CN105258920B - Detection method for loss of transmission optical fiber joint of Raman optical fiber amplifier - Google Patents
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Abstract
本发明提供一种拉曼光纤放大器传输光纤接头损耗的探测方法,其结构包括泵浦功率监测单元和带外ASE探测单元;其中,泵浦功率监测单元连接于中央控制处理器,且包括一功率探测器,该功率探测器通过WDM连接于功率耦合器;带外ASE探测单元包括ASE带探测器,且ASE带探测器连接至中央控制处理器,其步骤包括:第一步:设定初始泵浦光功率为P1;第二步:探测带外ASE功率值Pase1;第三步:设定泵浦光功率为P2;第四步:探测带外ASE功率值Pase2;第五步:程序自动收敛计算得到拉曼光纤放大器与传输光纤的接头损耗;在实际工作中,测量拉曼光纤放大器和传输光纤的接头损耗与工作带宽内的信号光功率无关;而且,通过此方法计算得到光纤接头损耗和传输光纤的衰减系数无关,一致性较好。
The present invention provides a method for detecting the loss of a Raman fiber amplifier transmission optical fiber joint. a detector, the power detector is connected to the power coupler through WDM; the out-of-band ASE detection unit includes an ASE band detector, and the ASE band detector is connected to the central control processor, and the steps include: the first step: setting an initial pump The pump optical power is P1; the second step: detect the out-of-band ASE power value Pase1; the third step: set the pump optical power to P2; the fourth step: detect the out-of-band ASE power value Pase2; the fifth step: the program automatically converges The joint loss of the Raman fiber amplifier and the transmission fiber is calculated; in practical work, the measured joint loss of the Raman fiber amplifier and the transmission fiber has nothing to do with the signal optical power within the working bandwidth; moreover, the optical fiber joint loss and The attenuation coefficient of the transmission fiber is irrelevant, and the consistency is good.
Description
技术领域technical field
本发明涉及一种拉曼光纤放大器,尤其是关于一种拉曼光纤放大器传输光纤接头损耗的探测方法。The invention relates to a Raman fiber amplifier, in particular to a method for detecting the loss of a Raman fiber amplifier transmission fiber joint.
背景技术Background technique
受激拉曼散射(SRS)是光纤中的一种非线性现象,其将一小部分入射光功率转移到频率比其低的斯托克斯波上;如果一个弱信号与一强泵浦光波同时在光纤中传输,并使弱信号波长置于泵浦光的拉曼增益带宽内,弱信号光就可以得到放大,这种基于受激拉曼散射机制的光放大器即称为光纤拉曼放大器(FRA)。Stimulated Raman Scattering (SRS) is a nonlinear phenomenon in optical fibers that transfers a small fraction of the incident optical power to a Stokes wave with a lower frequency; if a weak signal is simultaneous with a strong pump wave The weak signal light can be amplified by transmitting it in the fiber and placing the weak signal wavelength within the Raman gain bandwidth of the pump light. This kind of optical amplifier based on the stimulated Raman scattering mechanism is called a fiber Raman amplifier ( FRA).
对于分布式拉曼光纤放大器,一般通过定标增益和信号工作带宽外的某段波长内的自发辐射放大光功率来控制增益。如果传输光纤和拉曼光纤放大器之间存在较大的接头损耗,就会影响到自发辐射光功率和增益之间的定标关系,从而造成较大的增益误差,因此需对拉曼光纤放大器与传输光纤之间的接头损耗进行精确测量。For distributed Raman fiber amplifiers, the gain is generally controlled by scaling the gain and the amplified optical power of spontaneous emission within a certain wavelength outside the working bandwidth of the signal. If there is a large joint loss between the transmission fiber and the Raman fiber amplifier, it will affect the scaling relationship between the spontaneous emission optical power and the gain, resulting in a large gain error. Accurate measurement of splice loss between transmission fibers.
专利CN102749783中阐述了一种利用带外自发辐射放大光功率和泵浦光功率之间的数学关系,及确定接头损耗与带外自发辐射放大光功率之间的数学关系确定接头损耗值。但是,这种方法的局限性在于,通过计算得到的光纤接头损耗和传输光纤的损耗有关,而不是同批次的光纤之间存在一定的损耗差异,这就导致了计算得到的光纤接头损耗存在一定误差。Patent CN102749783 describes a mathematical relationship between the amplified optical power of the out-of-band spontaneous emission and the pump optical power, and the mathematical relationship between the joint loss and the out-of-band spontaneous emission amplified optical power to determine the joint loss value. However, the limitation of this method is that the calculated fiber splice loss is related to the loss of the transmission fiber, rather than a certain loss difference between fibers in the same batch, which leads to the existence of the calculated fiber splice loss. certain error.
发明内容SUMMARY OF THE INVENTION
为避免光纤损耗差异造成光纤接头损耗误差,本发明提供一种拉曼光纤放大器传输光纤接头损耗的探测方法。In order to avoid optical fiber splice loss errors caused by differences in optical fiber loss, the present invention provides a method for detecting the loss of a Raman optical fiber amplifier transmission optical fiber splice.
为了达到上述发明目的,本发明提供的技术方案如下:一种拉曼光纤放大器传输光纤接头损耗的探测方法,其结构包括泵浦功率监测单元和带外ASE探测单元;其中,泵浦功率监测单元连接于中央控制处理器,且包括一功率探测器,该功率探测器通过WDM连接于功率耦合器;带外ASE探测单元包括ASE带探测器,且ASE带探测器连接至中央控制处理器,其步骤包括:In order to achieve the above-mentioned purpose of the invention, the technical scheme provided by the present invention is as follows: a method for detecting the loss of a Raman fiber amplifier transmission optical fiber joint, the structure of which includes a pump power monitoring unit and an out-of-band ASE detection unit; wherein, the pump power monitoring unit Connected to the central control processor, and includes a power detector, the power detector is connected to the power coupler through WDM; the out-of-band ASE detection unit includes an ASE band detector, and the ASE band detector is connected to the central control processor, which is Steps include:
第一步:设定初始泵浦光功率为P1;Step 1: Set the initial pump light power as P1;
第二步:探测带外ASE功率值Pase1;The second step: detect the out-of-band ASE power value Pase1;
第三步:设定泵浦光功率为P2;Step 3: Set the pump optical power to P2;
第四步:探测带外ASE功率值Pase2;Step 4: Detect the out-of-band ASE power value Pase2;
第五步:程序自动收敛计算得到拉曼光纤放大器与传输光纤的接头损耗。Step 5: The program automatically converges to calculate the splice loss between the Raman fiber amplifier and the transmission fiber.
其中,优选实施方式为:对多泵浦拉曼光纤放大器,泵浦光功率设置为短波长泵浦功率、或多个泵浦光的功率之和,泵浦功率监测单元的功率探测器探测功率耦合器分离出的部分泵浦光的功率值并传送至中央控制处理器。Wherein, the preferred embodiment is: for a multi-pump Raman fiber amplifier, the pump optical power is set to the short-wavelength pump power or the sum of the powers of multiple pump lights, and the power detector of the pump power monitoring unit detects the power The power value of part of the pump light separated by the coupler is sent to the central control processor.
其中,优选实施方式为:带外ASE探测单元利用功率耦合器和滤波器将部分信号带宽之外的ASE光抽离,并将抽离的ASE光传输至ASE带探测器,ASE带探测器将该功率值传送至中央控制处理器,计算出实际系统中的带款范围内的ASE功率值。Among them, the preferred embodiment is: the out-of-band ASE detection unit uses a power coupler and a filter to extract the ASE light outside part of the signal bandwidth, and transmits the extracted ASE light to the ASE-band detector, and the ASE-band detector will The power value is sent to the central control processor to calculate the ASE power value within the range of the actual system.
本发明的一种拉曼光纤放大器传输光纤接头损耗的探测方法相比于现有技术来说具有以下优点和积极效果:在实际工作中,测量拉曼光纤放大器和传输光纤的接头损耗与工作带宽内的信号光功率无关;而且,通过此方法计算得到光纤接头损耗和传输光纤的衰减系数无关,一致性较好。Compared with the prior art, the method for detecting the splice loss of the Raman fiber amplifier transmission fiber of the present invention has the following advantages and positive effects: in actual work, the splice loss and working bandwidth of the Raman fiber amplifier and the transmission fiber are measured. The optical power of the signal inside is irrelevant; moreover, the fiber splice loss calculated by this method has nothing to do with the attenuation coefficient of the transmission fiber, and the consistency is good.
附图说明Description of drawings
图1为泵浦方式RFA应用于通信系统的示意图。FIG. 1 is a schematic diagram of a pumped RFA applied to a communication system.
图2为本发明的拉曼光纤放大器的功能模块结构示意图。FIG. 2 is a schematic structural diagram of a functional module of the Raman fiber amplifier of the present invention.
图3为本发明的拉曼光纤放大器传输光纤接头损耗的探测方法的流程示意图。FIG. 3 is a schematic flowchart of a method for detecting the loss of a Raman fiber amplifier transmission fiber splice according to the present invention.
具体实施方式Detailed ways
为使对本发明的目的、构造特征及其功能有进一步的了解,配合附图详细说明如下。应当理解,此部分所描述的具体实施例仅可用以解释本发明,并不用于限定本发明。In order to have a further understanding of the purpose, structural features and functions of the present invention, the following detailed description is provided in conjunction with the accompanying drawings. It should be understood that the specific embodiments described in this section are only used to explain the present invention, but not to limit the present invention.
如图1所示,以采用后向泵浦方式的分布式拉曼光纤放大器(RFA)为例,图中RFA的泵浦10光的初始功率设为P1;正向传输的为信号光S1;其中,信号光S1从远端发射,经过长距离的传输光纤110传输至RFA输入端I1,经RFA输出端O1输出。其中,RFA的输入端I1既是信号光S1的输入端,同时也是RFA泵浦光P1的输出端。As shown in Figure 1, taking the distributed Raman fiber amplifier (RFA) using the backward pumping method as an example, the initial power of the pump 10 light of the RFA in the figure is set to P1; the forward transmission is the signal light S1; The signal light S1 is emitted from the remote end, transmitted to the RFA input end I1 through the long-distance transmission fiber 110, and output through the RFA output end O1. Among them, the input end I1 of the RFA is not only the input end of the signal light S1, but also the output end of the RFA pump light P1.
请同时参照图2,图2为本发明的拉曼光纤放大器中的激光功能模块500,该功能模块500包括泵浦功率监测单元510和带外ASE探测单元530。其中,泵浦功率监测单元510连接于中央控制处理器,其包括一功率探测器,该功率探测器通过RFA100的WDM连接于RFA的功率耦合器。其中,带外ASE探测单元530包括ASE带探测器,且ASE带探测器连接至中央控制处理器。Please refer to FIG. 2 at the same time. FIG. 2 is a laser functional module 500 in the Raman fiber amplifier of the present invention. The functional module 500 includes a pump power monitoring unit 510 and an out-of-band ASE detection unit 530 . The pump power monitoring unit 510 is connected to the central control processor, and includes a power detector, and the power detector is connected to the power coupler of the RFA through the WDM of the RFA100. The out-of-band ASE detection unit 530 includes an ASE band detector, and the ASE band detector is connected to the central control processor.
请参照图3,本发明的拉曼光纤放大器传输光纤接头损耗(Connector Loss)的探测方法,包括以下步骤:Please refer to Fig. 3, the detection method of the Raman fiber amplifier transmission fiber connector loss (Connector Loss) of the present invention, comprises the following steps:
首先,设定初始泵浦10光功率为P1,单位为mW;对多泵浦拉曼光纤放大器,P1设置为短波长泵浦功率、或多个泵浦光的功率之和,泵浦功率监测单元510的功率探测器探测RFA的功率耦合器分离出的部分泵浦光的功率值并传送至中央控制处理器;First, set the initial pump 10 optical power as P1, in mW; for multi-pump Raman fiber amplifiers, set P1 as the short-wavelength pump power or the sum of the powers of multiple pump lights, and the pump power is monitored. The power detector of the unit 510 detects the power value of the partial pump light separated by the power coupler of the RFA and transmits it to the central control processor;
其次,探测带外ASE功率值Pase1,单位为dBm;带外ASE探测单元530利用功率耦合器和滤波器将部分信号带宽之外的ASE光抽离,并将抽离的ASE光传输至ASE带探测器,ASE带探测器探测出带外ASE功率值Pase1并传送至中央控制处理器;Secondly, detect the out-of-band ASE power value Pase1, the unit is dBm; the out-of-band ASE detection unit 530 uses a power coupler and a filter to extract the ASE light outside part of the signal bandwidth, and transmits the extracted ASE light to the ASE band The detector, the ASE band detector detects the out-of-band ASE power value Pase1 and transmits it to the central control processor;
再次,设定泵浦10光功率为P2,单位为mW;对多泵浦拉曼光纤放大器,P2设置为短波长泵浦功率、或多个泵浦光的功率之和,泵浦功率监测单元510的功率探测器探测RFA的功率耦合器分离出的部分泵浦光的功率值并传送至中央控制处理器;Again, set the pump 10 optical power as P2, in mW; for multi-pump Raman fiber amplifiers, set P2 as the short-wavelength pump power, or the sum of the powers of multiple pump lights, the pump power monitoring unit The power detector of 510 detects the power value of part of the pump light separated by the power coupler of the RFA and transmits it to the central control processor;
然后,探测带外ASE功率值Pase2,单位为dBm;带外ASE探测单元530利用功率耦合器和滤波器将部分信号带宽之外的ASE光抽离,并将抽离的ASE光传输至ASE带探测器,ASE带探测器探测出带外ASE功率值Pase1并传送至中央控制处理器;Then, detect the out-of-band ASE power value Pase2, the unit is dBm; the out-of-band ASE detection unit 530 uses a power coupler and a filter to extract the ASE light outside part of the signal bandwidth, and transmits the extracted ASE light to the ASE band The detector, the ASE band detector detects the out-of-band ASE power value Pase1 and transmits it to the central control processor;
最后,通过计算得到拉曼光纤放大器与传输光纤的接头损耗LossCon;其计算方法详细解释如下:Finally, the joint loss LossCon of the Raman fiber amplifier and the transmission fiber is obtained by calculation; the calculation method is explained in detail as follows:
拉曼光纤放大器在主光路中自发辐射ASE项为2h*ν*Δν*gR*Pp,其中h为普朗克常量,ν为自发辐射光频率,Δν为自发辐射相对于泵浦光的拉曼频移,gR为拉曼增益系数,Pp为泵浦光功率。The spontaneous emission ASE term of the Raman fiber amplifier in the main optical path is 2h*ν*Δν*gR*Pp, where h is Planck's constant, ν is the frequency of the spontaneous emission, and Δν is the Raman of the spontaneous emission relative to the pump light frequency shift, gR is the Raman gain coefficient, and Pp is the pump light power.
设G(ratio)为拉曼放大器的线性开关增益,当G(ratio)>>1时,对ASE功率作一系列近似后可得:Let G(ratio) be the linear switching gain of the Raman amplifier, when G(ratio)>>1, after a series of approximations to the ASE power, we can get:
Pase(dBm)=10*log10(G(ratio)-1)+a (1)Pase(dBm)=10*log10(G(ratio)-1)+a(1)
其中Pase(dBm)为ASE功率,单位为dBm;a是一个和光纤有效长度,拉曼增益系数相关的一个参数,其和泵浦功率,光纤衰减系数无关;Among them, Pase (dBm) is the ASE power in dBm; a is a parameter related to the effective length of the fiber and the Raman gain coefficient, which is independent of the pump power and the fiber attenuation coefficient;
而对G(ratio)存在下式:And there is the following formula for G(ratio):
G(ratio)=exp(gR*Pp*Leff/Aeff) (2)G(ratio)=exp(gR*Pp*Leff/Aeff) (2)
其中gR为拉曼增益系数,Pp为泵浦光功率,单位为mW;Leff为光纤的有效长度,Aeff为光纤的有效面积。如果G(ratio)的单位为dB,那么G(ratio)和泵浦功率Pp则成线性关系,Where gR is the Raman gain coefficient, Pp is the pump light power, in mW; Leff is the effective length of the fiber, and Aeff is the effective area of the fiber. If the unit of G(ratio) is dB, then there is a linear relationship between G(ratio) and the pump power Pp,
设Pase(mW)=10^(Pase(dBm)/10),单位为mW,根据(1)式,通过定标可以Set Pase(mW)=10^(Pase(dBm)/10), the unit is mW, according to the formula (1), the calibration can be
得到G(ratio)=ga1*Pase(mW)+ga2+1 (3)Get G(ratio)=ga1*Pase(mW)+ga2+1 (3)
其中ga1,ga2为与光纤损耗无关的定标系数。Among them, ga1 and ga2 are scaling coefficients independent of fiber loss.
首先将泵浦功率设置为P1,测量此时带外ASE功率Pase1(dBm),对应的线性开关增益为G1(ratio);随后将泵浦功率设置到P2,有P2>P1,取P2为P1的两倍,记录下此时的带外ASE功率Pase2(dBm),对应的线性开关增益为G2(ratio)。First, set the pump power to P1, measure the out-of-band ASE power Pase1 (dBm), and the corresponding linear switch gain is G1 (ratio); then set the pump power to P2, if P2>P1, take P2 as P1 twice, record the out-of-band ASE power Pase2 (dBm) at this time, and the corresponding linear switch gain is G2 (ratio).
由公式(2)式可得It can be obtained from formula (2)
10*log(G1(ratio))*P2/P1-10*log(G2(ratio))=0 (4)10*log(G1(ratio))*P2/P1-10*log(G2(ratio))=0 (4)
设拉曼光纤放大器与传输光纤的接头损耗为LossCon,单位为dB,对光纤接头损耗之前的Pase(mW)可折算如下Suppose the joint loss between the Raman fiber amplifier and the transmission fiber is LossCon, the unit is dB, and the Pase (mW) before the fiber joint loss can be converted as follows
Pase(mW)=10^((Pase(dBm)+LossCon)/10) (5)Pase(mW)=10^((Pase(dBm)+LossCon)/10) (5)
公式(5)式代入公式(3)可得到Substitute formula (5) into formula (3) to get
G(ratio)=ga1*10^((Pase(dBm)+LossCon)/10)+ga2+1 (6)G(ratio)=ga1*10^((Pase(dBm)+LossCon)/10)+ga2+1 (6)
公式(6)式代入公式(4)可得到Substitute formula (6) into formula (4) to get
10*log(ga1*10^((Pase1(dBm)+LossCon)/10)+ga2+1)*P2/P110*log(ga1*10^((Pase1(dBm)+LossCon)/10)+ga2+1)*P2/P1
-10*log(ga1*10^((Pase2(dBm)+LossCon)/10)+ga2+1)=Error (7)-10*log(ga1*10^((Pase2(dBm)+LossCon)/10)+ga2+1)=Error (7)
Error为误差,用迭代法求LossCon使得Error=0Error is the error, use the iterative method to find LossCon so that Error=0
设置收敛因子ke,使Set the convergence factor ke so that
LossCon=LossCon+Error*ke;LossCon=LossCon+Error*ke;
程序将自动收敛计算得到拉曼光纤放大器与传输光纤的接头损耗LossCon。The program will automatically converge to calculate the joint loss LossCon of the Raman fiber amplifier and the transmission fiber.
本发明的一种拉曼光纤放大器传输光纤接头损耗的探测方法相比于现有技术来说具有以下优点和积极效果:在实际工作中,测量拉曼光纤放大器和传输光纤的接头损耗与工作带宽内的信号光功率无关;而且,通过此方法计算得到光纤接头损耗和传输光纤的衰减系数无关,一致性较好。Compared with the prior art, the method for detecting the splice loss of the Raman fiber amplifier transmission fiber of the present invention has the following advantages and positive effects: in actual work, the splice loss and working bandwidth of the Raman fiber amplifier and the transmission fiber are measured. The optical power of the signal inside is irrelevant; moreover, the fiber splice loss calculated by this method has nothing to do with the attenuation coefficient of the transmission fiber, and the consistency is good.
以上所述,仅为本发明最佳实施例而已,并非用于限制本发明的范围,凡依本发明申请专利范围所作的等效变化或修饰,皆为本发明所涵盖。The above descriptions are only the best embodiments of the present invention, and are not intended to limit the scope of the present invention. Any equivalent changes or modifications made according to the scope of the patent application of the present invention are all covered by the present invention.
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CN108833003B (en) * | 2018-06-27 | 2021-01-08 | 武汉光迅科技股份有限公司 | Method and device for acquiring equivalent 0km joint loss of optical fiber attenuation coefficient in Raman optical fiber amplifier |
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CN104104428A (en) * | 2013-04-15 | 2014-10-15 | 昂纳信息技术(深圳)有限公司 | Laser safety protection device and method applied to distributed Raman fiber amplifier |
CN104242036A (en) * | 2014-10-11 | 2014-12-24 | 无锡市中兴光电子技术有限公司 | Raman fiber amplifier and automatic gain control method thereof |
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