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Numerical results show that the attenuation contribution from the homogeneous propagation (of any of the three faster waves) is only a little in the total attenuation of any of these attenuated waves.
Total attenuation of the phantom is low as there is no attenuating material surrounding the phantom.
Measurements are made for E approximately equal to 0, −1, and −2, corresponding to no change in vorticity, total attenuation of the vortex, and flame-generated vorticity, respectively.
Scattered light was found to be not more than about 5% with respect to the total attenuation of light.
In X-ray CT, the line integral represents the total attenuation of the beam of X-rays as it travels in a straight line through the object.
The total attenuation of GaP nanowires is much larger than InAs nanowires and third group nitrides due to their large thermal conductivity and acoustic coupling constants [29, 31, 32].
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Figure 8 shows the wavelength dependence of the total attenuation coefficients of these samples.
Figure 9(g) shows the wavelength dependence of the total attenuation coefficients of the enamel and dentine layers.
We observed wavelength dependence of the total attenuation coefficients of various samples in UHR-OCT. Figure 11(a) shows the total attenuation coefficients of the industrially used homogeneous materials.
The wavelength dependence of the total attenuation coefficients of the plastic cover and eraser were well-fitted to the λ−4 dependence.
The variation of the total attenuation coefficient of the dentine layer was 0.5 dB/mm, which is much less than that of the enamel layer, namely, 4.6 dB/mm.
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