[0006]
At present, the
photon microwave scheme that uses this type of
optical microcavity to generate
microwave signals, the main problem is that the size of the
optical microcavity such as F-P cavity is large, it is not easy to integrate, and the cavity mirror with
high reflectivity is expensive and requires high
assembly requirements; while
magnesium fluoride, silicon
Whispering gallery mode resonators of base and other
dielectric materials also have
processing difficulties, and the precision requirements of
processing equipment are particularly high. In addition, there are difficulties in optical
assembly and debugging, and complex production processes. This type of photonic
microwave technology produces high-quality microwave signal output. , in order to improve the stability of the
system, it is necessary to perform reverse self-
injection locking on the DFB laser, which requires special optical mode field and
phase matching for the reflected light of the
resonator, which leads to complex debugging and
assembly processes, which seriously increase the technical solutions of this type. The difficulty of large-scale application
[0007]
With the development of silicon-based integrated
photonics in recent years, the design of micro-ring cavity based on
silicon nitride waveguide has attracted more and more attention, and the Kerr nonlinear effect of the micro-ring cavity based on
silicon nitride through-ring
waveguide A lot of research has been done, and there is also a related plan based on
silicon nitride microring cavity to excite Kerr optical
frequency comb to generate 10GHz microwave signal after beat frequency, but there are still major technical problems, such as the need for high-power communication band The laser signal is pumped and excited, and the high-power DFB laser has poor
noise performance. The output
optical noise performance of the pump laser will have a direct
impact on the final beat-frequency microwave signal, making it difficult for the
system to obtain a microwave signal output with better
phase noise performance. ; Furthermore, in the process of outputting solitons based on the
Kerr effect of the silicon nitride microring cavity, the pump laser needs to be detuned. The ring cavity is actually in a thermally unstable state, and the system cannot obtain a relatively stable long-term working state
[0008]
For this reason, some have proposed a laser-assisted heating scheme. In addition to pumping the pump laser that generates the Kerr optical
frequency comb, an auxiliary laser is added, and the pump laser is injected into the microring cavity in the opposite direction of the transmission direction. In the micro-ring cavity, through the precise control of the red detuning
wavelength position of the pump laser and the blue detuning wavelength position of the auxiliary laser, the control and adjustment of the
thermal balance of the micro-ring cavity in the single
soliton state of the Kerr optical frequency comb is realized. Avoid the
thermal instability in the single
soliton state of the Kerr optical frequency comb, so as to realize the stable long-term operation of the silicon nitride microring cavity in the single
soliton state of the Kerr optical frequency comb, but add a laser to inject the laser into the microring cavity for
auxiliary heating Finally, the system needs to have two lasers for real-
time control at the same time, which increases the difficulty of system control and system complexity. Therefore, there are no reports about the practical application of this scheme.
[0009]
According to the latest research report, based on the
fiber microcavity, the Brillouin laser is generated by pump laser injection excitation. The Brillouin laser has ultra-narrow linewidth and very
low noise. The Brillouin laser is used as the pump light pair The microcavity is excited to generate a Kerr optical frequency comb. The
advantage of this scheme is that the Brillouin laser is used to pump and excite the Kerr optical frequency comb, which avoids the high
noise level caused by the initial high-power laser pump injection. It is a great progress for photonic
microwave technology, but the scheme uses
fiber F-P microcavity technology, by pressurizing the
fiber F-P microcavity outside to adjust the stress inside the fiber material, and realize the microcavity
resonance frequency parameter The adjustment of the
optical fiber microcavity in this scheme is sensitive to external stress, the
system stability is not high, and the parameter adjustment process is complicated