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This work presents a single-crystal X-ray diffraction study of an organic co-crystal composed of N-iodo­saccharin and pyridine (NISac·py) under hydro­static pressure ranging from 0.00 (5) GPa to 4.5 (2) GPa. NISac·py crystallizes in the monoclinic system (space group B21/e). The unconventional setting of the space group is adopted (the conventional setting is P21/c, No. 14) to emphasise the strongly pseudo-orthorhombic symmetry of the lattice, with a β angle very close to 90°. The crystal structure contains one molecule each of N-iodo­saccharin (NISac) and pyridine (py) in the asymmetric unit (Z′ = 1), linked via an Nsac...I...N′py halogen-bonding motif. A gradual modification of this motif is observed under pressure as a result of changes in the crystalline environment. Mechanical twinning is observed under compression and the sample splits into two domains, spanning an unequal volume that is mapped by a twofold rotation about the [100] direction of the B21/e unit cell. The twinning is particularly significant at high pressure, being reversible when the pressure is released. The structure of the twinned sample reveals the continuity of a substantial substructure across the composition plane. The presence of this common substructure in the two orientations of the twinned individuals can be interpreted as a structural reason for the formation of the twin and is the first observed example in a molecular crystal. These results indicate that the anisotropy of intermolecular interactions in the crystal structure results in an anisotropic strain generated upon the action of hydro­static compression. Periodic density functional theory calculations were carried out by considering an isotropic external pressure, the results showing good agreement with the experimental findings. The bulk modulus of the crystal was obtained from the equations of state, being 7 (1) GPa for experimental data and 6.8 (5) GPa for theoretical data.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520622002542/rm5056sup1.cif
Contains datablocks global, NISac_Py_crystal_1_RTP, NISac_Py_crystal_1_100K, dac_0.00_GPa, dac_0.00_d_GPa, dac_0.05_d_GPa, dac_0.20_GPa, dac_0.4_GPa, dac_0.5_GPa, dac_0.5_d_GPa, dac_0.8_d_GPa, dac_0.9_GPa, dac_1.3_d_GPa, dac_1.5_GPa, dac_1.9_d_GPa, dac_2.0_GPa, dac_2.4_d_GPa, dac_3.3_GPa, dac_4.5_GPa, NISac_Py_crystal_2_RTP

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056NISac_Py_crystal_1_RTPsup2.hkl
Contains datablock NISac_Py_crystal_1_RTP

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056NISac_Py_crystal_1_100Ksup3.hkl
Contains datablock NISac_Py_crystal_1_100K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_0.00_GPasup4.hkl
Contains datablock dac_0.00_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_0.00_d_GPasup5.hkl
Contains datablock dac_0.00_d_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_0.05_d_GPasup6.hkl
Contains datablock dac_0.05_d_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_0.20_GPasup7.hkl
Contains datablock dac_0.20_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_0.4_GPasup8.hkl
Contains datablock dac_0.4_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_0.5_GPasup9.hkl
Contains datablock dac_0.5_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_0.5_d_GPasup10.hkl
Contains datablock dac_0.5_d_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_0.8_d_GPasup11.hkl
Contains datablock dac_0.8_d_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_0.9_GPasup12.hkl
Contains datablock dac_0.9_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_1.3_d_GPasup13.hkl
Contains datablock dac_1.3_d_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_1.5_GPasup14.hkl
Contains datablock dac_1.5_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_1.9_d_GPasup15.hkl
Contains datablock dac_1.9_d_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_2.0_GPasup16.hkl
Contains datablock dac_2.0_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_2.4_d_GPasup17.hkl
Contains datablock dac_2.4_d_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_3.3_GPasup18.hkl
Contains datablock dac_3.3_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056dac_4.5_GPasup19.hkl
Contains datablock dac_4.5_GPa

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622002542/rm5056NISac_Py_crystal_2_RTPsup20.hkl
Contains datablock NISac_Py_crystal_2_RTP

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520622002542/rm5056sup21.pdf
Additional tables and figures

CCDC references: 2156534; 2156535; 2156536; 2156537; 2156538; 2156539; 2156540; 2156541; 2156542; 2156543; 2156544; 2156545; 2156546; 2156547; 2156548; 2156549; 2156550; 2156551; 2156552

Computing details top

For all structures, cell refinement: SAINT V8.40B (?, 2016); data reduction: SAINT V8.40B (?, 2016). Program(s) used to solve structure: XT (Sheldrick, 2015) for NISac_Py_crystal_1_RTP; SHELXT (Sheldrick, 2015) for NISac_Py_crystal_1_100K, dac_0.00_GPa, dac_0.00_d_GPa, dac_0.05_d_GPa, dac_0.20_GPa, dac_0.4_GPa, dac_0.5_GPa, dac_0.5_d_GPa, dac_0.8_d_GPa, dac_0.9_GPa, dac_1.3_d_GPa, dac_1.5_GPa, dac_1.9_d_GPa, dac_2.0_GPa, dac_2.4_d_GPa, dac_3.3_GPa, dac_4.5_GPa, NISac_Py_crystal_2_RTP. For all structures, program(s) used to refine structure: SHELXL 2014/3 (Sheldrick, 2015); molecular graphics: Olex2 1.3 (Dolomanov et al., 2009); software used to prepare material for publication: Olex2 1.3 (Dolomanov et al., 2009).

(NISac_Py_crystal_1_RTP) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 1.922 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 27.234 (3) ÅCell parameters from 9068 reflections
b = 7.8058 (7) Åθ = 3.0–35.3°
c = 12.6258 (10) ŵ = 2.55 mm1
β = 88.606 (2)°T = 296 K
V = 2683.2 (4) Å3Plate, colourless
Z = 80.15 × 0.12 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
3456 reflections with I > 2σ(I)
φ and ω scansRint = 0.034
Absorption correction: numerical
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction. wR2(int) was 0.0765 before and 0.0552 after correction. The Ratio of minimum to maximum transmission is 0.8748. The λ/2 correction factor is Not present.
θmax = 29.6°, θmin = 1.8°
Tmin = 0.569, Tmax = 0.650h = 3737
109428 measured reflectionsk = 1010
3759 independent reflectionsl = 1717
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.019H-atom parameters constrained
wR(F2) = 0.050 w = 1/[σ2(Fo2) + (0.021P)2 + 3.1655P]
where P = (Fo2 + 2Fc2)/3
S = 1.10(Δ/σ)max = 0.001
3759 reflectionsΔρmax = 0.73 e Å3
173 parametersΔρmin = 0.29 e Å3
0 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28444 (2)0.39783 (2)0.47942 (2)0.03977 (5)
S10.40406 (2)0.47307 (7)0.44942 (4)0.04072 (10)
N20.21598 (6)0.3842 (2)0.58768 (13)0.0402 (3)
O30.32802 (6)0.4083 (2)0.21415 (13)0.0553 (4)
O10.39561 (7)0.6158 (2)0.51840 (13)0.0625 (5)
C70.35993 (7)0.4390 (3)0.27664 (15)0.0383 (4)
C40.48580 (8)0.5932 (3)0.32890 (19)0.0478 (5)
H40.50420.61140.38900.057*
C100.13886 (9)0.4130 (3)0.73070 (18)0.0524 (5)
H100.11290.42430.77940.063*
N10.35443 (6)0.4241 (2)0.38535 (13)0.0423 (4)
C120.22003 (8)0.3230 (3)0.68637 (17)0.0478 (4)
H120.24910.27020.70570.057*
C50.43830 (6)0.5306 (2)0.33556 (14)0.0360 (3)
O20.42466 (6)0.3224 (2)0.49619 (13)0.0601 (4)
C60.41043 (6)0.5012 (2)0.24767 (14)0.0358 (3)
C90.13468 (8)0.4724 (3)0.62862 (18)0.0510 (5)
H90.10560.52260.60700.061*
C20.47715 (9)0.5993 (3)0.13878 (19)0.0557 (6)
H20.49060.62430.07210.067*
C80.17421 (7)0.4566 (3)0.55872 (16)0.0426 (4)
H80.17150.49740.48990.051*
C10.42997 (8)0.5343 (3)0.14777 (16)0.0498 (5)
H10.41180.51330.08780.060*
C110.18199 (9)0.3367 (3)0.75955 (17)0.0519 (5)
H110.18540.29490.82790.062*
C30.50463 (8)0.6275 (3)0.2281 (2)0.0545 (5)
H30.53640.67030.22020.065*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.03320 (7)0.04341 (7)0.04262 (7)0.00149 (4)0.00078 (5)0.00083 (5)
S10.0367 (2)0.0537 (3)0.0320 (2)0.00646 (19)0.00651 (16)0.00200 (19)
N20.0360 (8)0.0430 (8)0.0415 (8)0.0028 (6)0.0029 (6)0.0001 (6)
O30.0387 (7)0.0817 (12)0.0462 (8)0.0091 (7)0.0127 (6)0.0057 (7)
O10.0696 (11)0.0758 (12)0.0420 (8)0.0127 (9)0.0034 (7)0.0164 (8)
C70.0316 (8)0.0463 (10)0.0371 (9)0.0005 (7)0.0037 (6)0.0033 (7)
C40.0363 (10)0.0527 (12)0.0547 (12)0.0087 (8)0.0071 (8)0.0005 (9)
C100.0508 (12)0.0609 (13)0.0449 (11)0.0025 (10)0.0129 (9)0.0031 (9)
N10.0303 (7)0.0604 (10)0.0363 (8)0.0048 (7)0.0026 (6)0.0014 (7)
C120.0471 (11)0.0489 (11)0.0475 (11)0.0012 (9)0.0042 (8)0.0055 (9)
C50.0321 (8)0.0395 (9)0.0366 (8)0.0019 (7)0.0037 (6)0.0005 (7)
O20.0532 (9)0.0698 (11)0.0580 (9)0.0054 (8)0.0174 (7)0.0227 (8)
C60.0302 (8)0.0412 (9)0.0361 (8)0.0020 (7)0.0026 (6)0.0022 (7)
C90.0389 (10)0.0636 (13)0.0502 (11)0.0062 (9)0.0024 (8)0.0002 (10)
C20.0521 (12)0.0656 (15)0.0488 (12)0.0025 (10)0.0136 (10)0.0070 (10)
C80.0370 (9)0.0520 (11)0.0387 (9)0.0010 (8)0.0002 (7)0.0016 (8)
C10.0468 (11)0.0663 (14)0.0363 (9)0.0000 (10)0.0005 (8)0.0010 (9)
C110.0610 (13)0.0558 (12)0.0387 (10)0.0050 (10)0.0011 (9)0.0062 (9)
C30.0390 (10)0.0543 (13)0.0699 (15)0.0101 (9)0.0085 (10)0.0038 (11)
Geometric parameters (Å, º) top
I1—N22.2875 (16)C10—C91.377 (3)
I1—N12.2305 (16)C10—C111.374 (3)
S1—O11.4292 (17)C12—H120.9300
S1—N11.6371 (16)C12—C111.376 (3)
S1—C51.7529 (19)C5—C61.379 (2)
S1—O21.4365 (18)C6—C11.381 (3)
N2—C121.342 (3)C9—H90.9300
N2—C81.329 (3)C9—C81.381 (3)
O3—C71.212 (2)C2—H20.9300
C7—N11.382 (2)C2—C11.384 (3)
C7—C61.495 (2)C2—C31.386 (4)
C4—H40.9300C8—H80.9300
C4—C51.384 (3)C1—H10.9300
C4—C31.387 (3)C11—H110.9300
C10—H100.9300C3—H30.9300
N1—I1—N2174.88 (6)C4—C5—S1128.20 (15)
O1—S1—N1111.13 (11)C6—C5—S1108.97 (13)
O1—S1—C5111.99 (10)C6—C5—C4122.83 (18)
O1—S1—O2116.52 (11)C5—C6—C7112.23 (16)
N1—S1—C594.80 (8)C5—C6—C1119.76 (17)
O2—S1—N1110.34 (10)C1—C6—C7127.99 (17)
O2—S1—C5109.97 (10)C10—C9—H9120.4
C12—N2—I1119.15 (14)C10—C9—C8119.2 (2)
C8—N2—I1120.43 (13)C8—C9—H9120.4
C8—N2—C12119.82 (18)C1—C2—H2119.7
O3—C7—N1124.61 (18)C1—C2—C3120.7 (2)
O3—C7—C6125.08 (18)C3—C2—H2119.7
N1—C7—C6110.30 (15)N2—C8—C9121.41 (19)
C5—C4—H4121.7N2—C8—H8119.3
C5—C4—C3116.6 (2)C9—C8—H8119.3
C3—C4—H4121.7C6—C1—C2118.7 (2)
C9—C10—H10120.5C6—C1—H1120.7
C11—C10—H10120.5C2—C1—H1120.7
C11—C10—C9119.0 (2)C10—C11—C12119.4 (2)
S1—N1—I1117.61 (9)C10—C11—H11120.3
C7—N1—I1127.38 (12)C12—C11—H11120.3
C7—N1—S1113.60 (13)C4—C3—H3119.3
N2—C12—H12119.4C2—C3—C4121.4 (2)
N2—C12—C11121.2 (2)C2—C3—H3119.3
C11—C12—H12119.4
I1—N2—C12—C11169.76 (17)N1—C7—C6—C1179.1 (2)
I1—N2—C8—C9170.26 (17)C12—N2—C8—C90.8 (3)
S1—C5—C6—C72.8 (2)C5—S1—N1—I1164.79 (10)
S1—C5—C6—C1178.93 (17)C5—S1—N1—C72.66 (16)
N2—C12—C11—C100.7 (4)C5—C4—C3—C20.3 (3)
O3—C7—N1—I114.5 (3)C5—C6—C1—C21.0 (3)
O3—C7—N1—S1179.57 (18)O2—S1—N1—I181.83 (13)
O3—C7—C6—C5178.0 (2)O2—S1—N1—C7110.72 (16)
O3—C7—C6—C10.1 (3)O2—S1—C5—C468.5 (2)
O1—S1—N1—I148.99 (14)O2—S1—C5—C6110.52 (15)
O1—S1—N1—C7118.46 (16)C6—C7—N1—I1164.55 (13)
O1—S1—C5—C462.8 (2)C6—C7—N1—S11.4 (2)
O1—S1—C5—C6118.25 (15)C9—C10—C11—C120.6 (4)
C7—C6—C1—C2176.9 (2)C8—N2—C12—C111.4 (3)
C4—C5—C6—C7178.15 (19)C1—C2—C3—C40.6 (4)
C4—C5—C6—C10.1 (3)C11—C10—C9—C81.2 (4)
C10—C9—C8—N20.5 (4)C3—C4—C5—S1179.41 (18)
N1—S1—C5—C4177.9 (2)C3—C4—C5—C60.6 (3)
N1—S1—C5—C63.16 (15)C3—C2—C1—C61.2 (4)
N1—C7—C6—C51.0 (2)
(NISac_Py_crystal_1_100K) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 1.986 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 27.085 (5) ÅCell parameters from 9083 reflections
b = 7.6524 (9) Åθ = 3.0–39.5°
c = 12.5325 (14) ŵ = 2.63 mm1
β = 88.571 (2)°T = 296 K
V = 2596.7 (6) Å3Plate, colourless
Z = 80.15 × 0.12 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
Rint = 0.031
φ and ω scansθmax = 29.6°, θmin = 1.8°
104622 measured reflectionsh = 3737
3643 independent reflectionsk = 1010
3587 reflections with I > 2σ(I)l = 1717
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.015H-atom parameters constrained
wR(F2) = 0.038 w = 1/[σ2(Fo2) + (0.0114P)2 + 7.3244P]
where P = (Fo2 + 2Fc2)/3
S = 1.13(Δ/σ)max = 0.004
3643 reflectionsΔρmax = 1.04 e Å3
173 parametersΔρmin = 0.32 e Å3
0 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28300 (2)0.39845 (2)0.47823 (2)0.01169 (3)
S10.40329 (2)0.47536 (5)0.44910 (3)0.01222 (7)
N20.21478 (5)0.38605 (17)0.58721 (11)0.0132 (2)
O30.32790 (4)0.40777 (17)0.20950 (9)0.0175 (2)
O10.39427 (5)0.62153 (17)0.51888 (10)0.0197 (2)
C70.35965 (6)0.4398 (2)0.27347 (12)0.0125 (3)
C40.48635 (6)0.5980 (2)0.33047 (13)0.0156 (3)
H40.50430.61680.39170.019*
C100.13715 (6)0.4168 (2)0.73237 (13)0.0170 (3)
H100.11110.42880.78150.020*
N10.35361 (5)0.42507 (19)0.38311 (10)0.0138 (2)
C120.21934 (6)0.3238 (2)0.68716 (13)0.0154 (3)
H120.24870.27030.70620.018*
C50.43843 (5)0.5348 (2)0.33531 (12)0.0120 (3)
O20.42387 (4)0.32142 (17)0.49739 (10)0.0186 (2)
C60.41078 (5)0.5040 (2)0.24556 (12)0.0116 (3)
C90.13275 (6)0.4770 (2)0.62844 (13)0.0162 (3)
H90.10350.52800.60680.019*
C20.47903 (6)0.6025 (2)0.13742 (14)0.0179 (3)
H20.49310.62680.07060.021*
C80.17250 (6)0.4601 (2)0.55732 (12)0.0137 (3)
H80.16980.50080.48780.016*
C10.43103 (6)0.5370 (2)0.14481 (13)0.0155 (3)
H10.41310.51610.08380.019*
C110.18099 (6)0.3385 (2)0.76177 (13)0.0164 (3)
H110.18460.29640.83080.020*
C30.50623 (6)0.6319 (2)0.22873 (14)0.0171 (3)
H30.53830.67500.22170.021*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.01003 (5)0.01246 (5)0.01256 (5)0.00041 (3)0.00017 (3)0.00047 (3)
S10.01159 (15)0.01520 (17)0.00996 (15)0.00183 (13)0.00207 (12)0.00053 (13)
N20.0127 (6)0.0132 (6)0.0137 (6)0.0015 (5)0.0008 (5)0.0004 (5)
O30.0138 (5)0.0235 (6)0.0153 (5)0.0029 (4)0.0041 (4)0.0011 (4)
O10.0228 (6)0.0221 (6)0.0140 (5)0.0034 (5)0.0008 (4)0.0049 (5)
C70.0116 (6)0.0130 (6)0.0128 (6)0.0008 (5)0.0005 (5)0.0003 (5)
C40.0134 (7)0.0156 (7)0.0180 (7)0.0019 (5)0.0028 (5)0.0010 (6)
C100.0181 (7)0.0186 (7)0.0141 (7)0.0016 (6)0.0034 (6)0.0014 (6)
N10.0106 (6)0.0197 (6)0.0112 (6)0.0021 (5)0.0007 (4)0.0004 (5)
C120.0158 (7)0.0145 (7)0.0159 (7)0.0001 (6)0.0018 (5)0.0012 (6)
C50.0117 (6)0.0122 (6)0.0121 (6)0.0002 (5)0.0007 (5)0.0002 (5)
O20.0177 (5)0.0199 (6)0.0184 (6)0.0012 (5)0.0058 (4)0.0063 (5)
C60.0098 (6)0.0121 (6)0.0128 (6)0.0006 (5)0.0009 (5)0.0003 (5)
C90.0134 (7)0.0189 (7)0.0165 (7)0.0020 (6)0.0004 (5)0.0004 (6)
C20.0172 (7)0.0188 (8)0.0174 (7)0.0013 (6)0.0042 (6)0.0020 (6)
C80.0127 (6)0.0156 (7)0.0129 (6)0.0015 (5)0.0010 (5)0.0006 (5)
C10.0152 (7)0.0185 (7)0.0129 (7)0.0000 (6)0.0002 (5)0.0005 (6)
C110.0205 (7)0.0163 (7)0.0124 (7)0.0019 (6)0.0003 (6)0.0019 (6)
C30.0124 (7)0.0151 (7)0.0238 (8)0.0031 (6)0.0026 (6)0.0001 (6)
Geometric parameters (Å, º) top
I1—N22.2722 (14)C10—C91.389 (2)
I1—N12.2375 (13)C10—C111.388 (2)
S1—O11.4370 (13)C12—H120.9300
S1—N11.6426 (14)C12—C111.385 (2)
S1—C51.7546 (16)C5—C61.387 (2)
S1—O21.4428 (12)C6—C11.387 (2)
N2—C121.348 (2)C9—H90.9300
N2—C81.339 (2)C9—C81.386 (2)
O3—C71.2151 (19)C2—H20.9300
C7—N11.3842 (19)C2—C11.394 (2)
C7—C61.503 (2)C2—C31.395 (2)
C4—H40.9300C8—H80.9300
C4—C51.385 (2)C1—H10.9300
C4—C31.396 (2)C11—H110.9300
C10—H100.9300C3—H30.9300
N1—I1—N2174.57 (5)C4—C5—S1127.94 (12)
O1—S1—N1111.09 (8)C4—C5—C6123.24 (14)
O1—S1—C5111.92 (8)C6—C5—S1108.80 (11)
O1—S1—O2116.23 (8)C5—C6—C7112.33 (13)
N1—S1—C594.93 (7)C5—C6—C1119.86 (14)
O2—S1—N1110.48 (7)C1—C6—C7127.79 (14)
O2—S1—C5110.19 (7)C10—C9—H9120.4
C12—N2—I1118.75 (11)C8—C9—C10119.25 (15)
C8—N2—I1120.16 (10)C8—C9—H9120.4
C8—N2—C12120.52 (14)C1—C2—H2119.5
O3—C7—N1124.78 (14)C1—C2—C3120.95 (15)
O3—C7—C6125.15 (14)C3—C2—H2119.5
N1—C7—C6110.07 (13)N2—C8—C9121.01 (14)
C5—C4—H4121.8N2—C8—H8119.5
C5—C4—C3116.40 (15)C9—C8—H8119.5
C3—C4—H4121.8C6—C1—C2118.22 (15)
C9—C10—H10120.5C6—C1—H1120.9
C11—C10—H10120.5C2—C1—H1120.9
C11—C10—C9119.06 (15)C10—C11—H11120.4
S1—N1—I1116.94 (7)C12—C11—C10119.21 (15)
C7—N1—I1127.92 (10)C12—C11—H11120.4
C7—N1—S1113.75 (11)C4—C3—H3119.3
N2—C12—H12119.5C2—C3—C4121.32 (15)
N2—C12—C11120.94 (15)C2—C3—H3119.3
C11—C12—H12119.5
I1—N2—C12—C11169.89 (12)N1—C7—C6—C1179.41 (16)
I1—N2—C8—C9170.31 (12)C12—N2—C8—C91.0 (2)
S1—C5—C6—C72.93 (16)C5—S1—N1—I1164.71 (8)
S1—C5—C6—C1178.52 (12)C5—S1—N1—C72.91 (13)
N2—C12—C11—C100.7 (2)C5—C4—C3—C20.3 (2)
O3—C7—N1—I114.6 (2)C5—C6—C1—C20.6 (2)
O3—C7—N1—S1179.39 (14)O2—S1—N1—I181.58 (9)
O3—C7—C6—C5177.99 (15)O2—S1—N1—C7110.80 (12)
O3—C7—C6—C10.4 (3)O2—S1—C5—C467.73 (16)
O1—S1—N1—I148.93 (10)O2—S1—C5—C6110.58 (12)
O1—S1—N1—C7118.69 (12)C6—C7—N1—I1164.36 (10)
O1—S1—C5—C463.23 (17)C6—C7—N1—S11.62 (17)
O1—S1—C5—C6118.46 (12)C9—C10—C11—C120.6 (2)
C7—C6—C1—C2177.73 (15)C8—N2—C12—C111.5 (2)
C4—C5—C6—C7178.66 (14)C1—C2—C3—C40.4 (3)
C4—C5—C6—C10.1 (2)C11—C10—C9—C81.1 (2)
C10—C9—C8—N20.4 (2)C3—C4—C5—S1178.63 (13)
N1—S1—C5—C4178.32 (15)C3—C4—C5—C60.5 (2)
N1—S1—C5—C63.37 (12)C3—C2—C1—C60.8 (3)
N1—C7—C6—C51.00 (18)
NISac.Py_0GPa (dac_0.00_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 1.913 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 27.291 (14) ÅCell parameters from 3353 reflections
b = 7.8228 (16) Åθ = 3.0–20.9°
c = 12.628 (3) ŵ = 2.54 mm1
β = 88.579 (11)°T = 296 K
V = 2695.1 (16) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
595 reflections with I > 2σ(I)
φ and ω scansRint = 0.045
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction. wR2(int) was 0.0620 before and 0.0503 after correction. The Ratio of minimum to maximum transmission is 0.8187. The λ/2 correction factor is Not present.
θmax = 23.2°, θmin = 1.8°
Tmin = 0.461, Tmax = 0.563h = 1010
10351 measured reflectionsk = 88
770 independent reflectionsl = 1414
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.030H-atom parameters constrained
wR(F2) = 0.080 w = 1/[σ2(Fo2) + (0.0411P)2 + 9.578P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max < 0.001
770 reflectionsΔρmax = 0.46 e Å3
71 parametersΔρmin = 0.34 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28458 (5)0.39779 (7)0.47941 (4)0.0474 (9)
S10.40367 (19)0.4728 (3)0.44916 (15)0.047 (3)
N20.2162 (6)0.3857 (8)0.5884 (5)0.044
O30.3277 (6)0.4096 (8)0.2142 (5)0.058
O10.3962 (6)0.6150 (8)0.5179 (4)0.066
C70.3607 (9)0.4397 (10)0.2769 (6)0.041
C40.4870 (6)0.5916 (12)0.3292 (7)0.051
H40.50530.60750.38960.061*
C100.1388 (7)0.4111 (11)0.7304 (7)0.054
H100.11290.42140.77910.065*
N10.3546 (6)0.4264 (8)0.3848 (5)0.045
C120.2202 (7)0.3237 (10)0.6863 (6)0.053
H120.24920.27080.70550.063*
C50.4388 (6)0.5316 (10)0.3349 (6)0.038
O20.4250 (5)0.3225 (8)0.4960 (4)0.061
C60.4090 (7)0.5001 (10)0.2480 (5)0.037
C90.1345 (7)0.4699 (11)0.6280 (7)0.053
H90.10540.51910.60630.064*
C20.4781 (6)0.5980 (12)0.1396 (7)0.058
H20.49170.62100.07280.070*
C80.1743 (6)0.4545 (11)0.5576 (6)0.039
H80.17160.49280.48830.047*
C10.4301 (6)0.5363 (12)0.1474 (6)0.052
H10.41220.51930.08660.062*
C110.1820 (7)0.3373 (11)0.7589 (7)0.052
H110.18560.29640.82750.062*
C30.5065 (7)0.6263 (11)0.2284 (6)0.057
H30.53820.66820.22030.068*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.050 (3)0.0455 (4)0.0462 (4)0.0006 (5)0.0027 (5)0.0007 (2)
S10.048 (12)0.0565 (14)0.0359 (12)0.008 (2)0.001 (2)0.0011 (10)
N20.0440.0440.0440.0000.0020.001
O30.0450.0790.0490.0000.0000.000
O10.0680.0890.0410.0000.0020.000
C70.0400.0440.0390.0060.0000.000
C40.0370.0600.0560.0000.0000.000
C100.0520.0610.0500.0000.0190.000
N10.0410.0550.0390.0000.0000.002
C120.0660.0430.0480.0000.0000.005
C50.0380.0370.0380.0000.0000.000
O20.0560.0700.0570.0000.0000.018
C60.0270.0430.0400.0070.0000.000
C90.0420.0590.0580.0220.0000.000
C20.0530.0650.0550.0050.0130.006
C80.0260.0530.0390.0000.0000.006
C10.0470.0690.0390.0100.0000.000
C110.0610.0530.0420.0000.0000.006
C30.0370.0570.0760.0000.0110.004
Geometric parameters (Å, º) top
I1—N22.294 (13)C10—C91.381 (11)
I1—N12.239 (15)C10—C111.369 (18)
S1—O11.423 (7)C12—H120.9300
S1—N11.625 (16)C12—C111.376 (18)
S1—C51.773 (12)C5—C61.403 (12)
S1—O21.445 (8)C6—C11.411 (11)
N2—C121.335 (9)C9—H90.9300
N2—C81.329 (15)C9—C81.391 (19)
O3—C71.24 (2)C2—H20.9300
C7—N11.374 (11)C2—C11.397 (14)
C7—C61.44 (3)C2—C31.396 (12)
C4—H40.9300C8—H80.9300
C4—C51.398 (14)C1—H10.9300
C4—C31.394 (11)C11—H110.9300
C10—H100.9300C3—H30.9300
N1—I1—N2174.4 (3)C4—C5—S1128.2 (7)
O1—S1—N1111.9 (8)C4—C5—C6125.5 (10)
O1—S1—C5111.1 (5)C6—C5—S1106.2 (9)
O1—S1—O2116.1 (4)C5—C6—C7113.8 (9)
N1—S1—C595.0 (5)C5—C6—C1116.0 (12)
O2—S1—N1111.6 (5)C1—C6—C7130.2 (12)
O2—S1—C5109.2 (6)C10—C9—H9120.4
C12—N2—I1119.0 (10)C10—C9—C8119.1 (14)
C8—N2—I1120.0 (6)C8—C9—H9120.4
C8—N2—C12120.7 (12)C1—C2—H2118.8
O3—C7—N1123.3 (18)C3—C2—H2118.8
O3—C7—C6125.3 (9)C3—C2—C1122.4 (11)
N1—C7—C6111.4 (15)N2—C8—C9120.7 (10)
C5—C4—H4121.6N2—C8—H8119.6
C3—C4—H4121.6C9—C8—H8119.6
C3—C4—C5116.7 (11)C6—C1—H1120.2
C9—C10—H10120.6C2—C1—C6119.6 (11)
C11—C10—H10120.6C2—C1—H1120.2
C11—C10—C9118.7 (15)C10—C11—C12120.0 (10)
S1—N1—I1117.3 (4)C10—C11—H11120.0
C7—N1—I1128.2 (13)C12—C11—H11120.0
C7—N1—S1113.5 (13)C4—C3—C2119.8 (14)
N2—C12—H12119.7C4—C3—H3120.1
N2—C12—C11120.7 (13)C2—C3—H3120.1
C11—C12—H12119.7
I1—N2—C12—C11170.4 (7)N1—C7—C6—C1178.0 (9)
I1—N2—C8—C9170.9 (7)C12—N2—C8—C92.7 (15)
S1—C5—C6—C72.4 (11)C5—S1—N1—I1165.5 (4)
S1—C5—C6—C1179.2 (8)C5—S1—N1—C73.7 (7)
N2—C12—C11—C101.7 (15)C5—C4—C3—C21.0 (14)
O3—C7—N1—I112.3 (12)C5—C6—C1—C20.6 (14)
O3—C7—N1—S1179.9 (8)O2—S1—N1—I181.5 (6)
O3—C7—C6—C5177.2 (9)O2—S1—N1—C7109.3 (7)
O3—C7—C6—C11 (2)O2—S1—C5—C466.4 (11)
O1—S1—N1—I150.4 (5)O2—S1—C5—C6111.5 (7)
O1—S1—N1—C7118.8 (7)C6—C7—N1—I1165.0 (8)
O1—S1—C5—C462.9 (13)C6—C7—N1—S12.8 (12)
O1—S1—C5—C6119.2 (8)C9—C10—C11—C120.3 (16)
C7—C6—C1—C2178.6 (13)C8—N2—C12—C113.2 (14)
C4—C5—C6—C7179.6 (12)C1—C2—C3—C40.4 (16)
C4—C5—C6—C11.3 (14)C11—C10—C9—C80.9 (16)
C10—C9—C8—N20.6 (15)C3—C4—C5—S1179.0 (7)
N1—S1—C5—C4178.7 (10)C3—C4—C5—C61.5 (15)
N1—S1—C5—C63.4 (7)C3—C2—C1—C60.2 (17)
N1—C7—C6—C50.0 (14)
(dac_0.00_d_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 1.912 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 27.272 (19) ÅCell parameters from 2343 reflections
b = 7.834 (2) Åθ = 3.0–19.1°
c = 12.630 (4) ŵ = 2.53 mm1
β = 88.507 (15)°T = 296 K
V = 2697 (2) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
545 reflections with I > 2σ(I)
φ and ω scansRint = 0.069
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction.
θmax = 23.2°, θmin = 1.8°
Tmin = 0.461, Tmax = 0.563h = 1211
8714 measured reflectionsk = 88
830 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.040H-atom parameters constrained
wR(F2) = 0.113 w = 1/[σ2(Fo2) + (0.049P)2 + 19.6592P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max < 0.001
830 reflectionsΔρmax = 0.38 e Å3
71 parametersΔρmin = 0.51 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28457 (8)0.39800 (11)0.47952 (6)0.0552 (11)
S10.4038 (3)0.4724 (4)0.4494 (2)0.059 (4)
N20.2177 (8)0.3837 (13)0.5882 (7)0.051
O30.3287 (7)0.4098 (12)0.2144 (7)0.064
O10.3960 (8)0.6135 (12)0.5181 (6)0.071
C70.3598 (12)0.4394 (15)0.2777 (10)0.051
C40.4872 (8)0.5907 (18)0.3288 (9)0.057
H40.50610.60360.38850.069*
C100.1386 (9)0.4135 (17)0.7304 (10)0.068
H100.11290.42520.77960.081*
N10.3545 (9)0.4250 (12)0.3861 (7)0.049
C120.2204 (10)0.3231 (16)0.6859 (9)0.069
H120.24910.26970.70640.082*
C50.4386 (8)0.5342 (15)0.3352 (9)0.045
O20.4252 (7)0.3230 (12)0.4959 (6)0.068
C60.4092 (10)0.4984 (15)0.2480 (8)0.045
C90.1336 (10)0.4728 (16)0.6290 (9)0.057
H90.10460.52160.60640.069*
C20.4774 (7)0.5988 (17)0.1384 (10)0.060
H20.49080.62280.07150.072*
C80.1755 (9)0.4547 (17)0.5609 (10)0.050
H80.17330.49560.49200.060*
C10.4296 (8)0.5361 (17)0.1475 (9)0.055
H10.41130.51950.08720.066*
C110.1810 (9)0.3379 (16)0.7591 (10)0.063
H110.18400.29570.82750.076*
C30.5056 (9)0.6263 (16)0.2272 (8)0.064
H30.53730.66920.21860.077*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.056 (4)0.0574 (6)0.0515 (5)0.0010 (8)0.0009 (7)0.0005 (4)
S10.072 (14)0.065 (2)0.0395 (18)0.006 (3)0.003 (3)0.0004 (15)
N20.0510.0500.0500.0000.0030.001
O30.0500.0880.0550.0000.0000.000
O10.0730.0950.0450.0000.0020.000
C70.0490.0550.0490.0070.0000.000
C40.0420.0680.0620.0000.0000.000
C100.0650.0750.0610.0000.0230.000
N10.0440.0600.0420.0000.0000.002
C120.0860.0560.0630.0000.0000.007
C50.0460.0440.0450.0000.0000.000
O20.0620.0780.0630.0000.0000.020
C60.0330.0520.0480.0090.0000.001
C90.0460.0640.0630.0230.0000.000
C20.0550.0680.0570.0050.0140.007
C80.0330.0670.0490.0000.0000.007
C10.0490.0730.0410.0110.0000.000
C110.0740.0650.0510.0000.0000.007
C30.0410.0640.0860.0000.0120.005
Geometric parameters (Å, º) top
I1—N22.257 (18)C10—C91.372 (15)
I1—N12.23 (2)C10—C111.36 (2)
S1—O11.418 (10)C12—H120.9300
S1—N11.63 (2)C12—C111.40 (3)
S1—C51.772 (17)C5—C61.406 (14)
S1—O21.440 (12)C6—C11.404 (13)
N2—C121.326 (13)C9—H90.9300
N2—C81.331 (19)C9—C81.42 (3)
O3—C71.20 (3)C2—H20.9300
C7—N11.377 (15)C2—C11.396 (16)
C7—C61.46 (4)C2—C31.393 (14)
C4—H40.9300C8—H80.9300
C4—C51.399 (16)C1—H10.9300
C4—C31.394 (13)C11—H110.9300
C10—H100.9300C3—H30.9300
N1—I1—N2174.1 (5)C4—C5—S1128.3 (10)
O1—S1—N1111.5 (11)C4—C5—C6125.1 (14)
O1—S1—C5110.7 (7)C6—C5—S1106.2 (12)
O1—S1—O2116.1 (6)C5—C6—C7113.7 (12)
N1—S1—C595.4 (7)C1—C6—C7129.6 (16)
O2—S1—N1111.3 (7)C1—C6—C5116.6 (16)
O2—S1—C5109.9 (8)C10—C9—H9122.2
C12—N2—I1121.3 (14)C10—C9—C8115.7 (19)
C12—N2—C8117.5 (17)C8—C9—H9122.2
C8—N2—I1120.8 (9)C1—C2—H2119.3
O3—C7—N1126 (2)C3—C2—H2119.3
O3—C7—C6123.5 (14)C3—C2—C1121.5 (15)
N1—C7—C6111 (2)N2—C8—C9124.9 (15)
C5—C4—H4122.1N2—C8—H8117.5
C3—C4—H4122.1C9—C8—H8117.5
C3—C4—C5115.8 (16)C6—C1—H1120.2
C9—C10—H10119.9C2—C1—C6119.7 (15)
C11—C10—H10119.9C2—C1—H1120.2
C11—C10—C9120 (2)C10—C11—C12120.2 (15)
S1—N1—I1118.0 (5)C10—C11—H11119.9
C7—N1—I1127.0 (18)C12—C11—H11119.9
C7—N1—S1113.8 (18)C4—C3—H3119.4
N2—C12—H12119.3C2—C3—C4121.1 (18)
N2—C12—C11121.5 (19)C2—C3—H3119.4
C11—C12—H12119.3
I1—N2—C12—C11170.1 (11)N1—C7—C6—C1177.4 (13)
I1—N2—C8—C9171.1 (12)C12—N2—C8—C91 (2)
S1—C5—C6—C75.2 (15)C5—S1—N1—I1164.2 (6)
S1—C5—C6—C1179.5 (11)C5—S1—N1—C73.8 (11)
N2—C12—C11—C101 (2)C5—C4—C3—C23 (2)
O3—C7—N1—I114.0 (19)C5—C6—C1—C23 (2)
O3—C7—N1—S1179.3 (13)O2—S1—N1—I182.0 (9)
O3—C7—C6—C5176.6 (13)O2—S1—N1—C7110.0 (10)
O3—C7—C6—C12 (3)O2—S1—C5—C464.0 (16)
O1—S1—N1—I149.4 (7)O2—S1—C5—C6109.9 (11)
O1—S1—N1—C7118.6 (11)C6—C7—N1—I1165.4 (11)
O1—S1—C5—C465.6 (18)C6—C7—N1—S11.3 (17)
O1—S1—C5—C6120.6 (11)C9—C10—C11—C121 (2)
C7—C6—C1—C2177.0 (17)C8—N2—C12—C112 (2)
C4—C5—C6—C7179.3 (17)C1—C2—C3—C41 (2)
C4—C5—C6—C15 (2)C11—C10—C9—C82 (2)
C10—C9—C8—N21 (2)C3—C4—C5—S1178.3 (10)
N1—S1—C5—C4179.0 (15)C3—C4—C5—C65 (2)
N1—S1—C5—C65.1 (10)C3—C2—C1—C60 (2)
N1—C7—C6—C52.9 (19)
(dac_0.05_d_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 1.919 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 27.246 (16) ÅCell parameters from 2630 reflections
b = 7.819 (2) Åθ = 3.0–20.2°
c = 12.621 (3) ŵ = 2.54 mm1
β = 88.538 (13)°T = 296 K
V = 2687.7 (19) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
583 reflections with I > 2σ(I)
φ and ω scansRint = 0.063
Absorption correction: numerical
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction. wR2(int) was 0.0628 before and 0.0553 after correction. The Ratio of minimum to maximum transmission is 0.8355. The λ/2 correction factor is Not present.
θmax = 23.3°, θmin = 1.8°
Tmin = 0.470, Tmax = 0.563h = 1111
10196 measured reflectionsk = 88
817 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.041H-atom parameters constrained
wR(F2) = 0.103 w = 1/[σ2(Fo2) + (0.0332P)2 + 36.6993P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max < 0.001
817 reflectionsΔρmax = 0.45 e Å3
71 parametersΔρmin = 0.37 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28447 (8)0.39795 (10)0.47948 (6)0.0514 (11)
S10.4036 (3)0.4727 (4)0.4491 (2)0.059 (4)
N20.2174 (8)0.3836 (13)0.5880 (7)0.051
O30.3288 (7)0.4083 (12)0.2135 (7)0.062
O10.3963 (7)0.6156 (12)0.5180 (6)0.070
C70.3603 (11)0.4387 (14)0.2768 (9)0.043
C40.4873 (8)0.5907 (18)0.3289 (10)0.057
H40.50590.60410.38910.069*
C100.1380 (9)0.4143 (17)0.7304 (10)0.061
H100.11200.42610.77920.073*
N10.3534 (9)0.4260 (12)0.3850 (7)0.049
C120.2203 (9)0.3262 (15)0.6857 (9)0.059
H120.24940.27570.70690.070*
C50.4382 (8)0.5344 (15)0.3359 (9)0.046
O20.4251 (7)0.3225 (11)0.4959 (6)0.067
C60.4080 (10)0.5017 (15)0.2486 (8)0.041
C90.1336 (10)0.4727 (15)0.6289 (9)0.051
H90.10460.52190.60600.062*
C20.4783 (8)0.5993 (18)0.1382 (10)0.063
H20.49150.62230.07110.076*
C80.1753 (8)0.4546 (16)0.5602 (9)0.042
H80.17310.49510.49130.051*
C10.4300 (8)0.5386 (17)0.1487 (9)0.054
H10.41190.52220.08800.065*
C110.1806 (9)0.3388 (16)0.7592 (10)0.057
H110.18350.29550.82730.069*
C30.5070 (10)0.6257 (16)0.2273 (9)0.065
H30.53890.66630.21920.078*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.050 (4)0.0540 (5)0.0502 (5)0.0016 (8)0.0007 (7)0.0009 (4)
S10.074 (15)0.063 (2)0.0388 (18)0.008 (3)0.002 (3)0.0017 (15)
N20.0510.0500.0500.0000.0030.001
O30.0490.0850.0530.0000.0000.000
O10.0720.0940.0440.0000.0020.000
C70.0410.0460.0410.0060.0000.000
C40.0420.0680.0620.0000.0000.000
C100.0580.0670.0550.0000.0210.000
N10.0440.0600.0420.0000.0000.002
C120.0740.0480.0540.0000.0000.006
C50.0460.0450.0450.0000.0000.000
O20.0610.0770.0620.0000.0000.020
C60.0310.0480.0450.0080.0000.000
C90.0410.0570.0560.0210.0000.000
C20.0580.0710.0590.0050.0140.007
C80.0280.0570.0420.0000.0000.006
C10.0490.0720.0410.0100.0000.000
C110.0670.0580.0460.0000.0000.007
C30.0420.0660.0870.0000.0120.005
Geometric parameters (Å, º) top
I1—N22.258 (18)C10—C91.367 (15)
I1—N12.21 (2)C10—C111.36 (2)
S1—O11.427 (10)C12—H120.9300
S1—N11.65 (2)C12—C111.41 (3)
S1—C51.758 (17)C5—C61.415 (14)
S1—O21.445 (12)C6—C11.412 (14)
N2—C121.316 (13)C9—H90.9300
N2—C81.330 (19)C9—C81.42 (3)
O3—C71.21 (3)C2—H20.9300
C7—N11.377 (15)C2—C11.402 (16)
C7—C61.42 (4)C2—C31.400 (14)
C4—H40.9300C8—H80.9300
C4—C51.409 (16)C1—H10.9300
C4—C31.404 (14)C11—H110.9300
C10—H100.9300C3—H30.9300
N1—I1—N2174.6 (5)C4—C5—S1128.6 (10)
O1—S1—N1111.5 (10)C4—C5—C6125.3 (14)
O1—S1—C5110.2 (7)C6—C5—S1105.9 (12)
O1—S1—O2116.1 (6)C5—C6—C7114.3 (12)
N1—S1—C595.5 (7)C1—C6—C7131.1 (16)
O2—S1—N1111.7 (7)C1—C6—C5114.5 (16)
O2—S1—C5110.0 (8)C10—C9—H9121.6
C12—N2—I1121.3 (14)C10—C9—C8116.8 (19)
C12—N2—C8117.5 (17)C8—C9—H9121.6
C8—N2—I1120.6 (9)C1—C2—H2119.5
O3—C7—N1124 (2)C3—C2—H2119.5
O3—C7—C6124.0 (13)C3—C2—C1121.0 (15)
N1—C7—C6112 (2)N2—C8—C9124.3 (14)
C5—C4—H4121.4N2—C8—H8117.8
C3—C4—H4121.4C9—C8—H8117.8
C3—C4—C5117.3 (16)C6—C1—H1119.0
C9—C10—H10120.3C2—C1—C6122.0 (15)
C11—C10—H10120.3C2—C1—H1119.0
C11—C10—C9119 (2)C10—C11—C12120.0 (15)
S1—N1—I1117.5 (5)C10—C11—H11120.0
C7—N1—I1129.5 (18)C12—C11—H11120.0
C7—N1—S1112.0 (18)C4—C3—H3120.1
N2—C12—H12119.0C2—C3—C4119.8 (18)
N2—C12—C11121.9 (18)C2—C3—H3120.1
C11—C12—H12119.0
I1—N2—C12—C11170.8 (10)N1—C7—C6—C1178.1 (13)
I1—N2—C8—C9170.8 (11)C12—N2—C8—C90 (2)
S1—C5—C6—C72.4 (15)C5—S1—N1—I1164.7 (6)
S1—C5—C6—C1178.2 (11)C5—S1—N1—C75.2 (10)
N2—C12—C11—C101 (2)C5—C4—C3—C22 (2)
O3—C7—N1—I112.6 (19)C5—C6—C1—C21 (2)
O3—C7—N1—S1179.0 (12)O2—S1—N1—I181.3 (9)
O3—C7—C6—C5177.6 (13)O2—S1—N1—C7108.8 (10)
O3—C7—C6—C12 (3)O2—S1—C5—C463.6 (16)
O1—S1—N1—I150.5 (7)O2—S1—C5—C6111.2 (10)
O1—S1—N1—C7119.5 (10)C6—C7—N1—I1163.8 (12)
O1—S1—C5—C465.6 (17)C6—C7—N1—S14.6 (17)
O1—S1—C5—C6119.6 (11)C9—C10—C11—C122 (2)
C7—C6—C1—C2179.4 (19)C8—N2—C12—C110 (2)
C4—C5—C6—C7177.4 (17)C1—C2—C3—C40 (2)
C4—C5—C6—C13 (2)C11—C10—C9—C82 (2)
C10—C9—C8—N21 (2)C3—C4—C5—S1177.4 (10)
N1—S1—C5—C4179.1 (15)C3—C4—C5—C64 (2)
N1—S1—C5—C64.3 (10)C3—C2—C1—C60 (2)
N1—C7—C6—C51 (2)
(dac_0.20_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 1.946 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 27.185 (16) ÅCell parameters from 2886 reflections
b = 7.7444 (19) Åθ = 3.0–24.9°
c = 12.593 (3) ŵ = 2.58 mm1
β = 88.608 (12)°T = 296 K
V = 2650.4 (18) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
564 reflections with I > 2σ(I)
φ and ω scansRint = 0.071
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction.
θmax = 23.3°, θmin = 1.8°
Tmin = 0.461, Tmax = 0.563h = 1110
9901 measured reflectionsk = 88
777 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.036H-atom parameters constrained
wR(F2) = 0.096 w = 1/[σ2(Fo2) + (0.0489P)2 + 9.4112P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
777 reflectionsΔρmax = 0.39 e Å3
71 parametersΔρmin = 0.47 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28389 (6)0.39775 (8)0.47914 (5)0.0428 (10)
S10.4038 (2)0.4736 (4)0.44931 (18)0.053 (4)
N20.2167 (7)0.3847 (10)0.5880 (6)0.041
O30.3277 (7)0.4079 (10)0.2125 (6)0.055
O10.3969 (6)0.6194 (9)0.5183 (5)0.059
C70.3592 (11)0.4386 (13)0.2760 (8)0.042
C40.4876 (7)0.5929 (15)0.3293 (8)0.050
H40.50620.60770.38960.060*
C100.1383 (8)0.4145 (14)0.7309 (8)0.052
H100.11230.42590.77980.062*
N10.3538 (8)0.4256 (10)0.3840 (6)0.042
C120.2198 (8)0.3241 (13)0.6871 (7)0.052
H120.24880.27100.70740.063*
C50.4390 (7)0.5355 (12)0.3351 (7)0.035
O20.4243 (6)0.3217 (10)0.4973 (5)0.057
C60.4093 (8)0.5010 (13)0.2479 (7)0.035
C90.1338 (9)0.4742 (14)0.6283 (8)0.050
H90.10480.52490.60650.060*
C20.4786 (7)0.6011 (15)0.1380 (9)0.057
H20.49190.62660.07110.068*
C80.1737 (7)0.4567 (13)0.5589 (8)0.037
H80.17090.49600.48950.044*
C10.4306 (7)0.5375 (14)0.1477 (7)0.045
H10.41260.51900.08700.054*
C110.1816 (8)0.3379 (13)0.7599 (8)0.049
H110.18500.29560.82850.058*
C30.5065 (8)0.6266 (13)0.2275 (7)0.053
H30.53860.66710.21940.064*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.041 (3)0.0432 (5)0.0438 (5)0.0012 (6)0.0021 (6)0.0009 (3)
S10.075 (14)0.0527 (18)0.0316 (14)0.008 (3)0.002 (2)0.0029 (13)
N20.0410.0400.0400.0000.0020.001
O30.0430.0750.0470.0000.0000.000
O10.0610.0790.0370.0000.0020.000
C70.0400.0450.0400.0060.0000.000
C40.0360.0590.0540.0000.0000.000
C100.0500.0580.0470.0000.0180.000
N10.0380.0510.0360.0000.0000.002
C120.0660.0430.0480.0000.0000.005
C50.0360.0340.0350.0000.0000.000
O20.0520.0660.0540.0000.0000.017
C60.0260.0410.0380.0070.0000.000
C90.0400.0550.0540.0200.0000.000
C20.0520.0640.0540.0050.0130.006
C80.0250.0490.0370.0000.0000.005
C10.0410.0600.0340.0090.0000.000
C110.0570.0500.0390.0000.0000.006
C30.0340.0540.0720.0000.0100.004
Geometric parameters (Å, º) top
I1—N22.260 (15)C10—C91.380 (13)
I1—N12.231 (18)C10—C111.38 (2)
S1—O11.434 (8)C12—H120.9300
S1—N11.649 (19)C12—C111.37 (2)
S1—C51.774 (14)C5—C61.404 (13)
S1—O21.441 (10)C6—C11.405 (12)
N2—C121.338 (11)C9—H90.9300
N2—C81.353 (17)C9—C81.38 (2)
O3—C71.21 (2)C2—H20.9300
C7—N11.368 (13)C2—C11.396 (15)
C7—C61.48 (3)C2—C31.389 (13)
C4—H40.9300C8—H80.9300
C4—C51.395 (15)C1—H10.9300
C4—C31.394 (12)C11—H110.9300
C10—H100.9300C3—H30.9300
N1—I1—N2174.4 (4)C4—C5—S1128.3 (8)
O1—S1—N1112.5 (9)C4—C5—C6125.6 (12)
O1—S1—C5109.8 (6)C6—C5—S1105.9 (10)
O1—S1—O2115.8 (5)C5—C6—C7114.8 (10)
N1—S1—C595.2 (6)C5—C6—C1115.5 (14)
O2—S1—N1110.9 (6)C1—C6—C7129.6 (14)
O2—S1—C5110.7 (7)C10—C9—H9120.9
C12—N2—I1120.9 (12)C10—C9—C8118.3 (17)
C12—N2—C8118.2 (14)C8—C9—H9120.9
C8—N2—I1120.5 (8)C1—C2—H2119.8
O3—C7—N1126 (2)C3—C2—H2119.8
O3—C7—C6124.6 (12)C3—C2—C1120.5 (13)
N1—C7—C6109.7 (18)N2—C8—C9122.5 (12)
C5—C4—H4122.1N2—C8—H8118.8
C3—C4—H4122.1C9—C8—H8118.8
C3—C4—C5115.8 (14)C6—C1—H1119.5
C9—C10—H10120.4C2—C1—C6121.0 (13)
C11—C10—H10120.4C2—C1—H1119.5
C11—C10—C9119.3 (18)C10—C11—H11120.2
S1—N1—I1117.1 (5)C12—C11—C10119.6 (12)
C7—N1—I1127.6 (16)C12—C11—H11120.2
C7—N1—S1114.2 (16)C4—C3—H3119.3
N2—C12—H12118.9C2—C3—C4121.5 (16)
N2—C12—C11122.1 (16)C2—C3—H3119.3
C11—C12—H12118.9
I1—N2—C12—C11170.2 (9)N1—C7—C6—C1178.2 (11)
I1—N2—C8—C9170.4 (9)C12—N2—C8—C91.9 (18)
S1—C5—C6—C73.9 (13)C5—S1—N1—I1164.7 (5)
S1—C5—C6—C1178.7 (9)C5—S1—N1—C74.2 (9)
N2—C12—C11—C100.7 (18)C5—C4—C3—C21.1 (17)
O3—C7—N1—I113.4 (16)C5—C6—C1—C21.0 (17)
O3—C7—N1—S1179.1 (11)O2—S1—N1—I180.7 (7)
O3—C7—C6—C5177.3 (11)O2—S1—N1—C7110.4 (9)
O3—C7—C6—C10 (2)O2—S1—C5—C464.7 (13)
O1—S1—N1—I150.8 (6)O2—S1—C5—C6110.3 (9)
O1—S1—N1—C7118.1 (9)C6—C7—N1—I1165.0 (9)
O1—S1—C5—C464.4 (15)C6—C7—N1—S12.5 (14)
O1—S1—C5—C6120.7 (10)C9—C10—C11—C120.9 (19)
C7—C6—C1—C2178.0 (15)C8—N2—C12—C112.0 (17)
C4—C5—C6—C7179.0 (14)C1—C2—C3—C41.2 (19)
C4—C5—C6—C13.6 (17)C11—C10—C9—C81.0 (19)
C10—C9—C8—N20.4 (18)C3—C4—C5—S1177.7 (8)
N1—S1—C5—C4179.5 (12)C3—C4—C5—C63.6 (18)
N1—S1—C5—C64.5 (8)C3—C2—C1—C61 (2)
N1—C7—C6—C51.2 (17)
(dac_0.4_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 1.981 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 27.108 (16) ÅCell parameters from 2326 reflections
b = 7.6595 (19) Åθ = 3.1–20.6°
c = 12.539 (3) ŵ = 2.63 mm1
β = 88.662 (13)°T = 296 K
V = 2602.9 (18) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
536 reflections with I > 2σ(I)
φ and ω scansRint = 0.080
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction.
θmax = 23.2°, θmin = 1.8°
Tmin = 0.461, Tmax = 0.563h = 1110
8139 measured reflectionsk = 88
761 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.038H-atom parameters constrained
wR(F2) = 0.109 w = 1/[σ2(Fo2) + (0.0536P)2 + 2.7067P]
where P = (Fo2 + 2Fc2)/3
S = 1.17(Δ/σ)max < 0.001
761 reflectionsΔρmax = 0.51 e Å3
71 parametersΔρmin = 0.48 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28317 (7)0.39782 (10)0.47885 (6)0.0406 (12)
S10.4032 (3)0.4752 (4)0.4497 (2)0.048 (5)
N20.2161 (8)0.3857 (12)0.5884 (7)0.041
O30.3284 (8)0.4079 (11)0.2107 (7)0.051
O10.3956 (8)0.6223 (10)0.5182 (6)0.054
C70.3578 (12)0.4379 (14)0.2754 (9)0.036
C40.4884 (8)0.5948 (16)0.3313 (9)0.043
H40.50680.61050.39220.052*
C100.1371 (9)0.4141 (15)0.7319 (9)0.046
H100.11090.42300.78070.055*
N10.3521 (9)0.4266 (11)0.3831 (7)0.038
C120.2196 (9)0.3239 (14)0.6886 (8)0.045
H120.24860.26940.70850.053*
C50.4392 (8)0.5349 (14)0.3351 (8)0.031
O20.4235 (7)0.3218 (11)0.4984 (6)0.050
C60.4084 (10)0.5003 (15)0.2477 (7)0.032
C90.1320 (9)0.4758 (16)0.6284 (9)0.045
H90.10290.52740.60660.054*
C20.4788 (7)0.5984 (15)0.1380 (9)0.042
H20.49250.62010.07050.050*
C80.1725 (8)0.4568 (15)0.5588 (9)0.035
H80.16960.49460.48880.043*
C10.4300 (8)0.5361 (17)0.1472 (9)0.047
H10.41200.51830.08600.057*
C110.1812 (9)0.3394 (15)0.7624 (9)0.045
H110.18490.30010.83190.054*
C30.5074 (10)0.6289 (15)0.2281 (8)0.052
H30.53930.67200.21940.062*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.041 (4)0.0395 (5)0.0410 (5)0.0010 (7)0.0028 (7)0.0009 (4)
S10.069 (16)0.046 (2)0.0300 (17)0.002 (3)0.001 (3)0.0007 (14)
N20.0410.0400.0400.0000.0020.001
O30.0400.0700.0440.0000.0000.000
O10.0560.0730.0340.0000.0010.000
C70.0350.0390.0350.0050.0000.000
C40.0320.0510.0470.0000.0000.000
C100.0440.0510.0420.0000.0160.000
N10.0350.0470.0330.0000.0000.002
C120.0560.0360.0410.0000.0000.005
C50.0320.0310.0310.0000.0000.000
O20.0460.0580.0470.0000.0000.015
C60.0240.0370.0350.0060.0000.000
C90.0360.0500.0490.0180.0000.000
C20.0390.0470.0400.0030.0100.005
C80.0240.0470.0350.0000.0000.005
C10.0430.0630.0360.0090.0000.000
C110.0530.0460.0360.0000.0000.005
C30.0330.0520.0700.0000.0100.004
Geometric parameters (Å, º) top
I1—N22.256 (18)C10—C91.391 (15)
I1—N12.21 (2)C10—C111.39 (2)
S1—O11.429 (9)C12—H120.9300
S1—N11.68 (2)C12—C111.38 (2)
S1—C51.778 (16)C5—C61.419 (15)
S1—O21.439 (11)C6—C11.404 (13)
N2—C121.348 (13)C9—H90.9300
N2—C81.360 (19)C9—C81.39 (2)
O3—C71.17 (3)C2—H20.9300
C7—N11.358 (15)C2—C11.408 (16)
C7—C61.49 (4)C2—C31.404 (15)
C4—H40.9300C8—H80.9300
C4—C51.409 (16)C1—H10.9300
C4—C31.407 (13)C11—H110.9300
C10—H100.9300C3—H30.9300
N1—I1—N2174.5 (5)C4—C5—S1127.7 (9)
O1—S1—N1111.4 (10)C4—C5—C6127.5 (14)
O1—S1—C5110.6 (6)C6—C5—S1104.7 (11)
O1—S1—O2116.1 (6)C5—C6—C7115.9 (12)
N1—S1—C595.7 (7)C1—C6—C7129.6 (15)
O2—S1—N1111.0 (7)C1—C6—C5114.5 (16)
O2—S1—C5110.2 (8)C10—C9—H9121.5
C12—N2—I1120.6 (14)C10—C9—C8117.1 (18)
C12—N2—C8118.4 (16)C8—C9—H9121.5
C8—N2—I1120.7 (9)C1—C2—H2119.1
O3—C7—N1128 (3)C3—C2—H2119.1
O3—C7—C6122.6 (14)C3—C2—C1121.7 (14)
N1—C7—C6110 (2)N2—C8—C9123.2 (14)
C5—C4—H4122.6N2—C8—H8118.4
C3—C4—H4122.6C9—C8—H8118.4
C3—C4—C5114.7 (15)C6—C1—C2120.8 (14)
C9—C10—H10119.9C6—C1—H1119.6
C11—C10—H10119.9C2—C1—H1119.6
C11—C10—C9120.1 (19)C10—C11—H11120.3
S1—N1—I1116.7 (5)C12—C11—C10119.4 (14)
C7—N1—I1128.5 (19)C12—C11—H11120.3
C7—N1—S1113.9 (19)C4—C3—H3119.6
N2—C12—H12119.1C2—C3—C4120.8 (18)
N2—C12—C11121.7 (17)C2—C3—H3119.6
C11—C12—H12119.1
I1—N2—C12—C11169.9 (10)N1—C7—C6—C1177.9 (12)
I1—N2—C8—C9170.4 (11)C12—N2—C8—C93 (2)
S1—C5—C6—C72.9 (15)C5—S1—N1—I1166.0 (6)
S1—C5—C6—C1179.0 (10)C5—S1—N1—C74.1 (10)
N2—C12—C11—C103 (2)C5—C4—C3—C21.9 (18)
O3—C7—N1—I112.9 (19)C5—C6—C1—C20.9 (19)
O3—C7—N1—S1178.4 (13)O2—S1—N1—I179.9 (8)
O3—C7—C6—C5178.5 (13)O2—S1—N1—C7110.1 (10)
O3—C7—C6—C11 (3)O2—S1—C5—C466.1 (15)
O1—S1—N1—I151.2 (7)O2—S1—C5—C6111.0 (10)
O1—S1—N1—C7118.8 (10)C6—C7—N1—I1165.8 (11)
O1—S1—C5—C463.7 (17)C6—C7—N1—S12.8 (16)
O1—S1—C5—C6119.3 (11)C9—C10—C11—C121 (2)
C7—C6—C1—C2178.6 (16)C8—N2—C12—C113 (2)
C4—C5—C6—C7180.0 (16)C1—C2—C3—C41 (2)
C4—C5—C6—C12.0 (19)C11—C10—C9—C81 (2)
C10—C9—C8—N22 (2)C3—C4—C5—S1178.9 (10)
N1—S1—C5—C4179.1 (14)C3—C4—C5—C62 (2)
N1—S1—C5—C63.8 (9)C3—C2—C1—C61 (2)
N1—C7—C6—C50.3 (19)
(dac_0.5_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 2.017 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 26.998 (13) ÅCell parameters from 3214 reflections
b = 7.5869 (15) Åθ = 3.1–21.7°
c = 12.485 (3) ŵ = 2.67 mm1
β = 88.802 (11)°T = 296 K
V = 2556.7 (14) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
577 reflections with I > 2σ(I)
φ and ω scansRint = 0.054
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction. wR2(int) was 0.0782 before and 0.0572 after correction. The Ratio of minimum to maximum transmission is 0.8106. The λ/2 correction factor is Not present.
θmax = 23.3°, θmin = 1.8°
Tmin = 0.456, Tmax = 0.563h = 1010
9824 measured reflectionsk = 88
738 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.034H-atom parameters constrained
wR(F2) = 0.091 w = 1/[σ2(Fo2) + (0.0402P)2 + 16.5567P]
where P = (Fo2 + 2Fc2)/3
S = 1.15(Δ/σ)max < 0.001
738 reflectionsΔρmax = 0.53 e Å3
71 parametersΔρmin = 0.43 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28274 (6)0.39800 (8)0.47855 (5)0.0367 (10)
S10.4030 (2)0.4765 (3)0.44981 (18)0.033 (4)
N20.2164 (7)0.3857 (11)0.5885 (6)0.037
O30.3285 (7)0.4064 (9)0.2090 (6)0.044
O10.3946 (7)0.6256 (9)0.5178 (5)0.053
C70.3599 (10)0.4383 (12)0.2735 (8)0.030
C40.4878 (7)0.5960 (15)0.3317 (8)0.045
H40.50620.61100.39320.054*
C100.1370 (8)0.4156 (13)0.7340 (8)0.043
H100.11100.42480.78370.052*
N10.3520 (8)0.4262 (10)0.3821 (6)0.035
C120.2208 (8)0.3260 (12)0.6898 (7)0.042
H120.25040.27510.71060.051*
C50.4386 (7)0.5386 (12)0.3356 (7)0.027
O20.4225 (6)0.3218 (9)0.4993 (5)0.048
C60.4086 (9)0.5023 (13)0.2468 (7)0.032
C90.1317 (8)0.4783 (13)0.6286 (7)0.037
H90.10270.53220.60690.045*
C20.4800 (7)0.5996 (15)0.1379 (8)0.045
H20.49400.62180.07060.054*
C80.1718 (7)0.4559 (13)0.5590 (8)0.031
H80.16830.49040.48810.037*
C10.4311 (7)0.5364 (14)0.1461 (7)0.039
H10.41340.51690.08420.047*
C110.1819 (8)0.3396 (13)0.7624 (8)0.042
H110.18570.29730.83170.050*
C30.5076 (9)0.6294 (13)0.2292 (7)0.046
H30.53970.67220.22190.055*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.037 (3)0.0360 (4)0.0374 (4)0.0011 (6)0.0028 (6)0.0012 (3)
S10.028 (13)0.0433 (16)0.0279 (14)0.003 (2)0.003 (2)0.0009 (11)
N20.0370.0370.0370.0000.0020.001
O30.0350.0610.0380.0000.0000.000
O10.0540.0700.0330.0000.0010.000
C70.0290.0320.0280.0040.0000.000
C40.0330.0530.0490.0000.0000.000
C100.0420.0480.0400.0000.0150.000
N10.0310.0430.0300.0000.0000.002
C120.0530.0350.0390.0000.0000.004
C50.0280.0270.0270.0000.0000.000
O20.0440.0550.0450.0000.0000.014
C60.0230.0370.0340.0060.0000.000
C90.0300.0410.0410.0150.0000.000
C20.0420.0510.0430.0040.0100.005
C80.0210.0420.0310.0000.0000.004
C10.0350.0520.0300.0080.0000.000
C110.0490.0430.0340.0000.0000.005
C30.0300.0470.0620.0000.0090.003
Geometric parameters (Å, º) top
I1—N22.235 (15)C10—C91.408 (13)
I1—N12.214 (18)C10—C111.396 (19)
S1—O11.430 (8)C12—H120.9300
S1—N11.673 (19)C12—C111.38 (2)
S1—C51.767 (14)C5—C61.415 (14)
S1—O21.432 (10)C6—C11.409 (12)
N2—C121.350 (12)C9—H90.9300
N2—C81.375 (18)C9—C81.38 (2)
O3—C71.21 (2)C2—H20.9300
C7—N11.371 (13)C2—C11.405 (15)
C7—C61.43 (3)C2—C31.394 (14)
C4—H40.9300C8—H80.9300
C4—C51.399 (15)C1—H10.9300
C4—C31.399 (12)C11—H110.9300
C10—H100.9300C3—H30.9300
N1—I1—N2174.3 (4)C4—C5—S1127.7 (8)
O1—S1—N1111.0 (9)C4—C5—C6126.4 (12)
O1—S1—C5110.2 (5)C6—C5—S1105.6 (10)
O1—S1—O2116.6 (5)C5—C6—C7114.9 (11)
N1—S1—C595.3 (6)C1—C6—C7130.3 (14)
O2—S1—N1110.2 (7)C1—C6—C5114.8 (14)
O2—S1—C5111.6 (7)C10—C9—H9121.5
C12—N2—I1120.3 (12)C8—C9—C10116.9 (16)
C12—N2—C8118.3 (14)C8—C9—H9121.5
C8—N2—I1121.0 (7)C1—C2—H2119.6
O3—C7—N1123 (2)C3—C2—H2119.6
O3—C7—C6124.5 (11)C3—C2—C1120.8 (13)
N1—C7—C6112.0 (17)N2—C8—C9123.9 (12)
C5—C4—H4122.2N2—C8—H8118.1
C5—C4—C3115.6 (14)C9—C8—H8118.1
C3—C4—H4122.2C6—C1—H1119.5
C9—C10—H10120.6C2—C1—C6121.0 (13)
C11—C10—H10120.6C2—C1—H1119.5
C11—C10—C9118.8 (17)C10—C11—H11119.4
S1—N1—I1116.2 (4)C12—C11—C10121.2 (12)
C7—N1—I1131.0 (16)C12—C11—H11119.4
C7—N1—S1111.9 (16)C4—C3—H3119.4
N2—C12—H12119.6C2—C3—C4121.2 (16)
N2—C12—C11120.8 (15)C2—C3—H3119.4
C11—C12—H12119.6
I1—N2—C12—C11171.3 (8)N1—C7—C6—C1178.9 (11)
I1—N2—C8—C9169.2 (9)C12—N2—C8—C93.8 (17)
S1—C5—C6—C73.0 (13)C5—S1—N1—I1165.1 (5)
S1—C5—C6—C1177.6 (9)C5—S1—N1—C75.0 (9)
N2—C12—C11—C100.2 (18)C5—C4—C3—C22.5 (17)
O3—C7—N1—I112.6 (15)C5—C6—C1—C20.7 (17)
O3—C7—N1—S1179.2 (10)O2—S1—N1—I179.6 (7)
O3—C7—C6—C5177.2 (11)O2—S1—N1—C7110.3 (8)
O3—C7—C6—C12 (2)O2—S1—C5—C464.8 (13)
O1—S1—N1—I151.1 (6)O2—S1—C5—C6109.7 (9)
O1—S1—N1—C7119.0 (8)C6—C7—N1—I1164.2 (10)
O1—S1—C5—C466.3 (14)C6—C7—N1—S14.0 (14)
O1—S1—C5—C6119.1 (10)C9—C10—C11—C120.3 (18)
C7—C6—C1—C2180.0 (15)C8—N2—C12—C111.7 (17)
C4—C5—C6—C7177.6 (14)C1—C2—C3—C40.6 (18)
C4—C5—C6—C13.0 (17)C11—C10—C9—C81.4 (18)
C10—C9—C8—N23.6 (18)C3—C4—C5—S1177.3 (8)
N1—S1—C5—C4179.0 (12)C3—C4—C5—C63.8 (18)
N1—S1—C5—C64.5 (8)C3—C2—C1—C60.3 (19)
N1—C7—C6—C50.4 (17)
(dac_0.5_d_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 2.001 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 27.035 (13) ÅCell parameters from 3073 reflections
b = 7.6231 (15) Åθ = 3.1–24.9°
c = 12.507 (3) ŵ = 2.65 mm1
β = 88.799 (11)°T = 296 K
V = 2577.1 (14) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
603 reflections with I > 2σ(I)
φ and ω scansRint = 0.053
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction. wR2(int) was 0.0663 before and 0.0533 after correction. The Ratio of minimum to maximum transmission is 0.8630. The λ/2 correction factor is Not present.
θmax = 23.2°, θmin = 1.8°
Tmin = 0.486, Tmax = 0.563h = 1111
9685 measured reflectionsk = 88
773 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.039H-atom parameters constrained
wR(F2) = 0.100 w = 1/[σ2(Fo2) + (0.0416P)2 + 22.312P]
where P = (Fo2 + 2Fc2)/3
S = 1.15(Δ/σ)max < 0.001
773 reflectionsΔρmax = 0.54 e Å3
71 parametersΔρmin = 0.39 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28293 (7)0.39805 (9)0.47871 (5)0.0428 (10)
S10.4030 (2)0.4759 (4)0.4496 (2)0.043 (4)
N20.2166 (7)0.3840 (12)0.5893 (6)0.042
O30.3284 (7)0.4070 (10)0.2097 (6)0.050
O10.3946 (7)0.6223 (10)0.5178 (5)0.055
C70.3594 (11)0.4394 (14)0.2748 (9)0.039
C40.4884 (7)0.5959 (16)0.3303 (8)0.045
H40.50690.61170.39130.054*
C100.1369 (8)0.4162 (14)0.7328 (8)0.043
H100.11100.42810.78240.052*
N10.3530 (8)0.4264 (11)0.3829 (7)0.039
C120.2198 (8)0.3256 (13)0.6880 (7)0.045
H120.24900.27320.70910.054*
C50.4394 (7)0.5368 (13)0.3352 (7)0.032
O20.4236 (7)0.3225 (10)0.4988 (5)0.050
C60.4095 (9)0.5019 (14)0.2469 (7)0.034
C90.1317 (9)0.4755 (14)0.6293 (8)0.043
H90.10240.52550.60600.052*
C20.4798 (7)0.6006 (15)0.1375 (9)0.045
H20.49350.62410.07020.054*
C80.1739 (8)0.4552 (14)0.5605 (8)0.035
H80.17150.49440.49040.042*
C10.4315 (7)0.5367 (15)0.1463 (8)0.038
H10.41360.51690.08480.046*
C110.1805 (8)0.3398 (14)0.7623 (9)0.047
H110.18400.29740.83140.057*
C30.5075 (9)0.6296 (14)0.2279 (7)0.051
H30.53960.67230.22010.061*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.047 (3)0.0412 (5)0.0399 (5)0.0013 (6)0.0018 (6)0.0016 (3)
S10.048 (13)0.0496 (18)0.0305 (15)0.004 (3)0.000 (2)0.0017 (12)
N20.0420.0410.0410.0000.0020.001
O30.0390.0680.0430.0000.0000.000
O10.0570.0740.0350.0000.0010.000
C70.0380.0430.0380.0060.0000.000
C40.0320.0530.0490.0000.0000.000
C100.0420.0480.0390.0000.0150.000
N10.0350.0480.0340.0000.0000.002
C120.0570.0370.0410.0000.0000.005
C50.0330.0320.0320.0000.0000.000
O20.0460.0570.0470.0000.0000.015
C60.0250.0400.0370.0070.0000.000
C90.0340.0480.0470.0170.0000.000
C20.0420.0510.0430.0040.0100.005
C80.0230.0460.0340.0000.0000.005
C10.0340.0510.0290.0070.0000.000
C110.0560.0480.0380.0000.0000.005
C30.0330.0510.0680.0000.0090.004
Geometric parameters (Å, º) top
I1—N22.245 (16)C10—C91.382 (14)
I1—N12.231 (19)C10—C111.37 (2)
S1—O11.420 (8)C12—H120.9300
S1—N11.65 (2)C12—C111.40 (2)
S1—C51.780 (15)C5—C61.408 (14)
S1—O21.440 (10)C6—C11.404 (13)
N2—C121.317 (12)C9—H90.9300
N2—C81.332 (18)C9—C81.42 (2)
O3—C71.21 (2)C2—H20.9300
C7—N11.362 (14)C2—C11.397 (15)
C7—C61.47 (4)C2—C31.388 (14)
C4—H40.9300C8—H80.9300
C4—C51.399 (15)C1—H10.9300
C4—C31.395 (13)C11—H110.9300
C10—H100.9300C3—H30.9300
N1—I1—N2173.9 (5)C4—C5—S1128.8 (9)
O1—S1—N1111.2 (9)C4—C5—C6125.7 (12)
O1—S1—C5110.9 (6)C6—C5—S1105.3 (11)
O1—S1—O2116.1 (5)C5—C6—C7114.5 (11)
N1—S1—C595.6 (7)C1—C6—C7130.1 (14)
O2—S1—N1111.1 (7)C1—C6—C5115.4 (15)
O2—S1—C5110.0 (8)C10—C9—H9122.1
C12—N2—I1121.8 (13)C10—C9—C8115.7 (17)
C12—N2—C8117.7 (15)C8—C9—H9122.1
C8—N2—I1120.0 (8)C1—C2—H2119.6
O3—C7—N1125 (2)C3—C2—H2119.6
O3—C7—C6123.7 (12)C3—C2—C1120.8 (13)
N1—C7—C6110.9 (19)N2—C8—C9124.8 (12)
C5—C4—H4122.2N2—C8—H8117.6
C3—C4—H4122.2C9—C8—H8117.6
C3—C4—C5115.6 (14)C6—C1—H1119.5
C9—C10—H10120.1C2—C1—C6120.9 (13)
C11—C10—H10120.1C2—C1—H1119.5
C11—C10—C9119.7 (18)C10—C11—C12119.9 (12)
S1—N1—I1116.5 (5)C10—C11—H11120.0
C7—N1—I1129.0 (17)C12—C11—H11120.0
C7—N1—S1113.4 (17)C4—C3—H3119.3
N2—C12—H12118.9C2—C3—C4121.5 (17)
N2—C12—C11122.2 (16)C2—C3—H3119.3
C11—C12—H12118.9
I1—N2—C12—C11170.5 (9)N1—C7—C6—C1178.7 (11)
I1—N2—C8—C9170.9 (10)C12—N2—C8—C91.1 (19)
S1—C5—C6—C73.2 (14)C5—S1—N1—I1165.4 (6)
S1—C5—C6—C1178.6 (9)C5—S1—N1—C73.7 (10)
N2—C12—C11—C100.2 (19)C5—C4—C3—C21.8 (18)
O3—C7—N1—I113.8 (18)C5—C6—C1—C20.3 (17)
O3—C7—N1—S1178.7 (11)O2—S1—N1—I180.6 (8)
O3—C7—C6—C5178.2 (12)O2—S1—N1—C7110.3 (9)
O3—C7—C6—C10 (3)O2—S1—C5—C465.1 (14)
O1—S1—N1—I150.4 (6)O2—S1—C5—C6111.0 (9)
O1—S1—N1—C7118.7 (9)C6—C7—N1—I1165.1 (10)
O1—S1—C5—C464.7 (16)C6—C7—N1—S12.3 (15)
O1—S1—C5—C6119.2 (10)C9—C10—C11—C121 (2)
C7—C6—C1—C2178.2 (16)C8—N2—C12—C111.4 (19)
C4—C5—C6—C7179.5 (15)C1—C2—C3—C40.1 (19)
C4—C5—C6—C12.3 (18)C11—C10—C9—C81.5 (19)
C10—C9—C8—N20.3 (19)C3—C4—C5—S1178.4 (9)
N1—S1—C5—C4180.0 (13)C3—C4—C5—C63.1 (19)
N1—S1—C5—C63.8 (8)C3—C2—C1—C61 (2)
N1—C7—C6—C50.8 (18)
(dac_0.8_d_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 2.061 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 26.869 (13) ÅCell parameters from 3197 reflections
b = 7.4985 (14) Åθ = 3.1–22.0°
c = 12.418 (3) ŵ = 2.73 mm1
β = 88.952 (10)°T = 296 K
V = 2501.5 (14) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
603 reflections with I > 2σ(I)
φ and ω scansRint = 0.049
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction. wR2(int) was 0.0633 before and 0.0514 after correction. The Ratio of minimum to maximum transmission is 0.8516. The λ/2 correction factor is Not present.
θmax = 23.2°, θmin = 1.8°
Tmin = 0.479, Tmax = 0.563h = 1111
9489 measured reflectionsk = 88
759 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.037H-atom parameters constrained
wR(F2) = 0.101 w = 1/[σ2(Fo2) + (0.0423P)2 + 29.2986P]
where P = (Fo2 + 2Fc2)/3
S = 1.14(Δ/σ)max < 0.001
759 reflectionsΔρmax = 0.82 e Å3
71 parametersΔρmin = 0.49 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28186 (7)0.39836 (9)0.47820 (5)0.0373 (10)
S10.4022 (3)0.4777 (4)0.4498 (2)0.041 (4)
N20.2162 (7)0.3846 (12)0.5888 (6)0.034
O30.3288 (7)0.4043 (11)0.2070 (6)0.043
O10.3941 (7)0.6278 (10)0.5184 (5)0.047
C70.3601 (10)0.4379 (13)0.2727 (8)0.028
C40.4876 (7)0.5971 (16)0.3329 (9)0.041
H40.50580.61220.39520.049*
C100.1369 (8)0.4165 (14)0.7345 (8)0.038
H100.11080.42700.78420.045*
N10.3523 (8)0.4281 (12)0.3814 (7)0.035
C120.2198 (9)0.3253 (14)0.6900 (8)0.041
H120.24930.27200.71110.049*
C50.4380 (7)0.5395 (14)0.3355 (8)0.031
O20.4215 (7)0.3211 (10)0.5007 (6)0.044
C60.4088 (9)0.5040 (14)0.2452 (7)0.026
C90.1314 (9)0.4772 (14)0.6301 (8)0.036
H90.10190.52840.60750.043*
C20.4812 (7)0.5981 (17)0.1379 (9)0.046
H20.49600.61780.07060.055*
C80.1723 (8)0.4578 (15)0.5605 (9)0.030
H80.16930.49770.49000.036*
C10.4323 (7)0.5357 (15)0.1452 (8)0.035
H10.41480.51490.08240.042*
C110.1810 (8)0.3410 (15)0.7640 (9)0.044
H110.18490.30010.83400.052*
C30.5079 (9)0.6307 (15)0.2302 (7)0.045
H30.54010.67590.22400.054*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.041 (3)0.0354 (4)0.0351 (5)0.0017 (6)0.0003 (6)0.0012 (3)
S10.059 (12)0.0394 (17)0.0252 (15)0.003 (2)0.001 (2)0.0013 (12)
N20.0340.0340.0340.0000.0020.001
O30.0340.0590.0370.0000.0000.000
O10.0480.0630.0290.0000.0010.000
C70.0270.0300.0270.0040.0000.000
C40.0300.0480.0440.0000.0000.000
C100.0360.0420.0340.0000.0130.000
N10.0320.0440.0310.0000.0000.002
C120.0520.0340.0380.0000.0000.004
C50.0310.0300.0310.0000.0000.000
O20.0400.0500.0410.0000.0000.013
C60.0190.0300.0280.0050.0000.000
C90.0290.0400.0390.0150.0000.000
C20.0420.0520.0430.0040.0100.005
C80.0200.0400.0290.0000.0000.004
C10.0320.0470.0270.0070.0000.000
C110.0510.0450.0350.0000.0000.005
C30.0290.0460.0610.0000.0080.003
Geometric parameters (Å, º) top
I1—N22.219 (16)C10—C91.384 (14)
I1—N12.233 (19)C10—C111.37 (2)
S1—O11.427 (8)C12—H120.9300
S1—N11.64 (2)C12—C111.38 (2)
S1—C51.762 (15)C5—C61.406 (14)
S1—O21.434 (11)C6—C11.401 (13)
N2—C121.338 (13)C9—H90.9300
N2—C81.352 (18)C9—C81.39 (2)
O3—C71.21 (2)C2—H20.9300
C7—N11.365 (14)C2—C11.398 (15)
C7—C61.44 (3)C2—C31.386 (14)
C4—H40.9300C8—H80.9300
C4—C51.399 (15)C1—H10.9300
C4—C31.401 (13)C11—H110.9300
C10—H100.9300C3—H30.9300
N2—I1—N1173.7 (5)C4—C5—S1127.2 (9)
O1—S1—N1111.7 (9)C4—C5—C6125.7 (13)
O1—S1—C5110.4 (6)C6—C5—S1106.8 (11)
O1—S1—O2115.8 (5)C5—C6—C7113.3 (11)
N1—S1—C594.7 (7)C1—C6—C7131.5 (14)
O2—S1—N1110.3 (7)C1—C6—C5115.2 (14)
O2—S1—C5112.0 (8)C10—C9—H9121.6
C12—N2—I1121.7 (13)C10—C9—C8116.8 (17)
C12—N2—C8117.3 (15)C8—C9—H9121.6
C8—N2—I1120.5 (8)C1—C2—H2119.8
O3—C7—N1124 (2)C3—C2—H2119.8
O3—C7—C6123.6 (12)C3—C2—C1120.4 (14)
N1—C7—C6112.1 (18)N2—C8—C9124.2 (12)
C5—C4—H4122.2N2—C8—H8117.9
C5—C4—C3115.7 (15)C9—C8—H8117.9
C3—C4—H4122.2C6—C1—H1119.3
C9—C10—H10120.2C2—C1—C6121.4 (13)
C11—C10—H10120.2C2—C1—H1119.3
C11—C10—C9119.6 (17)C10—C11—C12120.2 (13)
S1—N1—I1115.9 (5)C10—C11—H11119.9
C7—N1—I1130.6 (17)C12—C11—H11119.9
C7—N1—S1112.7 (17)C4—C3—H3119.3
N2—C12—H12119.1C2—C3—C4121.4 (17)
N2—C12—C11121.9 (17)C2—C3—H3119.3
C11—C12—H12119.1
I1—N2—C12—C11170.2 (10)N1—C7—C6—C1179.7 (12)
I1—N2—C8—C9170.7 (10)C12—N2—C8—C91.0 (19)
S1—C5—C6—C72.3 (13)C5—S1—N1—I1165.5 (6)
S1—C5—C6—C1176.6 (9)C5—S1—N1—C75.6 (9)
N2—C12—C11—C101 (2)C5—C4—C3—C23.7 (18)
O3—C7—N1—I111.9 (17)C5—C6—C1—C20.1 (18)
O3—C7—N1—S1178.8 (11)O2—S1—N1—I179.0 (8)
O3—C7—C6—C5177.7 (12)O2—S1—N1—C7110.0 (9)
O3—C7—C6—C14 (3)O2—S1—C5—C464.8 (14)
O1—S1—N1—I151.3 (6)O2—S1—C5—C6109.7 (10)
O1—S1—N1—C7119.7 (9)C6—C7—N1—I1164.3 (10)
O1—S1—C5—C465.8 (15)C6—C7—N1—S15.0 (15)
O1—S1—C5—C6119.7 (10)C9—C10—C11—C120 (2)
C7—C6—C1—C2178.7 (16)C8—N2—C12—C111.4 (19)
C4—C5—C6—C7177.0 (14)C1—C2—C3—C42 (2)
C4—C5—C6—C12.0 (18)C11—C10—C9—C80.4 (19)
C10—C9—C8—N20.1 (19)C3—C4—C5—S1177.3 (9)
N1—S1—C5—C4179.0 (13)C3—C4—C5—C63.7 (19)
N1—S1—C5—C64.4 (9)C3—C2—C1—C60 (2)
N1—C7—C6—C51.5 (17)
(dac_0.9_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 2.087 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 26.806 (12) ÅCell parameters from 3682 reflections
b = 7.4450 (14) Åθ = 3.1–24.3°
c = 12.380 (2) ŵ = 2.77 mm1
β = 89.057 (10)°T = 296 K
V = 2470.4 (13) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
573 reflections with I > 2σ(I)
φ and ω scansRint = 0.046
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction.
θmax = 23.2°, θmin = 1.8°
Tmin = 0.461, Tmax = 0.563h = 1010
9464 measured reflectionsk = 88
706 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.033H-atom parameters constrained
wR(F2) = 0.090 w = 1/[σ2(Fo2) + (0.0368P)2 + 25.1886P]
where P = (Fo2 + 2Fc2)/3
S = 1.16(Δ/σ)max < 0.001
706 reflectionsΔρmax = 0.82 e Å3
71 parametersΔρmin = 0.43 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28149 (6)0.39844 (9)0.47798 (5)0.0334 (10)
S10.4022 (2)0.4789 (3)0.44983 (18)0.037 (4)
N20.2165 (7)0.3868 (11)0.5890 (6)0.032
O30.3292 (7)0.4050 (10)0.2060 (6)0.040
O10.3931 (7)0.6310 (10)0.5182 (5)0.044
C70.3602 (10)0.4380 (12)0.2718 (8)0.022
C40.4869 (7)0.5979 (16)0.3321 (8)0.041
H40.50500.61480.39470.049*
C100.1374 (8)0.4178 (13)0.7348 (8)0.032
H100.11160.42810.78550.039*
N10.3512 (8)0.4287 (11)0.3804 (6)0.033
C120.2209 (8)0.3256 (13)0.6911 (7)0.036
H120.25050.27120.71190.043*
C50.4376 (7)0.5393 (13)0.3360 (7)0.026
O20.4214 (6)0.3224 (9)0.5014 (5)0.039
C60.4096 (9)0.5041 (13)0.2447 (6)0.026
C90.1297 (8)0.4787 (13)0.6308 (7)0.032
H90.09980.52880.60900.038*
C20.4814 (7)0.5987 (15)0.1378 (8)0.038
H20.49630.61940.07060.046*
C80.1714 (7)0.4582 (14)0.5607 (8)0.026
H80.16790.49600.48960.031*
C10.4326 (7)0.5361 (14)0.1444 (7)0.030
H10.41510.51520.08140.036*
C110.1814 (8)0.3432 (13)0.7659 (8)0.035
H110.18520.30410.83660.042*
C30.5078 (9)0.6302 (14)0.2305 (7)0.040
H30.54020.67390.22490.048*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.038 (3)0.0305 (4)0.0320 (4)0.0012 (6)0.0027 (6)0.0013 (3)
S10.052 (13)0.0350 (15)0.0233 (13)0.004 (2)0.001 (2)0.0016 (11)
N20.0320.0320.0320.0000.0020.001
O30.0310.0540.0340.0000.0000.000
O10.0460.0600.0280.0000.0010.000
C70.0220.0240.0210.0030.0000.000
C40.0290.0480.0440.0000.0000.000
C100.0310.0360.0300.0000.0110.000
N10.0300.0400.0280.0000.0000.002
C120.0450.0290.0330.0000.0000.004
C50.0270.0260.0260.0000.0000.000
O20.0350.0450.0360.0000.0000.012
C60.0200.0310.0290.0050.0000.000
C90.0250.0350.0350.0130.0000.000
C20.0350.0430.0360.0030.0090.004
C80.0180.0350.0260.0000.0000.004
C10.0270.0410.0230.0060.0000.000
C110.0410.0360.0280.0000.0000.004
C30.0260.0400.0540.0000.0070.003
Geometric parameters (Å, º) top
I1—N22.203 (15)C10—C91.385 (13)
I1—N12.220 (18)C10—C111.364 (19)
S1—O11.433 (8)C12—H120.9300
S1—N11.67 (2)C12—C111.40 (2)
S1—C51.745 (14)C5—C61.393 (14)
S1—O21.430 (10)C6—C11.398 (13)
N2—C121.350 (12)C9—H90.9300
N2—C81.373 (18)C9—C81.41 (2)
O3—C71.20 (2)C2—H20.9300
C7—N11.364 (13)C2—C11.389 (15)
C7—C61.45 (3)C2—C31.379 (14)
C4—H40.9300C8—H80.9300
C4—C51.392 (15)C1—H10.9300
C4—C31.390 (13)C11—H110.9300
C10—H100.9300C3—H30.9300
N2—I1—N1173.5 (4)C4—C5—S1127.8 (8)
O1—S1—N1110.4 (9)C4—C5—C6123.7 (13)
O1—S1—C5111.0 (6)C6—C5—S1108.3 (11)
N1—S1—C594.7 (7)C5—C6—C7112.3 (11)
O2—S1—O1116.1 (5)C5—C6—C1117.0 (14)
O2—S1—N1110.7 (7)C1—C6—C7130.8 (13)
O2—S1—C5112.0 (8)C10—C9—H9123.0
C12—N2—I1121.1 (12)C10—C9—C8114.1 (16)
C12—N2—C8117.4 (14)C8—C9—H9123.0
C8—N2—I1121.1 (7)C1—C2—H2119.8
O3—C7—N1123 (2)C3—C2—H2119.8
O3—C7—C6123.6 (11)C3—C2—C1120.3 (13)
N1—C7—C6113.1 (17)N2—C8—C9125.2 (11)
C5—C4—H4121.5N2—C8—H8117.4
C3—C4—H4121.5C9—C8—H8117.4
C3—C4—C5117.0 (14)C6—C1—H1119.7
C9—C10—H10118.7C2—C1—C6120.7 (13)
C11—C10—H10118.7C2—C1—H1119.7
C11—C10—C9122.6 (16)C10—C11—C12119.9 (12)
S1—N1—I1115.6 (4)C10—C11—H11120.0
C7—N1—I1132.4 (16)C12—C11—H11120.0
C7—N1—S1111.3 (16)C4—C3—H3119.4
N2—C12—H12119.7C2—C3—C4121.2 (16)
N2—C12—C11120.7 (15)C2—C3—H3119.4
C11—C12—H12119.7
I1—N2—C12—C11170.5 (9)N1—C7—C6—C1178.7 (11)
I1—N2—C8—C9171.1 (9)C12—N2—C8—C92.4 (18)
S1—C5—C6—C72.7 (13)C5—S1—N1—I1166.0 (5)
S1—C5—C6—C1177.1 (9)C5—S1—N1—C75.9 (9)
N2—C12—C11—C102.0 (18)C5—C4—C3—C22.4 (17)
O3—C7—N1—I110.9 (16)C5—C6—C1—C20.6 (17)
O3—C7—N1—S1178.9 (10)O2—S1—N1—I178.3 (7)
O3—C7—C6—C5177.3 (11)O2—S1—N1—C7109.7 (8)
O3—C7—C6—C13 (2)O2—S1—C5—C465.1 (13)
O1—S1—N1—I151.6 (6)O2—S1—C5—C6109.6 (10)
O1—S1—N1—C7120.4 (8)C6—C7—N1—I1164.9 (10)
O1—S1—C5—C466.4 (15)C6—C7—N1—S15.3 (14)
O1—S1—C5—C6118.9 (10)C9—C10—C11—C120.1 (18)
C7—C6—C1—C2179.2 (15)C8—N2—C12—C113.1 (17)
C4—C5—C6—C7177.6 (13)C1—C2—C3—C41.0 (18)
C4—C5—C6—C12.2 (17)C11—C10—C9—C80.5 (17)
C10—C9—C8—N20.6 (17)C3—C4—C5—S1177.0 (9)
N1—S1—C5—C4179.6 (12)C3—C4—C5—C63.1 (18)
N1—S1—C5—C64.9 (8)C3—C2—C1—C60.0 (19)
N1—C7—C6—C51.5 (17)
(dac_1.3_d_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 2.117 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 26.742 (14) ÅCell parameters from 3223 reflections
b = 7.3842 (15) Åθ = 3.2–25.9°
c = 12.337 (3) ŵ = 2.81 mm1
β = 89.154 (11)°T = 296 K
V = 2436.0 (15) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
582 reflections with I > 2σ(I)
φ and ω scansRint = 0.053
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction. wR2(int) was 0.0628 before and 0.0541 after correction. The Ratio of minimum to maximum transmission is 0.8665. The λ/2 correction factor is Not present.
θmax = 23.3°, θmin = 1.8°
Tmin = 0.488, Tmax = 0.563h = 1111
8933 measured reflectionsk = 88
712 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.043H-atom parameters constrained
wR(F2) = 0.109 w = 1/[σ2(Fo2) + (0.0253P)2 + 80.1818P]
where P = (Fo2 + 2Fc2)/3
S = 1.14(Δ/σ)max < 0.001
712 reflectionsΔρmax = 0.72 e Å3
71 parametersΔρmin = 0.41 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28091 (9)0.39881 (12)0.47764 (7)0.0319 (12)
S10.4016 (3)0.4806 (5)0.4501 (3)0.037 (5)
N20.2164 (9)0.3876 (15)0.5891 (8)0.030
O30.3286 (9)0.4023 (14)0.2044 (8)0.038
O10.3938 (9)0.6329 (13)0.5183 (7)0.038
C70.3598 (13)0.4378 (17)0.2700 (11)0.025
C40.4869 (9)0.600 (2)0.3337 (11)0.040
H40.50510.61680.39650.048*
C100.1367 (10)0.4178 (19)0.7365 (10)0.034
H100.11020.42460.78610.040*
N10.3505 (11)0.4296 (15)0.3794 (9)0.031
C120.2205 (11)0.3260 (18)0.6916 (10)0.036
H120.25000.26990.71200.043*
C50.4375 (9)0.5401 (17)0.3371 (10)0.024
O20.4209 (9)0.3224 (13)0.5024 (7)0.036
C60.4099 (12)0.5059 (18)0.2440 (8)0.024
C90.1311 (11)0.4819 (18)0.6309 (10)0.032
H90.10150.53580.60870.038*
C20.4819 (9)0.598 (2)0.1379 (11)0.039
H20.49730.61700.07070.046*
C80.1714 (10)0.4616 (19)0.5609 (11)0.026
H80.16780.50070.48980.032*
C10.4329 (9)0.535 (2)0.1437 (10)0.032
H10.41550.51310.08040.039*
C110.1824 (10)0.3435 (18)0.7669 (11)0.034
H110.18710.30590.83800.041*
C30.5076 (12)0.6331 (19)0.2320 (9)0.039
H30.53980.68020.22690.046*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.034 (4)0.0300 (5)0.0318 (5)0.0013 (8)0.0018 (7)0.0013 (4)
S10.053 (17)0.035 (2)0.0228 (18)0.005 (3)0.000 (3)0.0017 (15)
N20.0300.0300.0300.0000.0020.001
O30.0300.0520.0330.0000.0000.000
O10.0390.0510.0240.0000.0010.000
C70.0240.0270.0240.0040.0000.000
C40.0290.0470.0430.0000.0000.000
C100.0320.0370.0310.0000.0120.000
N10.0280.0380.0260.0000.0000.002
C120.0450.0290.0330.0000.0000.004
C50.0240.0230.0240.0000.0000.000
O20.0330.0420.0340.0000.0000.011
C60.0180.0280.0260.0050.0000.000
C90.0250.0350.0350.0130.0000.000
C20.0360.0430.0370.0030.0090.004
C80.0180.0350.0260.0000.0000.004
C10.0290.0430.0250.0060.0000.000
C110.0400.0350.0280.0000.0000.004
C30.0250.0390.0520.0000.0070.003
Geometric parameters (Å, º) top
I1—N22.192 (19)C10—C91.397 (17)
I1—N12.22 (2)C10—C111.40 (2)
S1—O11.419 (10)C12—H120.9300
S1—N11.68 (3)C12—C111.37 (3)
S1—C51.737 (19)C5—C61.398 (16)
S1—O21.434 (13)C6—C11.390 (15)
N2—C121.351 (16)C9—H90.9300
N2—C81.37 (2)C9—C81.38 (3)
O3—C71.20 (3)C2—H20.9300
C7—N11.370 (18)C2—C11.390 (17)
C7—C61.46 (4)C2—C31.383 (16)
C4—H40.9300C8—H80.9300
C4—C51.394 (17)C1—H10.9300
C4—C31.384 (15)C11—H110.9300
C10—H100.9300C3—H30.9300
N2—I1—N1173.3 (6)C4—C5—S1128.1 (11)
O1—S1—N1111.8 (11)C4—C5—C6123.0 (17)
O1—S1—C5110.5 (7)C6—C5—S1108.8 (14)
O1—S1—O2115.4 (6)C5—C6—C7112.0 (14)
N1—S1—C594.9 (8)C1—C6—C7129.9 (18)
O2—S1—N1110.7 (9)C1—C6—C5118.1 (19)
O2—S1—C5111.7 (10)C10—C9—H9121.5
C12—N2—I1121.8 (16)C8—C9—C10117 (2)
C12—N2—C8117.1 (19)C8—C9—H9121.5
C8—N2—I1120.8 (10)C1—C2—H2120.1
O3—C7—N1122 (3)C3—C2—H2120.1
O3—C7—C6124.8 (15)C3—C2—C1119.9 (17)
N1—C7—C6113 (2)N2—C8—C9124.4 (16)
C5—C4—H4121.7N2—C8—H8117.8
C3—C4—H4121.7C9—C8—H8117.8
C3—C4—C5116.7 (19)C6—C1—C2120.2 (17)
C9—C10—H10120.3C6—C1—H1119.9
C11—C10—H10120.3C2—C1—H1119.9
C11—C10—C9119 (2)C10—C11—H11120.1
S1—N1—I1115.1 (6)C12—C11—C10119.9 (16)
C7—N1—I1133 (2)C12—C11—H11120.1
C7—N1—S1111 (2)C4—C3—H3119.0
N2—C12—H12118.9C2—C3—C4122 (2)
N2—C12—C11122 (2)C2—C3—H3119.0
C11—C12—H12118.9
I1—N2—C12—C11170.0 (13)N1—C7—C6—C1179.2 (15)
I1—N2—C8—C9171.0 (13)C12—N2—C8—C92 (2)
S1—C5—C6—C71.9 (17)C5—S1—N1—I1166.5 (7)
S1—C5—C6—C1176.7 (12)C5—S1—N1—C76.0 (12)
N2—C12—C11—C104 (2)C5—C4—C3—C24 (2)
O3—C7—N1—I111 (2)C5—C6—C1—C20 (2)
O3—C7—N1—S1178.4 (13)O2—S1—N1—I178.1 (10)
O3—C7—C6—C5178.2 (15)O2—S1—N1—C7109.4 (12)
O3—C7—C6—C13 (3)O2—S1—C5—C465.5 (17)
O1—S1—N1—I152.1 (8)O2—S1—C5—C6110.0 (12)
O1—S1—N1—C7120.4 (11)C6—C7—N1—I1164.9 (13)
O1—S1—C5—C464.5 (19)C6—C7—N1—S15.8 (19)
O1—S1—C5—C6120.0 (13)C9—C10—C11—C123 (2)
C7—C6—C1—C2179 (2)C8—N2—C12—C113 (2)
C4—C5—C6—C7177.7 (18)C1—C2—C3—C43 (3)
C4—C5—C6—C11 (2)C11—C10—C9—C82 (2)
C10—C9—C8—N22 (2)C3—C4—C5—S1177.9 (12)
N1—S1—C5—C4180.0 (16)C3—C4—C5—C63 (2)
N1—S1—C5—C64.5 (11)C3—C2—C1—C61 (3)
N1—C7—C6—C52 (2)
(dac_1.5_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 2.150 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 26.653 (12) ÅCell parameters from 3792 reflections
b = 7.3257 (13) Åθ = 3.2–23.3°
c = 12.284 (2) ŵ = 2.85 mm1
β = 89.236 (10)°T = 296 K
V = 2398.2 (12) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
582 reflections with I > 2σ(I)
φ and ω scansRint = 0.044
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction.
θmax = 23.3°, θmin = 1.8°
Tmin = 0.461, Tmax = 0.563h = 1010
9116 measured reflectionsk = 88
688 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.037H-atom parameters constrained
wR(F2) = 0.095 w = 1/[σ2(Fo2) + (0.0269P)2 + 58.096P]
where P = (Fo2 + 2Fc2)/3
S = 1.13(Δ/σ)max < 0.001
688 reflectionsΔρmax = 0.85 e Å3
71 parametersΔρmin = 0.44 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28047 (8)0.39904 (10)0.47741 (6)0.0301 (11)
S10.4016 (3)0.4811 (4)0.4502 (2)0.037 (4)
N20.2163 (8)0.3876 (13)0.5893 (7)0.029
O30.3285 (8)0.4022 (12)0.2033 (6)0.035
O10.3925 (8)0.6370 (11)0.5181 (6)0.038
C70.3598 (12)0.4375 (15)0.2701 (9)0.024
C40.4876 (8)0.5997 (19)0.3346 (10)0.037
H40.50560.61630.39820.044*
C100.1370 (8)0.4193 (15)0.7375 (9)0.029
H100.11090.42850.78820.034*
N10.3510 (9)0.4292 (12)0.3793 (7)0.028
C120.2209 (10)0.3263 (15)0.6931 (8)0.034
H120.25060.27110.71430.041*
C50.4380 (8)0.5408 (15)0.3365 (8)0.023
O20.4200 (7)0.3230 (11)0.5033 (6)0.034
C60.4103 (10)0.5053 (15)0.2432 (7)0.023
C90.1302 (9)0.4805 (16)0.6321 (9)0.030
H90.10010.53100.60990.036*
C20.4826 (8)0.5997 (18)0.1385 (9)0.038
H20.49810.62040.07130.045*
C80.1707 (8)0.4624 (16)0.5619 (9)0.026
H80.16700.50360.49090.031*
C10.4333 (8)0.5361 (17)0.1423 (9)0.030
H10.41600.51440.07840.036*
C110.1821 (9)0.3450 (16)0.7673 (9)0.033
H110.18650.30670.83870.040*
C30.5089 (10)0.6325 (16)0.2328 (8)0.035
H30.54150.67750.22780.042*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.033 (4)0.0274 (4)0.0294 (5)0.0001 (7)0.0022 (6)0.0011 (3)
S10.062 (14)0.0302 (17)0.0198 (15)0.004 (3)0.002 (3)0.0011 (12)
N20.0290.0290.0290.0000.0020.001
O30.0270.0470.0300.0000.0000.000
O10.0390.0510.0240.0000.0010.000
C70.0240.0260.0230.0030.0000.000
C40.0270.0430.0400.0000.0000.000
C100.0270.0320.0260.0000.0100.000
N10.0250.0340.0240.0000.0000.001
C120.0430.0280.0310.0000.0000.003
C50.0230.0230.0230.0000.0000.000
O20.0310.0400.0320.0000.0000.010
C60.0170.0270.0250.0050.0000.000
C90.0240.0330.0320.0120.0000.000
C20.0350.0420.0360.0030.0090.004
C80.0170.0340.0250.0000.0000.004
C10.0270.0400.0230.0060.0000.000
C110.0390.0340.0270.0000.0000.004
C30.0230.0360.0480.0000.0070.003
Geometric parameters (Å, º) top
I1—N22.181 (17)C10—C91.383 (15)
I1—N12.23 (2)C10—C111.37 (2)
S1—O11.433 (9)C12—H120.9300
S1—N11.66 (2)C12—C111.37 (2)
S1—C51.745 (17)C5—C61.396 (15)
S1—O21.419 (11)C6—C11.393 (14)
N2—C121.359 (13)C9—H90.9300
N2—C81.380 (19)C9—C81.38 (2)
O3—C71.21 (3)C2—H20.9300
C7—N11.360 (15)C2—C11.394 (16)
C7—C61.47 (4)C2—C31.383 (15)
C4—H40.9300C8—H80.9300
C4—C51.391 (16)C1—H10.9300
C4—C31.387 (14)C11—H110.9300
C10—H100.9300C3—H30.9300
N2—I1—N1172.9 (5)C4—C5—S1127.5 (9)
O1—S1—N1110.8 (10)C4—C5—C6123.8 (14)
O1—S1—C5110.7 (6)C6—C5—S1108.5 (12)
N1—S1—C594.8 (7)C5—C6—C7111.7 (12)
O2—S1—O1116.1 (5)C1—C6—C7130.3 (15)
O2—S1—N1110.0 (8)C1—C6—C5118.0 (16)
O2—S1—C5112.4 (9)C10—C9—H9121.8
C12—N2—I1121.7 (14)C8—C9—C10116.4 (18)
C12—N2—C8116.7 (16)C8—C9—H9121.8
C8—N2—I1121.1 (8)C1—C2—H2119.4
O3—C7—N1123 (2)C3—C2—H2119.4
O3—C7—C6124.0 (13)C3—C2—C1121.2 (15)
N1—C7—C6113 (2)N2—C8—H8117.6
C5—C4—H4121.8C9—C8—N2124.8 (13)
C3—C4—H4121.8C9—C8—H8117.6
C3—C4—C5116.5 (16)C6—C1—C2119.2 (15)
C9—C10—H10119.9C6—C1—H1120.4
C11—C10—H10119.9C2—C1—H1120.4
C11—C10—C9120.2 (18)C10—C11—C12121.0 (14)
S1—N1—I1115.1 (5)C10—C11—H11119.5
C7—N1—I1132.1 (19)C12—C11—H11119.5
C7—N1—S1112.1 (19)C4—C3—H3119.4
N2—C12—H12119.6C2—C3—C4121.3 (18)
N2—C12—C11120.9 (18)C2—C3—H3119.4
C11—C12—H12119.6
I1—N2—C12—C11170.3 (10)N1—C7—C6—C1178.9 (13)
I1—N2—C8—C9171.9 (11)C12—N2—C8—C91 (2)
S1—C5—C6—C72.3 (15)C5—S1—N1—I1166.3 (6)
S1—C5—C6—C1177.3 (11)C5—S1—N1—C75.5 (10)
N2—C12—C11—C103 (2)C5—C4—C3—C23 (2)
O3—C7—N1—I111.3 (19)C5—C6—C1—C20.3 (19)
O3—C7—N1—S1178.8 (12)O2—S1—N1—I177.8 (8)
O3—C7—C6—C5177.8 (13)O2—S1—N1—C7110.4 (10)
O3—C7—C6—C13 (3)O2—S1—C5—C465.4 (14)
O1—S1—N1—I152.0 (7)O2—S1—C5—C6109.6 (11)
O1—S1—N1—C7119.8 (10)C6—C7—N1—I1165.0 (11)
O1—S1—C5—C466.3 (16)C6—C7—N1—S15.0 (16)
O1—S1—C5—C6118.7 (11)C9—C10—C11—C121 (2)
C7—C6—C1—C2179.1 (17)C8—N2—C12—C112.2 (19)
C4—C5—C6—C7177.5 (15)C1—C2—C3—C41 (2)
C4—C5—C6—C12.0 (19)C11—C10—C9—C80 (2)
C10—C9—C8—N20 (2)C3—C4—C5—S1177.6 (10)
N1—S1—C5—C4179.4 (13)C3—C4—C5—C63 (2)
N1—S1—C5—C64.4 (9)C3—C2—C1—C60 (2)
N1—C7—C6—C51.6 (19)
(dac_1.9_d_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 2.190 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 26.581 (13) ÅCell parameters from 3433 reflections
b = 7.2485 (14) Åθ = 3.2–24.6°
c = 12.220 (2) ŵ = 2.90 mm1
β = 89.447 (10)°T = 296 K
V = 2354.4 (13) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
590 reflections with I > 2σ(I)
φ and ω scansRint = 0.047
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction.
θmax = 23.2°, θmin = 1.8°
Tmin = 0.461, Tmax = 0.563h = 1110
8768 measured reflectionsk = 88
687 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.042H-atom parameters constrained
wR(F2) = 0.102 w = 1/[σ2(Fo2) + (0.014P)2 + 86.6837P]
where P = (Fo2 + 2Fc2)/3
S = 1.17(Δ/σ)max < 0.001
687 reflectionsΔρmax = 0.81 e Å3
71 parametersΔρmin = 0.43 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.27982 (10)0.39972 (12)0.47704 (7)0.0298 (12)
S10.4010 (4)0.4827 (5)0.4503 (3)0.036 (5)
N20.2162 (9)0.3899 (16)0.5897 (8)0.028
O30.3275 (9)0.4005 (14)0.2005 (7)0.032
O10.3924 (9)0.6392 (13)0.5180 (7)0.035
C70.3580 (14)0.4373 (18)0.2677 (11)0.024
C40.4885 (10)0.599 (2)0.3361 (11)0.035
H40.50670.61340.40010.042*
C100.1367 (10)0.4216 (18)0.7385 (10)0.026
H100.11060.43320.78950.031*
N10.3512 (11)0.4305 (15)0.3783 (9)0.025
C120.2201 (12)0.3253 (18)0.6938 (10)0.031
H120.24960.26630.71460.037*
C50.4388 (9)0.5419 (18)0.3360 (10)0.022
O20.4195 (9)0.3245 (12)0.5048 (7)0.029
C60.4108 (12)0.5051 (18)0.2433 (8)0.019
C90.1298 (11)0.4814 (19)0.6327 (11)0.030
H90.09920.52890.60970.036*
C20.4826 (9)0.600 (2)0.1387 (11)0.032
H20.49820.61980.07130.038*
C80.1707 (10)0.467 (2)0.5622 (11)0.024
H80.16730.51330.49160.029*
C10.4332 (9)0.536 (2)0.1423 (10)0.028
H10.41560.51500.07810.034*
C110.1816 (10)0.3451 (18)0.7694 (11)0.028
H110.18600.30650.84130.034*
C30.5090 (13)0.6335 (19)0.2340 (9)0.033
H30.54140.68070.22890.040*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.036 (4)0.0253 (5)0.0284 (5)0.0001 (8)0.0020 (8)0.0012 (4)
S10.061 (17)0.030 (2)0.0184 (18)0.005 (3)0.002 (3)0.0022 (15)
N20.0280.0280.0280.0000.0020.001
O30.0250.0430.0270.0000.0000.000
O10.0370.0470.0220.0000.0010.000
C70.0230.0260.0230.0030.0000.000
C40.0250.0420.0380.0000.0000.000
C100.0250.0290.0240.0000.0090.000
N10.0230.0310.0210.0000.0000.001
C120.0390.0250.0290.0000.0000.003
C50.0220.0210.0220.0000.0000.000
O20.0260.0330.0270.0000.0000.009
C60.0140.0220.0200.0040.0000.000
C90.0240.0340.0330.0120.0000.000
C20.0290.0360.0300.0030.0070.003
C80.0160.0320.0240.0000.0000.003
C10.0250.0370.0210.0050.0000.000
C110.0330.0290.0230.0000.0000.003
C30.0220.0340.0450.0000.0060.002
Geometric parameters (Å, º) top
I1—N22.17 (2)C10—C91.378 (17)
I1—N12.25 (2)C10—C111.37 (2)
S1—O11.421 (11)C12—H120.9300
S1—N11.64 (3)C12—C111.38 (3)
S1—C51.77 (2)C5—C61.387 (16)
S1—O21.416 (13)C6—C11.383 (15)
N2—C121.360 (16)C9—H90.9300
N2—C81.38 (2)C9—C81.38 (3)
O3—C71.19 (3)C2—H20.9300
C7—N11.362 (18)C2—C11.393 (17)
C7—C61.51 (4)C2—C31.387 (16)
C4—H40.9300C8—H80.9300
C4—C51.385 (17)C1—H10.9300
C4—C31.378 (15)C11—H110.9300
C10—H100.9300C3—H30.9300
N2—I1—N1172.2 (6)C4—C5—S1127.5 (11)
O1—S1—N1111.7 (12)C4—C5—C6125.3 (17)
O1—S1—C5110.7 (8)C6—C5—S1107.1 (14)
N1—S1—C595.0 (8)C5—C6—C7113.9 (13)
O2—S1—O1115.3 (6)C1—C6—C7128.2 (18)
O2—S1—N1110.6 (9)C1—C6—C5117.9 (19)
O2—S1—C5111.7 (10)C10—C9—H9121.6
C12—N2—I1122.5 (16)C10—C9—C8117 (2)
C12—N2—C8116.4 (19)C8—C9—H9121.6
C8—N2—I1120.8 (10)C1—C2—H2119.5
O3—C7—N1126 (3)C3—C2—H2119.5
O3—C7—C6125.0 (15)C3—C2—C1121.1 (17)
N1—C7—C6109 (2)N2—C8—C9124.3 (16)
C5—C4—H4122.5N2—C8—H8117.8
C3—C4—H4122.5C9—C8—H8117.8
C3—C4—C5115 (2)C6—C1—C2118.6 (18)
C9—C10—H10119.7C6—C1—H1120.7
C11—C10—H10119.7C2—C1—H1120.7
C11—C10—C9121 (2)C10—C11—C12120.0 (16)
S1—N1—I1114.5 (6)C10—C11—H11120.0
C7—N1—I1130 (2)C12—C11—H11120.0
C7—N1—S1115 (2)C4—C3—C2122 (2)
N2—C12—H12119.1C4—C3—H3119.0
N2—C12—C11122 (2)C2—C3—H3119.0
C11—C12—H12119.1
I1—N2—C12—C11170.2 (13)N1—C7—C6—C1178.6 (15)
I1—N2—C8—C9174.1 (13)C12—N2—C8—C90 (2)
S1—C5—C6—C72.6 (17)C5—S1—N1—I1166.9 (7)
S1—C5—C6—C1178.3 (13)C5—S1—N1—C74.6 (13)
N2—C12—C11—C104 (2)C5—C4—C3—C25 (2)
O3—C7—N1—I112 (2)C5—C6—C1—C21 (2)
O3—C7—N1—S1178.0 (15)O2—S1—N1—I177.6 (10)
O3—C7—C6—C5178.8 (16)O2—S1—N1—C7110.9 (12)
O3—C7—C6—C10 (3)O2—S1—C5—C464.4 (17)
O1—S1—N1—I152.3 (8)O2—S1—C5—C6110.5 (12)
O1—S1—N1—C7119.2 (12)C6—C7—N1—I1166.4 (12)
O1—S1—C5—C465.6 (19)C6—C7—N1—S13.6 (19)
O1—S1—C5—C6119.5 (13)C9—C10—C11—C121 (2)
C7—C6—C1—C2179.8 (19)C8—N2—C12—C113 (2)
C4—C5—C6—C7177.7 (18)C1—C2—C3—C43 (3)
C4—C5—C6—C13 (2)C11—C10—C9—C83 (2)
C10—C9—C8—N23 (2)C3—C4—C5—S1179.0 (12)
N1—S1—C5—C4178.9 (16)C3—C4—C5—C65 (2)
N1—S1—C5—C64.0 (11)C3—C2—C1—C61 (3)
N1—C7—C6—C50 (2)
(dac_2.0_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 2.199 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 26.559 (12) ÅCell parameters from 3772 reflections
b = 7.2336 (13) Åθ = 3.2–22.5°
c = 12.209 (2) ŵ = 2.91 mm1
β = 89.462 (9)°T = 296 K
V = 2345.4 (12) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
580 reflections with I > 2σ(I)
φ and ω scansRint = 0.046
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction.
θmax = 23.3°, θmin = 1.8°
Tmin = 0.461, Tmax = 0.563h = 1010
8817 measured reflectionsk = 88
675 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.042H-atom parameters constrained
wR(F2) = 0.107 w = 1/[σ2(Fo2) + (0.0196P)2 + 88.6924P]
where P = (Fo2 + 2Fc2)/3
S = 1.19(Δ/σ)max < 0.001
675 reflectionsΔρmax = 0.70 e Å3
71 parametersΔρmin = 0.41 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.27970 (10)0.39989 (12)0.47694 (7)0.0285 (13)
S10.4009 (4)0.4831 (5)0.4505 (3)0.033 (5)
N20.2172 (9)0.3892 (17)0.5889 (9)0.028
O30.3273 (10)0.3998 (15)0.2000 (8)0.031
O10.3927 (9)0.6392 (14)0.5177 (7)0.036
C70.3585 (15)0.4365 (19)0.2674 (11)0.024
C40.4890 (10)0.601 (2)0.3364 (12)0.037
H40.50700.61900.40050.045*
C100.1366 (10)0.4203 (19)0.7394 (11)0.027
H100.11020.42800.78980.032*
N10.3518 (12)0.4304 (16)0.3783 (9)0.026
C120.2195 (12)0.3244 (19)0.6947 (10)0.029
H120.24850.26200.71560.035*
C50.4397 (10)0.5412 (18)0.3359 (10)0.019
O20.4195 (9)0.3233 (13)0.5048 (7)0.029
C60.4119 (12)0.5057 (19)0.2432 (8)0.017
C90.1306 (12)0.483 (2)0.6325 (11)0.033
H90.10040.53450.60950.039*
C20.4832 (10)0.601 (2)0.1384 (11)0.034
H20.49880.62340.07110.040*
C80.1704 (10)0.467 (2)0.5637 (11)0.021
H80.16650.51270.49300.025*
C10.4343 (10)0.536 (2)0.1427 (10)0.027
H10.41670.51380.07850.032*
C110.1827 (11)0.3454 (18)0.7693 (11)0.025
H110.18800.30990.84150.030*
C30.5090 (13)0.6329 (19)0.2340 (9)0.031
H30.54170.67820.22900.037*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.034 (4)0.0241 (5)0.0273 (5)0.0003 (8)0.0024 (8)0.0015 (4)
S10.051 (18)0.032 (2)0.0174 (18)0.004 (3)0.004 (3)0.0023 (15)
N20.0280.0280.0280.0000.0020.001
O30.0250.0430.0270.0000.0000.000
O10.0370.0480.0220.0000.0010.000
C70.0230.0260.0230.0030.0000.000
C40.0270.0440.0400.0000.0000.000
C100.0260.0300.0240.0000.0090.000
N10.0230.0310.0220.0000.0000.001
C120.0370.0240.0270.0000.0000.003
C50.0190.0190.0190.0000.0000.000
O20.0260.0330.0270.0000.0000.009
C60.0130.0200.0190.0030.0000.000
C90.0260.0360.0360.0130.0000.000
C20.0310.0380.0320.0030.0080.004
C80.0140.0280.0200.0000.0000.003
C10.0240.0360.0200.0050.0000.000
C110.0290.0250.0200.0000.0000.003
C30.0200.0310.0420.0000.0060.002
Geometric parameters (Å, º) top
I1—N22.14 (2)C10—C91.392 (18)
I1—N12.26 (3)C10—C111.39 (2)
S1—O11.411 (11)C12—H120.9300
S1—N11.63 (3)C12—C111.34 (3)
S1—C51.78 (2)C5—C61.381 (16)
S1—O21.422 (13)C6—C11.377 (16)
N2—C121.376 (16)C9—H90.9300
N2—C81.40 (2)C9—C81.35 (3)
O3—C71.20 (3)C2—H20.9300
C7—N11.365 (19)C2—C11.383 (17)
C7—C61.53 (5)C2—C31.378 (16)
C4—H40.9300C8—H80.9300
C4—C51.379 (17)C1—H10.9300
C4—C31.372 (16)C11—H110.9300
C10—H100.9300C3—H30.9300
N2—I1—N1171.9 (7)C4—C5—S1127.8 (11)
O1—S1—N1112.4 (12)C4—C5—C6125.3 (17)
O1—S1—C5110.7 (8)C6—C5—S1106.9 (14)
O1—S1—O2115.6 (6)C5—C6—C7113.9 (14)
N1—S1—C595.2 (9)C1—C6—C7128.1 (18)
O2—S1—N1110.2 (9)C1—C6—C5118 (2)
O2—S1—C5111.0 (10)C10—C9—H9121.3
C12—N2—I1124.7 (17)C8—C9—C10117 (2)
C12—N2—C8113 (2)C8—C9—H9121.3
C8—N2—I1121.9 (10)C1—C2—H2120.1
O3—C7—N1126 (3)C3—C2—H2120.1
O3—C7—C6125.7 (16)C3—C2—C1119.9 (18)
N1—C7—C6108 (2)N2—C8—H8117.0
C5—C4—H4123.0C9—C8—N2126.1 (16)
C3—C4—H4123.0C9—C8—H8117.0
C3—C4—C5114 (2)C6—C1—C2119.1 (19)
C9—C10—H10120.6C6—C1—H1120.5
C11—C10—H10120.6C2—C1—H1120.5
C11—C10—C9119 (2)C10—C11—H11119.8
S1—N1—I1114.4 (6)C12—C11—C10120.3 (17)
C7—N1—I1129 (2)C12—C11—H11119.8
C7—N1—S1116 (2)C4—C3—C2124 (2)
N2—C12—H12118.0C4—C3—H3118.2
C11—C12—N2124 (2)C2—C3—H3118.2
C11—C12—H12118.0
I1—N2—C12—C11168.7 (14)N1—C7—C6—C1178.6 (15)
I1—N2—C8—C9173.1 (14)C12—N2—C8—C91 (2)
S1—C5—C6—C71.7 (18)C5—S1—N1—I1167.2 (7)
S1—C5—C6—C1178.7 (13)C5—S1—N1—C74.1 (13)
N2—C12—C11—C107 (3)C5—C4—C3—C22 (3)
O3—C7—N1—I112 (2)C5—C6—C1—C20 (2)
O3—C7—N1—S1178.7 (15)O2—S1—N1—I178.2 (10)
O3—C7—C6—C5178.7 (17)O2—S1—N1—C7110.6 (13)
O3—C7—C6—C11 (3)O2—S1—C5—C466.2 (18)
O1—S1—N1—I152.3 (8)O2—S1—C5—C6110.8 (13)
O1—S1—N1—C7118.9 (13)C6—C7—N1—I1166.2 (12)
O1—S1—C5—C464 (2)C6—C7—N1—S14 (2)
O1—S1—C5—C6119.5 (14)C9—C10—C11—C124 (2)
C7—C6—C1—C2179 (2)C8—N2—C12—C115 (2)
C4—C5—C6—C7178.8 (19)C1—C2—C3—C41 (3)
C4—C5—C6—C12 (2)C11—C10—C9—C80 (2)
C10—C9—C8—N22 (3)C3—C4—C5—S1179.2 (12)
N1—S1—C5—C4179.9 (17)C3—C4—C5—C63 (3)
N1—S1—C5—C63.2 (11)C3—C2—C1—C60 (3)
N1—C7—C6—C51 (2)
(dac_2.4_d_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 2.232 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 26.482 (12) ÅCell parameters from 3775 reflections
b = 7.1755 (13) Åθ = 3.2–22.9°
c = 12.156 (2) ŵ = 2.96 mm1
β = 89.626 (10)°T = 296 K
V = 2309.9 (12) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
590 reflections with I > 2σ(I)
φ and ω scansRint = 0.046
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction.
θmax = 23.3°, θmin = 1.8°
Tmin = 0.461, Tmax = 0.563h = 1110
8506 measured reflectionsk = 77
673 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.037H-atom parameters constrained
wR(F2) = 0.083 w = 1/[σ2(Fo2) + 65.621P]
where P = (Fo2 + 2Fc2)/3
S = 1.15(Δ/σ)max < 0.001
673 reflectionsΔρmax = 0.34 e Å3
71 parametersΔρmin = 0.33 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.27921 (9)0.40037 (11)0.47668 (7)0.0282 (11)
S10.4006 (3)0.4838 (4)0.4506 (2)0.021 (4)
N20.2154 (9)0.3911 (15)0.5892 (8)0.025
O30.3278 (8)0.3983 (13)0.1977 (7)0.030
O10.3921 (8)0.6432 (11)0.5177 (6)0.033
C70.3590 (13)0.4383 (17)0.2652 (10)0.023
C40.4886 (9)0.600 (2)0.3371 (10)0.031
H40.50620.61670.40230.038*
C100.1351 (9)0.4232 (17)0.7410 (10)0.026
H100.10910.43480.79230.031*
N10.3511 (10)0.4318 (13)0.3771 (8)0.022
C120.2190 (11)0.3263 (16)0.6940 (9)0.025
H120.24850.26610.71470.030*
C50.4390 (9)0.5417 (16)0.3350 (9)0.018
O20.4196 (8)0.3238 (11)0.5060 (6)0.029
C60.4111 (11)0.5048 (17)0.2423 (8)0.016
C90.1292 (10)0.4831 (18)0.6325 (10)0.028
H90.09870.53100.60810.033*
C20.4837 (9)0.599 (2)0.1396 (10)0.030
H20.49940.62100.07220.036*
C80.1696 (9)0.4691 (17)0.5639 (10)0.019
H80.16600.51670.49330.023*
C10.4345 (9)0.5353 (18)0.1418 (10)0.025
H10.41730.51330.07660.030*
C110.1816 (9)0.3453 (16)0.7695 (10)0.024
H110.18680.30590.84140.029*
C30.5101 (12)0.6309 (17)0.2352 (9)0.033
H30.54320.67430.23080.040*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.035 (3)0.0239 (4)0.0254 (4)0.0004 (8)0.0024 (7)0.0018 (4)
S10.015 (15)0.0295 (19)0.0173 (16)0.004 (3)0.003 (3)0.0019 (14)
N20.0260.0250.0250.0000.0010.001
O30.0240.0410.0260.0000.0000.000
O10.0340.0440.0200.0000.0010.000
C70.0220.0250.0220.0030.0000.000
C40.0230.0370.0340.0000.0000.000
C100.0250.0290.0230.0000.0090.000
N10.0200.0270.0190.0000.0000.001
C120.0320.0210.0230.0000.0000.003
C50.0180.0180.0180.0000.0000.000
O20.0270.0340.0270.0000.0000.009
C60.0120.0190.0180.0030.0000.000
C90.0220.0310.0300.0110.0000.000
C20.0280.0340.0290.0020.0070.003
C80.0130.0260.0190.0000.0000.003
C10.0230.0330.0190.0050.0000.000
C110.0280.0240.0190.0000.0000.003
C30.0210.0340.0450.0000.0060.002
Geometric parameters (Å, º) top
I1—N22.168 (19)C10—C91.397 (16)
I1—N12.26 (2)C10—C111.40 (2)
S1—O11.422 (9)C12—H120.9300
S1—N11.63 (2)C12—C111.35 (3)
S1—C51.778 (18)C5—C61.378 (15)
S1—O21.424 (12)C6—C11.382 (15)
N2—C121.360 (14)C9—H90.9300
N2—C81.37 (2)C9—C81.36 (3)
O3—C71.20 (3)C2—H20.9300
C7—N11.375 (17)C2—C11.382 (17)
C7—C61.49 (4)C2—C31.379 (16)
C4—H40.9300C8—H80.9300
C4—C51.378 (16)C1—H10.9300
C4—C31.379 (15)C11—H110.9300
C10—H100.9300C3—H30.9300
N2—I1—N1172.3 (6)C4—C5—S1126.6 (10)
O1—S1—N1111.8 (10)C4—C5—C6126.1 (15)
O1—S1—C5110.7 (7)C6—C5—S1107.2 (13)
O1—S1—O2115.6 (5)C5—C6—C7114.2 (12)
N1—S1—C594.5 (8)C5—C6—C1117.0 (18)
O2—S1—N1111.2 (8)C1—C6—C7128.8 (17)
O2—S1—C5111.2 (9)C10—C9—H9121.1
C12—N2—I1122.9 (15)C8—C9—C10117.7 (19)
C12—N2—C8114.5 (18)C8—C9—H9121.1
C8—N2—I1122.2 (9)C1—C2—H2119.2
O3—C7—N1124 (3)C3—C2—H2119.2
O3—C7—C6126.1 (14)C3—C2—C1121.5 (16)
N1—C7—C6109 (2)N2—C8—H8117.0
C5—C4—H4122.5C9—C8—N2126.0 (15)
C5—C4—C3114.9 (18)C9—C8—H8117.0
C3—C4—H4122.5C6—C1—H1120.5
C9—C10—H10121.3C2—C1—C6119.0 (17)
C11—C10—H10121.3C2—C1—H1120.5
C11—C10—C9117.5 (19)C10—C11—H11119.6
S1—N1—I1113.9 (5)C12—C11—C10120.9 (15)
C7—N1—I1131 (2)C12—C11—H11119.6
C7—N1—S1115 (2)C4—C3—C2121 (2)
N2—C12—H12118.4C4—C3—H3119.3
C11—C12—N2123.1 (19)C2—C3—H3119.3
C11—C12—H12118.4
I1—N2—C12—C11169.9 (12)N1—C7—C6—C1178.6 (14)
I1—N2—C8—C9174.2 (12)C12—N2—C8—C91 (2)
S1—C5—C6—C72.3 (16)C5—S1—N1—I1167.6 (6)
S1—C5—C6—C1178.3 (11)C5—S1—N1—C74.5 (12)
N2—C12—C11—C104 (2)C5—C4—C3—C22 (2)
O3—C7—N1—I112 (2)C5—C6—C1—C20 (2)
O3—C7—N1—S1177.2 (14)O2—S1—N1—I177.7 (9)
O3—C7—C6—C5179.7 (15)O2—S1—N1—C7110.2 (11)
O3—C7—C6—C10 (3)O2—S1—C5—C464.8 (15)
O1—S1—N1—I153.2 (7)O2—S1—C5—C6110.9 (11)
O1—S1—N1—C7118.9 (11)C6—C7—N1—I1166.7 (11)
O1—S1—C5—C465.1 (17)C6—C7—N1—S13.7 (18)
O1—S1—C5—C6119.2 (12)C9—C10—C11—C121 (2)
C7—C6—C1—C2179.7 (18)C8—N2—C12—C113 (2)
C4—C5—C6—C7178.1 (17)C1—C2—C3—C40 (2)
C4—C5—C6—C12 (2)C11—C10—C9—C83 (2)
C10—C9—C8—N24 (2)C3—C4—C5—S1178.3 (10)
N1—S1—C5—C4179.6 (14)C3—C4—C5—C63 (2)
N1—S1—C5—C63.8 (10)C3—C2—C1—C61 (2)
N1—C7—C6—C51 (2)
(dac_3.3_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 2.309 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 26.304 (11) ÅCell parameters from 4330 reflections
b = 7.0512 (11) Åθ = 3.3–24.5°
c = 12.042 (2) ŵ = 3.06 mm1
β = 89.932 (9)°T = 296 K
V = 2233.5 (11) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
590 reflections with I > 2σ(I)
φ and ω scansRint = 0.040
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction.
θmax = 23.2°, θmin = 1.9°
Tmin = 0.461, Tmax = 0.563h = 1110
8569 measured reflectionsk = 77
656 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.020H-atom parameters constrained
wR(F2) = 0.038 w = 1/[σ2(Fo2) + (0.0102P)2 + 7.7918P]
where P = (Fo2 + 2Fc2)/3
S = 1.12(Δ/σ)max < 0.001
656 reflectionsΔρmax = 0.22 e Å3
71 parametersΔρmin = 0.22 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.27803 (5)0.40216 (5)0.47608 (3)0.0270 (5)
S10.39946 (15)0.4869 (2)0.45071 (12)0.025 (2)
N20.2121 (5)0.3927 (7)0.5911 (4)0.021
O30.3274 (4)0.3953 (6)0.1941 (3)0.026
O10.3908 (4)0.6506 (5)0.5176 (3)0.029
C70.3589 (7)0.4402 (8)0.2627 (5)0.020
C40.4879 (5)0.6001 (10)0.3392 (5)0.025
H40.50510.61850.40590.030*
C100.1345 (5)0.4229 (8)0.7438 (5)0.024
H100.10840.43340.79560.029*
N10.3498 (5)0.4324 (7)0.3763 (4)0.020
C120.2207 (5)0.3271 (8)0.6956 (4)0.029
H120.25180.27430.71540.035*
C50.4381 (5)0.5402 (8)0.3377 (5)0.019
O20.4175 (4)0.3249 (5)0.5097 (3)0.026
C60.4113 (6)0.5038 (9)0.2408 (4)0.017
C90.1282 (5)0.4872 (8)0.6358 (4)0.024
H90.09750.54010.61310.028*
C20.4858 (5)0.5974 (10)0.1400 (5)0.027
H20.50240.61590.07260.032*
C80.1681 (5)0.4712 (9)0.5631 (5)0.019
H80.16410.51720.49130.023*
C10.4358 (5)0.5357 (9)0.1405 (5)0.022
H10.41880.51580.07390.027*
C110.1810 (5)0.3424 (8)0.7721 (5)0.022
H110.18570.29740.84390.027*
C30.5117 (6)0.6320 (8)0.2384 (5)0.030
H30.54500.67660.23660.036*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.0364 (16)0.0241 (2)0.0206 (2)0.0014 (4)0.0023 (4)0.00113 (19)
S10.032 (7)0.0262 (9)0.0170 (8)0.0010 (14)0.0020 (14)0.0005 (7)
N20.0220.0210.0210.0000.0010.001
O30.0200.0350.0220.0000.0000.000
O10.0300.0390.0180.0000.0010.000
C70.0190.0220.0190.0030.0000.000
C40.0180.0290.0270.0000.0000.000
C100.0230.0270.0220.0000.0080.000
N10.0180.0240.0170.0000.0000.001
C120.0360.0240.0270.0000.0000.003
C50.0200.0190.0190.0000.0000.000
O20.0240.0300.0240.0000.0000.008
C60.0130.0200.0190.0030.0000.000
C90.0190.0260.0260.0100.0000.000
C20.0250.0300.0250.0020.0060.003
C80.0130.0260.0190.0000.0000.003
C10.0200.0300.0170.0040.0000.000
C110.0260.0230.0180.0000.0000.003
C30.0190.0300.0400.0000.0060.002
Geometric parameters (Å, º) top
I1—N22.218 (9)C10—C91.387 (8)
I1—N12.248 (11)C10—C111.391 (14)
S1—O11.425 (4)C12—H120.9300
S1—N11.630 (12)C12—C111.397 (14)
S1—C51.739 (9)C5—C61.388 (10)
S1—O21.427 (5)C6—C11.387 (10)
N2—C121.360 (7)C9—H90.9300
N2—C81.329 (13)C9—C81.369 (13)
O3—C71.213 (15)C2—H20.9300
C7—N11.389 (8)C2—C11.386 (13)
C7—C61.47 (2)C2—C31.389 (11)
C4—H40.9300C8—H80.9300
C4—C51.378 (12)C1—H10.9300
C4—C31.383 (9)C11—H110.9300
C10—H100.9300C3—H30.9300
N2—I1—N1172.8 (3)C4—C5—S1127.7 (6)
O1—S1—N1112.0 (5)C4—C5—C6123.6 (8)
O1—S1—C5111.1 (3)C6—C5—S1108.7 (8)
O1—S1—O2114.9 (2)C5—C6—C7112.5 (7)
N1—S1—C595.0 (4)C1—C6—C7129.8 (9)
O2—S1—N1110.6 (4)C1—C6—C5117.7 (10)
O2—S1—C5111.6 (5)C10—C9—H9120.7
C12—N2—I1117.2 (8)C8—C9—C10118.7 (10)
C8—N2—I1120.7 (5)C8—C9—H9120.7
C8—N2—C12121.5 (9)C1—C2—H2119.4
O3—C7—N1123.0 (13)C1—C2—C3121.2 (8)
O3—C7—C6126.6 (7)C3—C2—H2119.4
N1—C7—C6110.3 (11)N2—C8—C9122.7 (7)
C5—C4—H4121.1N2—C8—H8118.7
C5—C4—C3117.9 (9)C9—C8—H8118.7
C3—C4—H4121.1C6—C1—H1120.1
C9—C10—H10121.0C2—C1—C6119.7 (9)
C9—C10—C11117.9 (9)C2—C1—H1120.1
C11—C10—H10121.0C10—C11—C12121.9 (7)
S1—N1—I1113.7 (3)C10—C11—H11119.1
C7—N1—I1132.3 (11)C12—C11—H11119.1
C7—N1—S1113.3 (11)C4—C3—C2119.9 (11)
N2—C12—H12121.4C4—C3—H3120.0
N2—C12—C11117.3 (10)C2—C3—H3120.0
C11—C12—H12121.4
I1—N2—C12—C11172.5 (5)N1—C7—C6—C1178.3 (7)
I1—N2—C8—C9172.7 (6)C12—N2—C8—C91.7 (12)
S1—C5—C6—C72.3 (8)C5—S1—N1—I1168.4 (3)
S1—C5—C6—C1179.4 (6)C5—S1—N1—C73.0 (6)
N2—C12—C11—C100.7 (11)C5—C4—C3—C22.2 (11)
O3—C7—N1—I114.4 (11)C5—C6—C1—C21.5 (11)
O3—C7—N1—S1176.2 (7)O2—S1—N1—I176.3 (4)
O3—C7—C6—C5178.5 (7)O2—S1—N1—C7112.3 (5)
O3—C7—C6—C13.4 (16)O2—S1—C5—C465.6 (8)
O1—S1—N1—I153.2 (3)O2—S1—C5—C6111.5 (6)
O1—S1—N1—C7118.2 (5)C6—C7—N1—I1167.2 (6)
O1—S1—C5—C464.0 (9)C6—C7—N1—S12.1 (9)
O1—S1—C5—C6118.9 (6)C9—C10—C11—C120.6 (11)
C7—C6—C1—C2179.5 (9)C8—N2—C12—C111.2 (11)
C4—C5—C6—C7179.5 (8)C1—C2—C3—C41.7 (11)
C4—C5—C6—C12.1 (12)C11—C10—C9—C81.0 (11)
C10—C9—C8—N21.6 (12)C3—C4—C5—S1179.1 (5)
N1—S1—C5—C4179.8 (8)C3—C4—C5—C62.4 (12)
N1—S1—C5—C63.1 (5)C3—C2—C1—C61.4 (12)
N1—C7—C6—C50.2 (10)
(dac_4.5_GPa) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 2.385 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 26.020 (12) ÅCell parameters from 3659 reflections
b = 6.9618 (13) Åθ = 3.3–23.1°
c = 11.937 (2) ŵ = 3.16 mm1
β = 89.476 (10)°T = 296 K
V = 2162.3 (11) Å3Plate, colourless
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
553 reflections with I > 2σ(I)
φ and ω scansRint = 0.046
Absorption correction: empirical (using intensity measurements)
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction. wR2(int) was 0.0628 before and 0.0535 after correction. The Ratio of minimum to maximum transmission is 0.8928. The λ/2 correction factor is Not present.
θmax = 23.4°, θmin = 1.9°
Tmin = 0.502, Tmax = 0.563h = 1111
7793 measured reflectionsk = 77
635 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.029H-atom parameters constrained
wR(F2) = 0.049 w = 1/[σ2(Fo2) + 18.6464P]
where P = (Fo2 + 2Fc2)/3
S = 1.19(Δ/σ)max < 0.001
635 reflectionsΔρmax = 0.29 e Å3
71 parametersΔρmin = 0.31 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.27674 (7)0.40504 (7)0.47602 (5)0.0274 (7)
S10.3978 (2)0.4904 (3)0.45065 (17)0.025 (3)
N20.2126 (6)0.3969 (11)0.5922 (5)0.022
O30.3261 (5)0.3908 (9)0.1901 (4)0.025
O10.3892 (5)0.6572 (8)0.5165 (4)0.029
C70.3587 (9)0.4404 (12)0.2607 (7)0.022
C40.4880 (7)0.6036 (15)0.3427 (7)0.027
H40.50420.62380.41080.032*
C100.1339 (7)0.4246 (12)0.7459 (7)0.020
H100.10740.43450.79850.024*
N10.3494 (7)0.4354 (10)0.3742 (5)0.019
C120.2192 (7)0.3274 (11)0.6981 (6)0.027
H120.25020.27050.71810.033*
C50.4380 (7)0.5425 (12)0.3369 (6)0.019
O20.4163 (5)0.3261 (7)0.5120 (4)0.025
C60.4116 (8)0.5040 (13)0.2394 (6)0.016
C90.1269 (7)0.4926 (13)0.6390 (7)0.026
H90.09590.54650.61700.032*
C20.4880 (7)0.5973 (14)0.1415 (7)0.023
H20.50580.61540.07430.028*
C80.1674 (7)0.4773 (12)0.5666 (7)0.019
H80.16350.52600.49470.022*
C10.4375 (6)0.5345 (13)0.1392 (7)0.024
H10.42120.51320.07130.028*
C110.1795 (7)0.3426 (12)0.7751 (7)0.023
H110.18380.29650.84750.027*
C30.5127 (8)0.6335 (12)0.2413 (6)0.030
H30.54640.67860.24020.036*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.039 (2)0.0234 (3)0.0197 (3)0.0007 (6)0.0044 (5)0.0011 (3)
S10.034 (10)0.0236 (13)0.0171 (11)0.001 (2)0.0051 (19)0.0010 (10)
N20.0220.0220.0220.0000.0010.001
O30.0200.0340.0210.0000.0000.000
O10.0300.0390.0180.0000.0010.000
C70.0210.0230.0210.0030.0000.000
C40.0200.0320.0290.0000.0000.000
C100.0190.0220.0180.0000.0070.000
N10.0170.0230.0160.0000.0000.001
C120.0340.0220.0250.0000.0000.003
C50.0190.0190.0190.0000.0000.000
O20.0230.0290.0240.0000.0000.008
C60.0120.0190.0180.0030.0000.000
C90.0210.0290.0290.0110.0000.000
C20.0210.0260.0220.0020.0050.002
C80.0130.0250.0190.0000.0000.003
C10.0210.0320.0180.0050.0000.000
C110.0270.0230.0180.0000.0000.003
C30.0190.0300.0400.0000.0060.002
Geometric parameters (Å, º) top
I1—N22.162 (13)C10—C91.375 (11)
I1—N12.249 (16)C10—C111.366 (17)
S1—O11.419 (6)C12—H120.9300
S1—N11.606 (16)C12—C111.382 (18)
S1—C51.746 (13)C5—C61.382 (12)
S1—O21.444 (8)C6—C11.384 (12)
N2—C121.366 (9)C9—H90.9300
N2—C81.338 (16)C9—C81.361 (18)
O3—C71.25 (2)C2—H20.9300
C7—N11.375 (12)C2—C11.387 (14)
C7—C61.47 (3)C2—C31.381 (13)
C4—H40.9300C8—H80.9300
C4—C51.370 (14)C1—H10.9300
C4—C31.382 (11)C11—H110.9300
C10—H100.9300C3—H30.9300
N2—I1—N1172.0 (4)C4—C5—S1126.0 (7)
O1—S1—N1112.9 (7)C4—C5—C6125.6 (11)
O1—S1—C5110.6 (5)C6—C5—S1108.3 (10)
O1—S1—O2114.8 (3)C5—C6—C7112.7 (9)
N1—S1—C594.3 (6)C5—C6—C1117.1 (14)
O2—S1—N1111.5 (5)C1—C6—C7130.1 (13)
O2—S1—C5111.0 (7)C10—C9—H9121.5
C12—N2—I1119.9 (11)C8—C9—C10117.0 (13)
C8—N2—I1121.1 (6)C8—C9—H9121.5
C8—N2—C12118.6 (12)C1—C2—H2119.2
O3—C7—N1122.9 (19)C3—C2—H2119.2
O3—C7—C6127.6 (9)C3—C2—C1121.5 (11)
N1—C7—C6109.5 (15)N2—C8—C9124.4 (10)
C5—C4—H4122.1N2—C8—H8117.8
C5—C4—C3115.9 (13)C9—C8—H8117.8
C3—C4—H4122.1C6—C1—C2119.0 (12)
C9—C10—H10119.9C6—C1—H1120.5
C11—C10—H10119.9C2—C1—H1120.5
C11—C10—C9120.2 (13)C10—C11—C12120.6 (10)
S1—N1—I1112.0 (4)C10—C11—H11119.7
C7—N1—I1132.4 (15)C12—C11—H11119.7
C7—N1—S1115.0 (15)C4—C3—H3119.6
N2—C12—H12120.4C2—C3—C4120.8 (14)
N2—C12—C11119.2 (13)C2—C3—H3119.6
C11—C12—H12120.4
I1—N2—C12—C11172.9 (7)N1—C7—C6—C1178.4 (10)
I1—N2—C8—C9174.0 (8)C12—N2—C8—C91.0 (17)
S1—C5—C6—C72.2 (12)C5—S1—N1—I1169.0 (4)
S1—C5—C6—C1179.3 (8)C5—S1—N1—C73.1 (8)
N2—C12—C11—C100.5 (15)C5—C4—C3—C21.8 (15)
O3—C7—N1—I114.2 (15)C5—C6—C1—C21.3 (15)
O3—C7—N1—S1175.8 (9)O2—S1—N1—I176.4 (6)
O3—C7—C6—C5178.1 (10)O2—S1—N1—C7111.5 (8)
O3—C7—C6—C14 (2)O2—S1—C5—C465.6 (11)
O1—S1—N1—I154.5 (5)O2—S1—C5—C6112.0 (8)
O1—S1—N1—C7117.6 (8)C6—C7—N1—I1167.8 (8)
O1—S1—C5—C463.0 (12)C6—C7—N1—S12.2 (13)
O1—S1—C5—C6119.5 (8)C9—C10—C11—C120.2 (16)
C7—C6—C1—C2179.4 (13)C8—N2—C12—C110.1 (15)
C4—C5—C6—C7179.8 (12)C1—C2—C3—C41.6 (16)
C4—C5—C6—C11.7 (17)C11—C10—C9—C81.3 (16)
C10—C9—C8—N21.8 (17)C3—C4—C5—S1179.1 (7)
N1—S1—C5—C4179.4 (11)C3—C4—C5—C61.9 (17)
N1—S1—C5—C63.0 (8)C3—C2—C1—C61.3 (17)
N1—C7—C6—C50.2 (15)
(NISac_Py_crystal_2_RTP) top
Crystal data top
C12H9IN2O3SF(000) = 1504
Mr = 388.17Dx = 1.918 Mg m3
Monoclinic, ¯B2ybcMo Kα radiation, λ = 0.71073 Å
a = 27.272 (5) ÅCell parameters from 9316 reflections
b = 7.8156 (9) Åθ = 3.0–25.7°
c = 12.6155 (16) ŵ = 2.54 mm1
β = 88.703 (3)°T = 296 K
V = 2688.3 (7) Å3Plate, orange
Z = 80.11 × 0.09 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
2670 reflections with I > 2σ(I)
φ and ω scansRint = 0.049
Absorption correction: numerical
SADABS-2016/2 (Bruker,2016/2) was used for absorption correction. wR2(int) was 0.0713 before and 0.0583 after correction. The Ratio of minimum to maximum transmission is 0.8904. The λ/2 correction factor is Not present.
θmax = 26.4°, θmin = 1.8°
Tmin = 0.566, Tmax = 0.636h = 3434
67239 measured reflectionsk = 99
2738 independent reflectionsl = 1515
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.063H-atom parameters constrained
wR(F2) = 0.155 w = 1/[σ2(Fo2) + (0.0572P)2 + 59.271P]
where P = (Fo2 + 2Fc2)/3
S = 1.16(Δ/σ)max = 0.001
2738 reflectionsΔρmax = 2.49 e Å3
173 parametersΔρmin = 1.41 e Å3
18 restraints
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.

Refinement. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.28456 (2)0.39789 (7)0.47960 (4)0.0384 (2)
S10.40403 (8)0.4726 (3)0.44963 (16)0.0397 (5)
N20.2160 (3)0.3816 (9)0.5873 (6)0.0422 (17)
O30.3281 (2)0.4086 (10)0.2149 (5)0.0548 (18)
O10.3959 (3)0.6143 (11)0.5179 (6)0.064 (2)
C70.3601 (3)0.4393 (12)0.2768 (7)0.0384 (18)
C40.4855 (3)0.5933 (13)0.3284 (7)0.050 (2)
H40.50390.61120.38860.060*
C100.1392 (4)0.4133 (13)0.7307 (7)0.054 (2)
H100.11320.42390.77930.064*
N10.3549 (3)0.4259 (10)0.3854 (6)0.0421 (17)
C120.2198 (4)0.3229 (13)0.6860 (7)0.051 (2)
H120.24880.26950.70540.061*
C50.4383 (3)0.5312 (11)0.3358 (6)0.0337 (16)
O20.4245 (3)0.3237 (10)0.4954 (6)0.0580 (18)
C60.4104 (3)0.5007 (11)0.2480 (6)0.0344 (17)
C90.1347 (3)0.4722 (14)0.6283 (8)0.051 (2)
H90.10560.52150.60650.062*
C20.4769 (3)0.5993 (14)0.1392 (8)0.056 (3)
H20.49020.62340.07230.067*
C80.1742 (3)0.4566 (12)0.5592 (6)0.0375 (18)
H80.17170.49960.49080.045*
C10.4300 (3)0.5352 (14)0.1490 (7)0.050 (2)
H10.41170.51540.08890.060*
C110.1822 (4)0.3391 (13)0.7598 (8)0.049 (2)
H110.18600.30000.82880.059*
C30.5045 (4)0.6281 (14)0.2284 (7)0.054 (3)
H30.53610.67140.22070.065*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.0310 (3)0.0415 (3)0.0427 (3)0.0016 (2)0.0008 (2)0.0009 (2)
S10.0350 (10)0.0547 (13)0.0296 (9)0.0075 (9)0.0075 (8)0.0025 (9)
N20.044 (4)0.039 (4)0.043 (4)0.004 (3)0.001 (3)0.006 (3)
O30.043 (4)0.077 (5)0.045 (4)0.014 (3)0.012 (3)0.007 (3)
O10.066 (5)0.085 (6)0.042 (4)0.016 (4)0.001 (3)0.019 (4)
C70.035 (4)0.044 (5)0.036 (4)0.003 (4)0.005 (3)0.001 (4)
C40.039 (5)0.057 (6)0.053 (5)0.012 (4)0.008 (4)0.001 (5)
C100.052 (6)0.060 (6)0.047 (5)0.001 (5)0.020 (4)0.005 (5)
N10.037 (4)0.053 (5)0.037 (4)0.005 (3)0.003 (3)0.001 (3)
C120.057 (6)0.044 (5)0.051 (5)0.004 (5)0.007 (4)0.007 (4)
C50.033 (4)0.035 (4)0.034 (4)0.003 (3)0.002 (3)0.000 (3)
O20.053 (4)0.069 (5)0.052 (4)0.005 (4)0.013 (3)0.018 (4)
C60.028 (4)0.037 (4)0.038 (4)0.005 (3)0.003 (3)0.002 (3)
C90.036 (5)0.058 (6)0.060 (6)0.018 (4)0.002 (4)0.003 (5)
C20.054 (6)0.064 (7)0.049 (5)0.002 (5)0.015 (5)0.009 (5)
C80.033 (4)0.048 (5)0.032 (4)0.001 (4)0.001 (3)0.003 (4)
C10.047 (5)0.067 (6)0.036 (4)0.006 (5)0.005 (4)0.000 (4)
C110.057 (6)0.049 (5)0.042 (5)0.010 (5)0.001 (4)0.006 (4)
C30.038 (5)0.054 (6)0.071 (7)0.008 (4)0.010 (5)0.003 (5)
Geometric parameters (Å, º) top
I1—N22.291 (8)C10—C91.379 (12)
I1—N12.245 (7)C10—C111.367 (12)
S1—O11.417 (8)C12—H120.9300
S1—N11.623 (7)C12—C111.376 (12)
S1—C51.757 (8)C5—C61.378 (9)
S1—O21.419 (8)C6—C11.374 (9)
N2—C121.333 (10)C9—H90.9300
N2—C81.337 (10)C9—C81.376 (11)
O3—C71.208 (10)C2—H20.9300
C7—N11.378 (11)C2—C11.375 (10)
C7—C61.490 (11)C2—C31.386 (11)
C4—H40.9300C8—H80.9300
C4—C51.378 (9)C1—H10.9300
C4—C31.380 (10)C11—H110.9300
C10—H100.9300C3—H30.9300
N1—I1—N2175.1 (3)C4—C5—S1128.8 (6)
O1—S1—N1111.1 (5)C4—C5—C6122.6 (7)
O1—S1—C5111.5 (4)C6—C5—S1108.6 (5)
O1—S1—O2116.8 (5)C5—C6—C7112.4 (7)
N1—S1—C594.6 (4)C1—C6—C7128.5 (7)
O2—S1—N1110.8 (4)C1—C6—C5119.1 (7)
O2—S1—C5109.8 (4)C10—C9—H9120.7
C12—N2—I1119.5 (6)C8—C9—C10118.7 (8)
C12—N2—C8119.0 (8)C8—C9—H9120.7
C8—N2—I1120.5 (5)C1—C2—H2119.8
O3—C7—N1124.6 (8)C1—C2—C3120.4 (8)
O3—C7—C6125.5 (8)C3—C2—H2119.8
N1—C7—C6109.9 (7)N2—C8—C9122.0 (8)
C5—C4—H4121.3N2—C8—H8119.0
C5—C4—C3117.4 (8)C9—C8—H8119.0
C3—C4—H4121.3C6—C1—C2119.7 (8)
C9—C10—H10120.4C6—C1—H1120.2
C11—C10—H10120.4C2—C1—H1120.2
C11—C10—C9119.2 (9)C10—C11—C12119.2 (9)
S1—N1—I1117.6 (4)C10—C11—H11120.4
C7—N1—I1127.0 (6)C12—C11—H11120.4
C7—N1—S1114.3 (6)C4—C3—C2120.8 (8)
N2—C12—H12119.1C4—C3—H3119.6
N2—C12—C11121.8 (9)C2—C3—H3119.6
C11—C12—H12119.1
I1—N2—C12—C11167.9 (7)N1—C7—C6—C1178.1 (9)
I1—N2—C8—C9169.8 (8)C12—N2—C8—C91.3 (14)
S1—C5—C6—C73.4 (9)C5—S1—N1—I1165.1 (5)
S1—C5—C6—C1179.2 (7)C5—S1—N1—C73.5 (7)
N2—C12—C11—C101.8 (16)C5—C4—C3—C20.7 (16)
O3—C7—N1—I113.4 (14)C5—C6—C1—C20.0 (15)
O3—C7—N1—S1179.3 (8)O2—S1—N1—I181.6 (6)
O3—C7—C6—C5177.6 (9)O2—S1—N1—C7109.7 (7)
O3—C7—C6—C10.6 (16)O2—S1—C5—C468.2 (10)
O1—S1—N1—I149.9 (6)O2—S1—C5—C6110.1 (7)
O1—S1—N1—C7118.7 (7)C6—C7—N1—I1165.3 (6)
O1—S1—C5—C462.9 (10)C6—C7—N1—S12.0 (10)
O1—S1—C5—C6118.8 (7)C9—C10—C11—C120.9 (16)
C7—C6—C1—C2176.9 (9)C8—N2—C12—C110.7 (14)
C4—C5—C6—C7178.1 (9)C1—C2—C3—C40.0 (17)
C4—C5—C6—C10.8 (14)C11—C10—C9—C81.0 (16)
C10—C9—C8—N22.1 (16)C3—C4—C5—S1179.3 (8)
N1—S1—C5—C4177.7 (9)C3—C4—C5—C61.1 (15)
N1—S1—C5—C64.0 (7)C3—C2—C1—C60.4 (17)
N1—C7—C6—C51.1 (10)
 

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