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CN115603818A - Digital self-interference elimination device and method for optical frequency conversion and reference signal return - Google Patents

Digital self-interference elimination device and method for optical frequency conversion and reference signal return Download PDF

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CN115603818A
CN115603818A CN202211224421.3A CN202211224421A CN115603818A CN 115603818 A CN115603818 A CN 115603818A CN 202211224421 A CN202211224421 A CN 202211224421A CN 115603818 A CN115603818 A CN 115603818A
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optical
self
interference
polarization
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高从芮
朱子行
赵尚弘
李轩
李�赫
孟晴晴
王国栋
周逸潇
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Air Force Engineering University of PLA
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    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B10/00Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
    • H04B10/25Arrangements specific to fibre transmission
    • H04B10/2575Radio-over-fibre, e.g. radio frequency signal modulated onto an optical carrier
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B10/00Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
    • H04B10/50Transmitters
    • H04B10/501Structural aspects
    • H04B10/503Laser transmitters
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B10/00Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
    • H04B10/50Transmitters
    • H04B10/516Details of coding or modulation
    • H04B10/548Phase or frequency modulation
    • H04B10/556Digital modulation, e.g. differential phase shift keying [DPSK] or frequency shift keying [FSK]
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B10/00Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
    • H04B10/60Receivers
    • H04B10/61Coherent receivers
    • H04B10/616Details of the electronic signal processing in coherent optical receivers
    • H04B10/6162Compensation of polarization related effects, e.g., PMD, PDL
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B10/00Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
    • H04B10/60Receivers
    • H04B10/66Non-coherent receivers, e.g. using direct detection
    • H04B10/69Electrical arrangements in the receiver
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Abstract

The digital self-interference elimination device comprises a signal source (1) positioned at a base station A, an electric amplifier (2), a first electric power divider A (3), a transmitting antenna (4), a receiving antenna (5), a local vibration source (6), a second electric power divider B (7), a laser (8), a polarization controller (9) and a dual-polarization dual-drive Mach-Zehnder modulator (10); a single-mode optical fiber (15); an erbium-doped fiber amplifier (16), a polarization beam splitter (17), a first photoelectric detector A (18), a second photoelectric detector B (19) and a digital signal processor DSP (20) which are positioned at the central station B. The method for eliminating the digital self-interference under the condition of optical frequency conversion and reference signal simultaneous return in the in-band full-duplex ROF system is also provided. The invention converts the nonlinear problem into the linear problem for processing, thereby reducing the processing difficulty of the digital domain; the digital domain processing is carried out by using a high-digit ADC without realizing parameter tuning on an optical domain; the operation speed of the algorithm is greatly improved by using FTRLS multiplication.

Description

光学变频、参考信号回传的数字自干扰消除装置及方法Digital self-interference elimination device and method for optical frequency conversion and reference signal return

技术领域technical field

本发明属于微波光子信号处理技术领域,具体涉及一种带内全双工ROF系统下光学变频、参考信号同时回传的数字自干扰消除装置及方法。The invention belongs to the technical field of microwave photon signal processing, and in particular relates to a digital self-interference elimination device and method for optical frequency conversion and simultaneous return of reference signals under an in-band full-duplex ROF system.

背景技术Background technique

光载无线射频系统(RoF)是应高速大容量无线通信需求,新兴发展起来的将光子技术和无线通信结合起来的无线接入技术。光纤具有低损耗、高带宽和防止电磁干扰的特点,作为传输链路使得RoF技术在未来无线宽带通信、卫星通信以及智能交通系统等领域有着广阔的应用前景。面对当前日益紧张的频谱资源,带内全双工ROF系统能够保证基站在相同频段接收来自移动用户的上行信号同时发送下行信号,在提高信息吞吐量的同时倍增了频谱效率。Radio Frequency over Fiber (RoF) is a newly developed wireless access technology that combines photonic technology and wireless communication to meet the needs of high-speed and large-capacity wireless communication. Optical fiber has the characteristics of low loss, high bandwidth and anti-electromagnetic interference. As a transmission link, RoF technology has broad application prospects in the fields of wireless broadband communication, satellite communication, and intelligent transportation systems in the future. Faced with the current increasingly tight spectrum resources, the in-band full-duplex ROF system can ensure that the base station receives uplink signals from mobile users and sends downlink signals at the same time in the same frequency band, which improves the information throughput and doubles the spectrum efficiency.

在带内全双工ROF系统中,发射和接收信道之间的自干扰是当前亟需解决的问题,单纯光域自干扰消除方案在处理多径、非线性等问题上受到限制,而与数字算法的有效结合为实现高频段、大带宽、低损耗的自干扰消除提供了强有力的支撑。In the in-band full-duplex ROF system, the self-interference between the transmit and receive channels is an urgent problem to be solved at present. The pure optical domain self-interference cancellation scheme is limited in dealing with multipath, nonlinear and other issues, and the digital The effective combination of algorithms provides a strong support for self-interference cancellation with high frequency band, large bandwidth and low loss.

近几年,微波光子结合数字算法实现自干扰消除受到国内外科研机构的广泛研究,其中,重点针对非线性和多径效应的微波光子模拟域和非线性自适应滤波数字域的联合自干扰消除方案(1、Xiaolei,Yucheng,Zhang,et al.Optimized self-interferencecancellation based on optical dual-parallel MZM for co-frequency and co-timefull duplex wireless communication under nonlinear distortion and emulatedmultipath effect[J].Optics express,2019,27(26):37286-37297)。光载无线毫米波传输系统下基于深度学习算法的自干扰消除同时恢复有用信号的自干扰消除方案(2、ZhouQ,Shen S,Chen Y W,et al.Simultaneous nonlinear self-interference cancellationand signal of interest recovery using dual input deep neural network in newradio access networks[J].Journal of Lightwave Technology,2020,39(7):2046-2051.:1297-1300)。文献(3、Zheng L,Liu Z,Xiao S,et al.Hybrid wideband multipathself-interference cancellation with an LMS pre-adaptive filter for in-bandfull-duplex OFDM signal transmission[J].Optics Letters,2020,45(23):6382)将LMS作为预滤波器以匹配无线多径自干扰信号,并在光域上实现消除。文献(4、Han M,Shi T,Chen Y.Digital-assisted photonic analog wideband multipath self-interferencecancellation[J].IEEE Photonics Technology Letters,2022)将RLS作为预滤波器以匹配弱多径残余自干扰信号,与主径参考信号合成后,在光域上实现自干扰消除以及频率下变频。In recent years, microwave photons combined with digital algorithms to achieve self-interference cancellation has been widely studied by domestic and foreign scientific research institutions. Among them, the focus is on the joint self-interference cancellation of microwave photon analog domain and nonlinear adaptive filtering digital domain for nonlinear and multipath effects. Scheme (1. Xiaolei, Yucheng, Zhang, et al. Optimized self-interference cancellation based on optical dual-parallel MZM for co-frequency and co-timefull duplex wireless communication under nonlinear distortion and emulated multipath effect[J]. Optics express, 2019, 27(26):37286-37297). Self-interference cancellation and signal of interest recovery using self-interference cancellation based on deep learning algorithm in wireless millimeter wave transmission system over optical fiber (2, ZhouQ, Shen S, Chen Y W, et al.Simultaneous nonlinear self-interference cancellation and signal of interest recovery using dual input deep neural network in new radio access networks [J]. Journal of Lightwave Technology, 2020, 39(7): 2046-2051.: 1297-1300). Literature (3, Zheng L, Liu Z, Xiao S, et al. Hybrid wideband multipath self-interference cancellation with an LMS pre-adaptive filter for in-bandfull-duplex OFDM signal transmission[J]. Optics Letters, 2020, 45(23 ): 6382) LMS is used as a pre-filter to match wireless multi-path self-interference signals, and eliminate them in the optical domain. Literature (4, Han M, Shi T, Chen Y. Digital-assisted photonic analog wideband multipath self-interference cancellation [J]. IEEE Photonics Technology Letters, 2022) uses RLS as a pre-filter to match weak multipath residual self-interference signals, After being synthesized with the main path reference signal, self-interference elimination and frequency down-conversion are realized in the optical domain.

然而,上述方案存在一定的局限性。文献1没有考虑光纤传输以及下变频,且当残余自干扰信号非线性成分较强时,非线性自适应滤波算法RLS-Vollterra复杂度较高;文献2当自干扰信号与有用信号功率相差较大时,自干扰消除深度和有用信号的恢复能力受到限制;文献3、文献4均采用电延时线进行延时的精确匹配,电学调谐器件对于宽带信号来说不平坦频率响应会对算法性能造成影响,且涉及到高频的预匹配方案需要采用高性能的任意波形发生器。However, the above scheme has certain limitations. Document 1 does not consider optical fiber transmission and down-conversion, and when the nonlinear component of the residual self-interference signal is strong, the complexity of the nonlinear adaptive filtering algorithm RLS-Vollterra is high; Document 2 when the power difference between the self-interference signal and the useful signal is large , the self-interference cancellation depth and the recovery ability of useful signals are limited; Documents 3 and 4 both use electrical delay lines for precise delay matching, and the uneven frequency response of electrical tuning devices for broadband signals will have a negative impact on algorithm performance. Influence, and the high-frequency pre-matching scheme needs to use a high-performance arbitrary waveform generator.

发明内容Contents of the invention

针对现有技术存在的问题,本发明提供一种带内全双工ROF系统下光学变频、参考信号同时回传的数字自干扰消除装置,包括位于基站A处的信号源1、电放大器2、第一电功分器A3、发射天线4、接收天线5、本振源6、第二电第二电功分器B7、激光器8、偏振控制器9、双偏振双驱动马赫曾德尔调制器10;单模光纤15;位于中心站B处的掺饵光纤放大器16、偏振分束器17、第一光电探测器A18、第二光电探测器B19、数字信号处理器DSP 20;其中,双偏振双驱动马赫曾德尔调制器10含第一双驱动马赫曾德尔调制器A11、第二双驱动马赫曾德尔调制器B12、90度偏振旋转器13、偏振合束器14;Aiming at the problems existing in the prior art, the present invention provides a digital self-interference cancellation device for optical frequency conversion and simultaneous return of reference signals in an in-band full-duplex ROF system, including a signal source 1 located at a base station A, an electrical amplifier 2, First electric power divider A3, transmitting antenna 4, receiving antenna 5, local oscillator source 6, second electric second electric power divider B7, laser 8, polarization controller 9, dual polarization dual drive Mach-Zehnder modulator 10 ; Single-mode optical fiber 15; Erbium-doped fiber amplifier 16, polarization beam splitter 17, first photodetector A18, second photodetector B19, digital signal processor DSP 20 located at central station B place; The driving Mach-Zehnder modulator 10 includes a first dual-driving Mach-Zehnder modulator A11, a second dual-driving Mach-Zehnder modulator B12, a 90-degree polarization rotator 13, and a polarization beam combiner 14;

在基站A处:At base station A:

激光器8产生的光载波经偏振控制器9输入至双偏振双驱动马赫曾德尔调制器10;The optical carrier generated by the laser 8 is input to the dual-polarization dual-drive Mach-Zehnder modulator 10 through the polarization controller 9;

本振源6产生本振信号输出给第二电第二电功分器B7,第二电第二电功分器B7对本振信号④进行功率分配,一路输出至第一双驱动马赫曾德尔调制器A11,另一路输出至第二双驱动马赫曾德尔调制器B12;The local oscillator source 6 generates a local oscillator signal and outputs it to the second electric second electric power divider B7, and the second electric second electric power divider B7 performs power distribution on the local oscillator signal ④, and one output to the first dual-drive Mach-Zehnder modulation A11, another output to the second dual-drive Mach-Zehnder modulator B12;

信号源1产生的载波调制信号经电放大器2放大后输出给第一电功分器A3,第一电功分器A3对其进行功率分配,其中一路输出作为参考信号②与本振源6经第二电功分器B7产生的一路本振信号④均输入至第一双驱动马赫曾德尔调制器A11进行电光调制,产生X偏振态光信号Ex;另一路输出至发射天线4并由其发出;The carrier modulation signal generated by the signal source 1 is amplified by the electric amplifier 2 and then output to the first electric power divider A3, and the first electric power divider A3 performs power distribution on it, and one of the outputs is used as a reference signal ② and the local oscillator source 6 via One local oscillator signal ④ generated by the second electric power splitter B7 is input to the first dual-drive Mach-Zehnder modulator A11 for electro-optic modulation to generate X polarization state optical signal E x ; the other is output to the transmitting antenna 4 and then issue;

经多径自干扰信道传输的自干扰信号①与远端有用信号③一同被接收天线5接收,形成混合信号,之后,混合信号与本振源6经第二电功分器B7产生的另一路本振信号④都输入至第二双驱动马赫曾德尔调制器B12进行电光调制,所产生的X偏振态光信号经90度偏振旋转器13后改变偏振态后输出;The self-interference signal ① transmitted through the multi-path self-interference channel and the remote useful signal ③ are received by the receiving antenna 5 to form a mixed signal. After that, the mixed signal and the local vibration source 6 are generated by the second electric power splitter B7. All vibration signals ④ are input to the second dual-drive Mach-Zehnder modulator B12 for electro-optical modulation, and the generated X polarization state optical signal passes through the 90-degree polarization rotator 13 and then outputs after changing the polarization state;

第一双驱动马赫曾德尔调制器A11输出的光载波调制信号、90度偏振旋转器13输出的光载波调制信号,这两路不同偏振态的信号在偏振合束器14处合束,形成偏振合束光信号;偏振合束光信号经单模光纤15传输至中心站B;The optical carrier modulation signal output by the first dual-drive Mach-Zehnder modulator A11 and the optical carrier modulation signal output by the 90-degree polarization rotator 13, the two signals of different polarization states are combined at the polarization beam combiner 14 to form a polarization beam combining optical signal; the polarized beam combining optical signal is transmitted to the central station B through the single-mode optical fiber 15;

在中心站B处:At central station B:

经掺饵光纤放大器16放大后,通过偏振分束器17分束,分别输出到第一光电探测器A18、第二光电探测器B19,在第一光电探测器A18处经拍频后得到经过光学变频的中频参考信号,在第二光电探测器B19处经拍频后得到经过光学变频的中频接收信号,中频参考信号和中频接收信号均输入至数字信号处理器DSP 20中进行数字信号处理。After being amplified by the erbium-doped fiber amplifier 16, the beam is split by the polarization beam splitter 17, and output to the first photodetector A18 and the second photodetector B19 respectively, and obtained after being beat at the first photodetector A18. The frequency-converted intermediate-frequency reference signal is beaten at the second photodetector B19 to obtain an optically-converted intermediate-frequency received signal, and both the intermediate-frequency reference signal and the intermediate-frequency received signal are input to the digital signal processor DSP 20 for digital signal processing.

还提供一种带内全双工ROF系统下光学变频、参考信号同时回传的数字自干扰消除方法,其基于如权利要求1所述的带内全双工ROF系统下光学变频、参考信号同时回传的数字自干扰消除装置,假定自干扰信号①为

Figure BSA0000285872440000041
参考信号②为
Figure BSA0000285872440000042
有用信号③为
Figure BSA0000285872440000043
本振信号④为It also provides a digital self-interference elimination method for optical frequency conversion and reference signal simultaneous return under the in-band full-duplex ROF system, which is based on the optical frequency conversion under the in-band full-duplex ROF system as claimed in claim 1, and the reference signal is simultaneously The backhaul digital self-interference cancellation device assumes that the self-interference signal ① is
Figure BSA0000285872440000041
The reference signal ② is
Figure BSA0000285872440000042
The useful signal ③ is
Figure BSA0000285872440000043
The local oscillator signal ④ is

Figure BSA0000285872440000044
其中VSI、VR、VSOI、VLO分别为自干扰信号①、本地参考信号②、有用信号③、本振信号④的电压,ωSI、ωR、ωSOI、ωLO分别为自干扰信号①、本地参考信号②、有用信号③、本振信号④的角频率,
Figure BSA0000285872440000045
分别为自干扰信号①、本地参考信号②、有用信号③、本振信号④的相位;
Figure BSA0000285872440000044
Among them, V SI , VR , V SOI , and V LO are voltages of self-interference signal ①, local reference signal ②, useful signal ③, and local oscillator signalrespectively , and ω SI , ω R , ω SOI , and ω LO are self-interference Angular frequency of signal ①, local reference signal ②, useful signal ③, local oscillator signal ④,
Figure BSA0000285872440000045
are the phases of self-interference signal ①, local reference signal ②, useful signal ③, and local oscillator signal ④;

该方法具体包括下列步骤:The method specifically includes the following steps:

在基站A处:At base station A:

步骤1:信号源1产生的载波调制信号经电放大器2放大后输出给第一电功分器A3,第一电功分器A3对其进行功率分配,其中一路输出为参考信号②;另一路经多径自干扰信道传输后形成的自干扰信号①与远端有用信号③一同被接收天线5接收,形成混合信号(①+③);Step 1: The carrier modulation signal generated by the signal source 1 is amplified by the electric amplifier 2 and then output to the first electric power divider A3, and the first electric power divider A3 performs power distribution on it, one of which outputs the reference signal ②; the other one The self-interference signal ① formed after being transmitted through the multi-path self-interference channel is received by the receiving antenna 5 together with the remote useful signal ③ to form a mixed signal (①+③);

步骤2:激光器8产生光载波经偏振控制器9产生线偏振光,线偏振光输入至双偏振双驱动马赫曾德尔调制器10;Step 2: The laser 8 generates an optical carrier and the polarization controller 9 generates linearly polarized light, and the linearly polarized light is input to the dual-polarized dual-drive Mach-Zehnder modulator 10;

参考信号②与本振源6经第二电第二电功分器B7产生的一路本振信号④均输入至第一双驱动马赫曾德尔调制器A11进行电光调制,将第一双驱动马赫曾德尔调制器A11设为最小偏置点,输出X偏振态光信号Ex;第一电功分器A3的另一路输出至发射天线4并由其发出;The reference signal ② and the local oscillator signal ④ generated by the local oscillator source 6 via the second electric power divider B7 are both input to the first dual-drive Mach-Zehnder modulator A11 for electro-optical modulation, and the first dual-drive Mach-Zehnder The Del modulator A11 is set to the minimum bias point, and outputs the X polarization state optical signal E x ; the other output of the first electric power divider A3 is sent to the transmitting antenna 4 and sent by it;

混合信号(①+③)与本振源6经第二电功分器B7产生的另一路本振信号④都输入至第二双驱动马赫曾德尔调制器B12进行电光调制,同样将第二双驱动马赫曾德尔调制器B12设为最小偏置点,第二双驱动马赫曾德尔调制器B12输出的X偏振态光信号,该信号经90度偏振旋转器13旋转为Y偏振态光信号EyThe mixed signal (①+③) and another local oscillator signal ④ produced by the local oscillator source 6 through the second electric power divider B7 are all input to the second dual-drive Mach-Zehnder modulator B12 for electro-optical modulation, and the second dual The driving Mach-Zehnder modulator B12 is set to the minimum bias point, and the X polarization state optical signal output by the second dual driving Mach-Zehnder modulator B12 is rotated by the 90-degree polarization rotator 13 into a Y polarization state optical signal E y ;

这两路不同偏振态的信号Ex、Ey在偏振合束器14处合束,形成偏振光信号,偏振光信号包络E1(t)如公式1所示:These two signals E x and E y of different polarization states are combined at the polarization beam combiner 14 to form a polarized light signal. The envelope E 1 (t) of the polarized light signal is shown in Formula 1:

Figure BSA0000285872440000051
Figure BSA0000285872440000051

其中,

Figure BSA0000285872440000052
为光载波,Ec为光载波的幅度,ωc为输入光载波频率,mSI=πVSI/Vπ、mR=πVR/Vπ、mSOI=πVSOI/Vπ、mLO=πVLO/Vπ分别为自干扰信号①、参考信号②、有用信号③、本振信号④的调制系数,Vπ为双偏振双驱动马赫曾德尔调制器10的半波电压,J0()、J1()分别为0阶、1阶一类贝塞尔函数,t为时间;in,
Figure BSA0000285872440000052
is the optical carrier, E c is the amplitude of the optical carrier, ω c is the input optical carrier frequency, m SI =πV SI /V π , m R =πV R /V π , m SOI =πV SOI /V π , m LO = πV LO /V π are the modulation coefficients of the self-interference signal ①, reference signal ②, useful signal ③, and local oscillator signal ④ respectively, V π is the half-wave voltage of the dual-polarization dual-drive Mach-Zehnder modulator 10, J 0 () , J 1 () are a class of Bessel functions of order 0 and order 1 respectively, and t is time;

步骤3:合束信号经单模光纤15传输至中心站B;由于光纤的色散效应,光纤的传输函数为H(ω)=exp(-αL/2+jβ2L(ω-ωc)2/2),其中α为衰减常量,β2为群速度色散参量,L为光纤长度;因此信号经过单模光纤15后输出的光信号包络ESMF(t)如公式2所示:Step 3: The bundled signal is transmitted to the central station B through the single-mode optical fiber 15; due to the dispersion effect of the optical fiber, the transmission function of the optical fiber is H(ω)=exp(-αL/2+jβ 2 L(ω-ω c ) 2 /2), wherein α is an attenuation constant, β 2 is a group velocity dispersion parameter, and L is an optical fiber length; therefore, the signal envelope E SMF (t) of the output optical signal after passing through the single-mode optical fiber 15 is as shown in formula 2:

Figure BSA0000285872440000061
Figure BSA0000285872440000061

其中,ESMFx、ESMFy分别为Ex、Ey经单模光纤15传输后得到不同的偏振态光信号;Wherein, E SMFx and E SMFy are respectively E x and E y obtained after transmission through the single-mode optical fiber 15 to obtain different polarization state optical signals;

在中心站B处:At central station B:

步骤4:单模光纤15输出的光信号经掺饵光纤放大器16放大后,通过偏振分束器17分束,分别输出到第一光电探测器A18、第二光电探测器B19,在第一光电探测器A18处经拍频后得到经过光学变频的中频参考信号,在第二光电探测器B19处经拍频后得到经过光学变频的中频接收信号;中频参考信号iBPF1(t)、中频接收信号iBPF2(t)公式如下:Step 4: After the optical signal output by the single-mode optical fiber 15 is amplified by the erbium-doped fiber amplifier 16, it is split by the polarization beam splitter 17 and output to the first photodetector A18 and the second photodetector B19 respectively. Detector A18 place obtains the intermediate frequency reference signal through optical frequency conversion after beating frequency, obtains the intermediate frequency receiving signal through optical frequency conversion after beating frequency at the second photodetector B19 place; Intermediate frequency reference signal i BPF1 (t), intermediate frequency receiving signal The formula of i BPF2 (t) is as follows:

Figure BSA0000285872440000062
Figure BSA0000285872440000062

Figure BSA0000285872440000063
Figure BSA0000285872440000063

其中,GOA为掺饵光纤放大器放大系数,R1、R2分别为光电探测器A18、光电探测器B19的响应度;

Figure BSA0000285872440000064
作为有用信号的幅度项,当本振信号和有用信号的频率相差不大时,能够保证中频有用信号受功率周期性衰落影响较小;Among them, G OA is the amplification factor of the erbium-doped fiber amplifier, R 1 and R 2 are the responsivity of photodetector A18 and photodetector B19 respectively;
Figure BSA0000285872440000064
As the amplitude item of the useful signal, when the frequency difference between the local oscillator signal and the useful signal is not large, it can ensure that the intermediate frequency useful signal is less affected by the periodic power fading;

步骤5:中频参考信号和中频接收信号均输入至数字信号处理器DSP 20中进行数字信号处理;至此,中频接收信号含自干扰信号和有用信号以及中频参考信号共同传输至中心站,在数字信号处理器DSP 20中经高位数ADC采样、量化到数字域做进一步处理。Step 5: Both the intermediate frequency reference signal and the intermediate frequency received signal are input to the digital signal processor DSP 20 for digital signal processing; so far, the intermediate frequency received signal includes self-interference signal and useful signal and the intermediate frequency reference signal is jointly transmitted to the central station, and the digital signal In the processor DSP 20, it is sampled and quantized by a high-digit ADC to the digital domain for further processing.

在本发明的一个实施例中,在实际处理过程中,首先按照约定停止发送有用信号,在数字端仅接收到自干扰信号①和参考信号②,利用快速递归最小二乘FTRLS实现自适应滤波,使中频自干扰信号和中频参考信号的误差达到最小,得到滤波器参数值;随后按照约定接收远端发射的有用信号,将中频接收信号减去由中频参考信号经过滤波器得到的自干扰重构信号,最终得到中频有用信号,有用信号经下变频,频偏、相偏恢复,均衡后恢复出有用信号。In one embodiment of the present invention, in the actual processing process, first stop sending useful signals according to the agreement, only receive self-interference signal ① and reference signal ② at the digital end, and use fast recursive least squares FTRLS to realize adaptive filtering, Minimize the error between the intermediate frequency self-interference signal and the intermediate frequency reference signal, and obtain the filter parameter value; then receive the useful signal transmitted by the remote end according to the agreement, and subtract the self-interference obtained by the intermediate frequency reference signal from the intermediate frequency reference signal through the filter to reconstruct the intermediate frequency received signal Signal, and finally obtain the useful signal of intermediate frequency, the useful signal is down-converted, the frequency deviation and phase deviation are recovered, and the useful signal is recovered after equalization.

本发明优点如下:The advantages of the present invention are as follows:

1、自干扰信号经过电放大器、调制器等非线性器件以及多径线性信道,具有复杂的线性/非线性成分分量,利用数字基带信号进行非线性滤波或深度学习等算法消除非线性成分则会带来较大的处理难度和算法运算量,而参考信号回传的方式将参考信号的非线性成分同时传回了中心站,将非线性问题转变为线性问题进行处理,减低了数字域的处理难度。1. Self-interference signals pass through nonlinear devices such as electric amplifiers and modulators and multipath linear channels, and have complex linear/nonlinear components. Using digital baseband signals for nonlinear filtering or deep learning algorithms to eliminate nonlinear components will cause It brings great processing difficulty and algorithm calculation load, and the method of reference signal return transmits the nonlinear component of the reference signal back to the central station at the same time, transforms the nonlinear problem into a linear problem for processing, and reduces the processing in the digital domain difficulty.

2、相比于光域结合数字域的自干扰消除方案,不需要在光域上实现参数调谐,而使用高位数ADC,如12bit位数的ADC量化误差能够达到72.25dB的动态范围,为数字域实现大信号的自干扰深度消除提供可能。2. Compared with the self-interference elimination scheme combining the optical domain with the digital domain, it is not necessary to realize parameter tuning in the optical domain, but using a high-digit ADC, such as a 12-bit ADC quantization error can reach a dynamic range of 72.25dB, which is a digital It is possible to realize the self-interference depth cancellation of large signals in the domain.

3、由于对带有非线性成分分量的自干扰信号进行自适应滤波,需要设置较长的滤波器长度N来保证自干扰信号的消除深度,而传统的递归最小二乘RLS算法需要带来O(N2)的乘法运算量,而FTRLS的乘法远算量仅为O(7N+14),极大地提升了算法的运算速度,而其最显著的一个特征是不需要进行矩阵乘积运算。3. Due to the self-adaptive filtering of the self-interference signal with nonlinear components, it is necessary to set a longer filter length N to ensure the elimination depth of the self-interference signal, while the traditional recursive least squares RLS algorithm needs to bring O (N 2 ) multiplication amount, while FTRLS's multiplication amount is only O(7N+14), which greatly improves the operation speed of the algorithm, and its most notable feature is that it does not need to perform matrix product operations.

附图说明Description of drawings

图1为带内全双工ROF系统下基于光学变频、参考信号同时回传的数字自干扰消除方案装置图;Figure 1 is a device diagram of a digital self-interference cancellation scheme based on optical frequency conversion and simultaneous return of reference signals under an in-band full-duplex ROF system;

图2(a)为800MHz带宽自干扰信号消除前后对比图,图2(b)为自干扰信号消除前与400MHz带宽有用信号恢复对比图,图2(c)为恢复的有用信号星座图。Figure 2(a) is a comparison diagram before and after self-interference signal cancellation in 800MHz bandwidth, Figure 2(b) is a comparison diagram before self-interference signal cancellation and useful signal recovery in 400MHz bandwidth, and Figure 2(c) is a constellation diagram of the recovered useful signal.

具体实施方式detailed description

下面结合附图,详细描述本发明。The present invention will be described in detail below in conjunction with the accompanying drawings.

本发明提供一种带内全双工ROF系统下光学变频、参考信号同时回传的数字自干扰消除装置,包括位于基站A处的信号源1、电放大器2、第一电功分器A3、发射天线4、接收天线5、本振源6、第二电第二电功分器B7、激光器8、偏振控制器9、双偏振双驱动马赫曾德尔调制器10;单模光纤15;位于中心站B处的掺饵光纤放大器16、偏振分束器17、第一光电探测器A18、第二光电探测器B19、数字信号处理器DSP 20。其中,双偏振双驱动马赫曾德尔调制器10含第一双驱动马赫曾德尔调制器A11、第二双驱动马赫曾德尔调制器B12、90度偏振旋转器13、偏振合束器14。The present invention provides a digital self-interference elimination device for optical frequency conversion and simultaneous return of reference signals in an in-band full-duplex ROF system, including a signal source 1 located at a base station A, an electric amplifier 2, a first electric power divider A3, Transmitting antenna 4, receiving antenna 5, local oscillator source 6, second electric power divider B7, laser 8, polarization controller 9, dual polarization dual drive Mach-Zehnder modulator 10; single-mode optical fiber 15; located in the center Erbium-doped fiber amplifier 16, polarization beam splitter 17, first photodetector A18, second photodetector B19, digital signal processor DSP 20 at station B. Wherein, the dual-polarization dual-drive Mach-Zehnder modulator 10 includes a first dual-drive Mach-Zehnder modulator A11 , a second dual-drive Mach-Zehnder modulator B12 , a 90-degree polarization rotator 13 , and a polarization beam combiner 14 .

在基站A处:At base station A:

激光器8产生的光载波经偏振控制器9输入至双偏振双驱动马赫曾德尔调制器10。The optical carrier generated by the laser 8 is input to the dual-polarization dual-drive Mach-Zehnder modulator 10 through the polarization controller 9 .

本振源6产生本振信号输出给第二电第二电功分器B7,第二电第二电功分器B7对本振信号④进行功率分配,一路输出至第一双驱动马赫曾德尔调制器A11,另一路输出至第二双驱动马赫曾德尔调制器B12。The local oscillator source 6 generates a local oscillator signal and outputs it to the second electric second electric power divider B7, and the second electric second electric power divider B7 performs power distribution on the local oscillator signal ④, and one output to the first dual-drive Mach-Zehnder modulation device A11, and another output to the second dual-drive Mach-Zehnder modulator B12.

信号源1产生的载波调制信号经电放大器2放大后输出给第一电功分器A3,第一电功分器A3对其进行功率分配,其中一路输出作为参考信号②与本振源6经第二电功分器B7产生的一路本振信号④均输入至第一双驱动马赫曾德尔调制器A11进行电光调制,产生X偏振态光信号Ex;另一路输出至发射天线4并由其发出。The carrier modulation signal generated by the signal source 1 is amplified by the electric amplifier 2 and then output to the first electric power divider A3, and the first electric power divider A3 performs power distribution on it, and one of the outputs is used as a reference signal ② and the local oscillator source 6 via One local oscillator signal ④ generated by the second electric power splitter B7 is input to the first dual-drive Mach-Zehnder modulator A11 for electro-optic modulation to generate X polarization state optical signal E x ; the other is output to the transmitting antenna 4 and then issue.

经多径自干扰信道传输的自干扰信号①与远端有用信号③一同被接收天线5接收,形成混合信号,之后,混合信号与本振源6经第二电功分器B7产生的另一路本振信号④都输入至第二双驱动马赫曾德尔调制器B12进行电光调制,所产生的X偏振态光信号经90度偏振旋转器13后改变偏振态后输出。The self-interference signal ① transmitted through the multi-path self-interference channel and the remote useful signal ③ are received by the receiving antenna 5 to form a mixed signal. After that, the mixed signal and the local vibration source 6 are generated by the second electric power splitter B7. All vibration signals ④ are input to the second dual-drive Mach-Zehnder modulator B12 for electro-optical modulation, and the generated X polarization optical signal passes through the 90-degree polarization rotator 13 and then outputs after changing the polarization state.

第一双驱动马赫曾德尔调制器A11输出的光载波调制信号、90度偏振旋转器13输出的光载波调制信号,这两路不同偏振态的信号在偏振合束器14处合束,形成偏振合束光信号。偏振合束光信号经单模光纤15传输至中心站B。The optical carrier modulation signal output by the first dual-drive Mach-Zehnder modulator A11 and the optical carrier modulation signal output by the 90-degree polarization rotator 13, the two signals of different polarization states are combined at the polarization beam combiner 14 to form a polarization Combining light signals. The polarization-combined optical signal is transmitted to the central station B through the single-mode optical fiber 15 .

在中心站B处:At central station B:

经掺饵光纤放大器16放大后,通过偏振分束器17分束,分别输出到第一光电探测器A18、第二光电探测器B19,在第一光电探测器A18处经拍频后得到经过光学变频的中频参考信号,在第二光电探测器B19处经拍频后得到经过光学变频的中频接收信号,中频参考信号和中频接收信号均输入至数字信号处理器DSP 20中进行数字信号处理。After being amplified by the erbium-doped fiber amplifier 16, the beam is split by the polarization beam splitter 17, and output to the first photodetector A18 and the second photodetector B19 respectively, and obtained after being beat at the first photodetector A18. The frequency-converted intermediate-frequency reference signal is beaten at the second photodetector B19 to obtain an optically-converted intermediate-frequency received signal, and both the intermediate-frequency reference signal and the intermediate-frequency received signal are input to the digital signal processor DSP 20 for digital signal processing.

提供一种带内全双工ROF系统下光学变频、参考信号同时回传的数字自干扰消除方法。A digital self-interference elimination method in which optical frequency conversion and reference signals are simultaneously returned in an in-band full-duplex ROF system is provided.

在本发明中,数字域自干扰消除采取快速递归最小二乘FTRLS算法,利用中频参考信号将中频接收信号中的自干扰信号滤除,最终实现有用信号恢复。In the present invention, the self-interference elimination in the digital domain adopts the fast recursive least squares FTRLS algorithm, uses the intermediate frequency reference signal to filter out the self-interference signal in the intermediate frequency received signal, and finally realizes the recovery of the useful signal.

为方便说明信号在光域中的变频、传输,不考虑非线性、多径等因素,假定自干扰信号①为

Figure BSA0000285872440000101
参考信号②为
Figure BSA0000285872440000102
有用信号③为
Figure BSA0000285872440000103
本振信号④为
Figure BSA0000285872440000104
其中VSI、VR、VSOI、VLO分别为自干扰信号①、本地参考信号②、有用信号③、本振信号④的电压,ωSI、ωR、ωSOI、ωLO分别为自干扰信号①、本地参考信号②、有用信号③、本振信号④的角频率,
Figure BSA0000285872440000105
分别为自干扰信号①、本地参考信号②、有用信号③、本振信号④的相位。For the convenience of explaining the frequency conversion and transmission of signals in the optical domain, regardless of factors such as nonlinearity and multipath, it is assumed that the self-interference signal ① is
Figure BSA0000285872440000101
The reference signal ② is
Figure BSA0000285872440000102
The useful signal ③ is
Figure BSA0000285872440000103
The local oscillator signal ④ is
Figure BSA0000285872440000104
Among them, V SI , VR , V SOI , and V LO are voltages of self-interference signal ①, local reference signal ②, useful signal ③, and local oscillator signalrespectively , and ω SI , ω R , ω SOI , and ω LO are self-interference Angular frequency of signal ①, local reference signal ②, useful signal ③, local oscillator signal ④,
Figure BSA0000285872440000105
They are the phases of the self-interference signal ①, the local reference signal ②, the useful signal ③, and the local oscillator signal ④ respectively.

在基站A处:At base station A:

步骤1:信号源1产生的载波调制信号经电放大器2放大后输出给第一电功分器A3,第一电功分器A3对其进行功率分配,其中一路输出为参考信号②。另一路经多径自干扰信道传输后形成的自干扰信号①与远端有用信号③一同被接收天线5接收,形成混合信号(①+③)。Step 1: The carrier modulation signal generated by the signal source 1 is amplified by the electric amplifier 2 and then output to the first electric power divider A3, and the first electric power divider A3 performs power distribution on it, and one of the outputs is a reference signal ②. The self-interference signal ① and the remote useful signal ③ are received by the receiving antenna 5 together, forming a mixed signal (①+③).

步骤2:激光器8产生光载波经偏振控制器9产生线偏振光,线偏振光输入至双偏振双驱动马赫曾德尔调制器10。Step 2: The laser 8 generates an optical carrier and the polarization controller 9 generates linearly polarized light, and the linearly polarized light is input to the dual-polarized dual-drive Mach-Zehnder modulator 10 .

参考信号②与本振源6经第二电第二电功分器B7产生的一路本振信号④均输入至第一双驱动马赫曾德尔调制器A11进行电光调制,将第一双驱动马赫曾德尔调制器A11设为最小偏置点,输出X偏振态光信号Ex。第一电功分器A3的另一路输出至发射天线4并由其发出。The reference signal ② and the local oscillator signal ④ generated by the local oscillator source 6 via the second electric power divider B7 are both input to the first dual-drive Mach-Zehnder modulator A11 for electro-optical modulation, and the first dual-drive Mach-Zehnder The Del modulator A11 is set to the minimum bias point, and outputs the X polarization state optical signal Ex . The other output of the first electric power divider A3 is sent to the transmitting antenna 4 and sent therefrom.

混合信号(①+③)与本振源6经第二电功分器B7产生的另一路本振信号④都输入至第二双驱动马赫曾德尔调制器B12进行电光调制,同样将第二双驱动马赫曾德尔调制器B12设为最小偏置点,第二双驱动马赫曾德尔调制器B12输出的X偏振态光信号,该信号经90度偏振旋转器13旋转为Y偏振态光信号EyThe mixed signal (①+③) and another local oscillator signal ④ produced by the local oscillator source 6 through the second electric power divider B7 are all input to the second dual-drive Mach-Zehnder modulator B12 for electro-optical modulation, and the second dual The driving Mach-Zehnder modulator B12 is set to the minimum bias point, and the X polarization state optical signal output by the second dual driving Mach-Zehnder modulator B12 is rotated by the 90-degree polarization rotator 13 into a Y polarization state optical signal E y .

这两路不同偏振态的信号Ex、Ey在偏振合束器14处合束,形成偏振光信号,偏振光信号包络E1(t)如公式1所示:These two signals E x and E y of different polarization states are combined at the polarization beam combiner 14 to form a polarized light signal. The envelope E 1 (t) of the polarized light signal is shown in Formula 1:

Figure BSA0000285872440000111
Figure BSA0000285872440000111

其中,

Figure BSA0000285872440000112
为光载波,Ec为光载波的幅度,ωc为输入光载波频率,mSI=πVSI/Vπ、mR=πVR/Vπ、mSOI=πVSOI/Vπ、mLO=πVLO/Vπ分别为自干扰信号①、参考信号②、有用信号③、本振信号④的调制系数,Vπ为双偏振双驱动马赫曾德尔调制器10的半波电压,J0()、J1()分别为0阶、1阶一类贝塞尔函数,t为时间;in,
Figure BSA0000285872440000112
is the optical carrier, E c is the amplitude of the optical carrier, ω c is the input optical carrier frequency, m SI =πV SI /V π , m R =πV R /V π , m SOI =πV SOI /V π , m LO = πV LO /V π are the modulation coefficients of the self-interference signal ①, reference signal ②, useful signal ③, and local oscillator signal ④ respectively, V π is the half-wave voltage of the dual-polarization dual-drive Mach-Zehnder modulator 10, J 0 () , J 1 () are a class of Bessel functions of order 0 and order 1 respectively, and t is time;

步骤3:合束信号经单模光纤15传输至中心站B。由于光纤的色散效应,光纤的传输函数为H(ω)=exp(-αL/2+jβ2L(ω-ωc)2/2),其中α为衰减常量,β2为群速度色散参量,L为光纤长度。因此信号经过单模光纤15后输出的光信号包络ESMF(t)如公式2所示:Step 3: The bundled signal is transmitted to the central station B through the single-mode optical fiber 15 . Due to the dispersion effect of the fiber, the transmission function of the fiber is H(ω)=exp(-αL/2+jβ 2 L(ω-ω c ) 2 /2), where α is the attenuation constant and β 2 is the group velocity dispersion parameter , L is the fiber length. Therefore, the optical signal envelope E SMF (t) output after the signal passes through the single-mode optical fiber 15 is shown in formula 2:

Figure BSA0000285872440000113
Figure BSA0000285872440000113

其中,ESMFx、ESMFy分别为Ex、Ey经单模光纤15传输后得到不同的偏振态光信号。Wherein, E SMFx and E SMFy are respectively E x and E y to obtain optical signals with different polarization states after being transmitted through the single-mode optical fiber 15 .

在中心站B处:At central station B:

步骤4:单模光纤15输出的光信号经掺饵光纤放大器16放大后,通过偏振分束器17分束,分别输出到第一光电探测器A18、第二光电探测器B19,在第一光电探测器A18处经拍频后得到经过光学变频的中频参考信号,在第二光电探测器B19处经拍频后得到经过光学变频的中频接收信号。中频参考信号iBPF1(t)、中频接收信号iBPF2(t)公式如下:Step 4: After the optical signal output by the single-mode optical fiber 15 is amplified by the erbium-doped fiber amplifier 16, it is split by the polarization beam splitter 17 and output to the first photodetector A18 and the second photodetector B19 respectively. After frequency beating at the detector A18, an intermediate frequency reference signal through optical frequency conversion is obtained, and after frequency beating at the second photodetector B19, an intermediate frequency receiving signal through optical frequency conversion is obtained. The formulas of intermediate frequency reference signal i BPF1 (t) and intermediate frequency receiving signal i BPF2 (t) are as follows:

Figure BSA0000285872440000121
Figure BSA0000285872440000121

Figure BSA0000285872440000122
Figure BSA0000285872440000122

其中,GOA为掺饵光纤放大器放大系数,R1、R2分别为第一光电探测器A18、第二光电探测器B19的响应度。

Figure BSA0000285872440000123
作为有用信号的幅度项,当本振信号和有用信号的频率相差不大时,能够保证中频有用信号受功率周期性衰落影响较小。Wherein, G OA is the amplification factor of the erbium-doped fiber amplifier, and R 1 and R 2 are the responsivity of the first photodetector A18 and the second photodetector B19 respectively.
Figure BSA0000285872440000123
As the amplitude item of the useful signal, when the frequency difference between the local oscillator signal and the useful signal is not large, it can ensure that the intermediate frequency useful signal is less affected by the periodic power fading.

步骤5:中频参考信号和中频接收信号均输入至数字信号处理器DSP 20中进行数字信号处理。至此,中频接收信号含自干扰信号和有用信号以及中频参考信号共同传输至中心站B,在数字信号处理器DSP 20中经高位数ADC采样、量化到数字域做进一步处理。Step 5: Both the intermediate frequency reference signal and the intermediate frequency received signal are input to the digital signal processor DSP 20 for digital signal processing. So far, the received intermediate frequency signal including self-interference signal, useful signal and intermediate frequency reference signal is transmitted to the central station B, and is sampled by a high-bit ADC in the digital signal processor DSP 20, quantized to the digital domain for further processing.

在实际处理过程中,首先按照约定停止发送有用信号,在数字端仅接收到自干扰信号①和参考信号②,利用快速递归最小二乘FTRLS(Dechene D J.“Fast transversalrecursive least-squares(FT-RLS)algorithm[C]”IEEE Trans Signal Proc.Citeseer,2007.)实现自适应滤波,使中频自干扰信号和中频参考信号的误差达到最小,得到滤波器参数值。随后按照约定接收远端发射的有用信号,将中频接收信号减去由中频参考信号经过滤波器得到的自干扰重构信号,最终得到中频有用信号,有用信号经下变频,频偏、相偏恢复,均衡后恢复出有用信号。下变频、频偏、相偏恢复、均衡技术为本领域技术人员熟知,不再累述。In the actual processing process, first stop sending useful signals according to the agreement, and only receive self-interference signal ① and reference signal ② at the digital end, using fast recursive least squares FTRLS (Dechene D J. "Fast transversalrecursive least-squares (FT- RLS) algorithm[C] "IEEE Trans Signal Proc. Citeseer, 2007.) realizes adaptive filtering, minimizes the error between the intermediate frequency self-interference signal and the intermediate frequency reference signal, and obtains the filter parameter value. Then receive the useful signal transmitted by the remote end according to the agreement, and subtract the self-interference reconstruction signal obtained from the intermediate frequency reference signal through the filter from the intermediate frequency received signal, and finally obtain the intermediate frequency useful signal. The useful signal is down-converted, and the frequency offset and phase offset are restored. , the useful signal is restored after equalization. Down-conversion, frequency offset, phase offset recovery, and equalization techniques are well known to those skilled in the art and will not be repeated here.

本发明优点如下:The advantages of the present invention are as follows:

1、自干扰信号经过电放大器、调制器等非线性器件以及多径线性信道,具有复杂的线性/非线性成分分量,利用数字基带信号进行非线性滤波或深度学习等算法消除非线性成分则会带来较大的处理难度和算法运算量,而参考信号回传的方式将参考信号的非线性成分同时传回了中心站,将非线性问题转变为线性问题进行处理,减低了数字域的处理难度。1. Self-interference signals pass through nonlinear devices such as electric amplifiers and modulators and multipath linear channels, and have complex linear/nonlinear components. Using digital baseband signals for nonlinear filtering or deep learning algorithms to eliminate nonlinear components will cause It brings great processing difficulty and algorithm calculation load, and the method of reference signal return transmits the nonlinear component of the reference signal back to the central station at the same time, transforms the nonlinear problem into a linear problem for processing, and reduces the processing in the digital domain difficulty.

2、相比于光域结合数字域的自干扰消除方案,不需要在光域上实现参数调谐,而使用高位数ADC,如12bit位数的ADC量化误差能够达到72.25dB的动态范围,为数字域实现大信号的自干扰深度消除提供可能。2. Compared with the self-interference elimination scheme combining the optical domain with the digital domain, it is not necessary to realize parameter tuning in the optical domain, but using a high-digit ADC, such as a 12-bit ADC quantization error can reach a dynamic range of 72.25dB, which is a digital It is possible to realize the self-interference depth cancellation of large signals in the domain.

3、由于对带有非线性成分分量的自干扰信号进行自适应滤波,需要设置较长的滤波器长度N来保证自干扰信号的消除深度,而传统的递归最小二乘RLS算法需要带来O(N2)的乘法运算量,而FTRLS的乘法远算量仅为O(7N+14),极大地提升了算法的运算速度,而其最显著的一个特征是不需要进行矩阵乘积运算。3. Due to the self-adaptive filtering of the self-interference signal with nonlinear components, it is necessary to set a longer filter length N to ensure the elimination depth of the self-interference signal, while the traditional recursive least squares RLS algorithm needs to bring O (N 2 ) multiplication amount, while FTRLS's multiplication amount is only O(7N+14), which greatly improves the operation speed of the algorithm, and its most notable feature is that it does not need to perform matrix product operations.

为验证本发明的多径、非线性自干扰信号消除能力,以及有用信号的恢复能力,利用optisystem14.0以及matlab2021b进行仿真。In order to verify the multipath, non-linear self-interference signal elimination ability of the present invention, and the recovery ability of the useful signal, the simulation is carried out by using optisystem14.0 and matlab2021b.

设置自干扰信号为QAM调制信号,频率12.5GHz,带宽800MHz,功率30dBm,本振信号频率10GHz,功率27dBm,有用信号为16QAM信号,频率12.5GHz,带宽400M,功率-3dBm,自干扰信道由5条不同延时、衰减的路径组成,延时分别为[3,30,70,80,103]ps,衰减分别为[8,10,12,13,16]dB,光源波长为1550nm,功率为16dBm,线宽为0.1MHz,马赫曾德尔调制器消光比为30dB,单模光纤长度为10km,参考波长为1552nm,掺铒光纤放大器增益为10dB,噪声系数为4.5dB,偏振分束器偏移量为2°,光电探测器A响应度为0.9A/W,光电探测器B响应度为0.85A/W。在FTRLS算法中,滤波器阶数N为800,遗忘因子λ=1,前向/后向预测最小加权二乘误差

Figure BSA0000285872440000141
初始值均为0.00001。经过上述过程,方案的消除性能分别如下:Set self-jamming signal as QAM modulation signal, frequency 12.5GHz, bandwidth 800MHz, power 30dBm, local oscillator signal frequency 10GHz, power 27dBm, useful signal 16QAM signal, frequency 12.5GHz, bandwidth 400M, power -3dBm, self-jamming channel by 5 Paths with different delays and attenuations, the delays are [3, 30, 70, 80, 103] ps, the attenuations are [8, 10, 12, 13, 16] dB, the wavelength of the light source is 1550nm, and the power is 16dBm, linewidth 0.1MHz, Mach-Zehnder modulator extinction ratio 30dB, single-mode fiber length 10km, reference wavelength 1552nm, erbium-doped fiber amplifier gain 10dB, noise figure 4.5dB, polarization beam splitter offset The amount is 2°, the responsivity of photodetector A is 0.9A/W, and the responsivity of photodetector B is 0.85A/W. In the FTRLS algorithm, the filter order N is 800, the forgetting factor λ=1, and the forward/backward prediction minimum weighted square error
Figure BSA0000285872440000141
The initial value is 0.00001. After the above process, the elimination performance of the scheme is as follows:

图2(a)为自干扰消除前后的频谱图,在不发射有用信号时,自干扰信号能够达到48dB的消除深度,自干扰信号中的非线性成分同样被消除;图2(b)为自干扰信号与恢复的有用信号频谱图,当发射有用信号时,有用信号能够从接收信号中恢复出来,从图中能够看出,消除性能稍有降低,主要是由于自干扰信号和有用信号共同经过光链路拍频后得到的自干扰信号幅度略小于自干扰信号单独经过光链路拍频得到的幅度,在数字域中从接收信号中恢复有用信号时引起误差;其次,通过图2(a)(b)得出,自干扰信号、有用信号、参考信号能够经过光学变频到中心频率为2.5GHz的中频频率上;图(c)为恢复的16QAM有用信号的星座图,EVM达到了7.18%。Figure 2(a) is the spectrum diagram before and after self-interference cancellation. When the useful signal is not transmitted, the self-interference signal can reach a cancellation depth of 48dB, and the nonlinear components in the self-interference signal are also eliminated; Figure 2(b) is the self-interference signal The spectrum diagram of the interference signal and the restored useful signal. When the useful signal is transmitted, the useful signal can be recovered from the received signal. It can be seen from the figure that the elimination performance is slightly reduced, mainly because the self-interfering signal and the useful signal pass through together The amplitude of the self-interference signal obtained after the optical link beat frequency is slightly smaller than the amplitude obtained by the self-interference signal through the optical link beat frequency alone, which causes errors when recovering the useful signal from the received signal in the digital domain; secondly, through Fig. 2(a )(b) shows that the self-interfering signal, useful signal and reference signal can be optically converted to an intermediate frequency with a center frequency of 2.5 GHz; Figure (c) is the constellation diagram of the recovered 16QAM useful signal, and the EVM has reached 7.18% .

Claims (3)

1. A digital self-interference elimination device with optical frequency conversion and reference signal simultaneous return under an in-band full-duplex ROF system is characterized by comprising a signal source (1) positioned at a base station A, an electric amplifier (2), a first electric power divider A (3), a transmitting antenna (4), a receiving antenna (5), a local oscillation source (6), a second electric power divider B (7), a laser (8), a polarization controller (9) and a dual-polarization dual-drive Mach-Zehnder modulator (10); a single mode optical fiber (15); an erbium-doped fiber amplifier (16), a polarization beam splitter (17), a first photoelectric detector A (18), a second photoelectric detector B (19) and a digital signal processor DSP (20) which are positioned at the central station B; wherein, the dual-polarization dual-drive Mach-Zehnder modulator (10) comprises a first dual-drive Mach-Zehnder modulator A (11), a second dual-drive Mach-Zehnder modulator B (12), a 90-degree polarization rotator (13) and a polarization beam combiner (14);
at base station a:
an optical carrier generated by a laser (8) is input to a dual-polarization dual-drive Mach-Zehnder modulator (10) through a polarization controller (9);
the local oscillation source (6) generates a local oscillation signal and outputs the local oscillation signal to the second electric power divider B (7), the second electric power divider B (7) distributes the power of the local oscillation signal (4), one path of local oscillation signal is output to the first double-drive Mach-Zehnder modulator A (11), and the other path of local oscillation signal is output to the second double-drive Mach-Zehnder modulator B (12);
a carrier modulation signal generated by a signal source (1) is amplified by an electrical amplifier (2) and then output to a first electrical power divider A (3), the first electrical power divider A (3) distributes power, one output is used as a reference signal (2) and one local oscillation signal (4) generated by a local oscillation source (6) through a second electrical power divider B (7) are input to a first double-drive Mach-Zehnder modulator A (11) for electro-optical modulation, and an X polarization state optical signal E is generated x (ii) a The other path is output to a transmitting antenna (4) and is transmitted by the transmitting antenna;
the self-interference signal (1) transmitted by a multipath self-interference channel and a far-end useful signal (3) are received by a receiving antenna (5) together to form a mixed signal, then the mixed signal and another local oscillation signal (4) generated by a local oscillation source (6) through a second electric power divider B (7) are input to a second double-drive Mach-Zehnder modulator B (12) for electro-optical modulation, and the generated X polarization state optical signal is output after the polarization state is changed through a 90-degree polarization rotator (13);
the light carrier modulation signal output by a first double-drive Mach-Zehnder modulator A (11) and the light carrier modulation signal output by a 90-degree polarization rotator (13) are combined at a polarization beam combiner (14) to form a polarization combined light signal; the polarized beam combination optical signal is transmitted to a central station B through a single mode optical fiber (15);
at central station B:
the mixed signal is amplified by an erbium-doped fiber amplifier (16), split by a polarization beam splitter (17), and respectively output to a first photoelectric detector A (18) and a second photoelectric detector B (19), an intermediate frequency reference signal subjected to optical frequency conversion is obtained at the first photoelectric detector A (18) after beat frequency, an intermediate frequency receiving signal subjected to optical frequency conversion is obtained at the second photoelectric detector B (19) after beat frequency, and the intermediate frequency reference signal and the intermediate frequency receiving signal are both input to a digital signal processor DSP (20) for digital signal processing.
2. A digital self-interference elimination method for optical frequency conversion and reference signal simultaneous return under an in-band full-duplex ROF system, which is based on the digital self-interference elimination device for optical frequency conversion and reference signal simultaneous return under the in-band full-duplex ROF system as claimed in claim 1, and assumes that the self-interference signal (1) is
Figure FSA0000285872430000021
The reference signal (2) is
Figure FSA0000285872430000022
The useful signal (3) is
Figure FSA0000285872430000023
The local oscillator signal (4) is
Figure FSA0000285872430000024
Wherein V SI 、V R 、V SOI 、V LO Respectively, the voltages of the self-interference signal (1), the local reference signal (2), the useful signal (3) and the local oscillator signal (4), omega SI 、ω R 、ω SOI 、ω LO Respectively are angular frequencies of a self-interference signal (1), a local reference signal (2), a useful signal (3) and a local oscillator signal (4),
Figure FSA0000285872430000025
the phase positions of the self-interference signal (1), the local reference signal (2), the useful signal (3) and the local oscillator signal (4) are respectively;
the method is characterized by comprising the following steps:
at base station a:
step 1: a carrier modulation signal generated by a signal source (1) is amplified by an electric amplifier (2) and then output to a first electric power divider A (3), the first electric power divider A (3) distributes power to the carrier modulation signal, and one path of output is a reference signal (2); the other path of self-interference signal (1) formed after being transmitted through a multipath self-interference channel is received by a receiving antenna (5) together with a far-end useful signal (3) to form a mixed signal ((1) + (3));
step 2: a laser (8) generates an optical carrier, a polarization controller (9) generates linearly polarized light, and the linearly polarized light is input to a dual-polarization dual-drive Mach-Zehnder modulator (10);
a reference signal (2) and one local oscillation signal (4) generated by a local oscillation source (6) through a second electric power divider B (7) are input to a first double-drive Mach-Zehnder modulator A (11) for electro-optical modulation, the first double-drive Mach-Zehnder modulator A (11) is set as a minimum bias point, and an X polarized optical signal E is output x (ii) a The other path of the first power divider A (3) is output to a transmitting antenna (4) and transmitted by the transmitting antenna;
the mixed signal ((1) + (3)) and the other local oscillation signal (4) generated by the local oscillation source (6) through the second electric power divider B (7) are input to the second double-drive Mach-Zehnder modulator B (12) for electro-optical modulation, similarly, the second double-drive Mach-Zehnder modulator B (12) is set as a minimum offset point, and the signal is rotated into a Y-polarized optical signal E through a 90-degree polarization rotator (13) to form an X-polarized optical signal output by the second double-drive Mach-Zehnder modulator B (12) y
The two signals E with different polarization states x 、E y Combining the beams at a polarization beam combiner (14) to form a polarized light signal, the polarized light signal enveloping E 1 (t) is shown in equation 1:
Figure FSA0000285872430000031
wherein,
Figure FSA0000285872430000032
being optical carriers, E c Amplitude of the optical carrier, ω c For input light carrier frequency, m SI =πV SI /V π 、m R =πV R /V π 、m SOI =πV SOI /V π 、m LO =πV LO /V π The modulation coefficients are respectively self-interference signal (1), reference signal (2), useful signal (3) and local oscillator signal (4), V π Is the half-wave voltage, J, of the dual-polarization dual-drive Mach-Zehnder modulator (10) 0 ()、J 1 () The first-class Bessel functions are 0-order and 1-order respectively, and t is time;
and step 3: the combined beam signal is transmitted to a central station B through a single mode optical fiber (15); due to the dispersion effect of the optical fiber, the transmission function of the optical fiber is H (omega) = exp (-alpha L/2+ j beta) 2 L(ω-ω c ) 2 /2), where α is the damping constant, β 2 Is a group velocity dispersion parameter, L is the fiber length; so that the signal passes through the single-mode fiber (15) and the output optical signal envelope E SMF (t) is shown in equation 2:
Figure FSA0000285872430000041
wherein E is SMFx 、E SMFy Are respectively E x 、E y Different polarized optical signals are obtained after the transmission of the single mode optical fiber (15);
at the central station B:
and 4, step 4: an optical signal output by a single mode fiber (15) is amplified by an erbium-doped fiber amplifier (16), split by a polarization beam splitter (17), and output to a first photoelectric detector A (18) and a second photoelectric detector B (19) respectively, an intermediate frequency reference signal subjected to optical frequency conversion is obtained at the first photoelectric detector A (18) after beat frequency, and an intermediate frequency receiving signal subjected to optical frequency conversion is obtained at the second photoelectric detector B (19) after beat frequency; intermediate frequency reference signal i BPF1 (t) intermediate frequency received signal i BPF2 The formula (t) is as follows:
Figure FSA0000285872430000042
Figure FSA0000285872430000043
wherein G is OA For amplification factor, R, of an erbium-doped fiber amplifier 1 、R 2 Responsivity of a first photoelectric detector A (18) and responsivity of a second photoelectric detector B (19) are respectively measured;
Figure FSA0000285872430000044
as the amplitude term of the useful signal, when the frequency difference between the local oscillation signal and the useful signal is not large, the intermediate frequency useful signal can be ensured to be less influenced by power periodic fading;
and 5: the intermediate frequency reference signal and the intermediate frequency receiving signal are both input into a digital signal processor DSP (20) for digital signal processing; so far, the intermediate frequency receiving signal comprises a self-interference signal, a useful signal and an intermediate frequency reference signal which are transmitted to a central station B together, and the signal is sampled and quantized to a digital domain through a high-bit ADC in a digital signal processor DSP (20) for further processing.
3. The method for eliminating digital self-interference under optical frequency conversion and reference signal simultaneous return in the in-band full-duplex ROF system according to claim 2, characterized in that in the actual processing process, firstly, the sending of the useful signal is stopped according to convention, only the self-interference signal (1) and the reference signal (2) are received at the digital end, and the self-adaptive filtering is realized by using the fast recursive least squares (FTRLS), so that the error between the intermediate frequency self-interference signal and the intermediate frequency reference signal is minimized, and the filter parameter value is obtained; and then receiving a useful signal transmitted by a far end according to a convention, subtracting a self-interference reconstruction signal obtained by an intermediate frequency reference signal through a filter from the intermediate frequency received signal to finally obtain an intermediate frequency useful signal, and recovering the useful signal after down-conversion, frequency offset and phase offset equalization.
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