Enantiomerically Pure trans-ꢀ-Lactams from R-Amino Acids
A R T I C L E S
Scheme 4. Synthesis and Reaction of R-Diazo-ꢀ-ketoamide 11
Figure 2. Solid-phase structure of diazoketone 14.
pounds are, in general, thermally unstable. Accordingly, on a
1 g scale, the reaction was complete in 3.5 h (vs 0.6 g, 7 h for
the batch process) and afforded an 81% isolated yield of a
roughly 3:1 separable mixture of 12 and 13, respectively. The
improved reaction time and ease of processing material on a
larger scale made the modified continuous-flow photochemical
process the preferred method, despite slightly diminished
yields.31
Nonetheless, the use of the MVL was not without concern
regarding heat and UV radiation for the experimentalist, and
we were drawn to consider alternative light sources by the
photochemist’s adage that the wavelength choice should be “as
long as possible and as short as necessary”. Therefore, a 100
W CFL (Figure S2 in the Supporting Information), which
promised far greater safety and distinctly lower cost than the
conventional light source, was investigated. To our knowledge,
there are no previous reports of CFL use for the photochemical
Wolff rearrangement, but we were delighted to find that while
the rate of the reaction was diminished relative to that for the
MVL, the product yield was increased and the distributions were
comparable in both the batch and continuous-flow modes
(Scheme 4). In addition, the CFL-promoted reaction required
no external cooling.
What is the origin of the facile Wolff rearrangement of
R-diazo-ꢀ-ketoamide 11? Optimized yields arise from photo-
chemical decomposition as opposed to the use of metal catalysts
and point to a very facile rearrangement reaction. Recent studies
of the Wolff rearrangement32 have suggested that ketene can
form from two different reaction pathways: an extremely rapid
rearrangement of the diazo excited state concomitant with
nitrogen loss and a slower rearrangement from the ketocarbene
after nitrogen loss. The rearrangement is facilitated by the
antiperiplanar geometry of the leaving and migrating groups
(N2 and the amino acid chiral center, respectively), and it is
this geometry that was found in the single-crystal X-ray study
of diazoketone 14 (Figure 2 and the Supporting Information),
which is derived from aspartic acid (see below). The structure
shows the molecule in the s-ZK,s-EW conformation (K for ketone,
W for Weinreb amide), with the dihedral angle defined by
N2-C-CCdO-CR (all marked with *) having a value of 172.6°.
Thus, the solid-state structure possesses the exact conformation
necessary for efficient Wolff rearrangement.
diazabicyclo[5.4.0]undec-7-ene (DBU) gave compound 7 in an
overall 80% yield for the two steps. Under standard photo-
chemical conditions, compound 7 afforded a 63% yield of a
separable mixture of the desired trans-ꢀ-lactam 8 and alkene
9. The structure of ꢀ-lactam 8 was confirmed by X-ray
crystallography; alkene 9 was assigned by 2D NMR analysis.
While the mechanistic pathway for the alkene product is not
entirely clear, the new amide functionality clearly suggests that
9 originates from Wolff rearrangement/ꢀ-lactam cascade fol-
lowed by further reaction.26
The modest yield of ꢀ-lactam 8 prompted the search for a
C3 amide functionality that would maintain or exceed the higher
product yields encountered in our initial studies while offering
facile functional group manipulation. After some consideration,
the N-methoxy-N-methyl (Weinreb) amide was chosen for study,
as Weinreb amides27 hold a reserved place as valuable and
versatile synthetic intermediates.28
Weinreb ꢀ-ketoamide 10 was prepared by a modified
literature procedure (Scheme 4).29 Accordingly, serine imida-
zolide 1 was acylated with the lithium enolate (LHMDS) of
N-methoxy-N-methylacetamide to give the desired ꢀ-ketoamide
10 in 86% yield on a 9 g scale. Treatment with diazo transfer
reagent gave the desired R-diazo-ꢀ-ketoamide 11 in 89% yield.
Under standard photolysis conditions, diazo 11 was irradiated
with a medium-pressure mercury vapor lamp (MVL), which
afforded an easily separable, roughly 2.5:1 mixture of ꢀ-lactams
12 and 13, respectively, in 90% isolated yield. The identities
of the two ꢀ-lactam isomers were confirmed by X-ray crystal-
lography. To improve upon our processing capabilities, a simple
continuous-flow photochemical reactor was constructed from
common laboratory equipment30 and consisted of the requisite
tubing and a medium-pressure liquid chromatography pump in
addition to standard flasks (see Figure S1 in the Supporting
Information). External cooling was employed, as diazo com-
To more fully understand the preferred solution conformation
of the diazo substrates, hybrid density functional theory calcula-
tions on compound 14 were employed. The calculations were
performed with no explicit solvent incorporation, since the
dielectric constant of toluene is very low (D ) 2.38). The crystal
structure coordinates of compound 14 were used as the starting
point, and four conformations were generated by setting the
dihedral angles related to the ꢀ-dicarbonyl system to either 180
(26) For alkene formation accompanying Wolff rearrangement, see: Stork,
G.; Szajewski, R. P. J. Am. Chem. Soc. 1974, 96, 5787–5791.
(27) Nahm, S.; Weinreb, S. M. Tetrahedron Lett. 1981, 22, 3815–3818.
(28) For a recent review, see: Balasubramaniam, S.; Aidhen, I. S. Synthesis
2008, 3707–3738.
(29) Kulesza, A.; Ebetino, F. H.; Mazur, A. W. Tetrahedron Lett. 2003,
44, 5511–5514.
(30) (a) For a recent review, see: Wiles, C.; Watts, P. Eur. J. Org. Chem.
2008, 1655–1671. (b) Lainchbury, M. D.; Medley, M. I.; Taylor, P. M.;
Hirst, P.; Dohle, W.; Booker-Milburn, K. I. J. Org. Chem. 2008, 73,
6497–6505. (c) Hook, B. D. A.; Dohle, W.; Hirst, P. R.; Pickworth,
M.; Berry, M. B.; Booker-Milburn, K. I. J. Org. Chem. 2005, 70,
7558–7564.
(31) See the Supporting Information for experimental details and Figure
S1 for a picture of the continuous-flow photochemical reactor.
(32) Burdzinski, G. T.; Wang, J.; Gustafson, T. L.; Platz, M. S. J. Am.
Chem. Soc. 2008, 130, 3746–3747.
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J. AM. CHEM. SOC. VOL. 132, NO. 32, 2010 11381