frequency 3.35 GHz) and 16.52% (at center frequency 3.57 GHz) in the broadside direction (h 5 08, U 5 08) shown in Figure 7. It is observed that in the Figure 8 the RHCP is stronger than the left hand circular polarization (LHCP) in broadside direction so, the proposed antenna is called RHCP. The simulated and measured RHCP and LHCP radiation patterns in xz-and yz-plane at 3.35, 3.55, and 3.75 GHz are shown in Figure 8. It has been found that in broadside direction the RHCP leads the LHCP by 226.63 dB, 219.28 dB, and 226.05 dB at 3.35 GHz, 3.55 GHz, and 3.75 GHz, respectively. The electric field distribution observed inside the DRA at different phase, that is, 08, 908, 1808, and 2708 confirms the proposed design is CP and it also confirms that the mode of DRA is TE 12d mode shown in Figure 9. The average gain and radiation efficiency is 4.69 dB and 74.84% in the working band shown in Figure 10. Table 1 show the comparison of earlier published work. It has been observed that proposed work shows improvement in AR bandwidth within working band over earlier reported design.
CONCLUSIONIn this article, a new modified microstrip-line-fed rectangular dielectric resonator antenna coupled with slotted ground plane for circular polarization has been proposed. The measured impedance bandwidth is 17.87% (at center frequency 3.58 GHz) and measured AR bandwidth of proposed antenna is 16.52% (at center frequency 3.57 GHz) in the broadside direction (h 5 08, U 5 08), respectively. The proposed dielectric resonator antenna offer simple construction with sufficient bandwidth and excellent far-field properties. TE 12d mode has been excited in this proposed antenna. It has been observed that the proposed antenna shows RHCP in broadside direction (h 5 08, U 5 08). This antenna can be suitable for Wi-MAX (3.3-3.6 GHz) applications.