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71 INTRODUCTION In this chapter, some recently reported broadband or bandwidth-enhancement techniques are presented By applying the well-known method of using additional microstrip resonators [1, 2], a broadband design using both directly coupled and gap-coupled coplanar microstrip resonators for achieving an impedance bandwidth larger than 10% (with a thin dielectric substrate) [3] is presented in Section 72 In Section 73, some typical broadband designs with a thick air or foam substrate are demonstrated These designs include the use of modi ed probe feeds [4 11] or modi ed radiating patches [12 20] for overcoming the problem of large probe reactance owing to the long probe pin in the thick substrate layer The large probe reactance usually makes impedance matching over a wide bandwidth dif cult to achieve, and the obtained impedance bandwidth is in general less than 10%.

Table 45. Criterion value and Cram&-Rao variances for equidistant design and for optimal design if width is target parameter

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With the proposed designs [4 20], achieving an impedance bandwidth larger than 25% becomes easy For modi ed probe feeds, designs with gap-coupled probe feed [4, 5], capacitively coupled feed [6, 7], L-probe/L-strip coupled feed [8 10], and three-dimensional microstrip transition feed [11] have been reported For modi ed radiating patches, it has been shown that, by embedding a U-shaped slot in the radiating patch (U-slotted patch) [12 14], cutting a pair of wide slits (E-patch) at the boundary of the patch [15 18], or using a three-dimensional V-shaped patch [19] or a wedge-shaped patch [20], good impedance matching over a wide bandwidth can be obtained Experimental results for prototypes of these designs are presented and discussed Promising methods of embedding suitable slots [21 24] and integrating microstrip reactive loading [25 28] in an antenna s radiating patch are discussed in Sections 74 and 75, respectively.

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spectral width of Nd:YAG crystal is about 130 GHz. Thus, in the SBS PCM arrangement, the small-signal ampli cation factor, G0 23, was reduced by about 25%. However, the output power using the HR mirror was limited to 5.5 W due to the laser-induced damage of the dielectric polarizer caused by the pattern deformation of the laser beam and also by the parasitic oscillation between the Nd:YAG rod and the conventional HR mirror. The pulse duration changed from 18 to 14 ns due to the SBS threshold process. Figure 6.13 shows the typical oscilloscope trace of the incident and re ected pulse shapes. Transient pulse deformation was seen at the beginning of the pulse, because the re ection started after the onset of the SBS with an appropriate energy consumption to generate a density grating. The strong thermal lens effect could be almost compensated in the double-pass system by the SBS mirror made of fused quartz. Figure 6.14 shows the SBS re ectivity of a bulk fused-quartz glass as a function of the incident pulse energy at 16-ns pulse duration using the focal length of 300 mm and 500 mm. As the incident energy increases, the SBS re ectivity increases monotonically. Using single transverse mode for the pump light, a fusedquartz glass can be used for higher pumping energy of few joules, without laserinduced damage for the f 500 mm case. The SBS re ectivity reached the maximum value of 95% at the input energy of 2.3 J, which was approximately 153 times larger than the SBS threshold of about 15 mJ [32]. The incident energy was

These two methods are mainly applicable for microstrip antennas with thin substrates, and in this case, the low-pro le advantage of microstrip antennas is retained Finally, a typical design for a broadband microstrip antenna with.

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