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The sample prepared in optimal conditions had reflection loss of less than −10 dB (absorption >90%) and covering a frequency range of 8.4 11.6 GHz.
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For instance, the MWCNT/epoxy nanocomposite with 20 wt% CNT loading and 1.2 mm thickness reported by Che et al. [41] had a reflection loss of less than 2 dB.
Furthermore, non-woven fabric absorbing material has a reflection loss −26 dB with the matching thickness of 2.08 mm at 9.35 GHz.
The absorber of 3.74 GHz bandwidth has a minimum reflection loss of −31.32 dB at 11.13 GHz with a matching thickness of 3 mm and a low loading in paraffin of only 25% w/w.
From Fig. 4c f, it can be seen that composite of 10, 20, 30, 40 vol.% loading proportion have their approximate reflection loss R max at 11.5, 10, 8.5, 8 GHz at thickness t = 7 mm.
The RAS with CNT layer had a higher minimum reflection loss than that with carbon paste layer, and the absorbing frequency bandwidth was lower.
Most infrared transmitting optics have high refractive indices which in turn have high per surface reflection loss.
But everyone has reflections of that kind.
Yet in the non-detection state, the design has resulted in the reflection loss of less than −19 dB and the insertion loss of less than 0.6 dB.
On the basis of transmission line theory, the reflection loss has been calculated with variation of incident angles for both Transverse Electric (TE) and Transverse Magnetic (TM) polarization.
In the detection state, experiments demonstrate that the design of the improved power sensor has resulted in the reflection loss of less than −17 dB, the insertion loss of less than 0.8 dB, and the flatness of the frequency response at X-band.
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