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Proceedings of the National Academy of Sciences of the United States of America logoLink to Proceedings of the National Academy of Sciences of the United States of America
. 2019 Mar 4;116(11):5194–5195. doi: 10.1073/pnas.1902266116

Correction for Sato et al., Chiral intertwined spirals and magnetic transition dipole moments dictated by cylinder helicity

PMCID: PMC6421435  PMID: 30833388

CHEMISTRY Correction for “Chiral intertwined spirals and magnetic transition dipole moments dictated by cylinder helicity,” by Sota Sato, Asami Yoshii, Satsuki Takahashi, Seiichi Furumi, Masayuki Takeuchi, and Hiroyuki Isobe, which was first published November 27, 2017; 10.1073/pnas.1717524114 (Proc Natl Acad Sci USA 114:13097–13101).

The authors wish to note the following: “The values for |m| in Fig. 3 are incorrect due to usage of an incorrect conversion factor. The correct unit conversion is 1 a.u. = 9.27400968 × 10−21 erg G–1.” The corrected Fig. 3 and its legend appear below.

Fig. 3.

Fig. 3.

Chiroptical properties of cylindrical molecules. (A) CD spectra of (P)- and (M)-(12,8)-[4]CC in toluene at 25 °C. (B) CD spectra of (P)- and (M)-(11,9)-[4]CC in toluene at 25 °C. (C) Transition density (Left) and transition dipole moments (Right) of methyl-substituted (P)-(12,8)-[4]CC. In the transition density isosurface, hole (green) and electron (red) distributions are shown at an isovalue of 0.0004. For the dipole moments, the ETDM vector is shown in red, and the MTDM vector is shown in blue. (D) Transition density (Left) and transition dipole moments (Right) of the methyl-substituted (P)-(11,9)-[4]CC. In the transition density isosurface, hole (green) and electron (red) distributions are shown at an isovalue of 0.0004. For the dipole moments, the ETDM vector is shown in red, and the MTDM vector is shown in blue.


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