IntroductionFor high-speed broadband wireless communication systems, the unlicensed frequency band of 60 GHz is utilized. Millimeter-wave components using a post-wall waveguide have been studied because they are easily fabricated in a printed-circuit board [1]. One of them is the transition from a coaxial line to post-wall waveguide. Conventional transitions have wide frequency band by exploiting tapered or open-ended post as the center conductor from the coaxial line. However they are difficult to fabricate in a thin dielectric substrate board due to three-dimensional structure. On the other hand, a transition using short-ended straight post is easy to fabricate; however, it has a limited bandwidth [1]. To overcome this problem, a new technique realizing wide frequency band with simple structure is required. This paper introduces a dual-resonance technique to enhance the bandwidth of a transition using short-ended straight post structure. In our technique, dual resonance is achieved by using two cavity resonators. To confirm our technique, numerical study is performed to show that two resonant frequencies can be controlled by tuning the lengths of the cavities. Using our bandwidth enhancement technique, a transition with straight short-ended post is designed for the waveguide slot-array antenna at 60 GHz [2]. The effectiveness of our technique is evaluated by comparing the frequency characteristics of our designed transition with those of the conventional one with the short-ended straight post.
Bandwidth Enhancement TechniqueThe structure of the transition is shown in Fig. 1. In order to achieve wide bandwidth, we propose a dual-resonance technique by using two cavity resonators with width of w c , and length of l 1 and l 2 . The short-ended straight post with diameter of d is connected to the inner conductor of the coaxial line. The second cavity and the output waveguide with width of w g are connected via inductive window with width of w i . They are formed in a dielectric substrate with a relative permittivity of ε r and thickness of t.The principle of our technique can be explained by using the equivalent circuit as shown in Fig. 2. Two cavities are represented by two transmission lines having characteristic impedances Z 1 and Z 2 , respectively. The T-junction with the short-ended straight post can be expressed by three-port network K 1 , where the impedance of input coaxial port is Z 0 =50 ohm. The inductive window can be expressed by two-port network K 2 , where the impedance of output waveguide port is Z wg . The straight post connected to the center conductor of the coaxial line has two functions. One function is impedance matching between coaxial line with Z 0 and waveguides with Z 1 and Z 2 . The other is impedance inverter K 1 between two cavity resonators unlike conventional transitions. Therefore our transition realizes two resonances, resulting in wider bandwidth than conventional transition using straight post with one resonance.
Dual Resonance Behavior978-1-4244-2642-3/08/$25.00 ©2008 IEEE To co...