C O M M U N I C A T I O N S
and 2 is much easier to cleave homolytically. To test this hypothesis,
we treat the CH3CN-THF (1:4 v/v) solution of 1 with CO at room
temperature.
The insertion of CO into the NiII-methyl bond in monomeric
or dimeric alkylnickel model complexes producing the NiC(O)Me
species was described in the literature.2c,e,15 In contrast, the reaction
between CO and 1 leads to NiII-thiolate carbonyl [NiII(CO)(P(C6H3-
3-SiMe3-2-S)3)]s (3),10b as shown in Scheme 1b. The lack of
observation of the acylnickel species from the reaction of CO with
1 but isolation of 3 may imply that the formation of the proposed
[(CO)NiIII(CH3)(P(C6H3-3-SiMe3-2-S)3)]s intermediate followed by
Ni-CH3 homolytic cleavage seems preferable to methyl migration
or CO migratory insertion.
The methyl group of 1 can undergo alkyl-for-chalcogenate
exchange with diphenyl dichalcogenide or protonation with
phenylthiol.15e When 1 and (PhE)2 (E ) S or Se) or PhSH are
mixed in solution at ambient temperature, [PPN][NiIII(EPh)(P(C6H3-
3-SiMe3-2-S)3)] (E ) S (4); Se (5)) are isolated in high yield
(Scheme 1c) (Figure S6).10
Figure 1. Plot of the spin density of 1. Orbital and atomic contributions
to the spin densities of 1 are shown in Supporting Information (Table S1).
Selected computed structural data (Å): Ni-CMe 1.949, Ni-Sav 2.329, Ni-P
2.175 (B3LYP/6-31G*).
In summary, we succeeded in the syntheses and structural
characterization of thermally unstable high-valent NiIII-alkyl
species (alkyl ) Me (1), Et (2)) with tetradentate ligand [P(C6H3-
3-SiMe3-2-S)3]3s, although a high redox potential of the NiIII-alkyl
state might be expected to undergo spontaneous reduction and
polymerization. The stability of 1 and 2 might be attributed to the
tunable electron-donating functionalities of ligand [P(C6H3-3-SiMe3-
2-S)3]3s, which shares similar characteristics with the noninnocent
factor of the F430 in MCR.9b Additionally, the results obtained from
this work may lend support to the intermediacy of NiIII-CH3 species
proposed in both ACS and MCR catalytic cycles. We also note
that 1 and 2 are capable of being used in reagents for alkyl transfer.
Detailed investigations are ongoing.
Figure 2. ORTEP drawings of [NiIII(CH3)(P(C6H3-3-SiMe3-2-S)3)]s (a)
and [NiIII(CH2CH3)(P(C6H3-3-SiMe3-2-S)3)]s (b) with thermal ellipsoids
drawn at the 50% probability level. Selected bond distances (Å): Ni-C(1)
1.994(3) for 1; Ni-C(1) 2.015(3) for 2.
ligand [P(C6H3-3-SiMe3-2-S)3]3 s (Figure S2). Attempts to identify
resonances of R hydrogens in 1 and 2 were unsuccessful, presum-
ably due to paramagnetic broadening, but the peak at δ -45.07
(br) is most likely due to ꢀ hydrogens of 2 (Figure S2b).
The 77 K EPR spectrum of 1 exhibits rhombicity with three
principal g values of 2.44, 2.00, and 1.96 (2.44, 1.99, 1.93 for 2,
Figure S3). The average g value of 1 (gav ) 2.13) indicates that
the unpaired electron is primarily associated with the nickel ion.10a
Indeed, the spin density result from density functional theory
computation reveals that the unpaired electron resides predominantly
Acknowledgment. We thank the National Science Council
(Taiwan) for financial support and Prof. Wen-Feng Liaw, Peter
P.-Y. Chen, and Dr. Tsai-Te Lu for helpful discussions.
Supporting Information Available: Crystallographic data in CIF
format and additional figures and experimental details (PDF). This
in the dxy and dx -y orbitals of Ni.11 The spin density plot of 1 is
shown in Figure 1 (Figure S4 for 2). According to the figures, the
atomic spin densities are 0.98 on nickel and -0.08 on methyl
carbon, respectively. Similarly, for 2 the atomic spin densities are
0.99 on nickel and -0.09 on ethyl carbon (Table S1). These results
are comparable to that of the EPR-active state of MCR (g⊥ ) 2.10,
g| ) 2.22), in which the unpaired electron is primarily located in the
2
2
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