C O M M U N I C A T I O N S
L-enantiomer, negative (Figure 2a). The absence of any detectable
signal for the E-rotaxane shows that the CD signal is genuinely
only generated by controlling the position of the macrocycle in the
shuttle.
The most efficient ways of interconverting the rotaxane diaster-
eomers are photochemical: 350 nm, catalytic benzophenone
sensitizer, CH2Cl2, 70% for E-1fZ-1 and 400-670 nm, catalytic
Br2, CH2Cl2, >95% for Z-1fE-1 (Scheme 1). However, a modest
difference in the electronic absorption spectra of E-1 and Z-1 (Figure
2b) results in different photostationary states for the isomers at 254
(56% Z-1 in CH2Cl2; 49% Z-1 in CH3CN) and 312 nm (38% Z-1
in either CH2Cl2 or CH3CN), meaning that even for this first-
generation system a large net change (>1500 deg cm2 dmol-1) in
elliptical polarization can be achieved solely through irradiation
with light of different wavelengths. The photoisomerizations are
highly reproducible with five complete switching cycles (E-1fZ-
1fE-1) carried out with no decomposition detectable by NMR or
CD spectroscopy (Figure 2c).
In conclusion, we have demonstrated a system where a large
amplitude displacement of a macrocycle along a thread elicits a
chiral optical response. In addition to this being a novel mode of
switching to be explored for possible photonic and data storage
applications, control of the expression of chirality in switchable
interlocked systems through hiding or revealing chiral subunits
could find important applications in areas where chiral transmission
from one chemical entity to another underpins a physical or
chemical response, such as the seeding of supertwisted nematic
liquid crystalline phases or asymmetric synthesis.
Acknowledgment. This work was supported by the European
Union Future and Emerging Technology Program MechMol and
the EPSRC. D.A.L. is an EPSRC Advanced Research Fellow
(AF/982324).
Figure 2. (a) CD spectra (0.1 mM in CHCl3) at 298 K of Z-1 (blue), E-1
(purple), E-2 (green), and Z-2 (red). (b) UV-vis spectra of E-1 (purple)
and Z-1 (blue) in CHCl3 at 298 K, [ꢀ] ) mM-1‚cm-1. Dotted line represents
the Z-1/E-1 absorption ratio. (c) Percentage of E-1 in the photostationary
state (from 1H NMR data, 400 MHz, CD3CN, 298 K) after alternating
irradiation at 254 nm (half integers) and 312 nm (integers) for five complete
cycles. The right-hand Y axis shows the CD absorption at 246 nm.
Supporting Information Available: Experimental procedures and
spectral data for all new compounds (PDF). This material is available
References
E-rotaxane and thread (Figure 1, a and b) shows the excellent
discrimination of the macrocycle toward the different stations. While
the Gly-Leu protons are only slightly affected by the aromatic
shielding effect of the macrocycle, the E-olefin protons are
significantly shifted upfield (∼1.2 ppm), confirming that the co-
conformer having the macrocycle over the olefin station is the major
translational isomer in E-1.
Light-induced EfZ isomerization7 of the fumaramide unit
reverses8 the macrocycle-binding affinity of the two stations in the
molecular shuttle because the cis-olefin (maleamide) is largely self-
satisfying in terms of H-bonding and the amide carbonyl groups
are no longer suitably orientated for binding to the macrocycle.7
The 1H NMR spectra of Z-1 and Z-2 (Figure 1, c and d) reveal the
concomitant change in the position of the macrocycle. The Z-olefin
protons Hd′ and He′ occur at almost identical chemical shifts in
rotaxane and thread, whereas the Gly methylene protons are now
shielded by 0.9 ppm.
(1) (a) Sauvage, J.-P., Dietrich-Buchecker, C., Eds.; Molecular Catenanes,
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The shuttle design works remarkably well. When the macrocycle
is tightly bound close to the Leu residue in Z-1, the aromatic rings
of the rotaxane do, indeed, experience a well-expressed chiral
environment as evidenced by CD spectroscopy. Of the two
rotaxanes and two threads, only rotaxane Z-1 gives a CD response,
which is both strong (-13k deg cm2 dmol-1) and, for the
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