Sentence examples for reflection from the interface from inspiring English sources

Reflections from the top and bottom surfaces of the discs are temporally resolved, as is a reflection from the interface between acetone-wet polymer and dry polymer.

However, it has been shown previously by this group that reflection from the interface in composites can be used to increase reflection loss if the microwaves penetrate into the absorbing media.

In this work, the depth of 0 μm refers to the tissue surface where the multiphoton signal of reflection from the interface between the tissue and the glass coverslip reaches to maximum.

Initially, we estimate the maximum reflection from the interface as B = κ| r|, where κ = 44% is the expected coupling efficiency and r is the Fresnel coefficient at normal incidence; using the index of refraction for glass and buffer as 1.515 and 1.333, respectively, we have B ≈ 0.44×0.064 ≈ 0.028.

According to the Fresnel equations, when the light is at near-normal incidence, the reflection coefficient (reflectivity) from the interface between two contacting transparent materials is determined by their refractive indices n1 and n2: R = left( {frac{{n_{1} - n_{2} }}{{n_{1} + n_{2} }}} right)^{2}.

Obviously, this is accompanied by optical losses upon reflection from the interfaces air glass, glass TCO, TCO CdS, CdS CdTe as well as absorption in glass plate, TCO and CdS.

They surround the finite computational domain (obtained by truncation) and are designed to attenuate and completely absorb all the outgoing waves while producing no reflections from the interface between the domain and the layer.

These larger attenuations are, generally, translated into the stronger sources of attenuation, i.e., intrinsic physical processes, such as the interactions between the solid and the fluid, grain friction etc. Chapman et al. (2006) studied the reflections from the interface between the medium based on squirt flow concept and an elastic overburden.

Accordingly, in either region, ϕ and θ represent the phases that have accumulated following the reflection from the primary interface (optical elements or coverslip-buffer) and the secondary interface (coverslip-buffer or sample), respectively.

The λ/4 P2 layer introduces a π phase shift in the reflections from the interfaces either side of the P2 layer, suppressing the effect of these reflections in the transmitted beam (similar to an antireflection coating).

These interferences produce a vertically downgoing S wave from the surface and its upgoing reflection from the horizontal interface.