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CN102636337A - Method for measuring optical fiber dispersion - Google Patents

Method for measuring optical fiber dispersion Download PDF

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CN102636337A
CN102636337A CN2012101251188A CN201210125118A CN102636337A CN 102636337 A CN102636337 A CN 102636337A CN 2012101251188 A CN2012101251188 A CN 2012101251188A CN 201210125118 A CN201210125118 A CN 201210125118A CN 102636337 A CN102636337 A CN 102636337A
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optical fiber
light
dispersion
sample
pump light
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许孝芳
李宏刚
高永锋
吕柳
任乃飞
周明
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Jiangsu University
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Abstract

本发明公开了一种测量光纤色散的方法,涉及光纤损耗测量领域。本发明基于飞秒激光泵浦探测技术,通过飞秒激光系统、分束镜、反射镜、时间延迟线、斩波器、光电探测器、锁相放大器、光纤、样品,以及计算机系统来实现。用光电探测器分别探测加载光纤前后,样品表面瞬态反射光的变化情况,得出两种情况下瞬态反射率变化发生突变的时刻,计算得到光纤的色散。本发明适用于不同材料的光纤色散的测量,装置结构简单,重复性好。

Figure 201210125118

The invention discloses a method for measuring optical fiber dispersion and relates to the field of optical fiber loss measurement. The invention is based on the femtosecond laser pumping and detection technology, and is realized by a femtosecond laser system, a beam splitter, a reflector, a time delay line, a chopper, a photodetector, a lock-in amplifier, an optical fiber, a sample, and a computer system. A photodetector is used to detect the change of the transient reflected light on the sample surface before and after loading the optical fiber, and the moment when the transient reflectance changes abruptly in the two cases is obtained, and the dispersion of the optical fiber is calculated. The invention is applicable to the measurement of optical fiber dispersion of different materials, and the device has simple structure and good repeatability.

Figure 201210125118

Description

一种测量光纤色散的方法A Method for Measuring Optical Fiber Dispersion

技术领域 technical field

本发明涉及光纤损耗测量领域,特指一种测量光纤色散的方法,适用于任何类型光纤色散的测量。 The invention relates to the field of optical fiber loss measurement, in particular to a method for measuring optical fiber dispersion, which is applicable to the measurement of any type of optical fiber dispersion.

背景技术 Background technique

众所周知,光通信的发展离不开光电子器件的发展,光通信中的许多传输器件要求具有良好的色散特性,光纤的高阶色散导致的啁啾直接影响到光脉冲的传输,同时也影响到光孤子的形成以及光脉冲的压缩。此外,全球业务量的飞速增长促使光纤通信容量和速率都需大幅度提高,这就要求对光纤的色散进行控制。因为由于色散的存在,不仅会使输出激光光脉冲发生展宽,特别是在ROF光通信中,会引起输出光幅度随光纤长度的变化而周期性变化,造成输出能量不稳定,输出误码率的增加。通常采用光纤光栅,波导微环谐振器等色散补偿器件来补偿光纤的色散。因此随着对光纤研究的日益深入和广泛的实用化,对光纤相关参数的测试已经成为急需解决的技术问题。而激光的出现,尤其是飞秒激光的出现,为各种测试技术发展提供了强有力的工具。飞秒激光具有超快时间响应和超高峰值的特性,一方面可以从根本上避免光在光纤中传输时热扩散的存在和影响,另一方面,使激光与物质的非线性相互作用占主导地位,因此飞秒激光具有高精度,三维方向的可控性等特点。飞秒激光与物质作用后,载流子的激发和弛豫都是超快过程,飞秒波谱技术的出发点是超短脉冲激光与物质的瞬态相干作用效应,利用它可以探测信号光场的振幅、位相和波矢,也可以测量物质与激光瞬态相干作用的其他信息,如激发态布居数的变化、电子运动以及原子核振动等方面的信息。发明专利“一种光纤光学器件色散测量装置与方法”(中国专利,专利申请号:201110268543.8)提供了一种基于微波光电子学方法的光纤光学色散测试系统和方法,使用的测试方法是基于光波干涉,主要是使光波信号经过具有色散的光纤光学器件,并在传输过程获得一定的光程差,经探测器后两个微波信号发生干涉,通过干涉信号与色散的关系来判断色散的大小。本发明利用飞秒激光作为测量用光源,提供了一种无需进行干涉的全新的色散测量方法,操作方便,数据处理简单,能够测量各种类型光纤的色散。 As we all know, the development of optical communication is inseparable from the development of optoelectronic devices. Many transmission devices in optical communication require good dispersion characteristics. The chirp caused by the high-order dispersion of optical fiber directly affects the transmission of optical pulses, and also affects the Soliton formation and compression of optical pulses. In addition, the rapid growth of global business volume requires a substantial increase in the capacity and rate of optical fiber communication, which requires the control of optical fiber dispersion. Because of the existence of dispersion, not only will the output laser light pulse be broadened, especially in ROF optical communication, it will cause the output light amplitude to change periodically with the change of the fiber length, resulting in unstable output energy and lower output bit error rate. Increase. Dispersion compensation devices such as fiber gratings and waveguide microring resonators are usually used to compensate the dispersion of optical fibers. Therefore, with the deepening of research on optical fiber and its wide application, the testing of related parameters of optical fiber has become a technical problem that needs to be solved urgently. The emergence of lasers, especially femtosecond lasers, provides a powerful tool for the development of various testing technologies. Femtosecond laser has the characteristics of ultra-fast time response and ultra-high peak value. On the one hand, it can fundamentally avoid the existence and influence of thermal diffusion when light is transmitted in the optical fiber. On the other hand, it makes the nonlinear interaction between laser and matter dominate. Therefore, the femtosecond laser has the characteristics of high precision and three-dimensional controllability. After the femtosecond laser interacts with matter, the excitation and relaxation of carriers are both ultrafast processes. The starting point of femtosecond spectroscopy technology is the transient coherent effect of ultrashort pulse laser and matter. It can be used to detect the signal light field Amplitude, phase and wave vector can also measure other information of matter and laser transient coherence, such as the change of excited state population number, electron motion and nuclear vibration. Invention patent "A Device and Method for Measuring Dispersion of Fiber Optic Devices" (Chinese patent, patent application number: 201110268543.8) provides a fiber optic dispersion test system and method based on microwave optoelectronics. The test method used is based on light wave interference , mainly to make the light wave signal pass through the fiber optic device with dispersion, and obtain a certain optical path difference during the transmission process. After passing through the detector, the two microwave signals interfere, and the size of the dispersion is judged by the relationship between the interference signal and the dispersion. The invention uses a femtosecond laser as a light source for measurement, provides a brand-new dispersion measurement method without interference, has convenient operation, simple data processing, and can measure the dispersion of various types of optical fibers.

发明内容 Contents of the invention

本发明要解决的技术问题是提出了一种基于飞秒激光泵浦探测技术的测量光纤色散的方法。利用飞秒激光超快能量密度和超快时间响应的特点,结合泵浦探测技术,能够准确的测量出光纤的色散。这种方法原理简单,操作方便,可重复性好,能测量各种类型光纤的色散,应用范围非常广泛。 The technical problem to be solved by the present invention is to propose a method for measuring fiber dispersion based on femtosecond laser pumping detection technology. Utilizing the characteristics of ultrafast energy density and ultrafast time response of femtosecond laser, combined with pump detection technology, the dispersion of optical fiber can be accurately measured. This method is simple in principle, easy to operate, good in repeatability, can measure the dispersion of various types of optical fibers, and has a wide range of applications.

本发明所采用的技术方案是,提供了一种测量光纤色散的方法,用泵浦光激发样品,样品内的电子吸收到激光能量后,产生电子的非平衡弛豫,表现为探测光瞬态发射率的发生突变。探测光用于表征样品表面的发射光的变化。通过探测器,锁相放大器和计算机系统对样品表面瞬态反射率信号进行采集、消噪、处理,绘制出了瞬态反射率变化(△R/R)曲线,根据△R/R值发生突变对应的步长计算出光纤的色散。 The technical solution adopted in the present invention is to provide a method for measuring optical fiber dispersion. The sample is excited by pump light. After the electrons in the sample absorb the laser energy, non-equilibrium relaxation of electrons occurs, which is manifested as a transient state of the probe light. A sudden change in emissivity. The probe light is used to characterize changes in the emitted light from the sample surface. Through the detector, lock-in amplifier and computer system, the transient reflectance signal of the sample surface is collected, denoised and processed, and the transient reflectance change (△R/R) curve is drawn, and a sudden change occurs according to the value of △R/R The corresponding step size calculates the dispersion of the fiber.

本发明提出的基于飞秒激光泵浦探测技术的测量光纤色散的方法主要包括以下内容: The method for measuring optical fiber dispersion based on femtosecond laser pumping detection technology proposed by the present invention mainly includes the following contents:

(1)           钛宝石飞秒激光系统发出的飞秒激光脉冲经过分束镜后被分成泵浦光和探测光两束,两者的能量密度比控制在10:1左右,泵浦光进入泵浦光传输通道,探测光进入探测光传输通道。 (1) The femtosecond laser pulse emitted by the titanium sapphire femtosecond laser system is divided into two beams, the pump light and the probe light, after passing through the beam splitter. The energy density ratio of the two is controlled at about 10:1, and the pump light enters the pump The light transmission channel, the detection light enters the detection light transmission channel.

(2)           在泵浦光传输通道中将连续的泵浦光由斩波器调制成断续方波序列脉冲。若测量的是加载光纤前的瞬态反射信号,则断续的方波泵浦光脉冲直接传输至聚焦透镜。若测量的是加载光纤后的瞬态反射信号,则从斩波器中输出的泵浦光脉冲先通过聚焦透镜聚焦入光纤传输,从光纤中出射后传输至聚焦透镜。 (2) In the pump light transmission channel, the continuous pump light is modulated by a chopper into a discontinuous square wave sequence pulse. If the measurement is the transient reflection signal before loading the fiber, the intermittent square-wave pump light pulse is directly transmitted to the focusing lens. If the measurement is the transient reflection signal after loading the optical fiber, the pump light pulse output from the chopper is first focused into the optical fiber through the focusing lens for transmission, and then transmitted to the focusing lens after exiting the optical fiber.

(3)           将探测光经由一个直角反射镜后,进入到时间延迟光路,主要是通过步进电机控制探测光的延迟时间,以使泵浦光和探测光之间形成一个光程差。 (3) After the probe light passes through a right-angle mirror, it enters the time-delay optical path. The delay time of the probe light is mainly controlled by a stepping motor, so that an optical path difference is formed between the pump light and the probe light.

(4)           泵浦光和探测光分别从各自的传输通道出射后经聚焦透镜会聚到样品表面同一点,表面反射光被探测器接收,进入锁相放大器和计算机系统。 (4) The pump light and the probe light are respectively emitted from their respective transmission channels and then converged to the same point on the sample surface through the focusing lens. The surface reflected light is received by the detector and enters the lock-in amplifier and the computer system.

(5)           通过计算机软件绘制薄膜瞬态反射率变化曲线,并根据曲线中反射率突变时刻对应的步长计算得出光纤的色散。 (5) Draw the change curve of the transient reflectance of the film through computer software, and calculate the dispersion of the optical fiber according to the step size corresponding to the sudden change of reflectivity in the curve.

该方法将灵敏度高,抗干扰能力强的飞秒激光泵浦探测技术用于对光纤的色散进行测试,将光纤色散测量系统置于实验室普通环境下,对材料样品表面(通常是金属薄膜,如铬、镍等)的超快反射率变化过程进行探测研究,从而计算出待测光纤的色散。通过这种技术得到实验数据精确度高、可靠性强,且测试方法简便,重复性好,适用于各种类型光纤色散的测量。 In this method, the femtosecond laser pumping detection technology with high sensitivity and strong anti-interference ability is used to test the dispersion of the optical fiber. Such as chromium, nickel, etc.) to detect and study the ultrafast reflectivity change process, so as to calculate the dispersion of the optical fiber to be tested. The experimental data obtained by this technique has high accuracy and strong reliability, and the test method is simple and repeatable, and is suitable for measuring the dispersion of various types of optical fibers.

附图说明 Description of drawings

本发明具体实施的结构框图及附图说明如下: The structural block diagram and accompanying drawing of the present invention are as follows:

图1光纤色散测量系统示意图; Figure 1 Schematic diagram of optical fiber dispersion measurement system;

图2 泵浦光传输通路示意图; Figure 2 Schematic diagram of the pump light transmission path;

图3探测光传输通路示意图; Figure 3 is a schematic diagram of the detection light transmission path;

图4 飞秒激光作用下的样品表面瞬态反射率变化曲线; Figure 4 The change curve of the transient reflectance of the sample surface under the action of femtosecond laser;

图中,1.钛宝石飞秒激光系统2.分束镜3.泵浦光传输通路4.聚焦透镜5.样品6.反射镜7.探测光传输通路8.计算机9.锁相放大器10.探测器11.斩波器12.聚焦镜13.光纤14.时间延迟线15.反射镜16.反射镜。 In the figure, 1. Ti:Sapphire femtosecond laser system 2. Beam splitter 3. Pump light transmission path 4. Focusing lens 5. Sample 6. Mirror 7. Detection light transmission path 8. Computer 9. Lock-in amplifier 10. Detector 11. Chopper 12. Focusing mirror 13. Optical fiber 14. Time delay line 15. Mirror 16. Mirror.

具体实施方式 Detailed ways

1、采用最大输出功率为5W的Vedi CW激光器作为钛宝石激光器的泵浦源,其工作波长为532nm,经锁模后得到的钛宝石飞秒激光的中心波长为800nm,重复频率为82 MHz,单脉冲宽度30fs,输出激光能量控制在330mW左右。 1. The Vedi CW laser with a maximum output power of 5W is used as the pump source of the Ti:Sapphire laser, and its working wavelength is 532nm. The center wavelength of the Ti:Sapphire femtosecond laser obtained after mode locking is 800nm, and the repetition frequency is 82 MHz. The single pulse width is 30fs, and the output laser energy is controlled at about 330mW.

2、飞秒激光系统1发出的飞秒激光束经过分束镜2后被分成泵浦光和探测光两束,泵浦光的光功率约300mW,能量较高,主要用于激发样品;探测光光功率约30mW,主要用于探测被激样品表面瞬态反射率的变化信号。 2. The femtosecond laser beam emitted by the femtosecond laser system 1 passes through the beam splitter 2 and is divided into two beams, the pump light and the probe light. The optical power of the pump light is about 300mW, and the energy is relatively high. The optical power is about 30mW, which is mainly used to detect the change signal of the transient reflectivity of the excited sample surface.

3、泵浦光首先经过斩波器11,对泵浦光以频率为2000 Hz进行调制,将连续的泵浦光调制成占空比为1:1的断续方波序列脉冲,然后将泵浦脉冲经聚焦透镜12后聚焦进入光纤13传输,从光纤13出射后经透镜4汇聚后作用于样品5表面。 3. The pump light first passes through the chopper 11, and the pump light is modulated at a frequency of 2000 Hz, and the continuous pump light is modulated into an intermittent square wave sequence pulse with a duty ratio of 1:1, and then the pump light is After passing through the focusing lens 12, the pump pulse is focused into the optical fiber 13 for transmission, emerges from the optical fiber 13, converges through the lens 4, and acts on the surface of the sample 5.

4、探测光首先经过反射镜6和反射镜15,然后进入时间延迟线14,时间延迟线主要由一个步进电机组成,运动精度1步,每步为10μm, 换算成时间分辨率为66.7fs,探测光经过步进电机后再经一个反射镜16出射,然后同样经透镜4会聚后作用于样品5表面。 4. The probe light first passes through the reflector 6 and reflector 15, and then enters the time delay line 14. The time delay line is mainly composed of a stepping motor, and the motion accuracy is 1 step, each step is 10 μm, and the converted time resolution is 66.7fs , the probe light passes through the stepping motor and then exits through a reflector 16 , and is also converged by the lens 4 before acting on the surface of the sample 5 .

5、样品5表面的泵浦光会聚光斑和探测光会聚光斑两者必须重叠在一起,光斑越小越好。 5. The converging spot of pump light and the converging spot of probe light on the surface of sample 5 must overlap together, and the smaller the spot, the better.

6、用探测器10探测样品5上的瞬态反射信号,并将它转换为电信号,然后输入锁相放大器9进行消噪处理,最后输入到计算机8,用计算机专用软件绘制样品表面的瞬态反射率(ΔR/R) 变化曲线。 6. Use the detector 10 to detect the transient reflection signal on the sample 5, and convert it into an electrical signal, then input it into the lock-in amplifier 9 for denoising processing, and finally input it into the computer 8, and draw the transient reflection signal on the surface of the sample with special computer software. State reflectivity (ΔR/R) change curve.

7、计算待测光纤的色散值。光纤色散,即光脉冲通过光纤后产生的时间延迟,用                                               

Figure 2012101251188100002DEST_PATH_IMAGE002
表示。在样品表面瞬态反射率变化曲线中,曲线的横坐标表示探测光发生瞬态反射时对应的具体时刻,用步长(step)表示,1步长等于66.7飞秒。测量泵浦光传输通道中不加光纤前样品表面瞬态反射率变化发生突变时对应的步长
Figure 2012101251188100002DEST_PATH_IMAGE004
,以及泵浦光传输通道中加载光纤后样品表面瞬态反射率发生突变时对应的步长
Figure 2012101251188100002DEST_PATH_IMAGE006
,光纤色散引起的时间延迟用步长表示即为:。根据色散定义:,即可求出光纤的色散
Figure 288565DEST_PATH_IMAGE002
。 7. Calculate the dispersion value of the optical fiber to be tested. Optical fiber dispersion, that is, the time delay generated after the light pulse passes through the optical fiber, is used
Figure 2012101251188100002DEST_PATH_IMAGE002
express. In the transient reflectance change curve of the sample surface, the abscissa of the curve indicates the specific moment when the probe light is transiently reflected, and is represented by a step, and one step is equal to 66.7 femtoseconds. Measure the step size corresponding to the sudden change in the transient reflectance of the sample surface before the optical fiber is added to the pump light transmission channel
Figure 2012101251188100002DEST_PATH_IMAGE004
, and the corresponding step size when the transient reflectance of the sample surface changes abruptly after the optical fiber is loaded in the pump light transmission channel
Figure 2012101251188100002DEST_PATH_IMAGE006
, the time delay caused by fiber dispersion is represented by the step size: . According to the definition of dispersion: , the dispersion of the fiber can be obtained
Figure 288565DEST_PATH_IMAGE002
.

Claims (3)

1. the method for a measuring optical fiber chromatic dispersion is characterized in that, concrete steps are following:
A, employing peak power output are the pumping source of the Vedi CW laser instrument of 5W as ti sapphire laser; Its operation wavelength is 532nm; The centre wavelength of the titanium jewel femtosecond laser that behind locked mode, obtains is 800nm; Repetition frequency is 82 MHz, single pulse width 30fs, and the output laser energy is controlled at about 330mW;
Be divided into pump light behind the femtosecond laser beam process beam splitter (2) that B, fs-laser system (1) send and survey light two bundles, the luminous power 300mW of pump light is used for excited sample; Survey light luminous power 30mW, be used to survey the variable signal that is swashed sample surfaces transient state reflectivity;
C, pump light at first pass through chopper (11); Is that 2000 Hz modulate to pump light with frequency; Continuous pump light is modulated into the interrupted square wave train pulse that dutycycle is 1:1; Then pumping pulse line focus lens (12) backs is focused on and gets into optical fiber (13) transmission, from optical fiber (13) outgoing after lens (4) act on sample (5) surface after converging;
D, detection light at first pass through catoptron (6) and catoptron (15); Entry time lag line (14) then, the time delay line mainly is made up of a stepper motor, 1 step of kinematic accuracy; Per step is 10 μ m; Being converted into temporal resolution is 66.7fs, surveys light through a warp catoptron (16) outgoing again behind the stepper motor, after lens (4) are assembled, acts on sample (5) surface equally then;
The pump light focused light spot on E, sample (5) surface overlaps with detection optical convergence hot spot;
F, survey the transient state reflected signal on the sample (5) with detector (10); And convert it into electric signal; Import lock-in amplifier (9) then and carry out denoising Processing; Be input to computing machine (8) at last, draw transient state reflectivity (Δ R/R) change curve of sample surfaces with the computing machine special software;
The dispersion values of G, calculating testing fiber; Fibre-optical dispersion; Be that the time delay that produces behind the optical fiber is passed through in light pulse; The expression with
Figure 567394DEST_PATH_IMAGE002
; Measure and not add step-length corresponding when sample surfaces transient state reflectance varies is undergone mutation before the optical fiber in the pump light transmission channel; And loading step-length corresponding when sample surfaces transient state reflectivity is undergone mutation behind the optical fiber in the pump light transmission channel, the time delay that fibre-optical dispersion causes is represented to be with step-length: .
2. the method for a kind of measuring optical fiber chromatic dispersion according to claim 1; It is characterized in that; Calculate the dispersion values of testing fiber, in sample surfaces transient state reflectance varies curve, the horizontal ordinate of curve representes to survey the corresponding concrete moment of light generation transient state reflex time; With step-length (step) expression, 1 step-length equals 66.7 femtoseconds.
3. the method for a kind of measuring optical fiber chromatic dispersion according to claim 2; It is characterized in that CHROMATIC DISPERSION IN FIBER OPTICS
Figure 536170DEST_PATH_IMAGE010
.
CN2012101251188A 2012-04-26 2012-04-26 Method for measuring optical fiber dispersion Pending CN102636337A (en)

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CN104849027A (en) * 2015-05-14 2015-08-19 河南师范大学 Laser-beat-frequency-based method for chromatic dispersion measurement
CN107271146A (en) * 2017-06-02 2017-10-20 广州广电计量检测股份有限公司 The calibrating installation and equipment of optical fibre dispersion tester
CN107449738A (en) * 2017-06-20 2017-12-08 江苏大学 A kind of dual-beam pump probe experimental system
CN108168848A (en) * 2018-02-13 2018-06-15 南光高科(厦门)激光科技有限公司 A kind of multimode fibre test device
CN109374134A (en) * 2018-10-30 2019-02-22 北京工业大学 Ultrafast time-resolved transient reflectance spectroscopy imaging system

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Publication number Priority date Publication date Assignee Title
CN104849027A (en) * 2015-05-14 2015-08-19 河南师范大学 Laser-beat-frequency-based method for chromatic dispersion measurement
CN104849027B (en) * 2015-05-14 2017-08-15 河南师范大学 A kind of method that dispersion is measured based on laser beat frequency
CN107271146A (en) * 2017-06-02 2017-10-20 广州广电计量检测股份有限公司 The calibrating installation and equipment of optical fibre dispersion tester
CN107449738A (en) * 2017-06-20 2017-12-08 江苏大学 A kind of dual-beam pump probe experimental system
CN108168848A (en) * 2018-02-13 2018-06-15 南光高科(厦门)激光科技有限公司 A kind of multimode fibre test device
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CN109374134A (en) * 2018-10-30 2019-02-22 北京工业大学 Ultrafast time-resolved transient reflectance spectroscopy imaging system

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Application publication date: 20120815