Cu-Catalyzed Enantioselective Alkynylation of Aldehydes with Terminal Alkynes
FULL PAPER
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sulted in convergence to eight TS structures for each isomer
(see Table S2 in the Supporting Information). The two most
meaningful conformers out of the eight were further opti-
mized at the B3LYP level with a larger basis set BI (see Fig-
ure S5 in the Supporting Information). Figure 4 shows the
most stable structures of TSs that lead to the major (M) and
conformers without a C H···O hydrogen bond are no less
than 16.0 kJmolÀ1 higher in Gibbs free energy (B3LYP-D-
AHCTUNGTREG(NNNU PCM)/BI//B3LYP/B0; see Table S3 in the Supporting Infor-
mation). Consequently, the directional two-point hydrogen-
bonding orients the carbonyl group. Nevertheless, the M
and m structures are almost equal in stability, and calcula-
tions of the Boltzmann distribution at 258C from the Gibbs
free energies of all the optimized structures for this modeled
system give an M/m abundance ratio (e.r.) as low as
57.4:42.6 (see Table S4 in the Supporting Information).
We then performed calculations for a more advanced
ꢀ
model system (model 1b) with L1, 1a, and a C CSiiPr3
group (2a-H), which corresponds to the experiment that
showed the moderate enantiomeric ratio of 85:15 (Table 1,
entry 10). To decrease the cost of the calculations, only a
single conformation of the CyCHO molecule and the most
stable three conformations of the SiiPr3 moiety were consid-
ered; the latter were obtained by conformational analysis of
2a at the HF/6-31G* level with the Spartan 08 program.[38]
The calculations, albeit with considerable ambiguity due to
the conformational constraints in the CyCHO molecule,
gave a reasonable M/m abundance ratio of 74.9:25.1 e.r. (see
Figure S10 and Table S6 in the Supporting Information).
After preliminary examination of the other simplified
model system (model 2a) with the neopentyl-substituted
ligand L2 (see Figure S11 and Table S7 in the Supporting In-
formation), which gave a M/m ratio of 64.0:36.0 e.r., we per-
formed calculations for a system (i.e., model 2b) with L2,
Figure 4. The most stable structures of the major (M) and minor (m)
À ꢀ
transition states for model 1a (L1, MeCHO, C CSiMe3). Phenyl groups
are shown as light-blue balls for clarity.
ꢀ
1a, and a C CSiiPr3 group (2a-H). These conditions corre-
minor (m) enantiomeric products, in which the pyrrolidine
ring adopts an envelope-type conformation with an out-of-
plane N atom and an equatorial hydroxymethylene side
chain. A reasonable value of 72.9 kJmolÀ1 was obtained for
the Gibbs activation energy of alkynylation through the
most stable TS(M) (see Figure S7 in the Supporting Infor-
mation). In contrast, four-centered TSs, in which the carbon-
yl oxygen atom is directly coordinated to the Cu atom with
the OH group of the ligand free from coordination, were
greater than 70 kJmolÀ1 higher in total electronic energy rel-
ative to the six-centered TSs (see Table S5 and Figures S8
and S9 in the Supporting Information). Accordingly, for fur-
ther studies, we decided to consider only six-centered TSs
that adopted the pyrrolidine and P,N-chelate-ring conforma-
tions as in the most stable TSs of model 1a (Figure 4).
spond to the optimal reaction conditions in the experiments
(Table 1, entries 13–15, and Figure 2). Geometry optimiza-
tions were conducted for 27 conformers for each of TS(M)
and TS(m), with different conformations of the neopentyl
group (ꢂ3), the CyCHO molecule (ꢂ3), and the SiiPr3
group (ꢂ3; see Table S8 and Figure S12 in the Supporting
Information). The most stable structures of M and m are
shown in Figure 5a. The M/m abundance ratio based on the
Boltzmann distribution at 258C from the Gibbs free ener-
gies of all the optimized structures was 96.9:3.1 e.r. (see
Table S8 in the Supporting Information) in accord with the
efficient enantiocontrol (up to 97:3 e.r. in tBuOH at 258C)
with the Cu/L2 system in the experiments.
The neopentyl group of L2 is relatively distant from both
the alkyne and aldehyde substrates, thus overhanging the
Cu-bound hydroxy group with its tBu hammerhead: the hy-
drogen atom on the carbon atom at the a position to the
OH group and the OH oxygen atom have van der Waals
contacts with the nearest tBu hydrogen atoms (Figure 5a).
The P-phenyl groups (omitted in Figure 5a) are also located
in regions where no direct interaction with the substrates
occurs. Despite a lack of chiral ligand–substrate steric inter-
actions (which is unusual in enantioselective catalysis), the
directional two-point hydrogen bond arranges the aldehyde
carbonyl group asymmetrically in a well-defined manner. As
a result, the difference in the steric environment around the
aldehyde between TS(M) and TS(m) is evident, as shown in
the views from the plane of the aldehyde along the develop-
A surprising feature of the TSs of model 1a (Figure 4) is
that, in addition to the hydrogen bond between the OH
group and aldehyde oxygen atom with H···O atomic distan-
ces of 1.52 and 1.51 ꢁ, the pyrrolidine ring has a direct inter-
action with the carbonyl oxygen atom through a nonclassical
2
À
C
H···O hydrogen bond with an H···O atomic distance of
À
2.24 ꢁ for both TS(M) and TS(m). Although the C H bond
lengths are normal, the H···O atomic distances are consider-
ably shorter than the sum of van der Waals radii of the H
3
À
and O atoms (ca. 2.6 ꢁ). Similar sp -C H···O interactions
are found in organic crystal structures[29] and biomole-
cules,[30] although they have rarely been referred to in the
studies on artificial catalyst systems.[31–37] Other optimized
Chem. Eur. J. 2013, 00, 0 – 0
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