Abstract

This erratum corrects the errors that appeared in Photon. Res. 6, 709 (2018) [CrossRef]   associated with the polarization description of the experimental optical path, as well as the image errors.

© 2020 Chinese Laser Press

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References

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  1. W. Zheng, J. Yan, F. Li, and F. Huang, “Elucidation of “phase difference” in Raman tensor formalism,” Photon. Res. 6, 709–712 (2018).
    [Crossref]
  2. W. Zheng, R. Zheng, F. Huang, H. Wu, and F. Li, “Raman tensor of AlN bulk single crystal,” Photon. Res. 3, 38–43 (2015).
    [Crossref]

2018 (1)

2015 (1)

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Figures (1)

Fig. 1.
Fig. 1. Angle-dependent polarized Raman spectra of AlN, GaN, ZnO, SiC bulk single crystals obtained on the m plane under a parallel polarization configuration for different rotation angles increasing from 0° to 180° with a step of 5°. The A 1 ( TO ) , E 1 ( TO ) , E 2 2 phonons of each sample can be clearly identified. The parallel polarization configuration is written as X ( α α ) X ¯ in shorthand, where X and X ¯ denote the direction of propagation of incident and scattered lights, respectively; α represents the direction of polarization. Here, α = y · cos θ , in which θ is the angle between the polarization vector and the y axis.