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References and Notes
tional period, which is on the order of picoseconds.
Es between high- and low-chalcocite phases re-
sults from the different Cu arrangements in these
two phases and the related extra Ewald energy at
the interface. This is similar to the case of the inter-
face between wurtzite (WZ) and zincblende (ZB),
where the different second nearest-neighbor atomic
positions cause different Ewald energies in these
two phases. It has been found that the interface
energy between WZ and ZB per surface unit cell
is similar to the energy difference per unit cell
(28). Thus, if we take this approximation that the
interface energy between low- and high-chalcocite
is the same as the internal energy difference be-
tween these two phases, (e1 – e2) = 40 meV per
unit cell (23), and assume that there are N Cu2S
unit formulae inside a spherical core, we have Es =
(36p)1/3N2/3(e1 – e2). Note that C = Cunit N, and
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Acknowledgments: We thank U. Dahmen at National Center
for Electron Microscopy (NCEM) and E. Borrero and
C. Dellago at University of Vienna for helpful discussions.
The authors are grateful to the support of Helios Solar
Energy Research Center (SERC) and NCEM, which are
funded by the director of the Office of Science, Office of
Basic Energy Sciences (BES), Materials Science and
Engineering Division of the U.S. Department of Energy
(DOE) under contract no. DE-AC02-05CH11231. TEM
experiments were performed using TEAM0.5 microscope
at NCEM. X-ray experiments were performed at the
Stanford Synchrotron Radiation Laboratory, a DOE-BES
user facility. J.B.R. was funded by a fellowship from Intel
Corporation, and T.A.M. and A.L. were supported by the
DOE BES Materials Sciences and Engineering Division.
H.Z. conceived the work and performed the experiments;
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J.B.R. prepared nanorod samples, took ensemble x-ray
data, and edited the paper; B.S. contributed to nanorod
sample preparation and edited the paper; M.F.T., A.L.,
and T.A.M. provided x-ray analysis infrastructure; L.-W.W.
provided theoretical calculation and edited the paper; and
C.K. contributed to image analysis and edited the paper.
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Cunit = 52 J/mol·K (23). Thus, from Eq. 3, we get
t ~ 2 s when N = 1000 and t0 = 1 ps (29). This
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In summary, we have observed dynamic struc-
tural transformations of a single Cu2S nanorod
from a low- to a high-chalcocite structure. The
influence of the surface and interface energies
on nucleation and pinning phenomena of a par-
ticular phase by defects suggests strategies for
stabilizing metastable structures. The ability to
directly visualize these processes will aid in the
future design of materials with new and con-
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Supporting Online Material
Materials and Methods
SOM Text
Figs. S1 to S4
Table S1
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Movies S1 to S6
23 February 2011; accepted 25 May 2011
10.1126/science.1204713
two-step arene C–H borylation/oxidation pro-
cedure for the introduction of a hydroxyl group
into an aromatic ring, guided by steric rather
than electronic effects (2). Recent advances in
palladium-catalyzed aerobic oxidation reactions
(3–5) suggested to us that diverse phenol deriv-
atives, including those with meta substitution,
could be accessed by dehydrogenation of cyclo-
hexanones via sequential Pd-mediated C–H
activation/b-hydride elimination steps, followed by
tautomerization of the resulting dienone product
(Fig. 1A). This strategy is appealing because
PdII–hydride intermediates formed in this mech-
anism could be oxidized by molecular oxygen
(6, 7), thereby enabling the overall process to be
catalytic in Pd with water as the sole by-product
(Fig. 1B). Successful catalysts for this class of
reactions could find broad utility owing to the nu-
merous straightforward chemical reactions that
provide access to substituted cyclohexanones, in-
cluding enolate arylation and alkylation meth-
Palladium-Catalyzed Aerobic
Dehydrogenation of Substituted
Cyclohexanones to Phenols
Yusuke Izawa, Doris Pun, Shannon S. Stahl*
Aromatic molecules are key constituents of many pharmaceuticals, electronic materials, and
commodity plastics. The utility of these molecules directly reflects the identity and pattern of
substituents on the aromatic ring. Here, we report a palladium(II) catalyst system, incorporating an
unconventional ortho-dimethylaminopyridine ligand, for the conversion of substituted
cyclohexanones to the corresponding phenols. The reaction proceeds via successive
dehydrogenation of two saturated carbon-carbon bonds of the six-membered ring and uses
molecular oxygen as the hydrogen acceptor. This reactivity demonstrates a versatile and
efficient strategy for the synthesis of substituted aromatic molecules with fundamentally
different selectivity constraints from the numerous known synthetic methods that rely on
substitution of a preexisting aromatic ring.
henols are common precursors and core resents a key challenge in the preparation of these ods, conjugate addition to cyclohexenones, and
structures of industrial chemicals rang- molecules (1). Electrophilic aromatic substitutions Robinson annulation and Diels-Alder reactions
ing from pharmaceuticals to polymers. The are classical chemical reactions that remain among (Fig. 1C).
P
introduction of chemical functional groups with the most versatile methods for the synthesis of
The preparation of phenols from ketone pre-
specific patterns around the aromatic ring rep- substituted phenols; however, strong electronic cursors have been explored previously (8–16).
directing effects associated with these reactions Condensation reactions of acyclic ketones, for
limit their utility to the preparation of ortho- and example, with b-ketoaldehydes or b-diketones,
Department of Chemistry, University of Wisconsin–Madison,
para-substituted derivatives. This limitation has enable direct access to substituted phenols (8),
inspired extensive efforts to identify complemen- but low product yields, limited access to starting
tary routes to substituted phenols, such as a recent materials, and/or formation of isomeric products
1101 University Avenue, Madison, WI 53706, USA.
*To whom correspondence should be addressed. E-mail:
209