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This curve can be fitted with very well as shown in Fig. 5b, which indicates that the mechanism of electronic transportation of the sample is weak localized electron electron interaction [14].
Below 2.3 eV, the PDS absorption for the 200 °C, only air annealed sample is weak compared with that of the samples with additional vacuum annealing.
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The yellow luminescence for the LT-20 and LT-21 samples is nearly same, while that for the LT-32 sample is weaker.
When the temperature decreases to 343 K, a very standard force curve for a stiff surface is captured with an indentation of 89 nm, which indicates that the interaction between tip and sample is weaker.
The bands formed by the ss DNA sample were weak even at the maximum strain amplitude.
Although the inverse association between OHL and OHRQoL across the entire sample was weak, subjects in the "low" OHL group reported significantly more OHRQoL impacts versus those with higher literacy.
Emission of the La1 − x Ca x VO4 samples is weak and consists of wide bands in the 450 800 nm spectral range.
However, the strength of characteristic diffraction peaks of the both samples is weak indicating the ultra-thin layered structure and the relative weak crystallinity of HZ and HT in the composites.
The bands at 1550, 917, and 778 cm−1 of 30 μL PPy-coated urchin-like MnO2 sample are weaker than those of 50 μL PPy-coated caddice-clew-like MnO2 sample.
Similarly, the vRNA signal from the AMMM-infected sample was weaker than those of the MAMM sample and WSN control (MMMM).
Besides, the birefringence of the ferronematic samples is weaker than those of the corresponding pure MF samples.
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