Optical up/down-conversion-type optical phase conjugate pair signal transmission/reception circuit
By using optical phase conjugate signal pairs to generate double sideband waves and cancel nonlinear effects in optical fibers in optical radio systems, the problem of signal degradation in optical fibers is solved, simple and effective nonlinear effect compensation is achieved, and signal transmission is improved. linearity and quality.
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Embodiment 1
[0105] Next, the numerical analysis of the above system is carried out. In the following numerical analysis, the homodyne C-RoF system is used for analysis. It is assumed that multi-level signals with subcarriers of radio signals such as QPSK or QAM are transmitted to a distant distance through standard single-mode optical fiber. Figure 17 It is a schematic diagram of the system in the numerical analysis of an Example.
[0106] At the transmitter side of the C-RoF system, ie at the central station side, the continuous light is intensity modulated in a push-pull Mach-Zehnder modulator (MZM) set to zero bias. MZM uses RF signal for modulation as follows. The RF subcarrier signal with a frequency of 10 GHz is data-modulated by the IQ modulator to generate a QPSK signal. The symbol rate of this data is 5GBaud. This device can be used to generate a DSB-SC signal, that is, a C-RoF signal. The OSNR (at 0.1 nm) of the generated RoF signal was 27 dB.
[0107] The RoF signal is t...
Embodiment 2
[0111] Figure 19 It is the experimental structure diagram for the principle verification of the bias offset type electro-optic effect type phase conjugate signal pair generator. Here, through SMF transmission of 20-Gb / sQPSK, the compensation result of the self-phase modulation effect is shown. The transmission of the phase-conjugated signal pair is carried out through the structure of polarization multiplexing. On the transmitter side, the optical coupler branches the continuous light with a wavelength of 1552 nm output from the fiber laser with a line width of 10 kHz, and sends it to two independent quadrature modulators. The quadrature modulators are driven at the same time according to the same I, Q data. The driving signal is an NRZ signal generated by a pulse pattern generator, and is in the form of a waveform length of 215-1PRBS. The secondary Mach-Zehnder modulators of each quadrature modulator are biased at the null point. The main bias voltages are π / 2, -π / 2, res...
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