augment experimental development, we initially turned
to DFT calculations to discern to what, if any, extent this
process would afford enantioselection. Thus, working under
the assumption that allylation was the (R)- vs (S)-enantio-
selective-determining step of this reaction, the addition of 4
to 1 was modeled using the Gaussian 09 suite of programs
at the B3LYP/LanL2DZ level of theory with the IEFPCM
dielectric continuum solvation model and the default
parameters for THF (ε = 7.6).
Figure 1. Examples of natural products containing C(3)-chiral-
substituted phthalides.
optically enriched C(3)-chiral phthalides have been reported.8
Nevertheless, there remains a pressing need for sythetic
routes to C(3)-chiral phthalides, as the majority of the re-
ported approaches are limited in substrate scope, use
expensive and/or toxic rare earth transition metals, and
provide low levels of enantioselection.
Scheme 1. Envisioned Mechanistic Cycle for the Synthesis of
C
(3)-Substituted Phthalides
Fully aware of these limitations, we were drawn toward
the possibility of developing a more robust and syn-
thetically efficient strategy for preparing optically enriched
C(3)-chiral phthalides. Accordingly, we describe here a
target-oriented assembly of chiral C(3)-substituted phtha-
lides via the orchestrated use of rational forethought (i.e.,
density functional theory (DFT) calculations) in prelude to
experimental practice. Notably, this work has also pro-
vided theoretical models for rationalizating the enantioin-
duction of the reactions, and the ligand component used
was easily recoverable after the reaction. This work has
led to a revision of the stereochemical assignment of the
allylation products reported by Singaram et al. (vide infra).
At the outset of this work, with the goal of developing an
In-mediated protocol for preparing C(3)-chiral phthalides,
we envisioned using a reaction scenario such as that out-
lined in Scheme 1. In this mechanistic proposal, a highly
reactive In-allyl species, 4, is generated in situ from 3,
inexpensive indium metal, and allyl bromide (step 1).
Intermediate 4 then reacts with methyl-2-formylbenzoate
1 (step 2) to give allyl intermediate 5, which subsequently
undergoes a dual In-metal/pyridium salt (pyr-Hþ) cata-
lyzed intramolecular transesterification to afford (R)-3-
allylisobenzofuran-1(3H)-one 2 (step 3). However, because
of the frequently observed erosion in the enantioseletion
of catalytic asymmetric allylations of ortho-substituted
substrates,9ꢀ11 we were concerned if this process would
in fact impart enantioselectivity.12 For this reason, in
keeping with our philosophy of utilizing computation to
Surfacing from these calculations were a number of
insightful features with respect to the first-order saddle
points, (R)-TS1 and (S)-TS2, governing the (R)- vs (S)-
enantioselective allylation (Figure 2). A particularly domi-
nant feature of these transition states was the presence of a
bidentate mode of (LUMO-lowering) aldehdye activation
by the two In-metal centers (In(1) O(1) and In(2) O(1)),
3 3 3
3 3 3
which interestingly, because of geometric constraints, only
occurred in the two lowest transition structures, (R)-TS1
and (S)-TS2. A second notable feature of these two transi-
tion structures is that the In(1)-metal center resides within
the plane of the 5-membered ring system containing the
N- and O-atoms of the ligand, while the In(2)-metal center
resides below the plane of this same 5-membered ring
system and trans to the bulky phenyl substituents of the
ligand. Geometrically, this in-plane/below the plane rela-
tionship of the two In-metals with respect to the sterically
bulky vicinal phenyl groups of the ligand component in
(R)-TS1 and (S)-TS2 shields the top face of these struc-
tures, forcing allylation to take place on the bottom face in
a synclinal manner via a chairlike transition state.
(8) (a) Asami, M.; Mukaiyama, T. Chem. Lett. 1980, 17–20. (b) Meyers,
A. I.; Hanagan, M. A.; Trefonas, L. M.; Baker, R. J. Tetrahedron 1983,
39, 1991–1999. (c) Ohkuma, T.; Kitamura, M.; Noyori, R. Tetrahedron Lett.
1990, 31, 5509–5512. (d) Watanabe, M.; Hashimoto, N.; Araki, S.; Butsugan,
Y. J. Org. Chem. 1992, 57, 742–744. (e) Zhang, H.; Zhang, S.; Liu, L.; Luo,
G.; Duan, W.; Wang, W. J. Org. Chem. 2010, 75, 368–374. (f) Phan, D. H. T.;
Kim, B.;Dong, V. M.J. Am. Chem. Soc. 2009, 131, 15608–15609. (g) Huang,
X.; Pan, X.; Lee, G.; Chen, C. Adv. Synth. Catal. 2011, 353, 1949–1954.
(9) Mirabdolbaghi, R.; Dudding, T. Tetrahedron 2012, 68, 1988–
1991.
Importantly, these structural differences reduce the ac-
tivation barrier for Re-stereofacial addition by 2.15 kcal/
mol with respect to the Si-stereofacial mode of addi-
tion (ΔGq = 4.13 (Re-addition, (R)-TS1) vs 6.28 kcal/mol
(Si-addition, (S)-TS1), which translates to 98% en-
antioselectivity, agreeing well with experiment (see the
Supporting Information for additional details). The spe-
cific origin of this enantiofacial selectivity appears to result
(10) Yus, M.; Gonzalez-Gomez, J. C.; Foubelo, F. Chem. Rev. 2011,
111, 7774–7854.
(11) (a) Haddad, T. D.; Hirayama, L. C.; Singaram, B. J. Org. Chem.
2010, 75, 642–649. (b) Hrdina, R.; Valterova, I.; Hodacova, J.; Cisarova,
I.; Kotora, M. Adv. Synth. Catal. 2007, 349, 822–826.
(12) Knepper, K.; Ziegert, R. E.; Brase, S. Tetrahedron 2004,
60, 8591–8603.
B
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