TY - JOUR
T1 - Internal-Edge-Substituted Coumarin-Fused [6]Helicenes
T2 - Asymmetric Synthesis, Structural Features, and Control of Self-Assembly
AU - Usui, Kazuteru
AU - Yamamoto, Kosuke
AU - Ueno, Yuhei
AU - Igawa, Kazunobu
AU - Hagihara, Ryusuke
AU - Masuda, Toshinobu
AU - Ojida, Akio
AU - Karasawa, Satoru
AU - Tomooka, Katsuhiko
AU - Hirai, Go
AU - Suemune, Hiroshi
N1 - Publisher Copyright:
© 2018 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
PY - 2018/10/1
Y1 - 2018/10/1
N2 - π-Conjugated helicenes containing heteroatoms have attracted significant attention due to their diverse chemical and electronic structures, as well as tunable physical properties. It was rationally anticipated that the self-assembly of coumarin-fused helicenes would be controlled by the effects of a substituent on the internal edge of the helix. Here, this work reports the efficient syntheses of coumarin-fused helicenes 1 a,b (R=Ph, Me), and the enantioselective synthesis of 1 a (R=Ph) by chiral AuI-catalyzed hydroarylation. The helical structure of 1 was unambiguously determined by X-ray crystallography. Of particular note, the enantiomerically pure crystal of 1 a adopted a one-dimensional columnar structure based on π–π stacking interactions, as expected. Furthermore, a significant difference between the fluorescence quantum yields of the enantiomerically pure form and racemate of 1 a was observed.
AB - π-Conjugated helicenes containing heteroatoms have attracted significant attention due to their diverse chemical and electronic structures, as well as tunable physical properties. It was rationally anticipated that the self-assembly of coumarin-fused helicenes would be controlled by the effects of a substituent on the internal edge of the helix. Here, this work reports the efficient syntheses of coumarin-fused helicenes 1 a,b (R=Ph, Me), and the enantioselective synthesis of 1 a (R=Ph) by chiral AuI-catalyzed hydroarylation. The helical structure of 1 was unambiguously determined by X-ray crystallography. Of particular note, the enantiomerically pure crystal of 1 a adopted a one-dimensional columnar structure based on π–π stacking interactions, as expected. Furthermore, a significant difference between the fluorescence quantum yields of the enantiomerically pure form and racemate of 1 a was observed.
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U2 - 10.1002/chem.201803270
DO - 10.1002/chem.201803270
M3 - Article
C2 - 30062767
AN - SCOPUS:85053440464
SN - 0947-6539
VL - 24
SP - 14617
EP - 14621
JO - Chemistry - A European Journal
JF - Chemistry - A European Journal
IS - 55
ER -