C. A.
Laskowski
a,
G. R.
Morello‡
b,
C. T.
Saouma
c,
T. R.
Cundari
*b and
G. L.
Hillhouse
*a
aGordon Center for Integrative Science, Department of Chemistry, The University of Chicago, 929 E. 57th St., Chicago, IL 60637, USA. E-mail: g-hillhouse@uchicago.edu
bCenter for Advanced Computing and Modeling, Department of Chemistry, University of North Texas, Denton, TX 76203, USA. E-mail: t@unt.edu
cDepartment of Chemistry, Massachusetts Institute of Technology, Cambridge, MA 02139, USA
First published on 24th September 2012
The dimeric Ni(I)–Ni(I) N-heterocyclic carbene complex {(IPr)Ni(μ-Cl)}2 (3; IPr = 1,3-(2,6-iPr2C6H3)2imidazolin-2-ylidene)) reacts with the lithium terphenylamides LiNHdmp and LiNHdippp (dmp = 2,6-di(mesityl)phenyl; dippp = 2,6-bis(2,6-di-iso-propylphenyl)phenyl) to give the monomeric Ni(I) amides (IPr)Ni(NHdmp) (4) and (IPr)Ni(NHdippp) (5), respectively. These nickel amides are 1-electron paramagnets, and crystallographic characterization indicates both are stabilized by Ni–C(ipso) interactions with a flanking aryl group of the terphenyl fragment. This results in significant deviation from the linear CNHC–Ni–N geometry typical for a two-coordinate transition-metal complex (112.17(9)° in 4, 116.41(9)° in 5). One-electron oxidation of 4 by ferrocenium results in intramolecular deprotonation at a terphenyl benzylic position by the amide, giving the diamagnetic Ni(II) complex [(IPr)Ni(κ2-C,N:NH2C6H3(Mes)C10H9)][B(ArF)4] (7). DFT calculations on oxidized 4 (i.e., 4+) indicate short amide N⋯CH3 interactions. One-electron oxidation of 5 by ferrocenium gives a new high-spin Ni(II) amide complex salt, [(IPr)Ni(NHdippp)][B(ArF)4] (9). The solid-state structure of 9 indicates it maintains the bent CNHC–Ni–N core. Unlike three-coordinate cationic Ni(II) amides, 9 has not been observed to undergo smooth deprotonation (at N) to afford a two-coordinate imido complex.
The chemistry of 3-coordinate Ni imides like 2 is reasonably well-developed, and they can be prepared in good yield by three routes: (i) directly by reaction of Ni(0) derivatives with organoazides; (ii) by sequential oxidation and deprotonation of Ni(I) amides such as (dtbpe)Ni(NHAr); or (iii) by H-atom abstraction from Ni(I) amides (Scheme 1).2–4 The chemistry of 2-coordinate imides is much less developed, with 1 being the only example, and the organoazide route is thus far the only successful method for its synthesis (from the Ni(0) toluene adduct (IPr*)Ni(η6-C7H8)). Since 2 was originally prepared via sequential oxidation and deprotonation of (dtbpe)Ni(NHAr), we were curious if this method could be applied to generating 2-coordinate imides. We have found that the analogous transformation, requiring a cationic, 2-coordinate, 12-e− amide intermediate, presents unique challenges.
Scheme 1 Three independent routes to 3-coordinate Ni imides. |
Combination of LiNH(dmp) with 3 in Et2O solution results in elimination of LiCl with formation of the paramagnetic d9 amide (IPr)Ni(NHdmp) (4) that can be isolated in 84% yield as a rust-red solid (μeff = 1.88μB in C6D6; Scheme 2). Single crystal X-ray studies of 4 indicate significant steric congestion about Ni with Ni–N = 1.936(2) Å, greatly increased from the Ni–N distance of 1.831(4) Å found in (IPr)Ni(NHAr) (Fig. 1).5b Planes defined by the NHC five-membered core and the central terphenyl ring of the amide are twisted ∼7.3° from coplanarity. The C(1)–Ni–N(3) angle of 112.17(9)° deviates dramatically from linearity, allowing for a short, stabilizing contact with the ipso-carbon on a flanking mesityl group of the dmp ligand (Ni–C(51) = 2.137(2) Å), with longer Ni distances of 2.502(2) and 2.396(3) Å to the ortho carbons of that mesityl. Similar interactions are seen in the Ni(I) thiolate complex (IMes)Ni{S(dmp)}, where the metal center engages in an η2 Ni-aryl bonding mode with Ni–C distances of ∼2.1 Å.8
Scheme 2 Formation of IPr-supported terphenyl amides via chloride substitution from 3. Oxidation of the resulting Ni amides leads to either C–H activation or simple cation formation. A = B(ArF)4 anion. |
Fig. 1 X-ray structure of 4 (50% ellipsoids). The amide H-atom was located in the difference map and refined isotropically. Selected metrical parameters for 4: Ni–N(3) = 1.936(2), Ni–C(1) = 1.949(2), Ni–C(51) = 2.137(2), Ni–C(52) = 2.502(2), Ni–C(56) = 2.396(3) Å; C(1)–Ni–N(3) = 112.17(9), C(1)–Ni–C(51) = 165.81(9), C(51)–Ni–N(3) = 81.99(9)°. |
The bulkier amide LiNHdippp (dippp = 2,6-bis(2,6-di-iso-propylphenyl)phenyl) affords (IPr)Ni(NHdippp) (5) in 79% yield upon reaction with 3. The solid-state structure of 5 (Fig. 2) shows Ni–N(3) = 1.953(2), Ni–C(41) = 2.114(2) Å and C(1)–Ni–N(3) = 116.41(9)°. In contrast with the rigorously linear (N–Ni–N) geometry found in Ni(NHdippp)2 (6), 5 has a much shorter interaction with the ipso carbon of the dippp subunit (cf. 2.680 Å in 6).9 Similar bonding motifs have been observed by Power et al. in 2-coordinate terphenylamide complexes of other 3d metals.10
Fig. 2 X-ray structure of 5 (50% ellipsoids). The amide H-atom was located in the difference map and refined isotropically. Ni–N(3) = 1.953(2), Ni–C(1) = 1.959(2), Ni–C(41) = 2.114(2), Ni–C(42) = 2.385(2), Ni–C(46) = 2.380(2) Å; C(1)–Ni–N(3) = 116.41(9), C(1)–Ni–C(41) = 161.90(9), C(41)–Ni–N(3) = 81.62(9)°. |
A cyclic voltammogram of 4 exhibits an irreversible oxidation event at −0.63 V (vs. Cp2Fe/Cp2Fe+, THF/TBAH), attributed to oxidation of 4 to a Ni(II) species. Chemical oxidation can be accomplished with ferrocenium-based oxidants, and combination of Et2O solutions of 4 with [Cp2Fe][B(ArF)4] (ArF = 3,5-(CF3)2C6H3) allows for the subsequent isolation of a highly unsymmetric, diamagnetic species (Scheme 2). 1H-NMR spectra of the blue product show five singlets for inequivalent alkyl groups of the dmp fragment and four doublets for the isopropyl methyl groups in the IPr ligand.
X-ray studies revealed that the oxidation product, [(IPr)Ni(κ2-C,N:NH2C6H3(Mes)C10H9)][B(ArF)4] (7, Scheme 2; Fig. 3), contains an unusual 7-membered metallacycle featuring new Ni-κ1-benzyl and Ni-κ1-amine bonds. Thus, 1-electron oxidation of 4 results in formal deprotonation of a dmp ortho-methyl by the basic amide to give a 3-coordinate, 14-e− T-shaped Ni(II) benzyl amine complex salt. The neutral IPr and NH2R ligands occupy mutually trans positions (C(1)–Ni–N(3) = 159.8(2)°), with the strongly trans-directing benzyl moiety oriented cis to them (C(1)–Ni–C(421) = 102.3(2), C(421)–Ni–N(3) = 97.8(2)°). The amine ligand has a Ni–N(3) distance of 1.972(4) Å, similar to other σ-donor nickel amines,11 and its two hydrogen atoms were located in a difference map in the X-ray structure. The short Ni–C(421) distance (1.866(6) Å)12 is similar to the Ni–CH3 distance of 1.907(7) Å observed in T-shaped [(IPr)Ni(CH3){N(SiMe3) = SiMe2·Et2O}][B(ArF)4], in which the coordination site trans to the methyl ligand is also vacant.5b
Fig. 3 X-ray structure of 7 (50% ellipsoids). H-atoms except on N(3) and C(421) and the entire B(ArF)4 counterion have been omitted for clarity. Selected metrical parameters for 7: Ni–N(3) = 1.972(4), Ni–C(421) = 1.866(6), Ni–C(1) = 1.858(5) Å; C(1)–Ni–C(421) = 102.3(2), C(1)–Ni–N(3) = 159.8(2), N(3)–Ni–C(421) = 97.8(2)°. |
Carrying out the oxidation of 4 in THF, or addition of THF to solutions of 7, results in solvent coordination to give a 4-coordinate complex [(IPr)Ni(OC4H8)(κ2-C,N:NH2C6H3(Mes)C10H9)][B(ArF)4] (8) as a dark-red solid that has been characterized by NMR, X-ray crystallography (Fig. 4), and elemental analysis. Ligation of THF results in a slight elongation of both the trans carbyl group and the Ni–N bond (Ni–N(3) = 2.001(2), Ni–C(421) = 1.931(3), Fig. 4). Removal of the bound THF can be accomplished by precipitation of 8 from Et2O or CH2Cl2.
Fig. 4 X-ray structure of 8 (50% ellipsoids). H-atoms except on N(3) and C(421) and the entire B(ArF)4 counterion, have been omitted for clarity. Selected metrical parameters: Ni–N(3) = 2.001(2), Ni–C(421) = 1.931(3), Ni–C(1) = 1.904(3), Ni–O = 2.057(2) Å; C(1)–Ni–O = 95.05(10), O–Ni–N(3) = 84.86(9), N(3)–Ni–C(421) = 88.40(12), C(1)–Ni–C(421) = 91.74(12), C(1)–Ni–N(3) = 177.44(12), O–Ni–C(421) = 173.17(11)°. |
Unlike 4, a cyclic voltammogram of 5 indicates a quasi-reversible oxidation potential at E1/2 = −0.63 V (vs. Cp2Fe/Cp2Fe+, THF/TBAH). 5 can be cleanly oxidized with [Cp2Fe][B(ArF)4] to give a new paramagnetic Ni(II) complex, [(IPr)Ni(NHdippp)][B(ArF)4] (9, 94% yield, Scheme 2). Reaction of 9 with KC8 results in 1-e− reduction with reformation of 5 in 72% isolated yield. Electronically, replacing the strong-field alkyl ligand in 7 with a weaker-field amide in 9, and replacing an amine ligand in 7 with a weak Cipso–π interaction in 9 shifts the ground-state of these molecules from singlet (in 7) to triplet (in 9) configurations.
The solid-state structure of the cationic Ni core of 9 (Fig. 5) shows subtle differences from the parent neutral Ni(I) complex, with Ni–N = 1.854(2) and Ni–C(41) = 2.240(2) Å in 9. Despite the stabilizing contact between Ni and the flanking mesityl ring, 9 is high-spin d8 and with a magnetic moment of 3.2μB (SQUID) at room temperature, somewhat higher than the spin-only value of 2.83μB and similar in its magnetic profile to that seen for the bent, 2-coordinate Ni(II) amide Ni(NHdmp)2.10a Presumably, the increased steric bulk of the iso-propyl groups on the dippp ligand prevents C–H activation of an ortho-methine hydrogen as seen with the dmp derivative. A DFT analysis of the complex cation of 9 (B3LYP/6-31G(d) level) indicates a triplet ground state (ΔGST = 12 kcal mol−1) in which the optimized structure closely mimics that observed in the solid-state (Fig. 6). Interestingly, the optimized singlet and triplet DFT structures show similar Ni–N interactions, but an η6-coordination of one of the 2,6-diisopropylphenyl groups of the dippp ligand makes the singlet an 18-electron species. We have thus far been unsuccessful in cleanly deprotonating the amide ligand of 9 to give a neutral Ni(II) imide, possibly due to steric issues.13
Fig. 5 X-ray structure of the cation of 9 (left, 50% ellipsoids) and solid-state magnetic data at 5000 G (right). Most H-atoms and B(ArF)4 counterion omitted for clarity; selected metrical parameters: Ni–N(3) = 1.854(2), Ni–C(41) = 2.240(2), Ni–C(1) = 2.003(2) Å; C(1)–Ni–N(3) = 116.57(9), Ni–N(3)–C(31) = 122.0(2), N(3)–Ni–C(41) = 81.16(8), C(1)–Ni–C(41) = 162.17(8)°. |
Fig. 6 Optimized computed DFT structures of the complex cation of 9 for the triplet (left) and singlet (right) states, with calculated Ni–N distances of 1.846 and 1.872 Å, and angles of Ni–N–C (121.8 and 117.6°) and CNHC–Ni–N (117.0 and 99.1°), for the triplet and singlet structures, respectively. Ni is in green and N is in blue. |
The mechanism by which 4 undergoes benzylic activation of the NHdmp ligand is difficult to probe experimentally due to its paramagnetism. Cationic Ni(II) alkyls with γ-C–H agostic interactions, like the trimethylsilylmethyl complex cation [(dtbpe)Ni{CH2Si(CH3)3}][PF6], undergo smooth deprotonation by exogenous base to give neutral metallacyclobutane products (Scheme 3).14 It seemed reasonable that direct intramolecular deprotonation of a weak benzylic C–H bond (perhaps further weakened by an agostic interaction) in a cationic Ni(II) amide might be operative.
Scheme 3 Deprotonation with metallation of a –CH3 group in a cationic Ni(II) complex cation to give a new Ni-alkyl bond.13 |
DFT calculations were carried out at the B3LYP/6-31G(d) level to elucidate the transformation of 4 to 7. While the optimized structure of the cation generated by removal of an electron from DFT-optimized 5 (5+ singlet) shows no protons in the vicinity of the amide nitrogen (all >3 Å except that directly bonded to N), the optimized structure of 4+ (singlet generated from DFT optimized 4) has a benzylic proton very close to the amide (∼2.61 Å; Fig. 7). Moreover, the benzylic C–H should be more acidic for aryl-CH3versus aryl-CMe2H since carbanions are less stable for more substituted carbons. Finally, the free energy to convert 4+ to 7 is calculated to be exergonic by 9 kcal mol−1. Taken together, synthetic, crystallographic, and DFT studies implicate an intramolecular deprotonation mechanism for the conversion of 4 to 7 upon ferrocenium oxidation.
Fig. 7 Optimized computed DFT structure of 4+, the (experimentally unobserved) complex cation formed on 1-e− oxidation of 4 that ultimately gives the observed metallated product 7. ΔG4+/7 (calculated) = −9 kcal mol−1. |
Footnotes |
† Electronic supplementary information (ESI) available: Crystallographic details for 4, 5, 7, 8 and 9, data regarding the crystallographic refinements, and experimental and computational details (PDF). CCDC 896901–896905 contain the supplementary crystallographic data for this paper. See DOI: 10.1039/c2sc21345a |
‡ Current address: PPG Industries, 440 College Park Drive, Monroeville, PA, 15146, USA. |
This journal is © The Royal Society of Chemistry 2013 |