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The refractive index of samples n are computed from the obtained reflection and transmission spectrum.
The obtained reflection is below −20 dB in many frequency subranges, also under an oblique incident condition, within the band 2 18 GHz.
As model for input impedance (Z_{mathrm{liq}}), a full-wave model of [13] is employed; using fundamental TEM mode, and two lowest TM modes as basis functions, the input impedance is calculated from the obtained reflection coefficient.
The obtained reflection coefficients did not always coincide with theoretical values due to the uncertainty in focal mechanisms, large differences in P and PcP take-off angles, and other unknown causes.
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The obtained reflections could be indexed by a mixture of olivine and plagioclase single crystals.
Complicated AR parameter estimation method involving matrix inversion is not necessary for obtaining reflection coefficients.
We have shown this for some special cases by obtaining reflection dips at the particular angle of incidence.
It is possible to obtain reflection and image transmittance data by using a light source for the illumination and image analysis by a CCD/digital camera.
Reflectance standards (R = 10% and R = 50%, SRS-10-010, SRS-50 010, Labsphere®, North Sutton, New Hamsphire) were used to obtain reflection spectra (R10% and R50%) for calibration.
In the proposed algorithm, the effective CFRs for an AP are obtained by first obtaining reflection-rich CFRs for contiguous subcarriers from the CSI, then obtaining parameters of the sinusoids in the reflection-rich CFRs, and finally transforming the reflection-rich CFRs to obtain the result.
The Terahertz Time-Domain Spectroscopy (THz-TDS) setup used for obtaining reflections from normal and burned skin has been explained in the literature [ 20, 21].
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