reduced. As shown in Figure 7, the peak directivity of this case is less than 4 dBi at 5.80 GHz (compared with more than 7 dBi in the Fins PNRE case).
CONCLUSIONAn impedance-matched, 5.8-GHz extruded-fin heatsink antenna was introduced having two orthogonal fin orientations. The orientation was shown to have a significant effect on the antenna directivity and gain performance across a frequency range. Thus, the extruded-fin heatsink provides the flexibility of either a highor low-directivity antenna simply by the orientation of the fins. The best choice will be determined by the specific application.Furthermore, the results demonstrated that the extruded-fin heatsink can improve the antenna performance while reducing the component count and providing a mechanism for removing thermal energy from high-power electronics such as an RF power amplifier. These performance improvements allow the use of lowcost, lossy FR4 substrates (which would typically be considered a poor substrate choice) with high dielectric losses. FL, March 19 -22, 2007, pp. 419 -422. 3. C.A. Balanis, Antenna theory: Analysis and design, 3rd ed., Wiley, Hoboken, NJ, 2005, pp. 641-642. 4. T.A. Milligan, Modern antenna design, McGraw-Hill, New York, NY, 1985 Because BER is the most preferred parameter for fault management, its monitoring techniques are gaining importance. One such signal quality monitoring scheme is based on the Q-factor monitoring, which can be obtained from an amplitude histogram obtained using synchronous sampling [6,7]. However, this method requires clock recovery to ensure synchronization in the sampling process. In practice, clock recovery electronics are both bit-rate and signal-format dependent. To reduce system complexity, Shake et al. used the amplitude histogram generated by asynchronous sampling to calculate the averaged Q-factor (Q avg ) without clock recovery [8,9]. With this scheme, bit-rate and signal-format transparency can be achieved. Furthermore, the Q avg value was found to have a highly linear relationship with the real value of Q-factor (Q t ) [10]. Photonic sampling methods can be classified into two types: all-optical and electro-optical (EO) sampling. The former gates the signal with optical sampling pulses, and the gating process is usually based on second-order or third-order nonlinear optical effects [11,12]. The latter utilizes electrical pulses to drive an optical sampling gate, which is often an EO or electroabsorption (EA) modulator [13]. Because the modulators and electrical pulse generators are relatively simple and low in cost, EO sampling is widely used in high-speed sampling modules. The amplitude histogram depends on the sampling uniformity, which is related to the relationship between the signal rate (f s ) and sampling rate (f c ). This histogram is also affected by the sampling position. For asynchronous sampling with a small number of sampling points, the histogram cannot represent the real statistics of the original signal if f s is very close to an integer multiple of f c . In th...