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The measured SHG spectra from the urea reference sample were normalized to the SHG signal simultaneously recorded from a crystalline quartz plate. The frequency dependence of the nonlinear susceptibility of quartz was assumed to obey Miller’s rule
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The measured SHG spectra from the urea reference sample were normalized to the SHG signal simultaneously recorded from a crystalline quartz plate. The frequency dependence of the nonlinear susceptibility of quartz was assumed to obey Miller’s rule.
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85038278470
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The (Formula presented) energy of relaxed (Formula presented) is 3.18 eV (Ref. 3). From the spin-orbit-splitting, the deformation potentials, and the elastic constants, one calculates a stress-induced blueshift of about 10 meV for the (Formula presented) energy of strained (Formula presented) layers (Ref. 11
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The (Formula presented) energy of relaxed (Formula presented) is 3.18 eV (Ref. 3). From the spin-orbit-splitting, the deformation potentials, and the elastic constants, one calculates a stress-induced blueshift of about 10 meV for the (Formula presented) energy of strained (Formula presented) layers (Ref. 11).
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30
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85038342668
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We note that the energy of this interband resonance was actually not obtained from the fits but was kept fixed at a value of 4.40 eV. Because of the weak contribution of this resonance to the spectra, a free fit shifted its energy to an unrealistically large value without improving the quality of the fit. A reduction of this energy towards the bulk (Formula presented) energy of 4.27 eV clearly worsened the fits. In our investigations of various (Formula presented) interfaces (Refs. 8 and 11), we found the energy of this resonance to lie between 4.34 and 4.45 eV. Correspondingly, we give an error margin of (Formula presented) eV for the energy of this resonance
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We note that the energy of this interband resonance was actually not obtained from the fits but was kept fixed at a value of 4.40 eV. Because of the weak contribution of this resonance to the spectra, a free fit shifted its energy to an unrealistically large value without improving the quality of the fit. A reduction of this energy towards the bulk (Formula presented) energy of 4.27 eV clearly worsened the fits. In our investigations of various (Formula presented) interfaces (Refs. 8 and 11), we found the energy of this resonance to lie between 4.34 and 4.45 eV. Correspondingly, we give an error margin of (Formula presented) eV for the energy of this resonance.
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31
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85038283569
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The phase difference between these two resonances is about (Formula presented)
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The phase difference between these two resonances is about (Formula presented)
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