CN109187433A - Refractive index of transparent films with double-prisms measuring device and method based on space interference - Google Patents

Refractive index of transparent films with double-prisms measuring device and method based on space interference Download PDF

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CN109187433A
CN109187433A CN201810974484.8A CN201810974484A CN109187433A CN 109187433 A CN109187433 A CN 109187433A CN 201810974484 A CN201810974484 A CN 201810974484A CN 109187433 A CN109187433 A CN 109187433A
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interference
polarization
refractive index
interferometer
beam splitter
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张红霞
宋晓敏
李东阳
贾大功
刘铁根
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Tianjin University
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    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/41Refractivity; Phase-affecting properties, e.g. optical path length
    • G01N21/45Refractivity; Phase-affecting properties, e.g. optical path length using interferometric methods; using Schlieren methods

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Abstract

本发明公开了一种基于空间干涉的透明薄膜折射率测量装置及方法,搭建宽带光源(1)、起偏器(2)、保偏光纤(3)、平凸透镜(4)、作为迈克尔干涉仪的分束器(7)、光谱仪(11)以及控制与数据采集电路(12)的测量装置;利用作为迈克尔逊干涉仪移动臂进行扫描,实现对保偏光纤的空间分布寄生偏振耦合的测量,得到干涉耦合图像;步骤(3)、计算移动臂上反射镜的扫描移动距离Δs,计算出被测透明薄膜折射率nm。与现有技术相比,本发明可对等厚度的薄膜进行测量,精确度高;装置结构简单,测量方法操作简便。

The invention discloses a device and method for measuring the refractive index of a transparent thin film based on spatial interference. A broadband light source (1), a polarizer (2), a polarization-maintaining optical fiber (3), a plano-convex lens (4), and a Michael interferometer are constructed. The beam splitter (7), the spectrometer (11) and the measurement device of the control and data acquisition circuit (12) are used for scanning; the measurement of the spatially distributed parasitic polarization coupling of the polarization maintaining fiber is realized by using the moving arm as a Michelson interferometer, The interference coupling image is obtained; in step (3), the scanning moving distance Δs of the mirror on the moving arm is calculated, and the refractive index nm of the measured transparent film is calculated. Compared with the prior art, the present invention can measure films of equal thickness, with high precision; the device has a simple structure and the measurement method is easy to operate.

Description

Refractive index of transparent films with double-prisms measuring device and method based on space interference
Technical field
The present invention relates to optical device fields, more particularly to a kind of optical device materials refractive index measurement method.
Background technique
Refractive index is one of important parameter of optical material, is the important foundation for studying other optical properties of optical material; Directly affect the quality of optical system.Refractive index can reflect many information inside optical material, meanwhile, other some parameters (such as thermo-optical coeffecient, elasto-optical coefficient) is also closely related with refractive index.Therefore, measuring to the refractive index of certain material has Highly important meaning.
Patent CN106970045 proposes " a kind of transmission-type coating substances apparatus for measuring refractive index ", describes " coupling optical The light of module output is convergence or divergence form, has different incidence angles in the first prism measuring surface, different enters Firing angle causes the light energy of lens different, and the light greater than critical angle is totally reflected, and the light less than critical angle reflects, so that There is the transmitted light projected from the second prism the hot spot of terminator to calculate to be measured according to the corresponding relationship of itself and determinand The refractive index of object ".Patent CN106840002 proposes " a kind of contactless plate glass thickness and apparatus for measuring refractive index and side Method ", describe that " its measuring device includes source of parallel light, plate glass, the first line array CCD and the second line array CCD, source of parallel light The incident beam directive plate glass of injection, the propagation path of incident beam are equipped with slit, and the first line array CCD is set to incident light Beam is on the path of surface of plate glass back reflection light beam, and the second line array CCD is set on the extended line of incident beam, First Line Battle array CCD and the second line array CCD are connect with digital storage oscilloscope, are obtained source of parallel light by oscillograph collection voltages peak and are issued Incident light by plate glass once fold light, the reflected light of upper surface, following table surface launching light through upper surface reflect out It is emitted directly toward the abscissa positions of the light of the second line array CCD when penetrating light, taking plate glass away, calculates refraction by position coordinates Rate ".
Summary of the invention
The technical issues of based on the above-mentioned prior art, the transparent membrane refraction based on space interference that the invention proposes a kind of Rate measuring device and method, the moving distance of Michael's interferometer moving arm caused by being changed according to optical path difference, realize measured object The calculating of refractive index.
A kind of refractive index of transparent films with double-prisms measuring device based on space interference of the invention, including wideband light source 1, the polarizer 2, polarization maintaining optical fibre 3, plano-convex lens 4, the beam splitter 7 as Michael's interferometer, spectrometer 11, control and data acquisition circuit; Tested transparent membrane 6 is installed between beam splitter 7 and fixed reflecting mirror 5 as Michael's interferometer;Wherein: wideband light source The light of 1 outgoing becomes linearly polarized light after the polarizer 2, which is expanded after polarization maintaining optical fibre 3 by the first plano-convex lens 4 Beam collimation;Collimated light beam after expanding, which is inputted, is divided into two beams by beam splitter 7, is incident on respectively solid as Michelson's interferometer The fixed reflecting mirror 5 of fixed arm and the packaged type reflecting mirror 8 of scan arm control packaged type reflecting mirror 8 by stepper motor 9 Movement, the optical path difference in polarization maintaining optical fibre 3 between two orthogonal polarized light beams is compensated by optical path difference between interferometer two-arm;Through The interference light for crossing Michelson's interferometer is assembled by the second plano-convex lens 10, is obtained by spectrometer 11 and data acquisition circuit The polarization coupled figure of polarization maintaining optical fibre 3.
A kind of refractive index of transparent films with double-prisms measurement method based on space interference of the invention, method includes the following steps:
The light that wideband light source is emitted is become linearly polarized light by step 1 after the polarizer, which passes through polarization-maintaining light By 4 beam-expanding collimation of the first plano-convex lens after fibre;Collimated light beam after expanding, which is inputted, is divided into two beams by beam splitter, is incident on respectively As the fixed reflecting mirror of Michelson's interferometer fixed arm and the packaged type reflecting mirror of scan arm;By tested transparent membrane It is installed between beam splitter and fixed reflecting mirror as Michael's interferometer;
Step 2 is scanned using the packaged type reflecting mirror as Michelson's interferometer moving arm, is realized to mikey The measurement of the space distributed polarization coupling of your polarization maintaining optical fibre obtains interference coupling image.Tested transparent membrane is installed, is obtained again Interference coupling image.The abscissa of interference coupling image is number of scan points, and ordinate is interference strength;Extract the interference coupling of two width Interfere number of scan points corresponding to primary maximum envelope maximum position in image, by number of scan points difference Δ p, calculates interference main pole The mobile distance, delta s of big envelope, the i.e. mobile distance calculation formula of movable mirror are as follows:
Wherein, v is the mobile speed of packaged type reflecting mirror, and p is number of scan points system each second;
Step 3, the distance, delta s moved according to packaged type reflecting mirror, calculate tested refractive index of transparent films with double-prisms nm, formula It is as follows:
Wherein, hmFor the thickness for being tested transparent membrane.
Compared with prior art, the present invention is based on the refractive index of transparent films with double-prisms measuring device and method of space interference, as A kind of layer material refractive index measurement method based on polarization coupled, can the refractive index of transparent films with double-prisms to equal thickness accurately surveyed Amount, accuracy are high;Apparatus structure is simple, and measurement method is easy to operate.
Detailed description of the invention
Fig. 1 is the layer material refractometry system of the invention based on polarization coupled;
Fig. 2 is the polarization coupled interference pattern obtained before and after being inserted into measured object, the interference obtained before the insertion of (2a) measured object It couples the interference obtained after the insertion of image (2b) measured object and couples image;
Fig. 3 is the interference envelope diagram extracted, and (3a), (3b) are to extract the resulting image of envelope to (2a), (2b);
Appended drawing reference:
1, wideband light source, 2, the polarizer, 3, polarization maintaining optical fibre, the 4, first plano-convex lens, 5, fixed reflecting mirror, 6, tested saturating Bright film, 7, beam splitter, 8, packaged type reflecting mirror, 9, stepper motor, the 10, second plano-convex lens, 11, spectrometer.
Specific embodiment
Embodiments of the present invention are described in further detail below in conjunction with attached drawing.
It builds experimental provision as shown in Figure 1 and builds index path, by wideband light source 1, the polarizer 2, polarization maintaining optical fibre 3, first Plano-convex lens 4, the beam splitter 7 as Michael's interferometer, spectrometer 11 and control and data acquisition circuit, composition, wherein Tested transparent membrane 6 is installed between beam splitter 7 and fixed reflecting mirror 5 as Michael's interferometer;
The light that wideband light source 1 is emitted becomes linearly polarized light after the polarizer 2, and the linearly polarized light is after polarization maintaining optical fibre 3 4 beam-expanding collimation of plano-convex lens for being 15cm by focal length;Collimated light beam input beam splitter 7 after expanding is divided into two beams, respectively It is incident on the packaged type reflecting mirror 8 of the fixed reflecting mirror 5 and scan arm as Michelson's interferometer fixed arm, passes through step The movement that packaged type reflecting mirror 8 is controlled into motor 9 is compensated two in polarization maintaining optical fibre 3 by the optical path difference between interferometer two-arm Optical path difference between orthogonal polarized light beam;It is saturating by the second plano-convex that focal length is 15cm by the interference light of Michelson's interferometer Mirror 10 is assembled, and the polarization coupled figure of polarization maintaining optical fibre is obtained by spectrometer 11 and data acquisition circuit.Control and data acquisition electricity Road is mainly by data collecting card NI-USB6251, AC-DC12V Switching Power Supply, for believing to NI-USB6251 power supply and difference Number test macro.P0.0, P0.1, P0.2 mouth of data collecting card are controlled respectively at controllor for step-by-step motor power-on and power-off port, direction Port processed, step angle port switching are connected, and realize the control to stepping electrode movement speed, distance;Data collecting card NI- USB6251 data acquisition flow is by differential signal test macro, the voltage signal of photodetector output is quantified, Coding, obtained digital signal is saved in capture card memory on board.
Refractive index of transparent films with double-prisms test device based on space interference, the transparent membrane folding of the invention based on space interference Rate measurement method is penetrated, specifically includes the following steps:
Step 1 is scanned using the packaged type reflecting mirror 8 as Michelson's interferometer moving arm, is realized to advanced in years The measurement of the space distributed polarization coupling of Ke Er polarization maintaining optical fibre obtains interference coupling image.Tested transparent membrane is installed, is obtained again Interference coupling image is taken, the abscissa of interference coupling image is number of scan points, and ordinate is interference strength;Extract two width interference coupling It closes and interferes number of scan points corresponding to primary maximum envelope maximum position in image, by number of scan points difference Δ p, calculate interference master The mobile distance, delta s of very big envelope, the i.e. mobile distance of movable mirror, formula are as follows:
Wherein, v is the mobile speed of packaged type reflecting mirror, and p is number of scan points system each second;
When optical path difference caused by step 2, Δ s is equal to optical path difference caused by tested transparent membrane, i.e. 2 Δ s=2 (nm-1)hm Inverse goes out tested refractive index of transparent films with double-prisms nm, wherein hmFor the thickness for being tested transparent membrane.
Embodiment:
Tested film is polyvinyl alcohol film, with a thickness of 30 μm.Tested film is mounted on Michelson's interferometer point Between beam device and fixed reflecting mirror, the space beam splitting distributed polarization coupling of polarization maintaining optical fibre is measured, (2b) is obtained in Fig. 2 Shown in interference coupling image.The interference envelope that interference coupling is (2a) and (2b) of Fig. 2 is extracted by Hilbert transform algorithm, Acquired results are shown in (3a) and (3b) of Fig. 3.Corresponding number of scan points at interference primary maximum envelope maximum intensity is calculated, scanning is passed through It is 15.48 μm that points, which calculate the mobile distance of mobile mirror, and according to formula:
2 Δ s=2 (nm-1)hm
Obtain the refractive index 1.516 of transparent membrane.

Claims (2)

1.一种基于空间干涉的透明薄膜折射率测量装置,其特征在于,该装置包括宽带光源(1)、起偏器(2)、保偏光纤(3)、平凸透镜(4)、作为迈克尔干涉仪的分束器(7)、光谱仪(11)以及控制与数据采集电路(12);其中:宽带光源(1)出射的光经过起偏器(2)后变为线偏振光,该线偏振光经过保偏光纤(3)后被第一平凸透镜(4)扩束准直;经扩束后的准直光束输入被分束器(7)分成两束,分别入射到作为迈克尔逊干涉仪固定臂的固定式反射镜(5)和扫描臂的可移动式反射镜(8),通过步进电机(9)控制可移动式反射镜(8)的移动,通过干涉仪两臂之间的光程差补偿保偏光纤(3)中两正交偏振光束之间的光程差;经过迈克尔逊干涉仪的干涉光经过第二平凸透镜(10)会聚,经过光谱仪(11)和数据采集电路获取保偏光纤(3)的偏振耦合图。1. A transparent film refractive index measuring device based on spatial interference, characterized in that the device comprises a broadband light source (1), a polarizer (2), a polarization-maintaining fiber (3), a plano-convex lens (4), a A beam splitter (7), a spectrometer (11) and a control and data acquisition circuit (12) of the interferometer; wherein: the light emitted from the broadband light source (1) becomes linearly polarized light after passing through the polarizer (2), and the line The polarized light is beam expanded and collimated by the first plano-convex lens (4) after passing through the polarization maintaining fiber (3); the input collimated beam after beam expansion is divided into two beams by the beam splitter (7), which are incident respectively as Michelson interference beams. The fixed mirror (5) of the fixed arm of the instrument and the movable mirror (8) of the scanning arm are controlled by the stepping motor (9) to move the movable mirror (8), and pass between the two arms of the interferometer. The optical path difference compensates the optical path difference between the two orthogonally polarized light beams in the polarization maintaining fiber (3); the interference light passing through the Michelson interferometer is condensed through the second plano-convex lens (10), passed through the spectrometer (11) and the data acquisition The circuit acquires the polarization coupling diagram of the polarization maintaining fiber (3). 2.一种基于空间干涉的透明薄膜折射率测量方法,其特征在于,该方法包括以下步骤:2. a method for measuring the refractive index of a transparent thin film based on spatial interference, characterized in that the method comprises the following steps: 步骤(1)、将宽带光源出射的光经过起偏器后变为线偏振光,该线偏振光经过保偏光纤后被第一平凸透镜4扩束准直;经扩束后的准直光束输入被分束器分成两束,分别入射到作为迈克尔逊干涉仪固定臂的固定式反射镜和扫描臂的可移动式反射镜;将被测透明薄膜安装于作为迈克尔干涉仪的分束器和固定式反射镜之间;Step (1), the light emitted by the broadband light source is changed into linearly polarized light after passing through the polarizer, and the linearly polarized light is expanded and collimated by the first plano-convex lens 4 after passing through the polarization-maintaining fiber; the collimated beam after the expanded beam The input is split into two beams by the beam splitter, which are respectively incident on the fixed mirror as the fixed arm of the Michelson interferometer and the movable mirror as the scanning arm; the transparent film to be measured is mounted on the beam splitter and the beam splitter as the Michael interferometer. between fixed mirrors; 步骤(2)、利用迈克尔逊干涉仪移动臂的可移动式反射镜进行扫描,实现对保偏光纤的空间分布寄生偏振耦合的测量,获取干涉耦合图像;将被测透明薄膜安装于作为迈克尔干涉仪的分束器和固定式反射镜之间,再次获取干涉耦合图像。干涉耦合图像的横坐标为扫描点数,纵坐标为干涉强度;提取两幅干涉耦合图像中干涉主极大包络极大值位置所对应的扫描点数,通过扫描点数差Δp,计算干涉主极大包络移动的距离Δs,即可移动反射镜移动的距离计算公式如下:Step (2), use the movable mirror of the moving arm of the Michelson interferometer to scan, realize the measurement of the parasitic polarization coupling of the spatial distribution of the polarization maintaining fiber, and obtain the interference coupling image; The interferometric coupling image is obtained again between the beam splitter of the instrument and the fixed mirror. The abscissa of the interference coupling image is the number of scanning points, and the ordinate is the interference intensity; the number of scanning points corresponding to the position of the maximum value of the interference main maximum envelope in the two interference coupling images is extracted, and the difference Δp between the scanning points is used to calculate the interference main maximum value. The distance Δs that the envelope moves, the distance that the movable mirror moves, is calculated as follows: 其中,v为可移动式反射镜移动的速度,p为系统每秒钟扫描点数;Among them, v is the moving speed of the movable mirror, and p is the number of points scanned by the system per second; 步骤(3)、根据可移动式反射镜移动的距离Δs,计算被测透明薄膜折射率nm,公式如下:Step (3), according to the moving distance Δs of the movable mirror, calculate the refractive index n m of the transparent film to be measured, and the formula is as follows: 其中,hm为被测透明薄膜的厚度。Among them, h m is the thickness of the measured transparent film.
CN201810974484.8A 2018-08-24 2018-08-24 Refractive index of transparent films with double-prisms measuring device and method based on space interference Pending CN109187433A (en)

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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109916347A (en) * 2019-04-16 2019-06-21 合肥工业大学 A method for measuring the surface topography of silicon wafers based on near-infrared low coherence light
WO2023024467A1 (en) * 2021-08-26 2023-03-02 五邑大学 Crystal refractive index measurement method and apparatus, and storage medium

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20050254057A1 (en) * 2004-05-14 2005-11-17 Alphonse Gerard A Low coherence interferometry utilizing phase
CN103134776A (en) * 2011-11-30 2013-06-05 中国计量学院 Liquid refractive index absolute measurement sensor based on D-type polarization maintaining optical fibre
CN203720071U (en) * 2014-01-27 2014-07-16 中国科学院上海光学精密机械研究所 Polarization frequency domain optical coherence tomography system based on single detector

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20050254057A1 (en) * 2004-05-14 2005-11-17 Alphonse Gerard A Low coherence interferometry utilizing phase
CN103134776A (en) * 2011-11-30 2013-06-05 中国计量学院 Liquid refractive index absolute measurement sensor based on D-type polarization maintaining optical fibre
CN203720071U (en) * 2014-01-27 2014-07-16 中国科学院上海光学精密机械研究所 Polarization frequency domain optical coherence tomography system based on single detector

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
张红霞等: "白光扫描干涉仪用于保偏光纤偏振耦合检测", 《红外与激光工程》 *
杨修文等: "迈克尔逊干涉仪测量薄膜的折射率与厚度", 《郧阳师范高等专科学校学报》 *

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109916347A (en) * 2019-04-16 2019-06-21 合肥工业大学 A method for measuring the surface topography of silicon wafers based on near-infrared low coherence light
WO2023024467A1 (en) * 2021-08-26 2023-03-02 五邑大学 Crystal refractive index measurement method and apparatus, and storage medium

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