Photonics Research, 2018, 6 (7): 07000709, Published Online: Jul. 4, 2018
Elucidation of “phase difference” in Raman tensor formalism Download: 526次
Figures & Tables
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 = z · cos θ , in which θ is the angle between the polarization vector and the z axis.
Fig. 2. Fitted A 1 ( TO ) intensity-angle relationship of four wurtzite compounds using a traditional and a new Raman tensor, respectively. The “data” in the plot refers to the original experimental data, “Fitting 1” represents the fitting result using traditional theory, while “Fitting 2” represents the result of the new theory.
Table1. Raman Tensor Elements of Four Wurtzite Compounds Fitted from Angle-Dependent Polarized Raman Spectra Using Traditional and New Raman Tensor, Respectivelya
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Wei Zheng, Jingshen Yan, Fadi Li, Feng Huang. Elucidation of “phase difference” in Raman tensor formalism[J]. Photonics Research, 2018, 6(7): 07000709.