cations. To optimize the design parameters, the Sonnet (a method of moments (MoM) full-wave simulator) was used. Although the simulated results slightly disagree with the measured results due to the infinite-substrate presumption of the Sonnet simulator, the simulated results are still valuable and necessary. After the simulated optimum is obtained, the prototype is constructed by printing the patches on the 0.8-mm FR4 substrate. The reflection loss and radiation patterns are measured and discussed as follows.The simulated and measured results of reflection loss are shown in Figure 2. The resonant frequencies are indeed located at the EGSM and DCS bands. The measured bandwidths (determined by 1:2.5 VSWR) are about 120 and 124 MHz at the EGSM and DCS bands, respectively. The bandwidths are almost large enough to meet the bandwidth requirements of the EGSM/DCS systems, and are much better than those obtained in [2-4], especially at the EGSM band.Measured radiation patterns are presented in Figures 3 and 4 for the resonant frequencies at the EGSM and DCS bands, respectively. For both resonant frequencies, good omnidirectional radiation is observed. The maximum antenna gains for both the copolarization and cross-polarization patterns are estimated to be about 2.8 and 4.9 dBi across the EGSM and DCS bands, respectively.
CONCLUSIONA novel NMFGA design has been proposed. A dual-band NMFGA prototype has been shown as an example. It has been demonstrated that the resonant modes at the EGSM and DCS bands can be excited. As the measured and simulated results show, not only the radiation characteristics but also the impedance-matching bandwidths are very attractive for EGSM/DCS dual-band applications.