TY - JOUR
T1 - Correction to
T2 - Giant elasto-optic response of gallium selenide on flexible mica (npj Flexible Electronics, (2025), 9, 1, (2), 10.1038/s41528-024-00375-3)
AU - Barker, T.
AU - Gray, A.
AU - Weir, M. P.
AU - Sharp, J. S.
AU - Kenton, A.
AU - Kudrynskyi, Z. R.
AU - Rostami, H.
AU - Patané, A.
PY - 2025/1/4
Y1 - 2025/1/4
N2 - Correction to: npj Flexible Electronicshttps://doi.org/10.1038/s41528-024-00375-3, published online 04 January 2025 In the original version of the article in Figs. 2, 3 and 4 and corresponding text, the value of the strain is estimated for different bending radii, r, of the mica, i.e. the strain is calculated as t/2r, where t = 0.03 mm is the thickness of the mica. For example, for r = 4 cm, t/2r = 0.04%. However, as shown in Fig. 1, the mica is bent to a radius of approximately r = 4 mm, not r = 4 cm. Thus, the actual strain is a factor of 10 higher (0.4%) than that reported in the original manuscript and in the original Figs. 2, 3 and 4. The strain is used to calculate and discuss the strain sensitivity of the Raman and photoluminescence spectra (Figs. 2, 3) and its comparison with the modeling from the literature (Fig. 4). The experimental data on the energy shift of the photoluminescence emission versus the applied strain are now more aligned with the modelling, but reveal a variability amongst different samples that is discussed in terms of the exciton thermalization. The strain is used to calculate and discuss the strain sensitivity of the Raman and photoluminescence spectra (Figs. 2, 3) and its comparison with the modeling from the literature (Fig. 4). Thus, it is essential to correct the data to ensure the results are accurately presented. The original article has been corrected.
AB - Correction to: npj Flexible Electronicshttps://doi.org/10.1038/s41528-024-00375-3, published online 04 January 2025 In the original version of the article in Figs. 2, 3 and 4 and corresponding text, the value of the strain is estimated for different bending radii, r, of the mica, i.e. the strain is calculated as t/2r, where t = 0.03 mm is the thickness of the mica. For example, for r = 4 cm, t/2r = 0.04%. However, as shown in Fig. 1, the mica is bent to a radius of approximately r = 4 mm, not r = 4 cm. Thus, the actual strain is a factor of 10 higher (0.4%) than that reported in the original manuscript and in the original Figs. 2, 3 and 4. The strain is used to calculate and discuss the strain sensitivity of the Raman and photoluminescence spectra (Figs. 2, 3) and its comparison with the modeling from the literature (Fig. 4). The experimental data on the energy shift of the photoluminescence emission versus the applied strain are now more aligned with the modelling, but reveal a variability amongst different samples that is discussed in terms of the exciton thermalization. The strain is used to calculate and discuss the strain sensitivity of the Raman and photoluminescence spectra (Figs. 2, 3) and its comparison with the modeling from the literature (Fig. 4). Thus, it is essential to correct the data to ensure the results are accurately presented. The original article has been corrected.
UR - http://www.scopus.com/inward/record.url?scp=105003427937&partnerID=8YFLogxK
U2 - 10.1038/s41528-025-00406-7
DO - 10.1038/s41528-025-00406-7
M3 - Comment/debate
AN - SCOPUS:105003427937
SN - 2397-4621
VL - 9
JO - npj flexible electronics
JF - npj flexible electronics
IS - 1
M1 - 29
ER -