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Although the incident polarization of the light used to excite the luminescence affects the total emission intensity, it does not affect the polarization of the luminescence signal.
Total emission intensity of the La1 − x − y Eu y Ca x VO4 samples have shown essential increasing when dopant concentration increases up to x, y = 0.15 (Fig. 9, curve 1).
Skin AF is calculated as the ratio between the total emission intensity (420‒600 nm) and the total excitation intensity (300‒420 nm).
The total emission intensity from the stratum corneum as a function of excitation wavelength is shown in Fig. 3(f) for the different classification of oral mucosa.
From the Malus law, I H= I0 cos θ and I V= I0 sin θ, in which I0 is the total emission intensity of the in-plane projection.
However, in single fluorophore experiments where a large numerical aperture (NA) must be used, the total emission intensity is not always equivalent to I || + 2I ⊥, as it is for narrow beam angles [ 42, 43].
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b The NaGdF4:12%Er3+@NaGdF4:x%Er3+ (x = 9, 9.5, 10, 10.5, and 11) active-core/active-shell NPs under 1540-nm excitation Fig. 4 Enhancement factors of total emission intensities of NaGdF4:12%Er3+ core NPs, NaGdF4:12%Er3+@Nactive-core/inert-shell-shell NPs, and the NaGdF4:12%Er3+@NaGdF4:x%Er3+(x = 6, 8, 10, and 12) active-core/active-shell NPs under 1540-nm excitation.
The total spontaneous emission intensity is measured by modulating the device in the unamplified region, where I < I th.
Modelling of the electron temperature enhancements in the interaction region accounts for only one-third of the total O 1D) emission intensity.
Figure 7 shows the plot of ln(I) vs. ln(L sp 1/2), where I is the injection current and L sp is the total spontaneous emission intensity.
The total gamma emission intensity increased from 2.12 to 2.41 and from 2.41 to 3.04 for respectively the 238U and 232Th decay series.
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