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CN110736721B - Glass plate refractive index uniformity detection device and detection method based on diffraction grating - Google Patents

Glass plate refractive index uniformity detection device and detection method based on diffraction grating Download PDF

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CN110736721B
CN110736721B CN201810797550.9A CN201810797550A CN110736721B CN 110736721 B CN110736721 B CN 110736721B CN 201810797550 A CN201810797550 A CN 201810797550A CN 110736721 B CN110736721 B CN 110736721B
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diffraction grating
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refractive index
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段存丽
惠倩楠
赵鹏程
刘王云
郭荣礼
刘丙才
张玉虹
胡小英
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Kepu Ningbo Technology Co ltd
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Xian Technological University
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Abstract

本发明涉及基于衍射光栅的玻璃平板折射率均匀性检测装置及检测方法,该装置包括波长可调光源,沿波长可调光源出射光线光轴方向依次设置扩束镜、针孔光阑、准直镜、可调狭缝和反射式平面衍射光栅,反射式平面衍射光栅6的工作面与所述出射光线光轴之间构成20—45°的入射夹角,在反射式平面衍射光栅的下方竖直依次设光学成像镜头和CCD图像采集系统,CCD图像采集系统连接计算机;在反射式平面衍射光栅和光学成像镜头之间设置待测件。本发明的光路系统实现了大厚度、折射率变化大的光学玻璃的空间折射率均匀性分布的非接触式测量。

Figure 201810797550

The invention relates to a diffraction grating-based glass plate refractive index uniformity detection device and a detection method. The device comprises a wavelength-tunable light source, and a beam expander, a pinhole diaphragm, a collimator, Mirror, adjustable slit and reflective plane diffraction grating, the working surface of reflective plane diffraction grating 6 forms an incident angle of 20-45° with the optical axis of the outgoing light, and is vertically positioned below the reflective plane diffraction grating. An optical imaging lens and a CCD image acquisition system are set up in sequence, and the CCD image acquisition system is connected to the computer; the object to be tested is set between the reflective plane diffraction grating and the optical imaging lens. The optical path system of the invention realizes the non-contact measurement of the uniform distribution of the spatial refractive index of the optical glass with large thickness and large refractive index change.

Figure 201810797550

Description

基于衍射光栅的玻璃平板折射率均匀性检测装置及检测方法Glass plate refractive index uniformity detection device and detection method based on diffraction grating

技术领域technical field

本发明属于光学检测领域,涉及光的衍射技术、光谱分析技术以及计算机图像和数据处理技术,尤其涉及基于衍射光栅的玻璃平板折射率均匀性检测装置及检测方法。The invention belongs to the field of optical detection, relates to light diffraction technology, spectral analysis technology and computer image and data processing technology, in particular to a diffraction grating-based glass plate refractive index uniformity detection device and detection method.

背景技术Background technique

光学玻璃是制作光学透镜、光学棱镜、光学反射镜、分光镜、光纤、激光器等光学器件的主要材料,光学玻璃折射率均匀性好坏直接影响着光学器件的性能。因而光学玻璃均匀性测量是光学领域的研究热点。Optical glass is the main material for making optical lenses, optical prisms, optical mirrors, beam splitters, optical fibers, lasers and other optical devices. The uniformity of the refractive index of optical glass directly affects the performance of optical devices. Therefore, optical glass uniformity measurement is a research hotspot in the field of optics.

光学玻璃的折射率检测方法传统的方法主要有:(1)插针法;(2)分光计。主要是测定入射角和折射角,再根据玻璃的折射定律得到玻璃砖折射率。这两种方法优点是直接测量,测量仪器简单,操作方便。缺点是接触式测量,对待测件有磨损,测量精度低,检测的是光学玻璃平均折射率。The traditional methods of detecting the refractive index of optical glass mainly include: (1) pin-pin method; (2) spectrometer. It is mainly to measure the angle of incidence and the angle of refraction, and then obtain the refractive index of the glass brick according to the law of refraction of the glass. The advantages of these two methods are direct measurement, simple measurement instrument and convenient operation. The disadvantage is that the contact measurement, the wear of the test piece, the measurement accuracy is low, and the average refractive index of the optical glass is detected.

非接触式测量的方法有:主要有干涉法测量。干涉法测量是利用迈克尔孙干涉仪测量光学玻璃上下两个表面反射形成的干涉条纹,对干涉条纹进行图像和数据处理,得到光学平板玻璃的空间折射率分布。该方法优点是非接触式测量、检测的是空间折射率分布,测量精度高。缺点是由于干涉条件的限制,测量范围小,一般适用于光学玻璃厚度小,折射率变化小的光学玻璃材料测量。The methods of non-contact measurement are: mainly interferometric measurement. Interferometric measurement is to use a Michelson interferometer to measure the interference fringes formed by the reflection of the upper and lower surfaces of the optical glass, and perform image and data processing on the interference fringes to obtain the spatial refractive index distribution of the optical flat glass. The advantage of this method is that the non-contact measurement, the detection is the spatial refractive index distribution, and the measurement accuracy is high. The disadvantage is that due to the limitation of interference conditions, the measurement range is small, and it is generally suitable for the measurement of optical glass materials with small thickness of optical glass and small refractive index change.

基于衍射光栅的光学检测方法主要有两种:(1)利用透射式衍射光栅;(2)利用反射式衍射光栅。这两种方法主要利用衍射光栅的分光性能进行液体平均折射率的测量,测量范围大,测量方法简单。缺点是测量是液体平均折射率,且测量精度低。There are two main optical detection methods based on diffraction gratings: (1) using a transmissive diffraction grating; (2) using a reflective diffraction grating. These two methods mainly use the spectroscopic properties of the diffraction grating to measure the average refractive index of the liquid, with a large measurement range and a simple measurement method. The disadvantage is that the measurement is the average refractive index of the liquid, and the measurement accuracy is low.

发明内容SUMMARY OF THE INVENTION

本申请提供一种基于衍射光栅的玻璃平板折射率均匀性检测装置及检测方法,解决现有技术中对大厚度、折射率变化大的光学玻璃的折射率检测精度不高的问题。The present application provides a diffraction grating-based glass plate refractive index uniformity detection device and detection method, which solve the problem of low refractive index detection accuracy for optical glass with large thickness and large refractive index change in the prior art.

为了达到上述目的,本发明的技术方案如下:In order to achieve the above object, technical scheme of the present invention is as follows:

基于衍射光栅的玻璃平板折射率均匀性检测装置,包括波长可调光源,沿波长可调光源出射光线光轴方向依次设置扩束镜、针孔光阑、准直镜、可调狭缝和反射式平面衍射光栅,反射式平面衍射光栅6的工作面与所述出射光线光轴之间构成20—45°的入射夹角,在所述反射式平面衍射光栅的下方竖直依次设光学成像镜头和CCD图像采集系统,所述CCD图像采集系统连接计算机;在所述反射式平面衍射光栅和光学成像镜头之间设置待测件。A glass plate refractive index uniformity detection device based on a diffraction grating includes a wavelength-tunable light source, and a beam expander, a pinhole aperture, a collimating mirror, an adjustable slit and a reflector are sequentially arranged along the optical axis direction of the emitted light from the wavelength-tunable light source. The reflective plane diffraction grating forms an incident angle of 20-45° between the working surface of the reflective plane diffraction grating 6 and the optical axis of the outgoing light, and an optical imaging lens is vertically and sequentially arranged below the reflective plane diffraction grating. and a CCD image acquisition system, the CCD image acquisition system is connected to a computer; a piece to be tested is arranged between the reflective plane diffraction grating and the optical imaging lens.

进一步的,所述准直镜的焦距等于准直镜到针孔光阑的距离。Further, the focal length of the collimating mirror is equal to the distance from the collimating mirror to the pinhole diaphragm.

进一步的,所述可调狭缝的狭缝宽度可调范围0-10mm。Further, the slit width of the adjustable slit can be adjusted in the range of 0-10 mm.

基于衍射光栅的玻璃平板折射率均匀性检测方法,包括以下步骤:The method for detecting the uniformity of refractive index of glass plate based on diffraction grating includes the following steps:

步骤1,调节扩束镜的位置,使可调波长光源出射的光束会聚到一点,在会聚点处加针孔光阑,滤除杂散光,使出射的光波为球面波;Step 1: Adjust the position of the beam expander to make the light beam emitted by the adjustable wavelength light source converge to a point, and add a pinhole diaphragm at the convergence point to filter out the stray light, so that the emitted light wave is a spherical wave;

步骤2,调节准直镜的位置,使入射的球面波通过后变为平面光波;Step 2: Adjust the position of the collimating mirror so that the incident spherical wave becomes a plane light wave after passing through;

步骤3,调节可调狭缝缝宽,使平面光波通过狭缝后出射合适线状平面光波;Step 3: Adjust the slit width of the adjustable slit so that the plane light wave passes through the slit and emits a suitable linear plane light wave;

步骤4,调节反射式平面衍射光栅,使合适线状平面光波斜入射,反射光波为衍射光波;Step 4, adjust the reflective plane diffraction grating so that the suitable linear plane light wave is obliquely incident, and the reflected light wave is the diffracted light wave;

步骤5,调节反射式平面衍射光栅,使其+1级衍射波通过光学成像镜头会聚,在光学成像镜头的像平面上得到衍射图样A,调节CCD图像采集系统接收衍射图样A;Step 5: Adjust the reflective plane diffraction grating to make the +1st order diffracted waves converge through the optical imaging lens, obtain the diffraction pattern A on the image plane of the optical imaging lens, and adjust the CCD image acquisition system to receive the diffraction pattern A;

步骤6,为了400nm-800nm波长的+1级衍射波均匀投射到CCD的接收面上,选定可调光源的中心波长600nm进行光束入射角的标定,调节光束入射角使600nm波长的衍射波垂直入射到CCD接收面上,作为CCD接收的中心坐标;Step 6: In order to evenly project the +1-order diffracted wave with the wavelength of 400nm-800nm onto the receiving surface of the CCD, select the center wavelength of the adjustable light source at 600nm to calibrate the beam incident angle, and adjust the beam incident angle to make the 600nm wavelength diffracted wave perpendicular. Incident to the CCD receiving surface, as the center coordinate of the CCD receiving;

步骤7,在反射式平面衍射光栅和光学成像镜头之间加入待测件,在光学成像镜头的像平面上得到经待测件折射的衍射光波B,调节CCD图像采集系统接收衍射图样B;Step 7, adding the DUT between the reflective plane diffraction grating and the optical imaging lens, obtaining the diffracted light wave B refracted by the DUT on the image plane of the optical imaging lens, and adjusting the CCD image acquisition system to receive the diffraction pattern B;

步骤8,计算机对比处理衍射图样B和衍射图样A,得到待测件的折射率空间分布信息。In step 8, the computer compares and processes the diffraction pattern B and the diffraction pattern A to obtain the spatial distribution information of the refractive index of the test piece.

本发明的有益效果:Beneficial effects of the present invention:

本发明的光路系统实现了大厚度、折射率变化大的光学玻璃的空间折射率均匀性分布的非接触式测量。其利用反射式衍射光栅超强的分光性能和计算机的数据处理技术相结合,不但可以进行光学玻璃的均值折射率测量,也可进行空间折射率均匀性测量,测量精度高,测量范围广,操作简单。The optical path system of the invention realizes the non-contact measurement of the uniform distribution of the spatial refractive index of the optical glass with large thickness and large refractive index change. It combines the superior spectral performance of the reflective diffraction grating with the data processing technology of the computer, which can not only measure the average refractive index of optical glass, but also measure the uniformity of the spatial refractive index, with high measurement accuracy, wide measurement range, and easy operation. Simple.

附图说明Description of drawings

图1是本发明装置的整体结构示意图;Fig. 1 is the overall structure schematic diagram of the device of the present invention;

图2是本发明衍射图样A的测量光路示意图;Fig. 2 is the measurement light path schematic diagram of diffraction pattern A of the present invention;

图3是本发明衍射图样B的测量光路示意图;Fig. 3 is the measurement light path schematic diagram of diffraction pattern B of the present invention;

图中,1-波长可调光源,2-扩束镜,3-针孔光阑,4-准直镜,5-可调狭缝,6-反射式平面衍射光栅,7-待测件,8-光学成像镜头,9-CCD图像采集系统,10-计算机,11-平面单色光波,12-法线,13-0级衍射光束,14-+1级衍射光束,15-600mm+1级衍射光束,16-+1级衍射角,17-标准玻璃平板,18-入射角,19-未加待测件的光线,20-加待测件的光线。In the figure, 1-wavelength tunable light source, 2-beam expander, 3-pinhole diaphragm, 4-collimating mirror, 5-adjustable slit, 6-reflection plane diffraction grating, 7-test piece, 8-optical imaging lens, 9-CCD image acquisition system, 10-computer, 11-plane monochromatic light wave, 12-normal, 13-0th order diffracted beam, 14-+1st order diffracted beam, 15-600mm+1st order Diffracted beam, 16-+1st order diffraction angle, 17-standard glass plate, 18-incidence angle, 19-light without DUT, 20-light with DUT.

具体实施方式Detailed ways

下面通过具体实施方式结合附图对本发明作进一步详细说明。其中不同实施方式中类似元件采用了相关联的类似的元件标号。在以下的实施方式中,很多细节描述是为了使得本申请能被更好的理解。然而,本领域技术人员可以毫不费力的认识到,其中部分特征在不同情况下是可以省略的,或者可以由其他元件、材料、方法所替代。在某些情况下,本申请相关的一些操作并没有在说明书中显示或者描述,这是为了避免本申请的核心部分被过多的描述所淹没,而对于本领域技术人员而言,详细描述这些相关操作并不是必要的,他们根据说明书中的描述以及本领域的一般技术知识即可完整了解相关操作。The present invention will be further described in detail below through specific embodiments in conjunction with the accompanying drawings. Wherein similar elements in different embodiments have used associated similar element numbers. In the following embodiments, many details are described so that the present application can be better understood. However, those skilled in the art will readily recognize that some of the features may be omitted under different circumstances, or may be replaced by other elements, materials, and methods. In some cases, some operations related to the present application are not shown or described in the specification, in order to avoid the core part of the present application being overwhelmed by excessive descriptions, and for those skilled in the art, these are described in detail. The relevant operations are not necessary, and they can fully understand the relevant operations according to the descriptions in the specification and general technical knowledge in the field.

参见图1,基于衍射光栅的玻璃平板折射率均匀性检测装置,包括波长可调光源1,沿波长可调光源1出射光线光轴方向依次设置扩束镜2、针孔光阑3、准直镜4、可调狭缝5和反射式平面衍射光栅6,反射式平面衍射光栅6的工作面与所述出射光线光轴之间构成20—45°的入射夹角,在所述反射式平面衍射光栅6的下方竖直依次设光学成像镜头8和CCD图像采集系统9,所述CCD图像采集系统9连接计算机10;在所述反射式平面衍射光栅6和光学成像镜头8之间设置待测件7。Referring to Fig. 1, a glass plate refractive index uniformity detection device based on a diffraction grating includes a wavelength-tunable light source 1, and a beam expander 2, a pinhole aperture 3, a collimator, and The mirror 4, the adjustable slit 5 and the reflective plane diffraction grating 6 form an incident angle of 20-45° between the working surface of the reflective plane diffraction grating 6 and the optical axis of the outgoing light. Below the diffraction grating 6, an optical imaging lens 8 and a CCD image acquisition system 9 are arranged vertically in sequence, and the CCD image acquisition system 9 is connected to the computer 10; item 7.

波长可调光源1为氙灯光源,所述氙灯光源的波长调节范围为400nm-800nm。The wavelength adjustable light source 1 is a xenon lamp light source, and the wavelength adjustment range of the xenon lamp light source is 400nm-800nm.

反射式平面衍射光栅6的线对数600/mm,口径50mm×50mm。The number of line pairs of the reflective plane diffraction grating 6 is 600/mm, and the aperture is 50 mm×50 mm.

针孔光阑3的口径为1.5mm。The diameter of the pinhole diaphragm 3 is 1.5 mm.

准直镜4的焦距等于准直镜4到针孔光阑3的距离。The focal length of the collimating mirror 4 is equal to the distance from the collimating mirror 4 to the pinhole aperture 3 .

可调狭缝5的狭缝宽度可调范围0-10mm,缝长为30mm。The adjustable slit width of the adjustable slit 5 is 0-10mm, and the slit length is 30mm.

光学成像镜头8的焦距为25mm,口径30mm,反射式平面衍射光栅6与光学成像镜头8的距离为100mm。The focal length of the optical imaging lens 8 is 25 mm, the diameter is 30 mm, and the distance between the reflective plane diffraction grating 6 and the optical imaging lens 8 is 100 mm.

基于衍射光栅的玻璃平板折射率均匀性检测方法,包括以下步骤:The method for detecting the uniformity of refractive index of glass plate based on diffraction grating includes the following steps:

步骤1,波长可调光源1选取氙灯光源(400nm—800nm),选取可调波长光源某一波长出射,出射光束进入扩束镜2,调节扩束镜2的沿光轴距离,使波长可调光源1出射的光束会聚到一点,在会聚点处加小孔光阑3(口径为1.5mm),滤除杂散光,使出射的光波为球面光波;Step 1, the wavelength adjustable light source 1 selects a xenon lamp light source (400nm-800nm), selects a certain wavelength of the adjustable wavelength light source to emit, and the emitted beam enters the beam expander 2, and adjusts the distance along the optical axis of the beam expander 2 to make the wavelength adjustable. The light beam emitted by the light source 1 converges to a point, and a small aperture diaphragm 3 (a diameter of 1.5mm) is added at the convergence point to filter out the stray light, so that the emitted light wave is a spherical light wave;

步骤2,准直镜4的焦距为f,调节准直镜4的沿光轴与小孔光阑3距离为f,使入射的球面波通过准直镜4后变为平面光波;Step 2, the focal length of the collimating mirror 4 is f, and the distance between the optical axis of the collimating mirror 4 and the aperture diaphragm 3 is adjusted to be f, so that the incident spherical wave passes through the collimating mirror 4 and becomes a plane light wave;

步骤3,可调狭缝5(可调范围0-10mm),调节可调狭缝5缝宽为1mm,缝长为30mm使平面光波通过狭缝后出射线平面光波;Step 3: Adjustable slit 5 (adjustable range 0-10mm), adjust the slit width of adjustable slit 5 to 1mm, and the slit length to 30mm, so that the plane light wave passes through the slit and then emits the ray plane light wave;

步骤4,反射式平面衍射光栅6,线对数600/mm,口径50mm×50mm,调节反射式平面衍射光栅6,使线平面光波斜入射,入射角为α(20°—45°),反射光波为+1级衍射光波;Step 4, reflective plane diffraction grating 6, line logarithm 600/mm, aperture 50mm×50mm, adjust reflective plane diffraction grating 6, make the line plane light wave obliquely incident, the incident angle is α (20°-45°), reflect The light wave is the +1st order diffracted light wave;

步骤5,调节反射式平面衍射光栅6的衍射光波+1级衍射波通过光学成像镜头8会聚,光学成像镜头8的焦距为25mm,口径30mm,反射式平面衍射光栅6与光学成像镜头8的距离为100mm,利用光电定焦处理系统对光学成像镜头8后的像面进行定焦,使在光学成像镜头8后的像面上得到清晰的衍射图样A,用CCD图像采集系统9接收衍射图样A;Step 5, adjust the diffracted light wave + first-order diffracted wave of the reflective plane diffraction grating 6 to converge through the optical imaging lens 8, the focal length of the optical imaging lens 8 is 25mm, the aperture is 30mm, and the distance between the reflective plane diffraction grating 6 and the optical imaging lens 8 It is 100mm, and the photoelectric fixed focus processing system is used to fix the focus of the image surface behind the optical imaging lens 8, so that a clear diffraction pattern A is obtained on the image surface behind the optical imaging lens 8, and the CCD image acquisition system 9 is used to receive the diffraction pattern A. ;

步骤6,选定光源波长600nm进行标定;如附图2所示,选定光源波长为600nm,按照步骤5的方法调节反射式平面衍射光栅6的+1级衍射波照射到CCD图像采集系统9接收衍射图样M;因为是平面单色光波11入射到反射式平面衍射光栅6上,定义反射式平面衍射光栅6的法线12,0级衍射光束13,+1级衍射光束14仍为线光束,则衍射图样M为一线状光斑,记录线状光斑的位置P1。加入一块厚度10mm、折射率为K9标准玻璃平板17,记录线状光斑的位置P2。利用的原理是当光束垂直界面入标准玻璃平板17时,折射角和入射角均为0度,因而不分开。调节平面光波斜入射到反射式平面衍射光栅6的入射角18,使记录线状光斑的位置P1和位置P2完全重合,此时可确定光束垂直入射到标准玻璃板界面的位置。可标定波长为600nm的单色平面光波,以入射角α入射到反射式平面衍射光栅6上,对应波长600mm的+1级衍射光束15与平面单色光波11垂直,在CCD图像采集系统9上所形成的线光斑作为测量时的x坐标,线光斑几何中心为坐标原点,与线光斑垂直方向为z坐标。Step 6, select the light source wavelength of 600nm for calibration; as shown in Figure 2, the selected light source wavelength is 600nm, according to the method of step 5, adjust the +1 order diffraction wave of the reflective plane diffraction grating 6 to irradiate the CCD image acquisition system 9 Receive the diffraction pattern M; because the plane monochromatic light wave 11 is incident on the reflective plane diffraction grating 6, the normal line 12 of the reflective plane diffraction grating 6 is defined, the 0th order diffracted beam 13, and the +1st order diffracted beam 14 are still line beams , the diffraction pattern M is a linear light spot, and the position P1 of the linear light spot is recorded. A standard glass plate 17 with a thickness of 10 mm and a refractive index of K9 is added, and the position P2 of the linear light spot is recorded. The principle used is that when the light beam enters the standard glass plate 17 at the vertical interface, the refraction angle and the incident angle are both 0 degrees, so there is no separation. Adjust the incident angle 18 of the plane light wave obliquely incident on the reflective plane diffraction grating 6 so that the position P1 and the position P2 of the recorded linear light spot are completely coincident. The monochromatic plane light wave with a calibrated wavelength of 600 nm is incident on the reflective plane diffraction grating 6 at the incident angle α, and the +1-order diffracted beam 15 corresponding to the wavelength of 600 mm is perpendicular to the plane monochromatic light wave 11, on the CCD image acquisition system 9 The formed line spot is used as the x coordinate during measurement, the geometric center of the line spot is the origin of the coordinate, and the vertical direction to the line spot is the z coordinate.

步骤7,加入待测件7在反射式平面衍射光栅6前(不接触),在光学成像镜头8的像平面上得到变化衍射光波,调节CCD图像采集系统9接收衍射图样B。Step 7: Add the object to be tested 7 in front of the reflective plane diffraction grating 6 (without contact), obtain the variable diffracted light wave on the image plane of the optical imaging lens 8, and adjust the CCD image acquisition system 9 to receive the diffraction pattern B.

测试原理:如附图3所示,对步骤6标定的光学系统,衍射光栅的线对数为600/mm,带入衍射光栅方程:Test principle: As shown in Figure 3, for the optical system calibrated in step 6, the line logarithm of the diffraction grating is 600/mm, and the diffraction grating equation is brought into:

d(sinα±sinθ)=mλd(sinα±sinθ)=mλ

其中:α为入射角,θ为衍射角,

Figure BDA0001734595110000055
为入射光波波长,m为衍射级次。Where: α is the incident angle, θ is the diffraction angle,
Figure BDA0001734595110000055
is the wavelength of the incident light wave, and m is the diffraction order.

选定衍射级次m为+1级,入射角为步骤6标定的入射角,当可调波长光源1波长从400nm-800nm可见光范围变化时,代入衍射光栅方程,可计算出+1级衍射角范围为14°—29°,发散角为15°,若选定衍射光栅6到光学镜头9的距离为100mm,光学镜头的焦距为25mm,一般口径为30mm(大于投射光斑尺寸)。根据几何光学知识,可计算像面的位置以及光学镜头放大倍率β。The selected diffraction order m is the +1 order, and the incident angle is the incident angle calibrated in step 6. When the wavelength of the tunable wavelength light source 1 changes from the visible light range of 400nm-800nm, the diffraction grating equation can be substituted to calculate the +1 order diffraction angle. The range is 14°-29°, and the divergence angle is 15°. If the distance from the diffraction grating 6 to the optical lens 9 is 100mm, the focal length of the optical lens is 25mm, and the general aperture is 30mm (larger than the projected spot size). According to the knowledge of geometric optics, the position of the image plane and the magnification β of the optical lens can be calculated.

如附图3所示,由折射定律公式:As shown in Figure 3, from the formula of the law of refraction:

n1sinθ1=n2sinθ2 n 1 sinθ 1 =n 2 sinθ 2

其中:n1为入射介质折射率,n2为折射介质折射率,θ1为入射角,θ2为折射角。Where: n 1 is the refractive index of the incident medium, n 2 is the refractive index of the refracting medium, θ 1 is the incident angle, and θ 2 is the refraction angle.

可知加入待测件7折射角小于未加待测件7的角,如附图3所示,未加待测件7的光线19,加待测件7的光线20,两光束有一定的分开距离d,距离d可通过CCD图像采集系统9采集计算出,若已知待测件7的厚度h,入射角θ1通过折射定律和光束的直线传播定律形成的几何关系,建立待测件折射率n和相关参数数学模型:It can be seen that the refraction angle of adding the DUT 7 is smaller than the angle without the DUT 7. As shown in Figure 3, the light 19 without the DUT 7 and the light 20 adding the DUT 7 are separated to a certain extent. The distance d, the distance d can be collected and calculated by the CCD image acquisition system 9. If the thickness h of the DUT 7 is known, the incident angle θ 1 is formed through the geometric relationship formed by the law of refraction and the law of linear propagation of the light beam to establish the refraction of the DUT. Mathematical model of rate n and related parameters:

Figure BDA0001734595110000051
Figure BDA0001734595110000051

其中:n为待测件7折射率,θ1为入射角,h为待测件的厚度,d为未加待测件的光线19与加待测件光线20分开的距离。Wherein: n is the refractive index of the DUT 7, θ 1 is the incident angle, h is the thickness of the DUT, and d is the distance between the light 19 without the DUT and the light 20 with the DUT.

待测件折射率变化量Δn和相关参数数学模型:Mathematical model of the refractive index change Δn of the test piece and related parameters:

Figure BDA0001734595110000052
Figure BDA0001734595110000052

其中:n为待测件折射率,θ1为入射角,h为待测件的厚度,Δd为未加待测件7光线19与加待测件7光线20分开的距离的变化量。Wherein: n is the refractive index of the DUT, θ1 is the incident angle, h is the thickness of the DUT, and Δd is the change in the distance between the light 19 without the DUT 7 and the light 20 with the DUT 7 added.

步骤8,若CCD前光学镜头的放大倍率为β,从CCD图像采集系统9采集到衍射图样B和衍射图样A中计算出未加待测件光线19与加待测件光线20分开的距离d’及距离的变化量Δd’,则实际参数:Step 8, if the magnification of the CCD front optical lens is β, calculate the distance d that separates the light 19 without the object to be tested and the light 20 with the object to be tested from the diffraction pattern B and the diffraction pattern A collected by the CCD image acquisition system 9. ' and the change in distance Δd', then the actual parameters:

Figure BDA0001734595110000056
Figure BDA0001734595110000056

根据步骤7建立的数学模型,测试出的参数d’和Δd’,计算出待测件的折射率的平均值n和变化量Δn。According to the mathematical model established in step 7, and the measured parameters d' and Δd', calculate the average value n and variation Δn of the refractive index of the DUT.

步骤9,调节波长可调光源1的波长,使其从400nm-800nm范围变化,以波长差值5nm为步长,扫描采集不加待测件7多副衍射图样A,加待测件7多副衍射图样B分别存储,利用建立的模型以及编写的软件进行处理,计算得到待测件的空间折射率分布信息。Step 9, adjust the wavelength of the wavelength-tunable light source 1 to change it from 400nm to 800nm, take the wavelength difference of 5nm as a step, scan and collect more than 7 pairs of diffraction patterns A without adding the DUT, and add more than 7 DUTs. The secondary diffraction patterns B are stored separately, processed by the established model and the written software, and the spatial refractive index distribution information of the DUT is obtained by calculation.

以上应用了具体个例对本发明进行阐述,只是用于帮助理解本发明,并不用以限制本发明。对于本发明所属技术领域的技术人员,依据本发明的思想,还可以做出若干简单推演、变形或替换。The above specific examples are used to illustrate the present invention, which are only used to help understand the present invention, and are not intended to limit the present invention. For those skilled in the art to which the present invention pertains, according to the idea of the present invention, several simple deductions, modifications or substitutions can also be made.

Claims (1)

1. The method for detecting the uniformity of the refractive index of the glass plate based on the diffraction grating is characterized by comprising the following steps of:
step 1, adjusting the position of a beam expander to converge light beams emitted by a light source with adjustable wavelength to one point, adding a pinhole diaphragm at the convergence point, filtering stray light and enabling the emitted light waves to be spherical waves;
step 2, adjusting the position of the collimating mirror to enable incident spherical waves to become planar light waves after passing through;
step 3, adjusting the width of the adjustable slit to enable the planar light waves to pass through the slit and then emit appropriate linear planar light waves;
step 4, adjusting the reflective plane diffraction grating to enable the appropriate linear plane light waves to be incident obliquely, wherein the reflected light waves are diffraction light waves;
step 5, adjusting the reflective plane diffraction grating to enable + 1-order diffraction waves to be converged through the optical imaging lens, obtaining a diffraction pattern A on an image plane of the optical imaging lens, and adjusting the CCD image acquisition system to receive the diffraction pattern A;
step 6, in order to uniformly project + 1-order diffraction waves with the wavelength of 400nm-800nm onto a receiving surface of the CCD, selecting the central wavelength of 600nm of an adjustable light source to calibrate a light beam incident angle, and adjusting the light beam incident angle to enable the diffraction waves with the wavelength of 600nm to vertically incident on the receiving surface of the CCD to serve as a central coordinate received by the CCD;
step 7, adding a to-be-detected piece between the reflective plane diffraction grating and the optical imaging lens, obtaining diffracted light waves B refracted by the to-be-detected piece on an image plane of the optical imaging lens, and adjusting the CCD image acquisition system to receive the diffraction pattern B;
step 8, comparing the diffraction pattern B with the diffraction pattern A by the computer to obtain the spatial distribution information of the refractive index of the to-be-detected piece;
the detection device adopted by the detection method comprises a wavelength-adjustable light source (1), wherein a beam expander (2), a pinhole diaphragm (3), a collimating lens (4), an adjustable slit (5) and a reflective planar diffraction grating (6) are sequentially arranged along the optical axis direction of emergent light of the wavelength-adjustable light source (1), an incident included angle of 20-45 degrees is formed between the working surface of the reflective planar diffraction grating (6) and the optical axis of the emergent light, an optical imaging lens (8) and a CCD image acquisition system (9) are vertically and sequentially arranged below the reflective planar diffraction grating (6), and the CCD image acquisition system (9) is connected with a computer (10); a to-be-detected piece (7) is arranged between the reflection type plane diffraction grating (6) and the optical imaging lens (8);
the focal length of the collimating mirror (4) is equal to the distance from the collimating mirror (4) to the pinhole diaphragm (3);
the adjustable range of the slit width of the adjustable slit (5) is 0-10 mm.
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