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Thus, in the optical regime, two proposals have prevailed.
In the optical regime, metals are dispersive materials with finite conductivity.
Recently, nano-aperture is noticed due to its good transmission in the optical regime.
However, the plasmon bands are extremely lossy due to the intrinsic absorption of noble metals in the optical regime.
The first strain optical regime is linear where primarily the soft segments orient.
A probabilistic noiseless linear amplification scheme has already been demonstrated in the optical regime [60, 61], but it relies on the possibility of counting photons.
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The transition between the first and second strain optical regimes was found to correspond to the saturation of straining of the soft segments that lead to start of rotation of hard segments in the stretching direction.
We show that this fast and efficient new numerical description of zero-order Bessel beams can be used with advantage, for example, in the analysis of optical forces in optical trapping systems for arbitrary optical regimes.
Radial and axial radiation pressure forces were then calculated for both Gaussian and Bessel beams using first a ray optics approach, and further the generalized Lorenz-Mie theory (GLMT) with the integral localized approximation (ILA), thus allowing an all-optical regime analysis [ 16– 16].
Linear profile, taken as a standard, yields three stress-optical regimes (SOR) during deformation.
Furthermore, the graded waveguide can be easily realized and fabricated by GaAs-based waveguide in the infrared optical frequency regime.
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