Open Access Article
Ka-Pan
Shing‡
a,
Lin
Qin‡
a,
Liang-Liang
Wu
a,
Jie-Sheng
Huang
*a and
Chi-Ming
Che
*ab
aState Key Laboratory of Synthetic Chemistry, Department of Chemistry, The University of Hong Kong, Pokfulam Road, Hong Kong, China. E-mail: cmche@hku.hk
bHKU Shenzhen Institute of Research and Innovation, Shenzhen, China
First published on 2nd September 2023
Terminal Ru(V)–imido species are thought to be as reactive to group transfer reactions as their Ru(V)–oxo homologues, but are less studied. With the electron-rich corrole ligand, relatively stable and isolable Ru(V)–arylimido complexes [Ru(tBu–Cor)(NAr)] (H3(tBu–Cor) = 5,15-diphenyl-10-(p-tert-butylphenyl)corrole, Ar = 2,4,6-Me3C6H2 (Mes), 2,6-(iPr)2C6H3 (Dipp), 2,4,6-(iPr)3C6H2 (Tipp), and 3,5-(CF3)2C6H3 (BTF)) can be prepared from [Ru(tBu–Cor)]2 under strongly reducing conditions. This type of Ru(V)–monoarylimido corrole complex with S = ½ was characterized by high-resolution ESI mass spectrometry, X-band EPR, resonance Raman spectroscopy, magnetic susceptibility, and elemental analysis, together with computational studies. Under heating/light irradiation (xenon lamp) conditions, the complexes [Ru(tBu–Cor)(NAr)] (Ar = Mes, BTF) could undergo aziridination of styrenes and amination of benzylic C(sp3)–H bonds with up to 90% product yields.
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| Fig. 1 Examples of (a) in the literature and (b) in this work for spectroscopically characterized M(V)–imido species that can undergo alkene aziridination and/or C–H amination reactions. | ||
In order to obtain novel spectroscopically characterized M(V)–imido species reactive with hydrocarbons, and to improve the stability of such species, we attempted to focus on Ru(V) (considering the high reactivity of Ru(V)–acylimido porphyrin species1e) and the use of the trianionic corrole (Cor) ligand; the latter was previously shown to stabilize the [MV(Cor)(NAr)] (M = Cr, Mn, Re) species.6 One hurdle to overcome is that most of the reported Ru corroles are dimers with strong Ru
Ru triple bonds,7 in contrast to the case of Ru porphyrins, where Ru2(II,II) porphyrin dimers are highly sensitive to oxygen and are useful precursors for Ru–carbene, –oxo or –imido species.8a,f Here we report reductive activation of Ru2(III,III) corrole dimers followed by reaction with aryl azides to give Ru(V)–arylimido (RuV(NAr)) complexes; the latter have been isolated and characterized by X-band EPR, resonance Raman (rR), HR-ESI-MS, UV-vis spectroscopy, elemental analysis, and/or DFT calculations. This type of RuV(NAr) complex can undergo alkene aziridination and C(sp3)–H amination reactions, both of which have not been reported for [MV(Cor)(NAr)] (M = Cr, Mn, Re).6
Ru bond of 1 by reducing this complex. Reduction of 1 with excess potassium graphite (KC8) in rigorously deoxygenated and dried THF, followed by overnight stirring at RT (Pyrex® Spinbar), afforded a species 2, tentatively the reduced dimer {[Ru(tBu–Cor)]2}2−. The effective magnetic moment of 2 (in situ generated) was determined to be 2.81μB using the Evans method, which indicates that 2 is paramagnetic with two unpaired electrons (S = 1). This is in contrast to the dimer 1 (S = 0) and mononuclear Ru(II) corrole species, which are expected to be diamagnetic, similar to the Ru(II) porphyrin complexes [Ru(Por)(L)2] (L = vacant or L = N2, CH3CN, THF, Et2O).8g Based on its magnetic moment (2.81μB), complex 2 is likely to be a Ru2(II,II) corrole dimer, whose electronic configuration (S = 1) is similar to that (σ2π4(δnb)4(π*)2) of the Ru2(II,II) porphyrin dimers reported by Collman and co-workers.8d Redox titration of 2 with [Cp2Fe]PF6 showed that ca. 2 equiv. of Cp2Fe and 1 equiv. of 1 were generated. In a control experiment, 1 was not able to reduce [Cp2Fe]PF6 under the same reaction conditions. The UV-vis spectrum of 2 in THF shows pairwise Soret bands at 411 and 445 nm, which are red-shifted from that of 1 at 329 and 399 nm (Fig. S4 in the ESI†). A Ru2(II,II) species, {[Ru(Cor)]2}2−, was previously proposed as the two-electron reduced product of [Ru(Cor)]2 by Guilard and co-workers.7b
As shown in Scheme 1, treatment of 2 with aryl azides (ArN3, Ar = Mes, Dipp, Tipp, BTF) afforded a set of RuV(NAr) complexes [Ru(tBu–Cor)(NAr)] (3); [Ru(tBu–Cor)(NBTF)] (3d) bearing the CF3-substituted arylimido ligand is one of the rare examples of terminal imido complexes of late transition metals featuring strongly electron-withdrawing CF3 substituents on their imido ligands.9 The reactions using MesN3 (for 3a) and BTFN3 (for 3d) took only a few minutes, whereas the reactions with DippN3 (for 3b) and TippN3 (for 3c) bearing sterically more hindered aryl groups required stirring for 0.5 h at RT. Complexes 3 are likely formed via initial generation of [RuIV(tBu–Cor)(NAr)]− followed by disproportionation or one-electron oxidation. In the literature, Ru(IV)–oxo porphyrin was reported to undergo disproportionation;8f,10 Fe(IV)–oxo porphyrins and Mn(IV)–oxo corroles have been reported to convert into their one-electron oxidized counterparts in solution.11
MALDI-TOF MS was used to monitor the reaction. In initial trials using “1 + MesN3” in refluxing benzene solution, a cluster peak attributable to 3a was not observed. By using “2 + MesN3” (Fig. S6 in the ESI†), the ESI-MS spectrum of the reaction mixture showed a strong cluster peak at m/z 814.2479, which was attributed to the parent ion of [Ru(tBu–Cor)(NMes)] (3a, calcd for C50H42N5Ru: 814.2492; Fig. S12 in the ESI†), giving the simulated isotope pattern that matches that observed experimentally. As expected, the peak is isotopically sensitive, with the isotope pattern changing upon using a 50% 15N-enriched sample (14,15N–3a, prepared from 15N–MesN3; Fig. 2). Other Ru–arylimido complexes (3b–3d) have also been isolated and characterized by ESI-MS/MALDI-TOF MS. Complexes 3a–3d were found to gradually decompose within 24 h even under an inert atmosphere and at low temperature (argon filled glove box, refrigerator pre-equilibrated at −35 °C), as evidenced by UV-vis spectroscopy and ESI-MS analysis. Attempts to obtain diffraction-quality crystals of these complexes for X-ray crystal structure determination were not successful.
PPh3 were found (Fig. S9 in the ESI;†m/z calcd: 396.1858, found: 396.1881; 31P NMR in CDCl3: −13.85 ppm).
The EPR spectrum of 3a was simulated using the parameters of gx = 2.010, gy = 2.005, gz = 1.880; Ax, Ay, Az = 53, 14, 14 MHz (14N). Simulation for the EPR spectrum of 3b (Fig. S17 in the ESI†) was also carried out, by employing the g and A values of gx = 2.000, gy = 1.980, gz = 1.870; Ax, Ay, Az = 50, 14, 14 MHz (14N). The EPR spectrum of 3c (Fig. 3a) is similar to that of its structurally similar complex 3b (g and A values for the simulated spectrum: same as those of 3b), and the signal pattern is assigned to the superhyperfine coupling to the 14N nucleus of the imido ligand, similar to that of Fe(V)–imido species.12 For the 50% 15N-enriched sample, 14,15N–3c (prepared from 15N–TippN3), the corresponding EPR spectrum (Fig. 3b) shows a signal which can be reasonably fitted by summing the simulated spectra of 3c and 15N–3c, with a 1
:
1 ratio (Fig. 3b; 14N: I = 1, 15N: I = ½). The EPR signals of 3a–3c are characterized by giso (gx + gy + gz)/3) values of 1.950–1.965, which can be assigned to Ru(V) complexes with S = ½.1e,2a These giso values are similar to those of Ru(V)–acylimido and Ru(V)–oxo porphyrin complexes (giso = 1.94,1e 1.970 (ref. 2a)), but smaller than those commonly observed for Ru(III) complexes (giso = 2.1–2.3 (ref. 2c and 13)).
Complexes 3a–3d each exhibit one Soret band (at 406–411 nm) in the UV-vis spectrum; like mononuclear [RuVI(Cor)(N)] complexes each complex also has one Soret band (at 417–419 nm),7d but unlike the Ru2(III,III) dimer 1, which exhibits two Soret bands (at 329 and 399 nm). In accord with the [RuV(Cor)(NAr)] formulation, the UV-vis spectra of 3a–3d (Fig. S5 in the ESI†) do not show typical absorption bands of corrole π–cation radical (Cor+˙) complexes (above 650 nm14). For example, a band at 676 nm was observed for [MnV(Cor+˙)(N)],15 the EPR spectrum of which (at 4 K) showed an isotropic radical signal, in contrast to the anisotropic EPR signals of 3a–3c.
band could possibly be obscured by an intense band of the coordinated corrole ligand at 1016 cm−1; based on the FTIR spectroscopy, we tentatively assign the
band of 14,15N–3a at 972 cm−1. To observe the
and
bands, we measured the resonance Raman (rR) spectra of 3a and 14,15N–3a (isolated samples dissolved in CH2Cl2). The rR spectrum of 14,15N–3a (Fig. 4b, λexcitation: 416 nm) shows pairwise bands (ca. 1
:
1 ratio due to 50% 15N-enrichment) at ∼949 and 921 cm−1 with Δν of ∼28 cm−1 agreeing with the value of 28 cm−1 estimated using Hooke's law. These two bands are assigned to
and
respectively, and the band at 921 cm−1 is absent in the rR spectrum of 3a (Fig. 4a). By considering literature examples of rR studies on metal–arylimido (M(NAr), e.g., Fe(NPh)16) complexes, other 15N-isotopically sensitive bands within 820–1000 cm−1 may be associated with the coordinated arylimido ligand, where 15N-labelling resulted in a downshift of the bands involving M–Nimido and aryl groups.
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| Fig. 4 rR spectra of the isolated samples (dissolved in dry CH2Cl2) of (a) 3a and (b) 14,15N–3a. (c) DFT-calculated Raman spectra of 3a, 15N–3a and 14,15N–3a. | ||
C bond nor amination of the allylic C(sp3)–H bond was observed.
| a Ru(V)–arylimido complex (5.50 μmol) and the substrate (1.65 mmol) in benzene (1 mL); the product yields under UV-vis irradiation are presented in pink colour whereas the black ones refer to the yields obtained at 85 °C. |
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We then examined the amination of benzylic C(sp3)–H bonds with 3d. Treatment of 3d with excess isochroman gave the amination product in <1% yield, whereas the reaction of indane and phthalane with 3d gave the amination product in 12% and 18% yields, respectively (entries 7–9 in Table 1; 85 °C for 24 h). The reaction of 3d with tetralin gave the amination product in 31% yield (entry 10 in Table 1; 29% yield for a 1 h reaction). Complex 3d exhibited a relatively high reactivity towards indene (61% yield of the amine product; entry 11 in Table 1). We found that light irradiation at RT (xenon lamp) promoted the 3d-mediated amination of indane, phthalane and tetralin as revealed by the higher product yields obtained (50–66% yield; entries 8–10 in Table 1). Indane and phthalane gave higher yield of the amination product than isochroman, which may be related to the statistical factor because isochroman has a smaller number of equivalent C–H bonds for the amination. In the amination of tetralin and indane by 3d, the product yield was found to decrease with increasing dissociation energy of the reactive C–H bond (cf. 82.9 and 85.3 kcal mol−1 for tetralin and indane, respectively18).
Catalytic N-group transfer reactions were examined using Ru corrole complexes 1 and 2 as catalysts. For the 1-catalysed reaction of styrene with aryl azide BTFN3 in benzene at 85 °C, the aziridination product was obtained in 5% yield. Upon changing the catalyst to 2, a much higher product yield of 46% was achieved (entries 1 and 2 in Table 2). Complex 2 also catalysed the aziridination of para-substituted styrenes to aziridines in 38–54% yields (entries 3–6 in Table 2). Using cis-stilbene as the substrate, the reaction afforded trans-aziridine as the major product (trans/cis ratio: 2.9
:
1.0, 48% yield, entry 8 in Table 2).
Regarding the mechanism of the 3d-mediated aziridination of alkenes, we conceive that the aziridination proceeds in a stepwise manner due to the formation of trans-aziridine from cis-stilbene (entry 3 in Table 1). For the aziridination of para-substituted styrenes by 3d, the plot of log(krel) against σmb and
using a dual parameter equation developed by Jiang and co-workers,19 shows a good linearity (R2 = 0.9979) featuring ρmb = −0.54 and
(Fig. 5), with the linearity being better than that for the plot of log(krel) against σ+ (Fig. S15 in the ESI;†R2 = 0.9356). This is consistent with a stepwise mechanism in which a carboradical is involved. A positive value of
indicates the spin density of the radical centre delocalized by the para-substituent, while a negative value of ρmb supports electrophilic attack of styrene by 3d.
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Fig. 5 Hammett correlation for the aziridination of para-substituted styrenes mediated by 3d using a dual-parameter method (σmb and ). | ||
Furthermore, we examined the deuterium kinetic isotope effect (KIE) for 3d-mediated C(sp3)–H amination by using equimolar and excess of tetralin and d4-tetralin. The kH/kD value determined for such amination by 3d at 383 K is 4.0(2), comparable to that reported for the C(sp3)–H amination of ethylbenzene by [RuVI(TMP)(NNs)2] (kH/kD = 4.8) at 298 K.20 We propose that the C–H amination mediated by 3d involves a stepwise mechanism similar to that for the [RuVI(TMP)(NNs)2]-mediated amination,20 characterized by H atom abstraction followed by radical rebound.
and
are located at 944 and 923 cm−1, respectively (Fig. 4c), which are consistent with the respective experimental values (∼949 and 921 cm−1). By converting the Raman shifts to bond distances, 3a has a calculated Ru–Nimido distance of 1.756 Å. The calculated Ru–Nimido distances for 3b and 3d are 1.779 and 1.763 Å, respectively. In terms of the Wiberg bond index (WBI), 3a, 3b and 3d have predicted Ru–Nimido bond orders of 2.05, 1.96 and 2.04, respectively, indicating a multiple bond character. This is in contrast to the cobalt complex with the imidyl ligand NDipp+˙, which is characterized by a calculated single Co–Nimidyl bond character (WBI ≈ 1.0).21
Similar to the previously reported Ru(V)–oxo porphyrin,2a both 3a and 3b adopt an S = 1/2 ground state with (dxy)2(dxz,dyz)1(dz2)0(dx2−y2)0 configuration. In both species, the singly occupied molecular orbital (SOMO) corresponds to dπ, while the π orbitals of the corrole ligand are ca. 0.4–0.5 eV lower than the SOMO, indicating that the corrole ligand is not redox-active (Fig. S18 in the ESI†). We calculated g values for 3a by DFT calculations; the calculated results (g = 2.010, 2.000, 1.890) are in good agreement with the values based on the experimental EPR spectrum (g = 2.010, 2.005, 1.880) (Table S3 in the ESI†). By DFT calculations, the % spin density on Ru/Nimido atom (% SDRu/N) of 3a, 3b, and 3d is 44/27, 35/36, and 53/19, respectively, and that on the coordinated arylimido ligand (% SDNAr) of 3a/3b/3d is 40/54/26 (Fig. 6).
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| Fig. 6 DFT-optimized spin density distributions (contour value: 0.005), bond angles, bond distances and out-of-plane deviations. | ||
The decrease of spin density on the arylimido ligand (% SDNAr) along the series 3b > 3a > 3d is in line with the decrease of the Ru–Nimido–CAr angle along the same series (160°, 146° and 138° for the DFT-optimized structures of 3b, 3a, and 3d, respectively; Fig. 6). The arylimido ligand of 3b bears bulky 2,6-substituents (iPr) and adopts a basically linear coordination mode, which minimizes steric conflicts between these substituents and the corrole ligand. Complex 3a has less bulky 2,6-substituents (Me); its arylimido ligand can accommodate a relatively bent coordination mode.22 A more bent coordination mode of the arylimido ligand corresponds to 3d which possesses no 2,6-substituents and bears electron-withdrawing 3,5-CF3 groups, like the case of [RuVI(TPP)(NBTF)2] (Ru–Nimido–CAr angles: 139.8(3)° and 143.7(4)°).23 The bending of the Ru–Nimido–CAr moiety would reduce spin delocalization along the z-axis (and into the aryl ring), thus decreasing the spin density on the arylimido group.
As the spin density on Nimido is the highest in 3b among 3a, 3b, and 3d, we performed multi-reference calculations for 3b using the complete active space self-consistent field (CASSCF) method to check if Ru(IV)-imidyl character is involved.17a,24 The calculation results revealed that 3b can be described as “85.9% of [RuV(tBu–Cor)(NDipp)] + 3.6% of [RuIV(tBu–Cor)(NDipp+˙)]” (Fig. 7). For the Ru–Nimido bond of 3b, a calculated bond order of 2.04 was obtained by considering the matrix of atomic orbital coefficients for all relevant molecular orbitals. Based on the occupation numbers of orbitals within the active space, the calculated Ru–Nimido bond order is 2.27, close to the formal bond order of 2.5 with σ2π4(π*)1 configuration. The spin population obtained from the CASSCF calculation is 0.55 on Ru and 0.35 on Nimido (Fig. S19 in the ESI†), indicating that 3b has a doublet ground state with the unpaired electron mainly residing on the Ru centre. This provides support for the formulation of 3b, and also 3a and 3d, as a formal Ru(V)–arylimido corrole species bearing considerable spin density on Nimido.
We compared the DFT calculation results for the Ru(NAr) complexes having an S = 1/2 ground state, including % spin density on Ru/NAr (% SDRu/NAr) and the Ru–NNAr distance (Table S4 in the ESI†). The % SDRu/NAr of [(SiPiPr3)Ru(N–p-CF3C6H4)]25a and [Ru(PNP)(NPh)] (PNP = [(tBu2PCH2SiMe2)2N]−)25b with different types of monoanionic supporting ligands is 40/54 and 30/68, respectively. In the case of complexes 3 with the same trianionic tBu–Cor supporting ligand, a direct comparison of % SDRu/NAr among various Ar groups can be made (3a: 44/40, 3b: 35/54, and 3d: 53/26); the % SDNAr decreases along the 3b > 3a > 3d series as discussed above. The Ru–NNAr distances in [(SiPiPr3)Ru(N–p-CF3C6H4)] and [Ru(PNP)(NPh)] (ca. 1.81–1.87 Å) are longer than in complexes 3 (ca. 1.76–1.78 Å).
The electronic structure of the Ru(V)–arylimido complex 3b calculated by CASSCF is different from that of the Fe(V)–tosylimido species [FeV(TAML)(NTs)]− calculated by DFT;1b,26 the properties of the M–Nimido π- and π*-bonding of these two complexes are different. For 3b with an essentially linear M–Nimido–CAr moiety (bond angle: 160°), two sets of π and π* orbitals between M-dxz/yz and N-px/y are involved, reminiscent of the corresponding CASSCF calculation results for other M(NAr) complexes with linear M–Nimido–CAr moieties.27 However, for [FeV(TAML)(NTs)]− having a bent Fe–Nimido–STs moiety (bond angle: 126° (ref. 1b)), only the π and π* orbitals between M-dyz and N-py are involved, and the M-dxz is non-bonding.26
DFT calculations were also carried out for the aziridination of cis-stilbene by 3d, which was experimentally found to favour the formation of the trans-aziridine product. The calculated reaction profile (Fig. S20 in the ESI†) involving the formation of a carboradical intermediate (Int-trans and Int-cis for trans- and cis-configuration, respectively) is consistent with the proposed stepwise mechanism. The ring-closure barrier for Int-trans and Int-cis is 14.1 and 13.3 kcal mol−1, respectively, both of which are larger than the barrier of 10.7 kcal mol−1 required for isomerization of Int-cis to the thermodynamically more favourable Int-trans by rotation about the CPh–CPh bond, allowing such rotation to take place prior to the ring closure, giving trans-aziridine as the major product.28
Footnotes |
| † Electronic supplementary information (ESI) available: Abbreviations, experimental procedures, characterization of compounds, computational details, Tables S1–S4, Fig. S1–S21, NMR spectra of compounds, and Cartesian coordinates from DFT calculations. CCDC 2214628. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d3sc02266h |
| ‡ These authors contributed equally. |
| This journal is © The Royal Society of Chemistry 2023 |