Article
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inhibits the catalyst. It also implies that the methyl group of
2-amino-6-methylpyridine weakens the binding to the iridium centre,
thereby allowing alkene binding and insertion.
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To investigate the origin of the high levels of enantioselectivity in the
hydroamination, we conducted calculations on the alkene migratory
insertion using density functional theory (DFT). On the basis of the
kinetic experiments, this step is probably the rate-limiting and enantio-
determining step of the catalytic cycle. We calculated 12 possible iso-
meric transition states of migratory insertion that would lead to either
enantiomer of the products with cis-2-butene as the model alkene.
The structures of the lowest-energy transition states that lead to
the major and minor enantiomers are illustrated in Fig. 4d. The
two transition states of many metal-catalysed enantioselective
hydrofunctionalization reactions of alkenes to form two enantiomers
differ principally by the face of the alkene to which the metal is bound.
In the current system, the orientation of ancillary ligands around the
metal, in addition to the face of the alkene, differs greatly in the two
transition states. The geometry of TS-1a, the transition state leading
to the major enantiomer, contains meridionally oriented hydride,
pyridine and amido ligands with the hydride transto the amido group.
By contrast, these three ligands in TS-2a, which is the lowest-energy
transition state leading to the minor enantiomer, are arranged with
the hydride transto the pyridine donor. A geometry analogous to TS-
1a that would form the opposite enantiomer by orienting the methyl
groups away from the pyridine ligand (TS-2c and TS-2d; Supplemen-
tary Information Scheme S4) is higher in energy than is TS-2a. TS-1a
is probably the lowest-energy transition state for several reasons.
First, the Ir–Nam bond to the amido group, which is transto a hydride in
TS-1a, is elongated (2.32 Å), thereby leading to higher reactivity
towards insertion. Second, the alkene is perpendicular to the P–Ir–P
plane in TS-1a, whereas the alkene is almost co-planar with the P–Ir–P
plane in TS-2a. These orientations place the substituents on the alkene
in TS-1a farther from the phosphine ligand than those on the alkene
in TS-2a, leading to less steric hindrance in TS-1a than in TS-2a. This
analysis suggests that electronic and steric effects together impart
high enantioselectivity to the hydroamination.
Our work demonstrates that the direct N–H addition of amines
to unactivated internal alkenes can occur with high enantioselec-
tivity under thermal conditions, without the need for strategies
involving formal hydroamination. Despite the typically high barri-
ers and weak thermodynamic driving force for hydroamination,
the use of cationic bisphosphine-ligated iridium as the catalyst and
2-amino-6-methylpyridine as the amine led to enhancements of the
rates of multiple steps within the catalytic cycle and to suppression of
alkene isomerization and oxidative amination, enabling the hydroami-
nation of unactivated internal alkenes in high yield and with high enan-
tioselectivity. The hydroamination products can be converted to the
corresponding primary amines readily with preservation of the high
enantiomeric excess of the hydroamination products. These design
principles should provide a starting point to address the long-standing
challenge of applying hydroamination of unactivated internal alkenes
to the synthesis of chiral amines and inspire advances in other asym-
metric hydrofunctionalizations of internal alkenes.
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