evidence for the gel structure. Formation of only h–h photo-
dimers from the gel state definitely indicates that 2Ac
molecules are placed only in a h–h fashion (Fig. S7z). The
arrangement is so compact and directional that the non-
covalent interaction becomes enough to transfer the chirality
to the ground state packing of 2Ac molecules and this
preorientation in the ground state actually determines the ee
of the photoproducts. On the other hand, a photo-induced
structural change (gel to sol transition) that is fairly difficult in
the gel system can easily be attained in the present system.
Attachment of 2Ac molecules in the binary gelator via
hydrogen-bonding is evident from FT-IR spectra of the
xerogel (Fig. S8z) where the CQO stretching frequency
(at 1682 cmꢂ1) of 2Ac shifts to lower energy in the gel state.
In addition, unlike the previously reported system,11e the
ammonium counterpart is capable of forming intermolecular
hydrogen-bonding (via two amide groups) to align itself in the
gel structure, even though this does not seem to be enough
to resist the structural change during the photoreaction.
This situation means that 2Ac molecules definitely have an
active participation in constructing the gel structure via their
p–p stacking interaction which is more favourable in a h–h
orientation. The p–p stacking together with the intermolecular
hydrogen-bonding via two amide linkages cooperatively
construct the one-dimensional arrangement of the gelator
molecules (Fig. S7z) which is facilitated by the nonpolar
environment of the cyclohexane.
Notes and references
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A.D. warmly thanks Mr T. Kitahara, Mr T. Hara and
Mr H. Sato for their kind help in different stages of experi-
ment. Financial support was provided by Grants-in-Aid
(Nos. 19022031, 20045014, and 20685010) and the Global
COE program ‘Science for future molecular systems’ from
MEXT of Japan and a JSPS fellowship for A.D.
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2102 | Chem. Commun., 2009, 2100–2102