Open Access Article
Muhammad Sohail
,
Carsten Heinsen
,
Allen G. Oliver
and
Emily Y. Tsui
*
Department of Chemistry and Biochemistry, University of Notre Dame, Notre Dame, Indiana, USA. E-mail: etsui@nd.edu
First published on 11th February 2026
Dianionic bis(carboxamide)pyridine-supported metal(II) dithiolate complexes of Cd2+ and Hg2+ showed isostructural [N3S2] coordination to a previously reported zinc variant, but changes in ionic radius resulted in distortion of the coordination geometries. While addition of elemental sulfur to the zinc dithiolate complex selectively inserts an “S3” unit to form a zinc tetrasulfanide complex, addition of S8 to the Cd2+ or Hg2+ congeners formed multiple products corresponding to sulfur insertion at both thiolate moieties, with different equilibrium constants of insertion. These reactions were correlated to comparisons of metal thiolate nucleophilicity and electrochemical oxidation potentials of the dithiolate complexes. These results point to additional contributions from ring strain and other structural/steric effects in controlling the thermodynamics of sulfur insertion.
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| Scheme 1 (a) Formation of a zinc tetrasulfanide complex ([2-Zn]2−) by sulfur insertion into [1-Zn]2−. (b) Addition of S8 to the Cd and Hg congeners of [1-Zn]2− show metal-dependent reactivity. | ||
Like Zn2+, the other group 12 divalent ions Cd2+ and Hg2+ are coordinated strongly by sulfur-containing ligands, including the cysteine residues of the protein metallothionein.6–8 However, due to differences in the ionic and covalent radii and metal ion polarizability, the thermodynamics of metal–thiolate bonding and thiolate reactivity are expected to vary. For example, complexation studies between these metals and cysteine showed that the formation constants decrease in the order Hg2+ > Cd2+ > Zn2+, an order that is dictated by the metal–sulfur bonding rather than metal–oxygen or metal–nitrogen interactions.9 The larger metal ions are also known to exhibit relativistic effects, further stabilizing metal–sulfur bonding. These differences in bonding are expected to change the thiolate oxidation potentials, nucleophilicity, and basicity. For these reasons, we were interested in comparing the sulfur insertion reactivity of these metals when coordinated by the same chelating thiolate ligands.
Here, we present the sulfur insertion reactivity of the Cd2+ and Hg2+ congeners of the dithiolate complex [1-Zn]2−. These complexes are structurally analogous, with variations in bond lengths and angles due to differences in ionic radii. Increased metal size and stronger metal–thiolate bonding was found to decrease metal thiolate nucleophilicity and shift the thiolate oxidation potentials. While the Cd and Hg congeners also undergo sulfur insertion into the metal–thiolate bonds, the reactions proceed with lower equilibrium constants and form mixtures of products arising from sulfur insertion at both thiolate moieties. These results show that both the ligand and the metal are critical in determining the outcome of sulfur–thiolate reactivity.
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| Fig. 1 Solid-state structures of [Et4N]2[1-M] (M = Cd, Hg) as 50% probability ellipsoids. Hydrogen atoms and tetraethylammonium cations omitted for clarity. | ||
Table 1 compares the structural parameters of [1-M]2− (M = Zn, Cd, and Hg). While the metal–pyridine bond distances (M–N2) increase in the expected order based on the ionic radius of the divalent cations, with Zn < Cd < Hg, the metal–thiolate (M–S) distances increase in the order of Zn < Hg ∼ Cd. The slightly shorter metal–thiolate distances of [1-Hg]2− compared to [1-Cd]2− are consistent with previous comparisons of other mercury thiolate complexes with their cadmium thiolate congeners. These shorter Hg–X bonds compared to Cd–X bonds were previously proposed by Parkin and others to arise due to mercury's smaller covalent radius, as well as the influence of relativistic effects.12 The larger metal cations also exhibited greater differences between the two metal–sulfur distances of each complex.
| M | Bond length (Å) | Angle (°) | τ5 | |||
|---|---|---|---|---|---|---|
| M–S1 | M–S2 | M–N2 | S1−M–S2 | N1−M–N3 | ||
| Zn | 2.3532(8) | 2.3768(8) | 2.118(2) | 102.64(3) | 147.67(10) | 0.30(20) |
| Cd | 2.5058(16) | 2.5392(15) | 2.308(4) | 108.05(5) | 137.69(15) | 0.09(32) |
| Hg | 2.4890(9) | 2.5172(9) | 2.420(3) | 113.16(3) | 133.22(9) | 0.03(19) |
The 113Cd NMR spectrum of a DMSO-d6 solution of the methylated cadmium congener shows a single resonance at −275.7 ppm, referenced against Cd(ClO4)2 (δ −640.27 ppm), indicating a single Cd chemical environment. This assignment is inconsistent with a bimetallic helical structure like that of [3Me-Zn]2−, in which the two metal centers have different coordination environments. Diffusion ordered NMR spectroscopy (DOSY) measured a diffusion coefficient of 1.62 × 10−10 m2 s−1 for [3Me-Zn]2−, while that of the methylation product of [1-Cd]2− is 1.84 × 10−10 m2 s−1. Based on these data and other DOSY NMR benchmarks of different metal complexes supported by this chelating ligand framework (Table S1), we assign the Cd and Hg methylation products to have monometallic structures (Fig. 2, [4Me-M(solv)]−, M = Cd, Hg, solv = CH3CN or DMSO), in which the metal coordination sphere is completed by coordinated solvent molecules. This difference reflects the larger ionic radii of these metals compared to Zn2+, which more readily accommodates four-coordinate geometries.14
Although we have so far been unable to grow X-ray quality single crystals of [4Me-M(solv)]−, addition of tetraethylammonium 4-methylbenzenethiolate ([Et4N][Stol]) to [4Me-Cd(solv)]− or [4Me-Hg(solv)]− enabled the growth of single crystals of [Et4N]2[4Me-Cd(Stol)] and [Et4N]2[4Me-Hg(Stol)] (Fig. 2). Both complexes are monometallic with [N3S2] coordination in which the methyl thioether moiety is not coordinated to the metal but displaced by the –Stol anion. Addition of [Et4N][Stol] to a DMSO-d6 solution of [Et4N]2[3Me-Zn] also forms a new species by 1H NMR spectroscopy, indicating that the helical bimetallic structure of this complex can be disrupted by exogenous thiolate coordination.
To compare the influence of the different metal centers on the relative nucleophilicities of the thiolate moieties, competition experiments were performed by treatment of binary mixtures of different metal dithiolate complexes [1-M]2− with MeI. As a representative dataset, Fig. 3 compares the 1H NMR spectra of a 1
:
1 mixture of [Et4N]2[1-Zn] and [Et4N]2[1-Cd] in DMSO-d6 with that of the same mixture measured 1 min after addition of MeI. The spectrum measured after addition of MeI shows a mixture of [1-Zn]2−, [1-Cd]2−, [3Me-Zn]2−, and [4Me-Cd(solv)]−. Integration of the spectrum showed that ca. 44% of [1-Zn]2− was methylated compared to 15% of [1-Cd]2−. These results qualitatively suggest that the zinc thiolate moiety is more nucleophilic than the cadmium thiolate moiety.
We were unable to calculate the methylation reaction rate constants due to competitive metal cation exchange during the methylation reaction. For example, 1H NMR spectroscopy of a DMSO-d6 mixture of [Et4N]2[1-Zn] and [Et4N][4Me-Cd(solv)] showed the formation of [3Me-Zn]2− and [1-Cd]2− over 1 h at room temperature (eqn (1), Fig. S28).
| [1-Zn]2− + [4Me-Cd(solv)]− ⇌ 0.5[3Me-Zn]2− + [1-Cd]2− | (1) |
Similar cation exchange reactions were observed between [1-Zn]2− and [4Me-Hg(solv)]−, and between [1-Cd]2− and [4Me-Hg(solv)]− (Fig. S29 and S30).
Based on these results, the species observed in the spectra shown in Fig. 3 are likely formed from both thiolate alkylation and metal cation exchange. As metal cation exchange is apparently slower, on the order of tens of minutes, we approximated the spectrum taken immediately upon addition (<1 min) as arising only from thiolate alkylation. Table 2 shows the relative ratios for different mixtures. Based on these data, the thiolate nucleophilicities (kM) of [1-M]2− qualitatively decrease in the order [1-Zn]2− > [1-Cd]2− > [1-Hg]2−.
Although qualitative, the above results are consistent with previously reported experimental and theoretical measurements of metal thiolate nucleophilicity.15,16 The greater nucleophilicity of [1-Zn]2− compared to the cadmium and mercury congeners is consistent with the more ionic nature of the Zn–S bond compared to the Cd–S and Hg–S bonds, which are more covalent.15
The above results point to metal-dependent structural differences upon thiolate oxidation. The cyclic voltammograms (CVs) of CH3CN solutions of [Et4N]2[1-M] (M = Zn, Cd, Hg) with TBAPF6 electrolyte (TBA = tetrabutylammonium, 0.1 M) were measured (Fig. S38). Each voltammogram shows two broad, irreversible oxidation waves between −0.6 and 0.1 V vs. Fc+/Fc corresponding to oxidation of the thiolate moieties. The return reduction waves observed in the voltammograms are assigned to reduction of disulfide moieties formed after thiolate oxidation. Table 3 compares the onset potentials of the first thiolate oxidation waves for each complex, which shift to more positive potentials in the order [1-Zn]2− < [1-Hg]2− ∼ [1-Cd]2−. The more positive oxidation potentials of the cadmium and mercury congeners may correspond to the greater covalency of the M–S bonds in these compounds. These electrochemically measured differences are consistent with the reactivity of these complexes. A DMSO-d6 mixture of [5-Cd(solv)]2− and [1-Zn]2− showed reduction of the former and oxidation of the latter by 1H NMR spectroscopy (Fig. S39).
Fig. 4 compares the 1H NMR spectra of a DMSO-d6 solution of [Et4N]2[1-Cd] with added S8 (3/8 and 5/8 equiv.). One of these products is a C1-symmetric product with a downfield doublet resonance at δ 8.47 ppm, similar to that of [2-Zn]2− (Fig. S32) and is assigned as the cadmium tetrasulfanide complex [2-Cd]2− (Scheme 3). The downfield shift of the resonance is attributed to structural distortions resulting in closer interactions between the oxygen atom of the amide and an arene ring in the ligand framework. A second C2- or Cs-symmetric species ([6-Cd]2−) is also present in the mixture, whose concentration increases with further addition of S8. Due to the symmetry of this complex and its formation from [2-Cd]2−, we currently assign this species as the bis(tetrasulfanide) complex shown in Scheme 3 but cannot rule out sulfur rearrangement within this complex. These mixtures are assigned as equilibrium mixtures rather than slow, incomplete reactions, as the NMR spectra measured initially upon S8 addition do not change over 12 h.
As these species exist in dynamic exchange with [1-Cd]2− (at lower S8 concentrations) and with excess S8, we have so far been unable to cleanly isolate these complexes or to characterize them by XRD. However, ESI-MS of these mixtures are consistent with this assignment (Fig. S44–S47). For example, ESI-MS of a mixture of [1-Cd]2− and 5/8 S8 shows molecular ion peaks at 587.8581 m/z corresponding to [2-Cd]2− + H (with three added S atoms) and at 683.7771 m/z, corresponding to [6-M]2− + H, although additional ion peaks corresponding to sulfur–sulfur fragmentation are also observed. These signals shift as expected when isotopically enriched 34S8 is used. DOSY NMR of this mixture is also consistent with the assigned monometallic structures, with both species exhibiting a diffusion coefficient of 1.73 × 10−10 m2 s−1.
Using these proposed stoichiometries, the equilibrium constants for the formation of [2-M]2− (K1) and [6-M]2− (K2, M = Cd, Hg) were calculated by integration of the 1H NMR spectra of mixtures containing [1-M]2−, [2-M]2−, and [6-M]2−, where
and
For the cadmium congener, these values were found to be KCd1 = 14 ± 4 M−⅜ and KCd2 = 1.1 ± 0.1 M−⅜. For the mercury complex, these values were KHg1 = 7 ± 2 M−⅜ and KHg2 = 5 ± 1 M−⅜. These equilibrium constants differ from those of sulfur insertion into the Zn–S bond of [1-Zn]2−. For the zinc congener, the first sulfur insertion reaction exhibits a high equilibrium constant and is complete even upon addition of 3/8 equiv. of S8 (KZn1 ≫ KCd1 > KHg1). The second sulfur insertion process is not observed for the zinc complex (KZn2 ≪ KCd2 < KHg2).
If the polysulfanide mixtures of [2-Cd]2− and [6-Cd]2−or of [2-Hg]2− and [6-Cd]2− in DMSO are heated in the presence of moisture, protonolysis and demetallation occur alongside ligand oxidation, forming a previously reported trisulfide-bridged bis(carboxamide)pyridine framework.17 When heated under anhydrous conditions, [Et4N]2[2-Cd] converted to a new D2-symmetric product (1H NMR spectroscopy, [7]2−). The XRD structure of [Et4N]2[7] shows the anion to contain a six-coordinate cadmium complex in which two pyridine carboxamide ligands are bridged by trisulfide moieties (Fig. 5). A similar zinc congener was previously reported upon the treatment of [Et4N]2[2-Zn] with the electrophilic alkyne dimethyl acetylenedicarboxylate.17 As the formation of this pseudo-octahedral complex corresponds to a formal oxidation of the bis(carboxamide)pyridine dithiolate ligand and reduction of sulfur, the byproduct is presumed to be precipitated CdS. Similarly, when a solution of [Et4N]2[6-Hg] was heated under anhydrous conditions, HgS was observed as a byproduct (power X-ray diffraction, Fig. S41), along with a demetallated trisulfide-bridged bis(carboxamide)pyridine compound.17
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| Fig. 5 Solid-state structure of [Et4N]2[7] as 50% probability ellipsoids. Tetraethylammonium countercations, hydrogen atoms, and a water molecule not shown for clarity. | ||
Since no experimental crystal structures could be obtained for the complexes [2-Cd]2− and [6-Cd]2− (Scheme 3), the change in Gibbs free energy (ΔG) for the two proposed sulfur insertion steps was calculated (eqn (2)).
![]() | (2) |
For the formation of [2-Cd]2− from [1-Cd]2−, the Gibbs free energy was found to be −20.7 kJ mol−1. The energy of the second insertion step to form [6-Cd]2− from [2-Cd]2− was found to be −25.7 kJ mol−1. These calculations show that both sulfur insertion steps are favorable, consistent with the experimental results. However, these calculated energies are higher than expected, based on the observed equilibrium constants KCd1 and KCd2.
We also considered a second possible isomer of the C1-symmetric 3 S-atom insertion product, in which two sulfur atoms insert at one thiolate arm, and one sulfur atom inserts at the second ([2′-Cd]2−, Scheme 4). Based solely on the calculated Gibbs free energies, the formation of both [2-Cd]2− and [2′-Cd]2− seems thermodynamically feasible, with [2-Cd]2− as the more stable isomer by −6.4 kJ mol−1. This assessment does not take any reaction barriers into account.
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| Scheme 4 Possible products of sulfur insertion into the Cd–S(thiolate) bonds of [1-Cd]2− at ωB97X-D4/def2-QZVPPD/SMD(dmso)//ωB97X-D4/def2-TZVPPD/SMD(dmso) level of theory. | ||
For further insights, the frontier molecular orbitals were considered as shown in Fig. 6. The lowest unoccupied molecular orbital (LUMO) shows strongly ligand-centered character on the pyridine backbone of the ligand for all cadmium complexes considered ([1-Cd]2−, [2-Cd]2−, [2′-Cd]2− and [6-Cd]2−). However, the highest occupied molecular orbitals (HOMO) vary after sulfur insertion. The HOMO of the dithiolate complex [1-Cd]2− is localized on the sulfur atoms of the thiolate donors, consistent with the observed nucleophilic reactivity of this complex. Similarly, the HOMO of [2-Cd]2− is centered on the sulfur of the remaining thiolate donor, with little contribution from the sulfur atoms of the tetrasulfanide moiety. In contrast, the HOMO of complex [2′-Cd]2− shows contribution from both the trisulfanide and disulfanide “arms” of the complex.
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| Fig. 6 Frontier molecular orbitals for the most stable conformers of Cd complexes at ωB97X-D4/def2-QZVPPD/SMD(dmso)//ωB97X-D4/def2-TZVPPD/SMD(dmso) level of theory (isovalue = 0.05). | ||
As a qualitative analysis of these frontier orbital pictures, the HOMO of [1-Cd]2− appears to be consistent with the formation of either [2-Cd]2− or [2′-Cd]2− upon nucleophilic attack of the thiolate groups of [1-Cd]2− on an S8 molecule. However, as the second sulfur insertion step forms a C2- or Cs-symmetric complex such as [6-Cd]2−, we favor the intermediacy of structure [2-Cd]2− as the product of the first sulfur insertion step. Based on the HOMO of [2′-Cd]2−, there appears to be little electronic distinction between the two “arms” of the complex, possibly resulting in a greater mixture of products upon a second sulfur insertion step. This rough analysis does not account for thermodynamically-driven exchange, however.
As discussed above, we presume that the sulfur insertion reaction proceeds by nucleophilic attack of the thiolate moiety on S8, followed by S8 ring-opening. The thiolate moieties of [1-Zn]2− are more nucleophilic than those of [1-Cd]2− and [1-Hg]2−, as might be predicted from metal–sulfur covalency. However, as sulfur insertion into the metal thiolate complexes has been demonstrated to undergo fast exchange, the resulting tetrasulfanide complexes are thermodynamically stabilized rather than kinetically trapped.17 For these reasons, the nucleophilicity of the thiolate moiety is unlikely to be the major influence over metal-dependent sulfur reactivity. Similarly, when considering the thiolate oxidation potential as a proxy for electron availability, the minor shifts in potentials upon metal substitution are not consistent with the observed differences in sulfur insertion reactivity.
We hypothesize that the different geometries around the metal centers are the major factor influencing sulfur insertion reactivity, as these likely also affect the resulting stability of the polysulfanide products as well as the strain of the initial thiolate chelate itself. We have previously demonstrated that for tris(pyrazolyl)borate-supported zinc thiolate complexes, only the strained chelating 2-thiopyridine derivative was observed to insert sulfur upon treatment with S8.5 Although [1-Zn]2−, [1-Cd]2−, and [1-Hg]2− all show similar C2-symmetric geometries, the ∠S–M–S angles increase from Zn to Cd to Hg, perhaps indicating a decrease in thiolate–thiolate repulsion. When [1-Zn]2− reacts with S8 to form [2-Zn]2−, the ∠S–Zn–S angle increases from 102.64(3)° to 106.66°, showing a decrease in this sulfur–sulfur interaction. Sulfur insertion is less favored for [1-Cd]2− and [1-Hg]2− due to less of this repulsion within the dithiolate complexes. Similarly, for these reasons, sulfur insertion into the second thiolate arm is close in energy to that of sulfur insertion into the first thiolate arm, therefore forming two types of polysulfanide products.
Although this present study serves primarily as a simple description of coordination chemistry differences, these results may have broader implications for biological metal–thiolate motifs. For example, metallothioneins bind zinc, cadmium, and mercury, but have also been proposed to undergo persulfidation.31 While the regulatory role of such structures have yet to be determined, our results may indicate that metal substitution would affect incorporation of sulfane sulfur.
1H and 13C NMR spectra were recorded on Bruker 400 MHz, Bruker 500 MHz, or Varian 600 MHz instruments, with chemical shifts referenced to the residual solvent peaks (1H, δ 2.50 ppm and 13C, δ 39.5 ppm for DMSO-d6; 1H, δ 7.26 ppm and 13C, δ 77.16 ppm for CDCl3; 1H, δ 1.94 ppm for CD3CN). 113Cd NMR spectra were externally referenced to Cd(ClO4)2 in H2O (δ −640.27 ppm) and 31P NMR spectra were referenced to phosphoric acid (H3PO4, δ 0 ppm). Elemental analyses were performed by Midwest Microlabs, LLC, in Indianapolis, IN.
Caution! Cadmium and mercury compounds are highly toxic and should be handled with appropriate care.
[Et4N]2[1-Cd]. Yield: 0.314 g (64%). 1H NMR (400 MHz, DMSO-d6) δ 8.17–8.05 (m, 3H), 7.74 (dd, J = 7.5, 2H), 7.24 (dd, J = 7.5, 2H), 6.67 (td, J = 7.5, 2H), 6.51 (td, J = 7.5, 2H), 3.13 (q, J = 7.2, 16H), 1.19–1.01 (t, J = 7.2, 24H). 13C NMR (101 MHz, DMSO-d6): δ 161.44, 152.10, 147.40, 143.60, 139.54, 131.64, 123.48, 121.06, 119.49, 119.42, 51.35, 7.02. 113Cd NMR (89 MHz) δ −138.81. Anal. calcd for C35H51N5O2S2Cd: C, 56.02; H, 6.85; N, 9.33. Found: C, 56.01; H, 6.86; N, 9.35.
[Et4N]2[1-Hg]. Yield: 0.490 g (56%). 1H NMR (400 MHz, DMSO-d6) δ 8.16 (dd, J = 8.2, 2H), 8.05 (dd, J = 8.2, 1H), 7.71 (dd, J = 7.8, 2H), 7.27 (dd, J = 7.8, 2H), 6.71 (, J = 7.4, 2H), 6.54 (t, J = 7.4, 2H), 3.13 (q, J = 7.2 Hz, 16H), 1.15 (t, J = 7.2 Hz, 24H). 13C NMR (101 MHz, DMSO-d6) δ 161.74, 152.09, 147.30, 141.84, 138.41, 130.91, 123.73, 121.29, 120.00, 119.12, 51.35, 7.02. Anal. calcd for C35H51N5O2S2Hg: C, 50.13; H, 6.13; N, 8.35. Found: C, 50.12; H, 6.01; N, 8.43.
[Et4N][4Me-Cd(CH3CN)]. [Et4N]2[1-Cd] (0.469 g, 0.63 mmol, 1 equiv.) and CH3CN (20 mL) and MeI (38.9 μL, 0.63 mmol, 1 equiv.) was added by Hamilton syringe. Yield: 0.240 g (60%). 1H NMR (400 MHz, DMSO-d6) δ 8.72 (d, J = 7.7 Hz, 1H), 8.20 (t, J = 8.7 Hz, 1H), 8.15 (d, J = 7.4 Hz, 1H), 7.30 (d, J = 7.4 Hz, 1H), 7.24 (td, J = 8.0, 1H), 7.08 (t, J = 8.0 Hz, 1H), 6.96 (t, J = 8.0, 1H), 6.70 (t, J = 8.0 Hz, 1H), 6.50 (t, J = 7.4 Hz, 1H), 3.15 (q, J = 7.2 Hz, 8H), 2.37 (s, 3H), 1.21–1.02 (q, J = 7.2, 12H). 13C NMR (101 MHz, DMSO-d6) δ 161.38, 152.19, 149.87, 148.23, 145.93, 140.38, 139.29, 131.66, 131.32, 125.59, 125.41, 124.46, 122.24, 121.79, 121.62, 121.49, 120.88, 119.36, 51.41, 51.38, 51.35, 15.71, 7.05. 113Cd NMR (89 MHz) δ −275.60.
[Et4N][4Me-Hg(CH3CN)]. [Et4N]2[1-Hg] (0.724 g, 0.86 mmol, 1 equiv.) and CH3CN (15 mL) and MeI (54 μL, 0.86 mmol, 1 equiv.) was added by Hamilton syringe. Yield: 0.384 g (53%). 1H NMR (400 MHz, DMSO-d6) δ 8.71 (d, J = 8.0 Hz, 1H), 8.28 (dd, J = 8.0 Hz, 1H), 8.21–8.11 (m, 2H), 7.36–7.23 (m, 3H), 7.20–7.01 (m, 2H), 6.80 (t, J = 7.6 Hz, 1H), 6.58 (t, J = 7.6 Hz, 1H), 3.17 (q, J = 7.2 Hz, 8H), 2.39 (s, 3H), 1.18–1.07 (t, J = 7.2 Hz, 12H). 13C NMR (101 MHz, DMSO-d6) δ 163.00, 161.88, 151.35, 147.33, 147.13, 144.53, 140.41, 132.39, 131.26, 129.44, 126.48, 125.65, 124.66, 123.43, 123.38, 122.71, 122.44, 121.53, 51.40, 51.37, 51.34, 14.84, 7.03.
[Et4N]2[4Me-Cd(Stol)]. [Et4N][4Me-Cd(CH3CN)] (0.210 g, 0.33 mmol, 1 equiv.) and CH3CN (5 mL). [Et4N][Stol] (0.083 g, 0.33 mmol, 1 equiv.) was added as a solution in CH3CN (2 mL). Yield: 0.234 g (81%). 1H NMR (400 MHz, DMSO-d6) δ 8.41 (d, J = 7.4 Hz, 1H), 8.09 (m, 3H), 7.27 (d, J = 8.3 Hz, 1H), 7.05 (d, J = 7.4 Hz, 1H), 6.96–6.82 (m, 2H), 6.68 (d, J = 8.3 Hz, 2H), 6.47 (t, J = 7.4 Hz, 1H), 6.33–6.19 (d, J = 8.3 Hz, 1H), 3.08 (q, J = 7.2 Hz, 16H), 2.24 (s, 3H), 1.96 (s, 3H), 1.04 (t, J = 7.2 Hz, 24H). 13C NMR (101 MHz, DMSO-d6) δ 161.24, 153.40, 147.15, 139.05, 132.16, 131.77, 127.34, 123.61, 122.10, 121.49, 121.06, 119.93, 118.99, 118.09, 51.43, 51.40, 51.37, 40.20, 39.99, 39.78, 39.57, 39.36, 39.15, 38.94, 25.15, 20.33, 7.06. 113Cd NMR (89 MHz) δ −178.03. Anal. calcd for C43H61N5O2S3Cd: C, 58.12; H, 6.92; N, 7.88. Found: C, 58.59; H, 6.95; N, 7.70.
[Et4N]2[4Me-Hg(Stol)]. [Et4N][4Me-Hg(CH3CN)] (0.105 g, 0.32 mmol, 1 equiv.) and CH3CN (5 mL). [Et4N][Stol] (0.037 g, 0.32 mmol, 1 equiv.) was added as a solution in CH3CN (2 mL). Yield: 0.107 g (77%). 1H NMR (400 MHz, DMSO-d6) δ 8.38 (d, J = 7.6 Hz, 1H), 8.25 (d, J = 7.6 Hz, 1H), 8.12 (d, J = 7.3 Hz, 1H), 7.95 (t, J = 7.3 Hz, 1H), 7.57 (d, J = 7.3 Hz, 1H), 7.32 (d, J = 7.3 Hz, 1H), 6.97 (d, J = 7.3 Hz, 1H), 6.9–6.74 (m, 5H), 6.72 (t, J = 6.5 Hz, 1H), 6.53 (t, J = 6.5 Hz, 1H), 6.44 (d, J = 8.1 Hz, 2H), 3.07 (q, J = 7.2 Hz, 16H), 2.24 (s, 3H), 2.02 (s, 3H), 1.04 (t, J = 7.2 Hz, 24H). 13C NMR (101 MHz, DMSO-d6) δ 162.73, 162.42, 154.29, 153.41, 150.51, 146.82, 137.49, 133.32, 131.22, 130.80, 128.94, 127.82, 124.52, 123.41, 123.02, 122.58, 122.34, 121.99, 121.15, 120.14, 118.78, 51.57, 51.54, 51.51, 20.44, 14.44, 7.19. Anal. calcd for C43H61N5O2S3Hg: C, 53.65; H, 6.39; N, 5.82. Found: C, 53.91; H, 6.21; N, 5.41.
CCDC 2521016–2521020 ([Et4N]2[1-M], [Et4N]2[4Me-M(Stol)] (M = Cd, Hg), and [Et4N]2[7]) contain the supplementary crystallographic data for this paper.33a–e
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