RESEARCH
| REPORTS
also observed at temperatures <100°C. The opti-
mal temperature proved to be 150°C.
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We also observed that the reaction rate in-
creased with increasing ethylene pressure. To de-
termine the TOF, we measured TO after 4 hours
of reaction. Figure 4 shows a plot of TOF versus
ethylene pressure. A linear correlation is observed.
Thus, the reaction rate appears to have a first-
order dependence on ethylene concentration. This
is in contrast to previously reported Pt(II) and
Ru(II) catalysts for the hydrophenylation of eth-
ylene, which show an inverse dependence on
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6
2
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2
CH
2
Ph)(h -C
2 4
H ) complexes were
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in the catalyst resting state.
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1
ACKNOWLEDGMENTS
2
The authors acknowledge support from the U.S. Department of
Energy, Office of Basic Energy Sciences [DE-SC0000776 (T.B.G.)
and DE-FG02-03ER15387 (T.R.C.)] for studies of styrene catalysis;
the Center for Catalytic Hydrocarbon Functionalization, an Energy
Frontier Research Center (award DE-SC0001298), which funded
the initial catalyst discovery; and an AES Corporation Graduate
Fellowship in Energy Research (M.S.W.-G). The authors also thank
B. McKeown, G. Fortman, S. Kalman (University of Virginia), and
R. Nielsen (California Institute of Technology) for helpful discussions.
2
2. A. T. Luedtke, K. I. Goldberg, Angew. Chem. Int. Ed. 47,
694–7696 (2008).
6 6 6 6 H D
of C H and C D . After 1 hour, a k /k (ratio of
7
rate of reaction of protio-benzene and perdeutero-
benzene) of 3.1(2) was determined by exam-
ining the ratio of undeuterated styrene [mass/
2
3. T. Matsumoto, D. J. Taube, R. A. Periana, H. Taube, H. Yoshida,
J. Am. Chem. Soc. 122, 7414–7415 (2000).
24. T. Matsumoto, R. A. Periana, D. J. Taube, H. Yoshida,
J. Mol. Catal. A 180, 1–18 (2002).
5
charge ratio (m/z) = 104] to styrene-d (m/z = 109)
2
5. J. Oxgaard, R. P. Muller, W. A. Goddard 3rd, R. A. Periana,
in the mass spectra from three independent ex-
periments (fig. S5). After 2 hours, the observed
isotope effect was 3.0(2), statistically equivalent
to the data at 1 hour (fig. S5). Thus, the observed
J. Am. Chem. Soc. 126, 352–363 (2004).
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Organometallics 27, 4031–4033 (2008).
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30. D. Taube, R. Periana, T. Matsumoto, “Oxidative coupling
of olefins and aromatics using a rhodium catalyst and a
copper(II) redox agent” (U.S. Patent 6127590A, 2000).
SUPPLEMENTARY MATERIALS
www.sciencemag.org/content/348/6233/421/suppl/DC1
Materials and Methods
Figs. S1 to S4
Table S1
References (41–43)
2
2
2
H D
k /k of ~3.1 likely reflects a kinetic isotope ef-
fect (KIE) for the catalytic cycle. The KIE is con-
sistent with other transition metal–mediated C–H
activation reactions. (39, 40) The primary KIE
supports the hypothesis that a Rh catalyst is
facilitating a metal-mediated C–H activation
process, which occurs before or during the turnover-
limiting step. No change in the isotopic distribu-
tion for benzene was observed over the course
of the reaction, and no styrene-d6-8 products were
observed except those predicted by the natural
abundance of deuterium in ethylene.
3 November 2014; accepted 12 March 2015
10.1126/science.aaa2260
SELF-ASSEMBLY
Selective assemblies of giant
Although more detailed studies are required tetrahedra via precisely controlled
to understand the reactivity profile of 1, we be-
lieve that the highly electron-withdrawing per-
positional interactions
Fl
fluorophenyl groups on the DAB ligand help
suppress irreversible oxidation to inactive Rh(III)
1
1
1
1
1
1
Mingjun Huang, Chih-Hao Hsu, Jing Wang, Shan Mei, Xuehui Dong, Yiwen Li,
in the presence of Cu(II), possibly facilitate asso-
ciative ligand exchange between free ethylene
and coordinated styrene, and facilitate rapid eth-
ylene insertion into Rh–Ph bonds. Challenges
that remain for the continued development of
this class of catalyst include increasing activity
with the aim of achieving higher conversions
of benzene.
1
1
1
2
3
Mingxuan Li, Hao Liu, Wei Zhang, Takuzo Aida, Wen-Bin Zhang, *
1
1
Kan Yue, * Stephen Z. D. Cheng *
Self-assembly of rigid building blocks with explicit shape and symmetry is substantially
influenced by the geometric factors and remains largely unexplored. We report the selective
assembly behaviors of a class of precisely defined, nanosized giant tetrahedra constructed by
placing different polyhedral oligomeric silsesquioxane (POSS) molecular nanoparticles at the
vertices of a rigid tetrahedral framework. Designed symmetry breaking of these giant
tetrahedra introduces precise positional interactions and results in diverse selectively
assembled, highly ordered supramolecular lattices including a Frank-Kasper A15 phase, which
resembles the essential structural features of certain metal alloys but at a larger length scale.
These results demonstrate the power of persistent molecular geometry with balanced
enthalpy and entropy in creating thermodynamically stable supramolecular lattices with
properties distinct from those of other self-assembling soft materials.
REFERENCES AND NOTES
1.
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elf-assembled hierarchical structures in
soft materials have been intensely studied.
Among them, assemblies of building blocks
with specific geometric shapes and sym-
metry are of particular interest. As the sim-
plest case, ordered structures constructed from
packing of spherical motifs have been a classic yet
dynamic research field that can be traced back to
the study of metals and metal alloys. Most metal
atoms, viewed as congruent spheres, typically tend
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6.
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dehydrogenation of alkyl-aromatic hydrocarbons for the
S
4
24 24 APRIL 2015 • VOL 348 ISSUE 6233
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