at 3.8 GHz is clearly observed, which gives about À33 dB rejection. At the rejection band of 2.3-12 GHz, the rejection of the transmission is less than about À20 dB. In Figure 5, the simulated result is in well agreement with the measured result. In Figure 6, the measured result of the proposed LPF provides better rejection characteristics than that of the conventional one whose size is 38.3 Â 25 mm 2 .
CONCLUSIONSA compact LPF for wideband rejection is discussed and its brief design procedure is also described. DSISS and BDGS may yield slow wave effect, which can be resulted in small circuit size, sharp cutoff, and wide band rejection characteristics compared with the conventional LPF using SISS and CDGS. The size reduction of the proposed LPFs is about 23% compared with the conventional LPF. The proposed LPF is obtained in wideband rejection that is below À20 dB from 2.3 to 12 GHz. Photonic microwave filters (PMFs) have attracted a great deal of research interest recently because of their ability to allow the processing of radio frequency signals in the optical domain while maintaining the advantages of wide bandwidth, immunity to electromagnetic interference (EMI), and low loss [1][2][3]. They can be used in a wide range of radar applications and wireless communications. Generally, PMFs have been implemented based on the concept of a digital filter, in which the output is produced by summing the delayed components of the input signal with an individually assigned coefficient. The filter characteristic therefore depends on the number of optical sources being used and the available coefficients. To implement high quality multi-tap filters, then, several optical sources are required, increasing the system cost. For this reason, spectrum-sliced optical sources using the amplified spontaneous emission noise of an erbiumdoped fiber (EDFA) [4] and a broad band super-luminescent LED (SLED) [5] have been implemented to reduce the filter cost. These methods, however, are limited in their tuning range, notch dip, and modulation frequency.In this respect, we propose and experimentally demonstrate a tunable photonic microwave notch filter using a reflective semiconductor optical amplifier (RSOA) together with fiber Bragg gratings (FBGs) with no additional high cost optical source. The RSOA is self-injection locked by the individual grating and acts as a multi-wavelength source. The available wavelength peaks are determined by the gain bandwidth of the ROSA (C band, 30 nm), the optical power necessary for multiple locking, the pass band of the FBGs, and the wavelength spacing between the FBGs [6,7]. The central wavelength of an optical signal can easily be changed by adjusting the Bragg wavelength of the FBGs, which allows changes to the wavelength spacing between optical peaks. In our proposed tunable notch filter, we used a fixed FBG and a tunable FBG (TFBG), making the desired free spectral ranges (FSRs) with the deep notches of more than 35 dB obtainable by adjusting the wavelength spacing.
PRINCIPLE OF THE FILTER OPE...