Jung Jun
Bae
ab,
Hye Yun
Jeong
ab,
Gang Hee
Han
ab,
Jaesu
Kim
ab,
Hyun
Kim
ab,
Min Su
Kim
ab,
Byoung Hee
Moon
ab,
Seong Chu
Lim
*ab and
Young Hee
Lee
*abc
aCenter for Integrated Nanostructure Physics (CINAP), Institute for Basic Science (IBS), Suwon 16419, Republic of Korea. E-mail: seonglim@skku.edu
bDepartment of Energy Science, Department of Physics, Sungkyunkwan University (SKKU), Suwon 16419, Republic of Korea
cDepartment of Physics, Sungkyunkwan University (SKKU), Suwon 16419, Republic of Korea
First published on 23rd October 2018
Correction for ‘Thickness-dependent in-plane thermal conductivity of suspended MoS2 grown by chemical vapor deposition’ by Jung Jun Bae et al., Nanoscale, 2017, 9, 2541–2547.
Additionally, the authors wish to account for the difference between the trends observed in ref. 12 and their work. To clarify the origin of this trend for the thickness-dependent thermal conductivity, the authors would like to add the following paragraph:
“This finding is in stark contrast to that observed for graphene9 and exfoliated MoS2,12i.e. the in-plane thermal conductivity drops sharply with increasing thickness. The thickness-dependent thermal conductivity of MoS2 cannot be explained by the out-of-plane acoustic vibration mode, the ZA phonon, owing to the breaking of a selection rule in a non-centrosymmetric material (S10 in the ESI). Hence, the thickness dependence of MoS2 can be rationalized as follows”.
The Royal Society of Chemistry apologises for these errors and any consequent inconvenience to authors and readers.
This journal is © The Royal Society of Chemistry 2018 |