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The transmittable optical power is limited and the boundary layer causes undesired reflections.
The perfectly matched layers (PML) with a width of 50 nm are implemented on the top and bottom of the computation domain to eliminate undesired reflections from the domain boundary beta ={k}_0sqrt{1-{left(frac{2}{sigma_{mathrm{g}}sqrt{mu_{mathrm{r}hrm{r}}/{varepsilon}_0{varepsilon}_{mathrm{r}}}}right)}^2,} (1).
As a result, reflective imaging systems have been preferred over refractive ones, as they have the advantage of avoiding undesired reflections from refractive surfaces.
Current clinical ophthalmoscopes form images of the retina by delivering and collecting light through non overlapping portions of the eye's pupil in order to avoid undesired reflections from the cornea and crystalline lens.
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Thus, a specially designed experimental apparatus was constructed so as to minimise undesired wave reflections in the plate and, thus, achieve a high energy flow boundary crossing at the edges of the plate.
Finally, the positive results from this work suggest that annular pupil apodization could be used in refractive or catadioptric adaptive optics ophthalmoscopes to mitigate undesired back-reflections.
Finally, undesired back-reflections from the surfaces of refractive elements in most current AO ophthalmoscopes are removed by slightly tilting the elements.
Nanolayers with a negative neutron potential at the interfaces of magnetic and nonmagnetic layers in neutron coatings may suppress reflection of neutrons with undesired spin direction by one or even two orders of magnitude [N.K. Pleshanov, Nucl. Instr. and Meth. A 613 (2010) 15].
It is based on the use of layers with a negative potential of definite thickness to suppress reflection of neutrons with the undesired spin from the potential barriers formed by structural imperfections.
Optical measurements allow visualization of wave propagation and resonance patterns in SAW devices as well as the detection of loss sources and undesired responses, such as escaping acoustic beams, unwanted reflections and acoustic crosstalk.
Thus, the clean speech signal can be decomposed into the desired direct sound and early reflection part, n = 0…L, and the undesired reverberation components n = L+1…∞, begin{array}{*{20}l} y_{i}(k) &= sumlimits_{n = 0}^{L}s k-n h_{i}(n)[-2pt] &quad+ sumL}s k-n h = L+1}^{infty}s(k-n)h_{i}(n) + n_{i,text{a}}(k), [-2pt] &quad{i}(k) + n_{i}(k), end{array} (2).
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