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@@ -63,14 +63,15 @@ The E#sub[1] mode calculated at 746.91 cm#super[-1] (mode 7)
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are predicted to have much weaker Raman intensities and are located close to the most intense mode (mode 8),
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are predicted to have much weaker Raman intensities and are located close to the most intense mode (mode 8),
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making them indistinguishable in experimental spectra.
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making them indistinguishable in experimental spectra.
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Additionally, the A#sub[1] mode calculated at 812.87 cm#super[-1] (mode 10)
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Additionally, the A#sub[1] mode calculated at 812.87 cm#super[-1] (mode 10)
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exhibits very weak Raman intensity in the configuration polarized in the basal-plane (xx and yy, only 0.01)
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exhibits a very weak Raman intensity in the basal-plane polarized configurations (xx and yy, only 0.01)
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but an observable intensity in the configuration polarized along z-axis (1.78).
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but shows an observable intensity when the polarization is along the z-axis (1.78).
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Since most Raman experiments are performed in a back-scattering configuration with light incident along the z-direction
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Since most Raman experiments are performed in a back-scattering configuration with light incident along the z-direction
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(polarized in-plane)
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(i.e., with in-plane polarization)
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with photon energies much lower than the band gap,
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and with photon energies much lower than the band gap,
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this mode is generally not observed (cite).
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this mode is typically not observed (cite).
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However, it should become detectable when the incident light have z-direction polarization part (as in our experiment)
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However, it should become detectable if the incident light has a polarization component along the z-direction
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or when the incident light wavelength is near resonance conditions (cite).
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(as in our experiment),
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or when the excitation wavelength approaches resonance conditions (cite).
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Besides, there are other peeks in the experiment.
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Besides, there are other peeks in the experiment.
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The peek at 796 and 980 are caused by strong-polar phonons which will be discussed later.
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The peek at 796 and 980 are caused by strong-polar phonons which will be discussed later.
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