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Furthermore, polarized emissions with high polarization degree can be achieved by properly tuning the y:x ratio for certain x.
This is due to the fact that such ions have larger polarization degree and therefore are better attracted by polar group on the surface.
As a polarizing device of the instrument, two V-shaped polarizing super mirrors arranged in crossed geometry to enhance the polarization degree has been considered.
These 2D gases can inject spin-polarized carriers into the QW under applied voltage resulting in high polarization degree values.
It was found that the emission is linearly polarized along the c-crystal axis (along the electric field), and the polarization degree attains 50% at least.
We have evidence of highly polarized 2DEG and 2DHG in the RTD which can contribute to the polarization degree of carriers in the QW.
It was observed that the high QW polarization degree observed on those measurements is mostly due to a highly spin polarized carriers from the two dimensional gas formed in the accumulation layer next to the emitter barrier.
AK estimated the polarization degree.
The mean of polarization degree is 81.2%.
System efficiency-to-polarization degree ratio is inversely linear with demineralization, WRRTC, and polarization degree (PD).
Particularly, we have observed that the X− polarization degree is slightly lower than the X polarization degree.
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