Planar lightwave circuit high-speed optical modulator capable of shaping signals
A planar lightwave optical path and optical modulator technology, applied in the field of optoelectronics and integrated optics, can solve the problems of high-speed optical signal wavelength drift, time jitter, burst jitter, etc., to improve wavelength drift, improve performance, and reduce burst jitter Effect
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Embodiment 1
[0024] Figure 4 It is the first example of the present invention, consisting of an input channel 4 , an output channel 5 , a directional coupler 7 , an M-Z type optical modulation module 1 with a shaping component 6 and an adjustable optical shaping module 2 . The light wave is input from the input channel 4 and enters the 3dB directional coupler 7. After being divided by power, it enters the M-Z type optical modulation module 1 in two paths. Under the interaction of the high-speed broadband electrical signal and the material on the traveling wave electrode, the lower optical path The refractive index of the M-Z interferometer is changed, and the light wave at the output of the M-Z interferometer is modulated. At the same time, the shaping element in the M-Z optical modulation module performs preliminary shaping of the optical signal. Then, the optical signal enters the directional coupler again through the intermediate transmission channel, and is adjusted under the action ...
Embodiment 2
[0026] Figure 5 It is the second example of the present invention. It adopts single-port input, output, single-strip optical modulator and single ring resonant cavity modulation structure. Figure 6 is The scanning electron microscope photo of the chip, the terminal of the traveling wave electrode is a matching resistor of 50Ω.
[0027] Figure 7 The electrostatic test results of the optical modulator are given, and the optical signal is tested from Figure 6 Display left input. from Figure 7 (a) It can be seen that since the ring resonant cavity is integrated on the modulator, when there is no external electric field, the room-temperature exciton absorption in the MQW and the resonant cavity produce a common effect, which makes the spectrum sink at 1540nm, and a Filter peak; when the voltage is added to 4.2V ( Figure 7 (b)), the position of the absorption depression moves to the right at 1555nm, and two resonant filter peaks appear at 1535nm and 1565nm; when the volt...
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