0 . 06 0 . 04 ti. 02 2 4 6 8 1 0 Figure 7 Thickness d3 as a function of the pseudochirality admittance 0, normalized to the free-space impedance ( E ,~ = 5 . E " , F , , = 2 . E,,, eZ. = E(,. p t , = y z z = yo. f = 10 GHz, h = d13) the ordinary (&,) and extraordinary (a,,) waves, when the pseudochirality admittance is given by 7.In this article, based on our theoretical analysis, we studied novel features of the radiated pattern of a point source embedded in a pseudochiral slab. In particular, using the dyadic spectral Green's-function approach, we evaluated the farzone electromagnetic field and the radiated pattern for a horizontal electric point source. It has been shown that the shape of the radiation pattern of the elemental source is strongly affected by the pseudochiral admittance O,, unless the cp = i d 2 cut is considered. Nevertheless, in the cp = 7r/2 cut the radiated field seems to have interesting features for applications. First, we noted by appropriately varying the constitutive parameters and the thickness of the pseudochiral slab, the position of the maxima can be shifted. Second, such a structure can support radiation in the horizon plane.
ABSTRACTA common-collector common-emitter PIN-BJT receiver topology is considered for use with optical-fiber pulse position modulation (PPM). The PPM PIN-BJT system is shown to offer a sensitivity improvement of 8.6 d B over a comparable PCM system when both systems are operating at 140 Mbitls and h = 1.3 w . The sensitivity penalty in self-synchronized PPM due to slot clock jitter is considered. This is shown to be significant (3.6 and 6.3 dB) at the set of parameters considered. A n optimum presynchroriization filter is derived and shown to result in the minimization of the jitter penalty. The inclusion of the filter resulted in reduction in the jitter penalty to about 0.1 d B for the two sets of parameters considered. 0