Induction of Point Chirality by E/Z Photoisomerization
Induction of Point Chirality by E/Z Photoisomerization
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DOI:
10.1002/anie.201104614
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发表时间:
2011-01-01
影响因子:
16.6
通讯作者:
Tamaoki, Nobuyuki
中科院分区:
文献类型:
--
作者:
Hashim, P. K.;Tamaoki, Nobuyuki
Point chirality originates from having four different substituents bonded to a central atom to give nonplanar molecules with nonsuperimposable mirror images.[1] The induction of point chirality in molecular systems is of particular interest in connection with the origin of homochirality in nature, as seen in amino acids.[2–4] Our interest is to propose a new concept for the introduction of point chirality and also to understand how small differences in the substituents on the central carbon atom can cause detectable asymmetry in the structure. Previous work has shown that a small difference in the substituents such as position isomerism of pyridyl groups [5] or the presence of different isotopes [6] can cause detectable asymmetry in a molecule. However, chemical bonds need to be broken and made to make even such small differences in the substituents; this observation inspired us to envisage a molecular system in which the asymmetry can be introduced by photoisomerization of the substituents without any bond cleavage.Herein, a new class of azobenzene-based prochiral molecules and the on/off switching of point chirality is reported. We designed a molecule consisting of a carbon atom having two photoisomerizable azobenzene moieties and a methyl and a benzene group (Scheme 1). The conformational difference caused by the E/Z photoisomerization of one of the azobenzene moieties was successfully utilized for the generation of point chirality in the molecule. To the best of our knowledge this is the first example of the induction of point chirality in which two of the substituents around an sp3 carbon atom are geometric isomers. A solution of 1 in ethyl acetate exhibits a typical absorption spectrum for azobenzene derivatives; this spectrum features an intense π–π* transition band at 327 nm and a weak and broad n–π* transition band at 400–500nm. Irradiation of the solution at 366nm caused a gradual decrease in the intensity of the π–π* transition band, with a notable increase in the n–π* transition band owing to photochemical E/Z isomerization of the azobenzene moieties. The reverse spectral changes were observed upon irradiation at 436 nm. The solutions at the photostationary state (PSS) under 366 and 436nm light showed about 15 and 80%,