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´ ´ ´
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´
lez,
´
´
´
9 Enantioselective metalation: M. P. Webster and V. K. Aggarwal,
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Co, Weinheim, 2011, vol. 2, p. 479.
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11 See also: M. Rubina, M. Rubin and V. Gevorgyan, J. Am. Chem.
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12 The chirality of tmdBH was shown to be inconsequential, see
ref. 10.
Fig. 3 Relative energies of model octahedral intermediates leading to
g- and b-borylation for 1,1- and (E) 1,2-disubstituted substrates (A/B
and C/D, respectively; only the vinyl C–H and Rh–H included for clarity.
with favored formation of the g-borylated product upon alkene
insertion into the Rh–H bond (i.e., A); the lowest energy structure
leading to b-borylation (i.e., B) is calculated to be about 1.9 kcal
higher in energy and arises from complexation to the opposite
face of the p-system. Structures C and D model a simple
1,2-disubstituted alkene with the (E)-geometry (i.e., a model
for amide 1). Consistent with the experimental observations,
the b-leading isomer D is favored for this substitution pattern.
In contrast to tri- and other disubstitution patterns, CAHBs
of b,g-unsaturated methylidene amides and esters afford the
g-borylated product and proceed in the opposite sense of asym-
metric induction. Chiral g-borylated derivatives are intermediates
for inter- and intramolecular cross-couplings, the formation of
chiral g-hydroxy carbonyl derivatives, and b-substituted-g-lactones.
Preliminary computational studies suggest that the preferred
conformation of the chelated substrate relative to the Rh–H
bond may explain the observed regio- and p-facial selectivity.
Further studies are in progress.
13 R. Corbera
Ed., 2011, 50, 7079; C. Mazet and D. Ge
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J. Martinez, J. R. Medina, K. Matos and J. A. Soderquist,
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G. A. Molander, J. Am. Chem. Soc., 2010, 132, 17108; T. Awano,
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Financial support from the NSF (CHE-0809637) and NIH
(GM100101) is gratefully acknowledged. We thank D. Boadwine
for optimizing the reactions leading to 22.
20 J. W. Bode, M. P. Doyle, M. N. Protopopova and W.-L. Zhou,
J. Org. Chem., 1996, 61, 9146.
Notes and references
21 Computational studies were performed using density functional
theory (DFT) implemented in the ab initio package Gaussian09.
B3LYP functional along with 6-31+G(d,p) (all non-metal atoms)
and LANL2DZ (Rh) basis sets was employed. Frequency calcula-
tions were performed at the same level of theory for each of the
optimized structures to check for the absence of any imaginary
frequencies. See ESIw for more details.
1 (a) H. K. Scott and V. K. Aggarwal, Chem.–Eur. J., 2011,
17, 13124; (b) C. M. Crudden, B. W. Glasspoole and C. J. Lata,
Chem. Commun., 2009, 6704.
2 Catalytic asymmetric diboration of dienes and alkenes: L. T. Kliman,
S. N. Mlynarski, G. E. Ferris and J. P. Morken, Angew. Chem., Int.
Ed., 2012, 51, 521; C. H. Schuster, B. Li and J. P. Morken, Angew.
Chem., Int. Ed., 2011, 50, 7906; K. Hong and J. P. Morken, J. Org.
c
12182 Chem. Commun., 2012, 48, 12180–12182
This journal is The Royal Society of Chemistry 2012