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Compared with the structure without the concentric rings over the ground plane, it is found that our proposed structure can obtain stronger electric field enhancements and narrower radiation beams because the gold rings can help to couple the light into the nanoantenna and they also scatter light into the far field and modify the far-field radiation pattern.
It is evident that the wooden panel behaves rather differently from the others OUT, since it exhibits the narrower radiation lobe in the backward half-space and is the only item showing a clear scattering lobe also in the forward half-space.
The minimum Q for a prolate spheroid is found for a narrower radiation pattern than the sin θ-figure characteristic for an elementary dipole, while for the oblate, the minimum turns out for a broader pattern than that of an elementary dipole.
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RadLine® is tested in a beta and gamma narrow radiation field of 2.4 GBq, from a Caesium-137 (662 KeV) source, at doses rates between 0.125 mSvhr−1 and 10 mSvhr−10
When a gas mixture flows through a passage and a highly exothermic reaction takes place on the wall very steep temperature gradients may develop and, though the passage be narrow, radiation from wall to wall may be important.
The narrow-beam radiation effect can be explained by an exponentially decaying leaky plasmon wave[19].
Carriers excited by bias lighting do not contribute to the photo-emf signal measured at the modulation frequency of the narrow-band radiation.
The reference narrow-band radiation generates a potential between anode and cathode of this optically driven quantum dot triode; a magnitude of this voltage depends on the charge of the QD grid (Figure11).
In order to locate the source of the interference, a narrow directive radiation pattern can be shifted while monitoring SNR and traffic congestion metrics on the UL control channels, scanning this way the entire cell or sector.
This can be explained by peculiarities of the antenna system such as (1) elevation angle aliasing effect at which the maximum measurable elevation is limited by 45° (Milan et al. 1997; McDonald et al. 2013; Ponomarenko et al. 2015) and (2) partially by the narrow elevation radiation pattern (it affects the location of the power maximum that the procedure searches in each sounding session).
For this reason the effect of bias lighting on photo-emf generated by the narrow-band radiation in the fundamental absorption range is much stronger for the R 166 structure, which have a thick buffer layer, than for the R 163 one.
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