Lucas
Webster
a,
Liangbo
Liang
b and
Jia-An
Yan
*a
aDepartment of Physics, Astronomy, and Geosciences, Towson University, 8000 York Road, Towson, MD 21252, USA. E-mail: jiaanyan@gmail.com
bCenter for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
First published on 14th July 2022
Correction for ‘Distinct spin–lattice and spin–phonon interactions in monolayer magnetic CrI3’ by Lucas Webster et al., Phys. Chem. Chem. Phys., 2018, 20, 23546–23555, https://doi.org/10.1039/C8CP03599G.
Specifically, the monolayer CrI3 possesses a D3d point group of symmetry and the irreducible representations of the phonon modes at Γ should be decomposed into ΓD3d = 2A1g + 2A2g + A1u + 3A2u + 4Eg + 4Eu, instead of ΓD3d = 2A1g + 2A2g + 2A1u + 2A2u + 4Eg + 4Eu, as in the manuscript (Section 3.3).
The acoustic modes are Eu + A2u, i.e., the doubly degenerate Eu mode, and one A2u mode, not Eu + A1u. In addition, the A2g mode at 217.6 cm−1 is neither Raman active nor IR active, thus is a silent mode.
Finally, as shown in Fig. 4(j), the mode at 134.5 cm−1 is an A1u mode, while the mode at 264.7 cm−1 (Fig. 4(n)) should be an A2u mode.
The conclusions in the published manuscript are not affected by these corrections.
We are grateful to Liu et al.1 who pointed out these mistakes in our manuscript.
The Royal Society of Chemistry apologises for these errors and any consequent inconvenience to authors and readers.
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