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Here, the theoretical wavelengths are obtained assuming 100% theoretical polarization strength.
The theoretical polarization strength is calculated according to the non-linear polarization reported by Fiorentini and Barnardini et al. [3].
Because the polarization of III-nitrides originates from the displacement of the charge centers in wurtzite lattice, any disorders in the lattice can affect the polarization strength.
The quantum levels of electron and hole in the QWs are also calculated by self-consistent Poisson-Schrodinger calculation, assuming 100% polarization strength in the QWs.
In most of the cases, including the case of the circular polarization, strength of E z was the largest, indicating that linear polarization is p-polarization.
In addition, it is even possible to render θB=0 via proper manipulation of the permanent polarization strength and its orientation, as well as the magnetic permeability.
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a peak-to-peak voltage versus QW thickness for doping density ND = 1018 cm−3 and various polarization strengths, as marked b Saturated peak-to-peak voltage versus doping density ND for various polarization strengths c ratio of peak voltage to the polarization potential versus QW thickness for doping density ND = 1018 cm−3.
In this paper, the polarization strengths in quantum well structures with indium content varying from 14.8 to 26.5% are experimentally investigated through photoluminescence and high-resolution X-ray diffraction (HR-XRD).
This is illustrated in Fig. 9, plotting the ratio 2Vo/Vp versus doping density ND for fixed QWL = 8 nm and for various strengths Figure 9 ratio of peak voltage to the polarization potential versus doping density ND in a QW of thickness L = 8 nm, for various polarization strengths.
It is found that when the indium content is smaller than 17.3%, 100% theoretical polarization field strength can be maintained, while when the indium content is larger than 17.3%, the polarization field strength decreased significantly.
Analytic solutions of (23) and (24) in terms of the polarization field strength exist for certain degenerate and non-degenerate limits.
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