.1314 (17)143
C9—H9A···S1iii0.993.484.109 (2)124
C10—H10A···S1iii0.993.333.956 (2)123
C10—H10A···S1iv0.993.173.8614 (19)129
C11—H11B···S1iii0.993.434.123 (2)129
C12—H12A···S1iv0.993.073.8270 (19)134
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A210) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.355 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.569 (2) ÅCell parameters from 7094 reflections
b = 5.078 (1) Åθ = 2.4–24.1°
c = 14.355 (2) ŵ = 0.29 mm1
β = 107.612 (18)°T = 210 K
V = 942.7 (2) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.026
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8423 measured reflectionsh = 1919
2785 independent reflectionsk = 67
2507 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Primary atom site location: iterative
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.121H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.0657P)2 + 0.3341P]
where P = (Fo2 + 2Fc2)/3
2785 reflections(Δ/σ)max = 0.001
120 parametersΔρmax = 0.65 e Å3
0 restraintsΔρmin = 0.54 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64615 (3)0.32373 (8)0.53817 (2)0.03642 (13)
C20.64810 (10)0.5545 (3)0.62911 (9)0.0313 (3)
C30.55382 (10)0.6902 (3)0.61197 (9)0.0304 (3)
C40.48107 (10)0.5967 (3)0.52317 (9)0.0309 (3)
C50.54488 (11)0.8844 (3)0.67770 (10)0.0366 (3)
H50.4826970.9779180.6673130.044*
C60.62892 (12)0.9373 (3)0.75841 (10)0.0376 (3)
H60.6230081.0688420.8024840.045*
C70.72273 (11)0.8005 (3)0.77643 (9)0.0344 (3)
C80.73236 (11)0.6072 (3)0.71137 (10)0.0352 (3)
H80.7945320.5132650.7224200.042*
C90.81092 (12)0.8590 (3)0.86743 (10)0.0379 (3)
H9A0.8019551.0361340.8907010.046*
H9B0.8760710.8565060.8512110.046*
C100.81734 (13)0.6621 (3)0.94856 (10)0.0394 (3)
H10A0.7503540.6557650.9612390.047*
H10B0.8307480.4868360.9264570.047*
C110.90121 (12)0.7263 (3)1.04376 (9)0.0362 (3)
H11A0.9675400.7472491.0305560.043*
H11B0.8846610.8937631.0695360.043*
C120.91109 (12)0.5142 (3)1.11922 (10)0.0392 (3)
H12A0.8450800.4934471.1330530.047*
H12B0.9278850.3464441.0938820.047*
O130.98987 (9)0.5799 (2)1.20676 (7)0.0442 (3)
H130.9982 (13)0.461 (4)1.2439 (14)0.066*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.03197 (18)0.0430 (2)0.03142 (18)0.00506 (12)0.00521 (13)0.00803 (12)
C20.0327 (6)0.0350 (6)0.0256 (5)0.0006 (5)0.0079 (4)0.0017 (5)
C30.0322 (6)0.0333 (6)0.0255 (5)0.0017 (5)0.0084 (4)0.0015 (4)
C40.0302 (5)0.0354 (6)0.0264 (5)0.0004 (5)0.0072 (4)0.0018 (5)
C50.0376 (7)0.0395 (7)0.0313 (6)0.0010 (5)0.0086 (5)0.0067 (5)
C60.0442 (7)0.0384 (7)0.0287 (6)0.0040 (6)0.0089 (5)0.0067 (5)
C70.0387 (7)0.0372 (7)0.0245 (5)0.0081 (5)0.0054 (5)0.0000 (5)
C80.0334 (6)0.0400 (7)0.0295 (6)0.0015 (5)0.0053 (5)0.0015 (5)
C90.0422 (7)0.0380 (7)0.0279 (6)0.0100 (6)0.0020 (5)0.0008 (5)
C100.0486 (8)0.0322 (7)0.0291 (6)0.0091 (6)0.0006 (5)0.0009 (5)
C110.0436 (7)0.0308 (6)0.0278 (6)0.0054 (5)0.0014 (5)0.0021 (5)
C120.0483 (8)0.0324 (7)0.0291 (6)0.0041 (6)0.0001 (5)0.0010 (5)
O130.0516 (6)0.0404 (6)0.0297 (5)0.0019 (5)0.0040 (4)0.0003 (4)
Geometric parameters (Å, º) top
S1—C4i1.7316 (14)C9—C101.517 (2)
S1—C21.7486 (13)C9—H9A0.9800
C2—C81.3987 (18)C9—H9B0.9800
C2—C31.4074 (18)C10—C111.5258 (19)
C3—C51.3954 (18)C10—H10A0.9800
C3—C41.4364 (17)C10—H10B0.9800
C4—C4i1.370 (3)C11—C121.505 (2)
C5—C61.3840 (19)C11—H11A0.9800
C5—H50.9400C11—H11B0.9800
C6—C71.404 (2)C12—O131.4213 (16)
C6—H60.9400C12—H12A0.9800
C7—C81.388 (2)C12—H12B0.9800
C7—C91.5103 (19)O13—H130.79 (3)
C8—H80.9400
C4i—S1—C290.62 (6)C10—C9—H9A109.1
C8—C2—C3121.43 (12)C7—C9—H9B109.1
C8—C2—S1125.62 (11)C10—C9—H9B109.1
C3—C2—S1112.95 (9)H9A—C9—H9B107.9
C5—C3—C2119.22 (12)C11—C10—C9113.61 (12)
C5—C3—C4131.05 (13)C11—C10—H10A108.8
C2—C3—C4109.73 (11)C9—C10—H10A108.8
C4i—C4—C3114.19 (15)C11—C10—H10B108.8
C4i—C4—S1i112.51 (13)C9—C10—H10B108.8
C3—C4—S1i133.30 (10)H10A—C10—H10B107.7
C6—C5—C3119.02 (13)C12—C11—C10111.81 (12)
C6—C5—H5120.5C12—C11—H11A109.3
C3—C5—H5120.5C10—C11—H11A109.3
C5—C6—C7121.99 (13)C12—C11—H11B109.3
C5—C6—H6119.0C10—C11—H11B109.3
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.39 (12)O13—C12—C11110.35 (12)
C8—C7—C9120.64 (14)O13—C12—H12A109.6
C6—C7—C9119.95 (13)C11—C12—H12A109.6
C2—C8—C7118.95 (13)O13—C12—H12B109.6
C2—C8—H8120.5C11—C12—H12B109.6
C7—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.39 (12)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.66 (13)C3—C5—C6—C70.3 (2)
C4i—S1—C2—C30.58 (11)C5—C6—C7—C80.4 (2)
C8—C2—C3—C51.1 (2)C5—C6—C7—C9177.84 (13)
S1—C2—C3—C5178.72 (11)C3—C2—C8—C71.0 (2)
C8—C2—C3—C4179.74 (12)S1—C2—C8—C7178.77 (11)
S1—C2—C3—C40.49 (15)C6—C7—C8—C20.2 (2)
C5—C3—C4—C4i178.99 (16)C9—C7—C8—C2178.49 (13)
C2—C3—C4—C4i0.1 (2)C8—C7—C9—C1079.95 (18)
C5—C3—C4—S1i1.4 (2)C6—C7—C9—C1098.31 (17)
C2—C3—C4—S1i179.47 (11)C7—C9—C10—C11176.15 (14)
C2—C3—C5—C60.4 (2)C9—C10—C11—C12175.02 (14)
C4—C3—C5—C6179.40 (14)C10—C11—C12—O13179.89 (13)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.792.052.8030 (9)159
C6—H6···S1iii0.943.354.1336 (15)143
C9—H9A···S1iii0.983.494.1132 (18)124
C10—H10A···S1iii0.983.343.9594 (18)123
C10—H10A···S1iv0.983.183.8657 (16)129
C11—H11B···S1iii0.983.444.1275 (17)129
C12—H12A···S1iv0.983.083.8330 (17)134
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A220) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.352 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.587 (2) ÅCell parameters from 6932 reflections
b = 5.077 (1) Åθ = 2.2–25.5°
c = 14.368 (2) ŵ = 0.28 mm1
β = 107.690 (16)°T = 220 K
V = 944.3 (2) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.024
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8507 measured reflectionsh = 1919
2798 independent reflectionsk = 67
2563 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.038H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.117 w = 1/[σ2(Fo2) + (0.067P)2 + 0.2715P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max = 0.001
2798 reflectionsΔρmax = 0.70 e Å3
121 parametersΔρmin = 0.30 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.034 (4)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64601 (2)0.32374 (7)0.53824 (2)0.03750 (13)
C20.64812 (9)0.5542 (3)0.62923 (8)0.0320 (2)
C30.55384 (9)0.6901 (2)0.61200 (9)0.0314 (2)
C40.48110 (9)0.5966 (2)0.52319 (8)0.0315 (2)
C50.54487 (10)0.8842 (3)0.67770 (9)0.0377 (3)
H50.4827280.9776470.6672870.045*
C60.62874 (11)0.9370 (3)0.75832 (9)0.0386 (3)
H60.6228051.0683720.8023940.046*
C70.72264 (10)0.8003 (3)0.77644 (9)0.0353 (3)
C80.73220 (10)0.6073 (3)0.71140 (9)0.0362 (3)
H80.7943730.5136350.7224440.043*
C90.81079 (11)0.8587 (3)0.86744 (9)0.0393 (3)
H9A0.8018691.0359960.8906560.047*
H9B0.8758630.8561550.8512930.047*
C100.81719 (12)0.6618 (3)0.94856 (10)0.0407 (3)
H10A0.7502590.6555480.9611400.049*
H10B0.8305810.4864990.9265270.049*
C110.90099 (11)0.7262 (3)1.04378 (9)0.0370 (3)
H11A0.9672380.7473501.0306540.044*
H11B0.8844000.8935791.0695290.044*
C120.91101 (11)0.5143 (3)1.11913 (9)0.0403 (3)
H12A0.8450510.4931481.1327980.048*
H12B0.9279360.3466641.0938390.048*
O130.98962 (9)0.5801 (2)1.20679 (7)0.0458 (3)
H130.9986 (13)0.459 (4)1.2442 (13)0.069*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.03189 (18)0.0447 (2)0.03289 (18)0.00539 (11)0.00540 (12)0.00829 (11)
C20.0331 (5)0.0357 (6)0.0268 (5)0.0007 (4)0.0083 (4)0.0017 (4)
C30.0327 (5)0.0344 (6)0.0272 (5)0.0019 (4)0.0092 (4)0.0020 (4)
C40.0300 (5)0.0365 (6)0.0272 (5)0.0001 (4)0.0073 (4)0.0019 (4)
C50.0382 (6)0.0411 (7)0.0329 (6)0.0011 (5)0.0094 (5)0.0067 (5)
C60.0442 (7)0.0402 (7)0.0301 (5)0.0038 (5)0.0091 (5)0.0070 (5)
C70.0383 (6)0.0386 (6)0.0259 (5)0.0083 (5)0.0053 (4)0.0002 (4)
C80.0330 (6)0.0422 (7)0.0306 (5)0.0016 (5)0.0053 (4)0.0015 (5)
C90.0428 (7)0.0400 (7)0.0292 (5)0.0104 (5)0.0023 (5)0.0012 (5)
C100.0495 (7)0.0336 (6)0.0304 (6)0.0093 (5)0.0005 (5)0.0009 (4)
C110.0438 (6)0.0316 (6)0.0294 (5)0.0055 (5)0.0020 (5)0.0025 (4)
C120.0487 (7)0.0339 (6)0.0302 (5)0.0043 (5)0.0002 (5)0.0012 (5)
O130.0535 (6)0.0414 (5)0.0310 (4)0.0024 (4)0.0046 (4)0.0003 (4)
Geometric parameters (Å, º) top
S1—C4i1.7318 (12)C9—C101.5180 (19)
S1—C21.7481 (12)C9—H9A0.9800
C2—C81.3971 (16)C9—H9B0.9800
C2—C31.4093 (17)C10—C111.5260 (18)
C3—C51.3953 (17)C10—H10A0.9800
C3—C41.4367 (16)C10—H10B0.9800
C4—C4i1.370 (2)C11—C121.5026 (18)
C5—C61.3820 (17)C11—H11A0.9800
C5—H50.9400C11—H11B0.9800
C6—C71.405 (2)C12—O131.4217 (15)
C6—H60.9400C12—H12A0.9800
C7—C81.3869 (18)C12—H12B0.9800
C7—C91.5101 (17)O13—H130.80 (2)
C8—H80.9400
C4i—S1—C290.69 (6)C10—C9—H9A109.1
C8—C2—C3121.33 (11)C7—C9—H9B109.1
C8—C2—S1125.78 (10)C10—C9—H9B109.1
C3—C2—S1112.89 (9)H9A—C9—H9B107.9
C5—C3—C2119.25 (11)C11—C10—C9113.59 (11)
C5—C3—C4131.03 (11)C11—C10—H10A108.8
C2—C3—C4109.72 (11)C9—C10—H10A108.8
C4i—C4—C3114.22 (13)C11—C10—H10B108.8
C4i—C4—S1i112.48 (12)C9—C10—H10B108.8
C3—C4—S1i133.30 (9)H10A—C10—H10B107.7
C6—C5—C3118.99 (12)C12—C11—C10111.84 (11)
C6—C5—H5120.5C12—C11—H11A109.2
C3—C5—H5120.5C10—C11—H11A109.2
C5—C6—C7122.03 (12)C12—C11—H11B109.2
C5—C6—H6119.0C10—C11—H11B109.2
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.31 (11)O13—C12—C11110.44 (11)
C8—C7—C9120.68 (13)O13—C12—H12A109.6
C6—C7—C9119.99 (12)C11—C12—H12A109.6
C2—C8—C7119.07 (12)O13—C12—H12B109.6
C2—C8—H8120.5C11—C12—H12B109.6
C7—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.37 (11)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.80 (12)C3—C5—C6—C70.3 (2)
C4i—S1—C2—C30.61 (10)C5—C6—C7—C80.4 (2)
C8—C2—C3—C50.89 (19)C5—C6—C7—C9177.87 (12)
S1—C2—C3—C5178.72 (10)C3—C2—C8—C70.8 (2)
C8—C2—C3—C4179.81 (11)S1—C2—C8—C7178.76 (10)
S1—C2—C3—C40.58 (13)C6—C7—C8—C20.1 (2)
C5—C3—C4—C4i178.96 (15)C9—C7—C8—C2178.43 (12)
C2—C3—C4—C4i0.22 (19)C8—C7—C9—C1080.06 (17)
C5—C3—C4—S1i1.3 (2)C6—C7—C9—C1098.21 (16)
C2—C3—C4—S1i179.48 (10)C7—C9—C10—C11176.12 (13)
C2—C3—C5—C60.3 (2)C9—C10—C11—C12174.93 (13)
C4—C3—C5—C6179.44 (13)C10—C11—C12—O13179.97 (12)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.802.042.8022 (8)160
C6—H6···S1iii0.943.354.1392 (14)143
C9—H9A···S1iii0.983.504.1198 (17)124
C10—H10A···S1iii0.983.343.9639 (17)123
C10—H10A···S1iv0.983.183.8687 (15)129
C11—H11B···S1iii0.983.444.1306 (16)129
C12—H12A···S1iv0.983.083.8364 (15)135
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A230) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.350 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.606 (2) ÅCell parameters from 6988 reflections
b = 5.077 (1) Åθ = 2.2–24.4°
c = 14.379 (2) ŵ = 0.28 mm1
β = 107.770 (18)°T = 230 K
V = 945.9 (2) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.024
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8516 measured reflectionsh = 1919
2802 independent reflectionsk = 67
2550 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.039H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.123 w = 1/[σ2(Fo2) + (0.0726P)2 + 0.2488P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max = 0.001
2802 reflectionsΔρmax = 0.67 e Å3
121 parametersΔρmin = 0.30 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.038 (5)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64588 (2)0.32379 (7)0.53831 (2)0.03939 (14)
C20.64803 (9)0.5542 (3)0.62927 (8)0.0336 (2)
C30.55384 (10)0.6899 (2)0.61204 (9)0.0328 (2)
C40.48108 (9)0.5966 (3)0.52318 (8)0.0330 (2)
C50.54490 (11)0.8838 (3)0.67762 (10)0.0395 (3)
H50.4828480.9773740.6671020.047*
C60.62881 (11)0.9364 (3)0.75848 (9)0.0405 (3)
H60.6228391.0673700.8026440.049*
C70.72250 (11)0.8001 (3)0.77653 (9)0.0371 (3)
C80.73210 (10)0.6071 (3)0.71146 (9)0.0382 (3)
H80.7942120.5134660.7225200.046*
C90.81070 (12)0.8586 (3)0.86742 (10)0.0412 (3)
H9A0.8019421.0359790.8905610.049*
H9B0.8756490.8555240.8512750.049*
C100.81706 (12)0.6615 (3)0.94872 (10)0.0424 (3)
H10A0.7502470.6557630.9613050.051*
H10B0.8302880.4860780.9267640.051*
C110.90089 (11)0.7260 (3)1.04379 (9)0.0390 (3)
H11A0.9670190.7468001.0306250.047*
H11B0.8844500.8935331.0694660.047*
C120.91095 (12)0.5147 (3)1.11910 (10)0.0423 (3)
H12A0.8450720.4937581.1327440.051*
H12B0.9277310.3468701.0938620.051*
O130.98953 (9)0.5802 (2)1.20674 (7)0.0481 (3)
H130.9976 (13)0.457 (4)1.2457 (13)0.072*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.03333 (19)0.0470 (2)0.03469 (19)0.00566 (11)0.00573 (13)0.00871 (12)
C20.0347 (5)0.0372 (6)0.0281 (5)0.0006 (4)0.0086 (4)0.0015 (4)
C30.0342 (5)0.0362 (6)0.0278 (5)0.0021 (4)0.0092 (4)0.0018 (4)
C40.0311 (5)0.0383 (6)0.0286 (5)0.0004 (4)0.0077 (4)0.0022 (4)
C50.0401 (6)0.0429 (7)0.0343 (6)0.0011 (5)0.0098 (5)0.0067 (5)
C60.0457 (7)0.0424 (7)0.0317 (6)0.0040 (5)0.0093 (5)0.0074 (5)
C70.0404 (6)0.0403 (6)0.0275 (5)0.0091 (5)0.0058 (4)0.0003 (4)
C80.0343 (6)0.0445 (7)0.0329 (6)0.0021 (5)0.0058 (4)0.0022 (5)
C90.0448 (7)0.0418 (7)0.0306 (5)0.0113 (5)0.0021 (5)0.0010 (5)
C100.0513 (8)0.0355 (6)0.0313 (6)0.0099 (5)0.0008 (5)0.0012 (5)
C110.0459 (7)0.0333 (6)0.0313 (6)0.0059 (5)0.0022 (5)0.0026 (5)
C120.0509 (7)0.0356 (6)0.0319 (6)0.0046 (5)0.0002 (5)0.0014 (5)
O130.0557 (6)0.0435 (6)0.0326 (5)0.0024 (5)0.0050 (4)0.0002 (4)
Geometric parameters (Å, º) top
S1—C4i1.7311 (13)C9—C101.5208 (19)
S1—C21.7484 (13)C9—H9A0.9800
C2—C81.3971 (17)C9—H9B0.9800
C2—C31.4089 (17)C10—C111.5248 (18)
C3—C51.3937 (17)C10—H10A0.9800
C3—C41.4371 (16)C10—H10B0.9800
C4—C4i1.371 (2)C11—C121.5006 (19)
C5—C61.3843 (18)C11—H11A0.9800
C5—H50.9400C11—H11B0.9800
C6—C71.403 (2)C12—O131.4210 (16)
C6—H60.9400C12—H12A0.9800
C7—C81.3881 (19)C12—H12B0.9800
C7—C91.5096 (18)O13—H130.82 (2)
C8—H80.9400
C4i—S1—C290.69 (6)C10—C9—H9A109.1
C8—C2—C3121.38 (12)C7—C9—H9B109.1
C8—C2—S1125.72 (10)C10—C9—H9B109.1
C3—C2—S1112.90 (9)H9A—C9—H9B107.9
C5—C3—C2119.27 (11)C11—C10—C9113.55 (11)
C5—C3—C4130.98 (12)C11—C10—H10A108.9
C2—C3—C4109.74 (11)C9—C10—H10A108.9
C4i—C4—C3114.15 (14)C11—C10—H10B108.9
C4i—C4—S1i112.51 (12)C9—C10—H10B108.9
C3—C4—S1i133.34 (10)H10A—C10—H10B107.7
C6—C5—C3118.99 (13)C12—C11—C10111.84 (11)
C6—C5—H5120.5C12—C11—H11A109.2
C3—C5—H5120.5C10—C11—H11A109.2
C5—C6—C7122.00 (12)C12—C11—H11B109.2
C5—C6—H6119.0C10—C11—H11B109.2
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.36 (12)O13—C12—C11110.54 (11)
C8—C7—C9120.59 (13)O13—C12—H12A109.5
C6—C7—C9120.02 (12)C11—C12—H12A109.5
C2—C8—C7118.99 (13)O13—C12—H12B109.5
C2—C8—H8120.5C11—C12—H12B109.5
C7—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.33 (11)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.78 (13)C3—C5—C6—C70.1 (2)
C4i—S1—C2—C30.55 (10)C5—C6—C7—C80.3 (2)
C8—C2—C3—C50.97 (19)C5—C6—C7—C9178.06 (13)
S1—C2—C3—C5178.71 (10)C3—C2—C8—C70.8 (2)
C8—C2—C3—C4179.80 (12)S1—C2—C8—C7178.80 (10)
S1—C2—C3—C40.52 (14)C6—C7—C8—C20.2 (2)
C5—C3—C4—C4i178.92 (15)C9—C7—C8—C2178.53 (12)
C2—C3—C4—C4i0.19 (19)C8—C7—C9—C1080.28 (17)
C5—C3—C4—S1i1.4 (2)C6—C7—C9—C1098.02 (16)
C2—C3—C4—S1i179.52 (11)C7—C9—C10—C11176.12 (13)
C2—C3—C5—C60.5 (2)C9—C10—C11—C12174.90 (13)
C4—C3—C5—C6179.51 (13)C10—C11—C12—O13180.00 (13)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.822.022.8030 (9)158
C6—H6···S1iii0.943.354.1419 (14)143
C9—H9A···S1iii0.983.504.1268 (17)124
C10—H10A···S1iii0.983.343.9677 (18)123
C10—H10A···S1iv0.983.183.8713 (16)129
C11—H11B···S1iii0.983.454.1356 (16)129
C12—H12A···S1iv0.983.093.8409 (16)135
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A240) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.348 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.625 (2) ÅCell parameters from 6920 reflections
b = 5.076 (1) Åθ = 2.5–24.5°
c = 14.392 (2) ŵ = 0.28 mm1
β = 107.852 (19)°T = 240 K
V = 947.4 (2) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.026
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8471 measured reflectionsh = 1919
2793 independent reflectionsk = 67
2534 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.040H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.121 w = 1/[σ2(Fo2) + (0.0699P)2 + 0.272P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max = 0.001
2793 reflectionsΔρmax = 0.65 e Å3
121 parametersΔρmin = 0.31 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.036 (5)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64574 (2)0.32381 (7)0.53835 (2)0.04124 (14)
C20.64790 (10)0.5542 (3)0.62927 (9)0.0351 (3)
C30.55388 (10)0.6896 (3)0.61211 (9)0.0343 (3)
C40.48115 (9)0.5965 (3)0.52315 (9)0.0345 (3)
C50.54499 (11)0.8832 (3)0.67771 (10)0.0412 (3)
H50.4829720.9766990.6672200.049*
C60.62887 (11)0.9358 (3)0.75855 (9)0.0424 (3)
H60.6229701.0666880.8027310.051*
C70.72235 (11)0.7997 (3)0.77650 (9)0.0391 (3)
C80.73185 (10)0.6072 (3)0.71158 (10)0.0398 (3)
H80.7938960.5134330.7227330.048*
C90.81049 (12)0.8580 (3)0.86756 (10)0.0431 (3)
H9A0.8016921.0353840.8907030.052*
H9B0.8753720.8552750.8514980.052*
C100.81710 (13)0.6614 (3)0.94869 (10)0.0448 (3)
H10A0.7503530.6551630.9611690.054*
H10B0.8304750.4860480.9267910.054*
C110.90075 (12)0.7261 (3)1.04380 (9)0.0410 (3)
H11A0.9668050.7473671.0307710.049*
H11B0.8841660.8934951.0694430.049*
C120.91094 (12)0.5146 (3)1.11903 (10)0.0445 (3)
H12A0.8451200.4931161.1325040.053*
H12B0.9279330.3469751.0938590.053*
O130.98933 (9)0.5806 (2)1.20674 (7)0.0506 (3)
H130.9983 (14)0.457 (4)1.2449 (14)0.076*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.03491 (19)0.0493 (2)0.03614 (19)0.00581 (12)0.00589 (13)0.00905 (12)
C20.0362 (6)0.0392 (6)0.0293 (5)0.0012 (5)0.0090 (4)0.0018 (4)
C30.0361 (6)0.0375 (6)0.0293 (5)0.0023 (4)0.0099 (4)0.0017 (4)
C40.0327 (5)0.0401 (6)0.0296 (5)0.0002 (4)0.0081 (4)0.0021 (4)
C50.0418 (6)0.0443 (7)0.0360 (6)0.0014 (5)0.0099 (5)0.0069 (5)
C60.0485 (7)0.0437 (7)0.0332 (6)0.0039 (5)0.0099 (5)0.0075 (5)
C70.0427 (6)0.0425 (7)0.0288 (5)0.0095 (5)0.0059 (5)0.0002 (5)
C80.0359 (6)0.0463 (7)0.0337 (6)0.0019 (5)0.0056 (5)0.0017 (5)
C90.0468 (7)0.0439 (7)0.0320 (6)0.0116 (6)0.0022 (5)0.0013 (5)
C100.0547 (8)0.0373 (7)0.0329 (6)0.0100 (6)0.0004 (5)0.0012 (5)
C110.0478 (7)0.0358 (6)0.0325 (6)0.0060 (5)0.0020 (5)0.0028 (5)
C120.0530 (8)0.0377 (7)0.0335 (6)0.0049 (6)0.0004 (5)0.0014 (5)
O130.0581 (6)0.0463 (6)0.0344 (5)0.0024 (5)0.0052 (4)0.0000 (4)
Geometric parameters (Å, º) top
S1—C4i1.7313 (13)C9—C101.517 (2)
S1—C21.7485 (13)C9—H9A0.9800
C2—C81.3975 (17)C9—H9B0.9800
C2—C31.4071 (18)C10—C111.5244 (18)
C3—C51.3938 (18)C10—H10A0.9800
C3—C41.4375 (16)C10—H10B0.9800
C4—C4i1.370 (2)C11—C121.500 (2)
C5—C61.3841 (18)C11—H11A0.9800
C5—H50.9400C11—H11B0.9800
C6—C71.402 (2)C12—O131.4212 (16)
C6—H60.9400C12—H12A0.9800
C7—C81.385 (2)C12—H12B0.9800
C7—C91.5107 (18)O13—H130.82 (3)
C8—H80.9400
C4i—S1—C290.66 (6)C10—C9—H9A109.1
C8—C2—C3121.29 (12)C7—C9—H9B109.1
C8—C2—S1125.77 (10)C10—C9—H9B109.1
C3—C2—S1112.93 (9)H9A—C9—H9B107.8
C5—C3—C2119.27 (12)C11—C10—C9113.64 (11)
C5—C3—C4130.97 (12)C11—C10—H10A108.8
C2—C3—C4109.75 (11)C9—C10—H10A108.8
C4i—C4—C3114.15 (14)C11—C10—H10B108.8
C4i—C4—S1i112.51 (12)C9—C10—H10B108.8
C3—C4—S1i133.34 (10)H10A—C10—H10B107.7
C6—C5—C3118.98 (13)C12—C11—C10111.85 (11)
C6—C5—H5120.5C12—C11—H11A109.2
C3—C5—H5120.5C10—C11—H11A109.2
C5—C6—C7121.98 (13)C12—C11—H11B109.2
C5—C6—H6119.0C10—C11—H11B109.2
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.40 (12)O13—C12—C11110.51 (12)
C8—C7—C9120.63 (13)O13—C12—H12A109.5
C6—C7—C9119.95 (13)C11—C12—H12A109.5
C2—C8—C7119.07 (13)O13—C12—H12B109.5
C2—C8—H8120.5C11—C12—H12B109.5
C7—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.50 (11)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.69 (13)C3—C5—C6—C70.2 (2)
C4i—S1—C2—C30.47 (10)C5—C6—C7—C80.2 (2)
C8—C2—C3—C51.1 (2)C5—C6—C7—C9177.94 (13)
S1—C2—C3—C5178.76 (10)C3—C2—C8—C71.0 (2)
C8—C2—C3—C4179.79 (12)S1—C2—C8—C7178.82 (10)
S1—C2—C3—C40.36 (14)C6—C7—C8—C20.3 (2)
C5—C3—C4—C4i178.97 (15)C9—C7—C8—C2178.51 (12)
C2—C3—C4—C4i0.0 (2)C8—C7—C9—C1080.18 (18)
C5—C3—C4—S1i1.5 (2)C6—C7—C9—C1097.98 (17)
C2—C3—C4—S1i179.55 (11)C7—C9—C10—C11176.05 (14)
C2—C3—C5—C60.5 (2)C9—C10—C11—C12174.89 (14)
C4—C3—C5—C6179.40 (14)C10—C11—C12—O13179.95 (13)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.822.022.8026 (9)159
C6—H6···S1iii0.943.364.1462 (14)143
C9—H9A···S1iii0.983.514.1319 (18)124
C10—H10A···S1iii0.983.353.9738 (18)123
C10—H10A···S1iv0.983.193.8769 (16)129
C11—H11B···S1iii0.983.454.1390 (17)129
C12—H12A···S1iv0.983.093.8449 (16)135
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A250) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.345 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.644 (3) ÅCell parameters from 7096 reflections
b = 5.076 (1) Åθ = 2.3–25.4°
c = 14.405 (3) ŵ = 0.28 mm1
β = 107.94 (2)°T = 250 K
V = 949.2 (3) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.024
Rotating crystal scansθmax = 29.9°, θmin = 1.6°
8491 measured reflectionsh = 1919
2806 independent reflectionsk = 67
2530 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.039H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.119 w = 1/[σ2(Fo2) + (0.0676P)2 + 0.277P]
where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max = 0.001
2806 reflectionsΔρmax = 0.63 e Å3
121 parametersΔρmin = 0.27 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.035 (5)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64559 (2)0.32387 (7)0.53841 (2)0.04310 (13)
C20.64784 (10)0.5539 (3)0.62938 (9)0.0366 (3)
C30.55390 (10)0.6894 (2)0.61213 (9)0.0357 (3)
C40.48125 (9)0.5965 (3)0.52311 (9)0.0359 (3)
C50.54503 (11)0.8828 (3)0.67774 (10)0.0431 (3)
H50.4830290.9759850.6672630.052*
C60.62877 (11)0.9354 (3)0.75848 (10)0.0445 (3)
H60.6229031.0664650.8025690.053*
C70.72223 (11)0.7992 (3)0.77659 (9)0.0407 (3)
C80.73177 (10)0.6068 (3)0.71171 (10)0.0417 (3)
H80.7937800.5132020.7228940.050*
C90.81036 (12)0.8577 (3)0.86769 (10)0.0452 (3)
H9A0.8015341.0350790.8907950.054*
H9B0.8751570.8550830.8517000.054*
C100.81702 (13)0.6614 (3)0.94865 (10)0.0462 (3)
H10A0.7503580.6551680.9610580.055*
H10B0.8303340.4860490.9267360.055*
C110.90064 (12)0.7258 (3)1.04380 (9)0.0427 (3)
H11A0.9666320.7467571.0308490.051*
H11B0.8841790.8933111.0693730.051*
C120.91084 (12)0.5148 (3)1.11903 (10)0.0468 (3)
H12A0.8451100.4936541.1324820.056*
H12B0.9277100.3470171.0939540.056*
O130.98922 (9)0.5808 (2)1.20666 (8)0.0528 (3)
H130.9979 (13)0.457 (4)1.2453 (13)0.079*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.03661 (19)0.0514 (2)0.03782 (19)0.00608 (12)0.00634 (13)0.00933 (13)
C20.0376 (6)0.0409 (6)0.0304 (5)0.0010 (5)0.0092 (4)0.0019 (4)
C30.0378 (6)0.0388 (6)0.0305 (5)0.0024 (4)0.0105 (4)0.0020 (4)
C40.0341 (5)0.0415 (6)0.0310 (5)0.0004 (5)0.0086 (4)0.0019 (5)
C50.0438 (7)0.0472 (7)0.0367 (6)0.0014 (5)0.0100 (5)0.0076 (5)
C60.0511 (7)0.0461 (7)0.0344 (6)0.0049 (6)0.0105 (5)0.0079 (5)
C70.0443 (7)0.0443 (7)0.0300 (5)0.0097 (5)0.0063 (5)0.0000 (5)
C80.0378 (6)0.0480 (7)0.0357 (6)0.0020 (5)0.0063 (5)0.0019 (5)
C90.0491 (7)0.0460 (7)0.0336 (6)0.0119 (6)0.0027 (5)0.0014 (5)
C100.0559 (8)0.0387 (7)0.0344 (6)0.0099 (6)0.0005 (5)0.0015 (5)
C110.0498 (7)0.0373 (6)0.0341 (6)0.0062 (5)0.0025 (5)0.0030 (5)
C120.0555 (8)0.0397 (7)0.0354 (6)0.0053 (6)0.0006 (5)0.0016 (5)
O130.0611 (7)0.0475 (6)0.0361 (5)0.0024 (5)0.0053 (4)0.0002 (4)
Geometric parameters (Å, º) top
S1—C4i1.7318 (13)C9—C101.515 (2)
S1—C21.7483 (13)C9—H9A0.9800
C2—C81.3977 (17)C9—H9B0.9800
C2—C31.4076 (18)C10—C111.5244 (19)
C3—C51.3935 (18)C10—H10A0.9800
C3—C41.4375 (17)C10—H10B0.9800
C4—C4i1.369 (2)C11—C121.499 (2)
C5—C61.3825 (19)C11—H11A0.9800
C5—H50.9400C11—H11B0.9800
C6—C71.403 (2)C12—O131.4206 (16)
C6—H60.9400C12—H12A0.9800
C7—C81.385 (2)C12—H12B0.9800
C7—C91.5114 (18)O13—H130.82 (3)
C8—H80.9400
C4i—S1—C290.67 (6)C10—C9—H9A109.1
C8—C2—C3121.29 (12)C7—C9—H9B109.1
C8—C2—S1125.80 (11)C10—C9—H9B109.1
C3—C2—S1112.90 (9)H9A—C9—H9B107.8
C5—C3—C2119.28 (12)C11—C10—C9113.71 (12)
C5—C3—C4130.99 (12)C11—C10—H10A108.8
C2—C3—C4109.72 (11)C9—C10—H10A108.8
C4i—C4—C3114.21 (14)C11—C10—H10B108.8
C4i—C4—S1i112.49 (12)C9—C10—H10B108.8
C3—C4—S1i133.30 (10)H10A—C10—H10B107.7
C6—C5—C3119.00 (13)C12—C11—C10111.97 (12)
C6—C5—H5120.5C12—C11—H11A109.2
C3—C5—H5120.5C10—C11—H11A109.2
C5—C6—C7121.99 (13)C12—C11—H11B109.2
C5—C6—H6119.0C10—C11—H11B109.2
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.40 (12)O13—C12—C11110.54 (12)
C8—C7—C9120.62 (13)O13—C12—H12A109.5
C6—C7—C9119.95 (13)C11—C12—H12A109.5
C2—C8—C7119.03 (13)O13—C12—H12B109.5
C2—C8—H8120.5C11—C12—H12B109.5
C7—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.48 (12)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.71 (13)C3—C5—C6—C70.3 (2)
C4i—S1—C2—C30.57 (10)C5—C6—C7—C80.4 (2)
C8—C2—C3—C51.0 (2)C5—C6—C7—C9177.93 (13)
S1—C2—C3—C5178.76 (10)C3—C2—C8—C70.9 (2)
C8—C2—C3—C4179.86 (12)S1—C2—C8—C7178.78 (11)
S1—C2—C3—C40.40 (14)C6—C7—C8—C20.3 (2)
C5—C3—C4—C4i179.08 (15)C9—C7—C8—C2178.53 (12)
C2—C3—C4—C4i0.0 (2)C8—C7—C9—C1080.22 (18)
C5—C3—C4—S1i1.5 (2)C6—C7—C9—C1098.04 (17)
C2—C3—C4—S1i179.44 (11)C7—C9—C10—C11176.10 (14)
C2—C3—C5—C60.3 (2)C9—C10—C11—C12174.99 (14)
C4—C3—C5—C6179.31 (14)C10—C11—C12—O13179.97 (13)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.822.022.8037 (9)159
C6—H6···S1iii0.943.364.1516 (16)143
C9—H9A···S1iii0.983.514.1374 (19)124
C10—H10A···S1iii0.983.363.9788 (18)123
C10—H10A···S1iv0.983.193.8825 (16)129
C11—H11B···S1iii0.983.464.1443 (18)129
C12—H12A···S1iv0.983.093.8488 (17)135
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A260) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.343 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.664 (4) ÅCell parameters from 6937 reflections
b = 5.075 (1) Åθ = 2.4–25.7°
c = 14.419 (4) ŵ = 0.28 mm1
β = 108.02 (3)°T = 260 K
V = 950.8 (4) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.026
Rotating crystal scansθmax = 29.9°, θmin = 1.5°
8501 measured reflectionsh = 1919
2820 independent reflectionsk = 67
2523 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.041H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.126 w = 1/[σ2(Fo2) + (0.0729P)2 + 0.2289P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.007
2820 reflectionsΔρmax = 0.61 e Å3
121 parametersΔρmin = 0.33 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.039 (6)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64544 (2)0.32385 (8)0.53848 (2)0.04517 (14)
C20.64781 (10)0.5539 (3)0.62946 (9)0.0384 (3)
C30.55387 (10)0.6892 (3)0.61214 (9)0.0374 (3)
C40.48133 (10)0.5963 (3)0.52310 (9)0.0377 (3)
C50.54504 (11)0.8824 (3)0.67779 (10)0.0452 (3)
H50.4837760.9746350.6674250.054*
C60.62873 (12)0.9348 (3)0.75854 (10)0.0464 (3)
H60.6228861.0640720.8022310.056*
C70.72226 (11)0.7991 (3)0.77666 (9)0.0427 (3)
C80.73161 (11)0.6065 (3)0.71170 (10)0.0437 (3)
H80.7928510.5136680.7227780.052*
C90.81021 (12)0.8574 (3)0.86774 (10)0.0476 (3)
H9A0.8015091.0330870.8905170.057*
H9B0.8742790.8547110.8520110.057*
C100.81694 (13)0.6614 (3)0.94873 (10)0.0486 (3)
H10A0.7510290.6553240.9609190.058*
H10B0.8300910.4877440.9271400.058*
C110.90046 (12)0.7258 (3)1.04389 (10)0.0450 (3)
H11A0.9656950.7467091.0311570.054*
H11B0.8841520.8916801.0691400.054*
C120.91075 (13)0.5150 (3)1.11909 (10)0.0490 (3)
H12A0.8457770.4939601.1323320.059*
H12B0.9274510.3488771.0943320.059*
O130.98905 (10)0.5811 (2)1.20671 (8)0.0556 (3)
H130.9972 (14)0.459 (5)1.2452 (14)0.083*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0386 (2)0.0539 (2)0.0393 (2)0.00628 (13)0.00669 (13)0.00964 (13)
C20.0397 (6)0.0425 (6)0.0320 (5)0.0010 (5)0.0097 (4)0.0016 (5)
C30.0393 (6)0.0410 (6)0.0316 (5)0.0029 (5)0.0107 (4)0.0018 (4)
C40.0363 (5)0.0433 (6)0.0324 (5)0.0000 (5)0.0091 (4)0.0021 (5)
C50.0461 (7)0.0490 (7)0.0390 (6)0.0015 (6)0.0108 (5)0.0076 (5)
C60.0528 (8)0.0481 (7)0.0363 (6)0.0052 (6)0.0111 (5)0.0086 (5)
C70.0468 (7)0.0462 (7)0.0314 (6)0.0100 (5)0.0067 (5)0.0001 (5)
C80.0401 (6)0.0502 (7)0.0374 (6)0.0017 (5)0.0070 (5)0.0015 (5)
C90.0519 (8)0.0485 (7)0.0352 (6)0.0133 (6)0.0029 (5)0.0015 (5)
C100.0587 (8)0.0405 (7)0.0364 (6)0.0102 (6)0.0003 (6)0.0016 (5)
C110.0524 (7)0.0392 (6)0.0354 (6)0.0068 (5)0.0017 (5)0.0035 (5)
C120.0583 (8)0.0411 (7)0.0369 (6)0.0051 (6)0.0007 (5)0.0009 (5)
O130.0645 (7)0.0498 (6)0.0377 (5)0.0028 (5)0.0057 (5)0.0002 (4)
Geometric parameters (Å, º) top
S1—C4i1.7324 (14)C9—C101.515 (2)
S1—C21.7489 (13)C9—H9A0.9700
C2—C81.3959 (18)C9—H9B0.9700
C2—C31.4082 (18)C10—C111.5241 (19)
C3—C51.3939 (18)C10—H10A0.9700
C3—C41.4371 (17)C10—H10B0.9700
C4—C4i1.368 (3)C11—C121.499 (2)
C5—C61.3820 (19)C11—H11A0.9700
C5—H50.9300C11—H11B0.9700
C6—C71.403 (2)C12—O131.4201 (17)
C6—H60.9300C12—H12A0.9700
C7—C81.387 (2)C12—H12B0.9700
C7—C91.5100 (19)O13—H130.82 (3)
C8—H80.9300
C4i—S1—C290.68 (6)C10—C9—H9A109.1
C8—C2—C3121.37 (12)C7—C9—H9B109.1
C8—C2—S1125.79 (11)C10—C9—H9B109.1
C3—C2—S1112.84 (9)H9A—C9—H9B107.8
C5—C3—C2119.22 (12)C11—C10—C9113.78 (12)
C5—C3—C4131.05 (12)C11—C10—H10A108.8
C2—C3—C4109.72 (11)C9—C10—H10A108.8
C4i—C4—C3114.29 (14)C11—C10—H10B108.8
C4i—C4—S1i112.46 (13)C9—C10—H10B108.8
C3—C4—S1i133.25 (10)H10A—C10—H10B107.7
C6—C5—C3118.99 (14)C12—C11—C10112.02 (12)
C6—C5—H5120.5C12—C11—H11A109.2
C3—C5—H5120.5C10—C11—H11A109.2
C5—C6—C7122.06 (13)C12—C11—H11B109.2
C5—C6—H6119.0C10—C11—H11B109.2
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.28 (13)O13—C12—C11110.57 (12)
C8—C7—C9120.72 (14)O13—C12—H12A109.5
C6—C7—C9119.97 (13)C11—C12—H12A109.5
C2—C8—C7119.06 (13)O13—C12—H12B109.5
C2—C8—H8120.5C11—C12—H12B109.5
C7—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.57 (12)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.69 (13)C3—C5—C6—C70.2 (2)
C4i—S1—C2—C30.50 (11)C5—C6—C7—C80.1 (2)
C8—C2—C3—C51.0 (2)C5—C6—C7—C9177.94 (13)
S1—C2—C3—C5178.82 (11)C3—C2—C8—C71.0 (2)
C8—C2—C3—C4179.85 (12)S1—C2—C8—C7178.76 (11)
S1—C2—C3—C40.33 (14)C6—C7—C8—C20.5 (2)
C5—C3—C4—C4i179.10 (16)C9—C7—C8—C2178.52 (13)
C2—C3—C4—C4i0.1 (2)C8—C7—C9—C1080.25 (19)
C5—C3—C4—S1i1.5 (2)C6—C7—C9—C1097.81 (18)
C2—C3—C4—S1i179.49 (11)C7—C9—C10—C11176.09 (14)
C2—C3—C5—C60.4 (2)C9—C10—C11—C12174.93 (15)
C4—C3—C5—C6179.32 (14)C10—C11—C12—O13179.98 (14)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.822.032.8028 (9)158
C6—H6···S1iii0.933.374.1564 (17)143
C9—H9A···S1iii0.973.534.144 (2)124
C10—H10A···S1iii0.973.363.9832 (19)124
C10—H10A···S1iv0.973.203.8870 (17)129
C11—H11B···S1iii0.973.474.1477 (19)129
C12—H12A···S1iv0.973.103.8528 (19)135
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A270) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.341 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.684 (4) ÅCell parameters from 7068 reflections
b = 5.074 (1) Åθ = 2.3–24.8°
c = 14.433 (4) ŵ = 0.28 mm1
β = 108.11 (3)°T = 270 K
V = 952.5 (4) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.028
Rotating crystal scansθmax = 29.9°, θmin = 1.5°
8556 measured reflectionsh = 1919
2820 independent reflectionsk = 67
2505 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.041H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.127 w = 1/[σ2(Fo2) + (0.0721P)2 + 0.223P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.027
2820 reflectionsΔρmax = 0.58 e Å3
121 parametersΔρmin = 0.29 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.037 (5)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64527 (3)0.32388 (8)0.53853 (2)0.04703 (14)
C20.64764 (10)0.5535 (3)0.62945 (9)0.0400 (3)
C30.55373 (10)0.6890 (3)0.61207 (9)0.0391 (3)
C40.48127 (10)0.5962 (3)0.52312 (9)0.0391 (3)
C50.54510 (12)0.8820 (3)0.67776 (10)0.0472 (3)
H50.4839320.9743720.6673560.057*
C60.62871 (12)0.9341 (3)0.75862 (10)0.0485 (3)
H60.6228601.0630600.8023940.058*
C70.72218 (11)0.7984 (3)0.77668 (9)0.0446 (3)
C80.73146 (11)0.6066 (3)0.71186 (10)0.0454 (3)
H80.7927020.5140890.7229470.054*
C90.81006 (13)0.8567 (3)0.86778 (10)0.0499 (3)
H9A0.8014341.0324860.8904690.060*
H9B0.8740530.8537900.8521300.060*
C100.81686 (14)0.6613 (3)0.94871 (11)0.0507 (4)
H10A0.7510420.6554580.9608450.061*
H10B0.8299000.4874840.9271890.061*
C110.90039 (12)0.7255 (3)1.04391 (10)0.0468 (3)
H11A0.9655570.7460261.0312510.056*
H11B0.8842230.8915861.0690740.056*
C120.91063 (13)0.5154 (3)1.11903 (10)0.0511 (3)
H12A0.8457320.4947231.1322150.061*
H12B0.9272110.3490641.0943810.061*
O130.98896 (10)0.5816 (2)1.20666 (8)0.0582 (3)
H130.9969 (14)0.462 (5)1.2444 (14)0.087*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0402 (2)0.0562 (2)0.0407 (2)0.00652 (13)0.00694 (14)0.00996 (13)
C20.0410 (6)0.0448 (7)0.0333 (5)0.0012 (5)0.0102 (4)0.0018 (5)
C30.0417 (6)0.0427 (6)0.0328 (5)0.0029 (5)0.0116 (5)0.0019 (4)
C40.0378 (5)0.0448 (6)0.0336 (5)0.0004 (5)0.0094 (4)0.0021 (5)
C50.0482 (7)0.0515 (7)0.0404 (6)0.0014 (6)0.0115 (6)0.0078 (6)
C60.0554 (8)0.0508 (8)0.0370 (6)0.0052 (6)0.0111 (6)0.0092 (5)
C70.0491 (7)0.0483 (7)0.0324 (6)0.0109 (5)0.0068 (5)0.0001 (5)
C80.0415 (6)0.0522 (8)0.0385 (6)0.0021 (5)0.0068 (5)0.0020 (5)
C90.0542 (8)0.0509 (8)0.0368 (6)0.0135 (6)0.0030 (6)0.0017 (5)
C100.0614 (9)0.0427 (7)0.0374 (6)0.0111 (6)0.0003 (6)0.0019 (5)
C110.0546 (7)0.0408 (7)0.0367 (6)0.0065 (6)0.0023 (5)0.0034 (5)
C120.0607 (8)0.0436 (7)0.0380 (6)0.0054 (6)0.0008 (6)0.0019 (5)
O130.0673 (7)0.0522 (6)0.0396 (5)0.0036 (5)0.0061 (5)0.0000 (4)
Geometric parameters (Å, º) top
S1—C4i1.7311 (14)C9—C101.513 (2)
S1—C21.7477 (14)C9—H9A0.9700
C2—C81.3980 (18)C9—H9B0.9700
C2—C31.4094 (19)C10—C111.524 (2)
C3—C51.3931 (18)C10—H10A0.9700
C3—C41.4359 (17)C10—H10B0.9700
C4—C4i1.369 (3)C11—C121.496 (2)
C5—C61.382 (2)C11—H11A0.9700
C5—H50.9300C11—H11B0.9700
C6—C71.404 (2)C12—O131.4207 (17)
C6—H60.9300C12—H12A0.9700
C7—C81.383 (2)C12—H12B0.9700
C7—C91.5097 (19)O13—H130.80 (3)
C8—H80.9300
C4i—S1—C290.68 (6)C10—C9—H9A109.1
C8—C2—C3121.26 (13)C7—C9—H9B109.1
C8—C2—S1125.88 (11)C10—C9—H9B109.1
C3—C2—S1112.86 (10)H9A—C9—H9B107.8
C5—C3—C2119.15 (12)C11—C10—C9113.89 (12)
C5—C3—C4131.14 (13)C11—C10—H10A108.8
C2—C3—C4109.70 (11)C9—C10—H10A108.8
C4i—C4—C3114.25 (15)C11—C10—H10B108.8
C4i—C4—S1i112.51 (13)C9—C10—H10B108.8
C3—C4—S1i133.24 (10)H10A—C10—H10B107.7
C6—C5—C3119.08 (14)C12—C11—C10112.10 (12)
C6—C5—H5120.5C12—C11—H11A109.2
C3—C5—H5120.5C10—C11—H11A109.2
C5—C6—C7122.00 (13)C12—C11—H11B109.2
C5—C6—H6119.0C10—C11—H11B109.2
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.31 (13)O13—C12—C11110.59 (12)
C8—C7—C9120.74 (14)O13—C12—H12A109.5
C6—C7—C9119.91 (14)C11—C12—H12A109.5
C2—C8—C7119.18 (13)O13—C12—H12B109.5
C2—C8—H8120.4C11—C12—H12B109.5
C7—C8—H8120.4H12A—C12—H12B108.1
C7—C9—C10112.67 (12)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.82 (13)C3—C5—C6—C70.0 (2)
C4i—S1—C2—C30.48 (11)C5—C6—C7—C80.1 (2)
C8—C2—C3—C50.9 (2)C5—C6—C7—C9178.01 (14)
S1—C2—C3—C5178.80 (11)C3—C2—C8—C70.9 (2)
C8—C2—C3—C4179.86 (13)S1—C2—C8—C7178.77 (11)
S1—C2—C3—C40.42 (14)C6—C7—C8—C20.4 (2)
C5—C3—C4—C4i178.99 (16)C9—C7—C8—C2178.46 (13)
C2—C3—C4—C4i0.1 (2)C8—C7—C9—C1080.40 (19)
C5—C3—C4—S1i1.3 (2)C6—C7—C9—C1097.64 (18)
C2—C3—C4—S1i179.57 (11)C7—C9—C10—C11176.12 (15)
C2—C3—C5—C60.4 (2)C9—C10—C11—C12174.96 (15)
C4—C3—C5—C6179.46 (14)C10—C11—C12—O13179.97 (14)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.802.052.8032 (10)158
C6—H6···S1iii0.933.374.1606 (18)144
C9—H9A···S1iii0.973.544.152 (2)124
C10—H10A···S1iii0.973.373.989 (2)124
C10—H10A···S1iv0.973.213.8920 (18)129
C11—H11B···S1iii0.973.474.1536 (19)129
C12—H12A···S1iv0.973.113.8570 (19)135
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A280) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.338 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.705 (3) ÅCell parameters from 6934 reflections
b = 5.074 (1) Åθ = 2.3–25.8°
c = 14.447 (3) ŵ = 0.28 mm1
β = 108.20 (2)°T = 280 K
V = 954.4 (3) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.024
Rotating crystal scansθmax = 29.9°, θmin = 1.5°
8550 measured reflectionsh = 1919
2833 independent reflectionsk = 67
2496 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.042H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.130 w = 1/[σ2(Fo2) + (0.075P)2 + 0.230P]
where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max = 0.023
2833 reflectionsΔρmax = 0.56 e Å3
121 parametersΔρmin = 0.27 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.041 (5)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64509 (3)0.32388 (8)0.53858 (3)0.04930 (15)
C20.64762 (10)0.5535 (3)0.62956 (9)0.0418 (3)
C30.55374 (10)0.6887 (3)0.61223 (9)0.0410 (3)
C40.48133 (10)0.5962 (3)0.52311 (9)0.0409 (3)
C50.54511 (12)0.8814 (3)0.67781 (11)0.0494 (3)
H50.4839930.9737600.6673550.059*
C60.62866 (12)0.9336 (3)0.75869 (10)0.0508 (3)
H60.6228411.0623070.8024820.061*
C70.72204 (12)0.7980 (3)0.77669 (10)0.0466 (3)
C80.73134 (11)0.6061 (3)0.71192 (10)0.0475 (3)
H80.7924970.5135130.7230630.057*
C90.81003 (13)0.8562 (3)0.86786 (11)0.0522 (4)
H9A0.8015441.0321800.8904530.063*
H9B0.8739100.8529140.8522520.063*
C100.81682 (14)0.6614 (3)0.94879 (11)0.0530 (4)
H10A0.7510710.6558110.9608200.064*
H10B0.8297540.4874130.9273590.064*
C110.90021 (13)0.7253 (3)1.04398 (10)0.0492 (3)
H11A0.9653040.7456531.0314000.059*
H11B0.8841180.8914681.0690490.059*
C120.91053 (13)0.5158 (3)1.11912 (11)0.0540 (4)
H12A0.8457260.4952551.1322430.065*
H12B0.9270390.3493011.0945680.065*
O130.98872 (10)0.5817 (3)1.20666 (8)0.0612 (3)
H130.9968 (14)0.461 (5)1.2446 (14)0.092*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0422 (2)0.0588 (3)0.0427 (2)0.00682 (13)0.00721 (14)0.01032 (14)
C20.0427 (6)0.0465 (7)0.0350 (5)0.0011 (5)0.0105 (5)0.0016 (5)
C30.0432 (6)0.0449 (7)0.0345 (6)0.0026 (5)0.0118 (5)0.0017 (5)
C40.0396 (6)0.0472 (7)0.0348 (5)0.0002 (5)0.0099 (4)0.0017 (5)
C50.0505 (7)0.0539 (8)0.0422 (7)0.0014 (6)0.0120 (6)0.0083 (6)
C60.0581 (8)0.0533 (8)0.0386 (6)0.0055 (6)0.0116 (6)0.0095 (6)
C70.0514 (7)0.0501 (7)0.0338 (6)0.0112 (6)0.0069 (5)0.0000 (5)
C80.0434 (7)0.0545 (8)0.0406 (6)0.0021 (6)0.0072 (5)0.0019 (6)
C90.0563 (8)0.0535 (8)0.0383 (6)0.0140 (6)0.0024 (6)0.0017 (6)
C100.0633 (9)0.0448 (7)0.0395 (7)0.0110 (6)0.0004 (6)0.0022 (5)
C110.0571 (8)0.0432 (7)0.0383 (6)0.0076 (6)0.0020 (6)0.0041 (5)
C120.0640 (9)0.0452 (7)0.0407 (7)0.0053 (6)0.0012 (6)0.0020 (6)
O130.0707 (8)0.0547 (6)0.0413 (5)0.0037 (5)0.0067 (5)0.0000 (5)
Geometric parameters (Å, º) top
S1—C4i1.7309 (14)C9—C101.512 (2)
S1—C21.7485 (14)C9—H9A0.9700
C2—C81.3966 (19)C9—H9B0.9700
C2—C31.4099 (19)C10—C111.523 (2)
C3—C51.3919 (19)C10—H10A0.9700
C3—C41.4370 (18)C10—H10B0.9700
C4—C4i1.369 (3)C11—C121.494 (2)
C5—C61.382 (2)C11—H11A0.9700
C5—H50.9300C11—H11B0.9700
C6—C71.404 (2)C12—O131.4187 (17)
C6—H60.9300C12—H12A0.9700
C7—C81.383 (2)C12—H12B0.9700
C7—C91.5112 (19)O13—H130.81 (3)
C8—H80.9300
C4i—S1—C290.72 (7)C10—C9—H9A109.1
C8—C2—C3121.29 (13)C7—C9—H9B109.1
C8—C2—S1125.87 (11)C10—C9—H9B109.1
C3—C2—S1112.83 (10)H9A—C9—H9B107.8
C5—C3—C2119.20 (12)C11—C10—C9114.00 (12)
C5—C3—C4131.12 (13)C11—C10—H10A108.8
C2—C3—C4109.66 (12)C9—C10—H10A108.8
C4i—C4—C3114.29 (15)C11—C10—H10B108.8
C4i—C4—S1i112.49 (13)C9—C10—H10B108.8
C3—C4—S1i133.22 (11)H10A—C10—H10B107.6
C6—C5—C3119.06 (14)C12—C11—C10112.25 (12)
C6—C5—H5120.5C12—C11—H11A109.2
C3—C5—H5120.5C10—C11—H11A109.2
C5—C6—C7121.96 (14)C12—C11—H11B109.2
C5—C6—H6119.0C10—C11—H11B109.2
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.39 (13)O13—C12—C11110.71 (13)
C8—C7—C9120.67 (15)O13—C12—H12A109.5
C6—C7—C9119.91 (14)C11—C12—H12A109.5
C2—C8—C7119.08 (14)O13—C12—H12B109.5
C2—C8—H8120.5C11—C12—H12B109.5
C7—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.69 (12)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.76 (14)C3—C5—C6—C70.0 (2)
C4i—S1—C2—C30.39 (11)C5—C6—C7—C80.0 (2)
C8—C2—C3—C51.1 (2)C5—C6—C7—C9178.05 (14)
S1—C2—C3—C5178.80 (11)C3—C2—C8—C71.1 (2)
C8—C2—C3—C4179.90 (13)S1—C2—C8—C7178.78 (11)
S1—C2—C3—C40.25 (15)C6—C7—C8—C20.5 (2)
C5—C3—C4—C4i178.97 (16)C9—C7—C8—C2178.55 (13)
C2—C3—C4—C4i0.1 (2)C8—C7—C9—C1080.6 (2)
C5—C3—C4—S1i1.5 (3)C6—C7—C9—C1097.46 (18)
C2—C3—C4—S1i179.60 (11)C7—C9—C10—C11176.07 (15)
C2—C3—C5—C60.5 (2)C9—C10—C11—C12174.92 (16)
C4—C3—C5—C6179.33 (14)C10—C11—C12—O13179.98 (15)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.812.042.8033 (10)158
C6—H6···S1iii0.933.384.1651 (16)144
C9—H9A···S1iii0.973.554.161 (2)124
C10—H10A···S1iii0.973.373.994 (2)124
C10—H10A···S1iv0.973.213.8978 (18)129
C11—H11B···S1iii0.973.484.1586 (19)129
C12—H12A···S1iv0.973.113.8619 (19)135
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A290) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.336 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.725 (2) ÅCell parameters from 7019 reflections
b = 5.073 (1) Åθ = 2.2–24.9°
c = 14.461 (2) ŵ = 0.28 mm1
β = 108.301 (19)°T = 290 K
V = 955.9 (2) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.026
Rotating crystal scansθmax = 29.9°, θmin = 1.5°
8549 measured reflectionsh = 1919
2837 independent reflectionsk = 67
2459 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.042H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.131 w = 1/[σ2(Fo2) + (0.0738P)2 + 0.2136P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max = 0.020
2837 reflectionsΔρmax = 0.57 e Å3
121 parametersΔρmin = 0.25 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.038 (5)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64493 (3)0.32387 (8)0.53867 (3)0.05145 (15)
C20.64750 (10)0.5533 (3)0.62957 (9)0.0435 (3)
C30.55371 (10)0.6887 (3)0.61224 (9)0.0425 (3)
C40.48135 (10)0.5960 (3)0.52307 (9)0.0426 (3)
C50.54518 (12)0.8809 (3)0.67780 (11)0.0513 (3)
H50.4841160.9731370.6673790.062*
C60.62864 (12)0.9328 (3)0.75863 (10)0.0530 (3)
H60.6228471.0615230.8023910.064*
C70.72190 (12)0.7974 (3)0.77677 (10)0.0486 (3)
C80.73118 (11)0.6058 (3)0.71199 (10)0.0494 (3)
H80.7922900.5133190.7231580.059*
C90.80976 (13)0.8560 (3)0.86797 (11)0.0544 (4)
H9A0.8011871.0319300.8905190.065*
H9B0.8735880.8529100.8524980.065*
C100.81663 (14)0.6613 (3)0.94876 (11)0.0553 (4)
H10A0.7509730.6557570.9607490.066*
H10B0.8294800.4872800.9273230.066*
C110.90008 (13)0.7250 (3)1.04400 (10)0.0513 (3)
H11A0.9650880.7450961.0314680.062*
H11B0.8841260.8914201.0689960.062*
C120.91040 (14)0.5163 (3)1.11904 (11)0.0565 (4)
H12A0.8456740.4960191.1321140.068*
H12B0.9267830.3495831.0945720.068*
O130.98862 (10)0.5822 (3)1.20658 (8)0.0641 (3)
H130.9951 (14)0.466 (5)1.2447 (14)0.096*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0439 (2)0.0612 (3)0.0448 (2)0.00709 (14)0.00761 (14)0.01063 (14)
C20.0450 (6)0.0480 (7)0.0361 (5)0.0018 (5)0.0108 (5)0.0015 (5)
C30.0448 (6)0.0461 (7)0.0361 (6)0.0029 (5)0.0123 (5)0.0019 (5)
C40.0417 (6)0.0487 (7)0.0364 (5)0.0001 (5)0.0107 (5)0.0019 (5)
C50.0522 (7)0.0554 (8)0.0441 (7)0.0016 (6)0.0119 (6)0.0086 (6)
C60.0603 (8)0.0557 (8)0.0405 (6)0.0056 (6)0.0120 (6)0.0098 (6)
C70.0535 (7)0.0528 (8)0.0350 (6)0.0117 (6)0.0072 (5)0.0001 (5)
C80.0460 (7)0.0560 (8)0.0420 (6)0.0023 (6)0.0075 (5)0.0016 (6)
C90.0587 (8)0.0559 (8)0.0402 (6)0.0146 (6)0.0035 (6)0.0016 (6)
C100.0657 (9)0.0468 (7)0.0413 (7)0.0114 (6)0.0005 (6)0.0022 (6)
C110.0591 (8)0.0455 (7)0.0399 (6)0.0075 (6)0.0021 (6)0.0039 (5)
C120.0673 (9)0.0472 (7)0.0423 (7)0.0058 (6)0.0010 (6)0.0016 (6)
O130.0740 (8)0.0569 (7)0.0437 (6)0.0035 (6)0.0067 (5)0.0000 (5)
Geometric parameters (Å, º) top
S1—C4i1.7305 (14)C9—C101.510 (2)
S1—C21.7476 (14)C9—H9A0.9700
C2—C81.3969 (18)C9—H9B0.9700
C2—C31.4105 (19)C10—C111.524 (2)
C3—C51.3901 (19)C10—H10A0.9700
C3—C41.4373 (18)C10—H10B0.9700
C4—C4i1.368 (3)C11—C121.491 (2)
C5—C61.381 (2)C11—H11A0.9700
C5—H50.9300C11—H11B0.9700
C6—C71.403 (2)C12—O131.4190 (17)
C6—H60.9300C12—H12A0.9700
C7—C81.383 (2)C12—H12B0.9700
C7—C91.5110 (19)O13—H130.79 (3)
C8—H80.9300
C4i—S1—C290.69 (6)C10—C9—H9A109.1
C8—C2—C3121.24 (13)C7—C9—H9B109.1
C8—C2—S1125.87 (11)C10—C9—H9B109.1
C3—C2—S1112.90 (10)H9A—C9—H9B107.8
C5—C3—C2119.21 (12)C11—C10—C9114.02 (13)
C5—C3—C4131.22 (13)C11—C10—H10A108.7
C2—C3—C4109.57 (12)C9—C10—H10A108.7
C4i—C4—C3114.31 (15)C11—C10—H10B108.7
C4i—C4—S1i112.53 (13)C9—C10—H10B108.7
C3—C4—S1i133.15 (11)H10A—C10—H10B107.6
C6—C5—C3119.07 (14)C12—C11—C10112.32 (13)
C6—C5—H5120.5C12—C11—H11A109.1
C3—C5—H5120.5C10—C11—H11A109.1
C5—C6—C7122.05 (14)C12—C11—H11B109.1
C5—C6—H6119.0C10—C11—H11B109.1
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.33 (13)O13—C12—C11110.75 (13)
C8—C7—C9120.75 (15)O13—C12—H12A109.5
C6—C7—C9119.88 (14)C11—C12—H12A109.5
C2—C8—C7119.09 (14)O13—C12—H12B109.5
C2—C8—H8120.5C11—C12—H12B109.5
C7—C8—H8120.5H12A—C12—H12B108.1
C7—C9—C10112.68 (12)C12—O13—H13109.5
C7—C9—H9A109.1
C4i—S1—C2—C8179.76 (14)C3—C5—C6—C70.1 (2)
C4i—S1—C2—C30.38 (11)C5—C6—C7—C80.1 (2)
C8—C2—C3—C51.0 (2)C5—C6—C7—C9178.08 (14)
S1—C2—C3—C5178.86 (11)C3—C2—C8—C71.0 (2)
C8—C2—C3—C4179.87 (13)S1—C2—C8—C7178.84 (11)
S1—C2—C3—C40.27 (15)C6—C7—C8—C20.5 (2)
C5—C3—C4—C4i179.02 (16)C9—C7—C8—C2178.60 (14)
C2—C3—C4—C4i0.0 (2)C8—C7—C9—C1080.6 (2)
C5—C3—C4—S1i1.4 (3)C6—C7—C9—C1097.50 (19)
C2—C3—C4—S1i179.62 (11)C7—C9—C10—C11176.20 (15)
C2—C3—C5—C60.5 (2)C9—C10—C11—C12175.02 (16)
C4—C3—C5—C6179.36 (15)C10—C11—C12—O13179.97 (15)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.792.062.8039 (10)157
C6—H6···S1iii0.933.384.1720 (15)144
C9—H9A···S1iii0.973.554.166 (2)124
C10—H10A···S1iii0.973.373.999 (2)124
C10—H10A···S1iv0.973.223.9020 (18)129
C11—H11B···S1iii0.973.494.1637 (18)129
C12—H12A···S1iv0.973.123.8657 (18)135
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
(A300) top
Crystal data top
C22H24O2S2F(000) = 408
Mr = 384.53Dx = 1.333 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.700 Å
a = 13.748 (6) ÅCell parameters from 7097 reflections
b = 5.072 (1) Åθ = 2.2–26.0°
c = 14.477 (2) ŵ = 0.28 mm1
β = 108.402 (19)°T = 300 K
V = 957.9 (5) Å3Prism, colourless
Z = 20.12 × 0.06 × 0.02 mm
Data collection top
Huber 4-circles Kappa Goniometer, Pilatus 2M detector
diffractometer
Rint = 0.029
Rotating crystal scansθmax = 29.9°, θmin = 1.5°
8661 measured reflectionsh = 1919
2848 independent reflectionsk = 67
2430 reflections with I > 2σ(I)l = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.043H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.116 w = 1/[σ2(Fo2) + (0.0542P)2 + 0.4979P]
where P = (Fo2 + 2Fc2)/3
S = 0.87(Δ/σ)max = 0.002
2848 reflectionsΔρmax = 0.55 e Å3
121 parametersΔρmin = 0.29 e Å3
0 restraintsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: iterativeExtinction coefficient: 0.041 (4)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.64475 (3)0.32392 (9)0.53874 (3)0.05383 (15)
C20.64721 (11)0.5528 (3)0.62963 (10)0.0456 (3)
C30.55382 (11)0.6883 (3)0.61223 (10)0.0442 (3)
C40.48133 (11)0.5959 (3)0.52300 (10)0.0444 (3)
C50.54530 (13)0.8803 (3)0.67786 (11)0.0536 (4)
H50.4842990.9725100.6674290.064*
C60.62870 (13)0.9321 (4)0.75869 (11)0.0554 (4)
H60.6229491.0607500.8024360.066*
C70.72192 (12)0.7966 (3)0.77694 (10)0.0507 (3)
C80.73081 (12)0.6058 (4)0.71227 (11)0.0517 (3)
H80.7918310.5131930.7234850.062*
C90.80957 (14)0.8555 (4)0.86810 (11)0.0570 (4)
H9A0.8009081.0315080.8905220.068*
H9B0.8733230.8526220.8527400.068*
C100.81662 (15)0.6613 (3)0.94886 (11)0.0577 (4)
H10A0.7510380.6555560.9607160.069*
H10B0.8295260.4872360.9275150.069*
C110.89981 (14)0.7250 (3)1.04406 (11)0.0538 (4)
H11A0.9647360.7454901.0316560.065*
H11B0.8837590.8912761.0690110.065*
C120.91033 (14)0.5164 (3)1.11899 (11)0.0586 (4)
H12A0.8457030.4956631.1319430.070*
H12B0.9268760.3498361.0946080.070*
O130.98838 (11)0.5828 (3)1.20654 (8)0.0669 (4)
H130.9966 (15)0.467 (5)1.2428 (15)0.100*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0455 (2)0.0642 (3)0.0470 (2)0.00729 (16)0.00796 (15)0.01114 (17)
C20.0470 (7)0.0505 (8)0.0378 (6)0.0018 (6)0.0114 (5)0.0012 (6)
C30.0463 (7)0.0486 (8)0.0375 (6)0.0032 (6)0.0128 (5)0.0023 (5)
C40.0428 (6)0.0509 (8)0.0383 (6)0.0005 (6)0.0111 (5)0.0023 (6)
C50.0538 (8)0.0586 (9)0.0467 (8)0.0014 (7)0.0133 (6)0.0084 (7)
C60.0634 (9)0.0580 (9)0.0423 (7)0.0063 (7)0.0132 (6)0.0103 (7)
C70.0551 (8)0.0550 (9)0.0372 (6)0.0121 (7)0.0079 (6)0.0006 (6)
C80.0470 (7)0.0588 (9)0.0447 (7)0.0026 (6)0.0081 (6)0.0016 (7)
C90.0609 (9)0.0588 (9)0.0424 (7)0.0148 (7)0.0034 (6)0.0025 (7)
C100.0681 (10)0.0492 (8)0.0434 (7)0.0113 (7)0.0001 (7)0.0026 (6)
C110.0614 (9)0.0476 (8)0.0425 (7)0.0079 (7)0.0024 (6)0.0045 (6)
C120.0680 (10)0.0507 (9)0.0440 (7)0.0057 (7)0.0010 (7)0.0021 (7)
O130.0771 (8)0.0596 (7)0.0452 (6)0.0036 (6)0.0074 (6)0.0006 (5)
Geometric parameters (Å, º) top
S1—C4i1.7294 (16)C9—C101.508 (2)
S1—C21.7471 (15)C9—H9A0.9700
C2—C81.399 (2)C9—H9B0.9700
C2—C31.407 (2)C10—C111.522 (2)
C3—C51.391 (2)C10—H10A0.9700
C3—C41.4384 (19)C10—H10B0.9700
C4—C4i1.367 (3)C11—C121.489 (2)
C5—C61.381 (2)C11—H11A0.9700
C5—H50.9300C11—H11B0.9700
C6—C71.404 (3)C12—O131.4186 (18)
C6—H60.9300C12—H12A0.9700
C7—C81.378 (2)C12—H12B0.9700
C7—C91.510 (2)O13—H130.77 (3)
C8—H80.9300
C4i—S1—C290.62 (7)C10—C9—H9A109.0
C8—C2—C3121.07 (14)C7—C9—H9B109.0
C8—C2—S1125.96 (12)C10—C9—H9B109.0
C3—C2—S1112.96 (10)H9A—C9—H9B107.8
C5—C3—C2119.24 (13)C11—C10—C9114.16 (14)
C5—C3—C4131.13 (14)C11—C10—H10A108.7
C2—C3—C4109.62 (13)C9—C10—H10A108.7
C4i—C4—C3114.16 (16)C11—C10—H10B108.7
C4i—C4—S1i112.63 (14)C9—C10—H10B108.7
C3—C4—S1i133.21 (12)H10A—C10—H10B107.6
C6—C5—C3119.06 (15)C12—C11—C10112.41 (14)
C6—C5—H5120.5C12—C11—H11A109.1
C3—C5—H5120.5C10—C11—H11A109.1
C5—C6—C7122.07 (15)C12—C11—H11B109.1
C5—C6—H6119.0C10—C11—H11B109.1
C7—C6—H6119.0H11A—C11—H11B107.9
C8—C7—C6119.16 (14)O13—C12—C11110.76 (14)
C8—C7—C9121.02 (16)O13—C12—H12A109.5
C6—C7—C9119.80 (15)C11—C12—H12A109.5
C2—C8—C7119.39 (15)O13—C12—H12B109.5
C2—C8—H8120.3C11—C12—H12B109.5
C7—C8—H8120.3H12A—C12—H12B108.1
C7—C9—C10112.74 (14)C12—O13—H13109.5
C7—C9—H9A109.0
C4i—S1—C2—C8179.82 (15)C3—C5—C6—C70.1 (3)
C4i—S1—C2—C30.52 (12)C5—C6—C7—C80.0 (3)
C8—C2—C3—C50.8 (2)C5—C6—C7—C9178.14 (16)
S1—C2—C3—C5178.84 (12)C3—C2—C8—C70.9 (2)
C8—C2—C3—C4179.87 (14)S1—C2—C8—C7178.70 (12)
S1—C2—C3—C40.45 (16)C6—C7—C8—C20.5 (2)
C5—C3—C4—C4i179.07 (18)C9—C7—C8—C2178.65 (15)
C2—C3—C4—C4i0.1 (2)C8—C7—C9—C1080.6 (2)
C5—C3—C4—S1i1.3 (3)C6—C7—C9—C1097.5 (2)
C2—C3—C4—S1i179.53 (12)C7—C9—C10—C11176.21 (16)
C2—C3—C5—C60.3 (2)C9—C10—C11—C12174.94 (17)
C4—C3—C5—C6179.41 (16)C10—C11—C12—O13179.94 (16)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O13—H13···O13ii0.772.072.8041 (11)159
C6—H6···S1iii0.933.394.1776 (17)144
C9—H9A···S1iii0.973.564.173 (2)124
C10—H10A···S1iii0.973.384.004 (2)124
C10—H10A···S1iv0.973.223.908 (2)129
C11—H11B···S1iii0.973.494.167 (2)129
C12—H12A···S1iv0.973.123.871 (2)136
Symmetry codes: (ii) x+2, y1/2, z+5/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2.
 

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