Journal of the American Chemical Society
Communication
properties of guests via cage-driven conformational twisting.
Even better, the resulting conformation of the guest is easily
predicted from the cavity shape.
ASSOCIATED CONTENT
* Supporting Information
■
S
Experimental procedures, physical properties, and crystallo-
graphic data (CIF). This material is available free of charge via
AUTHOR INFORMATION
Corresponding Author
■
Notes
The authors declare no competing financial interest.
ACKNOWLEDGMENTS
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This research was supported by the CREST Project of the
Japan Science and Technology Agency (JST) and also in part
by the Global COE Program “Chemistry Innovation through
Cooperation of Science and Engineering” from MEXT, Japan.
REFERENCES
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(1) Overcrowded alkenes have been studied for over a century since
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Figure 5. (a) Schematic representation of the bromination of t-1a
within cage 2. (b) H NMR spectrum (300 K, 500 MHz, CDCl3) of
compound t-4 obtained after purification. (c) X-ray crystal structure of
t-4: (left) ORTEP drawing (ellipsoids at the 50% probability level);
(right) space-filling model (C, purple; H, white; O, red; Br, orange).
Solvents have been omitted for clarity.
1
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solid. The twisted structure of t-4 was clearly confirmed by X-
ray crystallographic analysis (Figure 5c). Because of steric
hindrance by the bromine substituents at the 1-, 3-, 6-, and 8-
positions, isomerization into the anti-folded conformer is no
longer possible. In fact, the deep-blue color of t-4 remained
unchanged even after heating at 100 °C for 2 h. These results
show that af-1a was converted to highly twisted alkene t-4 by
bromination within cage 2. The twist angle around the central
double bond in t-4 (53.3°)12 was significantly larger than that in
parent compound t-1b (42.3°).6b This means that the overlap
of the olefin p orbitals is poorer, resulting in elongation of the
double bond in t-4 [1.416(5) Å for t-4 compared with 1.401(6)
Å for t-1b].6b
The chromism between the two conformers of 1a is ascribed
to a change in the HOMO−LUMO gap of the molecule, which
depends on the overlap of the alkene p orbitals.6b Though
significantly distorted, the two p orbitals of the anti-folded
conformer are in the same plane. Thus, the HOMO−LUMO
gap is relatively large, and absorption occurs in shorter-
wavelength regions. When 1a is twisted, the orbital overlap in
the central double bond is reduced, and the HOMO−LUMO
gap is narrowed, bringing the absorption into the visible region.
In summary, we have succeeded in noncovalently twisting
the overcrowded alkene af-1a within self-assembled Td-
symmetric cage 2. A dramatic color change was observed as a
consequence of conformational switching by encapsulation.
Furthermore, the twisted conformation of the guest can be
either temporarily or permanently trapped. These observations
are applicable not only to molecular sensing and information
storage but also more generally to the control of physical
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