WO2020248451A1 - 检测bgo晶体的残余双折射的装置和方法 - Google Patents
检测bgo晶体的残余双折射的装置和方法 Download PDFInfo
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- WO2020248451A1 WO2020248451A1 PCT/CN2019/111279 CN2019111279W WO2020248451A1 WO 2020248451 A1 WO2020248451 A1 WO 2020248451A1 CN 2019111279 W CN2019111279 W CN 2019111279W WO 2020248451 A1 WO2020248451 A1 WO 2020248451A1
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- polarization state
- residual birefringence
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/21—Polarisation-affecting properties
- G01N21/23—Bi-refringence
Definitions
- the present application relates to the field of crystal optics, for example, to a device and method for detecting the residual birefringence of isotropic crystal Bismuth Germanium Oxide (BGO).
- BGO isotropic crystal Bismuth Germanium Oxide
- BGO is an important isotropic optical crystal. In theory, it has only one refractive index. However, due to thermal effects during crystal manufacturing and processing, and mechanical stress during optical cold processing, residual stresses will be generated, resulting in residual stress in the crystal. Birefringence ultimately makes BGO an anisotropic crystal.
- the residual birefringence is randomly generated during the thermal process and the cold working process, the residual birefringence is also uneven in size, which has many adverse effects on the use of BGO crystals. Especially when BGO is used as an electro-optic crystal, it is equivalent to a random initial voltage, which seriously affects the measurement accuracy. Therefore, it is a very important task to detect the residual birefringence of the BGO crystal to ensure the quality of the crystal.
- how to use a simple device to detect the residual birefringence of the BGO crystal there is no method and corresponding device for detecting the residual birefringence of the BGO crystal in the related art.
- This application provides a device and method for detecting the residual birefringence of the BGO crystal, which can directly calculate the residual small birefringence of the BGO crystal by detecting the polarization state of the output light.
- An embodiment provides a device for detecting the residual birefringence of a BGO crystal, which includes a light source, a polarizer, a quarter wave plate, an optical fine-tuning frame with functions of horizontal rotation and roll rotation, a polarization analyzer, and a computer,
- the polarizer is arranged at the output end of the light source, and the polarizer is arranged to convert the light generated by the light source into linearly polarized light and send it to the 1/4 wave plate to convert the light
- the linearly polarized light becomes circularly polarized light and then directly projected onto the polarization analyzer;
- the polarization analyzer is set to obtain the polarization state corresponding to the circularly polarized light and send the polarization state to the computer,
- the polarizer is also set to cause the circularly polarized light to pass through the BGO crystal to be tested placed on the optical fine-tuning frame and then project it onto the polarization analyzer, and to obtain the changed polarization by rotating the optical
- An embodiment provides a method for detecting the residual birefringence of a BGO crystal.
- the above-mentioned device can be used to detect the residual birefringence of a BGO crystal.
- the method includes:
- the circularly polarized light is injected into the polarization analyzer after passing through the BGO crystal to be tested;
- s 1out and s 3out are the two Stokes parameters of the polarization state recorded each time; k 0 is the wave number of light in vacuum; L is the length of the BGO crystal to be measured; ⁇ is the deviation from the initial angle Rotation angle; ⁇ e is the dielectric constant corresponding to residual birefringence, n e is the magnitude of residual birefringence; n o is the refractive index when there is no residual birefringence in the BGO crystal.
- FIG. 1 is a schematic structural diagram of a device for detecting the residual birefringence of a BGO crystal provided in the first embodiment
- FIG. 2 is a schematic structural diagram of a device for detecting the residual birefringence of a BGO crystal provided in the second embodiment
- Figure 3 is a schematic diagram of the change of the coordinate system when the incident angle of the BGO crystal is changed
- Figure 4(a) is the polarization state of the output light of the BGO crystal No. 1 measured in the first embodiment
- Figure 4(b) is the polarization state of the output light of the No. 2 BGO crystal measured in the first embodiment
- Figure 4(c) is the polarization state of the output light of the number three BGO crystal measured in the first embodiment
- Figure 4(d) is the polarization state of the output light of the No. 4 BGO crystal measured in the first embodiment
- Fig. 6 is a flowchart of a method for detecting residual birefringence of a BGO crystal provided by an embodiment.
- Patent CN201210088188 A polarization and birefringence measurement system (Institute of Optoelectronic Technology, Chinese Academy of Sciences). This patent uses a beam of light to illuminate, but the detection technology uses three wave plates and an image capture card to image the outgoing light on the capture card, and obtain polarization and birefringence information through image processing and analysis. The function of the image capture card is still to collect the light intensity distribution of the output light, which is more detailed than the aforementioned patent, and does not involve the measurement of the polarization state.
- Patent CN201210193165 has many similarities with this application. They are all single beam injection, and the injected polarization state is circularly polarized light. The difference between this application and the patent is: (1) The measurement principle is different. The patent rotates the crystal 45 degrees around the beam axis.
- Patent CN201310250980 is obviously different from this application.
- the patent uses a reflective detection structure, that is, the light source and the light detector are on the same side of the sample.
- the samples in many other patents are placed between the light source and the detector, and the transmitted light is detected; while this patent detects the reflected light and requires two sets of detection units.
- Patent CN201310019042 Stress and birefringence measuring instrument and measuring method based on orthogonally polarized solid-state laser (Tsinghua University).
- the sample to be tested is placed in the oscillation circuit (resonator) of the laser, and the birefringence of the sample is measured by measuring the beat frequency of the laser output light (light of two frequencies) caused by the birefringence.
- Patent CN201510549341.9 A device for measuring small linear birefringence in cascade of elasto-optical modulation and electro-optical modulation (North University of China).
- This patent has similarities with this application, and both use a beam of light to detect the transmitted light. But the difference is also very big: (1) The light injected into the sample in this patent is linearly polarized light and passes through the elasto-optical modulator (phase modulation); (2) In this patent, the receiving side first passes through an electro-optical modulator and then reaches Light detector; (3) The sample in the patent does not move.
- the injected light is circularly polarized light without phase modulation; during the measurement process, the sample is rotated at a small angle (changing the incident angle); the detection end does not require an electro-optic modulator and is directly measured by a polarization analyzer.
- This application provides a device for detecting the residual birefringence of a BGO crystal.
- the device includes a light source, a polarizer, a quarter wave plate, an optical fine-tuning frame (referred to as a fine-tuning frame) with the functions of horizontal rotation and roll rotation, and polarization analysis Instrument and computer.
- the present application also provides a method for detecting the residual birefringence of BGO crystals, which can calculate the residual birefringence of BGO crystals by using the above-mentioned device for detecting the residual birefringence of BGO crystals, wherein the method includes:
- s 1out and s 3out are the two Stokes parameters corresponding to the polarization state recorded each time (the Stokes parameters are defined as four according to the definition, of which only two are independent);
- k 0 is the light in vacuum
- the polarization analyzer is directly connected to the data acquisition card, the data acquisition card is directly connected to the computer, the data acquisition card collects real-time data, the computer calculates the residual birefringence in real time, and the entire data acquisition and calculation process is automatically completed; 1
- the fine-tuning frame in this embodiment can be a motorized precision fine-tuning frame.
- the polarization analyzer is directly connected to the data acquisition card, and the data acquisition card is directly connected to the computer.
- the data acquisition card collects real-time data, and the computer calculates the residual birefringence in real time. ;
- the computer controls the electric fine-tuning frame in real time through the feedback system to realize self-calibration and automatic measurement, and improve the measurement accuracy.
- the device for detecting the residual birefringence of the BGO crystal includes a light source 1, a polarizer 2, a quarter-wave plate 3, a precision fine-tuning frame 4, a BGO crystal to be tested 5, and a polarization analyzer 6 and computer 7.
- the wave vector of the crystal light direction is In order to facilitate the analysis, we will create a wave vector As the coordinate system of the new z-axis (optical axis), it is necessary to perform coordinate transformation on the dielectric tensor ⁇ r of the BGO crystal with residual birefringence. Then find the birefringence vector.
- the residual birefringence vector is:
- Equation (16) shows that the direction of the residual birefringence vector is the s 2 direction, and the magnitude of the residual birefringence vector is not only related to the residual ⁇ e of the crystal, but also related to the direction of light passing through the crystal.
- the basic idea of residual birefringence measurement is to make the BGO crystal rotate a small angle around the (0,0,1) direction while observing the changes in the polarization state of the output light, and finally calculate the residual birefringence of the BGO crystal according to equation (16) the size of.
- the experimental system is shown in Figure 1.
- four BGO crystals 5 of the same batch were tested.
- the four crystals are number 1, number 2, number 3 and number 4, so that the incident angle varies from 0 to 2.5° ,
- Four BGO crystals 5 sequentially obtain the output light polarization state changes as shown in Fig. 4(a), Fig. 4(b), Fig. 4(c) and Fig. 4(d).
- the device for detecting the residual birefringence of the BGO crystal includes a light source 1, a polarizer 2, a quarter-wave plate 3, an electric precision fine-tuning frame 4, a BGO crystal to be tested 5, and a polarization
- the light source 1, the polarizer 2 and the quarter-wave plate 3 form a circularly polarized light generator.
- This circularly polarized light enters the BGO crystal 5 to be tested, and the BGO crystal is placed in a rotating precision fine-tuning frame 4 rotates together with the precision fine-tuning frame 4, the BGO output light is received by the polarization analyzer 6 and the polarization state of the BGO light is output from the polarization analyzer 6, and then the measured data is directly sent to the computer 7 through the data acquisition card, After computer data processing, the result is fed back to the drive circuit of the precision fine-tuning frame 4, and the precision-fine-tuning frame 4 is further rotated until the measurement requirement is reached.
- This fully automated feedback system will further improve measurement accuracy and save time.
- This application can directly calculate the residual tiny birefringence of the BGO crystal by detecting the polarization state of the output light. Because the residual birefringence is very small, it is impossible to measure this small birefringence by using the principle that one beam of input light is divided into two birefringent lights. This application can not only measure the residual birefringence of BGO crystals, but also the residual birefringence in other isotropic media. At the same time, the device for detecting birefringence provided by this application is compared with other devices for detecting birefringence in the related art. The structure is simpler and the cost is lower.
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Abstract
Description
Claims (5)
- 一种检测BGO晶体的残余双折射的装置,包括:光源、起偏器、1/4波片、具有水平旋转和侧滚旋转功能的光学微调架、偏振分析仪和计算机;其中:所述起偏器设于所述光源的输出端,且所述起偏器设置为将所述光源产生的光转换为线偏振光并送入所述1/4波片,以将所述线偏振光变为圆偏振光后直接投射到所述偏振分析仪上;所述偏振分析仪设置为得到与所述圆偏振光对应的偏振态并将所述偏振态送入所述计算机,所述起偏器还设置为使所述圆偏振光经过置于所述光学微调架上的待测BGO晶体后再投射到所述偏振分析仪上,通过旋转所述光学微调架得到变化的偏振态轨迹后将所述偏振态轨迹送入所述计算机;所述计算机设置为根据接收的所述偏振态计算出所述待测BGO晶体的残余双折射。
- 根据权利要求1所述的检测BGO晶体的残余双折射的装置,其中,所述光学微调架包括电动的精密微调架和所述精密微调架的驱动电路,所述计算机通过所述驱动电路调节所述精密微调架的旋转角度。
- 一种检测BGO晶体的残余双折射的方法,采用权利要求1-2任一项所述的检测BGO晶体的残余双折射的装置,所述方法包括:获取起偏器和1/4波片产生的圆偏振光;将所述圆偏振光直接注入偏振分析仪;得到偏振态;将待测BGO晶体置于光学微调架上;所述圆偏振光经所述待测BGO晶体后注入所述偏振分析仪;得到与所述待测BGO晶体对应的偏振态;调节所述光学微调架,使与所述待测BGO晶体对应的偏振态与所述将所述圆偏振光直接注入所述偏振分析仪后得到的偏振态一致;调节所述光学微调架,使所述光学微调架水平旋转和侧滚旋转;得到所述光学微调架的旋转角度、与所述旋转角度对应的偏振态及所述偏振态随着所述旋转角度变化的轨迹;及将所述轨迹数据送入计算机,并根据公式计算残余双折射;其中,所述公式为:
- 根据权利要求3所述的检测BGO晶体的残余双折射的方法,其中,k 0采用k 0=2π/λ计算,其中λ为光在真空中的波长。
- 根据权利要求3所述的检测BGO晶体的残余双折射的方法,其中,Δ=Δ 0+θ,Δ为所述光学微调架每次旋转后的偏离角度,Δ 0为初始对准时所述光学微调架存在的起始角度,θ为所述光学微调架偏离所述起始角的角度;所述将所述轨迹数据送入计算机,并根据公式计算残余双折射包括:找到s 1out=0的特征点;根据θ及Δ 0+θ=0,找到起始角Δ 0;及根据所述公式及Δ 0+θ=0求出残余双折射n e。
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