CN107528638A - Wide-band microwave Direction-of-arrival method based on microwave photon filtering - Google Patents
Wide-band microwave Direction-of-arrival method based on microwave photon filtering Download PDFInfo
- Publication number
- CN107528638A CN107528638A CN201710655401.4A CN201710655401A CN107528638A CN 107528638 A CN107528638 A CN 107528638A CN 201710655401 A CN201710655401 A CN 201710655401A CN 107528638 A CN107528638 A CN 107528638A
- Authority
- CN
- China
- Prior art keywords
- microwave
- polarization
- mzm
- arrival
- signal
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 238000000034 method Methods 0.000 title claims abstract description 22
- 238000001914 filtration Methods 0.000 title claims abstract description 18
- 230000010287 polarization Effects 0.000 claims abstract description 69
- 230000003287 optical effect Effects 0.000 claims abstract description 38
- 238000005259 measurement Methods 0.000 claims description 13
- 230000005540 biological transmission Effects 0.000 claims description 3
- 238000012360 testing method Methods 0.000 claims description 3
- 230000000694 effects Effects 0.000 claims description 2
- 230000002265 prevention Effects 0.000 claims 1
- 238000000926 separation method Methods 0.000 claims 1
- 238000004891 communication Methods 0.000 abstract description 3
- 238000010276 construction Methods 0.000 abstract 1
- 238000005516 engineering process Methods 0.000 description 7
- 238000012545 processing Methods 0.000 description 3
- 238000001228 spectrum Methods 0.000 description 3
- 238000006243 chemical reaction Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000010363 phase shift Effects 0.000 description 2
- 230000001427 coherent effect Effects 0.000 description 1
- 230000001934 delay Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 230000009977 dual effect Effects 0.000 description 1
- 238000003780 insertion Methods 0.000 description 1
- 230000037431 insertion Effects 0.000 description 1
- 238000011017 operating method Methods 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 238000004611 spectroscopical analysis Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/70—Photonic quantum communication
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/60—Receivers
- H04B10/61—Coherent receivers
- H04B10/614—Coherent receivers comprising one or more polarization beam splitters, e.g. polarization multiplexed [PolMux] X-PSK coherent receivers, polarization diversity heterodyne coherent receivers
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/60—Receivers
- H04B10/61—Coherent receivers
- H04B10/615—Arrangements affecting the optical part of the receiver
- H04B10/6151—Arrangements affecting the optical part of the receiver comprising a polarization controller at the receiver's input stage
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/60—Receivers
- H04B10/61—Coherent receivers
- H04B10/616—Details of the electronic signal processing in coherent optical receivers
- H04B10/6162—Compensation of polarization related effects, e.g., PMD, PDL
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/60—Receivers
- H04B10/61—Coherent receivers
- H04B10/616—Details of the electronic signal processing in coherent optical receivers
- H04B10/6165—Estimation of the phase of the received optical signal, phase error estimation or phase error correction
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/60—Receivers
- H04B10/66—Non-coherent receivers, e.g. using direct detection
- H04B10/67—Optical arrangements in the receiver
- H04B10/671—Optical arrangements in the receiver for controlling the input optical signal
- H04B10/675—Optical arrangements in the receiver for controlling the input optical signal for controlling the optical bandwidth of the input signal, e.g. spectral filtering
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/60—Receivers
- H04B10/66—Non-coherent receivers, e.g. using direct detection
- H04B10/69—Electrical arrangements in the receiver
- H04B10/691—Arrangements for optimizing the photodetector in the receiver
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Optics & Photonics (AREA)
- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
- Optical Communication System (AREA)
Abstract
Description
技术领域technical field
本发明涉及光通信技术领域和微波技术领域,主要涉及光通信技术中基于微波光子滤波的宽带微波信号到达角估计的方法。The invention relates to the technical fields of optical communication and microwave technology, and mainly relates to a method for estimating the arrival angle of broadband microwave signals based on microwave photon filtering in the optical communication technology.
背景技术Background technique
在雷达系统和电子战等领域中,对波达角估计有着广泛的需求。然而,受电子瓶颈限制,利用现有电子技术实现对高频段、大瞬时带宽微波信号的到达角测量面临较大挑战。为了克服电子瓶颈的限制,微波光子学将电子技术和光子技术相结合,实现了在光域对微波信号的产生、传输和处理,其具有大带宽、抗电磁干扰等优点,因而逐渐成为各国研究热点之一。其中,基于微波光子的宽带微波信号测量技术具有结构简单易于实现,不受电子瓶颈影响等优点,进而受到各国研究机构的重视。In areas such as radar systems and electronic warfare, there is a wide range of needs for angle of arrival estimation. However, limited by the electronic bottleneck, the use of existing electronic technology to achieve angle-of-arrival measurement of microwave signals with high frequency bands and large instantaneous bandwidths faces great challenges. In order to overcome the limitations of electronic bottlenecks, microwave photonics combines electronic technology and photon technology to realize the generation, transmission and processing of microwave signals in the optical domain. One of the hot spots. Among them, the broadband microwave signal measurement technology based on microwave photons has the advantages of simple structure, easy implementation, and not being affected by electronic bottlenecks, and has thus attracted the attention of research institutions in various countries.
目前基于微波光子的微波信号到达角估计的基本原理是测量两个单独的天线单元处接收的射频信号之间的相移或相对时间延迟。根据实现方式的不同,主要可以分为三种:(1)将两个天线接收的微波信号及其相位延迟分量加载到两个电光调制器,通过测量光载波功率获得的相移,从而得到到达角;(2)采用双平行马赫-增德尔调制器(DP-MZM)或双驱动MZM构成的并行光延迟结构,通过抑制光载波,测量光边带功率来获得相位延迟,从而得到到达角;(3)基于一对微波光子下变频器,通过测量相应的中频(IF)信号之间的时间延迟来获得微波信号之间的时间延迟,获得到达角。The current basic principle of microwave photon-based angle-of-arrival estimation of microwave signals is to measure the phase shift or relative time delay between received RF signals at two separate antenna elements. According to different implementation methods, it can be mainly divided into three types: (1) The microwave signals received by two antennas and their phase delay components are loaded to two electro-optic modulators, and the phase shift obtained by measuring the optical carrier power is obtained to obtain the arrival (2) Using a parallel optical delay structure composed of a dual parallel Mach-Zehnder modulator (DP-MZM) or a dual-driver MZM, the phase delay is obtained by suppressing the optical carrier and measuring the optical sideband power, thereby obtaining the angle of arrival; (3) Based on a pair of microwave photonic downconverters, the time delay between microwave signals is obtained by measuring the time delay between corresponding intermediate frequency (IF) signals to obtain the angle of arrival.
基于相位检测的方法只能用于纯单音信号,而基于下变频的方法需要进一步的中频处理。因此,这几种方法对大瞬时带宽信号的处理能力有限。基于空间光谱材料中光谱烧孔效应的方法虽然能够处理宽带信号,但是需要在低温下运行。基于光子微波滤波的到达角估计系统通过测量传输陷波可以获得宽带信号的时间延迟。但是其需要以不同波长工作的两个激光源和一对强度调制器,这将增加系统的复杂性。Methods based on phase detection can only be used for pure single-tone signals, while methods based on down-conversion require further IF processing. Therefore, these methods have limited ability to process signals with large instantaneous bandwidth. Methods based on the spectral hole-burning effect in spatial spectroscopy materials can handle broadband signals but need to operate at low temperatures. The angle of arrival estimation system based on photonic microwave filtering can obtain the time delay of broadband signals by measuring the transmission notch. But it requires two laser sources operating at different wavelengths and a pair of intensity modulators, which increases the complexity of the system.
发明内容Contents of the invention
为了解决背景技术中所存在的技术问题,本发明提出了一种基于微波光子滤波的宽带微波信号到达角估计的方法。In order to solve the technical problems existing in the background technology, the present invention proposes a method for estimating the angle of arrival of broadband microwave signals based on microwave photon filtering.
本发明所采用的技术方案是:所述装置包括激光源、偏振复用马赫-曾德尔调制器、偏振合束器、偏振控制器、偏振分束器、光延迟线、可调光衰减器、光电探测器和电信号分析仪;激光源的输出端口与偏振复用马赫-曾德尔调制器输入端相连,该调制器的输出端与偏振控制器输入端口相连;偏振控制器的输出端口与偏振分束器的输入端口相连;偏振分束器的输出端口分别与光延迟线和可调光衰减器的输入端口相连;光延迟线和可调光衰减器的输出端口与偏振合束器输入端口相连;偏振合束器输出端口与光电探测器的输入端口相连,光电探测器的输出端口连接电信号分析仪进行观察测试。The technical scheme adopted in the present invention is: the device includes a laser source, a polarization multiplexing Mach-Zehnder modulator, a polarization beam combiner, a polarization controller, a polarization beam splitter, an optical delay line, an adjustable optical attenuator, A photodetector and an electrical signal analyzer; the output port of the laser source is connected to the input port of a polarization multiplexing Mach-Zehnder modulator, and the output port of the modulator is connected to the input port of a polarization controller; the output port of the polarization controller is connected to the polarization The input port of the beam splitter is connected; the output port of the polarization beam splitter is connected with the input port of the optical delay line and the adjustable optical attenuator respectively; the output port of the optical delay line and the adjustable optical attenuator is connected with the input port of the polarization beam combiner connected; the output port of the polarization beam combiner is connected with the input port of the photodetector, and the output port of the photodetector is connected with an electrical signal analyzer for observation and testing.
所述偏振复用马赫-曾德尔调制器由Y分路器、上下两路并行的马赫-增德尔调制器X-MZM和Y-MZM以及90°偏振旋转器、偏振合束器构成。The polarization multiplexing Mach-Zehnder modulator is composed of a Y splitter, two upper and lower parallel Mach-Zehnder modulators X-MZM and Y-MZM, a 90° polarization rotator, and a polarization beam combiner.
本发明在工作时包括以下步骤:The present invention comprises the following steps when working:
(1)从窄线宽激光器发出的光波注入到偏振复用马赫-曾德尔调制器中;(1) Light waves emitted from a narrow-linewidth laser are injected into a polarization-multiplexed Mach-Zehnder modulator;
(2)入射到偏振分复用马赫-曾德尔调制器的光信号经分路器分别进入X-MZM和Y-MZM中。天线接收到的信号经电放大器后分别输入到X-MZM和Y-MZM的射频端口。Y-MZM输出的信号经90°偏振旋转器后,与X-MZM的输出信号输入到偏振合束器后偏振态正交,实现了偏振态复用;(2) The optical signal incident on the polarization division multiplexing Mach-Zehnder modulator enters the X-MZM and Y-MZM respectively through the splitter. The signals received by the antenna are respectively input to the radio frequency ports of X-MZM and Y-MZM after passing through the electric amplifier. The output signal of Y-MZM passes through the 90° polarization rotator, and the output signal of X-MZM is input to the polarization beam combiner, and then the polarization state is orthogonal to realize polarization multiplexing;
(3)偏振复用马赫-曾德尔调制器的输出信号经偏振控制器注入到偏振分束器。通过调整偏振控制器,偏振复用光信号可以被精确地偏振解复用。偏振分束器输出的一路经过光延迟线引入相对时间延迟;另一路经过可变光衰减器以最小化两个分支之间的功率差;(3) Polarization multiplexing The output signal of the Mach-Zehnder modulator is injected into the polarization beam splitter through the polarization controller. By adjusting the polarization controller, the polarization multiplexed optical signal can be precisely polarization demultiplexed. One output of the polarization beam splitter passes through the optical delay line to introduce a relative time delay; the other passes through the variable optical attenuator to minimize the power difference between the two branches;
(4)两路光信号经偏振合束器输入到光电探测器进行光电转换,输出的电信号频谱通过电信号分析仪进行观察测试;(4) The two optical signals are input to the photodetector through the polarization beam combiner for photoelectric conversion, and the output electrical signal spectrum is observed and tested by the electrical signal analyzer;
本发明提出了一种基于微波光子滤波的宽带微波信号到达角估计的方法,该方案利用偏振分复用马赫-曾德尔调制器,结合光延迟线和光可调衰减器,构建了双抽头微波光子滤波器。对于不同角度的来波,滤波器的响应随着两路延时的不同而变化,通过对输入电信号进行陷波滤波,观察和记录陷波位置测量结果,从而计算出来波方向,对宽带微波信号到达角进行估计。The present invention proposes a method for estimating the angle of arrival of broadband microwave signals based on microwave photon filtering. The scheme uses a polarization division multiplexing Mach-Zehnder modulator, combined with an optical delay line and an optical adjustable attenuator, to construct a double-tap microwave photon filter. For incoming waves at different angles, the response of the filter changes with the difference of the two-way delay. By notch filtering the input electrical signal, observing and recording the measurement results of the notch position, and then calculating the direction of the incoming wave, the broadband microwave Estimate the angle of arrival of the signal.
本方案所构建了双抽头微波光子滤波器,通过正交偏振消除了激光源相干性的限制。所提出的方案只需要一个激光源和一个调制器,可以提高系统的稳定性,降低系统成本。In this scheme, a double-tap microwave photonic filter is constructed, which eliminates the limitation of laser source coherence through orthogonal polarization. The proposed scheme only needs one laser source and one modulator, which can improve the stability of the system and reduce the system cost.
本发明的微波光子滤波是在光域直接进行的,通过对光信号的处理达到微波信号滤波的目的,克服了传统的微波移相的带宽限制以及电磁干扰,因此系统的性能得到了很大的提高。The microwave photon filtering of the present invention is directly carried out in the optical domain, and the purpose of microwave signal filtering is achieved by processing the optical signal, which overcomes the bandwidth limitation and electromagnetic interference of traditional microwave phase shifting, so the performance of the system is greatly improved improve.
附图说明Description of drawings
图1为本发明基于微波光子滤波的宽带微波信号到达角估计的方法的原理图;图2、图3、图4为实验测试结果图,图2(a)为未经滤波的宽带信号的光谱,图2(b)为滤波后宽带信号的光谱,图3为测量的频率偏移值对于相对时间的延迟,图4为测量的相对时间延迟(点)和相应的测量误差(垂直条)。Fig. 1 is the schematic diagram of the method for the angle of arrival estimation of broadband microwave signal based on microwave photon filtering of the present invention; Fig. 2, Fig. 3, Fig. 4 are experimental test result figures, and Fig. 2 (a) is the spectrum of the broadband signal without filtering , Figure 2(b) is the spectrum of the filtered broadband signal, Figure 3 is the measured frequency offset value versus relative time delay, and Figure 4 is the measured relative time delay (points) and the corresponding measurement error (vertical bars).
具体实施方式detailed description
下面结合附图对本发明的实施例作详细说明:本实施例在以本发明技术方案为前提下进行实施,给出了详细的实施方式和具体的操作过程,但本发明的保护范围不限于下述的实施例:The embodiments of the present invention are described in detail below in conjunction with the accompanying drawings: this embodiment is implemented on the premise of the technical solution of the present invention, and detailed implementation methods and specific operating procedures are provided, but the protection scope of the present invention is not limited to the following The described embodiment:
图1为本发明基于微波光子滤波的宽带微波信号到达角估计的方法的原理图。其中偏振复用马赫-曾德尔调制器对微波信号进行调制,生成一个偏振复用信号;偏振复用马赫-曾德尔调制器由Y分路器、上下两路并行的马赫增德尔调制器X-MZM和Y-MZM以及90°偏振旋转器、偏振合束器构成;控制偏振控制器,通过偏振分束器将偏振复用信号解复用为两路,一路使用光延迟线引入相对时间延迟,另一路使用可变光衰减器以最小化两个分支之间的功率差;利用偏振合束器将两路信号合并,输出到光电探测器;经过光电探测器拍频后可得到经过滤波后的微波信号。激光源的输出端口与偏振复用马赫-曾德尔调制器输入端相连,该调制器的输出端与偏振控制器输入端口相连;偏振控制器的输出端口与偏振分束器的输入端口相连;偏振分束器的输出端口分别与光延迟线和可调光衰减器的输入端口相连;光延迟线和可调光衰减器的输出端口与偏振合束器输入端口相连;偏振合束器输出端口与光电探测器的输入端口相连;光电探测器输出电信号。FIG. 1 is a schematic diagram of a method for estimating the angle of arrival of a broadband microwave signal based on microwave photon filtering according to the present invention. The polarization multiplexed Mach-Zehnder modulator modulates the microwave signal to generate a polarization multiplexed signal; the polarization multiplexed Mach-Zehnder modulator consists of a Y splitter, an upper and lower parallel Mach-Zehnder modulator X- Composed of MZM and Y-MZM, 90° polarization rotator, and polarization beam combiner; the polarization controller is controlled to demultiplex the polarization multiplexed signal into two paths through the polarization beam splitter, and one path uses an optical delay line to introduce a relative time delay. The other uses a variable optical attenuator to minimize the power difference between the two branches; uses a polarization beam combiner to combine the two signals and outputs them to the photodetector; after the photodetector beats, the filtered signal can be obtained microwave signal. The output port of the laser source is connected to the input port of the polarization multiplexing Mach-Zehnder modulator, and the output port of the modulator is connected to the input port of the polarization controller; the output port of the polarization controller is connected to the input port of the polarization beam splitter; The output port of the beam splitter is connected with the input port of the optical delay line and the adjustable optical attenuator respectively; the output port of the optical delay line and the adjustable optical attenuator is connected with the input port of the polarization beam combiner; the output port of the polarization beam combiner is connected with the The input ports of the photodetectors are connected; the photodetectors output electric signals.
本实例中,方法的具体实施步骤是:In this example, the specific implementation steps of the method are:
步骤一:激光源产生波长为1552nm、功率为12dBm的连续光波,连续光波输入到半波电压为3.5V、插入损耗6dB的偏振复用马赫-曾德尔调制器中。任意波形生成器产生的1.6Gbps的不归零信号与微波信号生成器产生的18GHz本振混频,如图2(a)所示。混频后的信号分为两路分别输入到X-MZM和Y-MZM的射频端口。Step 1: The laser source generates a continuous light wave with a wavelength of 1552nm and a power of 12dBm, and the continuous light wave is input into a polarization multiplexing Mach-Zehnder modulator with a half-wave voltage of 3.5V and an insertion loss of 6dB. The 1.6Gbps non-return-to-zero signal generated by the arbitrary waveform generator is mixed with the 18GHz local oscillator generated by the microwave signal generator, as shown in Figure 2(a). The mixed signal is divided into two channels and input to the RF ports of X-MZM and Y-MZM respectively.
步骤二:偏振复用信号通过偏振控制器和偏振分束器解复用后分为两路,其中一路输入到光延时线,通过改变由光延时线引入的时间延迟来模拟到达角的变化。同时,记录与不同相对时间延迟对应的陷波频率,进行了两组测量。为了确定两路分支之间的初始时间延迟,将测量结果先用于校准。测量的频率偏移和相应的时间延迟如图3所示,斜率越大,固定频率测量误差将导致更大的时间延迟测量误差,理论曲线的斜率计算为-21.2ps/GHz。Step 2: The polarization multiplexed signal is demultiplexed by a polarization controller and a polarization beam splitter and then divided into two paths, one of which is input to the optical delay line, and the angle of arrival is simulated by changing the time delay introduced by the optical delay line Variety. Simultaneously, the notch frequencies corresponding to different relative time delays were recorded, and two sets of measurements were performed. To determine the initial time delay between the two branches, the measurement is first used for calibration. The measured frequency offset and the corresponding time delay are shown in Figure 3. The larger the slope, the greater the measurement error of the fixed frequency will lead to a larger measurement error of the time delay. The slope of the theoretical curve is calculated as -21.2ps/GHz.
步骤三:校准后通过电信号分析仪测量滤波后频率偏移量,计算相对时间延迟。图4显示了测量结果,其相应的测量误差小于±0.35ps。假设天线间隔为λ/2,则到达角的测量误差小于0.72°。的时间延迟范围为-14ps至16ps,对应的到达角范围为-30.26°至35.17°。Step 3: After calibration, measure the filtered frequency offset by an electrical signal analyzer, and calculate the relative time delay. Figure 4 shows the measurement results, which correspond to a measurement error of less than ±0.35ps. Assuming that the antenna spacing is λ/2, the measurement error of the angle of arrival is less than 0.72°. The time delay ranges from -14ps to 16ps, and the corresponding arrival angle ranges from -30.26° to 35.17°.
综上,本发明利用偏振复用马赫-曾德尔调制器、差分群延迟模块等实现基于微波光子滤波的宽带微波信号到达角估计,结构简单易于实现,价格低廉,不受电子瓶颈影响,可以在非相干条件下工作,这使得系统具有更好的鲁棒性。To sum up, the present invention utilizes polarization multiplexing Mach-Zehnder modulator, differential group delay module, etc. to realize the estimation of angle of arrival of broadband microwave signal based on microwave photon filtering. It works under non-coherent conditions, which makes the system more robust.
总之,以上所述实施方案仅为本发明的实施例而已,并非仅用于限定本发明的保护范围,应当指出,对于本技术领域的普通技术人员来说,在本发明公开的内容上,还可以做出若干等同变形和替换,该微波光子滤波器如果采用不同的差分群延迟值,测量能力不同,这些等同变形和替换以及频率范围的调整也应视为本发明保护的范围。In a word, the embodiments described above are only examples of the present invention, and are not only used to limit the protection scope of the present invention. Several equivalent deformations and replacements can be made. If the microwave photonic filter adopts different differential group delay values, the measurement capabilities will be different. These equivalent deformations and replacements as well as the adjustment of the frequency range should also be regarded as the protection scope of the present invention.
Claims (4)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201710655401.4A CN107528638B (en) | 2017-07-27 | 2017-07-27 | Estimation of Angle of Arrival for Broadband Microwave Signals Based on Microwave Photon Filtering |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201710655401.4A CN107528638B (en) | 2017-07-27 | 2017-07-27 | Estimation of Angle of Arrival for Broadband Microwave Signals Based on Microwave Photon Filtering |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN107528638A true CN107528638A (en) | 2017-12-29 |
| CN107528638B CN107528638B (en) | 2019-12-10 |
Family
ID=60680640
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201710655401.4A Active CN107528638B (en) | 2017-07-27 | 2017-07-27 | Estimation of Angle of Arrival for Broadband Microwave Signals Based on Microwave Photon Filtering |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN107528638B (en) |
Cited By (15)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN109725446A (en) * | 2019-03-12 | 2019-05-07 | 山东理工大学 | Microwave Photonic Transverse Filter Based on Single Wavelength and Multimode Fiber Delay Line Modules |
| CN109765702A (en) * | 2019-03-28 | 2019-05-17 | 山东理工大学 | Tunable multi-tap microwave photonic filter combining coherent and incoherent mechanisms |
| CN110350966A (en) * | 2019-06-26 | 2019-10-18 | 西南交通大学 | Wide-band microwave direction of arrival degree measuring device and method based on photon technology |
| CN111464241A (en) * | 2020-04-06 | 2020-07-28 | 陈浩 | Measuring system and measuring method for improving the accuracy of microwave signal arrival angle |
| CN111541483A (en) * | 2020-04-20 | 2020-08-14 | 苏州大学 | Optical signal-to-noise ratio monitoring method of coherent optical communication system based on high-order statistical moment |
| CN111698037A (en) * | 2020-06-08 | 2020-09-22 | 西安电子科技大学 | Single microwave signal direction-of-arrival angle estimation method based on microwave photons |
| CN111693932A (en) * | 2020-06-08 | 2020-09-22 | 西安电子科技大学 | Multi-microwave signal direction-of-arrival angle estimation method based on microwave photons |
| CN112104416A (en) * | 2019-06-17 | 2020-12-18 | 西安电子科技大学 | Double-parallel Mach-Zehnder modulator-based unambiguous arrival angle measurement method |
| CN112540341A (en) * | 2020-12-11 | 2021-03-23 | 南京航空航天大学 | Two-dimensional arrival angle measuring method and device |
| CN109257102B (en) * | 2018-09-30 | 2021-06-25 | 西南交通大学 | A Multi-Order Microwave Frequency Hopping Signal Generator Based on Photonic Technology |
| CN113391121A (en) * | 2020-03-13 | 2021-09-14 | 西安电子科技大学 | Method for realizing instantaneous frequency measurement based on frequency response monitoring |
| CN115085819A (en) * | 2022-07-26 | 2022-09-20 | 陕西浩兴坤达新能源科技有限公司 | A kind of information transmission method and system of natural electromagnetic pulse vector signal energy spectrum |
| CN115589263A (en) * | 2022-09-26 | 2023-01-10 | 贵州大学 | All-optical time domain integration system |
| CN117254859A (en) * | 2023-11-17 | 2023-12-19 | 鹏城实验室 | Coherent light transmission method and coherent light transmission system |
| CN120320853A (en) * | 2025-06-16 | 2025-07-15 | 浙江大学 | A silicon-based integrated device and measurement method for synchronous measurement of microwave frequency and arrival angle |
Family Cites Families (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0786972A (en) * | 1993-09-09 | 1995-03-31 | Nec Corp | Adaptive equalizer |
| CN1715952A (en) * | 2004-06-28 | 2006-01-04 | 上海无线电设备研究所 | Electronic angle tracing system for tracing microwave radiation source in air |
| CN105162523B (en) * | 2014-06-14 | 2017-09-22 | 西安电子科技大学 | Optics produces the device of microwave phase encoded signal |
| CN105675986B (en) * | 2016-02-03 | 2018-07-17 | 西安电子科技大学 | Angle-of- arrival estimation based on time frequency analysis narrow-band FM signal when shortage of data |
| CN106053938B (en) * | 2016-06-18 | 2018-09-28 | 西安电子科技大学 | The device and method that transient microwave frequency measures is realized using dual-polarization modulator |
| CN106953699B (en) * | 2016-11-04 | 2019-04-19 | 西安电子科技大学 | Methods for Broadband Microwave SSB Modulation in Photonics |
| CN106961252B (en) * | 2017-02-24 | 2019-08-20 | 西安电子科技大学 | A DPMZM Modulator Based Microwave Photon Image Suppression Downconversion Method |
-
2017
- 2017-07-27 CN CN201710655401.4A patent/CN107528638B/en active Active
Cited By (22)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN109257102B (en) * | 2018-09-30 | 2021-06-25 | 西南交通大学 | A Multi-Order Microwave Frequency Hopping Signal Generator Based on Photonic Technology |
| CN109725446B (en) * | 2019-03-12 | 2022-06-03 | 山东理工大学 | Microwave Photonic Transverse Filter Based on Single Wavelength and Multimode Fiber Delay Line Modules |
| CN109725446A (en) * | 2019-03-12 | 2019-05-07 | 山东理工大学 | Microwave Photonic Transverse Filter Based on Single Wavelength and Multimode Fiber Delay Line Modules |
| CN109765702A (en) * | 2019-03-28 | 2019-05-17 | 山东理工大学 | Tunable multi-tap microwave photonic filter combining coherent and incoherent mechanisms |
| CN112104416A (en) * | 2019-06-17 | 2020-12-18 | 西安电子科技大学 | Double-parallel Mach-Zehnder modulator-based unambiguous arrival angle measurement method |
| CN112104416B (en) * | 2019-06-17 | 2021-06-01 | 西安电子科技大学 | A ambiguity-free measurement method for angle of arrival based on dual parallel Mach-Zehnder modulators |
| CN110350966A (en) * | 2019-06-26 | 2019-10-18 | 西南交通大学 | Wide-band microwave direction of arrival degree measuring device and method based on photon technology |
| CN110350966B (en) * | 2019-06-26 | 2021-09-07 | 西南交通大学 | Device and method for measuring the angle of arrival of broadband microwave signal based on photonic technology |
| CN113391121A (en) * | 2020-03-13 | 2021-09-14 | 西安电子科技大学 | Method for realizing instantaneous frequency measurement based on frequency response monitoring |
| CN113391121B (en) * | 2020-03-13 | 2022-08-02 | 西安电子科技大学 | Method for realizing instantaneous frequency measurement based on frequency response monitoring |
| CN111464241A (en) * | 2020-04-06 | 2020-07-28 | 陈浩 | Measuring system and measuring method for improving the accuracy of microwave signal arrival angle |
| CN111464241B (en) * | 2020-04-06 | 2022-11-04 | 陈浩 | Measurement system and measurement method for improving precision of arrival angle of microwave signal |
| CN111541483A (en) * | 2020-04-20 | 2020-08-14 | 苏州大学 | Optical signal-to-noise ratio monitoring method of coherent optical communication system based on high-order statistical moment |
| CN111698037A (en) * | 2020-06-08 | 2020-09-22 | 西安电子科技大学 | Single microwave signal direction-of-arrival angle estimation method based on microwave photons |
| CN111693932A (en) * | 2020-06-08 | 2020-09-22 | 西安电子科技大学 | Multi-microwave signal direction-of-arrival angle estimation method based on microwave photons |
| CN112540341A (en) * | 2020-12-11 | 2021-03-23 | 南京航空航天大学 | Two-dimensional arrival angle measuring method and device |
| CN112540341B (en) * | 2020-12-11 | 2023-11-10 | 南京航空航天大学 | A two-dimensional arrival angle measurement method and device |
| CN115085819A (en) * | 2022-07-26 | 2022-09-20 | 陕西浩兴坤达新能源科技有限公司 | A kind of information transmission method and system of natural electromagnetic pulse vector signal energy spectrum |
| CN115085819B (en) * | 2022-07-26 | 2022-11-15 | 陕西浩兴坤达新能源科技有限公司 | A method and system for information transmission of natural electromagnetic pulse vector signal energy spectrum |
| CN115589263A (en) * | 2022-09-26 | 2023-01-10 | 贵州大学 | All-optical time domain integration system |
| CN117254859A (en) * | 2023-11-17 | 2023-12-19 | 鹏城实验室 | Coherent light transmission method and coherent light transmission system |
| CN120320853A (en) * | 2025-06-16 | 2025-07-15 | 浙江大学 | A silicon-based integrated device and measurement method for synchronous measurement of microwave frequency and arrival angle |
Also Published As
| Publication number | Publication date |
|---|---|
| CN107528638B (en) | 2019-12-10 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN107528638B (en) | Estimation of Angle of Arrival for Broadband Microwave Signals Based on Microwave Photon Filtering | |
| Zou et al. | Microwave frequency measurement based on optical power monitoring using a complementary optical filter pair | |
| CN109613335B (en) | Microwave signal frequency measurement device and method based on cyclic frequency shift | |
| CN103954356B (en) | A kind of optical device measurement of spectral response method, measuring system | |
| Pan et al. | Photonic approach to the simultaneous measurement of the frequency, amplitude, pulse width, and time of arrival of a microwave signal | |
| CN108616311B (en) | A device and method for frequency measurement based on Mach-Zehnder optical filter | |
| US10644806B2 (en) | Coherent optical receiver testing | |
| CN106093598B (en) | A system and method for measuring electromagnetic signal characteristics | |
| CN102638305A (en) | Optical single-side band modulation based optical device measuring method and optical single-side band modulation based optical device measuring device | |
| CN106850066A (en) | The device and method of Doppler shift measurement is realized based on dual-polarization modulator | |
| CN107085143A (en) | A photoelectric frequency response tester and test method | |
| Kang et al. | 6–40 GHz photonic microwave Doppler frequency shift measurement based on polarization multiplexing modulation and I/Q balanced detection | |
| CN106768896A (en) | Ultrahigh resolution light vector analysis method and device | |
| CN107634807A (en) | Optical vector analysis method and device based on chirp intensity modulation | |
| Chen et al. | Wideband Doppler frequency shift measurement and direction discrimination based on a DPMZM | |
| CN107947867B (en) | Single-sideband spectrum generation device and method based on multi-frequency phase modulation | |
| CN107741525A (en) | Photodetector Frequency Response Measuring Method and Device | |
| CN109084961A (en) | Optical device spectral response measurement method and device based on suppressed carrier frequency | |
| Meng et al. | Photonics-assisted simultaneous frequency and angle-of-arrival measurement using parameter mapping method | |
| US10389451B2 (en) | Coherent optical receiver testing | |
| CN117955557A (en) | A frequency and angle-of-arrival measurement method based on multi-path light undersampling phase shift analysis | |
| CN114964329A (en) | Double Sideband Optical Frequency Domain Reflectometer | |
| CN106452592A (en) | Tunable single pass band microwave photonics Hilbert transform filter system | |
| CN105353210B (en) | A kind of highly sensitive big bandwidth photon microwave frequency measurement apparatus and method | |
| Xue et al. | Ultrahigh-resolution optical vector analysis for arbitrary responses using low-frequency detection |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PB01 | Publication | ||
| PB01 | Publication | ||
| SE01 | Entry into force of request for substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| GR01 | Patent grant | ||
| GR01 | Patent grant |