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Using a co-axial EPD, titanium was successfully deposited uniformly on the inner surfaces of 12″ length of cladding with 4 mm inner diameter.
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V parameter of a PCF can be expressed by the following relation [9] V=frac{2pi rf}{c}sqrt{n_{co}^2 - {n}_{cl}^2} le 2.405 (4 where r is the half of the side length, f is the operating frequency, n co is the refractive index of core and n cl is the refractive index of cladding.
The choice of cladding materials was surprisingly important.
Thus, the main tasks observed were in the area of cladding.
This type of cladding layer is favorable for strong surface interactions [30].
Based on the analysis, the C type is the hardest cladding layer among the four types of cladding material, up to HRC66.9, the A cladding layer is a less hard layer, the B cladding layer is the least hard layer, with its hardness reaching HRC51.
Compared to the ideal condition of the SHP in air cladding, the propagation length of the AHP waveguide is approximately equal to that of the SHP waveguide in air (2.38 × 103 μm) with a comparable normalized modal area.
Compared to an SHP waveguide with the same structure embedded in air cladding, the propagation length of the AHP waveguide is approximately the same along with a comparable normalized modal area.
The results show the dominance of cladding and roofing materials.
The Fermi energy exhibits convergence with respect to the amount of cladding, as reported above.
If the length of the wire electrodes is longer than the cladding pipe, a nanostructured oxide layer will be prepared on the whole surface of the cladding pipe at the same time.
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