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Fig. 4 a Simulated reflection spectra and b experimental reflection spectra of samples with same diameter (D = 300 nm) and different depths (from 0 to 150 nm).
The experimental reflection spectra of the metal-coated NPs have broad dips at λ ~700 and ~1000 nm, indicated by α and β in Fig. 3a.
Using a spatial Fourier transform approach for the determination of the experimental reflection and transmission coefficients, the numerical results have been successfully validated.
The numerical simulations are shown to well reproduce the qualitative features of experimental reflection measurements performed for the corner sections of 16-ply CFRP laminate.
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We observe very good agreement between the calculated and experimental reflections.
Properly accounting for all the experimental reflections during the fitting exercise mandates the meridional reflections at q z = 0.34 Å–1 and 0.68 Å–1 to be the second- and forth-order reflections instead of the first- and second-order reflections in the out-of-plane direction.
The experimental coherent reflection coefficients are calculated using the attenuation corrected reflection coefficients and the normalized cross-correlation between successive backscatter echo signal waveforms in those areas.
Each experimental scenario (reflection conditions and scene group) was randomly assigned between the participants.
This behaviour may distort the extraction of biologically relevant genes in cases where expression patterns overlap several classes of samples or experimental conditions, a reflection of the dependence of the expression of most genes on multiple signals and their participation in more than one regulatory network.
Figure 3a, b shows the experimental and calculated reflection spectra of the bare and metal-coated Si NP arrays.
Rejection occurs most often when a PDB entry lacks experimental X-ray reflection data, which is the case for the ten structures listed.
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CEO of Professional Science Editing for Scientists @ prosciediting.com