CN111486939A - Ultrasonic measuring device for realizing optical path and polarization state regulation and control based on SAGNAC principle - Google Patents

Ultrasonic measuring device for realizing optical path and polarization state regulation and control based on SAGNAC principle Download PDF

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CN111486939A
CN111486939A CN202010333895.6A CN202010333895A CN111486939A CN 111486939 A CN111486939 A CN 111486939A CN 202010333895 A CN202010333895 A CN 202010333895A CN 111486939 A CN111486939 A CN 111486939A
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polarization
optical path
light
coupler
polarization controller
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CN111486939B (en
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王自鑫
蔡志岗
赵伟鸿
王福娟
王嘉辉
李佼洋
黄柱源
张锡斌
李文哲
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Sun Yat Sen University
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H9/00Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means
    • G01H9/004Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means using fibre optic sensors
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01CMEASURING DISTANCES, LEVELS OR BEARINGS; SURVEYING; NAVIGATION; GYROSCOPIC INSTRUMENTS; PHOTOGRAMMETRY OR VIDEOGRAMMETRY
    • G01C19/00Gyroscopes; Turn-sensitive devices using vibrating masses; Turn-sensitive devices without moving masses; Measuring angular rate using gyroscopic effects
    • G01C19/58Turn-sensitive devices without moving masses
    • G01C19/64Gyrometers using the Sagnac effect, i.e. rotation-induced shifts between counter-rotating electromagnetic beams
    • G01C19/72Gyrometers using the Sagnac effect, i.e. rotation-induced shifts between counter-rotating electromagnetic beams with counter-rotating light beams in a passive ring, e.g. fibre laser gyrometers

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Abstract

The invention discloses an ultrasonic measuring device for realizing optical path and polarization state regulation and control based on an SAGNAC (SAGNAC) principle, which comprises a light source, a sample probe, a circulator, a first polarization controller, a second polarization controller, a third polarization controller, a fourth polarization controller, a fifth polarization controller, a first unpolarized 1 x 2 coupler, a second unpolarized 1 x 2 coupler, a photoelectric detection device, a wavelength selector and a light path selector, wherein the sample probe is connected with the light source; light from a light source firstly passes through a wavelength selector, a first polarization controller and a circulator and is divided into two paths with different lengths through a first non-polarization coupler, wherein one path is CW light along the clockwise direction, and the other path is CCW light along the counterclockwise direction; compared with the prior art, the method for realizing non-contact ultrasonic detection by utilizing the SAGNAC effect has the characteristics of simple structure, low cost, small volume, high sensitivity and wide application range.

Description

一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置An Ultrasonic Measurement Device Based on the Principle of SAGNAC for Optical Length and Polarization Control

技术领域technical field

本发明属于光纤陀螺技术领域,尤其涉及一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置。The invention belongs to the technical field of fiber optic gyroscopes, and in particular relates to an ultrasonic measuring device for realizing optical path and polarization state regulation and control based on the SAGNAC principle.

技术背景technical background

声波与物质相互作用时,声速及声波的能量会发生变化,通过对声速和声波衰减的测量,可以确定物质的一些基本物理参数。这就是超声检测技术,它是研究物质结构及其特性的基本方法之一,在许多领域已获得成功应用。传统的超声产生和接收方法是使用超声环能器,如压电换能器、CMUT换能器,这些方法都是接触式的测量方法。当前,传统的接触式换能器越来越多的被非接触的光学方法代替,包括了干涉法和光束偏转法等。由于光学技术的不断提高,这方面的研究也在飞速发展,并不断产生新的探测技术,包括光纤传感技术。光纤传感器是一种新兴的超声传感器件,因为具有体积小、重量轻、环境适应性强、可靠性强、检测信号传输容易、保密性好等许多优点而得到广泛应用。但是将光纤传感器用于超声检测,尤其是非接触式检测的研究还相对较少,尤其是国内研究很少。将光纤传感技术与非接触式超声检测技术相结合,在材料的超声检测、探伤应用方面将具有广阔的前景。When the sound wave interacts with the material, the sound speed and the energy of the sound wave will change. By measuring the sound speed and the attenuation of the sound wave, some basic physical parameters of the material can be determined. This is ultrasonic testing technology, which is one of the basic methods to study the structure and properties of matter, and has been successfully applied in many fields. The traditional method of ultrasonic generation and reception is to use ultrasonic circulators, such as piezoelectric transducers, CMUT transducers, and these methods are all contact measurement methods. Currently, traditional contact transducers are increasingly being replaced by non-contact optical methods, including interferometric methods and beam deflection methods. Due to the continuous improvement of optical technology, research in this area is also developing rapidly, and new detection technologies are continuously produced, including optical fiber sensing technology. Optical fiber sensor is a new type of ultrasonic sensor, which is widely used because of its small size, light weight, strong environmental adaptability, strong reliability, easy transmission of detection signals, and good confidentiality. However, there are relatively few studies on the use of optical fiber sensors for ultrasonic testing, especially non-contact testing, especially in domestic research. Combining optical fiber sensing technology with non-contact ultrasonic testing technology will have broad prospects in the application of ultrasonic testing and flaw detection of materials.

发明内容SUMMARY OF THE INVENTION

本发明的目的是提供一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置,其采用了SAGNAC干涉仪的基本原理,样品表面的振动会带来光程差的变化,利用CW光和CCW光先后到达样品表面的时间不同引起光程差变化形成的干涉信号进行样品表面超声波的检测。本发明的核心在于与波长选择技术和光路选择技术结合,通过选波长、选光纤长度的方式实现工作中心频率的切换。The purpose of the present invention is to provide an ultrasonic measuring device that realizes the regulation of optical path and polarization state based on the SAGNAC principle. The interference signal formed by the change of the optical path difference caused by the time when the CCW light reaches the surface of the sample successively is used to detect the ultrasonic wave on the surface of the sample. The core of the invention lies in combining with the wavelength selection technology and the optical path selection technology, and realizes the switching of the working center frequency by selecting the wavelength and the length of the optical fiber.

具体内容如下:The details are as follows:

一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置,其特征在于,包括光源,样品探头,环形器,第一偏振控制器、第二偏振控制器、第三偏振控制器、第四偏振控制器、第五偏振控制器、第一非偏振1*2耦合器,第二非偏振1*2耦合器,光电探测装置,波长选择器和光路选择器,所述波长选择器用于不同光源波长的选择;所述光路选择器用于不同光纤长度的选择;通过选波长、选光纤长度的方式实现工作中心频率的切换;An ultrasonic measurement device based on the SAGNAC principle to realize the regulation of optical path and polarization state, characterized in that it includes a light source, a sample probe, a circulator, a first polarization controller, a second polarization controller, a third polarization controller, a fourth polarization controller, and a fourth polarization controller. Polarization controller, fifth polarization controller, first unpolarized 1*2 coupler, second unpolarized 1*2 coupler, photodetection device, wavelength selector and optical path selector, the wavelength selector is used for different light sources The selection of wavelength; the optical path selector is used for the selection of different fiber lengths; the switching of the working center frequency is realized by selecting the wavelength and the length of the fiber;

所述光源、波长选择器、第一偏振控制器相连、环形器依次相连,所述环形器的其中一个输出端与第五偏振控制器、光电探测装置依次相连,另外一个输出端与第一非偏振1*2耦合器相连,所述第一非偏振1*2耦合器的其中一个输出端与第二偏振控制器、第二非偏振1*2耦合器依次相连,另外一个输出端与第三偏振控制器、光路选择器、第二非偏振1*2耦合器依次相连,所述第二非偏振1*2耦合器与第四偏振控制器、样品探头依次相连。The light source, the wavelength selector, the first polarization controller are connected, and the circulator is connected in sequence. One of the output ends of the circulator is connected to the fifth polarization controller and the photoelectric detection device in sequence, and the other output end is connected to the first non-polarization device. The polarized 1*2 coupler is connected, one of the output ends of the first unpolarized 1*2 coupler is connected to the second polarization controller and the second unpolarized 1*2 coupler in sequence, and the other output end is connected to the third The polarization controller, the optical path selector, and the second unpolarized 1*2 coupler are connected in sequence, and the second unpolarized 1*2 coupler is connected with the fourth polarization controller and the sample probe in sequence.

进一步的改进在于,所述光电探测装置包括偏振分束器和平衡探测器。A further improvement is that the photodetection device includes a polarization beam splitter and a balanced detector.

进一步的改进在于,所述CW光和CCW光经过所述第二非偏振1*2耦合器、第四偏振控制器和所述样品探头到达超声样品,反回光再次进入样品探头返回光纤光路。A further improvement is that the CW light and the CCW light pass through the second unpolarized 1*2 coupler, the fourth polarization controller and the sample probe to reach the ultrasonic sample, and the returned light enters the sample probe and returns to the optical fiber optical path again.

进一步的改进在于,所述CW光和CCW光的返回光再次经过所述第一非偏振1*2耦合器后进入所述环形器,实现入射光和返回光的隔离。A further improvement is that the return light of the CW light and the CCW light enters the circulator after passing through the first unpolarized 1*2 coupler again, so as to realize the isolation of the incident light and the return light.

进一步的改进在于,所述光源采用1310nm或者1550nm SLED宽谱光纤光源。A further improvement is that the light source is a 1310nm or 1550nm SLED broad-spectrum fiber light source.

进一步的改进在于,所述样品探头采用准直器加透镜的结构聚焦样品,实现携带样品表面超声信息的光信号返回光纤光路。A further improvement is that the sample probe adopts the structure of a collimator and a lens to focus the sample, so that the optical signal carrying the ultrasonic information on the surface of the sample is returned to the optical path of the optical fiber.

进一步的改进在于,所述偏振分束器采用的是三个带保偏接口的光纤。A further improvement is that the polarization beam splitter adopts three fibers with polarization maintaining interfaces.

进一步的改进在于,除所述偏振分束器以外其它所有的光纤和光纤器件都是采用非偏振式的。A further improvement is that all other optical fibers and optical fiber components except the polarization beam splitter are non-polarized.

本发明的有益效果为:本发明所采用的所有光纤器件除了偏振分束器以外全部采用非偏振式的,降低了成本;相比于传统的通过相位调制器进行pi/2相位偏置的方法,本发明的方案更加方便,且控制效果好;相比于传统的利用保偏光纤保持干涉光的正交或平行,本发明的方案采用调节五个偏振控制器中的任意两个就能实现同样的效果,且容易调节;相比于单端信号检测,本发明所述的用平衡探测器探测差分干涉信号的方法,具有更好的探测灵敏度。与波长选择技术和光路选择技术结合,通过选波长、选光纤长度的方式实现工作中心频率的切换,达到更好的灵敏度效果。The beneficial effects of the present invention are as follows: all the optical fiber devices used in the present invention are non-polarized except for the polarization beam splitter, which reduces the cost; , the solution of the present invention is more convenient and has good control effect; compared with the traditional use of polarization-maintaining fibers to keep the interference light orthogonal or parallel, the solution of the present invention can be realized by adjusting any two of the five polarization controllers. The same effect and easy adjustment; compared with single-ended signal detection, the method for detecting differential interference signals with a balanced detector according to the present invention has better detection sensitivity. Combined with wavelength selection technology and optical path selection technology, the switching of the working center frequency is realized by selecting the wavelength and the length of the optical fiber to achieve a better sensitivity effect.

附图说明Description of drawings

为了更清楚地说明本发明实施例或现有技术中的技术方案,下面将对实施例或现有技术描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他的附图。In order to explain the embodiments of the present invention or the technical solutions in the prior art more clearly, the following briefly introduces the accompanying drawings that need to be used in the description of the embodiments or the prior art. Obviously, the accompanying drawings in the following description are only These are some embodiments of the present invention. For those of ordinary skill in the art, other drawings can also be obtained according to these drawings without creative efforts.

图1为所述装置的整个光纤光路系统图;Fig. 1 is the whole optical fiber optical path system diagram of described device;

图2为所述装置的环路部分示意图;Fig. 2 is the schematic diagram of the loop part of the device;

图3为当CW光和CCW光的光程差在半个波长范围以内的分析图;Fig. 3 is the analysis diagram when the optical path difference of CW light and CCW light is within half wavelength range;

图4为干涉系统的频率选择效应分析图;Fig. 4 is the frequency selective effect analysis diagram of the interference system;

图5为干涉信号经过偏振分束器之后被分成两路的分析图;Fig. 5 is the analysis diagram that the interference signal is divided into two paths after passing through the polarization beam splitter;

图6为保偏光纤的应力主轴和PBS晶体的o光、e光所形成的xy坐标轴是重合的,旋转保偏光纤端口的慢轴夹角,使得快、慢轴和两个正交的偏振方向成45°或135°的夹角图;Figure 6 shows that the main axis of stress of the polarization-maintaining fiber and the xy-coordinate axes formed by the o-light and e-light of the PBS crystal are coincident. The angle of polarization direction is 45° or 135°;

具体实施方式Detailed ways

下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。The technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the accompanying drawings in the embodiments of the present invention. Obviously, the described embodiments are only a part of the embodiments of the present invention, but not all of the embodiments. Based on the embodiments of the present invention, all other embodiments obtained by those of ordinary skill in the art without creative efforts shall fall within the protection scope of the present invention.

一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置,其特征在于,包括光源,样品探头,环形器,第一偏振控制器、第二偏振控制器、第三偏振控制器、第四偏振控制器、第五偏振控制器、第一非偏振1*2耦合器,第二非偏振1*2耦合器,光电探测装置,波长选择器和光路选择器;所述波长选择器用于不同光源波长的选择;所述光路选择器用于不同光纤长度的选择;通过选波长、选光纤长度的方式实现工作中心频率的切换;An ultrasonic measurement device based on the SAGNAC principle to realize the regulation of optical path and polarization state, characterized in that it includes a light source, a sample probe, a circulator, a first polarization controller, a second polarization controller, a third polarization controller, a fourth polarization controller, and a fourth polarization controller. Polarization controller, fifth polarization controller, first unpolarized 1*2 coupler, second unpolarized 1*2 coupler, photodetection device, wavelength selector and optical path selector; the wavelength selector is used for different light sources The selection of wavelength; the optical path selector is used for the selection of different fiber lengths; the switching of the working center frequency is realized by selecting the wavelength and the length of the fiber;

所述光源、波长选择器、第一偏振控制器相连、环形器依次相连,所述环形器的其中一个输出端与第五偏振控制器、光电探测装置依次相连,另外一个输出端与第一非偏振1*2耦合器相连,所述第一非偏振1*2耦合器的其中一个输出端与第二偏振控制器、第二非偏振1*2耦合器依次相连,另外一个输出端与第三偏振控制器、光路选择器、第二非偏振1*2耦合器依次相连,所述第二非偏振1*2耦合器与第四偏振控制器、样品探头依次相连。The light source, the wavelength selector, the first polarization controller are connected, and the circulator is connected in sequence. One of the output ends of the circulator is connected to the fifth polarization controller and the photoelectric detection device in sequence, and the other output end is connected to the first non-polarization device. The polarized 1*2 coupler is connected, one of the output ends of the first unpolarized 1*2 coupler is connected to the second polarization controller and the second unpolarized 1*2 coupler in sequence, and the other output end is connected to the third The polarization controller, the optical path selector, and the second unpolarized 1*2 coupler are connected in sequence, and the second unpolarized 1*2 coupler is connected with the fourth polarization controller and the sample probe in sequence.

在本发明所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置中,所述光电探测装置包括平衡探测器和偏振分束器。In the ultrasonic measurement device based on the SAGNAC principle to realize the regulation of optical path and polarization state, the photoelectric detection device includes a balanced detector and a polarization beam splitter.

在本发明所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置中,所述CW光和CCW光经过所述第二非偏振1*2耦合器、第四偏振控制器和所述样品探头到达超声样品,反回光再次进入样品探头返回光纤光路。In the ultrasonic measuring device based on the SAGNAC principle to realize the regulation of optical path and polarization state, the CW light and the CCW light pass through the second unpolarized 1*2 coupler, the fourth polarization controller and the The sample probe reaches the ultrasonic sample, and the reflected light enters the sample probe and returns to the optical fiber optical path again.

在本发明所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置中,所述CW光和CCW光的返回光再次经过所述第一非偏振1*2耦合器后进入所述环形器,实现入射光和返回光的隔离。In the ultrasonic measuring device based on the SAGNAC principle to realize the regulation of optical path and polarization state, the return light of the CW light and the CCW light enters the first non-polarized 1*2 coupler again after passing through the first non-polarized 1*2 coupler. The circulator is used to realize the isolation of incident light and return light.

在本发明所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置中,所述光源采用1310nm或者1550nm SLED宽谱光纤光源。In the ultrasonic measuring device based on the SAGNAC principle to realize the regulation of optical path and polarization state, the light source is a 1310nm or 1550nm SLED broad-spectrum fiber light source.

在本发明所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置中,所述光电探测装置为一个光电探测器。In the ultrasonic measuring device based on the SAGNAC principle to realize the regulation of optical path and polarization state, the photoelectric detection device is a photoelectric detector.

在本发明所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置中,所述样品探头采用准直器加透镜的结构聚焦样品,实现携带样品表面超声信息的光信号返回光纤光路。In the ultrasonic measurement device based on the SAGNAC principle to realize the regulation of optical path and polarization state, the sample probe adopts the structure of a collimator and a lens to focus the sample, so that the optical signal carrying the ultrasonic information on the surface of the sample is returned to the optical fiber light path.

在本发明所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置中,所述偏振分束器采用的是三个带保偏接口的光纤。In the ultrasonic measurement device based on the SAGNAC principle to realize the regulation of optical path and polarization state, the polarization beam splitter adopts three optical fibers with polarization-maintaining interfaces.

在本发明所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置中,除所述偏振分束器以外其它所有的光纤和光纤器件都是采用非偏振式的。In the ultrasonic measuring device that realizes the regulation of optical path and polarization state based on the SAGNAC principle according to the present invention, all other optical fibers and optical fiber components except the polarization beam splitter are non-polarized.

如图1所示,系统的光源采用1310/1550nm SLED宽带低相干光源,以避免相干噪声的干扰。光源出来的光首先经过波长选择器、第一偏振控制器PC1,然后经过第一非偏振1*2耦合器BS1,设CW光先走的是图1中的上面一路,那么CW光会依次经过第二偏振控制器PC2,第二非偏振1*2耦合器BS2,第四偏振控制器PC4,样品探头,然后再返回第四偏振控制器PC4,第二非偏振1*2耦合器BS2,之后走下面一路,经过第一非偏振1*2耦合器BS1,光路选择器,第三偏振控制器PC2,然后进入环形器,CCW光也是类似的情况:先走下面的光路,返回的时候走上面的光路,如图2所示。As shown in Fig. 1, the light source of the system adopts 1310/1550nm SLED broadband low-coherence light source to avoid the interference of coherent noise. The light from the light source first passes through the wavelength selector, the first polarization controller PC1, and then the first non-polarized 1*2 coupler BS1. Assuming that the CW light first goes to the upper one in Figure 1, then the CW light will pass through in turn. Second polarization controller PC2, second unpolarized 1*2 coupler BS2, fourth polarization controller PC4, sample probe, then back to fourth polarization controller PC4, second unpolarized 1*2 coupler BS2, after that Go the following way, go through the first non-polarized 1*2 coupler BS1, the optical path selector, and the third polarization controller PC2, and then enter the circulator, the CCW light is also similar: first take the lower optical path, and go to the top when returning. light path, as shown in Figure 2.

由于CW光和CCW光走的大部分光路都是完全一样的,只有在经过偏振控制器的时候CW光和CCW光会由于双折射效应导致这两束光的偏振面改变不一样,而且附加的光程也不一样。利用光程改变和偏振改变的这种效应,找到需要的光程和偏振的组合,例如图1的光路中需要调节光程(相位)差为pi/2,偏振面正交。Since most of the optical paths of the CW light and the CCW light are exactly the same, only when the CW light and the CCW light pass through the polarization controller, the polarization planes of the two beams of light will change due to the birefringence effect, and the additional The light path is also different. Using the effect of optical path change and polarization change, find the required combination of optical path and polarization. For example, in the optical path in Figure 1, the optical path (phase) difference needs to be adjusted to pi/2, and the polarization planes are orthogonal.

其中一种具体的调节过程是:首先调节第二偏振控制器PC2,使得CW光和CCW光附加的光程差为pi/2,此时不仅光程差改变了,CW光和CCW光的偏振面也会相应地发生偏转,导致干涉效率降低。然后再次调节第一偏振控制器PC1使得CW光和CCW光的偏振方向正交,两路正交的光干涉效率几乎为0,但是经过偏振分束器PBS会由原来的不干涉变成干涉效率最大的两路差分干涉信号(如图6所示),再进入平衡探测器。One specific adjustment process is: firstly adjust the second polarization controller PC2, so that the additional optical path difference between the CW light and the CCW light is pi/2. At this time, not only the optical path difference changes, but also the polarization of the CW light and the CCW light. The surface will also be deflected accordingly, resulting in reduced interference efficiency. Then adjust the first polarization controller PC1 again so that the polarization directions of the CW light and the CCW light are orthogonal, and the interference efficiency of the two orthogonal lights is almost 0, but the polarization beam splitter PBS will change from the original non-interference to the interference efficiency The largest two-way differential interference signal (as shown in Figure 6) enters the balanced detector.

本发明的原理如下:其中,λ为波长,c为光的波速,

Figure BDA0002465918010000062
为相位差,ΔL为光纤的长短臂长度差,Δτ为长短臂的延时;The principle of the present invention is as follows: wherein, λ is the wavelength, c is the wave speed of light,
Figure BDA0002465918010000062
is the phase difference, ΔL is the length difference between the long and short arms of the fiber, and Δτ is the delay of the long and short arms;

考虑样品的振荡:

Figure BDA0002465918010000061
Consider the oscillation of the sample:
Figure BDA0002465918010000061

SAGNAC干涉仪长短臂的延时:

Figure BDA0002465918010000071
The delay of the long and short arms of the SAGNAC interferometer:
Figure BDA0002465918010000071

延时对应的光程差:The optical path difference corresponding to the delay:

Figure BDA0002465918010000072
Figure BDA0002465918010000072

最大灵敏度条件:Maximum Sensitivity Conditions:

一个合适的工作点,应该在系统零信号时,也就是样品无振动时具有最大的灵敏度。在样品无信号时,由于两路光光程差相同,

Figure BDA0002465918010000074
此时系统工作在干涉极大的位置,根据余弦函数的性质,该点的导数为0,也就是工作在最不灵敏的地方。为了提高静态工作点的灵敏度,在样品无信号发生的时候应该给予一个初始的相位差
Figure BDA0002465918010000075
A suitable operating point should have maximum sensitivity when the system has zero signal, that is, when the sample has no vibration. When the sample has no signal, since the optical path difference of the two paths is the same,
Figure BDA0002465918010000074
At this time, the system works at the position where the interference is extremely large. According to the properties of the cosine function, the derivative of this point is 0, that is, it works at the most insensitive place. In order to improve the sensitivity of the static working point, an initial phase difference should be given when no signal occurs in the sample
Figure BDA0002465918010000075

相位连续条件:如图3所示:Phase Continuity Condition: As shown in Figure 3:

若考虑非线性的情况,则只需要让ωAΔτ工作在半个波长以内的范围,从而避免相位折叠的现象。但是由于非线性会造成信号失真,因此需要对测量的信号经过一个逆运算才能复原出样品的振荡信号。If the nonlinear situation is considered, it is only necessary to make ω A Δτ work within the range of half wavelength, so as to avoid the phenomenon of phase folding. However, since nonlinearity will cause signal distortion, it is necessary to perform an inverse operation on the measured signal to recover the oscillation signal of the sample.

保证相位连续的条件是:

Figure BDA0002465918010000073
The conditions for ensuring phase continuity are:
Figure BDA0002465918010000073

SAGNAC干涉仪的频率选择效应:Frequency selection effect of SAGNAC interferometer:

从前面的推导可看出,SAGNAC干涉仪的本质是一个速度干涉仪,也就是对振荡求微分。微分器具有低通滤波的效应,但是实际上的SAGNAC干涉系统不是一个严格的微分器,由于系统的灵敏度有限,两束光到达样品表面的时间差不可能做的无限小。这种非理想的微分效应,导致SAGNAC干涉仪会出现一个频率选择效应,在某些频率最敏感,而在另一些频率最不敏感。如图4所描述的情况中,当Δτ=π/ωA时,干涉仪最敏感;当Δτ=2π/ωA时,干涉仪最不敏感。当第一束光(CCW光)在t1时刻到达,第二束光(CW光)经过Δτ=π/ωA后到达时,干涉信号也是个正弦信号,此时信号的强度最大;当第一束光(CCW)在t2时刻到达,第二束光(CW)在Δτ=2π/ωA后到达时,此时无信号,相当于ωA/2的信号被滤掉了。It can be seen from the previous derivation that the essence of the SAGNAC interferometer is a velocity interferometer, which is to differentiate the oscillation. The differentiator has the effect of low-pass filtering, but the actual SAGNAC interference system is not a strict differentiator. Due to the limited sensitivity of the system, the time difference between the two beams reaching the sample surface cannot be infinitely small. This non-ideal differential effect causes the SAGNAC interferometer to exhibit a frequency-selective effect, being most sensitive at some frequencies and least sensitive at others. In the situation described in Figure 4, when Δτ=π/ ωA , the interferometer is the most sensitive; when Δτ=2π/ ωA , the interferometer is the least sensitive. When the first beam of light (CCW light) arrives at time t1 and the second beam of light (CW light) arrives after Δτ=π/ω A , the interference signal is also a sinusoidal signal, and the signal intensity is the largest at this time; When the beam of light (CCW) arrives at time t2, and the second beam of light (CW) arrives after Δτ=2π/ω A , there is no signal at this time, and the signal equivalent to ω A /2 is filtered out.

可见,在该技术中不同光源波长的选择以及光纤长度的选择是至关重要的,因为它直接影响到测量的中心频率。为了解决这个问题,在此装置基础上与波长选择技术和光路选择技术结合,通过选波长、选光纤长度的方式实现工作中心频率的切换。It can be seen that the choice of wavelengths of different light sources and the choice of fiber length are crucial in this technique because it directly affects the center frequency of the measurement. In order to solve this problem, on the basis of this device, it is combined with wavelength selection technology and optical path selection technology, and the switching of the working center frequency is realized by selecting the wavelength and the length of the optical fiber.

需要说明的是,在本文中,诸如第一和第二等之类的关系术语仅仅用来将一个实体或者操作与另一个实体或操作区分开来,而不一定要求或者暗示这些实体或操作之间存在任何这种实际的关系或者顺序。而且,术语“包括”、“包含”或者其任何其他变体意在涵盖非排他性的包含,从而使得包括一系列要素的过程、方法、物品或者设备不仅包括那些要素,而且还包括没有明确列出的其他要素,或者是还包括为这种过程、方法、物品或者设备所固有的要素。在没有更多限制的情况下,由语句“包括一个……”限定的要素,并不排除在包括所述要素的过程、方法、物品或者设备中还存在另外的相同要素。It should be noted that, in this document, relational terms such as first and second are only used to distinguish one entity or operation from another entity or operation, and do not necessarily require or imply any relationship between these entities or operations. any such actual relationship or sequence exists. Moreover, the terms "comprising", "comprising" or any other variation thereof are intended to encompass a non-exclusive inclusion such that a process, method, article or device that includes a list of elements includes not only those elements, but also includes not explicitly listed or other elements inherent to such a process, method, article or apparatus. Without further limitation, an element qualified by the phrase "comprising a..." does not preclude the presence of additional identical elements in a process, method, article or apparatus that includes the element.

尽管已经示出和描述了本发明的实施例,对于本领域的普通技术人员而言,可以理解在不脱离本发明的原理和精神的情况下可以对这些实施例进行多种变化、修改、替换和变型,本发明的范围由所附权利要求及其等同物限定。Although embodiments of the present invention have been shown and described, it will be understood by those skilled in the art that various changes, modifications, and substitutions can be made in these embodiments without departing from the principle and spirit of the invention and modifications, the scope of the present invention is defined by the appended claims and their equivalents.

Claims (10)

1.一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置,其特征在于,包括光源,样品探头,环形器,第一偏振控制器、第二偏振控制器、第三偏振控制器、第四偏振控制器、第五偏振控制器、第一非偏振1*2耦合器,第二非偏振1*2耦合器,光电探测装置,波长选择器和光路选择器;所述波长选择器用于不同光源波长的选择;所述光路选择器用于不同光纤长度的选择;通过选波长、选光纤长度的方式实现工作中心频率的切换;1. an ultrasonic measuring device that realizes optical path and polarization state regulation and control based on SAGNAC principle, is characterized in that, comprises light source, sample probe, circulator, the first polarization controller, the second polarization controller, the third polarization controller, The fourth polarization controller, the fifth polarization controller, the first unpolarized 1*2 coupler, the second unpolarized 1*2 coupler, the photodetection device, the wavelength selector and the optical path selector; the wavelength selector is used for The selection of different light source wavelengths; the optical path selector is used for the selection of different optical fiber lengths; the switching of the working center frequency is realized by selecting the wavelength and the optical fiber length; 所述光源、波长选择器、第一偏振控制器、环形器依次相连,所述环形器的其中一个输出端与第五偏振控制器、光电探测装置依次相连,另外一个输出端与第一非偏振1*2耦合器相连,所述第一非偏振1*2耦合器的其中一个输出端与第二偏振控制器、第二非偏振1*2耦合器依次相连,另外一个输出端与第三偏振控制器、光路选择器、第二非偏振1*2耦合器依次相连,所述第二非偏振1*2耦合器与第四偏振控制器、样品探头依次相连。The light source, the wavelength selector, the first polarization controller, and the circulator are connected in sequence, and one output end of the circulator is connected to the fifth polarization controller and the photoelectric detection device in sequence, and the other output end is connected to the first non-polarization device. The 1*2 coupler is connected, one of the output ends of the first unpolarized 1*2 coupler is connected to the second polarization controller and the second unpolarized 1*2 coupler in sequence, and the other output end is connected to the third polarization The controller, the optical path selector, and the second unpolarized 1*2 coupler are connected in sequence, and the second unpolarized 1*2 coupler is connected with the fourth polarization controller and the sample probe in sequence. 2.根据权利要求1所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置,其特征在于,所述光源出来的光首先经过所述波长选择器,然后经过所述第一偏振控制器和所述环形器,然后经过所述第一非偏振1*2耦合器分成长度不同的两路,其中一路为沿顺时针方向的CW光,另外一路为沿逆时针方向的CCW光。2. a kind of ultrasonic measuring device that realizes optical path and polarization state regulation and control based on SAGNAC principle according to claim 1, is characterized in that, the light that described light source comes out first passes through described wavelength selector, and then passes through described first The polarization controller and the circulator are then divided into two paths with different lengths through the first unpolarized 1*2 coupler, one of which is the CW light in the clockwise direction, and the other one is the CCW light in the counterclockwise direction . 3.根据权利要求1所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置,其特征在于,所述光电探测装置包括偏振分束器和平衡探测器。3 . The ultrasonic measuring device for realizing optical path and polarization state regulation based on the SAGNAC principle according to claim 1 , wherein the photoelectric detection device comprises a polarization beam splitter and a balanced detector. 4 . 4.根据权利要求2所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置,其特征在于,所述CW光和CCW光经过所述第二非偏振1*2耦合器、第四偏振控制器和所述样品探头到达超声样品,反回光再次进入样品探头返回光纤光路。4. a kind of ultrasonic measuring device that realizes optical path and polarization state regulation and control based on SAGNAC principle according to claim 2, is characterized in that, described CW light and CCW light pass through described second non-polarization 1*2 coupler, The fourth polarization controller and the sample probe reach the ultrasonic sample, and the reflected light enters the sample probe and returns to the optical fiber optical path again. 5.根据权利要求4所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置,其特征在于所述CW光和CCW光的返回光再次经过所述第一非偏振1*2耦合器后进入所述环形器,实现入射光和返回光的隔离。5. a kind of ultrasonic measuring device that realizes optical path and polarization state regulation and control based on SAGNAC principle according to claim 4, it is characterized in that the return light of described CW light and CCW light passes through described first non-polarization 1*2 again After the coupler enters the circulator, the isolation of incident light and return light is realized. 6.根据权利要求1所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置,其特征在于,所述光源采用1310nm或者1550nm SLED宽谱光纤光源。6 . The ultrasonic measuring device for realizing optical path and polarization state regulation based on the SAGNAC principle according to claim 1 , wherein the light source adopts a 1310 nm or 1550 nm SLED broad-spectrum fiber light source. 7 . 7.根据权利要求1所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置,其特征在于,所述样品探头采用准直器加透镜的结构聚焦样品,实现携带样品表面超声信息的光信号返回光纤光路。7. a kind of ultrasonic measuring device that realizes optical path and polarization state regulation and control based on SAGNAC principle according to claim 1, is characterized in that, described sample probe adopts the structure of collimator and lens to focus sample, realizes carrying sample surface ultrasonic wave The optical signal of the information is returned to the optical fiber path. 8.根据权利要求3所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置,其特征在于,所述偏振分束器采用的是三个带保偏接口的光纤。8 . The ultrasonic measuring device for realizing optical path and polarization state regulation based on the SAGNAC principle according to claim 3 , wherein the polarization beam splitter adopts three optical fibers with polarization-maintaining interfaces. 9 . 9.根据权利要求3所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置,其特征在于除所述偏振分束器以外其它所有的光纤和光纤器件都是采用非偏振式的。9. a kind of ultrasonic measuring device that realizes optical path and polarization state regulation and control based on SAGNAC principle according to claim 3, it is characterized in that all other optical fibers and optical fiber devices except described polarization beam splitter adopt non-polarization type of. 10.根据权利要求1所述的一种基于SAGNAC原理实现光程和偏振态调控的超声测量装置,其特征在于五个偏振控制器中任意两个的组合可以实现初始光程差和偏振态的非独立调控。10. a kind of ultrasonic measuring device that realizes optical path and polarization state regulation and control based on SAGNAC principle according to claim 1, it is characterized in that the combination of any two in five polarization controllers can realize initial optical path difference and polarization state. non-independent regulation.
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