Abstract:We propose a novel scheme to generate ultrawideband (UWB) monocycle pulses based on cross-phase modulation (XPM) of a semiconductor optical amplifier (SOA). The proposed system consists of a SOA and an optical bandpass filter (OBF). Due to the XPM, a continuous wave (CW) probe signal is phase modulated by another optical Gauss pulse in the SOA. The OBF will convert the phase modulation to intensity modulation. A pair of polarity-reversed UWB monocycle pulses is achieved by locating the probe carrier at the pos… Show more
“…UWB signal generation in the optical domain is recently developed rapidly, because of the low loss over long-distance transmission in the optical fiber. Many electro-optical methods [3][4][5][6] and all-optical methods [7][8][9] have been proposed. Particularly, an optically switchable and tunable scheme has been demonstrated using the semiconductor optical amplifier (SOA) and single-mode fiber (SMF), but a long span of optical fiber should be used [10].…”
An all-optical ultrawideband monocycle generator based on wavelength conversion in a semiconductor optical amplifier (SOA) and optical tunable delay in an optical delay line (ODL) is proposed and simulated. The system achieves optically switchable in pulse polarity and tunable in both the pulsewidth and radio frequency (RF) spectrum.
“…UWB signal generation in the optical domain is recently developed rapidly, because of the low loss over long-distance transmission in the optical fiber. Many electro-optical methods [3][4][5][6] and all-optical methods [7][8][9] have been proposed. Particularly, an optically switchable and tunable scheme has been demonstrated using the semiconductor optical amplifier (SOA) and single-mode fiber (SMF), but a long span of optical fiber should be used [10].…”
An all-optical ultrawideband monocycle generator based on wavelength conversion in a semiconductor optical amplifier (SOA) and optical tunable delay in an optical delay line (ODL) is proposed and simulated. The system achieves optically switchable in pulse polarity and tunable in both the pulsewidth and radio frequency (RF) spectrum.
“…The Federal Communications Commission (FCC) defined the UWB signal as a radio frequency (RF) signal that occupies a spectral bandwidth of more than 500 MHz or more than 20% fractional bandwidth with a power density no more than −41.3 dBm∕MHz [2] . Up to now, various approaches have been proposed to generate UWB signals in the centimeter-wave (CMW) band (3.1 to 10.6 GHz) for indoor communications [3][4][5][6][7] and in the millimeter-wave (MMW) band (22 to 29 GHz) for outdoor communications [8][9][10][11][12][13][14][15][16][17][18][19] . In this Review, we review recent progress on the photonic generation of UWB signals in the MMW band with emphasis on the generation of background-free and FCC compliant MMW-UWB pulses.…”
We review the recent progress of photonic generation of millimeter wave (MMW)-ultra-wideband (UWB) signals. To fully satisfy the standard defined by the Federal Communications Commission (FCC), the baseband signal (background signal) and the residual local oscillator (LO) signal should be well controlled. We discuss several schemes in this work for generating background-free MMW-UWB signals that are fully compliant with the FCC requirement.
“…The same group also obtained UWB pulses by synthesizing a bandpass coherent microwave filter by combining an electro-optic phase modulator (EOPM) with fiber dispersion [6], acting globally as an electronic differentiator at low frequencies but implemented in the optical domain. More recently, some reported optical UWB signal generation approaches take advantage of the nonlinear optical properties of semiconductor optical amplifiers (SOAs) [7][8][9]. By exploiting cross-gain modulation [7], the output light of the SOA consisted of two reversed polarized pulses.…”
Optical pulses generated by current modulation of semiconductor lasers are strongly frequency chirped. This effect has been considered pernicious for optical communications. We take advantage of this effect for the generation of ultrawideband microwave signals by using an optical filter to achieve chirp-to-intensity conversion. We also experimentally achieve propagation through a 20 km nonzero dispersion shifted fiber with no degradation of the signal at the receiver. Our method constitutes a prospective low-cost solution and offers integration capabilities with fiber-to-the-customer-premise systems.
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