Open Access Article
Yuyang
Dong
a,
James T.
Lukens
b,
Ryan M.
Clarke
a,
Shao-Liang
Zheng
a,
Kyle M.
Lancaster
b and
Theodore A.
Betley
*a
aDepartment of Chemistry and Chemical Biology, Harvard University, 12 Oxford Street, Cambridge, Massachusetts 02138, USA. E-mail: betley@chemistry.harvard.edu
bDepartment of Chemistry and Chemical Biology, Baker Laboratory, Cornell University, Ithaca, New York 14853, USA
First published on 11th December 2019
Metalation of the deprotonated dipyrrin (AdFL)Li with NiCl2(py)2 afforded the divalent Ni product (AdFL)NiCl(py)2 (1) (AdFL: 1,9-di(1-adamantyl)-5-perfluorophenyldipyrrin; py: pyridine). To generate a reactive synthon on which to explore oxidative group transfer, we used potassium graphite to reduce 1, affording the monovalent Ni synthon (AdFL)Ni(py) (2) and concomitant production of a stoichiometric equivalent of KCl and pyridine. Slow addition of mesityl- or 1-adamantylazide in benzene to 2 afforded the oxidized Ni complexes (AdFL)Ni(NMes) (3) and (AdFL)Ni(NAd) (4), respectively. Both 3 and 4 were characterized by multinuclear NMR, EPR, magnetometry, single-crystal X-ray crystallography, theoretical calculations, and X-ray absorption spectroscopies to provide a detailed electronic structure picture of the nitrenoid adducts. X-ray absorption near edge spectroscopy (XANES) on the Ni reveals higher energy Ni 1s → 3d transitions (3: 8333.2 eV; 4: 8333.4 eV) than NiI or unambiguous NiII analogues. N K-edge X-ray absorption spectroscopy performed on 3 and 4 reveals a common low-energy absorption present only for 3 and 4 (395.4 eV) that was assigned via TDDFT as an N 1s promotion into a predominantly N-localized, singly occupied orbital, akin to metal-supported iminyl complexes reported for iron. On the continuum of imido (i.e., NR2−) to iminyl (i.e., 2NR−) formulations, the complexes are best described as NiII-bound iminyl species given the N K-edge and TDDFT results. Given the open-shell configuration (S = 1/2) of the iminyl adducts, we then examined their propensity to undergo nitrenoid-group transfer to organic substrates. The adamantyl complex 4 readily consumes 1,4-cyclohexadiene (CHD) via H-atom abstraction to afford the amide (AdFL)Ni(NHAd) (5), whereas no reaction was observed upon treatment of the mesityl variant 3 with excess amount of CHD over 3 hours. Toluene can be functionalized by 4 at room temperature, exclusively affording the N-1-adamantyl-benzylidene (6). Slow addition of the organoazide substrate (4-azidobutyl)benzene (7) with 2 exclusively forms 4-phenylbutanenitrile (8) as opposed to an intramolecular cyclized pyrrolidine, resulting from facile β-H elimination outcompeting H-atom abstraction from the benzylic position, followed by rapid H2-elimination from the intermediate Ni hydride ketimide intermediate.
Formation of later transition metal MLMBs can also diminish MLMB bond order in two ways: (1) higher d-electron counts necessarily populate more M–L antibonding orbitals; (2) progression through the 3d transition metal series should lead to diminished energetic overlap between the transition metal and N valence orbitals, potentially impacting the electronic structure and reactivity of the resultant MLMB.17 Indeed, four Ni imido systems have been thus far reported by Hillhouse1,3–6,10–12 and Warren.2,13 The seminal work by Hillhouse and coworkers first described the synthesis and reactivity of phosphine-supported NiII imidos (Fig. 1a and b),10–12 later establishing both higher valent imido cations (Fig. 1a and b)4 and lower-coordinate, carbene supported imido complexes (Fig. 1c and d).3,5,6 Warren and coworkers reported β-diketiminate supported neutral, nominally NiIII imides (Fig. 1e).2,13 Of note, Hillhouse's two-coordinate, carbene supported NiII imido5 and Warren's NiIII imido complexes2,13 are competent for nitrene transfer into vinylic and benzylic C–H bonds, respectively. Each example represents a highly electrophilic imido complex capable of functional group transfer. Given the promising capability Ni imido species exhibit towards C–H bond functionalization, we were interested in investigating the synthesis of dipyrrin-supported Ni analogues. We report herein the synthesis, characterization, and reactivity of two Ni iminyl complexes bearing aryl and alkyl N-substituents.
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| Fig. 1 All previously reported Ni imides.1–6 | ||
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| Fig. 2 Solid-state molecular structure for (a) (AdFL)NiCl(py)2 (1) and (b) (AdFL)Ni(py) (2) with thermal ellipsoids at 50% probability level. Color scheme: Ni, pink; N, blue; C, gray; Cl, yellowgreen; F, green. H atoms omitted for clarity. (c) Frozen solution EPR spectrum of (AdFL)Ni(py) (2) collected at 77 K in toluene (red). Blue line represents a fit of the data using the program EasySpin.7 Fitting parameters: S = 1/2, g1 = 2.438, g2 = 2.121, g3 = 2.064. | ||
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| Scheme 1 Synthesis of (AdFL)NiCl(py)2 (1), (AdFL)Ni(py) (2), (AdFL)Ni(NMes) (3), and (AdFL)Ni(NAd) (4). | ||
Chemical reduction of 1 with KC8 in thawing THF solution cleanly generated the pyridine adduct (AdFL)Ni(py) (2, Scheme 1) as a dark brown solid. Crystals of 2 suitable for single-crystal X-ray diffraction were obtained by storing a concentrated hexanes solution at −35 °C overnight (Fig. 2b). The solid-state structure of 2 unveils a pyramidally distorted T-shape geometry around the Ni center with an NL–Ni–Npy angle of 146.4(2)°, similar to the previously reported three-coordinate NiI β-diketiminate complex by Warren and coworkers (Fig. 1e).2 The EPR spectrum of 2 collected at 77 K in toluene indicates that the unpaired electron occupies a rhombic environment (g1 = 2.438, g2 = 2.121, g3 = 2.064; Fig. 2c).
The Ni–Nim distance of 1.696(2) Å in 3 is longer than the bis-phosphine supported cationic NiIII aryl imide [(dtbpe)Ni(NAr)]+ (1.674(3) Å)4 but similar to those three coordinated NiII aryl imides supported by the same ligand (1.697(2) → 1.703(4) Å)1,3,4 and bis-N-heterocylic carbene (NHC) ligand ((NHC2)Ni(NAr): 1.718(2) → 1.732(4) Å) (Fig. 1 and S7†).6 The imido linkage in 3 strongly deviates from linearity [∠(Ni–Nim–CMes): 146.5(2)°] in contrast to its linear bisphosphine supported analogue [(dtbpe)Ni(NAr)]+ [∠(Ni–Nim–CAr): 178.4(3)°]4 but similar to the bis-NHC system [(NHC2)Ni(NAr), ∠(Ni–Nim–CAr), Ar: 127.3(3)°, Mes; 170.0(2)°, DIPP] (Fig. 1 and S7†).6 The deviation from linearity for the Ni–N–CAr linkages occur most often with late transition metals featuring population of high-energy, antibonding (M–N)π* orbitals. Other factors that can contribute to distortions away from non-linearity include imido-group constraints incorporated into a chelate ring and crystal-packing effects within the crystalline lattice.6
Close inspection of the C–C bond lengths within the mesityl group of 3 (Fig. 3a and b) reveals the elongation of the Cipso–Cortho bonds (1.423(4), 1.429(4) Å), analogous to our previously reported FeIII iminyl species37–40 as well as all the previously reported Ni aryl imido complexes (Fig. S7†).1,3–6 The Nimido–CMes distance in 3 (1.348(4) Å) is in the range of a partial C–N double bond, indicating delocalization of electron density from Ni–Nimido π system to the mesityl aryl moiety.17
The Ni–Nim distance of 1.642(7) Å in 4 is consistent with reported three-coordinate NiIII alkyl imide supported by β-diketiminate ligand (1.662(2) Å)2 and Ni alkyl imides [(dtbpe)Ni(NAd)]n (n: +1, 1.673(2); n: 0, 1.657 (5) Å);3,4 and comparatively shorter than the Ni–aryl imido complexes (Fig. 1 and S7†). The shortened Ni–Nim bond is consistent across all ancillary ligand platforms, potentially due to the lack of π-delocalization into the imido aryl moiety. The alkyl imido linkage in 4 is more linear [∠(Ni–Nim–CAd): 164.8(17)°] compared to 3, and similar to all three reported Ni alkyl imides [∠(Ni–Nim–CAd): 163.0(2) → 165.2(4)°], regardless of ancillary ligand or oxidation state.2–4
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Fig. 4 (a) Frozen solution EPR spectrum of (AdFL)Ni(NMes) (3) collected at 77 K: S1 = 1/2, g11 = 2.238, g12 = 2.106, g13 = 1.940; S2 = 1/2, g21 = 2.302, g22 = 2.128, g23 = 1.962, relative weight = 1 : 1 (red); blue line represents a fit of the data using the program EasySpin;7 (inset) enlarged spectrum showing hyperfine splitting attributable to two mesityl ring orientations. (b) Frozen solution EPR spectrum of (AdFL)Ni(NAd) (4) collected at 77 K: S = 1/2, g1 = 2.185, g2 = 2.063, g3 = 1.924 (red); blue line represents a fit of the data using the program EasySpin;7,8 (inset) enlarged spectrum showing hyperfine splitting, A = 21.3 G (14N, I = 1).7,9 (c) Variable-temperature susceptibility data for of 3 collected at 1.0 T, with χMT = 0.41 cm3 K mol−1 at 295 K; (inset) solid-state magnetometry data for 3 of M vs. H at 100 K, showing the absence of ferromagnetic impurities. | ||
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| Fig. 5 Cyclic voltammogram of 3 obtained in THF at 25 °C, with 0.1 M (nBu4N)(PF6); 100 mV s−1; referenced to [Cp2Fe]+/0 couple; OCP = −1.25 V; ΔE = 310 mV. | ||
The 0.8 V cathodic shift comparing [(dtbpe)Ni(NAr)]+versus neutral 3 likely largely reflects the change in molecular charge between the two species as opposed to effects originating with ligand field strength. Chemical reduction of 3 was attempted using decamethylcobaltacene
or KC8 as a reductant in frozen-thawing THF.46 In both cases, unfortunately, only inseparable mixtures of decomposition of 3 as ascertained by analysis of the crude reaction mixture by 19F NMR spectroscopy were obtained. Similar results were obtained when similar chemical reduction was attempted with alkyl imide 4.
To gain further insight into the redox states in the Ni/N pairs in 3 and 4, the nitrogen valence was probed directly using nitrogen K-edge XAS. As seen in Fig. 6b, pre-edge features at 398.0 and 400.9 eV are observed for all the complexes surveyed (2–5) that can be assigned as transitions into high-lying antibonding molecular orbitals of N 2p parentage.40,47 Two low-lying pre-edge absorptions are present for both 3 and 4 at 395.4 eV, accompanied by a smaller side-band at 396.3 eV. These peak energies are consistent with those encountered for the redox-active N-donor ligands in Fe-iminyl (394.5 and 394.8 eV),40 Ni–aminyl (397.0 eV),47 and Cu–nitrene48 (doublet with peaks at 395.3 and 395.9 eV) complexes. This tentative assignment of these transitions as N 1s into partially occupied, N-localized orbitals present in 3 and 4, respectively is further supported by time-dependent density functional theory (TDDFT) calculations (vide infra). However, quantitative covalency analysis was precluded by sensitivity of these samples to rapid photodamage that principally affected the low-energy pre-edge peaks of interest (Fig. S13†).
49,50 generalized gradient approximation (GGA) functional as well as the B3LYP51,52 hybrid density functional. The broken symmetry (BS)53–55 method was applied in both cases to ascertain whether antiferromagnetic coupling between a high-spin d8 NiII and a ligand radical (i.e., imido oxidized to an iminyl) could plausibly be invoked to yield the experimentally observed S = 1/2 ground states. No BS(2,1) solution was obtained for either species using the BP86 functional. Analogous calculations using B3LYP gave broken symmetry solutions with corresponding orbital overlap values near unity (3 = 0.68, 4 = 0.89) and whose total energies were effectively identical to those obtained using a standard unrestricted DFT approach.
To afford some justification for selecting between BP86 and B3LYP results, TDDFT calculations47,56,57 to model the N K-edge XAS obtained for 3 and 4 were carried out starting from either unrestricted single point solution. Spectra calculated using BP86 gave insufficient resolved peak structure to reliably correlate to the experimental data (Fig. S14†), whereas B3LYP-calculated spectra adequately reproduced pre-edge features, with a linear fit of experimental to calculated data giving R2 = 0.99 (Fig. 7). Agreement between calculated and experimental spectra is quite good in the case of 3, but less so in the case of 4.
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| Fig. 7 Experimental and TDDFT-calculated N K-edge XAS pre-edge regions for (a) (AdFL)Ni(NMes) (3), and (b) (AdFL)Ni(NAd) (4). Calculations were initiated from spin-unrestricted B3LYP single points using the CP(PPP) basis set on Ni and the ZORA-def2-TZVP(-f) basis set on all other atoms. Energies for the calculated spectra were adjusted using a linear correction presented as Fig. S15.† Unrestricted Kohn–Sham orbitals corresponding to the acceptor MOs involved the excitation giving the ca. 395 eV pre-edge peak are plotted at an isovalue of 0.03 au. | ||
The first peak in the N K-edge XAS of 3 is predicted as an excitation from N 1s to an MO dominated by iminyl character, because the MO is less than 50% Ni in character.58 This MO is delocalized over the NMes fragment and is comprised of 32.3% N 2p, 33.3% Mes arene π*, and 10.2% Ni 3d. The weaker, second pre-edge peak is assigned as an excitation involving a near equal mix of two acceptor MOs featuring large (10–20%) contributions from the orthogonal Nim 2p orbitals as well as dipyrrin π* contributions. In the case of 4, qualitatively similar excitations are involved, although the ordering is reversed from 3: the first excitation features contributions from 2 MOs, while the second excitation is analogous to the first excitation of 3. The estimated error in peak energy prediction from our prior N K-edge TDDFT study is on the order of 0.5 eV, so this discrepancy is not unexpected. Regardless, the pre-edge of 4 also features excitations to an MO with a large degree of Nim N 2p vacancy. Much less delocalization is possible in the imido fragment of 4, consequently this acceptor MO features 42.8% total contribution from NAd (37.7% N 2p), and 35.0% Ni 3d.
Quasi-restricted orbitals (QROs)59 were generated from the unrestricted B3LYP solutions to facilitate interpretation of the ground-state electronic structures of 3 and 4 (Fig. 8). The picture that emerges for both is that the unpaired electron resides in a MO of principally Ni 3d and Nim character reflecting a π* interaction. For 3, this MO comprises 58.5% Ni 3d and 24.3% NMes N 2p character. For 4, corresponding parentages are 33.0% Ni 3d and 46% NAd N 2p. The ca. 2-fold larger N 2p contribution to the SOMO of 4 is consistent with the resolved 14N HFC in its EPR spectrum—such fine structure is not resolved in the spectrum of 3. Each complex has one remaining unoccupied orbital featuring Ni 3d character, reflecting a π* interaction with Nim 2p. This is the LUMO for 3, which comprises 37.7% Ni 3d and 20.9% NMes N 2p. For 4, this is LUMO+1, which features 47.3% Ni 3d and 27.7% NAd N 2p. The ground state electronic configuration for 4 appears more consistent with a formal iminyl assignment, while the larger Ni parentage of the SOMO (58.5% Ni 3d) for 3 suggests 3 presents more imido-like character. Overall, the highly covalent Ni–Nim interactions can be viewed as total donation of a single electron from the Nim 2p orbitals involved in Ni–N bonding, giving rise to the iminyl character observed.
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| Fig. 9 Molecular structure of (AdFL)Ni(NHAd) (5) with the ellipsoid probabilities set at 50%. C, gray; N, blue; H, white; Ni, pink; F green. | ||
Dissolving 4 in toluene resulted in slow conversion into 5 along with decomposition into ligand over the course of two days. The amount of 5 generated is quantified by 19F NMR spectrum to be 46% against an internal standard (trifluorotoluene), and the organic product is identified to be N-1-adamantyl-benzilidene (6) as evidenced by 1H NMR spectrum of the quenched reaction mixture (Scheme 2). The concentration of 4 in toluene was monitored by 19F NMR spectroscopy and can be fitted as a first-order decay (Fig. 10). An intermolecular KIE of 40 was measured over 80 days when d8-toluene was used as the solvent. However, due to the slow rate of the reaction, decomposition of 4 can also contribute to the large KIE value. Based on the C–H amination reaction mediated by previously reported NiIII β-diketiminate imides, we hypothesized that 4 can outcompete 5 (in situ) at capturing tolyl radical, giving rise to a secondary amido intermediate. This intermediate would then undergo β-hydride elimination and release the imine product. A similar mechanism was proposed by Warren et al. as a rationale towards their crystallographically characterized rearranged NiII product.2,13 An alternative mechanism would involve H-atom abstraction of benzyladamantylamine with a second equivalent of 4, generating both the imine product observed and 5 as a byproduct.
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| Fig. 10 Concentration profile of 4 during reaction between (h8/d8-)toluene and 4 by 19F NMR spectroscopy. Trifluorotoluene is used as internal standard. | ||
In order to facilitate the radical recombination with the amido species formed in situ, the activated C–H bond was installed onto the azide. Addition of 1 equiv. of (4-azidobutyl)benzene (7)22 to a C6D6 solution of 2 resulted in instantaneous color change from dark brown to dark pink along with vigorous effervescence. The bubbling ceased after 10 min along with the solution reversion to a dark brown color, and 19F NMR spectrum revealed full regeneration of 2. However, rather than the anticipated cyclized pyrrolidine product,22,31,411H NMR analysis revealed the major organic product to be 4-phenylbutanenitrile (8, Scheme 3). To test the possibility of catalytically converting azide 7 to nitrile 8, 3–6 equivalents of azide 7 were added slowly to a C6D6 solution of 2. Full decomposition of catalyst 2 was observed when greater than five equivalents of the azide substrate 7 were used, potentially due to the high concentration of product nitrile 8. With 20 mol% catalyst loading of 2, azide 7 is catalytically converted to 4-phenylbutanenitrile 8, providing a moderate isolated yield of 78%. We propose the product is formed by iminyl generation following N2 extrusion from azide 7; β-H elimination (originating from the α-methylene unit) outcompetes intramolecular H-atom abstraction from the benzylic position to generate a Ni(hydride)(ketimide) intermediate. A rapid H2-elimination via deprotonation of the ketimide Ni(hydride) furnishes the final nitrile 8. Attempts to slow down this pathway by deutero-substitution at the gem position were ineffective.
Footnote |
| † Electronic supplementary information (ESI) available. CCDC 1953729–1953733. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c9sc04879k |
| This journal is © The Royal Society of Chemistry 2020 |