CN104618013B - A kind of related optical time domain reflectometer based on all -fiber wide range chaos light source - Google Patents
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Abstract
该发明公开了一种基于全光纤宽谱混沌光源的相关光时域反射仪,涉及混沌光纤激光器及光时域反射仪领。该反射仪包括:全光纤混沌光源和相关型光时域反射系统;相关型光时域反射系统包括:可调衰减器、光滤波器、耦合器、环行器、光电探测器、示波器;全光纤混沌光源的出射光射入相关型光时域反射系统,首先依次通过可调衰减器、光滤波器、耦合器,通过耦合器的混沌光信号被分为参考信号和探测信号,参考信号直接由光电探测器转换为电信号由示波器采集并存储;探测信号经过环形器实现反射仪功能,反射信号被另一光电探测器转换为电信号后由同一示波器采集并存储。具有系统结构简单、稳定性高、能同时实现传感高分辨率、距离长的效果。
The invention discloses a correlated optical time domain reflectometer based on an all-fiber wide-spectrum chaotic light source, and relates to the fields of chaotic fiber lasers and optical time domain reflectometers. The reflectometer includes: all-fiber chaotic light source and related optical time-domain reflection system; related optical time-domain reflectometry system includes: adjustable attenuator, optical filter, coupler, circulator, photodetector, oscilloscope; all-fiber The output light of the chaotic light source is injected into the correlation type optical time domain reflection system, and first passes through the adjustable attenuator, the optical filter, and the coupler in turn, and the chaotic optical signal passing through the coupler is divided into a reference signal and a detection signal, and the reference signal is directly obtained by the The photoelectric detector is converted into an electrical signal and collected and stored by an oscilloscope; the detection signal is passed through a circulator to realize the function of a reflector, and the reflected signal is converted into an electrical signal by another photodetector and then collected and stored by the same oscilloscope. The invention has the advantages of simple system structure, high stability, high resolution sensing and long distance at the same time.
Description
技术领域technical field
本发明涉及混沌光纤激光器及光时域反射仪领域,尤其是一种基于全光纤宽带混沌激光器的相关型光时域反射仪。The invention relates to the fields of chaotic fiber lasers and optical time domain reflectometers, in particular to a correlation type optical time domain reflectometer based on full fiber broadband chaotic lasers.
背景技术Background technique
随着信息社会的发展,光纤通信和传感网络越来越庞大,在人们的生活中也扮演着越来越重要的角色。对于光网络和器件而言,光反射仪技术是一种重要的故障诊断手段,在这种背景下,光反射仪技术的发展得到了越来越多的关注。With the development of the information society, optical fiber communication and sensor networks are becoming larger and larger, and they are playing an increasingly important role in people's lives. For optical networks and devices, optical reflectometer technology is an important means of fault diagnosis. In this context, the development of optical reflectometer technology has received more and more attention.
光反射仪技术主要包括三种:光时域反射、低相干频域反射、相干光频域反射。这三种光反射仪技术在测量距离、空间分辨率、探测灵敏度以及精度等各指标上都有制约。比如说,低相干频域反射技术有极高的探测灵敏度,亚毫米级的空间分辨率,但是其探测距离通常不超过数米;而光时域反射技术通常用于长距离甚至超长距离(数十公里)的应用场合,但是分辨率较低,通常只能到米量级;光频域反射仪技术通过基于扫频光源的零差相干检测技术可以实现毫米级的传感精度并能达到数公里的传感距离。Optical reflectometer technology mainly includes three types: optical time domain reflectometry, low coherent frequency domain reflectometry, and coherent optical frequency domain reflectometry. These three optical reflectometer technologies are restricted in various indicators such as measurement distance, spatial resolution, detection sensitivity and accuracy. For example, low-coherence frequency-domain reflectometry has extremely high detection sensitivity and submillimeter-level spatial resolution, but its detection distance usually does not exceed several meters; while optical time-domain reflectometry is usually used for long distances or even ultra-long distances ( Tens of kilometers) applications, but the resolution is low, usually only to the meter level; optical frequency domain reflectometer technology can achieve millimeter-level sensing accuracy and reach Sensing distance of several kilometers.
可以说光频域反射仪技术的综合探测传感能力居于另两种技术之间,是他们的一种有效补充。但是,光频域反射技术需要精细的扫频光源和零差相干检测,其技术难度相比光时域反射技术而言更大,低相干频域反射技术基本上不可能做到长距离传感。在先技术CN101226100A利用LD泵浦的混沌光源实现了6cm传感精度,但受其信号功率和探测器增益限制,其传感距离仅数十米。It can be said that the comprehensive detection and sensing capability of optical frequency domain reflectometer technology is between the other two technologies, and it is an effective supplement to them. However, optical frequency domain reflectometry requires fine frequency-sweeping light sources and homodyne coherent detection, and its technical difficulty is greater than that of optical time domain reflectometry, and low-coherence frequency domain reflectometry is basically impossible for long-distance sensing . The prior technology CN101226100A uses LD-pumped chaotic light source to achieve 6cm sensing accuracy, but limited by its signal power and detector gain, its sensing distance is only tens of meters.
本发明所述的全光纤宽带混沌光源和利用半导体激光器泵浦的混沌激光器相比,拥有更大的带宽,更简易的设置,可以实现数十公里的传感长度,厘米量级的分辨率。Compared with the chaotic laser pumped by the semiconductor laser, the all-fiber broadband chaotic light source of the present invention has a larger bandwidth and simpler setting, and can realize a sensing length of tens of kilometers and a centimeter-level resolution.
而本发明所述的基于全光纤宽谱混沌光源的相关光时域反射仪利用全光纤器件产生的宽带连续混沌光信号分别作参考信号和探测信号,再将反射信号和参考信号做互相关运算即可探测定位光纤网络的断点。其定位精度可以达到厘米甚至毫米量级,传感长度达到数十公里。And the correlative optical time domain reflectometer based on the all-fiber wide-spectrum chaotic light source of the present invention utilizes the wide-band continuous chaotic optical signal produced by all-fiber devices as reference signal and detection signal respectively, and then performs cross-correlation calculation on the reflected signal and reference signal The breakpoint of the optical fiber network can be detected and located. Its positioning accuracy can reach the order of centimeters or even millimeters, and the sensing length can reach tens of kilometers.
发明内容Contents of the invention
本发明的目的是针对背景技术的光反射仪技术存在的问题,提供一种系统结构简单、稳定性高、能同时实现传感高分辨率、距离长的相关型光时域反射仪。The purpose of the present invention is to provide a correlation type optical time domain reflectometer with simple system structure, high stability, high resolution sensing and long distance, aiming at the problems existing in the optical reflectometer technology in the background technology.
本发明的技术方案是一种基于全光纤宽谱混沌光源的相关光时域反射仪,该反射仪包括:全光纤混沌光源和相关型光时域反射系统;所述相关型光时域反射系统包括:可调衰减器、光 滤波器、耦合器、环行器、光电探测器、示波器;所述全光纤混沌光源的出射光射入相关型光时域反射系统,首先依次通过可调衰减器、光滤波器、耦合器,通过耦合器的混沌光信号被分为参考信号和探测信号,参考信号直接由光电探测器转换为电信号由示波器采集并存储;探测信号经过环形器实现反射仪功能,反射信号被另一光电探测器转换为电信号后由同一示波器采集并存储。The technical solution of the present invention is a correlated optical time-domain reflectometer based on an all-fiber wide-spectrum chaotic light source, which includes: an all-fiber chaotic light source and a correlated optical time-domain reflection system; Including: an adjustable attenuator, an optical filter, a coupler, a circulator, a photodetector, and an oscilloscope; the outgoing light of the all-fiber chaotic light source is injected into a related optical time domain reflection system, and first passes through the adjustable attenuator, Optical filter, coupler, the chaotic optical signal passing through the coupler is divided into reference signal and detection signal, the reference signal is directly converted into an electrical signal by the photodetector and collected and stored by the oscilloscope; the detection signal realizes the reflectometer function through the circulator, The reflected signal is converted into an electrical signal by another photodetector and collected and stored by the same oscilloscope.
所述全光纤混沌光源包括:拉曼泵浦光源、光隔离器、零色散位移光纤,拉曼泵浦光源发出的泵浦光依次通过光隔离器、零色散位移光纤。The all-fiber chaotic light source includes: a Raman pump light source, an optical isolator, and a zero-dispersion-shifted optical fiber. The pump light emitted by the Raman pump light source passes through the optical isolator and the zero-dispersion-shifted optical fiber in sequence.
所述零色散位移光纤长度的长度为10~20km。The length of the zero-dispersion-shifted optical fiber is 10-20 km.
所述全光纤混沌光源中拉曼泵浦光源为1455nm拉曼泵浦光源。The Raman pumping light source in the all-fiber chaotic light source is a 1455nm Raman pumping light source.
综上所述,由于采用了上述技术方案,本发明的有益效果是:In summary, owing to adopting above-mentioned technical scheme, the beneficial effect of the present invention is:
1.本发明采用全光纤化的宽带混沌光源,利用拉曼光纤激光器泵浦零色散位移光纤实现超宽带的混沌光源输出,相比传统的半导体激光器泵浦产生的混沌光源,其结构更简单,输出带宽更大,能实现更高精度的空间分辨率;1. The present invention adopts an all-fiber broadband chaotic light source, and uses a Raman fiber laser to pump a zero-dispersion shifted optical fiber to realize an ultra-broadband chaotic light source output. Compared with a traditional semiconductor laser pumped chaotic light source, its structure is simpler. Larger output bandwidth can achieve higher precision spatial resolution;
2.因为输入信号是连续信号而非脉冲信号,所以所述基于全光纤宽谱混沌光源的相关光时域反射仪的空间分辨率不由信号脉宽决定,因此所述基于全光纤宽谱混沌光源的相关光时域反射仪可以在保证较高空间分辨率的情况下实现长距离的定位传感;2. Because the input signal is a continuous signal rather than a pulse signal, the spatial resolution of the correlated optical time domain reflectometer based on the full-fiber broadband chaotic light source is not determined by the pulse width of the signal, so the full-fiber wide-spectrum chaotic light source based on The correlative optical time domain reflectometer can realize long-distance positioning sensing while ensuring high spatial resolution;
3.本发明与现有技术相比,不用高性能的脉冲光源,也不用昂贵的电域随机信号发生器,成本更低,实用性更好。3. Compared with the prior art, the present invention does not need a high-performance pulse light source or an expensive electrical domain random signal generator, so the cost is lower and the practicability is better.
附图说明Description of drawings
本发明将通过例子并参照附图的方式说明,其中:The invention will be illustrated by way of example with reference to the accompanying drawings, in which:
图1是本发明所述基于全光纤宽谱混沌光源的相关光时域反射仪的结构示意图;Fig. 1 is the structural representation of the correlative optical time domain reflectometer based on the all-fiber broadband chaotic light source of the present invention;
图2是本发明实施例中的宽带全光纤混沌光源的光谱图;Fig. 2 is the spectrogram of the broadband all-fiber chaotic light source in the embodiment of the present invention;
图3是本发明实施例中的宽带全光纤混沌光源的时域图;Fig. 3 is the time-domain diagram of the broadband all-fiber chaotic light source in the embodiment of the present invention;
图4是本发明实施例中25km测试光纤的反射点定位结果,空间分辨率达到5.2cm,信噪比18dB。Fig. 4 is the reflection point positioning result of the 25km test optical fiber in the embodiment of the present invention, the spatial resolution reaches 5.2cm, and the signal-to-noise ratio is 18dB.
图1中:1.1455nm拉曼泵浦光源;2.光隔离器;3.零色散位移光纤;4.可调光衰减器;5.光滤波器;6.耦合器;7.光电探测器;8.环形器;9.光电探测器(同7);10.测试光纤(G.652);11.实时示波器。In Figure 1: 1. 1455nm Raman pump light source; 2. Optical isolator; 3. Zero dispersion shifted fiber; 4. Adjustable optical attenuator; 5. Optical filter; 6. Coupler; 7. Photodetector; 8. Circulator; 9. Photodetector (same as 7); 10. Test fiber (G.652); 11. Real-time oscilloscope.
具体实施方式detailed description
下面结合附图对本发明作详细说明。The present invention will be described in detail below in conjunction with the accompanying drawings.
如图1所示为本发明所述基于全光纤宽谱混沌光源的相关光时域反射仪结构示意图,该系统包括1455nm拉曼泵浦光源1、光隔离器2、零色散位移光纤3,1、2、3组成全光纤化的超宽带混沌光源;该系统还包括可调光衰减器4、光滤波器5、耦合器6、光电探测器7和9、环形器8;测试光纤(G.652)10和实时示波器11。所述零色散位移光纤3长度为16km,其长度决定超宽带混沌光源所需泵浦功率,在本发明所述中,零色散位移光纤3其长度应在10-20km之间。所述光滤波器5的中心波长为1550.2nm,3dB带宽为0.26nm。As shown in Figure 1, it is a schematic structural diagram of a correlated optical time domain reflectometer based on an all-fiber wide-spectrum chaotic light source according to the present invention. The system includes a 1455nm Raman pump light source 1, an optical isolator 2, and a zero-dispersion-shifted optical fiber 3,1. . 652)10 and real-time oscilloscope11. The length of the zero-dispersion-shifted optical fiber 3 is 16 km, and its length determines the pump power required by the ultra-broadband chaotic light source. In the present invention, the length of the zero-dispersion-shifted optical fiber 3 should be between 10-20 km. The center wavelength of the optical filter 5 is 1550.2nm, and the 3dB bandwidth is 0.26nm.
所述环形器8具有端口一、端口二和端口三,所述端口一与耦合器相连,所述端口二与测试光纤连接,所述端口三与光电探测器连接。The circulator 8 has port one, port two and port three, the port one is connected to the coupler, the port two is connected to the test fiber, and the port three is connected to the photodetector.
图2是本发明所述的全光纤混沌光源的光谱图,图3是本发明实施例中的宽带全光纤混沌光源的时域图;图4是本发明所述的探检测技术应用于25km光纤断点定位检测的实例结果。实验所用非零色散位移光纤全长15km,零色散位移波长为1440nm,色散斜率0.045ps/nm2/km,1455nm泵浦工作在正常色散区。随着泵浦功率逐渐增大,产生的混沌光源的带宽也逐渐增大,当泵浦功率达到1.48W时,混沌光源的带宽达到最大141nm(10dB带宽)。继续增大泵浦功率,由于受激拉曼散射的原因,功率逐渐向二阶和三阶斯托克斯光转移,并在1550nm到1650nm附近集聚。Fig. 2 is the spectrogram of the all-fiber chaotic light source of the present invention, and Fig. 3 is the time-domain diagram of the broadband all-fiber chaotic light source in the embodiment of the present invention; Fig. 4 is that the detection technology of the present invention is applied to 25km optical fiber Example results of breakpoint location detection. The non-zero dispersion-shifted fiber used in the experiment has a total length of 15km, the zero-dispersion-shifted wavelength is 1440nm, the dispersion slope is 0.045ps/nm 2 /km, and the 1455nm pump works in the normal dispersion region. As the pump power increases gradually, the bandwidth of the chaotic light source also increases gradually. When the pump power reaches 1.48W, the bandwidth of the chaotic light source reaches a maximum of 141nm (10dB bandwidth). Continue to increase the pump power, due to stimulated Raman scattering, the power gradually shifts to the second-order and third-order Stokes light, and gathers around 1550nm to 1650nm.
图3是本发明所述的基于全光纤宽谱混沌光源的相关光时域反射仪技术应用于25km测试光纤的定点测试结果图。拉曼泵浦光源为1.48W以使混沌光源有最大带宽输出。耦合器分束比为1:99,1%端输出作为参考光,99%端输出作为探测光。通过调节可调衰减器,使经过耦合器分束后的两路信号都有较合适的光功率,本实验中,1%端的输出功率为-17dBm,99%端输出功率为0.8dBm,光纤尾端以菲涅尔反射模拟断点,考虑反射率为4%,所述环形器三端口输出光功率为-25dBm。另外所用两个光电探测器为相同带宽的1GHz探测器,所用示波器为25GHz带宽,采样率设为25Gs/s。最终经过计算两路信号的互相关函数,得到图3所示的互相关曲线。互相关曲线的峰值处即光纤反射点位置,本发明所述技术准确测出光纤长度24768.94米,通过判断峰值曲线的半高全宽确定空间分辨率为5.2cm。Fig. 3 is a fixed-point test result diagram of the application of the correlative optical time domain reflectometer technology based on the all-fiber wide-spectrum chaotic light source according to the present invention to a 25km test fiber. The Raman pump light source is 1.48W so that the chaotic light source has the maximum bandwidth output. The splitting ratio of the coupler is 1:99, 1% end output is used as reference light, and 99% end output is used as probe light. By adjusting the adjustable attenuator, the two signals after splitting by the coupler have more appropriate optical power. In this experiment, the output power of the 1% end is -17dBm, and the output power of the 99% end is 0.8dBm. The Fresnel reflection is used to simulate the break point at the end, and the reflectivity is considered to be 4%, and the output optical power of the three ports of the circulator is -25dBm. In addition, the two photodetectors used are 1GHz detectors with the same bandwidth, the oscilloscope used has a bandwidth of 25GHz, and the sampling rate is set to 25Gs/s. Finally, after calculating the cross-correlation function of the two signals, the cross-correlation curve shown in Figure 3 is obtained. The peak of the cross-correlation curve is the position of the reflection point of the fiber. The technology of the present invention accurately measures the length of the fiber to 24768.94 meters, and the spatial resolution is determined to be 5.2 cm by judging the full width at half maximum of the peak curve.
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