C O M M U N I C A T I O N S
Scheme 2
bended molecules with inherent helical chirality. Moreover, we
demonstrated that the introduction of elements of central chirality
in the design allowed preparation and optical separation of the
helical stereoisomers but contributed little to their chiroptical
properties. Chemical stability as well as the rigid and stable ridge-
tile-like structure of these helical molecules was also demonstrated.
Taking into account these structural features, one can expect that
these novel type of helical molecules might be useful structural
elements in macromolecular design or can be used as chiral
nanoscale building blocks in the field of chiral nanotechnology.
Scheme 3
Acknowledgment. The authors are thankful to Dr Takada
(JASCO corp.) for the CD spectra. This work was supported by
the Department of Chemistry and Biochemistry, University of
Oklahoma. The authors gratefully acknowledge generous financial
support from Central Glass Company (Tokyo, Japan) and Ajino-
moto Company (Tokyo, Japan).
132.25(8)° (a), 137.21(15)° (b), and 130.83(8)° (c), respectively.
The deviation of the bridging imine nitrogens was ranging from
0.322 to 0.882 Å and the Ni,Ni distances were 2.6427(4) (a),
2.6952(9) (b), 2.6156(3) Å (c).
Supporting Information Available: Experimental procedures,
characterizations of new compounds, and crystallographic data. This
Finally to prepare this new type of helical molecules in
enantiomerically pure form and taking advantage of the modular
nature of our design, we synthesized chiral complex 8 and subjected
it to the standard dimerization procedure. The application of chiral
complex 8 resulted in formation of two diastereomers (M,S,S)-9
and (P,S,S)-9, isolated in quantitative yield and in a ratio of 21:79,
respectively (Scheme 3). The diastereomers (P,S,S)-9 and (M,S,S)-9
were easily separated by regular column chromatography on silica
gel and fully characterized including X-ray crystallographic studies.
As it follows from the structure of the diastereomer (M,S,S)-9, the
corresponding N-benzyl groups are in close proximity to each other
rendering (M,S,S)-9 relatively unstable as compared to major
diastereomer (P,S,S)-9 in which the N-benzyl groups point away
from each other. This different mode of stereochemical interactions
in the diastereomers (P,S,S)-9 and (M,S,S)-9 is probably responsible
for some geometric differences between them. Thus, both diaster-
eomers exhibited significant folded, ridge-tile structures, however
the torsion angles θ between two square planar faces were 132.80-
(8)° for (P,S,S)-9 and 136.02(7)°, slightly larger, for (M,S,S)-9.
Moreover, as a result of different torsion angles θ, short Ni-Ni
distances were found to be also different, measuring 2.6341(3) Å
for (P,S,S)-9 and 2.6813(4) Å for (M,S,S)-9. Examination of the
chiroptical properties, such as CD spectra and optical rotation,
revealed that diastereomers (P,S,S)-9 and (M,S,S)-9 behave rather
as helical pseudo-enantiomers. Thus, extraordinary large [R]D values
of -1022 for (M,S,S)-9 and +1222 for (P,S,S)-9 as well as strong
and opposite Cotton effects in the CD spectra indicated that helical
chirality virtually completely overwhelmed the two stereogenic
centers in the compounds (P,S,S)-9 and (M,S,S)-9.16
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Finally, to demonstrate thermal stability of these ridge-tile
1
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toluene. Thus, heating compound 7a gradually from ambient
temperature to 100 °C did not result in any changes or broadening
of peaks, indicating the absence of any transformations.
In summary, we report the first example of design and synthesis
of helical molecules using ridge-tile-like topological mode of
nonplanarity. The modular nature of the design of starting glycine
derivatives renders this approach general for the preparation of
structurally varied and functionalized derivatives of this type of
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(16) See the Supporting Information.
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