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We have observed a good correlation between the I V) curve and integrated PL intensity for the QD emission for both circular σ+ and σ- polarizations.
In this section, we discuss how to control the molecule emission for both transmitters in Figure 1, i.e., how to control n 1 for TX I and how to control n 2 for TX II.
The deep trap emission is much more intense than the band edge emission for both samples compared to normal ZnO nanowires, indicating that the as-prepared nanostructures contained many defects related to oxygen vacancies [35].
As it can be seen from Figure 4c,f, for the excitation wavelength of 980 nm, thermal quenching of Er3+-related emission for both samples can be well characterized with only one deactivation energy (EErQ1) equal to approximately 20 meV.
We have observed a voltage-controlled circular polarization degree from the quantum well emission for both lines, with values up to −88% at 15 T at low voltages which are ascribed to an efficient spin injection from the 2D gases formed at the accumulation layers.
In our buffer system, the maximal emission for both NATA and MSI1 is 350 nm.
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Carbon monoxide (CO) is selected as a representative of gaseous traffic emissions for both field observations and numerical models.
Nonetheless, the total emissions associated with the manufacturing stage still only contribute an additional 1% to lifetime CO2 emissions for both fuel cell types.
Although fertilizer use was the same for both treatments the RT CC treatment had significantly (p < 0.05) higher N2O emissions for both present and future climate.
A reduced chemical reaction mechanism was developed for modeling the combustion process and soot emissions for both non-oxygenated and oxygenated hydrocarbon fuels.
Results show a drastic reduction of primary non-renewable energy (PNRE) demand and greenhouse gas (GHG) emissions for both mobility and dwelling-related consumption.
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