IntroductionThe coplanar waveguide with a lower ground plane forms the conductor-backed coplanar waveguide (CBCPW). Due to the lower ground plane, the mechanical strength and heat-sinking capability of the conventional coplanar waveguide are improved [1]. In practice, the substrate and the ground planes of the CBCPW are usually of finite width. The CBCPW mode and the microstrip-like mode coexist in the finite-width CBCPW. Both of them have zero cutoff frequency [2]- [3]. The phase velocity of the microstrip-like mode (MSL) is slower than the CBCPW mode. Therefore, the MSL mode takes power away all the time. The leaky MSL mode causes the resonances of the side-plane conductors. The transmitted power is reduced by the reflected and radiated power when the side-plane conductors resonate [4]. The unwanted radiation maybe degrades the performance of the finite-width CBCPW-fed antenna unless through-plated vias are placed at the inner edges of the side-plane conductors [5]. Using through-plated vias increases the manufacturing cost. With proper design, the side-plane conductors fed by finite-width CBCPW can form a simple, vialess, unidirectional, and linearly polarized antenna [6]. In this paper, a compact finite-width CBCPW-fed circularly polarized (CP) side-plane antenna is proposed.
Antenna DesignThe geometry of the proposed antenna is shown in Fig. 1. The transverse slotlines cut the side-plane conductors into four separate conductors. The whole structure of antenna is composed of four nearly square conductors except the two shorting strips. The two shorting strips excite the upper right conductor and the upper left conductor to form a CP antenna. The offset between the two shorting strips excites the two conductors to radiate in phase as that in the previous work [6]. The nearly square conductor has two spatially orthogonal resonant modes [7]-[8]. The two modes have closely resonant frequencies, which are utilized to produce 90 degrees phase delay between them. Therefore, the CP radiation is achieved. In our design, there are four nearly square conductors. The upper pair is excited directly by the shorting strips. The lower pair is not only part of the transmission line but also part of the antenna. The radiation of the lower two conductors help the upper two directly-fed conductors achieve better CP radiation due to the small gap G h .978-1-4244-4968-2/10/$25.00 ©2010 IEEE For large G h , the coupling between the upper and lower conductors is weak and the CP radiation is small. There is an optimum value of G h for the axial ratio and the bandwidth of axial ratio. For simplicity, we let W a , L a and G v equal to W g , L g and G, respectively. The value of L f is fixed to (L a -L c ). The various value of G-S-G is restricted due to the characteristic impedance of 50 ohm CBCPW line. The structure in Fig. 1 forms a left-handed CP (LHCP) radiation. We can feed the upper right conductor with shorting strip first and then feed the upper left conductor at the end of the structure to obtain a right-handed CP (RHCP) anten...