Thanks to the flat magnitude and phase response of optical devices, it is quite easy to realize broadband signal phase shifting and power manipulating with very small frequen-cy-dependent variations. One example is illustrated in Fig. 4 (c) and (d), showing the frequency responses of a commercial optical 90 hybrid. The power and phase variations are 0.1 dB and 1 over a 6-THz frequency range, which is much better than its electrical counterpart. The excellent amplitude-phase con-sistency would enable wideband noise and interference can-cellation in the optical domain. Previously, coherent cancellation is explicitly or implicitly used in many microwave photonic systems, such as high-linearity analog optical links [141-145], image-reject mixers [10, 146-152], co-site interference cancellation [153-159], and frequency multipliers [160-162] to suppress the noise, undesirable nonlinear components, interference and image frequencies. For example, a linearized analog optical link with the third-order intermodulation distortion (IMD3) component suppressed by 40 dB was built in [142]; an im-age-reject mixer with an image-rejection ratio of 25 dB for a 1.2-GHz instantaneous bandwidth linearly frequen-cy-modulated (LFM) signal was realized in [150] (as a com-parison, the instantaneous bandwidth of an electrical im-age-reject mixer is less than 160 MHz [146]); a 30-dB co-site interference cancellation ratio over 9.5 GHz frequency range was obtained in [156] (while for electrical method the maxi-mum reported bandwidth is only 120 MHz [163]); and an op-tical link with the common-mode noise suppressed by 15 dB over an 18-GHz frequency range was implemented in [164].