In the crystal structure of the title compound, the [SbS4]3− anions are linked by the Co(cyclam) complex cations into rings, which are further connected into layers that are linked by intermolecular hydrogen bonding via the water solvate molecules and are arranged in such a way that cavities are formed, in which the disordered acetonitrile solvate molecules are located.
Keywords: crystal structure, cobalt thioantimonate, layered structure, hydrogen bonding
Abstract
Reaction of Co(ClO4)2·6H2O with cyclam (cyclam = 1,4,8,11-tetraazacyclotetradecane) and Na3SbS4·9H2O (Schlippesches salt) in a mixture of acetonitrile and water leads to the formation of crystals of the title compound with the composition {[Co3(SbS4)2(C10H24N4)3]·2CH3CN·2H2O} n or {[(Co-cyclam)3(SbS4)2]·2(acetonitrile)·2H2O} n . The crystal structure of the title compound consists of three crystallographically independent [Co-cyclam]2+ cations, which are located on centers of inversion, one [SbS4]3− anion, one water and one acetonitrile molecule that occupy general positions. The acetonitrile molecule is disordered over two orientations and was refined using a split model. The CoII cations are coordinated by four N atoms of the cyclam ligand and two trans-S atoms of the tetrathioantimonate anion within slightly distorted octahedra. The unique [SbS4]3− anion is coordinated to all three crystallographically independent CoII cations and this unit, with its symmetry-related counterparts, forms rings composed of six Co-cyclam cations and six tetrathioantimonate anions that are further condensed into layers. These layers are perfectly stacked onto each other so that channels are formed in which acetontrile solvate molecules that are hydrogen bonded to the anions are embedded. The water solvate molecules are located between the layers and are connected to the cyclam ligands and the [SbS4]3− anions via intermolecular N—H⋯O and O—H⋯S hydrogen bonding.
Chemical context
Inorganic–organic chalcogenidometallates are an important class of compounds and many such compounds have been reported in the literature (Sheldrick & Wachhold, 1988 ▸; Bensch et al., 1997 ▸; Dehnen & Melullis, 2007 ▸; Wang et al., 2016 ▸; Zhou, 2016 ▸; Zhu & Dai, 2017 ▸; Nie et al., 2017 ▸). A large part of this family of compounds consists of thioantimonates, which exhibit a variety of coordination numbers that can lead to networks of different dimensionality (Jia et al., 2004 ▸; Powell et al., 2005 ▸; Spetzler et al., 2004 ▸; Zhang et al., 2007 ▸; Liu & Zhou, 2011 ▸; Engelke et al., 2004 ▸; Puls et al., 2006 ▸). Moreover, some of them have potential for applications, for example in the field of superionic conductors (Zhou et al., 2019 ▸) or as photoconductive materials (Pienack et al., 2008a
▸). For these reasons, we have explored such compounds over many years (Schaefer et al., 2003 ▸; Stähler et al., 2001 ▸; Schur et al., 1998 ▸, 2001 ▸; Kiebach et al., 2004 ▸; Spetzler et al., 2004 ▸; Lühmann et al., 2008 ▸; Pienack et al., 2008b
▸). In the beginning, we synthesized new thioantimonates using elemental antimony, sulfur and amine molecules under solvothermal conditions but later we found that many of these compounds are also available under solvothermal conditions if Schlippesches salt (Na3SbS4·9H2O) or NaSbS3 are used as reactants (Anderer et al., 2014 ▸, 2016 ▸; Danker et al., 2020 ▸). In this case, different SbS
x
species are present in solution, because Schlippesches salt is unstable and forms different reactive species such as [SbS3O]3−, HS−, [S2O3]2− or [SbS4]3− anions (Rammelsberg, 1841 ▸; Long & Bowen, 1970 ▸; Mosselmanns et al., 2000 ▸; Planer-Friedrich & Scheinost, 2011 ▸; Planer-Friedrich & Wilson, 2012 ▸; Anderer et al., 2014 ▸). In addition, a variety of complex redox and condensation reactions occur, generating polymeric thioantimonate(III) anions, which are found in the structures of the reaction products. To prevent the reduction of SbV to SbIII, a different synthesis strategy is required and the reaction temperature must be reduced to slow down the decomposition of Schlippesches salt. Using an aqueous solution of Na3SbS4·9H2O and adding a solution of late transition-metal cations leads to immediate precipitation of sulfides or hydroxides, even when chelating amine molecules are added. To solve the problem we developed a two-solution strategy: an organic solution contains the transition-metal cations and the chelating amine molecule and a second solution comprises Schlippesches salt. In the organic solution, the transition-metal complex is already generated in situ and mixing the two solutions leads to nucleation and successive growth of the product. A challenge is the integration of transition-metal cations into a thioantimonate(V) network, despite the [SbS4]3− anion offering four possible binding sites. In the course of this project we became interested in cyclam (cyclam = 1,4,8,11-tetraazacyclotetradecane), which is a tetradentate ligand. This means that in an octahedral coordination of a transition-metal cation, two coordination sites are provided to which thioantimonate(V) anions can coordinate, which, depending on the nature of the anion, can lead to the formation of the desired thioantimonate(V) networks.
In this context, we have reported on two new polymeric thioantimonates with the composition [(Cu-cyclam)3(SbS4)2]·20H2O and [(Zn-cyclam)3(SbS4)2]·8H2O (Danker et al., 2021 ▸). In the crystal structure of the Cu compound, the copper cations are sixfold coordinated by the four N atoms of the cyclam ligand and two trans-sulfur atoms of the [SbS4]3− anions within slightly distorted octahedra. The copper cations are linked by the anions into rings by corner-sharing SbS4 and CuN4S2 units, which are condensed into layers. These layers are stacked in such a way that large pores are formed. Between the layers, water molecules are embedded. At first glance, the arrangement of the building blocks in the crystal structure of the Zn compound looks similar, but in this case the ZnII cation is disordered above and below the N4 plane in a 1:1 ratio, which means that it is in a fivefold coordination of the four N atoms of the cyclam ligand and one S atom of the [SbS4]3− anions in a square-pyramidal geometry. The structural difference between the Cu and Zn coordinations was reproduced by DFT calculations (Danker et al., 2021 ▸). In the course of our systematic work we tried to prepare a similar compound with cobalt using the same synthetic approach. This led to crystals of the title compound, which were characterized by single-crystal X-ray diffraction.
Structural commentary
The asymmetric unit of the title compound consists of three crystallographically independent CoII cations and three independent cyclam ligands that are located on centers of inversion, as well as one [SbS4]3− anion, one water and one acetonitrile molecule that occupy general positions (Fig. 1 ▸). The acetonitrile molecule is disordered over two orientations and was refined using a split model (see Refinement). The CoII cations are six-coordinate being bound to the four N atoms of cyclam ligand that are located in the equatorial plane and two trans-S atoms of two inversion-related tetrathioantimonate anions that occupy the apical positions (Fig. 2 ▸). The Co—N bond lengths are very similar for the three crystallographically independent CoII cations whereas significant differences are found for the Co—S bond lengths (Table 1 ▸). These changes, however, do not correlate with the Sb—S distances (Table 1 ▸). The angles around the Co centers prove that the octahedra are slightly distorted (see supporting information). The cyclam ligands are in the trans-III(S,S,R,R) configuration, which is the most stable arrangement for the first row transition-metal cation-centered cyclam complexes (Bosnich et al., 1965 ▸).
Figure 1.
Crystal structure of the title compound with labeling and displacement ellipsoids drawn at the 50% probability level. The hydrogen atoms are omitted for clarity and the disordering of the acetonitrile ligands is shown with full and open bonds. Symmetry codes for the generation of equivalent atoms: (i) −x + 1, −y, −z + 2; (ii) −x + 1, −y + 1, −z + 1; (iii) −x + 2, −y, −z + 1.
Figure 2.
Crystal structure of the title compound with a view of the coordination sphere of the three crystallographically independent Co cations.
Table 1. Selected bond lengths (Å).
Sb1—S4 | 2.3195 (13) | S1—Co1 | 2.7258 (12) |
Sb1—S1 | 2.3200 (12) | S2—Co2 | 2.6932 (11) |
Sb1—S3 | 2.3221 (12) | S3—Co3 | 2.7821 (12) |
Sb1—S2 | 2.3382 (11) |
The Sb—S bond lengths in the tetrathioantimonate anion (Table 1 ▸) are comparable and correspond to those observed in other compounds with this anion. From the S—Sb—S bond angles it is obvious that the tetrahedron is only slightly distorted (see supporting information). The [SbS4]3− anion shows the rare tridentate coordination mode and is linked to each of the three crystallographically independent CoII cations and with inversion-related counterparts, forming rings composed of six [SbS4]3− anions and six [Co(cyclam]2+ cations (Fig. 3 ▸). These rings are condensed into layers parallel to the bc plane (Fig. 4 ▸). This layer topology is identical to that in [Cu(cyclam)3[SbS4)2]·20H2O but the two compounds are not isotypic (Danker et al., 2021 ▸). The layers are stacked perfectly onto each other, forming channels extending along the a-axis direction (Fig. 5 ▸).
Figure 3.
Crystal structure of the title compound with a view of an 24-membered ring composed of six Co cations and six [SbS4]3− anions.
Figure 4.
Crystal structure of the title compound with a view of the Co3(SbS4)2 network along the crystallographic a axis. The cyclam ligands are not shown for clarity.
Figure 5.
Crystal structure of the title compound with a view in the a-axis direction with intermolecular hydrogen bonding shown as dashed lines. The disorder of the acetonitrile molecules is omitted for clarity.
Supramolecular features
Within the channels are embedded acetonitrile solvate molecules that are disordered and hydrogen bonded to the tetrathioantimonate anion (Fig. 5 ▸). The C—H⋯S angles are close to linear, indicating that this is a significant interaction (Table 2 ▸). Water molecules are located between the layers and are connected to the [SbS4]3− anions via intermolecular O—H⋯S hydrogen bonding, which is classed as strong because the angles are close to linearity and relatively short H⋯S distances are observed (Table 2 ▸). These water molecules also act as acceptors for N—H⋯O hydrogen bonding to the cyclam ligands (Table 2 ▸). The layers are linked by additional C—H⋯S and N—H⋯S hydrogen bonds between the cyclam ligands and the tetrathioantimonate anions. There are additional H⋯S contacts but at distances close to van der Waals contacts with angles ranging between about 110 and 125°.
Table 2. Hydrogen-bond geometry (Å, °).
D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
---|---|---|---|---|
N1—H1⋯S2i | 1.00 | 2.48 | 3.442 (4) | 161 |
C1—H1B⋯S4ii | 0.99 | 2.95 | 3.858 (5) | 152 |
N2—H2⋯S4 | 1.00 | 2.49 | 3.448 (4) | 159 |
N11—H11⋯O1iii | 1.00 | 2.23 | 3.151 (6) | 153 |
N12—H12⋯S3iv | 1.00 | 2.43 | 3.378 (4) | 157 |
N21—H21⋯O1 | 1.00 | 2.08 | 2.920 (6) | 141 |
N22—H22⋯S1 | 1.00 | 2.35 | 3.290 (4) | 156 |
O1—H1C⋯S2iii | 0.84 | 2.49 | 3.276 (4) | 157 |
O1—H1D⋯S4v | 0.84 | 2.46 | 3.280 (4) | 166 |
C32—H32B⋯S4 | 0.98 | 2.81 | 3.71 (4) | 154 |
C32′—H32F⋯S4 | 0.98 | 2.88 | 3.85 (5) | 172 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
; (v)
.
Database survey
A search for structures of cobalt-centered cylam complexes in the Cambridge Structural Database (CSD version 5.42, last update November 2020; Groom et al., 2016 ▸) gave 152 hits, in four of which the cobalt cations are in an N4S2 coordination. In one of these structures (Refcode: NIMVIQ; Zeisler et al., 2013 ▸), a thiostannate acts as anion but none of them contains thioantimonate anions. The same results are obtained if the search is expanded to any transition-metal cation. Therefore, only the Cu and Zn compounds mentioned above have been published (Danker et al., 2021 ▸).
However, 21 structures with CoII and tetrathioantimonate anions have been published and in two of these structures, the cobalt cations are linked to a tetrathioantimonate anion, viz. [Co(diethylenetriamine)2][Co(tris(2-aminomethyl)amine)SbS4]2·4H2O (Engelke et al., 2008 ▸) and [Co(diethylenetriamine)2][Co(tris(2-aminomethyl)amine)SbS4]2·0.5H2O (Lichte, et al., 2009 ▸).
Synthesis and crystallization
Synthesis of Na3SbS4·9H2O
Na3SbS4·9H2O was synthesized by adding 16.6 g (0.213 mol) of Na2S·xH2O (technical grade, purchased from Acros Organics) to 58 mL of demineralized water. This solution was heated to 323 K for 1 h. Afterwards, 19.6 g (0.058 mol) of Sb2S3 (98%, purchased from Alfa Aesar) and 3.69 g (0.115 mol) of sulfur (min. 99%, purchased from Alfa Aesar) were added and the reaction mixture was heated to 343 K for 6 h. The reaction mixture was filtered and the filtrate was stored overnight, leading to the formation of slightly yellow crystals, which were filtered off, washed with small amounts of water and dried under vacuum (yield about 30% based on Sb2S3).
Synthesis of the title compound
16 mg (0.044 mmol) of Co(ClO4)2·6H2O (purchased from Alfa Aesar) and 16 mg (0.08 mmol) of cyclam (purchased from Strem Chemicals) were dissolved in 2 mL of acetonitrile (purchased from Merck). To this solution, a solution of 50 mg (0.14 mmol) of Na3SbS4·9H2O dissolved in 1 mL of H2O was added. Within 3d a few colorless crystals of the title compound were obtained, which were always contaminated with an additional and unknown phase that is amorphous to X-rays. This additional phase is also present if the reaction conditions are varied slightly. Therefore, one of the colorless crystals was selected for structure determination.
Refinement
Crystal data, data collection and structure refinement details are summarized in Table 3 ▸. All non-hydrogen atoms were refined anisotropically. The C- and N-bound H atoms were located in the difference map but were positioned with idealized geometry (methyl H atoms allowed to rotate but not to tip) and were refined isotropically with U iso(H) = 1.2U eq(C,N) (1.5 for methyl H atoms) using a riding model. The O-bound H atoms were located in the difference map, their bond lengths were set to ideal values and finally they were refined isotropically with U iso(H) = 1.5U eq(O) using a riding model. The acetontrile molecule is disordered over two orientations and was refined using a split model (ratio: 1:1) with restraints for the geometry and the components of the anisotropic displacement parameters.
Table 3. Experimental details.
Crystal data | |
Chemical formula | [Co3(SbS4)2(C10H24N4)3]·2C2H3N·2H2O |
M r | 1395.90 |
Crystal system, space group | Triclinic, P
![]() |
Temperature (K) | 200 |
a, b, c (Å) | 8.7292 (3), 12.9680 (5), 13.8936 (5) |
α, β, γ (°) | 66.218 (3), 77.035 (3), 83.321 (3) |
V (Å3) | 1401.93 (9) |
Z | 1 |
Radiation type | Mo Kα |
μ (mm−1) | 2.16 |
Crystal size (mm) | 0.15 × 0.10 × 0.07 |
Data collection | |
Diffractometer | Stoe IPDS2 |
Absorption correction | Numerical (X-RED and X-SHAPE; Stoe, 2008 ▸) |
T min, T max | 0.649, 0.774 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 15304, 6098, 5078 |
R int | 0.030 |
(sin θ/λ)max (Å−1) | 0.639 |
Refinement | |
R[F 2 > 2σ(F 2)], wR(F 2), S | 0.047, 0.126, 1.06 |
No. of reflections | 6098 |
No. of parameters | 321 |
No. of restraints | 87 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.81, −1.56 |
Supplementary Material
Crystal structure: contains datablock(s) I. DOI: 10.1107/S2056989022001074/mw2184sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989022001074/mw2184Isup2.hkl
CCDC reference: 2146891
Additional supporting information: crystallographic information; 3D view; checkCIF report
Acknowledgments
Financial support by the state of Schleswig-Holstein is gratefully acknowledged.
supplementary crystallographic information
Crystal data
[Co3(SbS4)2(C10H24N4)3]·2C2H3N·2H2O | Z = 1 |
Mr = 1395.90 | F(000) = 711 |
Triclinic, P1 | Dx = 1.653 Mg m−3 |
a = 8.7292 (3) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 12.9680 (5) Å | Cell parameters from 15304 reflections |
c = 13.8936 (5) Å | θ = 1.6–27.0° |
α = 66.218 (3)° | µ = 2.16 mm−1 |
β = 77.035 (3)° | T = 200 K |
γ = 83.321 (3)° | Block, red |
V = 1401.93 (9) Å3 | 0.15 × 0.10 × 0.07 mm |
Data collection
Stoe IPDS-2 diffractometer | 5078 reflections with I > 2σ(I) |
ω scans | Rint = 0.030 |
Absorption correction: numerical (X-Red and X-Shape; Stoe, 2008) | θmax = 27.0°, θmin = 1.6° |
Tmin = 0.649, Tmax = 0.774 | h = −11→11 |
15304 measured reflections | k = −16→16 |
6098 independent reflections | l = −17→17 |
Refinement
Refinement on F2 | Hydrogen site location: mixed |
Least-squares matrix: full | H-atom parameters constrained |
R[F2 > 2σ(F2)] = 0.047 | w = 1/[σ2(Fo2) + (0.084P)2 + 0.1597P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.126 | (Δ/σ)max = 0.047 |
S = 1.06 | Δρmax = 0.81 e Å−3 |
6098 reflections | Δρmin = −1.56 e Å−3 |
321 parameters | Extinction correction: SHELXL2016/6 (Sheldrick 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
87 restraints | Extinction coefficient: 0.0136 (11) |
Special details
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)
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Sb1 | 0.73888 (3) | 0.19084 (2) | 0.69041 (2) | 0.03283 (12) | |
S1 | 0.64905 (15) | 0.01167 (10) | 0.80137 (9) | 0.0414 (3) | |
S2 | 0.51359 (13) | 0.30840 (9) | 0.67415 (9) | 0.0380 (3) | |
S3 | 0.86596 (14) | 0.19636 (10) | 0.52265 (9) | 0.0416 (3) | |
S4 | 0.90553 (14) | 0.24527 (12) | 0.76901 (10) | 0.0461 (3) | |
Co1 | 0.500000 | 0.000000 | 1.000000 | 0.0350 (2) | |
N1 | 0.6290 (4) | −0.1388 (3) | 1.0629 (3) | 0.0392 (8) | |
H1 | 0.583701 | −0.171109 | 1.141506 | 0.047* | |
C1 | 0.7871 (6) | −0.1025 (5) | 1.0528 (4) | 0.0461 (11) | |
H1A | 0.847663 | −0.085872 | 0.979114 | 0.055* | |
H1B | 0.843932 | −0.162998 | 1.103578 | 0.055* | |
C2 | 0.7700 (6) | 0.0016 (5) | 1.0773 (4) | 0.0465 (11) | |
H2A | 0.720658 | −0.016978 | 1.153611 | 0.056* | |
H2B | 0.874555 | 0.032869 | 1.063722 | 0.056* | |
N2 | 0.6701 (5) | 0.0849 (3) | 1.0071 (3) | 0.0391 (8) | |
H2 | 0.736736 | 0.114228 | 0.933522 | 0.047* | |
C3 | 0.6268 (7) | 0.1831 (4) | 1.0369 (4) | 0.0465 (11) | |
H3A | 0.723689 | 0.218535 | 1.033103 | 0.056* | |
H3B | 0.567730 | 0.157340 | 1.111845 | 0.056* | |
C4 | 0.5275 (7) | 0.2697 (4) | 0.9642 (4) | 0.0502 (12) | |
H4A | 0.584251 | 0.290889 | 0.889012 | 0.060* | |
H4B | 0.515488 | 0.338203 | 0.980459 | 0.060* | |
C5 | 0.3653 (6) | 0.2311 (4) | 0.9738 (4) | 0.0462 (11) | |
H5A | 0.309991 | 0.205729 | 1.049576 | 0.055* | |
H5B | 0.304013 | 0.295721 | 0.930767 | 0.055* | |
Co2 | 0.500000 | 0.500000 | 0.500000 | 0.0342 (2) | |
N11 | 0.3450 (4) | 0.4238 (3) | 0.4693 (3) | 0.0375 (8) | |
H11 | 0.350102 | 0.342674 | 0.518595 | 0.045* | |
C11 | 0.1850 (5) | 0.4666 (4) | 0.5023 (4) | 0.0422 (10) | |
H11A | 0.105455 | 0.411439 | 0.515475 | 0.051* | |
H11B | 0.160604 | 0.538662 | 0.445200 | 0.051* | |
C12 | 0.1825 (5) | 0.4840 (4) | 0.6041 (4) | 0.0422 (10) | |
H12A | 0.083455 | 0.523577 | 0.622556 | 0.051* | |
H12B | 0.188964 | 0.410337 | 0.664261 | 0.051* | |
N12 | 0.3180 (4) | 0.5518 (3) | 0.5857 (3) | 0.0370 (8) | |
H12 | 0.291146 | 0.630110 | 0.537533 | 0.044* | |
C13 | 0.3355 (6) | 0.5600 (4) | 0.6854 (4) | 0.0433 (10) | |
H13A | 0.348209 | 0.483093 | 0.739725 | 0.052* | |
H13B | 0.238416 | 0.594863 | 0.713526 | 0.052* | |
C14 | 0.4744 (7) | 0.6285 (5) | 0.6695 (5) | 0.0500 (12) | |
H14A | 0.471829 | 0.639111 | 0.736564 | 0.060* | |
H14B | 0.464296 | 0.703873 | 0.612383 | 0.060* | |
C15 | 0.6317 (6) | 0.5751 (4) | 0.6397 (4) | 0.0435 (10) | |
H15A | 0.717003 | 0.616669 | 0.643320 | 0.052* | |
H15B | 0.637578 | 0.496295 | 0.691914 | 0.052* | |
Co3 | 1.000000 | 0.000000 | 0.500000 | 0.0441 (2) | |
N21 | 0.8192 (5) | −0.0196 (3) | 0.4448 (3) | 0.0409 (9) | |
H21 | 0.851395 | −0.081969 | 0.418885 | 0.049* | |
C21 | 0.6910 (6) | −0.0636 (5) | 0.5384 (5) | 0.0480 (11) | |
H21A | 0.610940 | −0.097814 | 0.520863 | 0.058* | |
H21B | 0.639594 | −0.001829 | 0.559812 | 0.058* | |
C22 | 0.7616 (6) | −0.1511 (4) | 0.6284 (4) | 0.0484 (12) | |
H22A | 0.680551 | −0.178519 | 0.694862 | 0.058* | |
H22B | 0.805027 | −0.216022 | 0.609610 | 0.058* | |
N22 | 0.8886 (5) | −0.0960 (3) | 0.6442 (3) | 0.0401 (9) | |
H22 | 0.833782 | −0.042725 | 0.677357 | 0.048* | |
C23 | 0.9780 (7) | −0.1761 (4) | 0.7226 (4) | 0.0477 (12) | |
H23A | 1.027418 | −0.235259 | 0.696736 | 0.057* | |
H23B | 0.904885 | −0.213090 | 0.791464 | 0.057* | |
C24 | 1.1039 (7) | −0.1201 (5) | 0.7413 (4) | 0.0549 (13) | |
H24A | 1.148426 | −0.175116 | 0.802670 | 0.066* | |
H24B | 1.055165 | −0.056814 | 0.761253 | 0.066* | |
C25 | 1.2359 (6) | −0.0757 (5) | 0.6455 (4) | 0.0496 (12) | |
H25A | 1.320806 | −0.049907 | 0.666612 | 0.060* | |
H25B | 1.279912 | −0.137189 | 0.621601 | 0.060* | |
O1 | 0.7600 (5) | −0.1823 (3) | 0.3619 (3) | 0.0554 (9) | |
H1C | 0.704099 | −0.205901 | 0.333522 | 0.08 (2)* | |
H1D | 0.850839 | −0.202701 | 0.339072 | 0.10 (3)* | |
N31 | 0.748 (3) | 0.4588 (19) | 1.0545 (11) | 0.116 (7) | 0.5 |
C31 | 0.815 (5) | 0.457 (4) | 0.9743 (13) | 0.101 (7) | 0.5 |
C32 | 0.908 (4) | 0.469 (4) | 0.8707 (12) | 0.090 (7) | 0.5 |
H32A | 0.899961 | 0.547550 | 0.820009 | 0.135* | 0.5 |
H32B | 0.869880 | 0.419111 | 0.844728 | 0.135* | 0.5 |
H32C | 1.018580 | 0.449588 | 0.876821 | 0.135* | 0.5 |
N31' | 0.814 (3) | 0.4114 (18) | 1.0734 (10) | 0.112 (7) | 0.5 |
C31' | 0.833 (5) | 0.452 (4) | 0.9817 (11) | 0.093 (7) | 0.5 |
C32' | 0.854 (5) | 0.488 (4) | 0.8670 (12) | 0.122 (12) | 0.5 |
H32D | 0.943593 | 0.537807 | 0.831978 | 0.183* | 0.5 |
H32E | 0.758528 | 0.529186 | 0.843259 | 0.183* | 0.5 |
H32F | 0.873030 | 0.422251 | 0.847836 | 0.183* | 0.5 |
Atomic displacement parameters (Å2)
U11 | U22 | U33 | U12 | U13 | U23 | |
Sb1 | 0.03142 (17) | 0.03401 (17) | 0.02939 (17) | −0.00144 (10) | −0.00454 (10) | −0.00920 (11) |
S1 | 0.0463 (6) | 0.0347 (5) | 0.0360 (6) | −0.0044 (4) | 0.0013 (5) | −0.0103 (5) |
S2 | 0.0336 (5) | 0.0376 (5) | 0.0357 (6) | 0.0022 (4) | −0.0059 (4) | −0.0085 (4) |
S3 | 0.0441 (6) | 0.0424 (6) | 0.0312 (5) | 0.0026 (5) | −0.0021 (4) | −0.0111 (5) |
S4 | 0.0384 (6) | 0.0608 (7) | 0.0406 (6) | −0.0107 (5) | −0.0073 (5) | −0.0189 (6) |
Co1 | 0.0331 (4) | 0.0364 (4) | 0.0342 (4) | −0.0022 (3) | −0.0069 (3) | −0.0119 (3) |
N1 | 0.0383 (19) | 0.041 (2) | 0.0338 (19) | 0.0015 (16) | −0.0068 (15) | −0.0103 (16) |
C1 | 0.036 (2) | 0.055 (3) | 0.044 (3) | 0.002 (2) | −0.0090 (19) | −0.016 (2) |
C2 | 0.038 (2) | 0.061 (3) | 0.039 (3) | −0.008 (2) | −0.0099 (19) | −0.016 (2) |
N2 | 0.040 (2) | 0.045 (2) | 0.0311 (18) | −0.0077 (16) | −0.0064 (15) | −0.0122 (16) |
C3 | 0.060 (3) | 0.043 (3) | 0.041 (3) | −0.014 (2) | −0.007 (2) | −0.018 (2) |
C4 | 0.065 (3) | 0.040 (2) | 0.040 (3) | −0.010 (2) | 0.000 (2) | −0.013 (2) |
C5 | 0.053 (3) | 0.038 (2) | 0.038 (2) | 0.003 (2) | −0.001 (2) | −0.011 (2) |
Co2 | 0.0295 (4) | 0.0378 (4) | 0.0331 (4) | −0.0022 (3) | −0.0049 (3) | −0.0118 (3) |
N11 | 0.0363 (19) | 0.0381 (19) | 0.0348 (19) | −0.0025 (15) | −0.0086 (15) | −0.0095 (16) |
C11 | 0.032 (2) | 0.047 (3) | 0.044 (3) | −0.0011 (18) | −0.0105 (19) | −0.013 (2) |
C12 | 0.030 (2) | 0.042 (2) | 0.043 (3) | −0.0043 (17) | −0.0024 (18) | −0.006 (2) |
N12 | 0.0352 (18) | 0.0370 (18) | 0.0337 (19) | 0.0011 (15) | −0.0061 (15) | −0.0093 (15) |
C13 | 0.044 (2) | 0.048 (3) | 0.035 (2) | 0.003 (2) | −0.0039 (19) | −0.016 (2) |
C14 | 0.057 (3) | 0.050 (3) | 0.046 (3) | −0.004 (2) | −0.008 (2) | −0.022 (2) |
C15 | 0.049 (3) | 0.043 (2) | 0.043 (3) | −0.003 (2) | −0.015 (2) | −0.017 (2) |
Co3 | 0.0412 (5) | 0.0448 (5) | 0.0438 (5) | −0.0033 (4) | −0.0067 (4) | −0.0149 (4) |
N21 | 0.0363 (19) | 0.042 (2) | 0.046 (2) | 0.0010 (16) | −0.0086 (16) | −0.0195 (18) |
C21 | 0.035 (2) | 0.055 (3) | 0.058 (3) | −0.004 (2) | −0.006 (2) | −0.027 (3) |
C22 | 0.046 (3) | 0.044 (3) | 0.052 (3) | −0.009 (2) | 0.003 (2) | −0.020 (2) |
N22 | 0.042 (2) | 0.0364 (19) | 0.037 (2) | −0.0024 (16) | −0.0023 (16) | −0.0117 (16) |
C23 | 0.056 (3) | 0.039 (2) | 0.037 (2) | 0.003 (2) | −0.002 (2) | −0.009 (2) |
C24 | 0.067 (3) | 0.060 (3) | 0.042 (3) | 0.011 (3) | −0.020 (3) | −0.022 (2) |
C25 | 0.044 (3) | 0.058 (3) | 0.051 (3) | 0.007 (2) | −0.019 (2) | −0.023 (2) |
O1 | 0.054 (2) | 0.060 (2) | 0.061 (2) | −0.0025 (18) | −0.0136 (19) | −0.031 (2) |
N31 | 0.150 (16) | 0.126 (13) | 0.073 (4) | −0.026 (10) | 0.011 (6) | −0.052 (5) |
C31 | 0.141 (15) | 0.097 (11) | 0.071 (4) | −0.041 (10) | 0.014 (6) | −0.045 (5) |
C32 | 0.117 (15) | 0.094 (14) | 0.066 (4) | −0.033 (11) | 0.002 (6) | −0.041 (7) |
N31' | 0.162 (19) | 0.106 (13) | 0.070 (3) | −0.046 (12) | −0.019 (5) | −0.026 (5) |
C31' | 0.114 (13) | 0.100 (13) | 0.070 (3) | −0.052 (11) | −0.017 (5) | −0.026 (5) |
C32' | 0.18 (3) | 0.12 (2) | 0.070 (3) | −0.07 (2) | −0.020 (6) | −0.026 (5) |
Geometric parameters (Å, º)
Sb1—S4 | 2.3195 (13) | N12—H12 | 1.0000 |
Sb1—S1 | 2.3200 (12) | C13—C14 | 1.510 (8) |
Sb1—S3 | 2.3221 (12) | C13—H13A | 0.9900 |
Sb1—S2 | 2.3382 (11) | C13—H13B | 0.9900 |
S1—Co1 | 2.7258 (12) | C14—C15 | 1.514 (7) |
S2—Co2 | 2.6932 (11) | C14—H14A | 0.9900 |
S3—Co3 | 2.7821 (12) | C14—H14B | 0.9900 |
Co1—N2i | 1.990 (4) | C15—H15A | 0.9900 |
Co1—N2 | 1.990 (4) | C15—H15B | 0.9900 |
Co1—N1 | 1.993 (4) | Co3—N22 | 1.976 (4) |
Co1—N1i | 1.993 (4) | Co3—N22iii | 1.976 (4) |
N1—C1 | 1.468 (6) | Co3—N21 | 1.985 (4) |
N1—C5i | 1.470 (7) | Co3—N21iii | 1.985 (4) |
N1—H1 | 1.0000 | N21—C21 | 1.472 (7) |
C1—C2 | 1.504 (8) | N21—C25iii | 1.488 (6) |
C1—H1A | 0.9900 | N21—H21 | 1.0000 |
C1—H1B | 0.9900 | C21—C22 | 1.506 (8) |
C2—N2 | 1.481 (6) | C21—H21A | 0.9900 |
C2—H2A | 0.9900 | C21—H21B | 0.9900 |
C2—H2B | 0.9900 | C22—N22 | 1.486 (7) |
N2—C3 | 1.476 (6) | C22—H22A | 0.9900 |
N2—H2 | 1.0000 | C22—H22B | 0.9900 |
C3—C4 | 1.511 (8) | N22—C23 | 1.468 (6) |
C3—H3A | 0.9900 | N22—H22 | 1.0000 |
C3—H3B | 0.9900 | C23—C24 | 1.506 (9) |
C4—C5 | 1.517 (8) | C23—H23A | 0.9900 |
C4—H4A | 0.9900 | C23—H23B | 0.9900 |
C4—H4B | 0.9900 | C24—C25 | 1.510 (8) |
C5—H5A | 0.9900 | C24—H24A | 0.9900 |
C5—H5B | 0.9900 | C24—H24B | 0.9900 |
Co2—N11ii | 1.975 (4) | C25—H25A | 0.9900 |
Co2—N11 | 1.975 (4) | C25—H25B | 0.9900 |
Co2—N12 | 1.985 (4) | O1—H1C | 0.8400 |
Co2—N12ii | 1.985 (4) | O1—H1D | 0.8400 |
N11—C15ii | 1.475 (6) | N31—C31 | 1.145 (15) |
N11—C11 | 1.486 (6) | C31—C32 | 1.442 (17) |
N11—H11 | 1.0000 | C32—H32A | 0.9800 |
C11—C12 | 1.514 (7) | C32—H32B | 0.9800 |
C11—H11A | 0.9900 | C32—H32C | 0.9800 |
C11—H11B | 0.9900 | N31'—C31' | 1.145 (15) |
C12—N12 | 1.470 (6) | C31'—C32' | 1.442 (16) |
C12—H12A | 0.9900 | C32'—H32D | 0.9800 |
C12—H12B | 0.9900 | C32'—H32E | 0.9800 |
N12—C13 | 1.474 (6) | C32'—H32F | 0.9800 |
S4—Sb1—S1 | 109.86 (5) | H12A—C12—H12B | 108.4 |
S4—Sb1—S3 | 110.64 (5) | C12—N12—C13 | 111.3 (4) |
S1—Sb1—S3 | 110.81 (5) | C12—N12—Co2 | 108.0 (3) |
S4—Sb1—S2 | 110.32 (5) | C13—N12—Co2 | 119.6 (3) |
S1—Sb1—S2 | 105.36 (4) | C12—N12—H12 | 105.6 |
S3—Sb1—S2 | 109.73 (4) | C13—N12—H12 | 105.6 |
Sb1—S1—Co1 | 112.07 (5) | Co2—N12—H12 | 105.6 |
Sb1—S2—Co2 | 122.01 (4) | N12—C13—C14 | 112.7 (4) |
Sb1—S3—Co3 | 119.94 (5) | N12—C13—H13A | 109.0 |
N2i—Co1—N2 | 180.00 (19) | C14—C13—H13A | 109.0 |
N2i—Co1—N1 | 93.50 (17) | N12—C13—H13B | 109.0 |
N2—Co1—N1 | 86.50 (17) | C14—C13—H13B | 109.0 |
N2i—Co1—N1i | 86.50 (17) | H13A—C13—H13B | 107.8 |
N2—Co1—N1i | 93.50 (17) | C13—C14—C15 | 113.7 (4) |
N1—Co1—N1i | 180.0 | C13—C14—H14A | 108.8 |
N2i—Co1—S1 | 89.02 (12) | C15—C14—H14A | 108.8 |
N2—Co1—S1 | 90.98 (12) | C13—C14—H14B | 108.8 |
N1—Co1—S1 | 88.50 (12) | C15—C14—H14B | 108.8 |
N1i—Co1—S1 | 91.50 (12) | H14A—C14—H14B | 107.7 |
N2i—Co1—S1i | 90.98 (12) | N11ii—C15—C14 | 111.5 (4) |
N2—Co1—S1i | 89.02 (12) | N11ii—C15—H15A | 109.3 |
N1—Co1—S1i | 91.50 (12) | C14—C15—H15A | 109.3 |
N1i—Co1—S1i | 88.50 (12) | N11ii—C15—H15B | 109.3 |
S1—Co1—S1i | 180.0 | C14—C15—H15B | 109.3 |
C1—N1—C5i | 111.8 (4) | H15A—C15—H15B | 108.0 |
C1—N1—Co1 | 107.1 (3) | N22—Co3—N22iii | 180.00 (19) |
C5i—N1—Co1 | 119.1 (3) | N22—Co3—N21 | 86.93 (17) |
C1—N1—H1 | 106.0 | N22iii—Co3—N21 | 93.07 (17) |
C5i—N1—H1 | 106.0 | N22—Co3—N21iii | 93.07 (17) |
Co1—N1—H1 | 106.0 | N22iii—Co3—N21iii | 86.93 (17) |
N1—C1—C2 | 108.2 (4) | N21—Co3—N21iii | 180.0 |
N1—C1—H1A | 110.1 | N22—Co3—S3iii | 87.74 (11) |
C2—C1—H1A | 110.1 | N22iii—Co3—S3iii | 92.26 (11) |
N1—C1—H1B | 110.1 | N21—Co3—S3iii | 87.89 (12) |
C2—C1—H1B | 110.1 | N21iii—Co3—S3iii | 92.11 (12) |
H1A—C1—H1B | 108.4 | N22—Co3—S3 | 92.26 (11) |
N2—C2—C1 | 107.9 (4) | N22iii—Co3—S3 | 87.74 (11) |
N2—C2—H2A | 110.1 | N21—Co3—S3 | 92.11 (12) |
C1—C2—H2A | 110.1 | N21iii—Co3—S3 | 87.89 (12) |
N2—C2—H2B | 110.1 | S3iii—Co3—S3 | 180.00 (5) |
C1—C2—H2B | 110.1 | C21—N21—C25iii | 111.9 (4) |
H2A—C2—H2B | 108.4 | C21—N21—Co3 | 106.4 (3) |
C3—N2—C2 | 111.7 (4) | C25iii—N21—Co3 | 119.8 (3) |
C3—N2—Co1 | 118.9 (3) | C21—N21—H21 | 105.9 |
C2—N2—Co1 | 107.0 (3) | C25iii—N21—H21 | 105.9 |
C3—N2—H2 | 106.2 | Co3—N21—H21 | 105.9 |
C2—N2—H2 | 106.2 | N21—C21—C22 | 107.7 (4) |
Co1—N2—H2 | 106.2 | N21—C21—H21A | 110.2 |
N2—C3—C4 | 112.0 (4) | C22—C21—H21A | 110.2 |
N2—C3—H3A | 109.2 | N21—C21—H21B | 110.2 |
C4—C3—H3A | 109.2 | C22—C21—H21B | 110.2 |
N2—C3—H3B | 109.2 | H21A—C21—H21B | 108.5 |
C4—C3—H3B | 109.2 | N22—C22—C21 | 107.0 (4) |
H3A—C3—H3B | 107.9 | N22—C22—H22A | 110.3 |
C3—C4—C5 | 114.6 (4) | C21—C22—H22A | 110.3 |
C3—C4—H4A | 108.6 | N22—C22—H22B | 110.3 |
C5—C4—H4A | 108.6 | C21—C22—H22B | 110.3 |
C3—C4—H4B | 108.6 | H22A—C22—H22B | 108.6 |
C5—C4—H4B | 108.6 | C23—N22—C22 | 112.3 (4) |
H4A—C4—H4B | 107.6 | C23—N22—Co3 | 119.9 (3) |
N1i—C5—C4 | 112.6 (4) | C22—N22—Co3 | 106.9 (3) |
N1i—C5—H5A | 109.1 | C23—N22—H22 | 105.6 |
C4—C5—H5A | 109.1 | C22—N22—H22 | 105.6 |
N1i—C5—H5B | 109.1 | Co3—N22—H22 | 105.6 |
C4—C5—H5B | 109.1 | N22—C23—C24 | 112.5 (4) |
H5A—C5—H5B | 107.8 | N22—C23—H23A | 109.1 |
N11ii—Co2—N11 | 180.0 | C24—C23—H23A | 109.1 |
N11ii—Co2—N12 | 93.73 (16) | N22—C23—H23B | 109.1 |
N11—Co2—N12 | 86.27 (16) | C24—C23—H23B | 109.1 |
N11ii—Co2—N12ii | 86.27 (16) | H23A—C23—H23B | 107.8 |
N11—Co2—N12ii | 93.73 (16) | C23—C24—C25 | 113.8 (5) |
N12—Co2—N12ii | 180.0 | C23—C24—H24A | 108.8 |
N11ii—Co2—S2ii | 86.16 (11) | C25—C24—H24A | 108.8 |
N11—Co2—S2ii | 93.84 (11) | C23—C24—H24B | 108.8 |
N12—Co2—S2ii | 91.31 (11) | C25—C24—H24B | 108.8 |
N12ii—Co2—S2ii | 88.69 (11) | H24A—C24—H24B | 107.7 |
N11ii—Co2—S2 | 93.84 (11) | N21iii—C25—C24 | 111.6 (4) |
N11—Co2—S2 | 86.16 (11) | N21iii—C25—H25A | 109.3 |
N12—Co2—S2 | 88.69 (11) | C24—C25—H25A | 109.3 |
N12ii—Co2—S2 | 91.31 (11) | N21iii—C25—H25B | 109.3 |
S2ii—Co2—S2 | 180.0 | C24—C25—H25B | 109.3 |
C15ii—N11—C11 | 111.4 (4) | H25A—C25—H25B | 108.0 |
C15ii—N11—Co2 | 118.1 (3) | H1C—O1—H1D | 102.1 |
C11—N11—Co2 | 108.6 (3) | N31—C31—C32 | 172 (5) |
C15ii—N11—H11 | 106.0 | C31—C32—H32A | 109.4 |
C11—N11—H11 | 106.0 | C31—C32—H32B | 109.5 |
Co2—N11—H11 | 106.0 | H32A—C32—H32B | 109.5 |
N11—C11—C12 | 107.6 (4) | C31—C32—H32C | 109.5 |
N11—C11—H11A | 110.2 | H32A—C32—H32C | 109.5 |
C12—C11—H11A | 110.2 | H32B—C32—H32C | 109.5 |
N11—C11—H11B | 110.2 | N31'—C31'—C32' | 172 (5) |
C12—C11—H11B | 110.2 | C31'—C32'—H32D | 109.5 |
H11A—C11—H11B | 108.5 | C31'—C32'—H32E | 109.5 |
N12—C12—C11 | 108.2 (4) | H32D—C32'—H32E | 109.5 |
N12—C12—H12A | 110.1 | C31'—C32'—H32F | 109.4 |
C11—C12—H12A | 110.1 | H32D—C32'—H32F | 109.5 |
N12—C12—H12B | 110.1 | H32E—C32'—H32F | 109.5 |
C11—C12—H12B | 110.1 |
Symmetry codes: (i) −x+1, −y, −z+2; (ii) −x+1, −y+1, −z+1; (iii) −x+2, −y, −z+1.
Hydrogen-bond geometry (Å, º)
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···S2i | 1.00 | 2.48 | 3.442 (4) | 161 |
C1—H1B···S4iv | 0.99 | 2.95 | 3.858 (5) | 152 |
N2—H2···S4 | 1.00 | 2.49 | 3.448 (4) | 159 |
N11—H11···O1v | 1.00 | 2.23 | 3.151 (6) | 153 |
N12—H12···S3ii | 1.00 | 2.43 | 3.378 (4) | 157 |
N21—H21···O1 | 1.00 | 2.08 | 2.920 (6) | 141 |
N22—H22···S1 | 1.00 | 2.35 | 3.290 (4) | 156 |
O1—H1C···S2v | 0.84 | 2.49 | 3.276 (4) | 157 |
O1—H1D···S4iii | 0.84 | 2.46 | 3.280 (4) | 166 |
C32—H32B···S4 | 0.98 | 2.81 | 3.71 (4) | 154 |
C32′—H32F···S4 | 0.98 | 2.88 | 3.85 (5) | 172 |
Symmetry codes: (i) −x+1, −y, −z+2; (ii) −x+1, −y+1, −z+1; (iii) −x+2, −y, −z+1; (iv) −x+2, −y, −z+2; (v) −x+1, −y, −z+1.
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) I. DOI: 10.1107/S2056989022001074/mw2184sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989022001074/mw2184Isup2.hkl
CCDC reference: 2146891
Additional supporting information: crystallographic information; 3D view; checkCIF report