Jagodish C.
Sarker
ab,
Rosie
Nash
a,
Suwimon
Boonrungsiman
c,
David
Pugh
a and
Graeme
Hogarth
*a
aDepartment of Chemistry, King's College London, Britannia House, 7 Trinity Street, London SE1 1DB, UK. E-mail: graeme.hogarth@kcl.ac.uk
bDepartment of Chemistry, Jagannath University, Dhaka-1100, Bangladesh
cCentre for Ultrastructural Engineering, King's College London, New Hunt's House, London SE1 1UL, UK
First published on 9th August 2022
Air and moisture stable diaryl dithiocarbamate salts, Ar2NCS2Li, result from addition of CS2 to Ar2NLi, the latter being formed upon deprotonation of diarylamines by nBuLi. Oxidation with K3[Fe(CN)6] affords the analogous thiuram disulfides, (Ar2NCS2)2, two examples of which (Ar = p-C6H4X; X = Me, OMe) have been crystallographically characterised. The interconversion of dithiocarbamate and thiuram disulfides has also been probed electrochemically and compared with that established for the widely-utilised diethyl system. While oxidation reactions are generally clean and high yielding, for Ph(2-naphthyl)NCS2Li an ortho-cyclisation product, 3-phenylnaphtho[2,1-d]thiazole-2(3H)-thione, is also formed, resulting from a competitive intramolecular free-radical cyclisation. To demonstrate the coordinating ability of diaryl dithiocarbamates, a small series of Co(III) complexes have been prepared, with two examples, [Co{S2CN(p-tolyl)2}3] and [Co{S2CNPh(m-tolyl)}3] being crystallographically characterised. Solvothermal decomposition of [Co{S2CN(p-tolyl)2}3] in oleylamine generates phase pure CoS2 nanospheres in an unexpected phase-selective manner.
Diarylamines are significantly less basic than their dialkyl or alkyl–aryl counterparts, as seen from a comparison of aqueous pKa values for Et2NH (10.98), PhEtNH (4.17) and Ph2NH (0.79). Consequently, and despite a number of reports to the contrary,9–12 diaryl-DTCs cannot be prepared upon addition of the amine to CS2 in the presence of alkali metal hydroxides or tertiary amines. The synthesis of NaS2CNPh2 has been reported upon addition of excess NaH to Ph2NH followed by CS2 addition,13–15 and also from the (slow) reaction (ca. 24 h) of Ph2NH with NaNH2 (again followed by CS2 addition) in benzene,16,17 but in our hands the NaH route has proved difficult to reproduce. In 1995, Snaith and co-workers reported a high yielding synthesis of LiS2CNPh2 from the reaction of Ph2NLi with CS2 in toluene, the amide being generated upon deprotonation of Ph2NH by nBuLi at −70 °C (Scheme 1b).18 While this synthesis must be carried out under an inert atmosphere, the high yields and simple work-up procedure were appealing to us, and others have also identified the utility of this route.19,20
A current focus is the use of DTC complexes as single source precursors (SSPs) towards nanoscale metal-sulfides.21–26 We, and others, have focused almost exclusively on the use of dialkyl-DTC derivatives,27 and as far as we are aware there are no substantiated reports of the use of diaryl-DTC complexes as SSPs. Herein we describe the synthesis and characterisation of a small series of diaryl-DTC salts, together with initial studies on the formation of thiuram disulfides (TDS), themselves useful precursors to metal–DTC complexes.28 We also report the synthesis of octahedral d6-cobalt(III) complexes, which serve as exemplars for this type of ligand coordination, and their use as SSPs, decomposing in oleylamine to afford CoS2 nanomaterials.
All show a low field signal at ca. 219 ppm in the 13C{1H} NMR spectrum, being associated with the quaternary backbone carbon of the DTC, the position of which varies little upon changing substituents. This can be compared with that for NaS2CNEt2 at ca. 207.5 ppm.30 Other signals in both the 1H NMR and 13C{1H} NMR spectra are similar to those in the parent amines. IR spectra of dialkyl-DTCs contain peaks associated with ν(C–N) in the range of 1450–1580 cm−1 and between 940–1060 cm−1 associated with the asymmetric ν(C–S).1,30 For 1a, these absorptions are seen at 1490 and 1045 cm−1 respectively. Electrospray ionisation mass spectrometry (ESI-MS) data for 1 do not show a molecular ion, but base peaks are consistent with Ar2NCS2+ fragments (i.e. M+ − Li).
We did not attempt to characterise 1 by X-ray diffraction but note that in Snaith's original paper he reports the structure of 1a recrystallised from THF.18 This shows the coordination of two molecules of THF and confirms the chelate nature of the DTC, with lithium adopting a distorted tetrahedral geometry. The C–N bond of 1.364(3) Å shows some degree of double bond character and can be compared to that of ca. 1.33–1.36 Å in dialkyl DTCs and 1.41–1.44 Å in pyrrole and pyrrolidine DTCs.31 Importantly the two phenyl rings are orientated approximately perpendicular to the LiS2CN plane (ca. 80–87°) suggesting that there is no conjugation of the aryl groups with the DTC functionality. Thus, while these substituents can still be considered as electron-withdrawing, as noted from the 13C{1H} NMR chemical shift, they are not fully conjugated. This view is also supported by the UV-vis spectrum of 1b which shows two strong absorptions at 263 and 293 cm−1 for 1b being associated with π–π* transitions characteristic of the NCS2 moiety,31 being comparable with those of simple dialkyl-DTC salts. In contrast, carbazole-DTCs, in which the aromatic ring is constrained to lie in the same plane as the NCS2 unit, also show a third band at ca. 340–350 nm attributed to intramolecular charge transfer from the NCS2 group to the aromatic ring, a feature missing from the UV-vis spectrum of 1.
While the route for preparation of diaryl DTCs using nBuLi is convenient and high yielding, the use of a pyrophoric base under inert conditions means that it cannot be used in less well-equipped laboratory environments. A number of groups have previously reported the formation of KS2CNPh2 from reaction of Ph2NH and CS2 in the presence of KOH,32–34 but as was the case for NaOH, in our hands this reaction did not work. Tatsumi and co-workers reported that KNPh2 can be prepared from HNPh2 and KOtBu in THF35 and taking inspiration from this, we stirred a solution of (p-tolyl)2NH, KOtBu and CS2 in THF for 24 h at room temperature, which gave a yellow suspension affording KS2CN(p-tolyl)2 (1h), small pale-yellow crystals in 70% yields after workup. Characterising data are similar to that of the lithium salt 2b, the quaternary carbon appearing at 218.3 ppm. Thus, while we have not developed the KOtBu route is seems accessible and applicable in a non-specialist laboratory setting. We also note that the phosphonium salt [PPh4][S2CNPh2]36 has been reported, being prepared upon mixing stoichiometric amounts of [Ph4P]Br and NaS2CNPh2 in MeCN, but 13C{1H} NMR data were not given.
We chose K3[Fe(CN)6] as the oxidising agent since it is self-indicating (Scheme 3).45 Dropwise addition of an aqueous solution of K3[Fe(CN)6] (ca. 0.6 M) to 1a–g suspended in water resulted in formation of off-white precipitates. These were taken up in CH2Cl2, separated from the water, and dried to afford 2a–g in ca. 50–80% yields. We suspect that reactions proceed in high (ca. quantitative) yields but isolating the product is not always simple. Thus, solids are quite “claggy” and not easily separated by filtration, while their solubility in CH2Cl2 varies depending upon the substituents. Once isolated, they are dry off-white solids that can be stored indefinitely in air. In the 13C{1H} NMR spectrum, the quaternary backbone carbon is now seen at ca. 197 ppm and 1H NMR spectra are somewhat broader than those for the diaryl-DTC salts, presumably resulting from restricted rotation about the S–S bond.
Unlike other diaryl-DTCs, the 2-naphthyl-N-phenyl derivative 1g oxidised to give a mixture of the expected Ar4TDS 2g, along with a red ortho-cyclisation product, 3-phenylnaphtho[2,1-d]thiazole-2(3H)-thione, C17H11NS2 (2h) (Scheme 4). Thus, after crystallisation a mixture of crystals of 2g and 2h resulted which were separated manually. While 2h has been described in the literature, being prepared in 74% yield upon refluxing 3-phenyl-6,7-benzobenzothiazolone and P2S5 in xylene, no characterising data was presented.46 Benzothiazolethiones show interesting biological properties and are normally prepared from the corresponding 1-iodo, 2-amino arenes.47,48 Elemental analysis, IR and 1H and 13C{1H} NMR data are consistent with the molecular formula, but very similar to those for 2g except the heterocyclic thioketo group, –S–CS signal in the 13C{1H} NMR spectrum which appears at δ 197.5, while the thioureide signal in 2h is at δ 189.5. A plausible mechanism of co-formation of 2g and 2h is shown (Scheme 4). Presumably, the close proximity of the ortho-naphthyl proton to the sulfur centre allows a competitive intra-molecular radical addition reaction alongside the expected radical dimerization.
In a similar manner to the reactions with dialkyl-DTC salts, addition of cobalt(II) acetate to ca. three equivalents of 1a–g in water resulted in immediate formation of a green precipitate and simple work up afforded high yields (ca. 90%) of green [Co(S2CNAr2)3] (3a–g) (Scheme 5). Due to the quadrupolar effect of cobalt, NMR signals are broad, and the quaternary carbon signal was not visible in 13C{1H} NMR spectra, while signals in 1H NMR spectra did not show JHH couplings. Each gave a molecular ion peak in the EIMS and elemental analyses and IR spectra are fully consistent with proposed formulations.
![]() | ||
Fig. 1 Molecular structures of (a) one conformer of 2b and (b) 2c showing 50% probability thermal ellipsoids with hydrogen atoms omitted for clarity. |
![]() | ||
Fig. 2 Molecular structure of one (of six) independent molecules of 2h showing 50% probability thermal ellipsoids. |
![]() | ||
Fig. 3 Molecular structures of (a) [Co{S2CN(p-tolyl)2}3] (3b) and (b) [Co{S2CNPh(m-anisyl)2}3] (3e). |
Molecular structures of a number of dialkyl50–55 and alkyl–aryl TDS56,57 have previously been reported and gross structural features of diaryl derivatives are similar. The structure of 2c is crystallographically straightforward (Fig. 1b) its centrosymmetric nature and C–S–S–C torsional angle of 180° being previously observed for iPr4TDS.53 In contrast, that of 2b is more complicated as there is a whole-molecule disorder (Fig. 1a). Thus, there are two orientations in a ca. 84:
16 ratio (major form is shown) differing with respect to the C–S–S–C torsional angle [97.7(1) and −104.3(1)°]. These can be compared with the C–S–S–C torsion angles of 85.8° (R = iBu),52 96.4° (R = Et)50 and 89.27° (R = CH2CH2OMe).52 A second important metric parameter is the S–S bond distance which is normally ca. 2.0 Å. Distances of 2.0139(4) and 2.0861(6) Å in 2b and 2c respectively are slightly longer than those found in the dialkyl derivatives, while in the ethyl-phenyl derivative it is similar at 2.0112(5) Å.57
The molecular structure of one independent molecule of 2h is shown in Fig. 2. Crystallographically it is unusual as there are six independent molecules in the asymmetric unit but fortunately (and somewhat remarkably) there is no disorder. The major difference between the six is the dihedral angle between the plane of the phenyl ring and the plane defined by the 13 atoms of the activated naphthyl group.
Many Co(III) DTCs have been characterised crystallographically57–64 and in all the metal adopts a distorted octahedral coordination environment with average Co–S bond lengths of ca. 2.26 Å. White and co-workers60 showed that the effects of different alkyl substituents on the structures of [Co(S2CNR2)3] is minor. This is also true for bis(p-tolyl) (3b) and Ph(m-anisyl) (3e) analogues (Fig. 3). [For 3e each molecule contains a disordered m-anisyl group.] Average S–Co–S bite angle and trans S–Co–S angles are 77.06 (2), 164.46(2) 3b; and 76.53(2), 166.82(2) 3e being very similar to those in dialkyl-derivatives. Dihedral angles do change significantly when aryl groups are introduced. Thus, dihedral angle between alkyl/aryl groups are ca. 1.3°,63 17.1 for EtH,58ca. 74 for EtPh,57ca. 77° for 3b and ca. 70° for 3e.
Fig. 4 displays experimental electrochemical data for 1b–2b and maintain the key characteristics of the dialkyl redox behaviour. At 0.5 V s−1 (in MeCN), reduction of 2b occurs at Epeak(a) = −2.02 V (vs. Fc+/0); a 260 mV cathodic shift as compared to that seen for Et4TDS (Fig. S1†). Scanning back in the positive direction leads to the expected oxidation of the [DTC]− that is generated at the electrode upon cleavage of [TDS]−. For 1b this oxidation occurs at Epeak(c) = −0.298 V, as compared to Epeak(c) = −0.348 V for [Et2DTC]−. The peak separation for 2b is 1.722 V, being around 210 mV smaller than the 1.932 V peak separation observed for Et4TDS under these conditions. At slower scan rates (<0.1 V s−1), back oxidation of 2b is not observed, which suggests an instability of the 1b at the electrode surface. This is in contrast to Et4TDS where back-oxidation is seen at <0.05 V s−1. At suitably high scan rates (>2.0 V s−1) a broad plateau is observed ca. −1.4 V, a feature also present (but not as distinct) for slower scan rates, as well as for Et4TDS. This may result from reduction of the DTC radical, which could be stabilised by the delocalised electron character of the aryl groups, which is very similar to the proposed model as well as the experimental results for iPr4TDS.71,72
Nomura and Nakai first reported the use of a cobalt DTC complex as SSPs in 2003, showing that chemical vapour deposition (CVD) of [Co(S2CNEt2)3] at 450 °C gave thin films of cubic Co9S8.76 Soon after, O'Brien and co-workers reported the deposition of a phase pure Co3S4 film from [Co(S2CNMeHex)3] at 450 °C.77 Solvothermal decomposition of cobalt DTCs has not been widely studied. Thirumaran and co-workers decomposed furfuryl complexes [Co(S2CNR2)3] and [Co(S2CNRBz)3] (R = CH2C4H3O) in triethylenetetramine to give nanorods of Co3S4,78 while Revaprasadu and co-workers have reported that hot injection (HI) of [Co(S2CNC8H8O)3] in oleylamine (OLA) affords nanoplates of CoS.79 There are also reports of Co(II) complexes [Co(S2CNR2)2]80–84 being used as SSPs, although as these are extremely oxygen sensitive, they are most likely to be the Co(III) complexes.1 Most notably, ultra-thin, defect-rich, Co9S8 nanosheets have been prepared by Li and co-workers from decomposition of (putative) [Co(S2CNBu2)2] at 220 °C in oleic acid in the presence of excess PPh3.85 Importantly, as far as we are aware, cobalt DTC SSPs have not previously been used to generate CoS2.
To this end we have carried out preliminary studies on the solvothermal decomposition of 3b in oleylamine (OLA) using heat up (HU) and hot-injection (HI) methods. At room temperature 3b is partially soluble in OLA and as the temperature is increased it slowly dissolves to give an ever-darker green solution which is clear (indicative of stability) up to ca. 180 °C. Above this temperature, the solution turns black and becomes darker as the temperature is raised to ca. 230 °C being maintained there for 1 h. After slowly cooling to room temperature, MeOH was added to precipitate the generated black nanoparticles, which were isolated by standard procedures (see Experimental section). For HI process, OLA (15 mL) was heated to 230 °C for 15 min and 3b (300 mg in 5 mL OLA at 80 °C) injected into the flask. Immediately, the colour changed from green to black and the solution was maintained at 230 °C for 1 h followed by standard workup.
Powder XRD (Fig. 5) of both samples from HU and HI revealed the crystalline phase of the decomposed black powders to be CoS2 (cattierite). The peak at 46.7°2θ for the (220) lattice plane is more intense than in the reference pattern, suggesting preferred growth in this direction. A small peak at ca. 26° is unaccounted for. TEM images (Fig. 6) for particles generated by the HI method show that they are predominantly nanospheres with an average diameter of 580 nm. Unfortunately, we have been unable to record suitable TEM images of the HU sample to date.
The important finding here is that solvothermal decomposition in OLA of 3b cleanly affords CoS2 nanospheres. An aim of our work is to understand the molecules to materials process and in previous work on di-iso-butyl DTCs of Ni(II),24,25 Zn(II)21 and Fe(III)23 we have utilised in situ EXAFS studies and DFT calculations to probe decomposition mechanism(s). Unfortunately we have not yet been able to do this for Co(III) complexes, but can reflect on findings for the closely related d5 complex [Fe(S2CNiBu2)3].23 This shows three distinct decomposition steps; (i) amine coordination with formation of monodentate DTC ligands (up to 60 °C), (ii) reductive-elimination of DTC to afford Fe(II) species above 90 °C, (iii) amine-exchange to generate [Fe(S2CNHR)(S2CNR2)] and/or [Fe(S2CNHR)2] which rapidly decompose to iron sulfides. For [Co(S2CNAr2)3] a major difference is the high crystal field stabilisation energy (CFSE) resulting from the low spin d6 configuration, while [Fe(S2CNR2)3] and [Fe(S2CNAr2)3] are spin cross-over complexes, and likely the high spin (CFSE = 0) form is that which decomposes.23 The high CFSE of 3b is seen in the maintenance of its structural integrity up to ca. 180 °C, as evidenced by the lack of colour change or any turbidity noted in the HU process. Thus, decomposition probably occurs catastrophically above 180 °C, which is supported by the similar product formation from HU and HI methods. With the accessibility of Co(II) bis(dithiocarbamate) complexes, it is tempting to suggest that reductive-elimination of TDS is the first step in this process (following from that established for iron), being followed by the fast amine-exchange to give afford [Co(S2CNHR)2] (R = oleyl) which in turn rapidly eliminates two equivalents of RNCS to leave CoS2. Thus, we have previously established that while amine-exchange is fast at four-coordinate centres, it is much slower at six-coordinate centres, something we have rationalised in terms of an intramolecular process requiring metal pre-coordination of the primary amine (Scheme 7).27
Exclusive formation of CoS2 upon decomposition of 3b in OLA contrasts with the report of Revaprasadu and co-workers who heated [Co(S2CNC8H8O)3] in the same solvent to form hexagonal CoS at both 200 and 260 °C.79 They did, however, note that the quality of their PXRD data was poor and thus there is some uncertainty over this assignment. Interestingly, when the same SSP was studied by TGA the residue mass was consistent with formation of CoS2. Clearly further work is required here but the preliminary data suggest that Co(III) diaryl-DTC complexes may be a fruitful source of CoS2 and we are currently carrying out further decomposition experiments on 3a–g while also targeting aniline-derived complexes [Co(S2CNHAr)3] which have briefly been mentioned in the literature85 but have not been considered as SSPs.
Footnote |
† Electronic supplementary information (ESI) available. CCDC 2175344–2175348. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d2dt01767a |
This journal is © The Royal Society of Chemistry 2022 |