TY - JOUR
T1 - Erratum
T2 - Shape-controlled anisotropy of superparamagnetic micro-/nanohelices (Nanoscale (2016) 8 (14127–14138) DOI: 10.1039/C6NR01803C)
AU - Leshansky, Alexander M.
AU - Morozov, Konstantin I.
AU - Rubinstein, Boris Y.
N1 - Publisher Copyright:
© 2022 The Royal Society of Chemistry.
PY - 2022/6/16
Y1 - 2022/6/16
N2 - The authors regret that in Fig. 3 of the original manuscript, images B and C were interchanged without a corresponding update to the caption. Fig. 3B shows the normal helix, while Fig. 3C depicts the binormal helix. The figure and the updated caption are therefore as displayed herein. Two sentences on page 14132 which reference Fig. 3 are also updated accordingly as below: “This non-local intrafilament interaction is most pronounced for binormal helices (see Fig. 3C), where elongation of the filament cross-section contributes to preservation of the longitudinal orientation of the easy axis, so that Φ ≲ 20° for all values of Θ”. “For normal helices the situation is the opposite – elongation of the filament cross-section along the normal vector (see Fig. 3B) contributes to transverse orientation of the easy axis and, therefore, the transition shifts to lower Θ* when compared to the regular helix” (Figure presented). The Royal Society of Chemistry apologises for these errors and any consequent inconvenience to authors and readers.
AB - The authors regret that in Fig. 3 of the original manuscript, images B and C were interchanged without a corresponding update to the caption. Fig. 3B shows the normal helix, while Fig. 3C depicts the binormal helix. The figure and the updated caption are therefore as displayed herein. Two sentences on page 14132 which reference Fig. 3 are also updated accordingly as below: “This non-local intrafilament interaction is most pronounced for binormal helices (see Fig. 3C), where elongation of the filament cross-section contributes to preservation of the longitudinal orientation of the easy axis, so that Φ ≲ 20° for all values of Θ”. “For normal helices the situation is the opposite – elongation of the filament cross-section along the normal vector (see Fig. 3B) contributes to transverse orientation of the easy axis and, therefore, the transition shifts to lower Θ* when compared to the regular helix” (Figure presented). The Royal Society of Chemistry apologises for these errors and any consequent inconvenience to authors and readers.
UR - http://www.scopus.com/inward/record.url?scp=85132357099&partnerID=8YFLogxK
U2 - 10.1039/d2nr90117j
DO - 10.1039/d2nr90117j
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AN - SCOPUS:85132357099
SN - 2040-3364
VL - 14
SP - 9192
JO - Nanoscale
JF - Nanoscale
IS - 25
ER -