
浏览全部资源
扫码关注微信
上海大学 特种光纤与光接入网重点实验室,上海 200444
姬迪(1993-),男,河南开封人。硕士,主要研究方向为光生微波光通信系统以及微纳光子芯片测试系统。
叶楠,副教授。E-mail:aslanye@shu.edu.cn
纸质出版日期:2024-04-10,
收稿日期:2023-01-20,
修回日期:2023-02-10,
扫 描 看 全 文
姬迪,胡志涛,王柱天,等. 基于U波段光波产生频率可调谐的微波载波[J].光通信研究,2024(2):220054.
Ji D, Hu Z T, Wang Z T, et al. Generation of Frequency-tunable Microwave Carriers based on the U-band Lightwave Carrier[J]. Study on Optical Communications, 2024(2):220054.
姬迪,胡志涛,王柱天,等. 基于U波段光波产生频率可调谐的微波载波[J].光通信研究,2024(2):220054. DOI: 10.13756/j.gtxyj.2024.220054.
Ji D, Hu Z T, Wang Z T, et al. Generation of Frequency-tunable Microwave Carriers based on the U-band Lightwave Carrier[J]. Study on Optical Communications, 2024(2):220054. DOI: 10.13756/j.gtxyj.2024.220054.
【目的】
2
具有可调谐能力的高频微波载波(GHz)在第五代移动通信技术(5G)/第六代移动通信技术(6G)无线网络、雷达系统和卫星通信领域中有着广泛的应用。由于比较简单的系统结构、大带宽和低损耗的优点,基于光子技术生成高频可调谐微波载波的技术方案吸引了国内外研究团队的广泛关注。由于目前C波段有着成熟的商用器件,因此目前光生微波实验多在C波段进行。随着波分复用(WDM)—光载射频(ROF)技术借助WDM系统在光频域的合/分波来灵活实现微波频段的合/分波,利用ROF系统采用光生微波技术来简化基站配置,使得C波段的有限带宽资源(35 nm,1 530~1 565 nm)越来越紧张。因此,光生微波技术的研究有着向更宽光谱范围扩展的驱动力。U波段可以提供宽至50 nm(1 625~1 675 nm)的信道带宽来缓解C波段的信道利用压力。在U波段,标准单模光纤已实现低至0.195 dB/km(@1 625 nm)的光功率损耗,特别是,掺铥光纤放大器在U波段也可实现达到18.7 dB(@1 655 nm)的大带宽增益。因此,基于标准单模光纤的WDM系统可向U波段扩展,从而促使WDM-ROF技术向这一波段延伸,进而带动光生微波技术向U波段拓展。文章研究了U波段的光生微波技术。
【方法】
2
从数学模型上看,现有光生微波技术对所应用的光载波波段是透明的,只需选择对应工作波段的光子学器件就可在任意波段使用这些方法来产生微波载波。从原理上看,C波段的光子学器件(如偏振控制器、相位调制器(PM)和光纤移相器(FPS)等)可以工作在U波段,这些器件的工艺技术成熟并易于购置。因此,文章采用C波段的PM、FPS和光耦合器等光子学器件,基于U波段光载波搭建了光生微波载波系统。
【结果】
2
最终基于该系统产生了调谐范围覆盖7.5~12.0 GHz、杂散抑制比达29.6~35.2 dB的可调谐微波载波。
【结论】
2
文章通过公式原理分析和实验验证,实现了将光生微波载波技术的工作波段扩展至U波段。
【Objective】
2
High-frequency microwave carriers (GHz) with tunable capability have a wide range of applications in 5th Generation Mobile Communication Technology (5G)/ 6th Generation Mobile Communication Technology (6G) wireless networks
radar systems
and satellite communications. Due to the relatively simple structure of the system
the large bandwidth and the low loss
the technical scheme of generating high-frequency tunable microwave carriers based on photonic technology has attracted extensive attention from domestic and international research teams. Current photogenerated microwave experiments are mostly conducted in C-band wavelengths because of the mature commercial devices. Meanwhile
the Wavelength Division Multiplexing (WDM)-Radio Over Fiber (ROF) technology integrates the WDM technology with the ROF technology so as to flexibly realize the combining/splitting of microwave bands with the help of the combining/splitting of WDM system in the optical frequency domain. The ROF part of the system employs photogenerated microwave technology to simplify the base station configuration. Constrained by the limited bandwidth resources in the C-band wavelengths(35 nm
1 530~1 565 nm)
there is a drive for the generation of microwave to expand to wider spectral ranges. The U-band wavelengths can also provide channel bandwidths as wide as 50 nm (1 625~1 675 nm) to alleviate the channel utilization pressure in the C-band wavelengths; In the U-band wavelengths
Standard Single Mode Fibers(SSMFs) have achieved optical power loss as low as 0.195 dB/km (@1 625 nm); In particular
thulium-doped fiber amplifiers have also demonstrated a large bandwidth gain of 18.7 dB (@1 655 nm). These advantages attract SSMFs-based WDM systems to expand into the U-band
which leads to the extension of WDM-ROF technology into long wavelengths
and in turn leads to the expansion of photogenerated microwave technology. Therefore
this paper studies the photogenerated microwave technology in the U-band.
【Methods】
2
From the mathematical model
the commonly used photogenerated microwave carriers technologies are transparent to the applied optical carrier bands
and can be used to generate microwave carriers at arbitrary bands by selecting photonics devices corresponding to the operating bands. In principle
C-band wavelengths photonics devices (such as polarization controllers
Phase Modulator (PM)
Fiber Phase Shifter (FPS)
etc.) can work in the U-band
and the process technology of these devices is mature. Therefore
in this paper
photonics devices such as C-band wavelengths PM
FPS and optocouplers are used to build a photogenerated microwave carrier system based on U-band optical carriers.
【Results】
2
Finally
tunable microwave carrier with a tuning range of 7.5~12.0 GHz and a spurious rejection ratio of 29.6~35.2 dB is ultimately generated based on this system.
【Conclusion】
2
Through formula principle analysis and experimental verification
this paper extends the working band wavelengths of the photogenerated microwave carrier to the U-band wavelengths.
光生微波载波U波段光相位调制器强度调制频率可调谐杂散抑制比
photogenerated microwave carrierU-bandoptical PMintensity modulationfrequency-tunablespurious suppression ratio
Zhang F, Pan S. Microwave Photonic Signal Generation for Radar Applications [C]//2016 IEEE International Workshop on Electromagnetics: Applications and Student Innovation Competition (iWEM). Nanjing, China: IEEE, 2016: 7504991.
Serafino G, Maresca S, Porzi C, et al.Microwave Photonics for Remote Sensing: from Basic Concepts to High-level Functionalities [J]. Journal of Lightwave Technology, 2020, 38(19): 5339-5355.
Liu J Q, Lucas E, Raja A S, et al. Photonic Microwave Generation in the X- and K-band Using Integrated Soliton Microcombs [J]. Nature Photonics, 2020, 14(8): 486-491.
Yao J P. Microwave Photonics [J]. Journal of Lightwave Technology, 2009, 27(3): 314-335.
Lim C, Tian Y, Ranaweera C, et al. Evolution of Radio-over-fiber Technology [J]. Journal of Lightwave Technology, 2019, 37(6): 1647-1656.
Wang Y X, Hou X Y, Li T, et al. Simultaneous Detection of the Distance and Direction for a Noncooperative Target based on the Microwave Photonic Radar [J]. Optics Express, 2021, 29(20): 31561-31573.
Meena D, Harshitha B S, Kavyashree B K.Direct Generation of RF Signals Using Photonic Heterodyne Method for Radar Applications [C]//2019 URSI Asia-Pacific Radio Science Conference (URSI AP-RASC). New Delhi, India: IEEE, 2019: 1-4.
Xüe C P, Ji S K, Hong Y H, et al. Numerical Investigation of Photonic Microwave Generation in an Optically Injected Semiconductor Laser Subject to Filtered Optical Feedback [J]. Optics Express, 2019, 27(4): 5065-5082.
Balakier K, Fice M J, Ponnampalam L, et al. Foundry Fabricated Photonic Integrated Circuit Optical Phase Lock Loop [J]. Optics Express, 2017, 25(15): 16888-16897.
Jia Q S, Zhang P, Wang T S, et al. 40 GHz Narrow Linewidth Frequency-switched Microwave Signal Generation based on a Single-longitudinal-mode Double-Brillouin-frequency Spaced Brillouin Fiber Laser [J]. Applied Optics, 2017, 56(19): 5323-5328.
Chen H, Ning T, Li J, et al. Optical Millimeter-wave Generation with Tunable Multiplication Factors and Reduced Power Fluctuation by Using Cascaded Modulators [J]. Optics and Laser Technology, 2018, 103: 206-211.
Zhang W, Yao J. Silicon Photonic Integrated Optoelectronic Oscillator for Frequency-tunable Microwave Generation [J]. Journal of Lightwave Technology, 2018, 36(19): 4655-4663.
Zhang C, Ning T, Li J, et al. A Full-duplex WDM-RoF System based on Tunable Optical Frequency Comb Generator [J]. Optics Communications, 2015, 344: 65-70.
Liu Y, Gao H, Chen Y, et al. Full-duplex WDM-RoF System based on OFC with Dual Frequency Microwave Signal Generation and Wavelength Reuse [J]. Optical Fiber Technology, 2020, 58(8): 102252.
贺作为, 陈伟, 张良, 等.高速传输系统用低损耗单模光纤的研究[J].光通信研究, 2015(2): 35-38.
He Z W, Chen W, Zhang L, et al. Study on Low-loss Single-mode Optical Fibers for High-rate Transmission Systems [J]. Study on Optical Communications, 2015(2): 35-38.
Chen S, Jung Y, Alam S U, et al. Ultra-short Wavelength Operation of Thulium-doped Fibre Amplifier in the 1 628-1 655 nm Waveband [C]//2018 European Conference on Optical Communication (ECOC). Rome, Italy: IEEE, 2018: 8535134.
0
浏览量
0
下载量
0
CSCD
关联资源
相关文章
相关作者
相关机构
鄂公网安备 42011202002092号