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In a study to evaluate the impact of flexible positional isomeric ligands on the coordination geometry and self-assembly process of 3d metal complexes, the synthesis of eight new cobalt(II) complexes with the 2-phenyl­imidazole (LH) and 5-phenyl­imidazole (L′H) ligands has been carried out. A variety of parameters/conditions have been probed using the general CoII/X/LH or L′H (X = Cl, Br, I, NO3, NCS, ClO4, SO42−) reaction system. Interestingly, X-ray analyses reveal two distinct groups of complexes: reactions with LH only lead to tetrahedral or quasi-tetrahedral complexes {i.e. [CoCl2(LH)2] (1), [CoI2(LH)2] (2), [Co(NO3)2(LH)2] (3), [Co(NCS)2(LH)2] (4)}, whereas L′H favours octahedral coordination {i.e. [Co(L′H)4(MeCN)(H2O)]I2 (5), [Co(L′H)4(MeCN)(H2O)](NO3)2 (6) and [Co(NCS)2(L′H)4)]·2MeOH (7·2MeOH)}. A tetrahedral [Co(NCS)2(L′H)2)] (8) complex was also concurrently isolated with complex 7. The effects of the positional isomeric ligands LH and L′H and of the coordinated inorganic anions on the stoichiometry and packing arrangements of the complexes are thoroughly discussed. The supramolecular assembly is firmly directed, in all types of complexes, by robust N—H...X (X = Cl, I, O or S) motifs, leading to varying dimensionalities (1D, 2D or 3D) and packing arrangements. The formation of these motifs has been activated by choosing appropriate anions X, acting as terminal ligands or counterions. At a second level of organization, additional subordinate C—H...X (X = Cl, I, O or S), C—H...π and π...π intermolecular interactions complement the rigidity of the complexes' packing towards compact 3D assemblies. Hirshfeld surface analyses provided insight into the intermolecular interactions, allowed quantification of the individual contact types and comparison between the complexes.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S205252061900636X/aw5026sup1.cif
Contains datablocks global, 1, 2, 3, 4, 5, 6, 7, 8

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S205252061900636X/aw5026sup10.pdf
Supplementary material

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205252061900636X/aw50261sup2.hkl
Contains datablock 1

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205252061900636X/aw50262sup3.hkl
Contains datablock 2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205252061900636X/aw50263sup4.hkl
Contains datablock 3

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205252061900636X/aw50264sup5.hkl
Contains datablock 4

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205252061900636X/aw50265sup6.hkl
Contains datablock 5

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205252061900636X/aw50266sup7.hkl
Contains datablock 6

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205252061900636X/aw50267sup8.hkl
Contains datablock 7

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205252061900636X/aw50268sup9.hkl
Contains datablock 8

CCDC references: 1914027; 1914028; 1914029; 1914030; 1914031; 1914032; 1914033; 1914034

Computing details top

For all structures, data collection: CrysAlis PRO 1.171.38.43 (Rigaku OD, 2015); cell refinement: CrysAlis PRO 1.171.38.43 (Rigaku OD, 2015); data reduction: CrysAlis PRO 1.171.38.43 (Rigaku OD, 2015); program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXL2014/7 (Sheldrick, 2014); molecular graphics: PLATON (Spek, 2011); Mercury (Bruno et al. 2002); DIAMOND (Brandenburg, 2014); X-SEED (Barbour, 2001); software used to prepare material for publication: WinGX (Farrugia, 2012).

(1) top
Crystal data top
C18H16Cl2CoN4Dx = 1.551 Mg m3
Mr = 418.18Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pca21Cell parameters from 6008 reflections
a = 14.8764 (9) Åθ = 3.0–29.0°
b = 8.9742 (4) ŵ = 1.26 mm1
c = 26.8271 (9) ÅT = 100 K
V = 3581.5 (3) Å3Prism, blue
Z = 80.32 × 0.15 × 0.15 mm
F(000) = 1704
Data collection top
Oxford Diffraction SuperNova with Atlas CCD detector
diffractometer
6080 independent reflections
Radiation source: SuperNova (Mo) X-ray Source5795 reflections with I > 2σ(I)
Detector resolution: 10.4223 pixels mm-1Rint = 0.030
ω scansθmax = 27.0°, θmin = 3.0°
Absorption correction: multi-scan
CrysAlisPro 1.171.38.43 (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 1219
Tmin = 0.667, Tmax = 1.000k = 911
11547 measured reflectionsl = 3134
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.027H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.068 w = 1/[σ2(Fo2) + (0.0333P)2 + 0.5291P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max < 0.001
6080 reflectionsΔρmax = 0.41 e Å3
464 parametersΔρmin = 0.28 e Å3
5 restraintsAbsolute structure: Refined as an inversion twin.
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.495 (15)
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 inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C2A0.4731 (3)0.4790 (4)0.68182 (15)0.0143 (8)
C2B0.3825 (2)0.2020 (4)0.55021 (14)0.0146 (7)
C2C0.6418 (3)0.2780 (4)0.46363 (14)0.0159 (8)
C2D0.7237 (3)0.0203 (4)0.33211 (15)0.0150 (8)
C4A0.3852 (3)0.6551 (4)0.65507 (14)0.0173 (8)
H4A0.33480.70520.64320.021*
C4B0.3486 (3)0.0478 (4)0.60959 (13)0.0174 (8)
H4B0.33140.01030.64050.021*
C4C0.6262 (3)0.4257 (4)0.40016 (14)0.0181 (8)
H4C0.61280.46070.36840.022*
C4D0.6410 (3)0.1637 (4)0.35724 (15)0.0190 (8)
H4D0.59210.21870.36870.023*
C5A0.4648 (3)0.7178 (4)0.66531 (15)0.0218 (8)
H5A0.48010.81770.66160.026*
C5B0.3706 (3)0.0347 (4)0.56942 (14)0.0183 (8)
H5B0.37140.13810.56740.022*
C5C0.6597 (3)0.5074 (4)0.43737 (14)0.0207 (8)
H5C0.67390.60830.43630.025*
C5D0.7228 (3)0.2188 (4)0.34705 (15)0.0215 (9)
H5D0.74100.31750.35010.026*
C6A0.5075 (3)0.3337 (4)0.69759 (13)0.0138 (7)
C6B0.3999 (3)0.3350 (4)0.52053 (14)0.0178 (8)
C6C0.6414 (3)0.1499 (4)0.49703 (14)0.0159 (8)
C6D0.7552 (3)0.1684 (4)0.31749 (13)0.0154 (7)
C7A0.4515 (3)0.2365 (4)0.72295 (15)0.0176 (8)
H7A0.39280.26420.73050.021*
C7B0.4404 (3)0.4582 (4)0.54174 (16)0.0230 (9)
H7B0.45690.45640.57520.028*
C7C0.6708 (3)0.0114 (4)0.48021 (16)0.0222 (9)
H7C0.69290.00090.44800.027*
C7D0.6998 (3)0.2604 (4)0.28959 (14)0.0175 (8)
H7D0.64280.22810.28020.021*
C8A0.4831 (3)0.0989 (4)0.73688 (13)0.0188 (8)
H8A0.44560.03270.75360.023*
C8B0.4562 (3)0.5834 (4)0.51360 (17)0.0291 (10)
H8B0.48310.66630.52810.035*
C8C0.6672 (3)0.1097 (4)0.51159 (16)0.0255 (9)
H8C0.68650.20230.50040.031*
C8D0.7296 (3)0.4011 (4)0.27574 (14)0.0191 (8)
H8D0.69240.46350.25730.023*
C9A0.5704 (3)0.0588 (4)0.72612 (14)0.0210 (8)
H9A0.59140.03490.73520.025*
C9B0.4321 (3)0.5869 (5)0.46344 (16)0.0318 (11)
H9B0.44190.67220.44450.038*
C9C0.6349 (3)0.0945 (4)0.55966 (15)0.0231 (9)
H9C0.63180.17710.58060.028*
C9D0.8142 (3)0.4483 (4)0.28920 (13)0.0195 (8)
H9D0.83410.54220.27960.023*
C10A0.6266 (3)0.1567 (4)0.70200 (14)0.0201 (8)
H10A0.68580.12960.69540.024*
C10B0.3936 (3)0.4627 (5)0.44212 (16)0.0282 (10)
H10B0.37840.46330.40850.034*
C10C0.6074 (3)0.0426 (4)0.57647 (15)0.0230 (8)
H10C0.58600.05280.60890.028*
C10D0.8694 (3)0.3576 (4)0.31670 (14)0.0203 (9)
H10D0.92620.39050.32600.024*
C11A0.5956 (3)0.2948 (4)0.68754 (14)0.0184 (8)
H11A0.63350.36120.67120.022*
C11B0.3775 (3)0.3374 (4)0.47050 (15)0.0208 (8)
H11B0.35140.25400.45590.025*
C11C0.6111 (3)0.1647 (4)0.54578 (14)0.0179 (8)
H11C0.59340.25750.55760.021*
C11D0.8405 (3)0.2165 (4)0.33060 (14)0.0192 (8)
H11D0.87830.15430.34870.023*
N1A0.5190 (2)0.6066 (3)0.68212 (12)0.0181 (7)
H1A0.5733 (13)0.613 (5)0.6920 (17)0.027*
N1B0.3914 (2)0.0634 (3)0.53248 (12)0.0174 (7)
H1B0.409 (3)0.043 (5)0.5028 (8)0.026*
N1C0.6691 (2)0.4142 (3)0.47731 (12)0.0202 (7)
H1C0.692 (3)0.433 (5)0.5058 (9)0.030*
N1D0.7739 (2)0.1022 (3)0.33140 (12)0.0186 (7)
H1D0.8288 (13)0.113 (5)0.3229 (18)0.028*
N3A0.3898 (2)0.5047 (3)0.66493 (13)0.0147 (7)
N3B0.3556 (2)0.1972 (3)0.59755 (11)0.0146 (6)
N3C0.6147 (2)0.2811 (3)0.41633 (12)0.0151 (6)
N3D0.6411 (2)0.0118 (3)0.34801 (13)0.0144 (7)
Cl10.20519 (7)0.48821 (10)0.58987 (4)0.0201 (2)
Cl20.21558 (6)0.24886 (9)0.69847 (3)0.01686 (19)
Cl30.46731 (6)0.24859 (10)0.31794 (3)0.01758 (19)
Cl40.45880 (7)0.01587 (10)0.42304 (4)0.0191 (2)
Co10.29988 (3)0.35776 (5)0.63889 (2)0.01224 (11)
Co20.54962 (3)0.12868 (5)0.37588 (2)0.01262 (11)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C2A0.0143 (19)0.0161 (17)0.0126 (18)0.0029 (16)0.0003 (18)0.0015 (13)
C2B0.0127 (18)0.0132 (16)0.0178 (16)0.0021 (15)0.0032 (15)0.0001 (13)
C2C0.0113 (18)0.0183 (18)0.0181 (17)0.0027 (15)0.0024 (15)0.0047 (14)
C2D0.019 (2)0.0153 (17)0.0110 (18)0.0030 (16)0.0016 (18)0.0017 (13)
C4A0.020 (2)0.0126 (16)0.0192 (17)0.0007 (15)0.0004 (16)0.0022 (13)
C4B0.020 (2)0.0147 (16)0.0173 (17)0.0036 (16)0.0018 (16)0.0038 (13)
C4C0.020 (2)0.0180 (17)0.0164 (16)0.0022 (16)0.0020 (16)0.0024 (14)
C4D0.022 (2)0.0120 (16)0.0231 (18)0.0024 (16)0.0029 (17)0.0030 (14)
C5A0.029 (2)0.0112 (16)0.025 (2)0.0029 (17)0.0005 (18)0.0017 (15)
C5B0.024 (2)0.0126 (16)0.0187 (17)0.0030 (16)0.0003 (16)0.0029 (13)
C5C0.027 (2)0.0168 (18)0.0180 (18)0.0057 (17)0.0024 (18)0.0001 (14)
C5D0.026 (2)0.0132 (17)0.025 (2)0.0025 (17)0.0042 (19)0.0008 (14)
C6A0.0142 (19)0.0151 (16)0.0121 (16)0.0016 (16)0.0028 (15)0.0030 (13)
C6B0.016 (2)0.0177 (17)0.0198 (18)0.0041 (16)0.0066 (17)0.0016 (14)
C6C0.0125 (19)0.0191 (17)0.0161 (17)0.0004 (15)0.0030 (15)0.0015 (13)
C6D0.0152 (19)0.0183 (17)0.0128 (17)0.0003 (16)0.0021 (15)0.0006 (14)
C7A0.0143 (19)0.0206 (18)0.0178 (18)0.0010 (16)0.0001 (15)0.0000 (14)
C7B0.026 (2)0.0190 (18)0.024 (2)0.0003 (18)0.0101 (18)0.0023 (16)
C7C0.026 (2)0.0216 (19)0.0187 (19)0.0037 (17)0.0051 (18)0.0067 (15)
C7D0.0141 (19)0.0223 (19)0.0161 (18)0.0019 (16)0.0006 (15)0.0005 (14)
C8A0.022 (2)0.0186 (17)0.0158 (18)0.0036 (17)0.0014 (17)0.0030 (14)
C8B0.032 (3)0.0183 (19)0.037 (2)0.0032 (18)0.013 (2)0.0042 (17)
C8C0.031 (2)0.0163 (17)0.030 (2)0.0072 (18)0.010 (2)0.0052 (16)
C8D0.020 (2)0.0176 (17)0.0197 (18)0.0057 (17)0.0000 (17)0.0047 (15)
C9A0.026 (2)0.0180 (18)0.0193 (18)0.0050 (18)0.0046 (18)0.0018 (14)
C9B0.038 (3)0.022 (2)0.035 (2)0.003 (2)0.017 (2)0.0139 (17)
C9C0.026 (2)0.0185 (18)0.025 (2)0.0029 (18)0.0084 (18)0.0061 (15)
C9D0.028 (2)0.0143 (17)0.0165 (18)0.0034 (18)0.0028 (17)0.0014 (14)
C10A0.015 (2)0.0263 (19)0.0188 (18)0.0061 (16)0.0007 (16)0.0022 (15)
C10B0.029 (2)0.031 (2)0.024 (2)0.007 (2)0.0067 (19)0.0114 (17)
C10C0.023 (2)0.0251 (19)0.0206 (19)0.0042 (18)0.0024 (18)0.0007 (15)
C10D0.018 (2)0.025 (2)0.0173 (18)0.0071 (16)0.0015 (17)0.0053 (14)
C11A0.0157 (19)0.0234 (19)0.0161 (17)0.0025 (17)0.0012 (16)0.0007 (14)
C11B0.020 (2)0.0209 (18)0.0213 (19)0.0024 (17)0.0019 (17)0.0038 (15)
C11C0.020 (2)0.0160 (17)0.0179 (18)0.0002 (16)0.0031 (16)0.0019 (13)
C11D0.017 (2)0.0221 (19)0.0186 (18)0.0029 (17)0.0016 (16)0.0003 (14)
N1A0.0162 (17)0.0173 (15)0.0209 (16)0.0036 (15)0.0041 (15)0.0004 (13)
N1B0.0211 (17)0.0153 (14)0.0158 (14)0.0022 (14)0.0030 (14)0.0019 (12)
N1C0.028 (2)0.0178 (15)0.0148 (15)0.0074 (15)0.0028 (15)0.0026 (12)
N1D0.0160 (17)0.0169 (15)0.0230 (17)0.0068 (14)0.0042 (15)0.0036 (13)
N3A0.0179 (18)0.0108 (14)0.0154 (17)0.0021 (12)0.0005 (15)0.0008 (11)
N3B0.0161 (16)0.0118 (14)0.0161 (15)0.0029 (13)0.0010 (13)0.0020 (11)
N3C0.0131 (16)0.0140 (14)0.0184 (14)0.0019 (13)0.0005 (13)0.0028 (11)
N3D0.0149 (18)0.0139 (15)0.0145 (17)0.0005 (13)0.0011 (15)0.0004 (11)
Cl10.0230 (5)0.0216 (4)0.0157 (5)0.0087 (4)0.0023 (4)0.0014 (3)
Cl20.0137 (4)0.0177 (4)0.0192 (4)0.0005 (4)0.0019 (4)0.0033 (3)
Cl30.0139 (4)0.0182 (4)0.0207 (4)0.0013 (4)0.0021 (4)0.0031 (3)
Cl40.0231 (5)0.0178 (4)0.0164 (5)0.0053 (4)0.0039 (4)0.0017 (3)
Co10.0128 (2)0.0113 (2)0.0126 (2)0.00102 (18)0.0001 (2)0.00035 (18)
Co20.0127 (2)0.0116 (2)0.0136 (2)0.00019 (18)0.0001 (2)0.00131 (18)
Geometric parameters (Å, º) top
C2A—N1A1.333 (5)C7C—C8C1.376 (6)
C2A—N3A1.340 (5)C7C—H7C0.9300
C2A—C6A1.463 (5)C7D—C8D1.389 (5)
C2B—N3B1.332 (5)C7D—H7D0.9300
C2B—N1B1.338 (5)C8A—C9A1.378 (6)
C2B—C6B1.458 (5)C8A—H8A0.9300
C2C—N3C1.331 (5)C8B—C9B1.393 (6)
C2C—N1C1.340 (5)C8B—H8B0.9300
C2C—C6C1.457 (5)C8C—C9C1.383 (6)
C2D—N1D1.329 (5)C8C—H8C0.9300
C2D—N3D1.333 (5)C8D—C9D1.376 (6)
C2D—C6D1.463 (5)C8D—H8D0.9300
C4A—C5A1.340 (6)C9A—C10A1.374 (6)
C4A—N3A1.377 (4)C9A—H9A0.9300
C4A—H4A0.9300C9B—C10B1.378 (6)
C4B—C5B1.348 (5)C9B—H9B0.9300
C4B—N3B1.382 (4)C9C—C10C1.373 (6)
C4B—H4B0.9300C9C—H9C0.9300
C4C—C5C1.336 (5)C9D—C10D1.371 (6)
C4C—N3C1.379 (4)C9D—H9D0.9300
C4C—H4C0.9300C10A—C11A1.378 (5)
C4D—C5D1.341 (6)C10A—H10A0.9300
C4D—N3D1.386 (4)C10B—C11B1.378 (5)
C4D—H4D0.9300C10B—H10B0.9300
C5A—N1A1.359 (5)C10C—C11C1.371 (5)
C5A—H5A0.9300C10C—H10C0.9300
C5B—N1B1.361 (5)C10D—C11D1.388 (5)
C5B—H5B0.9300C10D—H10D0.9300
C5C—N1C1.367 (5)C11A—H11A0.9300
C5C—H5C0.9300C11B—H11B0.9300
C5D—N1D1.360 (5)C11C—H11C0.9300
C5D—H5D0.9300C11D—H11D0.9300
C6A—C11A1.383 (5)N1A—H1A0.852 (13)
C6A—C7A1.385 (5)N1B—H1B0.858 (13)
C6B—C7B1.382 (6)N1C—H1C0.855 (13)
C6B—C11B1.383 (6)N1D—H1D0.852 (13)
C6C—C11C1.389 (5)N3A—Co12.004 (3)
C6C—C7C1.393 (5)N3B—Co11.999 (3)
C6D—C7D1.386 (5)N3C—Co21.997 (3)
C6D—C11D1.385 (6)N3D—Co22.000 (3)
C7A—C8A1.373 (5)Cl1—Co12.2548 (11)
C7A—H7A0.9300Cl2—Co12.2544 (10)
C7B—C8B1.374 (6)Cl3—Co22.2524 (10)
C7B—H7B0.9300Cl4—Co22.2603 (11)
N1A—C2A—N3A109.1 (3)C10A—C9A—C8A120.3 (4)
N1A—C2A—C6A125.8 (4)C10A—C9A—H9A119.8
N3A—C2A—C6A125.0 (3)C8A—C9A—H9A119.8
N3B—C2B—N1B109.8 (3)C10B—C9B—C8B119.4 (4)
N3B—C2B—C6B126.9 (3)C10B—C9B—H9B120.3
N1B—C2B—C6B123.3 (3)C8B—C9B—H9B120.3
N3C—C2C—N1C109.5 (3)C10C—C9C—C8C119.8 (4)
N3C—C2C—C6C127.0 (3)C10C—C9C—H9C120.1
N1C—C2C—C6C123.5 (3)C8C—C9C—H9C120.1
N1D—C2D—N3D110.1 (3)C10D—C9D—C8D120.4 (3)
N1D—C2D—C6D124.7 (4)C10D—C9D—H9D119.8
N3D—C2D—C6D125.3 (3)C8D—C9D—H9D119.8
C5A—C4A—N3A109.2 (3)C9A—C10A—C11A120.3 (4)
C5A—C4A—H4A125.4C9A—C10A—H10A119.9
N3A—C4A—H4A125.4C11A—C10A—H10A119.9
C5B—C4B—N3B109.1 (3)C9B—C10B—C11B120.2 (4)
C5B—C4B—H4B125.4C9B—C10B—H10B119.9
N3B—C4B—H4B125.4C11B—C10B—H10B119.9
C5C—C4C—N3C109.2 (3)C11C—C10C—C9C120.4 (4)
C5C—C4C—H4C125.4C11C—C10C—H10C119.8
N3C—C4C—H4C125.4C9C—C10C—H10C119.8
C5D—C4D—N3D109.0 (4)C9D—C10D—C11D120.0 (4)
C5D—C4D—H4D125.5C9D—C10D—H10D120.0
N3D—C4D—H4D125.5C11D—C10D—H10D120.0
C4A—C5A—N1A106.5 (3)C10A—C11A—C6A119.3 (4)
C4A—C5A—H5A126.8C10A—C11A—H11A120.4
N1A—C5A—H5A126.8C6A—C11A—H11A120.4
C4B—C5B—N1B106.4 (3)C10B—C11B—C6B120.5 (4)
C4B—C5B—H5B126.8C10B—C11B—H11B119.8
N1B—C5B—H5B126.8C6B—C11B—H11B119.8
C4C—C5C—N1C106.7 (3)C10C—C11C—C6C120.1 (4)
C4C—C5C—H5C126.6C10C—C11C—H11C119.9
N1C—C5C—H5C126.6C6C—C11C—H11C119.9
C4D—C5D—N1D106.7 (3)C6D—C11D—C10D120.0 (4)
C4D—C5D—H5D126.7C6D—C11D—H11D120.0
N1D—C5D—H5D126.7C10D—C11D—H11D120.0
C11A—C6A—C7A120.4 (3)C2A—N1A—C5A109.0 (3)
C11A—C6A—C2A120.0 (3)C2A—N1A—H1A123 (3)
C7A—C6A—C2A119.6 (3)C5A—N1A—H1A128 (3)
C7B—C6B—C11B119.5 (4)C2B—N1B—C5B108.7 (3)
C7B—C6B—C2B120.5 (4)C2B—N1B—H1B124 (3)
C11B—C6B—C2B120.0 (3)C5B—N1B—H1B128 (3)
C11C—C6C—C7C119.5 (3)C2C—N1C—C5C108.2 (3)
C11C—C6C—C2C120.3 (3)C2C—N1C—H1C123 (3)
C7C—C6C—C2C120.2 (4)C5C—N1C—H1C128 (3)
C7D—C6D—C11D119.7 (3)C2D—N1D—C5D108.6 (3)
C7D—C6D—C2D119.7 (3)C2D—N1D—H1D129 (3)
C11D—C6D—C2D120.5 (4)C5D—N1D—H1D122 (3)
C8A—C7A—C6A119.6 (4)C2A—N3A—C4A106.2 (3)
C8A—C7A—H7A120.2C2A—N3A—Co1128.5 (2)
C6A—C7A—H7A120.2C4A—N3A—Co1123.0 (3)
C8B—C7B—C6B120.2 (4)C2B—N3B—C4B106.1 (3)
C8B—C7B—H7B119.9C2B—N3B—Co1129.1 (2)
C6B—C7B—H7B119.9C4B—N3B—Co1122.5 (2)
C8C—C7C—C6C119.6 (4)C2C—N3C—C4C106.4 (3)
C8C—C7C—H7C120.2C2C—N3C—Co2130.5 (3)
C6C—C7C—H7C120.2C4C—N3C—Co2122.3 (2)
C6D—C7D—C8D119.7 (3)C2D—N3D—C4D105.7 (3)
C6D—C7D—H7D120.1C2D—N3D—Co2127.7 (2)
C8D—C7D—H7D120.1C4D—N3D—Co2123.6 (3)
C7A—C8A—C9A120.1 (4)N3B—Co1—N3A113.02 (13)
C7A—C8A—H8A120.0N3B—Co1—Cl2108.16 (9)
C9A—C8A—H8A120.0N3A—Co1—Cl2114.16 (10)
C7B—C8B—C9B120.3 (4)N3B—Co1—Cl1108.05 (9)
C7B—C8B—H8B119.8N3A—Co1—Cl1106.18 (9)
C9B—C8B—H8B119.8Cl2—Co1—Cl1106.93 (4)
C7C—C8C—C9C120.5 (4)N3C—Co2—N3D107.77 (13)
C7C—C8C—H8C119.8N3C—Co2—Cl3108.14 (9)
C9C—C8C—H8C119.8N3D—Co2—Cl3114.40 (10)
C9D—C8D—C7D120.1 (3)N3C—Co2—Cl4112.26 (9)
C9D—C8D—H8D119.9N3D—Co2—Cl4104.73 (9)
C7D—C8D—H8D119.9Cl3—Co2—Cl4109.60 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1A—H1A···Cl2i0.85 (2)2.46 (3)3.229 (3)151 (4)
N1B—H1B···Cl40.86 (3)2.33 (3)3.183 (3)179 (6)
N1C—H1C···Cl1i0.85 (3)2.37 (3)3.190 (3)161 (4)
N1D—H1D···Cl3ii0.85 (2)2.40 (3)3.184 (3)154 (4)
Symmetry codes: (i) x+1/2, y+1, z; (ii) x+1/2, y, z.
(2) top
Crystal data top
C18H16CoI2N4F(000) = 1140
Mr = 601.08Dx = 2.020 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 7.5817 (4) ÅCell parameters from 2244 reflections
b = 18.625 (1) Åθ = 2.9–28.6°
c = 14.2346 (11) ŵ = 4.00 mm1
β = 100.448 (7)°T = 100 K
V = 1976.7 (2) Å3Plate, blue
Z = 40.21 × 0.14 × 0.07 mm
Data collection top
Agilent Technologies SuperNova with Atlas detector
diffractometer
2136 independent reflections
Radiation source: SuperNova (Mo) X-ray Source1949 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.022
Detector resolution: 10.4223 pixels mm-1θmax = 27.0°, θmin = 2.9°
ω scansh = 99
Absorption correction: multi-scan
CrysAlisPro 1.171.38.43 (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 2123
Tmin = 0.605, Tmax = 1.000l = 188
4313 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.022Hydrogen site location: mixed
wR(F2) = 0.057H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.0312P)2 + 0.5775P]
where P = (Fo2 + 2Fc2)/3
2136 reflections(Δ/σ)max < 0.001
117 parametersΔρmax = 0.57 e Å3
1 restraintΔρmin = 0.62 e Å3
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I0.64585 (2)0.10658 (2)0.13296 (2)0.01864 (8)
Co0.50000.18344 (2)0.25000.01323 (12)
N10.1429 (3)0.31000 (12)0.06410 (16)0.0180 (5)
H10.114 (4)0.3442 (12)0.0256 (18)0.027*
N30.3093 (3)0.23837 (11)0.16429 (15)0.0137 (4)
C70.6293 (3)0.33201 (15)0.14263 (18)0.0168 (5)
H70.65790.28340.14800.020*
C60.4513 (3)0.35340 (14)0.12489 (19)0.0167 (5)
C20.3065 (3)0.30033 (13)0.11763 (18)0.0149 (5)
C40.1401 (3)0.20807 (16)0.13807 (19)0.0180 (6)
H40.10360.16450.16000.022*
C110.4104 (4)0.42593 (15)0.1160 (2)0.0259 (6)
H110.29130.44070.10390.031*
C90.7235 (4)0.45505 (15)0.1442 (2)0.0299 (7)
H90.81450.48920.15140.036*
C50.0375 (3)0.25212 (15)0.0757 (2)0.0206 (6)
H50.08100.24470.04640.025*
C80.7648 (4)0.38288 (15)0.1525 (2)0.0222 (6)
H80.88410.36830.16470.027*
C100.5460 (4)0.47631 (16)0.1250 (3)0.0356 (8)
H100.51760.52480.11820.043*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I0.01936 (11)0.01558 (12)0.02040 (12)0.00516 (6)0.00205 (8)0.00084 (6)
Co0.0117 (2)0.0111 (2)0.0157 (2)0.0000.00068 (18)0.000
N10.0149 (10)0.0222 (11)0.0161 (11)0.0067 (9)0.0007 (9)0.0012 (9)
N30.0100 (9)0.0138 (10)0.0168 (11)0.0008 (8)0.0005 (8)0.0018 (9)
C70.0208 (12)0.0146 (13)0.0150 (13)0.0005 (10)0.0028 (10)0.0005 (10)
C60.0203 (12)0.0165 (12)0.0139 (13)0.0001 (10)0.0047 (10)0.0010 (10)
C20.0150 (11)0.0160 (12)0.0131 (12)0.0041 (9)0.0008 (10)0.0026 (10)
C40.0120 (12)0.0196 (14)0.0217 (14)0.0003 (9)0.0012 (11)0.0046 (11)
C110.0236 (13)0.0193 (14)0.0359 (17)0.0063 (11)0.0086 (13)0.0033 (13)
C90.0302 (16)0.0206 (14)0.043 (2)0.0093 (12)0.0178 (14)0.0078 (14)
C50.0119 (11)0.0287 (14)0.0202 (14)0.0030 (10)0.0001 (10)0.0068 (12)
C80.0182 (13)0.0273 (14)0.0221 (15)0.0025 (11)0.0064 (11)0.0042 (12)
C100.0389 (18)0.0142 (14)0.058 (2)0.0007 (12)0.0218 (17)0.0013 (14)
Geometric parameters (Å, º) top
I—Co2.5915 (3)C6—C111.386 (4)
Co—N31.997 (2)C6—C21.467 (3)
Co—N3i1.997 (2)C4—C51.348 (4)
Co—Ii2.5916 (3)C4—H40.9300
N1—C21.345 (3)C11—C101.380 (4)
N1—C51.369 (4)C11—H110.9300
N1—H10.843 (10)C9—C81.381 (4)
N3—C21.330 (3)C9—C101.382 (5)
N3—C41.389 (3)C9—H90.9300
C7—C61.386 (3)C5—H50.9300
C7—C81.386 (4)C8—H80.9300
C7—H70.9300C10—H100.9300
N3—Co—N3i118.35 (11)N1—C2—C6123.5 (2)
N3—Co—I103.67 (6)C5—C4—N3108.9 (2)
N3i—Co—I109.25 (6)C5—C4—H4125.5
N3—Co—Ii109.25 (6)N3—C4—H4125.5
N3i—Co—Ii103.67 (6)C10—C11—C6120.2 (2)
I—Co—Ii112.933 (18)C10—C11—H11119.9
C2—N1—C5109.0 (2)C6—C11—H11119.9
C2—N1—H1125 (2)C8—C9—C10119.6 (3)
C5—N1—H1126 (2)C8—C9—H9120.2
C2—N3—C4106.8 (2)C10—C9—H9120.2
C2—N3—Co133.94 (16)C4—C5—N1106.2 (2)
C4—N3—Co119.15 (17)C4—C5—H5126.9
C6—C7—C8120.1 (3)N1—C5—H5126.9
C6—C7—H7120.0C9—C8—C7120.3 (3)
C8—C7—H7120.0C9—C8—H8119.9
C7—C6—C11119.4 (2)C7—C8—H8119.9
C7—C6—C2120.7 (2)C11—C10—C9120.4 (3)
C11—C6—C2119.9 (2)C11—C10—H10119.8
N3—C2—N1109.2 (2)C9—C10—H10119.8
N3—C2—C6127.3 (2)
Symmetry code: (i) x+1, y, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···Iii0.84 (2)2.86 (3)3.584 (2)144 (2)
Symmetry code: (ii) x+1/2, y+1/2, z.
(3) top
Crystal data top
C18H16CoN6O6F(000) = 964
Mr = 471.30Dx = 1.596 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.54184 Å
a = 9.4982 (9) ÅCell parameters from 2592 reflections
b = 14.9627 (11) Åθ = 3.2–72.3°
c = 14.5081 (14) ŵ = 7.32 mm1
β = 107.938 (10)°T = 100 K
V = 1961.6 (3) Å3Prism, purple
Z = 40.18 × 0.13 × 0.09 mm
Data collection top
Agilent Technologies SuperNova with Atlas detector
diffractometer
3563 independent reflections
Radiation source: SuperNova (Cu) X-ray Source2849 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.041
Detector resolution: 10.4223 pixels mm-1θmax = 68.5°, θmin = 4.4°
ω scansh = 1110
Absorption correction: multi-scan
CrysAlisPro 1.171.38.43 (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1817
Tmin = 0.671, Tmax = 1.000l = 1217
7276 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.048Hydrogen site location: mixed
wR(F2) = 0.104H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0392P)2 + 1.633P]
where P = (Fo2 + 2Fc2)/3
3563 reflections(Δ/σ)max = 0.001
286 parametersΔρmax = 0.27 e Å3
2 restraintsΔρmin = 0.45 e Å3
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Co0.94789 (5)0.27868 (3)0.58536 (3)0.02162 (14)
N1A1.3875 (3)0.33670 (19)0.60016 (19)0.0252 (6)
H1A1.4778 (16)0.326 (2)0.606 (3)0.038*
C2A1.2830 (3)0.2755 (2)0.6001 (2)0.0228 (6)
N3A1.1525 (3)0.31661 (17)0.58262 (18)0.0223 (5)
C4A1.1774 (3)0.4063 (2)0.5701 (2)0.0258 (7)
H4A1.10560.45080.55620.031*
C5A1.3229 (3)0.4190 (2)0.5812 (2)0.0270 (7)
H5A1.36930.47290.57680.032*
C6A1.3145 (3)0.1803 (2)0.6187 (2)0.0255 (7)
C7A1.2024 (4)0.1165 (2)0.5868 (2)0.0303 (7)
H7A1.10780.13430.55030.036*
C8A1.2313 (4)0.0269 (2)0.6094 (3)0.0392 (9)
H8A1.15600.01520.58850.047*
C9A1.3724 (4)0.0000 (3)0.6631 (3)0.0428 (9)
H9A1.39140.05970.68020.051*
C10A1.4845 (4)0.0624 (3)0.6910 (3)0.0398 (9)
H10A1.58010.04370.72430.048*
C11A1.4571 (3)0.1521 (2)0.6703 (2)0.0325 (8)
H11A1.53340.19350.69080.039*
N1B1.0491 (3)0.08421 (19)0.7992 (2)0.0283 (6)
H1B1.102 (4)0.055 (2)0.8468 (18)0.042*
C2B1.0705 (3)0.1665 (2)0.7693 (2)0.0236 (7)
N3B0.9615 (3)0.18704 (17)0.68944 (18)0.0230 (6)
C4B0.8672 (3)0.1141 (2)0.6705 (3)0.0298 (7)
H4B0.78030.10980.61900.036*
C5B0.9204 (3)0.0501 (2)0.7383 (3)0.0328 (8)
H5B0.87840.00530.74250.039*
C6B1.1979 (3)0.2220 (2)0.8192 (2)0.0255 (7)
C7B1.1813 (4)0.3129 (2)0.8327 (2)0.0335 (8)
H7B1.08840.33940.81020.040*
C8B1.3046 (4)0.3640 (3)0.8800 (3)0.0439 (10)
H8B1.29430.42490.88910.053*
C9B1.4426 (4)0.3245 (3)0.9136 (2)0.0479 (11)
H9B1.52490.35880.94540.058*
C10B1.4587 (4)0.2343 (3)0.9002 (3)0.0435 (10)
H10B1.55190.20810.92230.052*
C11B1.3374 (3)0.1829 (3)0.8542 (2)0.0332 (8)
H11B1.34840.12190.84640.040*
N10.8206 (3)0.2518 (2)0.3997 (2)0.0318 (7)
O10.8483 (2)0.19681 (15)0.47246 (15)0.0282 (5)
O20.8512 (2)0.33213 (17)0.42164 (18)0.0376 (6)
O30.7668 (3)0.22440 (19)0.31765 (17)0.0450 (7)
N20.7467 (3)0.38976 (18)0.61369 (18)0.0249 (6)
O40.8840 (2)0.40133 (15)0.61863 (16)0.0281 (5)
O50.6984 (2)0.31153 (14)0.59877 (15)0.0251 (5)
O60.6716 (2)0.45384 (16)0.62207 (18)0.0362 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co0.0153 (2)0.0250 (3)0.0237 (3)0.0015 (2)0.00489 (19)0.0002 (2)
N1A0.0148 (11)0.0335 (15)0.0290 (15)0.0004 (11)0.0091 (11)0.0030 (11)
C2A0.0167 (13)0.0300 (17)0.0224 (16)0.0009 (12)0.0072 (12)0.0018 (13)
N3A0.0165 (11)0.0283 (14)0.0223 (14)0.0009 (10)0.0059 (10)0.0008 (10)
C4A0.0188 (14)0.0298 (17)0.0295 (18)0.0004 (13)0.0084 (13)0.0006 (13)
C5A0.0226 (15)0.0291 (18)0.0304 (18)0.0030 (13)0.0097 (13)0.0014 (13)
C6A0.0242 (15)0.0307 (17)0.0248 (17)0.0031 (13)0.0123 (13)0.0004 (13)
C7A0.0287 (16)0.0328 (18)0.0332 (19)0.0007 (14)0.0150 (14)0.0055 (14)
C8A0.042 (2)0.034 (2)0.050 (2)0.0010 (16)0.0269 (18)0.0046 (17)
C9A0.052 (2)0.034 (2)0.054 (2)0.0158 (18)0.035 (2)0.0080 (18)
C10A0.0361 (19)0.050 (2)0.037 (2)0.0189 (18)0.0176 (16)0.0095 (17)
C11A0.0250 (16)0.042 (2)0.0332 (19)0.0065 (15)0.0123 (14)0.0023 (15)
N1B0.0236 (14)0.0298 (15)0.0299 (16)0.0021 (11)0.0059 (12)0.0095 (12)
C2B0.0192 (14)0.0277 (17)0.0257 (17)0.0023 (12)0.0097 (13)0.0017 (13)
N3B0.0166 (11)0.0252 (14)0.0266 (14)0.0011 (10)0.0056 (11)0.0015 (11)
C4B0.0207 (15)0.0279 (18)0.038 (2)0.0036 (13)0.0040 (13)0.0006 (14)
C5B0.0256 (16)0.0264 (18)0.043 (2)0.0018 (14)0.0062 (15)0.0043 (15)
C6B0.0215 (14)0.0381 (19)0.0178 (16)0.0044 (13)0.0070 (12)0.0038 (14)
C7B0.0283 (16)0.041 (2)0.0283 (19)0.0076 (15)0.0049 (14)0.0046 (15)
C8B0.052 (2)0.047 (2)0.028 (2)0.0228 (19)0.0062 (17)0.0012 (16)
C9B0.036 (2)0.082 (3)0.0169 (19)0.029 (2)0.0048 (15)0.0108 (18)
C10B0.0231 (17)0.077 (3)0.026 (2)0.0086 (18)0.0022 (14)0.0209 (19)
C11B0.0221 (15)0.054 (2)0.0243 (18)0.0003 (15)0.0080 (14)0.0123 (15)
N10.0197 (12)0.0466 (19)0.0295 (17)0.0027 (12)0.0082 (12)0.0008 (13)
O10.0253 (11)0.0360 (13)0.0213 (12)0.0012 (10)0.0043 (9)0.0026 (9)
O20.0315 (12)0.0377 (15)0.0427 (15)0.0051 (11)0.0102 (11)0.0076 (11)
O30.0389 (14)0.073 (2)0.0201 (14)0.0050 (13)0.0050 (11)0.0065 (13)
N20.0167 (12)0.0312 (15)0.0257 (15)0.0032 (11)0.0046 (11)0.0016 (11)
O40.0135 (9)0.0312 (12)0.0397 (13)0.0034 (9)0.0082 (9)0.0039 (10)
O50.0188 (10)0.0270 (12)0.0274 (12)0.0042 (9)0.0041 (9)0.0021 (9)
O60.0216 (11)0.0308 (13)0.0575 (17)0.0043 (10)0.0143 (11)0.0088 (12)
Geometric parameters (Å, º) top
Co—N3B2.014 (3)N1B—C5B1.368 (4)
Co—O12.031 (2)N1B—H1B0.838 (10)
Co—N3A2.037 (2)C2B—N3B1.330 (4)
Co—O42.037 (2)C2B—C6B1.463 (4)
Co—O22.404 (2)N3B—C4B1.385 (4)
N1A—C2A1.351 (4)C4B—C5B1.353 (5)
N1A—C5A1.366 (4)C4B—H4B0.9300
N1A—H1A0.852 (10)C5B—H5B0.9300
C2A—N3A1.336 (4)C6B—C7B1.390 (5)
C2A—C6A1.463 (4)C6B—C11B1.393 (4)
N3A—C4A1.384 (4)C7B—C8B1.390 (5)
C4A—C5A1.354 (4)C7B—H7B0.9300
C4A—H4A0.9300C8B—C9B1.383 (6)
C5A—H5A0.9300C8B—H8B0.9300
C6A—C11A1.396 (4)C9B—C10B1.378 (6)
C6A—C7A1.398 (4)C9B—H9B0.9300
C7A—C8A1.388 (5)C10B—C11B1.375 (5)
C7A—H7A0.9300C10B—H10B0.9300
C8A—C9A1.386 (5)C11B—H11B0.9300
C8A—H8A0.9300N1—O31.213 (4)
C9A—C10A1.379 (5)N1—O21.254 (4)
C9A—H9A0.9300N1—O11.300 (4)
C10A—C11A1.383 (5)N2—O61.223 (3)
C10A—H10A0.9300N2—O51.252 (3)
C11A—H11A0.9300N2—O41.295 (3)
N1B—C2B1.341 (4)
N3B—Co—O195.77 (10)C2B—N1B—C5B109.1 (3)
N3B—Co—N3A111.28 (10)C2B—N1B—H1B129 (3)
O1—Co—N3A111.25 (9)C5B—N1B—H1B122 (3)
N3B—Co—O4113.00 (10)N3B—C2B—N1B109.8 (3)
O1—Co—O4129.47 (9)N3B—C2B—C6B127.0 (3)
N3A—Co—O496.29 (9)N1B—C2B—C6B123.1 (3)
N3B—Co—O2152.12 (9)C2B—N3B—C4B105.8 (3)
O1—Co—O257.49 (9)C2B—N3B—Co131.6 (2)
N3A—Co—O287.96 (9)C4B—N3B—Co120.0 (2)
O4—Co—O283.30 (9)C5B—C4B—N3B109.8 (3)
C2A—N1A—C5A109.1 (2)C5B—C4B—H4B125.1
C2A—N1A—H1A126 (3)N3B—C4B—H4B125.1
C5A—N1A—H1A125 (3)C4B—C5B—N1B105.4 (3)
N3A—C2A—N1A109.0 (3)C4B—C5B—H5B127.3
N3A—C2A—C6A127.5 (3)N1B—C5B—H5B127.3
N1A—C2A—C6A123.5 (3)C7B—C6B—C11B119.8 (3)
C2A—N3A—C4A106.6 (2)C7B—C6B—C2B120.9 (3)
C2A—N3A—Co134.7 (2)C11B—C6B—C2B119.4 (3)
C4A—N3A—Co118.38 (19)C6B—C7B—C8B119.5 (3)
C5A—C4A—N3A109.3 (3)C6B—C7B—H7B120.2
C5A—C4A—H4A125.3C8B—C7B—H7B120.2
N3A—C4A—H4A125.3C9B—C8B—C7B120.1 (4)
C4A—C5A—N1A106.0 (3)C9B—C8B—H8B119.9
C4A—C5A—H5A127.0C7B—C8B—H8B119.9
N1A—C5A—H5A127.0C10B—C9B—C8B120.2 (3)
C11A—C6A—C7A119.1 (3)C10B—C9B—H9B119.9
C11A—C6A—C2A120.2 (3)C8B—C9B—H9B119.9
C7A—C6A—C2A120.7 (3)C11B—C10B—C9B120.2 (3)
C8A—C7A—C6A120.4 (3)C11B—C10B—H10B119.9
C8A—C7A—H7A119.8C9B—C10B—H10B119.9
C6A—C7A—H7A119.8C10B—C11B—C6B120.2 (4)
C9A—C8A—C7A120.0 (4)C10B—C11B—H11B119.9
C9A—C8A—H8A120.0C6B—C11B—H11B119.9
C7A—C8A—H8A120.0O3—N1—O2124.6 (3)
C10A—C9A—C8A119.6 (4)O3—N1—O1120.1 (3)
C10A—C9A—H9A120.2O2—N1—O1115.3 (3)
C8A—C9A—H9A120.2N1—O1—Co101.58 (18)
C9A—C10A—C11A121.1 (3)N1—O2—Co85.42 (18)
C9A—C10A—H10A119.4O6—N2—O5123.8 (2)
C11A—C10A—H10A119.4O6—N2—O4119.8 (3)
C10A—C11A—C6A119.7 (3)O5—N2—O4116.3 (2)
C10A—C11A—H11A120.1N2—O4—Co103.59 (18)
C6A—C11A—H11A120.1
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1A—H1A···O5i0.85 (2)2.14 (2)2.983 (4)171 (4)
N1B—H1B···O4ii0.84 (3)2.35 (3)2.974 (4)132 (3)
N1B—H1B···O6ii0.84 (3)2.55 (4)3.206 (4)135 (3)
Symmetry codes: (i) x+1, y, z; (ii) x+2, y1/2, z+3/2.
(4) top
Crystal data top
C20H16CoN6S2F(000) = 1896
Mr = 463.44Dx = 1.482 Mg m3
Monoclinic, I2/aMo Kα radiation, λ = 0.71073 Å
a = 17.5108 (14) ÅCell parameters from 2206 reflections
b = 13.8088 (13) Åθ = 4.6–28.3°
c = 18.9150 (16) ŵ = 1.05 mm1
β = 114.745 (9)°T = 100 K
V = 4153.7 (7) Å3Prism, blue
Z = 80.15 × 0.10 × 0.09 mm
Data collection top
Oxford Diffraction SuperNova with Atlas CCD detector
diffractometer
4413 independent reflections
Radiation source: SuperNova (Mo) X-ray Source3003 reflections with I > 2σ(I)
Detector resolution: 10.4223 pixels mm-1Rint = 0.065
ω scansθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan
CrysAlisPro 1.171.38.43 (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 2217
Tmin = 0.665, Tmax = 1.000k = 1517
9606 measured reflectionsl = 2423
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.054Hydrogen site location: mixed
wR(F2) = 0.151H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.0617P)2]
where P = (Fo2 + 2Fc2)/3
4413 reflections(Δ/σ)max = 0.001
268 parametersΔρmax = 0.90 e Å3
1 restraintΔρmin = 0.84 e Å3
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Co0.62170 (2)0.56587 (4)0.24871 (2)0.02358 (17)
C2A0.51801 (18)0.4464 (2)0.31250 (18)0.0227 (7)
C2B0.71798 (19)0.4339 (2)0.18356 (19)0.0224 (7)
C4A0.6213 (2)0.5236 (3)0.40307 (18)0.0292 (8)
H4A0.66940.56110.42800.035*
C4B0.61548 (19)0.5123 (3)0.09384 (18)0.0275 (8)
H4B0.56860.55170.06960.033*
C5A0.5751 (2)0.4832 (3)0.4376 (2)0.0320 (9)
H5A0.58510.48740.48980.038*
C5B0.6564 (2)0.4655 (3)0.0573 (2)0.0320 (9)
H5B0.64340.46660.00430.038*
C6A0.46063 (18)0.4052 (2)0.23887 (19)0.0239 (8)
C6B0.77741 (19)0.3920 (2)0.25700 (18)0.0215 (7)
C7A0.4883 (2)0.3823 (3)0.18236 (19)0.0281 (8)
H7A0.54480.39010.19290.034*
C7B0.7523 (2)0.3711 (3)0.31584 (18)0.0254 (8)
H7B0.69690.38190.30810.030*
C8A0.4331 (2)0.3479 (3)0.1105 (2)0.0392 (10)
H8A0.45250.33290.07290.047*
C8B0.8094 (2)0.3342 (3)0.38565 (19)0.0286 (8)
H8B0.79220.31990.42480.034*
C9A0.3495 (2)0.3357 (3)0.0945 (2)0.0475 (12)
H9A0.31220.31320.04600.057*
C9B0.8926 (2)0.3182 (3)0.3982 (2)0.0304 (9)
H9B0.93100.29400.44570.036*
C10A0.3208 (2)0.3570 (3)0.1506 (3)0.0458 (11)
H10A0.26450.34740.13980.055*
C10B0.9176 (2)0.3383 (3)0.3397 (2)0.0296 (8)
H10B0.97270.32640.34730.036*
C11A0.37491 (19)0.3923 (3)0.2226 (2)0.0320 (9)
H11A0.35510.40750.25980.038*
C11B0.86089 (19)0.3761 (2)0.26988 (19)0.0238 (8)
H11B0.87850.39110.23110.029*
N1A0.51046 (17)0.4350 (2)0.38003 (17)0.0283 (7)
H1A0.4761 (19)0.397 (2)0.387 (2)0.042*
N1B0.72080 (17)0.4162 (2)0.11392 (16)0.0275 (7)
H1B0.757 (2)0.378 (3)0.110 (2)0.041*
N3A0.58572 (15)0.5002 (2)0.32495 (15)0.0252 (6)
N3B0.65360 (15)0.4930 (2)0.17253 (15)0.0231 (6)
N10.52229 (17)0.6411 (2)0.18263 (16)0.0279 (7)
C10.4587 (2)0.6756 (3)0.14190 (19)0.0241 (8)
S10.36848 (5)0.72505 (7)0.08600 (5)0.0304 (3)
N20.72600 (17)0.6298 (2)0.31726 (17)0.0327 (7)
C20.7899 (2)0.6578 (3)0.36301 (19)0.0270 (8)
S20.87915 (5)0.69905 (8)0.42763 (6)0.0376 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co0.0172 (2)0.0267 (3)0.0263 (3)0.00093 (17)0.00859 (18)0.0028 (2)
C2A0.0191 (15)0.025 (2)0.0233 (18)0.0036 (13)0.0077 (12)0.0017 (15)
C2B0.0211 (16)0.023 (2)0.0246 (18)0.0027 (13)0.0108 (13)0.0010 (15)
C4A0.0274 (17)0.036 (2)0.0211 (19)0.0004 (16)0.0073 (13)0.0044 (17)
C4B0.0214 (16)0.033 (2)0.0253 (19)0.0028 (15)0.0072 (13)0.0028 (16)
C5A0.0346 (19)0.036 (2)0.024 (2)0.0059 (17)0.0110 (14)0.0002 (17)
C5B0.0350 (19)0.038 (2)0.0205 (19)0.0004 (17)0.0086 (14)0.0025 (17)
C6A0.0167 (15)0.021 (2)0.0293 (19)0.0016 (13)0.0050 (13)0.0051 (15)
C6B0.0221 (15)0.0202 (19)0.0221 (18)0.0007 (13)0.0092 (13)0.0026 (15)
C7A0.0241 (17)0.025 (2)0.028 (2)0.0026 (14)0.0040 (13)0.0031 (16)
C7B0.0199 (15)0.029 (2)0.0250 (19)0.0001 (14)0.0076 (13)0.0012 (16)
C8A0.039 (2)0.033 (2)0.032 (2)0.0036 (17)0.0014 (16)0.0065 (18)
C8B0.0295 (18)0.032 (2)0.0235 (19)0.0010 (15)0.0101 (14)0.0029 (16)
C9A0.029 (2)0.040 (3)0.046 (3)0.0070 (17)0.0118 (17)0.013 (2)
C9B0.0238 (17)0.033 (2)0.028 (2)0.0011 (15)0.0036 (14)0.0042 (17)
C10A0.0164 (17)0.029 (2)0.074 (3)0.0035 (16)0.0008 (17)0.002 (2)
C10B0.0207 (16)0.027 (2)0.038 (2)0.0002 (14)0.0098 (14)0.0005 (17)
C11A0.0204 (17)0.021 (2)0.054 (2)0.0016 (14)0.0150 (15)0.0014 (18)
C11B0.0263 (17)0.018 (2)0.0295 (19)0.0005 (13)0.0144 (14)0.0016 (15)
N1A0.0258 (15)0.030 (2)0.0301 (17)0.0037 (12)0.0130 (12)0.0059 (14)
N1B0.0264 (15)0.031 (2)0.0270 (17)0.0017 (13)0.0129 (12)0.0026 (14)
N3A0.0187 (13)0.0319 (18)0.0231 (15)0.0006 (12)0.0067 (10)0.0005 (13)
N3B0.0198 (13)0.0273 (18)0.0213 (15)0.0000 (12)0.0078 (10)0.0008 (13)
N10.0270 (15)0.0261 (18)0.0360 (18)0.0025 (13)0.0185 (13)0.0038 (14)
C10.0290 (18)0.021 (2)0.0274 (19)0.0037 (14)0.0171 (14)0.0025 (15)
S10.0239 (4)0.0340 (6)0.0324 (5)0.0037 (4)0.0109 (3)0.0099 (4)
N20.0221 (14)0.037 (2)0.0411 (19)0.0026 (13)0.0156 (13)0.0092 (15)
C20.0250 (17)0.026 (2)0.034 (2)0.0021 (15)0.0168 (15)0.0055 (16)
S20.0217 (4)0.0442 (7)0.0399 (6)0.0005 (4)0.0058 (4)0.0176 (5)
Geometric parameters (Å, º) top
Co—N21.953 (3)C7A—C8A1.381 (4)
Co—N11.962 (3)C7A—H7A0.9300
Co—N3A2.015 (3)C7B—C8B1.377 (4)
Co—N3B2.019 (3)C7B—H7B0.9300
C2A—N3A1.334 (4)C8A—C9A1.376 (5)
C2A—N1A1.347 (4)C8A—H8A0.9300
C2A—C6A1.450 (4)C8B—C9B1.393 (4)
C2B—N3B1.335 (4)C8B—H8B0.9300
C2B—N1B1.361 (4)C9A—C10A1.382 (6)
C2B—C6B1.462 (4)C9A—H9A0.9300
C4A—C5A1.355 (5)C9B—C10B1.378 (4)
C4A—N3A1.381 (4)C9B—H9B0.9300
C4A—H4A0.9300C10A—C11A1.381 (5)
C4B—C5B1.350 (4)C10A—H10A0.9300
C4B—N3B1.379 (4)C10B—C11B1.380 (4)
C4B—H4B0.9300C10B—H10B0.9300
C5A—N1A1.370 (4)C11A—H11A0.9300
C5A—H5A0.9300C11B—H11B0.9300
C5B—N1B1.368 (4)N1A—H1A0.851 (10)
C5B—H5B0.9300N1B—H1B0.84 (4)
C6A—C7A1.382 (5)N1—C11.158 (4)
C6A—C11A1.412 (4)C1—S11.638 (3)
C6B—C7B1.388 (4)N2—C21.158 (4)
C6B—C11B1.395 (4)C2—S21.631 (3)
N2—Co—N1121.15 (13)C7A—C8A—H8A120.0
N2—Co—N3A102.35 (12)C7B—C8B—C9B120.7 (3)
N1—Co—N3A103.56 (11)C7B—C8B—H8B119.7
N2—Co—N3B103.78 (11)C9B—C8B—H8B119.7
N1—Co—N3B104.25 (11)C8A—C9A—C10A120.0 (4)
N3A—Co—N3B123.31 (12)C8A—C9A—H9A120.0
N3A—C2A—N1A109.3 (3)C10A—C9A—H9A120.0
N3A—C2A—C6A126.6 (3)C10B—C9B—C8B119.5 (3)
N1A—C2A—C6A124.1 (3)C10B—C9B—H9B120.3
N3B—C2B—N1B109.2 (3)C8B—C9B—H9B120.3
N3B—C2B—C6B127.5 (3)C11A—C10A—C9A120.8 (3)
N1B—C2B—C6B123.3 (3)C11A—C10A—H10A119.6
C5A—C4A—N3A109.0 (3)C9A—C10A—H10A119.6
C5A—C4A—H4A125.5C9B—C10B—C11B120.1 (3)
N3A—C4A—H4A125.5C9B—C10B—H10B119.9
C5B—C4B—N3B109.8 (3)C11B—C10B—H10B119.9
C5B—C4B—H4B125.1C10A—C11A—C6A119.2 (4)
N3B—C4B—H4B125.1C10A—C11A—H11A120.4
C4A—C5A—N1A106.2 (3)C6A—C11A—H11A120.4
C4A—C5A—H5A126.9C10B—C11B—C6B120.5 (3)
N1A—C5A—H5A126.9C10B—C11B—H11B119.7
C4B—C5B—N1B106.1 (3)C6B—C11B—H11B119.7
C4B—C5B—H5B126.9C2A—N1A—C5A108.6 (3)
N1B—C5B—H5B126.9C2A—N1A—H1A126 (2)
C7A—C6A—C11A119.1 (3)C5A—N1A—H1A125 (2)
C7A—C6A—C2A120.4 (3)C2B—N1B—C5B108.4 (3)
C11A—C6A—C2A120.3 (3)C2B—N1B—H1B122 (2)
C7B—C6B—C11B119.2 (3)C5B—N1B—H1B130 (2)
C7B—C6B—C2B120.4 (3)C2A—N3A—C4A106.8 (3)
C11B—C6B—C2B120.4 (3)C2A—N3A—Co130.2 (2)
C8A—C7A—C6A120.9 (3)C4A—N3A—Co121.6 (2)
C8A—C7A—H7A119.6C2B—N3B—C4B106.4 (3)
C6A—C7A—H7A119.6C2B—N3B—Co131.4 (2)
C8B—C7B—C6B119.9 (3)C4B—N3B—Co121.4 (2)
C8B—C7B—H7B120.0C1—N1—Co172.1 (3)
C6B—C7B—H7B120.0N1—C1—S1178.7 (3)
C9A—C8A—C7A119.9 (4)C2—N2—Co172.0 (3)
C9A—C8A—H8A120.0N2—C2—S2179.0 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1A—H1A···S2i0.85 (3)2.51 (3)3.355 (3)171 (3)
N1B—H1B···S1ii0.84 (4)2.61 (4)3.451 (3)173 (3)
Symmetry codes: (i) x1/2, y+1, z; (ii) x+1/2, y+1, z.
(5) top
Crystal data top
C38H37CoN9O·2(I)Dx = 1.626 Mg m3
Mr = 948.49Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pnn2Cell parameters from 3415 reflections
a = 11.3550 (12) Åθ = 3.2–28.7°
b = 12.680 (3) ŵ = 2.08 mm1
c = 13.4516 (14) ÅT = 100 K
V = 1936.8 (5) Å3Prism, red
Z = 20.20 × 0.11 × 0.10 mm
F(000) = 938
Data collection top
Oxford Diffraction SuperNova with Atlas CCD detector
diffractometer
3201 independent reflections
Radiation source: SuperNova (Mo) X-ray Source3101 reflections with I > 2σ(I)
Detector resolution: 10.4223 pixels mm-1Rint = 0.033
ω scansθmax = 27.0°, θmin = 3.2°
Absorption correction: multi-scan
CrysAlisPro 1.171.38.43 (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 1014
Tmin = 0.859, Tmax = 1.000k = 916
6159 measured reflectionsl = 1615
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.027H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.065 w = 1/[σ2(Fo2) + (0.0352P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max = 0.001
3201 reflectionsΔρmax = 0.72 e Å3
251 parametersΔρmin = 0.68 e Å3
16 restraintsAbsolute structure: Flack x determined using 964 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259).
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.01 (2)
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Co0.50000.50000.54738 (7)0.0145 (2)
I0.52089 (2)0.68918 (2)0.88794 (3)0.02375 (10)
C2A0.3291 (4)0.6733 (4)0.4875 (4)0.0194 (10)
H2A0.29670.62760.44090.023*
C2B0.7337 (4)0.6137 (4)0.4862 (4)0.0198 (10)
H2B0.71000.62260.42060.024*
C4A0.4361 (4)0.7380 (4)0.6031 (3)0.0180 (9)
H4A0.49420.74430.65150.022*
C4B0.7356 (4)0.5735 (4)0.6418 (3)0.0188 (9)
H4B0.71180.54800.70340.023*
C5A0.3564 (4)0.8138 (4)0.5806 (4)0.0186 (10)
C5B0.8416 (4)0.6185 (4)0.6228 (3)0.0180 (10)
C6A0.3348 (4)0.9197 (4)0.6201 (4)0.0203 (10)
C6B0.9423 (4)0.6363 (4)0.6870 (3)0.0193 (10)
C7A0.2883 (4)0.9995 (4)0.5620 (4)0.0280 (12)
H7A0.26960.98580.49590.034*
C7B1.0549 (4)0.6521 (5)0.6494 (4)0.0268 (11)
H7B1.06660.65460.58110.032*
C8A0.2689 (5)1.0991 (4)0.6000 (4)0.0334 (13)
H8A0.23731.15180.56000.040*
C8B1.1496 (4)0.6640 (5)0.7132 (4)0.0291 (12)
H8B1.22500.67260.68730.035*
C9A0.2971 (4)1.1200 (4)0.6990 (4)0.0298 (12)
H9A0.28491.18690.72540.036*
C9B1.1331 (4)0.6633 (5)0.8147 (4)0.0298 (12)
H9B1.19670.67330.85730.036*
C10A0.3432 (4)1.0411 (5)0.7571 (4)0.0296 (12)
H10A0.36221.05520.82300.035*
C10B1.0223 (4)0.6479 (6)0.8525 (5)0.0403 (17)
H10B1.01120.64550.92090.048*
C11A0.3616 (4)0.9410 (4)0.7195 (4)0.0255 (11)
H11A0.39180.88810.76010.031*
C11B0.9274 (4)0.6357 (5)0.7897 (4)0.0343 (14)
H11B0.85240.62700.81620.041*
N1A0.2893 (3)0.7714 (3)0.5050 (3)0.0208 (8)
H1A0.229 (4)0.798 (4)0.476 (4)0.031*
N1B0.8393 (3)0.6425 (3)0.5223 (3)0.0196 (8)
H1B0.896 (3)0.674 (4)0.493 (4)0.029*
N3A0.4192 (3)0.6500 (3)0.5445 (3)0.0174 (8)
N3B0.6680 (3)0.5710 (3)0.5566 (3)0.0175 (8)
O10.50000.50000.7070 (4)0.0183 (10)
H10.498 (5)0.552 (3)0.744 (4)0.027*
N10.50000.50000.3865 (6)0.0240 (12)
C120.506 (2)0.5201 (10)0.3025 (7)0.020 (4)0.5
C130.5101 (13)0.5390 (14)0.1980 (10)0.046 (4)0.5
H13A0.59070.54050.17640.069*0.5
H13B0.47360.60550.18350.069*0.5
H13C0.46900.48370.16370.069*0.5
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co0.0139 (3)0.0158 (5)0.0137 (4)0.0006 (4)0.0000.000
I0.02090 (14)0.03002 (19)0.02032 (16)0.00471 (11)0.00410 (17)0.00928 (17)
C2A0.019 (2)0.020 (2)0.020 (2)0.001 (2)0.0031 (18)0.001 (2)
C2B0.018 (2)0.020 (2)0.021 (2)0.001 (2)0.0017 (17)0.001 (2)
C4A0.0156 (18)0.022 (2)0.017 (2)0.002 (2)0.0007 (17)0.001 (2)
C4B0.0167 (19)0.023 (2)0.016 (2)0.002 (2)0.0013 (16)0.001 (2)
C5A0.0149 (19)0.022 (2)0.019 (2)0.0009 (19)0.0020 (17)0.0035 (19)
C5B0.0141 (19)0.018 (2)0.022 (2)0.000 (2)0.0014 (18)0.001 (2)
C6A0.0147 (19)0.020 (2)0.026 (3)0.003 (2)0.0022 (18)0.000 (2)
C6B0.0138 (18)0.022 (2)0.022 (2)0.003 (2)0.0004 (18)0.002 (2)
C7A0.034 (2)0.023 (3)0.026 (3)0.005 (2)0.003 (2)0.003 (2)
C7B0.020 (2)0.034 (3)0.026 (3)0.004 (2)0.003 (2)0.006 (2)
C8A0.038 (3)0.023 (3)0.039 (3)0.007 (3)0.008 (3)0.007 (3)
C8B0.016 (2)0.039 (3)0.032 (3)0.006 (2)0.001 (2)0.010 (3)
C9A0.026 (2)0.021 (3)0.042 (3)0.001 (2)0.010 (2)0.007 (3)
C9B0.020 (2)0.038 (3)0.031 (3)0.001 (2)0.006 (2)0.005 (3)
C10A0.020 (2)0.034 (3)0.035 (3)0.001 (2)0.002 (2)0.007 (3)
C10B0.023 (3)0.078 (5)0.021 (3)0.003 (3)0.0000 (19)0.014 (3)
C11A0.019 (2)0.028 (3)0.030 (3)0.001 (2)0.001 (2)0.001 (2)
C11B0.017 (2)0.062 (4)0.025 (3)0.003 (3)0.005 (2)0.008 (3)
N1A0.0156 (17)0.025 (2)0.021 (2)0.0019 (18)0.0049 (15)0.0039 (19)
N1B0.0159 (16)0.024 (2)0.0185 (19)0.0032 (17)0.0018 (14)0.0021 (18)
N3A0.0147 (14)0.0175 (19)0.0200 (19)0.0017 (16)0.0002 (15)0.0026 (17)
N3B0.0139 (14)0.021 (2)0.0178 (18)0.0008 (16)0.0013 (14)0.0009 (18)
O10.025 (2)0.015 (3)0.015 (3)0.004 (2)0.0000.000
N10.023 (2)0.028 (3)0.021 (3)0.001 (2)0.0000.000
C120.014 (5)0.020 (11)0.024 (5)0.001 (9)0.003 (5)0.002 (4)
C130.030 (5)0.068 (10)0.039 (7)0.015 (7)0.001 (5)0.004 (7)
Geometric parameters (Å, º) top
Co—N3Ai2.112 (4)C7B—C8B1.384 (7)
Co—N3A2.113 (4)C7B—H7B0.9300
Co—N3B2.113 (3)C8A—C9A1.395 (8)
Co—N3Bi2.113 (3)C8A—H8A0.9300
Co—O12.148 (5)C8B—C9B1.379 (7)
Co—N12.163 (9)C8B—H8B0.9300
C2A—N3A1.312 (6)C9A—C10A1.373 (8)
C2A—N1A1.344 (6)C9A—H9A0.9300
C2A—H2A0.9300C9B—C10B1.371 (7)
C2B—N3B1.322 (6)C9B—H9B0.9300
C2B—N1B1.344 (6)C10A—C11A1.383 (8)
C2B—H2B0.9300C10A—H10A0.9300
C4A—C5A1.355 (6)C10B—C11B1.379 (7)
C4A—N3A1.378 (6)C10B—H10B0.9300
C4A—H4A0.9300C11A—H11A0.9300
C4B—C5B1.356 (6)C11B—H11B0.9300
C4B—N3B1.379 (5)N1A—H1A0.85 (2)
C4B—H4B0.9300N1B—H1B0.853 (13)
C5A—N1A1.379 (6)O1—H10.829 (13)
C5A—C6A1.465 (6)N1—C12i1.161 (12)
C5B—N1B1.386 (6)N1—C121.161 (12)
C5B—C6B1.451 (6)C12—C12i0.53 (2)
C6A—C7A1.383 (7)C12—C131.427 (16)
C6A—C11A1.397 (7)C12—C13i1.603 (17)
C6B—C7B1.389 (6)C13—H13A0.9600
C6B—C11B1.391 (7)C13—H13B0.9600
C7A—C8A1.380 (7)C13—H13C0.9600
C7A—H7A0.9300
N3Ai—Co—N3A177.9 (2)C9B—C8B—C7B120.5 (5)
N3Ai—Co—N3B89.57 (13)C9B—C8B—H8B119.8
N3A—Co—N3B90.55 (13)C7B—C8B—H8B119.8
N3Ai—Co—N3Bi90.55 (13)C10A—C9A—C8A119.5 (5)
N3A—Co—N3Bi89.57 (13)C10A—C9A—H9A120.3
N3B—Co—N3Bi173.2 (2)C8A—C9A—H9A120.3
N3Ai—Co—O191.03 (11)C10B—C9B—C8B119.5 (5)
N3A—Co—O191.03 (11)C10B—C9B—H9B120.2
N3B—Co—O186.62 (11)C8B—C9B—H9B120.2
N3Bi—Co—O186.62 (11)C9A—C10A—C11A121.2 (5)
N3Ai—Co—N188.97 (11)C9A—C10A—H10A119.4
N3A—Co—N188.97 (11)C11A—C10A—H10A119.4
N3B—Co—N193.38 (11)C9B—C10B—C11B120.4 (6)
N3Bi—Co—N193.38 (11)C9B—C10B—H10B119.8
O1—Co—N1180.0C11B—C10B—H10B119.8
N3A—C2A—N1A111.6 (4)C10A—C11A—C6A119.7 (5)
N3A—C2A—H2A124.2C10A—C11A—H11A120.2
N1A—C2A—H2A124.2C6A—C11A—H11A120.2
N3B—C2B—N1B110.9 (4)C10B—C11B—C6B120.8 (5)
N3B—C2B—H2B124.6C10B—C11B—H11B119.6
N1B—C2B—H2B124.6C6B—C11B—H11B119.6
C5A—C4A—N3A110.7 (4)C2A—N1A—C5A107.7 (4)
C5A—C4A—H4A124.6C2A—N1A—H1A123 (4)
N3A—C4A—H4A124.6C5A—N1A—H1A129 (4)
C5B—C4B—N3B110.3 (4)C2B—N1B—C5B108.0 (4)
C5B—C4B—H4B124.8C2B—N1B—H1B130 (4)
N3B—C4B—H4B124.8C5B—N1B—H1B122 (4)
C4A—C5A—N1A104.9 (4)C2A—N3A—C4A105.1 (4)
C4A—C5A—C6A133.0 (5)C2A—N3A—Co123.5 (3)
N1A—C5A—C6A122.1 (4)C4A—N3A—Co131.1 (3)
C4B—C5B—N1B105.0 (4)C2B—N3B—C4B105.8 (4)
C4B—C5B—C6B130.8 (4)C2B—N3B—Co129.9 (3)
N1B—C5B—C6B124.1 (4)C4B—N3B—Co124.1 (3)
C7A—C6A—C11A118.8 (5)Co—O1—H1127 (5)
C7A—C6A—C5A122.0 (5)C12i—N1—Co166.9 (6)
C11A—C6A—C5A119.2 (5)C12—N1—Co166.9 (6)
C7B—C6B—C11B118.3 (4)C12i—C12—N176.9 (6)
C7B—C6B—C5B122.1 (4)C12i—C12—C1399.9 (8)
C11B—C6B—C5B119.6 (4)N1—C12—C13176.7 (13)
C8A—C7A—C6A121.4 (6)C12i—C12—C13i61.3 (7)
C8A—C7A—H7A119.3N1—C12—C13i138.2 (11)
C6A—C7A—H7A119.3C12—C13—H13A109.5
C8B—C7B—C6B120.4 (5)C12—C13—H13B109.5
C8B—C7B—H7B119.8H13A—C13—H13B109.5
C6B—C7B—H7B119.8C12—C13—H13C109.5
C7A—C8A—C9A119.4 (5)H13A—C13—H13C109.5
C7A—C8A—H8A120.3H13B—C13—H13C109.5
C9A—C8A—H8A120.3
Symmetry code: (i) x+1, y+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1A—H1A···Iii0.86 (5)2.65 (5)3.467 (4)160 (4)
N1B—H1B···Iii0.85 (4)2.65 (5)3.475 (4)163 (4)
O1—H1···I0.83 (5)2.62 (5)3.426 (4)167 (4)
Symmetry code: (ii) x1/2, y+3/2, z1/2.
(6) top
Crystal data top
C38H37CoN9O·2(NO3)Dx = 1.403 Mg m3
Mr = 818.71Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pnn2Cell parameters from 3240 reflections
a = 11.3655 (6) Åθ = 4.4–28.9°
b = 12.5153 (7) ŵ = 0.51 mm1
c = 13.6247 (6) ÅT = 100 K
V = 1938.01 (17) Å3Prism, purple
Z = 20.20 × 0.12 × 0.12 mm
F(000) = 850
Data collection top
Oxford Diffraction SuperNova with Atlas CCD detector
diffractometer
3470 independent reflections
Radiation source: SuperNova (Mo) X-ray Source3354 reflections with I > 2σ(I)
Detector resolution: 10.4223 pixels mm-1Rint = 0.026
ω scansθmax = 27.0°, θmin = 3.0°
Absorption correction: multi-scan
CrysAlisPro 1.171.38.43 (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 814
Tmin = 0.853, Tmax = 1.000k = 1514
6658 measured reflectionsl = 1717
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.027 w = 1/[σ2(Fo2) + (0.033P)2 + 0.7309P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.072(Δ/σ)max = 0.001
S = 1.05Δρmax = 0.32 e Å3
3470 reflectionsΔρmin = 0.23 e Å3
279 parametersAbsolute structure: Refined as an inversion twin.
10 restraintsAbsolute structure parameter: 0.178 (17)
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 inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Co0.50000.00000.29392 (4)0.01557 (12)
N1A0.1533 (2)0.13514 (19)0.32243 (16)0.0197 (5)
H1A0.102 (3)0.163 (3)0.359 (2)0.029*
C2A0.2608 (3)0.1076 (2)0.3574 (2)0.0221 (6)
H2A0.28240.11160.42310.026*
N3A0.33061 (17)0.07466 (15)0.28666 (18)0.0190 (4)
C4A0.2646 (2)0.0826 (2)0.2022 (2)0.0213 (6)
H4A0.29190.06500.13990.026*
C5A0.1546 (2)0.1193 (2)0.2215 (2)0.0194 (5)
C6A0.0544 (2)0.1385 (2)0.1565 (2)0.0208 (5)
C7A0.0603 (3)0.1499 (3)0.1911 (2)0.0340 (7)
H7A0.07470.14800.25820.041*
C8A0.1534 (3)0.1640 (3)0.1262 (3)0.0344 (7)
H8A0.22940.17220.15030.041*
C9A0.1337 (3)0.1660 (3)0.0267 (3)0.0317 (7)
H9A0.19600.17550.01670.038*
C10A0.0210 (3)0.1539 (4)0.0079 (2)0.0461 (10)
H10A0.00730.15490.07520.055*
C11A0.0718 (3)0.1402 (3)0.0558 (2)0.0383 (8)
H11A0.14750.13200.03080.046*
N1B0.7095 (2)0.27619 (19)0.33912 (18)0.0224 (5)
H1B0.766 (2)0.303 (3)0.370 (2)0.034*
C2B0.6716 (2)0.1766 (2)0.3566 (2)0.0222 (6)
H2B0.70320.13150.40410.027*
N3B0.58371 (17)0.15045 (15)0.29784 (19)0.0182 (4)
C4B0.5650 (2)0.2393 (2)0.2396 (2)0.0196 (5)
H4B0.50770.24470.19110.023*
C5B0.6429 (2)0.3178 (2)0.26387 (19)0.0192 (5)
C6B0.6633 (2)0.4243 (2)0.2216 (2)0.0227 (5)
C7B0.7044 (3)0.5090 (2)0.2783 (2)0.0317 (7)
H7B0.71980.49880.34470.038*
C8B0.7224 (3)0.6087 (2)0.2360 (3)0.0399 (8)
H8B0.75010.66490.27420.048*
C9B0.6995 (3)0.6247 (3)0.1378 (3)0.0355 (8)
H9B0.71160.69150.10980.043*
C10B0.6586 (3)0.5410 (3)0.0809 (3)0.0341 (7)
H10B0.64240.55190.01470.041*
C11B0.6416 (3)0.4409 (2)0.1225 (2)0.0280 (6)
H11B0.61550.38460.08370.034*
O10.50000.00000.1352 (3)0.0223 (8)
H10.480 (3)0.050 (2)0.100 (3)0.034*
N10.50000.00000.4543 (3)0.0248 (10)
C120.496 (2)0.0187 (9)0.5362 (4)0.027 (3)0.5
C130.4917 (9)0.0380 (7)0.6421 (5)0.051 (3)0.5
H13A0.41730.01400.66730.076*0.5
H13B0.50050.11300.65470.076*0.5
H13C0.55410.00050.67370.076*0.5
N20.4680 (2)0.1961 (2)0.03418 (18)0.0248 (5)
O20.56214 (19)0.1728 (2)0.00745 (17)0.0369 (5)
O30.45595 (19)0.28495 (17)0.07561 (16)0.0319 (5)
O40.38331 (19)0.13228 (18)0.03354 (19)0.0400 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co0.0135 (2)0.0151 (2)0.0180 (2)0.00016 (18)0.0000.000
N1A0.0153 (10)0.0233 (11)0.0204 (11)0.0044 (9)0.0015 (9)0.0025 (9)
C2A0.0223 (13)0.0236 (14)0.0202 (12)0.0010 (11)0.0004 (12)0.0015 (10)
N3A0.0167 (9)0.0180 (9)0.0222 (10)0.0003 (8)0.0009 (12)0.0007 (10)
C4A0.0170 (13)0.0256 (14)0.0215 (12)0.0008 (11)0.0000 (12)0.0001 (10)
C5A0.0187 (13)0.0180 (12)0.0215 (12)0.0002 (10)0.0000 (12)0.0010 (11)
C6A0.0160 (13)0.0200 (13)0.0263 (13)0.0004 (11)0.0007 (12)0.0011 (10)
C7A0.0214 (15)0.051 (2)0.0291 (15)0.0078 (15)0.0011 (13)0.0082 (14)
C8A0.0199 (14)0.0449 (18)0.0385 (16)0.0089 (14)0.0013 (14)0.0102 (15)
C9A0.0209 (14)0.0388 (17)0.0354 (15)0.0005 (13)0.0076 (14)0.0069 (14)
C10A0.0256 (15)0.087 (3)0.0260 (16)0.0017 (19)0.0013 (15)0.0146 (18)
C11A0.0170 (14)0.070 (2)0.0283 (15)0.0013 (15)0.0053 (14)0.0074 (16)
N1B0.0182 (10)0.0216 (11)0.0274 (11)0.0035 (9)0.0036 (10)0.0031 (9)
C2B0.0201 (13)0.0199 (13)0.0268 (13)0.0013 (11)0.0028 (12)0.0018 (11)
N3B0.0147 (9)0.0180 (9)0.0217 (10)0.0007 (8)0.0015 (11)0.0011 (10)
C4B0.0173 (11)0.0187 (12)0.0227 (12)0.0018 (10)0.0003 (11)0.0005 (10)
C5B0.0164 (12)0.0186 (12)0.0225 (12)0.0013 (10)0.0017 (11)0.0006 (10)
C6B0.0191 (12)0.0172 (12)0.0317 (13)0.0001 (10)0.0067 (13)0.0008 (11)
C7B0.0402 (16)0.0226 (13)0.0322 (19)0.0054 (12)0.0054 (15)0.0030 (12)
C8B0.048 (2)0.0204 (14)0.051 (2)0.0072 (14)0.0115 (19)0.0090 (14)
C9B0.0349 (17)0.0237 (15)0.0480 (19)0.0002 (13)0.0133 (16)0.0089 (13)
C10B0.0307 (16)0.0326 (16)0.0391 (17)0.0001 (13)0.0063 (15)0.0101 (14)
C11B0.0247 (14)0.0248 (14)0.0345 (15)0.0016 (12)0.0018 (14)0.0025 (12)
O10.0227 (18)0.024 (2)0.0201 (17)0.0036 (12)0.0000.000
N10.024 (2)0.028 (2)0.022 (2)0.0036 (14)0.0000.000
C120.021 (4)0.032 (10)0.027 (2)0.010 (9)0.001 (4)0.003 (3)
C130.044 (4)0.083 (7)0.024 (3)0.020 (6)0.002 (4)0.009 (3)
N20.0223 (11)0.0323 (13)0.0198 (10)0.0005 (11)0.0003 (11)0.0024 (10)
O20.0235 (11)0.0487 (14)0.0384 (12)0.0037 (10)0.0136 (10)0.0098 (10)
O30.0290 (10)0.0324 (12)0.0344 (11)0.0022 (9)0.0029 (10)0.0121 (10)
O40.0254 (10)0.0401 (13)0.0543 (14)0.0111 (10)0.0127 (12)0.0207 (11)
Geometric parameters (Å, º) top
Co—N3Bi2.1103 (19)N1B—H1B0.84 (2)
Co—N3B2.1103 (19)C2B—N3B1.321 (3)
Co—N3A2.1423 (19)C2B—H2B0.9300
Co—N3Ai2.1423 (19)N3B—C4B1.382 (3)
Co—O12.163 (3)C4B—C5B1.363 (4)
Co—N12.186 (4)C4B—H4B0.9300
N1A—C2A1.356 (4)C5B—C6B1.471 (4)
N1A—C5A1.390 (4)C6B—C11B1.388 (4)
N1A—H1A0.84 (2)C6B—C7B1.393 (4)
C2A—N3A1.315 (4)C7B—C8B1.390 (4)
C2A—H2A0.9300C7B—H7B0.9300
N3A—C4A1.378 (4)C8B—C9B1.378 (5)
C4A—C5A1.358 (4)C8B—H8B0.9300
C4A—H4A0.9300C9B—C10B1.383 (5)
C5A—C6A1.462 (4)C9B—H9B0.9300
C6A—C11A1.386 (4)C10B—C11B1.389 (4)
C6A—C7A1.394 (4)C10B—H10B0.9300
C7A—C8A1.390 (5)C11B—H11B0.9300
C7A—H7A0.9300O1—H10.82 (2)
C8A—C9A1.374 (5)N1—C121.140 (8)
C8A—H8A0.9300C12—C131.464 (9)
C9A—C10A1.373 (4)C13—H13A0.9600
C9A—H9A0.9300C13—H13B0.9600
C10A—C11A1.377 (5)C13—H13C0.9600
C10A—H10A0.9300N2—O21.246 (3)
C11A—H11A0.9300N2—O41.251 (3)
N1B—C2B1.340 (4)N2—O31.254 (3)
N1B—C5B1.377 (3)
N3Bi—Co—N3B177.10 (15)C6A—C11A—H11A119.5
N3Bi—Co—N3A89.15 (7)C2B—N1B—C5B107.9 (2)
N3B—Co—N3A90.99 (7)C2B—N1B—H1B122 (2)
N3Bi—Co—N3Ai90.99 (7)C5B—N1B—H1B130 (2)
N3B—Co—N3Ai89.15 (7)N3B—C2B—N1B111.4 (2)
N3A—Co—N3Ai174.71 (14)N3B—C2B—H2B124.3
N3Bi—Co—O191.45 (7)N1B—C2B—H2B124.3
N3B—Co—O191.45 (7)C2B—N3B—C4B105.4 (2)
N3A—Co—O187.35 (7)C2B—N3B—Co125.24 (18)
N3Ai—Co—O187.35 (7)C4B—N3B—Co129.32 (18)
N3Bi—Co—N188.55 (7)C5B—C4B—N3B109.9 (2)
N3B—Co—N188.55 (7)C5B—C4B—H4B125.0
N3A—Co—N192.65 (7)N3B—C4B—H4B125.0
N3Ai—Co—N192.65 (7)C4B—C5B—N1B105.4 (2)
O1—Co—N1180.0C4B—C5B—C6B131.4 (3)
C2A—N1A—C5A107.6 (2)N1B—C5B—C6B123.2 (2)
C2A—N1A—H1A121 (2)C11B—C6B—C7B119.0 (3)
C5A—N1A—H1A131 (2)C11B—C6B—C5B119.3 (3)
N3A—C2A—N1A111.5 (2)C7B—C6B—C5B121.7 (3)
N3A—C2A—H2A124.3C8B—C7B—C6B120.1 (3)
N1A—C2A—H2A124.3C8B—C7B—H7B119.9
C2A—N3A—C4A105.1 (2)C6B—C7B—H7B119.9
C2A—N3A—Co130.2 (2)C9B—C8B—C7B120.4 (3)
C4A—N3A—Co124.01 (18)C9B—C8B—H8B119.8
C5A—C4A—N3A111.4 (2)C7B—C8B—H8B119.8
C5A—C4A—H4A124.3C8B—C9B—C10B119.9 (3)
N3A—C4A—H4A124.3C8B—C9B—H9B120.1
C4A—C5A—N1A104.5 (2)C10B—C9B—H9B120.1
C4A—C5A—C6A131.0 (3)C9B—C10B—C11B120.0 (3)
N1A—C5A—C6A124.6 (3)C9B—C10B—H10B120.0
C11A—C6A—C7A117.8 (3)C11B—C10B—H10B120.0
C11A—C6A—C5A119.4 (3)C6B—C11B—C10B120.5 (3)
C7A—C6A—C5A122.7 (3)C6B—C11B—H11B119.7
C8A—C7A—C6A120.7 (3)C10B—C11B—H11B119.7
C8A—C7A—H7A119.7Co—O1—H1125 (3)
C6A—C7A—H7A119.7C12—N1—Co168.0 (6)
C9A—C8A—C7A120.3 (3)N1—C12—C13177.6 (10)
C9A—C8A—H8A119.8C12—C13—H13A109.5
C7A—C8A—H8A119.8C12—C13—H13B109.5
C10A—C9A—C8A119.3 (3)H13A—C13—H13B109.5
C10A—C9A—H9A120.4C12—C13—H13C109.5
C8A—C9A—H9A120.4H13A—C13—H13C109.5
C9A—C10A—C11A120.8 (3)H13B—C13—H13C109.5
C9A—C10A—H10A119.6O2—N2—O4120.5 (2)
C11A—C10A—H10A119.6O2—N2—O3120.4 (2)
C10A—C11A—C6A121.1 (3)O4—N2—O3119.0 (2)
C10A—C11A—H11A119.5
Symmetry code: (i) x+1, y, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1A—H1A···O3ii0.84 (3)2.00 (3)2.821 (3)167 (3)
N1B—H1B···O3iii0.84 (3)2.53 (3)3.127 (3)128 (3)
N1B—H1B···O4iii0.84 (3)2.03 (3)2.868 (3)170 (3)
O1—H1···O2i0.82 (3)2.05 (3)2.865 (3)177 (3)
Symmetry codes: (i) x+1, y, z; (ii) x1/2, y+1/2, z+1/2; (iii) x+1/2, y+1/2, z+1/2.
(7) top
Crystal data top
C38H32CoN10S2·2(CH4O)Z = 1
Mr = 815.87F(000) = 425
Triclinic, P1Dx = 1.320 Mg m3
a = 8.6822 (8) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.4570 (9) ÅCell parameters from 3225 reflections
c = 13.6578 (12) Åθ = 4.3–29.6°
α = 103.023 (8)°µ = 0.57 mm1
β = 95.901 (7)°T = 100 K
γ = 107.217 (8)°Prism, orange
V = 1026.15 (17) Å30.24 × 0.15 × 0.14 mm
Data collection top
Oxford Diffraction SuperNova with Atlas CCD detector
diffractometer
4241 independent reflections
Radiation source: SuperNova (Mo) X-ray Source3549 reflections with I > 2σ(I)
Detector resolution: 10.4223 pixels mm-1Rint = 0.032
ω scansθmax = 26.5°, θmin = 2.8°
Absorption correction: multi-scan
CrysAlisPro 1.171.38.43 (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 1010
Tmin = 0.780, Tmax = 1.000k = 119
8705 measured reflectionsl = 1617
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.039Hydrogen site location: mixed
wR(F2) = 0.093H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.0309P)2 + 0.5771P]
where P = (Fo2 + 2Fc2)/3
4241 reflections(Δ/σ)max < 0.001
260 parametersΔρmax = 0.28 e Å3
3 restraintsΔρmin = 0.38 e Å3
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Co0.50000.00000.00000.01496 (11)
N1A0.8245 (2)0.1512 (2)0.28699 (13)0.0206 (4)
H1A0.9216 (16)0.186 (3)0.3232 (16)0.031*
C2A0.7864 (2)0.1130 (2)0.18446 (15)0.0186 (4)
H2A0.86300.11820.14140.022*
N3A0.62656 (19)0.06713 (18)0.15296 (12)0.0175 (4)
C4A0.5598 (2)0.0779 (2)0.24040 (15)0.0190 (4)
H4A0.44830.05300.24180.023*
C5A0.6804 (2)0.1303 (2)0.32429 (15)0.0192 (4)
C6A0.6744 (3)0.1620 (2)0.43391 (16)0.0238 (5)
C7A0.8039 (3)0.1675 (3)0.50515 (17)0.0322 (6)
H7A0.89720.15160.48380.039*
C8A0.7939 (3)0.1967 (3)0.60824 (18)0.0416 (7)
H8A0.88150.20190.65590.050*
C9A0.6552 (3)0.2181 (3)0.64033 (18)0.0413 (7)
H9A0.64930.23750.70940.050*
C10A0.5255 (3)0.2106 (3)0.57024 (18)0.0354 (6)
H10A0.43150.22410.59200.042*
C11A0.5343 (3)0.1830 (3)0.46733 (16)0.0275 (5)
H11A0.44640.17860.42030.033*
N1B0.7994 (2)0.3840 (2)0.08532 (13)0.0202 (4)
H1B0.809 (3)0.4694 (17)0.0993 (18)0.030*
C2B0.6720 (2)0.3065 (2)0.04877 (15)0.0203 (4)
H2B0.58550.34100.03280.024*
N3B0.68554 (19)0.17517 (19)0.03846 (12)0.0179 (4)
C4B0.8302 (2)0.1702 (2)0.07021 (15)0.0185 (4)
H4B0.87240.09040.07120.022*
C5B0.9025 (2)0.2985 (2)0.09994 (14)0.0173 (4)
C6B1.0529 (2)0.3429 (2)0.14259 (14)0.0176 (4)
C7B1.1047 (3)0.4777 (2)0.17281 (17)0.0257 (5)
H7B1.04420.54450.16500.031*
C8B1.2461 (3)0.5135 (2)0.21452 (17)0.0267 (5)
H8B1.27940.60400.23440.032*
C9B1.3368 (2)0.4163 (2)0.22663 (16)0.0237 (5)
H9B1.43120.44050.25470.028*
C10B1.2868 (3)0.2819 (3)0.19674 (19)0.0301 (5)
H10B1.34750.21520.20500.036*
C11B1.1465 (3)0.2465 (3)0.15450 (18)0.0275 (5)
H11B1.11470.15660.13380.033*
N20.63040 (19)0.15390 (19)0.04664 (13)0.0195 (4)
C120.6937 (2)0.2233 (2)0.09897 (15)0.0176 (4)
S0.78707 (7)0.31891 (7)0.17439 (4)0.02719 (15)
C130.2128 (4)0.4090 (3)0.4679 (2)0.0525 (8)
H13A0.16140.40200.52640.079*
H13B0.18680.48450.43890.079*
H13C0.32950.43860.48830.079*
O10.15494 (19)0.2647 (2)0.39439 (13)0.0382 (4)
H10.199 (3)0.274 (4)0.3431 (15)0.057*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co0.01664 (19)0.0152 (2)0.01317 (19)0.00462 (14)0.00512 (15)0.00379 (14)
N1A0.0180 (8)0.0248 (10)0.0176 (9)0.0057 (7)0.0020 (7)0.0050 (7)
C2A0.0191 (9)0.0197 (11)0.0170 (10)0.0062 (8)0.0049 (8)0.0043 (8)
N3A0.0192 (8)0.0168 (9)0.0164 (8)0.0054 (7)0.0055 (7)0.0043 (7)
C4A0.0201 (9)0.0200 (11)0.0181 (10)0.0062 (8)0.0078 (8)0.0061 (8)
C5A0.0220 (10)0.0181 (10)0.0179 (10)0.0065 (8)0.0058 (8)0.0050 (8)
C6A0.0280 (11)0.0214 (11)0.0170 (10)0.0017 (9)0.0042 (9)0.0040 (8)
C7A0.0285 (11)0.0378 (14)0.0229 (11)0.0014 (10)0.0020 (10)0.0078 (10)
C8A0.0446 (15)0.0470 (16)0.0181 (11)0.0040 (12)0.0054 (11)0.0097 (11)
C9A0.0544 (16)0.0383 (15)0.0168 (11)0.0031 (12)0.0103 (12)0.0022 (10)
C10A0.0447 (14)0.0310 (14)0.0252 (12)0.0057 (11)0.0162 (11)0.0022 (10)
C11A0.0323 (11)0.0256 (12)0.0199 (11)0.0049 (9)0.0061 (9)0.0023 (9)
N1B0.0243 (8)0.0172 (9)0.0227 (9)0.0080 (7)0.0101 (7)0.0079 (7)
C2B0.0216 (10)0.0193 (11)0.0200 (10)0.0056 (8)0.0080 (8)0.0045 (8)
N3B0.0180 (8)0.0167 (9)0.0172 (8)0.0036 (7)0.0038 (7)0.0036 (7)
C4B0.0187 (9)0.0186 (10)0.0195 (10)0.0071 (8)0.0047 (8)0.0055 (8)
C5B0.0186 (9)0.0164 (10)0.0145 (9)0.0054 (8)0.0017 (8)0.0008 (8)
C6B0.0168 (9)0.0187 (10)0.0127 (9)0.0023 (8)0.0003 (8)0.0011 (8)
C7B0.0283 (11)0.0198 (11)0.0336 (12)0.0111 (9)0.0151 (10)0.0076 (9)
C8B0.0300 (11)0.0160 (11)0.0341 (12)0.0044 (9)0.0146 (10)0.0074 (9)
C9B0.0196 (10)0.0245 (12)0.0253 (11)0.0045 (8)0.0100 (9)0.0044 (9)
C10B0.0272 (11)0.0315 (13)0.0421 (14)0.0170 (10)0.0159 (10)0.0161 (11)
C11B0.0266 (11)0.0266 (12)0.0367 (13)0.0114 (9)0.0119 (10)0.0170 (10)
N20.0209 (8)0.0192 (9)0.0199 (9)0.0070 (7)0.0060 (7)0.0068 (7)
C120.0140 (9)0.0176 (10)0.0207 (10)0.0018 (8)0.0027 (8)0.0091 (8)
S0.0298 (3)0.0282 (3)0.0332 (3)0.0158 (2)0.0186 (2)0.0128 (2)
C130.0496 (16)0.0419 (17)0.0497 (17)0.0032 (13)0.0053 (14)0.0066 (14)
O10.0300 (9)0.0495 (11)0.0311 (9)0.0059 (8)0.0042 (7)0.0130 (8)
Geometric parameters (Å, º) top
Co—N3Ai2.1194 (16)N1B—C5B1.374 (3)
Co—N3A2.1195 (16)N1B—H1B0.854 (10)
Co—N2i2.1241 (17)C2B—N3B1.318 (3)
Co—N22.1241 (17)C2B—H2B0.9300
Co—N3B2.1452 (16)N3B—C4B1.380 (2)
Co—N3Bi2.1452 (16)C4B—C5B1.362 (3)
N1A—C2A1.344 (3)C4B—H4B0.9300
N1A—C5A1.376 (3)C5B—C6B1.471 (3)
N1A—H1A0.861 (10)C6B—C11B1.385 (3)
C2A—N3A1.318 (2)C6B—C7B1.390 (3)
C2A—H2A0.9300C7B—C8B1.389 (3)
N3A—C4A1.377 (2)C7B—H7B0.9300
C4A—C5A1.358 (3)C8B—C9B1.371 (3)
C4A—H4A0.9300C8B—H8B0.9300
C5A—C6A1.469 (3)C9B—C10B1.384 (3)
C6A—C7A1.390 (3)C9B—H9B0.9300
C6A—C11A1.394 (3)C10B—C11B1.385 (3)
C7A—C8A1.389 (3)C10B—H10B0.9300
C7A—H7A0.9300C11B—H11B0.9300
C8A—C9A1.377 (4)N2—C121.152 (3)
C8A—H8A0.9300C12—S1.650 (2)
C9A—C10A1.375 (4)C13—O11.413 (3)
C9A—H9A0.9300C13—H13A0.9600
C10A—C11A1.385 (3)C13—H13B0.9600
C10A—H10A0.9300C13—H13C0.9600
C11A—H11A0.9300O1—H10.840 (10)
N1B—C2B1.345 (3)
N3Ai—Co—N3A180.0C10A—C11A—C6A120.3 (2)
N3Ai—Co—N2i91.85 (6)C10A—C11A—H11A119.9
N3A—Co—N2i88.15 (6)C6A—C11A—H11A119.9
N3Ai—Co—N288.15 (6)C2B—N1B—C5B108.22 (18)
N3A—Co—N291.85 (6)C2B—N1B—H1B124.0 (16)
N2i—Co—N2180.0C5B—N1B—H1B127.7 (16)
N3Ai—Co—N3B88.63 (6)N3B—C2B—N1B111.28 (18)
N3A—Co—N3B91.37 (6)N3B—C2B—H2B124.4
N2i—Co—N3B91.49 (6)N1B—C2B—H2B124.4
N2—Co—N3B88.51 (6)C2B—N3B—C4B105.14 (17)
N3Ai—Co—N3Bi91.37 (6)C2B—N3B—Co125.05 (13)
N3A—Co—N3Bi88.63 (6)C4B—N3B—Co129.30 (14)
N2i—Co—N3Bi88.51 (6)C5B—C4B—N3B110.55 (18)
N2—Co—N3Bi91.49 (6)C5B—C4B—H4B124.7
N3B—Co—N3Bi180.0N3B—C4B—H4B124.7
C2A—N1A—C5A107.82 (16)C4B—C5B—N1B104.81 (17)
C2A—N1A—H1A126.3 (16)C4B—C5B—C6B130.81 (19)
C5A—N1A—H1A125.9 (16)N1B—C5B—C6B124.34 (18)
N3A—C2A—N1A111.18 (18)C11B—C6B—C7B118.20 (19)
N3A—C2A—H2A124.4C11B—C6B—C5B119.11 (19)
N1A—C2A—H2A124.4C7B—C6B—C5B122.69 (19)
C2A—N3A—C4A105.52 (16)C6B—C7B—C8B120.6 (2)
C2A—N3A—Co127.11 (13)C6B—C7B—H7B119.7
C4A—N3A—Co127.33 (13)C8B—C7B—H7B119.7
C5A—C4A—N3A110.20 (17)C9B—C8B—C7B120.5 (2)
C5A—C4A—H4A124.9C9B—C8B—H8B119.7
N3A—C4A—H4A124.9C7B—C8B—H8B119.7
C4A—C5A—N1A105.28 (17)C8B—C9B—C10B119.50 (19)
C4A—C5A—C6A131.59 (18)C8B—C9B—H9B120.3
N1A—C5A—C6A123.13 (18)C10B—C9B—H9B120.3
C7A—C6A—C11A119.0 (2)C9B—C10B—C11B120.1 (2)
C7A—C6A—C5A121.4 (2)C9B—C10B—H10B120.0
C11A—C6A—C5A119.5 (2)C11B—C10B—H10B120.0
C8A—C7A—C6A120.0 (2)C6B—C11B—C10B121.1 (2)
C8A—C7A—H7A120.0C6B—C11B—H11B119.5
C6A—C7A—H7A120.0C10B—C11B—H11B119.5
C9A—C8A—C7A120.4 (2)C12—N2—Co158.73 (17)
C9A—C8A—H8A119.8N2—C12—S178.69 (19)
C7A—C8A—H8A119.8O1—C13—H13A109.5
C10A—C9A—C8A120.0 (2)O1—C13—H13B109.5
C10A—C9A—H9A120.0H13A—C13—H13B109.5
C8A—C9A—H9A120.0O1—C13—H13C109.5
C9A—C10A—C11A120.2 (2)H13A—C13—H13C109.5
C9A—C10A—H10A119.9H13B—C13—H13C109.5
C11A—C10A—H10A119.9C13—O1—H1108 (2)
Symmetry code: (i) x+1, y, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1A—H1A···O1ii0.86 (2)2.00 (2)2.853 (3)174 (2)
N1B—H1B···Siii0.85 (2)2.49 (2)3.328 (2)167 (2)
O1—H1···Si0.84 (2)2.44 (2)3.224 (2)155 (2)
Symmetry codes: (i) x+1, y, z; (ii) x+1, y, z; (iii) x, y+1, z.
(8) top
Crystal data top
C20H16CoN6S2F(000) = 948
Mr = 463.44Dx = 1.517 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 24.4747 (19) ÅCell parameters from 1570 reflections
b = 5.5932 (5) Åθ = 4.6–29.3°
c = 14.8644 (16) ŵ = 1.07 mm1
β = 94.172 (8)°T = 100 K
V = 2029.4 (3) Å3Prism, blue
Z = 40.15 × 0.09 × 0.09 mm
Data collection top
Oxford Diffraction SuperNova with Atlas CCD detector
diffractometer
2176 independent reflections
Radiation source: SuperNova (Mo) X-ray Source1794 reflections with I > 2σ(I)
Detector resolution: 10.4223 pixels mm-1Rint = 0.030
ω scansθmax = 27.0°, θmin = 3.3°
Absorption correction: multi-scan
CrysAlisPro 1.171.38.43 (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 3024
Tmin = 0.935, Tmax = 1.000k = 57
4333 measured reflectionsl = 1817
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.033Hydrogen site location: mixed
wR(F2) = 0.077H atoms treated by a mixture of independent and constrained refinement
S = 1.02 w = 1/[σ2(Fo2) + (0.0224P)2 + 3.0766P]
where P = (Fo2 + 2Fc2)/3
2176 reflections(Δ/σ)max = 0.001
135 parametersΔρmax = 0.43 e Å3
1 restraintΔρmin = 0.27 e Å3
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Co0.50000.71417 (8)0.75000.01835 (13)
N10.39936 (7)0.2486 (3)0.59807 (12)0.0183 (4)
H10.3954 (10)0.129 (3)0.5626 (14)0.027*
C20.44728 (8)0.3524 (4)0.62177 (14)0.0208 (5)
H20.48010.31410.59740.025*
N30.44203 (7)0.5165 (3)0.68420 (11)0.0183 (4)
C40.38688 (8)0.5172 (4)0.70008 (14)0.0182 (5)
H40.37090.61660.74090.022*
C50.35966 (8)0.3511 (4)0.64724 (13)0.0157 (4)
C60.30160 (8)0.2847 (4)0.63634 (13)0.0150 (4)
C70.28427 (8)0.0706 (4)0.59538 (13)0.0173 (4)
H70.30990.03770.57660.021*
C80.22878 (8)0.0193 (4)0.58257 (13)0.0182 (4)
H80.21750.12340.55510.022*
C90.19019 (8)0.1782 (4)0.61027 (13)0.0173 (4)
H90.15310.14380.60040.021*
C100.20690 (8)0.3885 (4)0.65270 (13)0.0163 (4)
H100.18100.49440.67240.020*
C110.26228 (8)0.4416 (4)0.66587 (13)0.0148 (4)
H110.27330.58310.69460.018*
N20.45765 (7)0.9051 (4)0.83063 (13)0.0243 (4)
C120.43880 (8)1.0272 (4)0.88384 (15)0.0185 (5)
S0.41467 (2)1.20455 (10)0.95819 (4)0.02081 (15)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co0.0102 (2)0.0229 (2)0.0220 (2)0.0000.00118 (15)0.000
N10.0168 (8)0.0183 (10)0.0201 (10)0.0038 (8)0.0032 (7)0.0032 (7)
C20.0146 (10)0.0251 (12)0.0230 (11)0.0059 (9)0.0036 (8)0.0024 (10)
N30.0127 (8)0.0214 (10)0.0207 (9)0.0006 (8)0.0020 (7)0.0004 (8)
C40.0127 (9)0.0234 (12)0.0187 (10)0.0004 (9)0.0027 (8)0.0017 (9)
C50.0146 (9)0.0177 (11)0.0149 (10)0.0043 (9)0.0020 (8)0.0033 (8)
C60.0157 (10)0.0180 (11)0.0112 (10)0.0001 (9)0.0001 (7)0.0025 (8)
C70.0208 (10)0.0153 (11)0.0160 (10)0.0027 (9)0.0020 (8)0.0006 (9)
C80.0239 (11)0.0152 (11)0.0150 (10)0.0029 (9)0.0018 (8)0.0024 (9)
C90.0157 (9)0.0237 (11)0.0121 (10)0.0038 (9)0.0012 (8)0.0023 (9)
C100.0161 (10)0.0200 (11)0.0129 (10)0.0020 (9)0.0014 (8)0.0014 (8)
C110.0162 (9)0.0147 (10)0.0131 (10)0.0009 (8)0.0005 (7)0.0005 (8)
N20.0164 (9)0.0268 (11)0.0296 (11)0.0013 (8)0.0012 (8)0.0043 (9)
C120.0112 (9)0.0191 (11)0.0246 (11)0.0029 (9)0.0028 (8)0.0036 (9)
S0.0190 (3)0.0190 (3)0.0249 (3)0.0007 (2)0.0054 (2)0.0006 (2)
Geometric parameters (Å, º) top
Co—N21.9576 (19)C6—C111.397 (3)
Co—N2i1.9576 (19)C6—C71.395 (3)
Co—N3i1.9974 (18)C7—C81.388 (3)
Co—N31.9974 (18)C7—H70.9300
N1—C21.333 (3)C8—C91.381 (3)
N1—C51.382 (3)C8—H80.9300
N1—H10.852 (10)C9—C101.383 (3)
C2—N31.318 (3)C9—H90.9300
C2—H20.9300C10—C111.388 (3)
N3—C41.387 (2)C10—H100.9300
C4—C51.359 (3)C11—H110.9300
C4—H40.9300N2—C121.165 (3)
C5—C61.466 (3)C12—S1.628 (2)
N2—Co—N2i113.88 (12)C11—C6—C7118.83 (19)
N2—Co—N3i113.01 (7)C11—C6—C5119.36 (19)
N2i—Co—N3i102.29 (7)C7—C6—C5121.80 (19)
N2—Co—N3102.29 (7)C8—C7—C6120.05 (19)
N2i—Co—N3113.02 (7)C8—C7—H7120.0
N3i—Co—N3112.80 (10)C6—C7—H7120.0
C2—N1—C5108.56 (18)C9—C8—C7120.6 (2)
C2—N1—H1124.4 (16)C9—C8—H8119.7
C5—N1—H1126.8 (16)C7—C8—H8119.7
N3—C2—N1111.13 (18)C8—C9—C10119.83 (19)
N3—C2—H2124.4C8—C9—H9120.1
N1—C2—H2124.4C10—C9—H9120.1
C2—N3—C4105.52 (18)C9—C10—C11120.00 (19)
C2—N3—Co128.89 (14)C9—C10—H10120.0
C4—N3—Co125.49 (14)C11—C10—H10120.0
C5—C4—N3109.99 (18)C10—C11—C6120.62 (19)
C5—C4—H4125.0C10—C11—H11119.7
N3—C4—H4125.0C6—C11—H11119.7
C4—C5—N1104.79 (17)C12—N2—Co171.38 (17)
C4—C5—C6131.85 (19)N2—C12—S177.68 (19)
N1—C5—C6123.34 (19)
Symmetry code: (i) x+1, y, z+3/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···Sii0.85 (2)2.49 (2)3.317 (2)162 (2)
Symmetry code: (ii) x, y+1, z1/2.
 

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