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Here, c is the speed of light; Γa, the absorption width; and Γs, the scattering width.
Thus, one obtains the following scattering width for the system: Γ s E = q 2 4 π ε 0 2 ω 4 3 c 3 k.
a Scattering width spectra (TM-polarized light) of an infinitely long dielectric cylinder with (red solid line) and without (black dashed line) a metasurface mantle cloak.
Figure 3c shows the calculated scattering width spectra of an infinitely long dielectric cylinder with various types of mantle cloaks, revealing that NIC-loaded (green solid line) and non-Foster (red solid line) mantle cloaks exhibit significantly improved cloaking bandwidth compared to that of the passive metasurface mantle cloak (blue solid line).
This maximum displacement of the peaks is ∼10% of the intrinsic scattering width of the profiles in a typical powder diffraction experiment.
This is because in general the instrument capture is significantly larger than the intrinsic scattering width of the crystallites; the likelihood of this being the case is considered next.
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A half-scatter width of 30° was used.
The spherical scatter width of the components was also taken into account as an optimization parameter.
b X-ray phase contrast image of the same acquisition as a, but processed to show the scatter width.
In particular, it would be interesting to see whether the scatter width image could show a signal from the carbon-based inks.
The field of view is ~ 2 cm × 5 cm and multiple images, showing parameters such as X-ray absorption, refraction and scatter width are obtained [32, 33].
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com