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Effective sampling thickness, linearity and energy resolution were measured.
However, in our study, the estimated sampling thickness for short-period PKKP waveforms is about one or two wavelength, which is on the order of tens of km above the CMB (Sylvander et al. 1997).
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There is no limitation to the sample thickness – the model is valid for thin as well as for thick samples.
Moreover, with the increase of sample thickness, the shielding effectiveness is also enhanced.
for the sample thickness used in this study up to 180 nm.
It is clear that with the increase of sample thickness, the shielding effectiveness is enhanced.
where log(Io/I is the optical density, d is the sample thickness and λ is the wavelength.
The effect of sample thickness on electromagnetic shielding for the dust filler materials is shown in Fig. 9.
The sample thickness is matched with the electron mean-free-path at the Fermi level (70 nm)25.
For the synchrotron measurement, the sample thickness was 2 μm, and the cell walls were 100 nm Si3N4.
The sample thickness was varied from 0.1 to 8 mm.
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