本篇論文提出兩種部分反射面之設計。第一種具高反射量與正相位梯度之線性極化部分反射面,並製作於印刷電路板上。而後形成一空腔共振天線,並加上金屬壁面後,再針對其尺寸作分析。最後,使用一背向饋入之基板集成波導激發此空腔。在操作頻率12.9GHz時,正向輻射(broadside)方向增益有15dB,且其3dB方向增益頻寬百分比有8.8%。第二種部分反射面則是利用兩片印刷電路板構成,並進一步組裝成雙空腔共振天線,透過調整第二片部分反射面的反射量可形成寬頻方向增益的設計。接著,利用一印刷電路板所組成的背覆空腔式孔徑天線來激發空腔設計,此設計可透過抽換一片印刷電路板且無須更動其他參數設計下,達成線性或圓形極化輻射。線性極化具有17.5dB方向增益與13%的方向增益頻寬百分比;圓形極化具有18.4dB方向增益與11.6%的方向增益頻寬百分比以及6.7%的3dB軸長比(axial ratio)頻寬百分。
This thesis presents two types of partially reflective surface (PRS). The first one is a PRS of high reflectivity and positive phase gradient fabricated on printed circuit board (PCB), where a cavity resonant antenna is built with such a PRS. After adding metallic walls to the cavity edges, we analyze the cavity dimension for optimal aperture efficiency. Then, we use a backed substrate integrated waveguide (SIW) to excite the cavity. A broadside gain of 15dB is obtained at 12.9GHz and the corresponding 3dB fractional gain flatness bandwidth is 8.8%. The second PRS design is composed of two PCBs, and we further use it to form a double cavity resonant antenna. Through adjusting the reflectivity of PRS2, the broadside radiation could be wideband. Next, we use a cavity-backed aperture antenna which is composed of multi-PCB to excite the resonant cavity, and we can switch a piece of PCB of this antenna to get linear polarized or circular polarized radiation. In the linearly polarized case, a broadside gain is 17.5dB and the corresponding 3dB gain flatness bandwidth is 13%. In the circularly polarized case, a broadside gain is 18.4dB and the corresponding 3dB gain flatness bandwidth is 11.7% and 3dB axial ratio bandwidth is 6.7%.