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. Author manuscript; available in PMC: 2011 Oct 15.
Published in final edited form as: Inorganica Chim Acta. 2010 Oct 15;363(12):2857–2864. doi: 10.1016/j.ica.2010.04.004

Synthesis, characterization, spectroscopy, electronic and redox properties of a new nickel dithiolene system

Partha Basu 1,*, Archana Nigam 1, Benjamin Mogesa 1, Suzanne Denti 1, Victor Nemykin 2
PMCID: PMC2967771  NIHMSID: NIHMS206246  PMID: 21057604

Abstract

A new dithiolene ligand with 3,5-dibromo substituted phenyl groups was designed and synthesized. The protected form of the ligand was reacted with a nickel salt providing neutral Ni(S2C2(3,5-C6H3Br2)2)2 and anionic [Ni(S2C2(3,5-C6H3Br2)2)2] isolated as a Bu4N+ salt. Both were characterized by UV-visible and IR spectroscopy and compared with the similar known molecular systems. They exhibit intense low-energy transitions that are characteristic of such systems. The electrochemical behavior of these molecules was investigated by cyclic voltammetry.

Introduction

The long standing interest in the development of sulfur coordinated nickel centers stems from their relevance in the biological systems as model complexes for the active sites of nickel enzymes as well as their application in material chemistry. Nickel complexes with sulfur donors are known to exhibit interesting properties such as metallic-conductivity,[1] optical nonlinearity,[2] ability to reversibly react with olefins through a redox couple leading to olefin purification,[3] and strong absorbance in the near infrared region suitable in laser Q-switch dyes.[4] Among these, bis-dithiolene complexes of nickel display important and unusual properties such as very intense electronic transition in the near IR region, capability to exist in different well-defined oxidation states that can be achieved reversibly, and electrical conductivity.[5] These square planar complexes exhibit a high degree of electron delocalization within the chelate ring involving the metal ion that significantly contributes to the low-energy electronic transition between the HOMO and the LUMO, which occurs at an unusually low energy. This extensive electron delocalization, while making these complexes useful as near-infrared (NIR) dyes, is irrelevant to intramolecular charge transfer, a crucial factor in generating second order non-linear optical properties. The delocalized system can exist in three distinct oxidation states: dianionic, monoanionic, and neutral that differ in their spectroscopic signature and magnetic properties. Significant early research has been conducted with unsubstituted or unbranched dithiolene system such as the maleonitrile (Figure 1: 3b and 3c). Phenyl substituted dithiolene ligands and their nickel complex was originally synthesized by Schrauzer,[6] which provides an entry towards substituted dithiolene system which can be tailored towards specific function with judicious choice of substituents.[7] A majority of the cases though the functionalization is done at the para position of the phenyl group attached to the dithiolene ligand. Herein we report the synthesis, characterization, redox and spectroscopic properties of a new dithiolene nickel system with 3,5-dibromo substituted phenyl groups. These bromo substitution set targets for further development of functionalized materials. These results are complemented with computational analyses using density functional theory. We also report the molecular structure of 3b.

Figure 1.

Figure 1

The compounds used in this investigation.

Experimental

Unless specified all experiments were performed using oven-dried glassware under inert atmosphere using Schlenk (argon) and dry box (nitrogen) techniques. Reagents used in this investigation were of analytical grade and they were purchased either from Aldrich or from Acros Chemical Company and used as received without further purification. Commercial grade solvents were dried and distilled before use: dioxane, hexane, and diethyl ether were dried and distilled over Na-benzophenone; methanol and ethanol were distilled over Mg-turnings; methylene chloride (CH2Cl2) was dried and distilled over CaH2; CH3CN was distilled over P2O5. Anhydrous N,N-dimethylformamide (DMF) was obtained from Acros chemicals. 3,5-dibromobenzaldehyde,[8] 2a,[6] 2b, 3b and 3c,[9] (Figure 1) were synthesized following reported procedures.

Room temperature 1H and 13C NMR spectra were recorded using a Bruker ACP-300 spectrometer at 300.133 MHz and 75.469 MHz frequencies, respectively. Mass spectra were recorded in a Waters LCQ ESI/APCI Quadrupole Mass spectrometer in ESI and/or APCI modes. Electronic spectra were recorded in Cary 3 or Cary 14 spectrophotometers. Infrared spectra were recorded on a Perkin-Elmer FT-IR 1760X spectrometer on NaCl plates or in KBr pellets. Electrochemical investigations were performed at room temperature using CV-50W voltammetric analyzer with a typical three-electrode system: platinum or graphite-working electrode, Ag/Ag+ -reference electrode, and Pt wire-auxiliary electrode. 0.1M Tetra butyl ammonium perchlorate (TBAP) was used as a supporting electrolyte. Redox potentials were referenced internally with ferrocenium/ferrocene (Fc+/Fc) couple. Magnetic susceptibility was measured on a Johnson-Matthey Evans balance, and conductivity was recorded on a VWR conductivity meter. Elemental analyses were performed at Midwest Microlab, LLC, Indianapolis, IN.

Syntheses of 3,3′,5,5′-tetrabromobenzoin and 3,3′,5,5′-tetrabromobenzil

First Method

3,5-dibromobenzaldehyde (300 mg, 1.14 mmol) was dissolved in ethanol (7 mL), which was mixed with an aqueous solution (4 mL) of KCN (36 mg, 0.57 mmol) and stirred for 10 min. The solution was heated overnight at 80 °C in a water bath, and the resulting solution was treated with aqueous NaHCO3 and extracted with chloroform followed by diethyl ether. Both organic layers were washed with saturated aqueous NaHSO3 solution and dried over anhydrous Na2SO4. Evaporation of the chloroform layer yielded a pale yellow solid (3,3′,5,5′-tetrabromobenzil, 110 mg, 0.21 mmol) and the ether layer yielded a yellow solid (3,3′,5,5′-tetrabromobenzoin, 50 mg, 0.094 mmol). 3,3′,5,5′-tetrabromobenzil: 1H NMR (CDCl3): δ= 8.05 (s, 2H, aromatic), 7.8 (s, 1H, aromatic); 13C NMR (CDCl3): δ= 164 (C=O), 138, 134, 131, 123 (aromatic); IR (KBr): 1642 (C=O); yield = 38%. 3,3′,5,5′-tetrabromobenzoin: 1H NMR (CDCl3): δ = 8.0 (s, aromatic), 7.8 (s, aromatic); 7.5 (s, aromatic), 6.4 (br, s, CHOH), 5.9 (br, s, CHOH); 13C NMR (CDCl3): δ= 164 (C=O), 142, 138, 134, 133, 131, 128, 122 (aromatic), 72 (CHOH); IR (KBr): 1727 (C=O). Yield: 17%.

Second Method

3,5-dibromobenzaldehyde (3.14 g, 11.89 mmol) was dissolved in 12 mL DMF in a Schlenk flask at room temperature. Tetra butyl ammonium bromide (0.32 g, 1.0 mmol) and KCN (0.015 g, 0.211 mmol) were added into the reaction mixture sequentially and the resulting solution was stirred at room temperature for 18–20 h. The solvent was removed by distillation and the resulting residue was poured into water (100 mL) and extracted with CH2Cl2. The organic extracts were washed with saturated NaCl solution and dried over anhydrous MgSO4. The gummy material obtained after evaporation of the solvent was crystallized at a low temperature by keeping the material in a refrigerator. The product was recrystallized using CH2Cl2/ethanol to obtain pure benzoin as a yellow solid. Yield: 30%, 1.87g (3.56 mmol).

Synthesis of Ni(S2C2(3,5-C6H3Br2)2)2 (1a)

A mixture of 3,3′,5,5′-tetrabromobenzil or tetrabromobenzoin 0.32 g (0.61 mmol), 2 equivalents of P4S10 (0.53 g, 1.19 mmol) and dry dioxane (7 mL) was placed in a 250 ml Schlenk flask. The reaction mixture was heated at 110 °C for 5–6 h, cooled, filtered to remove unreacted P4S10 and washed with minimum dioxane. To the filtrate, an alcoholic solution (5 mL) of NiCl2·6H2O (0.16g, 0.68 mmol) was added whereby the color changed to reddish brown. The solution was refluxed with stirring at 90 °C for 2 h, and the reaction flask was capped and kept in refrigerator for 20 h. Excess P4S10 precipitated out and was centrifuged and a clear reddish brown solution was evaporated. The residue was dissolved in a minimal quantity of CH2Cl2, and the target compound was precipitated as a green crystalline material by adding methanol. Yield: 12%, 0.082 g (0.07 mmol). Absorption spectrum: (CH2Cl2) λmax, nm (ε, M−1cm−1): 270 (43000), 316 (60000), 383 (sh, 11800) 582 (2200), 834 (30660); ESIMS (−): 1173 (100%), calculated for C28H12S4Br8Ni (M), 1173.

Synthesis of (Bu4N)[Ni(S2C2(3,5-C6H3Br2)2)2] (1b)

The reaction was carried out similar to that for the synthesis of 1a. A mixture of 3,3′,5,5′-tetrabromobenzil or tetrabromobenzoin (0.94 g, 1.79 mmol), 2 equivalents of P4S10 (1.58 g) and dry dioxane (7 mL) was placed in a 250 ml Schlenk flask. The reaction mixture was heated at 101 °C for 5–6 h, cooled and filtered to remove unreacted P4S10 and washed with minimum dioxane. To the filtrate, an aqueous solution (1 mL) of NiCl2·6H2O (0.47 g, 1.99 mmol) was added. The mixture was refluxed at 90°C for 2 h and allowed to cool down to room temperature. Tetrabutylammonium bromide was added to the reaction mixture and stirred overnight. The solvent was evaporated, and the oily residue was washed with petroleum-ether several times. The residue was recrystallized from warm CH2Cl2 and isopropanol by overnight standing yielding dark reddish violet crystals, which were collected by filtration. Yield: (48%, 0.6 g). Absorption spectrum (CH2Cl2) λmax, nm (ε, M−1cm−1): 280 (23000), 320 (25000), 380 (sh, 13000), 518 (2000), 680 (500), 934 (5000). ESIMS(−): 1173 (100%) calculated for C28H12S4Br8Ni ([M-Bu4N]), 1173.

Synthesis of Ni(S2C2(C6H5)2)2 (2a)

In a 500 mL Schlenk flask, benzil or benzoin (5g, 23.8 mmol), P4S10 (21.1g, 47.6 mmol) and dry dioxane (7mL) were added under argon atmosphere and the mixture was refluxed at 110°C for 5–6h. After refluxing, the reaction was filtered to remove unreacted P4S10 and washed with minimal quantity of dioxane. To the filtrate, NiCl2·6H2O (6.27g, 26.4 mmol) in distilled water (1mL) was added. The mixture was refluxed at 90°C for 2h. A green colored compound was isolated, which was filtered and washed with methanol, water. The crude product was recrystallized using CH2Cl2/MeOH. Yield: (30%, 7.19 mmol). Absorption spectrum (CH2Cl2) λmax, nm (εM, mol−1cm−1): 312 (44074), 371 (sh, 10785), 437 (sh, 2643), 596 (1920), 852 (27475). ESIMS(−): 542 (100%) calculated for C28H20S4Ni (M), 542. Anal calcd. C, 61.89; H 3.71. Anal exptl. C, 61.52; H 3.81.

Synthesis of [Et4N][Ni(S2C2(C6H5)2)2] (2b)

First Method

0.1g, 0.18 mmol of 2a was dissolved in THF. An acetonitrile solution of Et4NBH4 (0.03g, 0.18 mmol) prepared was gradually added to the solution Ni-complex. The color of mixture changed from bluish green to reddish violet. The mixture was stirred for 21 h. The solvent was evaporated to dryness and the residue was redissolved in CH3CN and filtered to get reddish violet filtrate and orange colored compound as a residue. The filtrate was concentrated and layered with ether to get reddish violet compound, which was dissolved in THF and filtered to get clear reddish violet solution. The solvent was evaporated to give a reddish violet compound. The crude product was further recrystallized from hot acetone and methanol. The reddish purple colored compound was obtained which was washed with methanol and dried in vacuum. Yield: 12% (0.02 mmol). Absorption Spectrum (CH2Cl2) λmax, nm (εM, mol−1cm−1): 264 (38320), 313 (43640), 367 (sh, 12640), 528 (1624), 680 (500), 935 (15217). ESIMS (−): 542 (100%) calculated for C28H20S4Ni ([M-Et4N]), 542. Anal calcd. C, 64.18; H 5.98; N, 2.08. Anal exptl. C, 64.23; H 6.00; N, 2.18.

Second Method

Complex 2a (0.500g, 0.92 mmol) and p-phenylene diamine (0.25g, 2.3 mmol) were dissolved in dry methyl sulfoxide (10mL). The reaction mixture was stirred and color of mixture changed from dark green to reddish brown. After 2 h of stirring, the mixture was poured into a solution of Et4NBr (0.42g, 2.01 mmol) in EtOH (15mL). Red crystalline compound was recrystallized using hot acetone/MeOH to give dark purple red compound, which was washed with cold methanol and dried under reduced pressure. Yield: 55% (0.51 mmol).

Reduction of Ni(S2C2(C6H5)2)2 (2a)

In a Schlenk flask, fresh sodium (0.01g, 0.37 mmol) was added to a solution of anthracene (0.065g, 0.37 mmol) in 2 mL of THF in anaerobic condition. The dark blue solution was stirred for 6–7 h and then filtered. The filtrate was added drop-wise by a cannula to a solution of 2a (0.1g, 0.18 mmol) in THF (2mL). The reaction mixture became reddish violet. The solution was stirred overnight and then a solution of Et4NBr (0.08g, 0.37 mmol) in CH3CN was added. The solvent was evaporated and the residue was washed with diethyl ether. The residue was dissolved in minimal quantity of acetonitrile, filtered and layered with ether. The dark purple colored compound 2b was isolated (yield was not measured).

Synthesis of [Bu4N]2[Ni(S2C2(CN)2)2] (3c)

1.71g, 9.24 mmol Na2mnt (Na2S2C2(CN)2) was dissolved in 30 mL of ethanol/water (1:1) and stirred. This solution was added slowly to another flask containing a solution of NiCl2·6H2O (1g, 4.2 mmol) in 7.5 mL of H2O with stirring. A dark red solution was formed, and the stirring continued for another 5 minutes after the addition was complete followed by filtration. To the filtrate, an ethanolic solution of t-Bu4NBr was slowly added to the filtrate, which separated orange red crystals immediately. The crystals were separated by filtration, washed with H2O (10 mL) followed by ethanol/water (10 mL, 1:1) and dried. The crude product was recrystallized from hot acetone (80 mL) and isobutyl alcohol (35 mL) for overnight, the crystals were washed with isobutyl alcohol and hexane. Yield: (45.2%, 1.89 mmol.). Absorption Spectrum (CH3CN) λmax, nm (εM, mol−1cm−1): 377 (8258), 468 (4474), 514 (1736), 855 (80).

The corresponding dianionic Et4N+ salt was synthesized similarly using Et4NBr as a source of the cation instead of Bu4NBr. From this dianionic compound, X-ray quality single crystal of the monoanionic complex was prepared in air by slow evaporation of a CH3CN solution.

Synthesis of [Bu4N][Ni(S2C2(CN)2)2] (3b)

An iodine solution (0.3g, 1.2 mmol) in methyl sulfoxide (1 mL) was added to the solution of dianionic complex of [Bu4N]2[Ni(S2C2(CN)2] (0.5g, 0.75 mmol) in methyl sulfoxide (4 mL). The mixture was immediately added to ethanol (12.7mL) and stirred for 20–30 min at room temperature. The black crystalline compound was isolated, filtered and washed with ethanol (5–6 times) followed by ether. The compound was recrystallized by dissolving the compound in hot acetone and adding ether. Keeping the mixture overnight at room temperature gives black crystalline compound. Yield: (65.3%, 0.4 mmol). Absorption spectrum (CH3CN) λmax, nm (εM, mol−1cm−1): 346 (sh, 11372), 475 (2510), 538 (670), 602 (461), 863 (9700). mass spectra (m/z) (ESI-): 338 (100%, m/z) [C8S4N4Ni ([M-Bu4N]), 338].

X-ray Crystallography

X-ray quality single crystals were selected under the microscope, and mounted on glass fibers. X-ray intensities were measured on a Rigaku AFC-7R four-circle diffractometer using graphite-monochromatized Mo radiation (λ = 0.71069Å) at room temperature using the ω−2θ scan technique. Three standard reflections were measured every 150 reflections; a linear correction factor was applied. The structure of complex was initially solved by Patterson method using TeXsan crystallographic software package of Molecular Structure Corporation[10] then they were refined using Crystals for Windows package.[11] The cut off limit for the reflection was I>2σ(I). Selected crystal data for 3b are presented in Table 1.

Table 1.

Crystallographic data for 3b.

3b
Formula C16H20N5S4Ni
Fw 469.34
Crystal system Monoclinic
Space group P21/n
a, Å 8.180(3)
b, Å 18.411(3)
c, Å 14.435(3)
β, deg 92.79(2)
V, Å3 2171.3(10)
Z 4
ρcalcd (g cm−1) 1.44
Data collected 4238
R(F2) 0.0476
wR(F2) 0.1176
Max. residual electron density 0.51

Computational Methods

All calculations were carried out using Gaussian 03W software package.[12] For the electronic structure calculations, all geometries were optimized at DFT level of theory using BP86 exchange correlation functional and 6–311G(d) basis set for all atoms. Frequency calculations were conducted on all optimized structures in order to ensure the optimized structures represent a local minimum. The percentages of atomic orbital contributions to their respective molecular orbitals were calculated by using the VMOdes program. [13]

Results and Discussion

Syntheses and Characterization

The synthetic strategy for 3,5-dibromophenyl dithiolene ligand and its nickel complexes [Ni{C2S2(3,5-C6H3Br2)2}2]0,−1 (1a and 1b) is presented in Scheme 1. The starting material 3,5-dibromobenzaldehyde was synthesized from commercially available 1,3,5-tribromobenzene following a reported method in good yield.[8] 3,3′,5,5′-tetrabromo benzoin as well as 3,3′,5,5′-tetrabromo benzyl were synthesized from 3,5-dibromobenzaldehyde following benzoin condensation reaction, which were purified by extraction with diethyl ether and chloroform respectively, and were characterized by 1H, 13C NMR and IR spectroscopy. The 1H NMR spectrum for benzil revealed a symmetric structure, while that of benzoin exhibits two CHOH resonances at 6.4 and 5.9 ppm. The yields for both benzil and benzoin were moderate (17% for benzoin and 38% for benzil) due to the deactivating nature of the Br-group at the meta positions of the phenyl ring. However, better yield for 3,3′,5,5′-tetrabromobenzoin (30%) was achieved when 3,5-dibromobenzaldehyde was reacted directly with KCN and Bu4NBr in DMF.[14]

Scheme I.

Scheme I

As benzil and benzoin are reported to form the same thiophosphoric ester,[15] both 3,3′,5,5′-tetrabromobenzoin and 3,3′,5,5′-tetrabromobenzil were reacted with P4S10 under inert atmosphere forming the thiophosphoric ester, which was used in preparing the nickel complex.

Complex 1a and the alkyl ammonium salt, 1b were obtained following the method initially developed by Schrauzer et al [6] and later modified by Holm et al. [15] The mechanistic details of this reaction has recently been elucidated by Arumugam et al through isolation and structural characterization thiophosphoryl compound.[16] Reaction of thiophosphoric ester with Ni(II) salts, hydrated NiCl2, gave a reddish-brown solution (Scheme 1). The green colored neutral 1a was isolated from CH2Cl2 at a low temperature (5 °C). Complex 1b was synthesized by using an analogous procedure for 1a i.e., direct reaction between the metal and the pro-ligand. Here thiophosphoric ester was refluxed with NiCl2 followed by precipitation of the tetrabutylammonium salt using Bu4NBr as a precipitant. The compound was initially obtained as a reddish violet oil, which was washed with petroleum ether and recrystallized from CH2Cl2 to get a reddish violet needle shaped crystalline compound. A neutral nickel complex, Ni(C2S2Me2)2, has been successfully reduced to dianionic [Ni(C2S2Me2)2]2− using sodium anthracide.[17] Similar attempts to synthesize dianionic [Ni{C2S2(3,5-C6H3Br2)2}2]2− were unsuccessful, although neutral 2a could be reduced to monoanaionic 2b. Similarly, synthesis of neutral maleonitrile complex (i.e., neutral 3a) through oxidation of 3b, or 3c was also not successful. Thus, poising of redox potentials play a major role in stabilizing a specific oxidation state, and the redox potentials can be modulated by suitable substituents (vide infra).[18]

The compositions of the complexes were confirmed by electrospray ionization mass spectrometry (ESIMS) in the negative ion mode. The characteristic molecular ion peaks for complexes were detected with ~100% intensity. Both 1a and 1b gave peak clusters with a base peak with mass to charge ratio at 1173 consistent for [M] for 1a and [M-Bu4N] for 1b respectively. Conductivity of complexes was measured in nitromethane solutions at room temperature (Table 2). 1b exhibits characteristic conductivity for a 1:1 complex like 3b,[19] while 1a was non-conducting indicating its electroneutrality. Solid state magnetic susceptibilities of 1b at 293 K showed paramagnetism with spin only value corresponds to one unpaired electron (Table 2), whereas 1a is diamagnetic. These measurements probed the neutral and mono-anionic nature of 1a and 1b respectively, indicating that metal ion is formally in +3 oxidation state in 1b, dithiolene acts as a monoanionic ligand i.e., in its oxidized form. ESIMS of 3b gave a molecular ion at ~338 peak due to anionic [Ni(S2C2(CN)2)2] whose isotope distribution pattern matches well with that of the calculated molecular ion. The corresponding dianionic complex (3c) a peak cluster was observed at the same m/z value even though the electronic spectra of the solution is different and showed a 2:1 electrolyte. This suggests that during the mass spectral analyses the complex is oxidized. Such oxidation chemistry under mass spectrometric conditions has been observed before in transition metal chemistry.[20]

Table 2.

Characterization data for the nickel complexes used in this investigation.

Complex Base Peak in ESI-MS UV-Vis Spectra ε (λ,nm) M−1cm−1 E 1/2 (ΔE) mV vs. Fc+/Fc μeff, B.M. ΛM Ohm−1 cm2 mol−1 in nitromethane
1a 1173 30,660 (834) −288 (114) 0 Non-conducting
1b 1173 6500 (927) −1065 (130) 1.77 63
2a 542 27,500 (852) −258 (94) 0 Non-conducting
2b 542 15,200 (935) −1275 (133) 1.82 68
3c 338 80 (855) −262 (68.5) 0 187
3b 338 9700 (863) 1.54 69

Electronic Spectroscopy

The electronic spectroscopy is an excellent tool to define the neutral or anionic nature of the Ni-dithiolene complexes. A strong absorption band at the low energy region (near IR region) is a characteristic of neutral complex, which shifts to a lower energy with less intensity in the monoanionic complex and this band is not present in the dianionic complex. Electronic spectra of 1a and 1b were recorded in CH2Cl2 (Figure 2). Compounds 3b and 3c were insoluble in CH2Cl2 and spectra were recorded in CH3CN. Figure 2 also shows electronic spectra 2a, 2b, 3b, and 3c.

Figure 2.

Figure 2

Electronic spectra of Ni-complexes recorded at room temperature.

1a, 1b, 2a, and 2b were recorded in CH2Cl2. 3b and 3c were recorded in CH3CN.

High level density functional calculations[21] on Ni(S2C2Me2)2 suggest the ground state to be …(18a1g)2(4b3g)2(6b1u)2(5b2g)0(13b1g)0…In the neutral species, the HOMO is the b1u orbital is fully occupied which is primarily ligand based with minor contribution from the metal. The intense charge transfer absorption is due to the transition from b1u → b2g transition. The b2g orbital in the one-electron reduced monoanionic species is singly occupied. The contributions from nickel to this b2g orbital increase with reduction, and the band position also shifts. Because of the involvement of the dithiolene orbitals, the position of the low energy transition is dependent on the substituent on the dithiolene ligand itself. For example, in monoanionic complexes the low energy band shifts to lower energy with increasing electron-releasing character of the substituent. The results presented in here indicate that the effect of distal substituents (ca. the substituents on the phenyl ring that is attached to the dithiolene) is small. The electronic spectra show some variation: the first band near 852 nm for the 2a shifts to 834 nm, a shift of 18 nm, while 935 nm band in 2b moved to 927 nm in 1b, which is only an 8 nm shift. However, this band shifts to 863 nm in the case of 3b. With the exception of 3c no other dianionic species was isolated where this band is absent. Thus, the low energy band maxima follow the order: 1b ~ 2b > 3b. This is consistent with the reported results on neutral complexes of general formula, Ni{(S2C2(p-C6H4X)2}2.[15] The intensities of these band in three compounds are different, 3b being the least intense. Because the intensity comes from the mixing of the orbital coefficients involved in the optical transition, it is suggestive that the ground and the excited states do not mix as efficiently, and inclusion of the phenyl ring increases the mixing perhaps by lowering the symmetry. Thus, while significant differences exist going from localized dithiolene to phenyl substituted dithiolene, there little difference with substitution on the phenyl ring.

Electrochemical Properties

Electrochemical properties of all complexes were investigated by cyclic voltammetry in CH2Cl2 (compounds 1a and 1b) or CH3CN (3b and 3c). Cyclic voltammogram of 1a is shown in Figure 3. Two quasi-reversible one-electron redox couples were observed for 1a and 2a, while only one redox couple was observed for 3b. A detailed spectroscopic study on 3b (monoanionic) suggests that the singly occupied molecular orbital (SOMO) of this compound largely dominated by sulfur from the dithiolene ligand, which underscores the highly delocalized nature of the metal-sulfur orbitals in these molecules.[21] Our electronic structure calculations, detailed later, are in good agreement with the precious findings. Thus, assigning the redox potentials only to metal based orbitals is ambiguous at best. We therefore designate the redox potentials in terms of the overall charge of the molecule – neutral (N), monoanionic (M) to dianionic (D), and these species are related by equation 1.

Figure 3.

Figure 3

Room temperature cyclic voltammogram of 1a in CH2Cl2.

Ne+eMe+eD (Equation 1)

It is interesting to note that maleonitrile complexes (3) exhibited only one redox couple at −260 mV, which is due to the M/D couple. This couple is moved significantly cathodically in the phenyl substituted compounds by 800 mV and 1013 mV for molecular systems 1 and 2, respectively. Thus, introduction of the highly electron withdrawing nitrile group moves the N/M couple beyond the solvent window. Interestingly this couple has been proposed to lie beyond 1 V,[17] which is consistent with the difficulty in the synthetic procedures described here.

Compared to the unsubstituted phenyl derivative, introduction of electron withdrawing Br-groups also influences the redox potentials. The direction of the change in the M/D couple is however, in the expected order. Introduction of eight Br-groups in the molecule shifts the redox potential towards more positive direction. Interestingly, the difference between the two couples N/M-M/D is smaller in the case of Br-substituted compound. Thus, clearly redox orbital (b1u) in this case is influenced significantly by the substitution at the phenyl ring. However, the direction of shift for the N/M couple is counter intuitive, which becomes more difficult by 30 mV for 1 compared to 2. Taking together, the redox properties of these complexes are influenced by the substituents on the dithiolene ligands because of the ligand-based nature of the HOMO.

Molecular Structure

X-ray quality single crystals of [Et4N][Ni(S2C2(CN)2)2] were obtained by slow evaporation of an CH3CN solution of [Et4N]2[Ni(S2C2(CN)2)2] in air. It is interesting to point out that the structure of this compound has been solved before with different cell parameters and space groups.[22] The structure of this complex was as expected with very little unusual features and thus the discussion will be limited. The Ni-S distances are as expected 2.14 Å, and the bite angles of the two ligands are ~92°. The molecular structure is shown in Figure 4. The nickel center shows a square planar geometry coordinated by the four sulfur donors of the two dithiolene ligands. We were pleased with no disorder problem with the ethyl groups of the cation, which often exhibit a positional disorder. The packing diagram of the complex (Figure 5) shows that the planar Ni-complexes are stacked and in between the layers, the tetraethyl ammonium ions are positioned, which may explain rigidity of the tetraethyl ammonium groups.

Figure 4.

Figure 4

Thermal ellipsoid (50% probability) representation of molecular structure of [NEt4] [Ni(S2C2(CN)2)2].

Figure 5.

Figure 5

Packing diagram of [NEt4][Ni(S2C2(CN)2)2].

Electronic Structure

The electronic structures of the Ni-complexes were investigated by density functional theory using optimized geometries. The [Ni(S2C2(CN)2)2]−1/−2 exhibited a D2h symmetry while that for the phenyl complexes was converged to D2 point group. The monoanionic complexes were calculated using spin-unrestricted model, while neutral and dianionic complexes were calculated with a spin restricted model.

The compositions of the frontier orbitals are listed in Table 3 and energy levels are shown in Figures 6 and 7, and pictorial representations of selected orbitals are presented in Figure 8. The compositions the HOMO and the LUMO of 1b, 2b and 3b show small difference. In all cases metal and the sulfur orbitals contribute significantly, however, incorporation of phenyl rings in the ligand architecture reduces the metal electron density by ~10%. There is virtually no difference in the orbital compositions with and without the Br-substitution in the phenyl ring. The high S contributions in the frontier orbitals indicate a facile electron delocalization pathway involving the Ni and sulfur orbitals underscoring the importance of the non-innocent nature of the dithiolene ligand. The presence of the phenyl ring impacts the energetic more significantly; the HOMO in 3b is stabilized by 1.5 eV due to the electron donating phenyl group. The destabilization caused by phenyl ring is attenuated (by ~0.8 eV) in 1b due to the presence of the electron withdrawing Br-derivative. Interestingly, the HOMO-LUMO separation is not significantly different, the maximum difference being 0.2 eV. This indicates that introduction of the phenyl ring while does not significantly alter the orbital composition, but the overall energies are affected, which of course can influence not only the reduction potentials but also the optical spectra. A similar situation has been observed in X-ray absorption spectroscopy.[21, 23]

Table 3.

The composition of selected orbitals.

Compound Orbital Symmetry Energy, eV % Ni % S
1b α HOMO−1 B3 −2.796 49.6 15.1
HOMO B2 −1.951 13.4 49.2
LUMO B1 −0.754 16.6 33.1
LUMO+1 A −0.426 0.40 12.5
β HOMO−1 B1 −2.804 0.70 46.9
HOMO B3 −2.587 48.2 13.7
LUMO B2 −1.579 21.9 43.2
LUMO+1 B1 −0.621 16.5 30.4
2b α HOMO−1 B3 −1.919 51.5 15.7
HOMO B2 −1.088 14.0 51.0
LUMO B1 0.130 17.7 36.3
LUMO+1 A 0.583 0.5 13.3
β HOMO−1 B1 −1.921 0.7 45.9
HOMO B3 −1.712 50.2 14.3
LUMO B2 −0.719 23.0 45.2
LUMO+1 B1 0.270 17.9 34.2
3b α HOMO−1 B1g −3.426 64.9 17.3
HOMO B2g −2.566 16.5 62.7
LUMO B3g −1.371 18.6 35.9
LUMO+1 B1g −0.682 2.7 19.1
β HOMO−1 B3u −3.435 0.7 55.9
HOMO B1g −3.215 64.5 15.7
LUMO B2g −2.178 27.6 56.6
LUMO+1 B3g −1.221 19.0 34.2
1a HOMO−1 B3 −6.042 48.6 17.0
HOMO B1 −5.932 0.7 36.9
LUMO B2 −4.977 13.5 49.6
LUMO+1 B1 −3.821 18.3 37.0
2a HOMO−1 B3 −5.345 50.1 17.6
HOMO B1 −5.212 0.8 35.8
LUMO B2 −4.283 13.8 50.4
LUMO+1 B1 −3.125 18.7 38.3
3c HOMO−1 Ag 1.159 85.1 7.7
HOMO B2g 1.916 47.6 43.0
LUMO B3g 2.771 20.6 32.9
LUMO+1 B1g 3.049 5.6 21.3

Figure 6.

Figure 6

Molecular orbital diagram of 3b, 2b, and 1b calculated in spin unrestricted DFT method. The dashed line represents the separation between the HOMO and the LUMO. The formal oxidation state of Ni in these complexes is considered to be +3.

Figure 7.

Figure 7

Molecular orbital diagram of 3c (a), 2a (b) and 1a (c) calculated in spin restricted DFT method. The dashed line represents the separation between the HOMO and the LUMO.

Figure 8.

Figure 8

Pictorial representation of the HOMOs. The complexes are arranged vertically in order of increasing charge. The left panel shows complex 3 while the right panel shows complex 2.

The diamagnetic compounds are different such that compound 1a and 2a are neutral, compound 3c is dianionic. The frontier orbitals in 1a and 2a are much more stabilized than those in 3c, although the HOMO-LUMO gap differs only by 0.1 eV. The orbitals compositions are significantly different: metal contribution to HOMO in 1a and 2a is virtually negligible, but that in 3c substantial. Contribution from the S orbitals to the HOMO is 35% in 1a and 2a which is ~10% than that in 3c. In 3c both Ni and S contributes equally to the HOMO. These differences not only affect the physical properties but also impact their chemical reactivity.

Summary

We have designed and synthesized new nickel dithiolene complexes containing 3,5-C6H3Br2 substituted phenyl groups. Compounds (1a and 1b) have been characterized by NMR, UV-visible, and IR spectroscopy. The redox potentials exhibit exquisite sensitivity with respect to the substituents and the optical spectra show little variation (in similarly charged molecular systems like 1a and 2a). The differential sensitivity is a result of different alignment of the redox orbitals. We determined the molecular structure of the 3b, and the electronic structures of 1b, 2b, and 3b show a variation in the energies of the orbitals without significantly effecting the composition. Similar calculations on diamagnetic 1a, 2a and 3c indicate not only a difference in energy but also compositional variation of frontier orbitals.

Supplementary Material

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Acknowledgments

We thank Dr. Raghvendra S. Sengar for insightful discussions. Financial assistance from the National Institutes of Health (GM061555) is gratefully acknowledged. We also acknowledge the Minnesota Supercomputing Institute for the generous support of computer time.

Footnotes

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