J. He et al.
On the other hand, in the (2R,3R) transition state, the
C3-O3···H3 that is preserved in (2S,1’R) transition state.
Meanwhile, the aldehyde moiety (O6) and nitro moiety
(O8) in 4-nitrobenzaldehyde also form H-bonds with LDH
layer, which are 2.31 and 2.19 ꢁ in (2S,1’R) transition state,
whereas they are 2.32 and 2.25 ꢁ in (2R,1’S) transition state.
It can be predicted from either the alteration of H-bonds in
the substrate access and the difference between the H-
bonds in the transition states that LDH layers are to pro-
mote ee values with (2S,1’R) as the excess enantiomer.
À
À
C2 O1···H1 and C2 O2···H2 bonds are calculated to be 1.85
and 1.61 ꢁ when catalytic centers are located at the inner
interlayer regions, which are both stronger than those in the
(2S,3S) transition state (1.95 and 1.67 ꢁ). Moreover, a new
H-bond is formed between the alcoholic moiety (O4) in 2-
methyl-cinnamyl alcohol and the LDH layer, which is also
stronger in the (2R,3R) transition state than in the (2S,3S)
transition state (1.72 versus 1.81 ꢁ). When the catalytic cen-
ters are located at the edges of interlayer regions (Figure 3),
For the catalytic system in which the catalytic centers are
located at the edges of interlayer regions, the Si face attack
of aldehyde to the syn-enolate to form the (2R,1’S) transi-
À
although the C2 O1···H1 is stronger in the (2R,3R) transi-
tion state than in (2S,3S) transition state (2.05 vs. 2.10 ꢁ),
À
À
À
the C2 O2···H2 is weaker than in (2S,3S) transition state
tion state strengthens the C2 O1···H1 and C3 O3···H4 from
1.78 and 1.99 ꢁ to 1.74 and 1.91 ꢁ, whereas the Re face
attack of aldehyde to anti-enolate to form the (2S,1’R) tran-
(1.84 vs. 1.82 ꢁ). In addition, the 2-methyl-cinnamyl alcohol
molecules that attack in either concave or convex conforma-
tion form no new H-bond with the LDH layer, which de-
creases the difference in the H-bonding interaction between
(2R,3R) and (2S,3S) transition states. As a result, the energy
difference between (2R,3R) and (2S,3S) transition states is
2.94 kJmolÀ1 kJmolÀ1 lower when vanadium centers are lo-
cated at edge than at inner interlayer region, accounting for
less increment of the ee value when the catalytic centers are
located at edge than at inner interlayer region (80 vs.
91% ee for trans isomers). According to the calculation re-
sults based on experimental observations, it is apparent that
the efficient enhancement of enantioselective induction orig-
inates from the location of catalytic centers at the inner in-
terlayer regions, which supports the rational presumption
(Figure 1) of the significance of the plane-symmetry of inor-
ganic nanosheet as the substituent.
À
sition state preserves the C3 O3···H4 but has to weaken
À
C2 O1···H1 to 2.22 ꢁ (Figure 4). That means, it is easier for
Figure 4. The calculated energies and primary bonding distances for the
optimized transition states in the direct asymmetric aldol reaction when
the catalytic centers are located at the edges of the interlayer regions.
On the basis of the results for the vanadium-catalyzed ep-
oxidation, further theoretical prediction is performed on the
zinc-catalyzed direct asymmetric aldol addition of cyclohex-
anone to 4-nitrobenzaldehyde using l-glutamate as chiral
ligand. According to the optimized configuration (Fig-
ure 2c), both carboxylates of a-amino acid anion afford co-
ordination to Zn, facilitating the formation of an eight-
member ring to orient the carboxyl groups to the LDH
layer. The H-bonds between LDH layers and attached a-
(2R,1’S) to be formed than (2S,1’R) transition state. On the
À
À
other hand, although, the C2 O1···H1 and C3 O3···H4 are
weaker in (2S,1’R) transition state than in (2R,1’S) transition
state (2.22 and 1.99 ꢁ vs. 1.74 and 1.91 ꢁ), the H-bonds be-
tween the nitro moiety (O7 and O8) in 4-nitrobenzaldehyde
and LDH layer are calculated to be both stronger in
(2S,1’R) transition state than in (2R,1’S) transition state
(1.75 and 1.88 ꢁ vs. 1.96 and 2.00 ꢁ). That means, (2S,1’R)
is more stable than (2R,1’S) transition state. The difference
between the H-bonds in the transition states is conflict to
the alteration of H-bonds in the substrate access, making
neither (2S,1’R) nor (2R,1’S) isomer favored.
À
amino acid anions are calculated to be 2.22 (C2 O1···H1),
À
À
1.69 (C2 O2···H2), and 1.82 ꢁ (C3 O3···H3) when the Zn
centers are coordinated at the inner interlayer regions,
À
whereas they are calculated as 1.78 (C2 O1···H1) and 1.99
À
(C3 O3···H4) when the Zn centers are coordinated at the
edge interlayer regions. Our previous work[29] has revealed
that in the direct aldol addition of cyclohexanone to 4-nitro-
benzaldehyde, the Si face attack of aldehyde to syn-enolate
Experimental verification of LDH nanosheets as a valid
plane-symmetric substituent to enhance enantioselectivity in
zinc-catalyzed direct asymmetric aldol addition: According
to the theoretical prediction, the locations of catalytic cen-
ters are altered experimentally, and the relationship between
the ee value and locations of active centers have then been
explored (Figure 5). The dispersion of Zn centers along the
2D interlayer region has been probed by line-scanning
energy dispersive spectroscopy (EDS; Figure 5a). The Zn
centers are mainly located at the edges of interlayer regions
À
to form the (2R,1’S) transition state has to break C2
À
O2···H2 and C3 O3···H3 bonds when the catalytic centers
are located at the inner interlayer regions, whereas the Re
face attack of aldehyde to anti-enolate to form the (2S,1’R)
À
transition state well preserves C3 O3···H3 (1.83 vs. 1.82 ꢁ)
À
and only weakens C2 O2···H2 from 1.69 to 2.08 ꢁ. That
means, the formation of (2S,1’R) transition state is favored,
whereas (2R,1’S) is inhibited. In the (2R,1’S) transition state,
À
À
the H-bond C3 O3···H4 is formed instead of C3 O3···H3.
(Figure 5b) using Zn
to the l-glutamate-intercalated Zn/Al-LDH. With the Zn
ACHTUNGRTEN(NUNG OAc)2 as the precursor to coordinate
À
C3 O3···H4 is calculated to be 2.00 ꢁ, which is weaker than
12352
ꢀ 2013 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 2013, 19, 12350 – 12355