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This optical fiber sensor first realizes sampling from the surface of the optical fiber rather than the fiber ends.
Typical fiber sensor applications require films coated on the side surface of the optical fiber and optical properties of that curved films are crucial for design purposes.
The method effectively removes defective In2O3SnO2 nanostructures from the surface of the optical PET-film (PET) of e-paper and allows the substrate to be returned to the production line.
This fusion of two innovative technologies, and in particular the flexibility afforded by femtosecond laser inscription and micromachining, has led to the realisation of microfluidic channels, ring resonators, resonator disc, Mach-Zehnder and complex microfluidic designs in the surface of the optical chip, whereas Bragg grating waveguides have been recorded in the bulk volume of the optical chips.
In addition, another object and reference beam areas of O2 and R2 are also reflected from the back surface of the optical window glass.
The grating normal is parallel to y-axis, the grating grooves are parallel to z-axis, and the y´-axis is perpendicular to the right-angle surface of the optical wedge.
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We designed a series of photonic crystal (PhC) nanocavities using atomically flat silicon (111) interfaces and examined the impacts of the surfaces on the optical confinement.
Here, the hologram pattern is generated by controlling the sizes of the object beams which are reflected from the front and back surfaces of the optical window glass.
After being reflected from the front and back surfaces of the optical window glass, two sheared object beams, in which each object beam is composed of half-object and half-reference beams, are generated.
When the core of nanocrystal cover by inorganic materials with higher band gap, because of quantum confinement effect (Burda et al. 2005), eliminating of trap, development of dangling bond, and astonishingly decrease of defect in the surface of core, the optical characterizations of QDs are improved (Fig. 5b, c, and d) and is shown in Table 3.
It was demonstrated under similar conditions that the layers located 3 mm and less under the surface make substantial contributions to the surface recordings of the optical action potential [ 24, 25].
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