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CN2397505Y - Optical fiber confocal scanning microscope - Google Patents

Optical fiber confocal scanning microscope Download PDF

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CN2397505Y
CN2397505Y CN 99240337 CN99240337U CN2397505Y CN 2397505 Y CN2397505 Y CN 2397505Y CN 99240337 CN99240337 CN 99240337 CN 99240337 U CN99240337 U CN 99240337U CN 2397505 Y CN2397505 Y CN 2397505Y
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fiber
optical fiber
microscope
sampling
detector
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王桂英
杨莉松
徐至展
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Shanghai Institute of Optics and Fine Mechanics of CAS
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Abstract

一种光纤共焦扫描显微镜,包括照明光束输入部分A,光纤扫描部分B,与光纤扫描部分B交错置放的测量定位部分C,探测采样部分D和控制数据采集处理部分E。其中A、B、D和E构成光纤共焦扫描显微镜,而A、B和C构成准共焦小视场显微镜。也说是说,本实用新型的一台显微镜具有两种显微镜的功能,既有显微扫描层析成像的功能,又有一次成像的功能,即是对测定目标进行自定位的功能。适用于纳米深度,亚微米宽度的三维结构检测。

Figure 99240337

A fiber confocal scanning microscope comprises an illumination beam input part A, a fiber scanning part B, a measurement positioning part C interlaced with the fiber scanning part B, a detection sampling part D and a control data acquisition processing part E. A, B, D and E constitute a fiber confocal scanning microscope, while A, B and C constitute a quasi-confocal small field microscope. In other words, a microscope of the utility model has the functions of two microscopes, namely, the function of microscopic scanning tomography and the function of primary imaging, that is, the function of self-positioning the measurement target. It is suitable for three-dimensional structure detection with nanometer depth and submicron width.

Figure 99240337

Description

光纤共焦扫描显微镜Fiber Confocal Scanning Microscope

本实用新型是一种光纤共焦扫描显微镜,适用于纳米深度,亚微米宽度的三维结构检测。The utility model is an optical fiber confocal scanning microscope, which is suitable for three-dimensional structure detection with nanometer depth and submicron width.

已有技术:Existing technology:

在90年代出现了利用单模光纤代替针孔的技术,从此利用光纤器件的共焦扫描显微技术发展很快,原因有二。其一把激光直接输入至光纤中可以避免激光制冷系统产生的振动;其二是为了简化结构,使扫描共焦系统更紧凑。但在性能上并没有大的改进。在1996年本实用新型专利申请人也提供了一种由单模光纤耦合器为基础元件的光纤共焦扫描显微镜(参见发表在《中国激光》杂志英文版上:Fiber Optical Confocal Scanning Microscope Using Single mode Fiber Coupler,Chinese Journal of Laser,1996,B5(1):81)。该仪器无论在结构上还是在性能上都很有代表性。In the 1990s, the technology of using single-mode fiber instead of pinhole appeared. Since then, confocal scanning microscopy technology using fiber optic devices has developed rapidly. There are two reasons. One is to directly input the laser into the optical fiber to avoid the vibration generated by the laser cooling system; the other is to simplify the structure and make the scanning confocal system more compact. But there is no big improvement in performance. In 1996, the utility model patent applicant also provided a fiber optic confocal scanning microscope based on a single-mode fiber coupler (see the English version published in "China Laser" magazine: Fiber Optical Confocal Scanning Microscope Using Single mode Fiber Coupler, Chinese Journal of Laser, 1996, B5(1): 81). The instrument is very representative both in structure and performance.

上述已有技术中的光纤共焦扫描显微镜存在下述问题(1)检测目标定位问题。由于光纤扫描显微镜是点成像的,经过扫描采样,由计算机拓扑成像。这种结构自身无法对大范围内的小目标定位。解决该问题的方案,一般是借助于普通光学显微镜完成定位。这样就需要利用光纤器件加普通光学显微镜组合起来实现定位观测。因此它并没有脱离普通显微镜的模式,仪器体积庞大,且分辨率不能进一步提高。在这种仪器中无非利用光纤代替原有小孔,从整体结构上没有更多新意。(2)在探测端,利用光纤作为滤波小孔,直接把光纤耦合器射出的光束输入探测器,其灰度细度的探测分辨率受探测器的分辨率制约。(3)在数据采集上,直接利用三维扫描采样,进行三维图像拓扑,采样所用时间长,带来的误差大。其空间分辨率受采样步长的限制。The fiber optic confocal scanning microscope in the prior art has the following problems: (1) The detection target positioning problem. Since the fiber scanning microscope is point-imaging, it is scanned and sampled and topographically imaged by a computer. This structure itself cannot locate small targets in a wide range. The solution to this problem is generally to complete the positioning by means of an ordinary optical microscope. This requires the combination of optical fiber devices and ordinary optical microscopes to achieve positioning observation. So it is not out of the ordinary microscope mode, the instrument is bulky, and the resolution cannot be further improved. In this instrument, it is nothing more than using optical fiber to replace the original small hole, and there is no more novelty in the overall structure. (2) At the detection end, the optical fiber is used as a filter hole, and the light beam emitted by the fiber coupler is directly input into the detector, and the detection resolution of the gray fineness is restricted by the resolution of the detector. (3) In terms of data acquisition, directly use 3D scanning sampling to perform 3D image topology, which takes a long time for sampling and brings large errors. Its spatial resolution is limited by the sampling step size.

本实用新型的目的是:The purpose of this utility model is:

第一、保持光纤器件轻巧和稳定之特点,既解决上述已有技术中点扫描显微镜的自身检测范围定位问题,而又不失原来仪器紧凑、轻巧和稳定的优点,达到多功能的实用目的。First, keep the characteristics of lightness and stability of optical fiber devices, which not only solves the problem of positioning the detection range of the point scanning microscope in the prior art, but also maintains the advantages of compactness, lightness and stability of the original instrument, and achieves the practical purpose of multi-function.

第二、进一步提高光纤共焦扫描显微镜的分辨率,尤其是纵向分辨率,使该类仪器能达到纳米分辨率,实现真正的超分辨。能够在分子生物学、光存储器件,以及超大规模集成电路检测中得到广泛的使用。Second, further improve the resolution of the fiber confocal scanning microscope, especially the longitudinal resolution, so that this type of instrument can reach nanometer resolution and realize real super-resolution. It can be widely used in molecular biology, optical storage devices, and VLSI detection.

本实用新型的显微镜,其光路如图1所示。它包括照明光束输入部分A,光纤扫描部分B,测量定位部分C,探测采样部分D以及控制数据采集处理部分E。其中照明光束输入部分A包括沿着作为光源的激光器1出射光束前进的方向上,依次置有耦合物镜2,光纤耦合器4,光纤耦合器4的第一输出端O1上有盛放折射率匹配液的容器3。光纤扫描部分B包括沿光纤耦合器4第二输出端O2输出光束前进方向上,依次置有光束准直镜5,采样物镜6和置于采样物镜6的焦面f上的被测样品7;与光纤扫描部分B交错置放的有测量定位部分C。测量定位部分C包括沿着置于样品调节架17上,在采样物镜6的离焦面P上的被测样品7反射回来的光束前进方向上依次有采样物镜6,分光板9,在分光板9反射光束的前进方向上,依次有放大目镜10和观察屏11;探测采样部分D包括沿着光纤耦合器4第三输出端O3出射光束的前进方向上,依次置有放大目镜16和带探测器电源14的探测器15;控制数据采集处理部分E包括置放被测样品7的带压电陶瓷驱动器(PZT)8的由压电陶瓷构成的样品调节架17,压电陶瓷驱动器8通过带平衡器的电源13与计算机12相联。计算机12同时还与探测采样部分D中的探测器15相联。Microscope of the present utility model, its light path as shown in Figure 1. It includes an illumination beam input part A, an optical fiber scanning part B, a measurement positioning part C, a detection sampling part D and a control data acquisition and processing part E. Wherein the illuminating beam input part A includes along the direction along which the light beam emitted by the laser 1 as the light source advances, a coupling objective lens 2 and a fiber coupler 4 are placed in sequence, and the first output end O1 of the fiber coupler 4 has a refractive index Matching liquid container3. The optical fiber scanning part B includes a beam collimating mirror 5, a sampling objective lens 6 and a measured sample 7 placed on the focal plane f of the sampling objective lens 6 along the advancing direction of the output beam at the second output port O2 of the fiber coupler 4 ; There is a measurement positioning part C interlaced with the fiber scanning part B. The measurement positioning part C includes a sample objective lens 6, a beam splitter 9, and a beam splitter on the direction of the light beam reflected back from the sample 7 on the out-of-focus plane P of the sample objective lens 6 along the sample adjustment frame 17. 9 In the forward direction of the reflected light beam, there are magnifying eyepiece 10 and observation screen 11 in turn; the detection sampling part D includes along the third output port O of the fiber coupler 4. On the forward direction of the outgoing light beam, there are in turn a magnifying eyepiece 16 and a belt The detector 15 of the detector power supply 14; the control data acquisition processing part E includes a sample adjustment rack 17 made of piezoelectric ceramics with a piezoelectric ceramic driver (PZT) 8 for placing the measured sample 7, and the piezoelectric ceramic driver 8 passes through the The power supply 13 with the balancer is connected with the computer 12 . The computer 12 is also connected to the detector 15 in the detection sampling section D at the same time.

本实用新型如上述结构的显微镜具有两种显微镜的功能,其一是显微扫描层析成像功能;其二是一次成像功能。光路如图1所示。A部分是照明光束输入部分。由作为光源的激光器1出射的光束依次输入至耦合物镜2和光纤耦合器4的输入端i,进入到光纤耦合器4中。返回的探测光以及杂散光由光纤耦合器4的其中第一输出端O1射出,射至放有折射率匹配液的容器3中。B部分是光纤扫描部分。由光纤耦合器4第二输出端O2输出光束进入光束准直镜5,再由采样物镜6把光纤出射光斑进一步聚焦为小光斑投射在焦面f上的被测样品7上,进行对被测样品7结构的探测。D部分为探测采样部分。其中14为探测器的电源,由光纤耦合器4的第三输出端O3输出的探测光首先经过放大目镜16放大再输入至探测器15的接收面上,探测器15会把光信息转化为电信息,输入至E部分的计算机12。E部分是控制数据采集处理部分。该被测样品7由可精密扫描的压电陶瓷驱动器(PZT)8带动样品调节架17来支撑,由计算机12控制扫描步长,计算机12同时还控制着D部分的采样,并进行数据处理。计算机12控制着带平衡器的PZT电源13。C部分为测量定位部分。当进行定位操作时,离焦面P的光束从被测样品7反射回来,经过采样物镜6和分光板9进入放大目镜10,成像在观察屏11上。C部分包括B部分的采样物镜6。首先为了使被测样品7被探测部分一次成像,必须把被测样品7放置于探测光的离焦面P上。当被测样品7置于离焦面P上时,则一束发散光从被测样品7表面返回到采样物镜6,在采样物镜6之后利用分光板9,仅使小于10%的光反射出来,进入放大目镜10放大,一次成像到观察屏11上。观察屏11可以是直接观察屏面,或者是探测器的接收面。直接对被测样品7焦点附近的区域即离焦面P进行一次成像。这一分路光束形成准共焦小视场一次成像显微镜,以便用来为点扫描的显微镜定位。经过定位之后,把被测样品7推到采样物镜6的焦面f处,进行共焦点成像。由被测样品7一点上返回的探测光经过分光板9的透射光,再次被耦合到光纤耦合器4中,由光纤耦合器4的第三输出端O3输出,进入放大目镜16中,成像在探测器15的接收面上。进行扫描成像。The utility model has two kinds of microscope functions as the above-mentioned structure, one is microscopic scanning tomography imaging function; the other is primary imaging function. The light path is shown in Figure 1. Part A is the lighting beam input part. The light beam emitted by the laser 1 as the light source is sequentially input into the input end i coupling the objective lens 2 and the fiber coupler 4 , and enters into the fiber coupler 4 . The returned probe light and stray light are emitted from the first output end O1 of the fiber coupler 4, and are emitted into the container 3 containing the refractive index matching liquid. Part B is the fiber scanning part. The light beam output from the second output port O2 of the fiber coupler 4 enters the beam collimating mirror 5, and then the sampling objective lens 6 further focuses the light spot emitted by the fiber into a small light spot and projects it on the sample 7 on the focal plane f to perform the calibration. The detection of the structure of test sample 7. Part D is the detection sampling part. Wherein 14 is the power supply of the detector, the detection light output by the third output port O3 of the fiber coupler 4 is first amplified by the magnifying eyepiece 16 and then input to the receiving surface of the detector 15, and the detector 15 will convert the light information into Electronic information, input to the computer 12 of the E section. Part E is the control data acquisition and processing part. The measured sample 7 is supported by a sample adjustment frame 17 driven by a piezoelectric ceramic driver (PZT) 8 capable of precise scanning, and the scanning step is controlled by a computer 12, which also controls the sampling of part D and performs data processing. Computer 12 controls PZT power supply 13 with balancer. Part C is the measurement and positioning part. When the positioning operation is performed, the light beam from the out-of-focus plane P is reflected back from the measured sample 7 , passes through the sampling objective lens 6 and the beam splitter 9 , enters the magnifying eyepiece 10 , and is imaged on the observation screen 11 . Part C includes the sampling objective lens 6 of part B. First, in order to image the detected portion of the sample 7 under test, the sample 7 under test must be placed on the defocused plane P of the probe light. When the measured sample 7 is placed on the defocus plane P, a bundle of divergent light returns to the sampling objective lens 6 from the surface of the measured sample 7, and after the sampling objective lens 6, the beam splitter 9 is used to reflect less than 10% of the light , enter the magnifying eyepiece 10 to enlarge, and image on the observation screen 11 at one time. The viewing screen 11 may be a direct viewing screen, or a receiving surface of a detector. Imaging is performed directly on the area near the focal point of the measured sample 7 , that is, the out-of-focus plane P. This split beam forms a quasi-confocal small field-of-view primary imaging microscope for use in positioning for point-scanning microscopes. After being positioned, the tested sample 7 is pushed to the focal plane f of the sampling objective lens 6 for confocal imaging. The probe light returned from one point of the tested sample 7 passes through the transmitted light of the beam splitter 9, is coupled into the fiber coupler 4 again, is output by the third output port O3 of the fiber coupler 4, enters the magnifying eyepiece 16, and forms an image on the receiving face of the detector 15. Perform scanning imaging.

该显微镜按功能可分为两大部分,其中一部分是由A、B、D和E构成的光纤共焦扫描显微镜,另一部分由A、B和C组成的准共焦小视场显微镜。本实用新型的光路与已有技术中光纤共焦扫描显微镜的光路相比较,本实用新型的光路在保持原光纤共焦扫描显微镜的紧凑结构的前提下,仅利用测量定位部分C中的分光板9分束构成一个新的小视场准共焦显微镜,使它具有了定位显微镜功能。该定位显微镜本身也是一个准共焦高分辨率的显微镜,它具有亚微米的横向分辨率。它与光纤共焦扫描显微镜有机的结合在一起。已有技术中的光纤共焦扫描显微镜利用点扫描成像形式,无法一次成像,因此没有观察屏11直接观测定位的功能。本实用新型含有A、B、C的小视场显微镜是一次成像结构,可以在观察屏11处用人眼直接观测,为点扫描成像的光纤共焦扫描显微镜预先定位。在操作上,为了对被测样品7成像,必须在轴向移动一些距离,即移到离焦面P的位置,离开夫琅霍斐衍射区。否则在观察屏11上观察到的是夫琅霍斐衍射花样,而不是样品表面的像。本实用新型的光纤共焦扫描显微镜有了测量定位部分C,就像发射炮弹的人有了望远镜。他可以在所看到的广阔视野中,选定目标。反过来讲,若没有望远镜,将是很难确定目标的。本实用新型为光纤共焦扫描显微镜增添了这一重要功能而又未破坏它的结构紧凑轻巧之特点。这必将进一步开拓它在材料科学,生物医学乃至生命科学等学科领域中的应用。The microscope can be divided into two parts according to functions, one part is a fiber confocal scanning microscope composed of A, B, D and E, and the other part is a quasi-confocal small field microscope composed of A, B and C. Compared with the optical path of the optical fiber confocal scanning microscope in the prior art, the optical path of the present utility model only utilizes the beam splitter in the measurement positioning part C under the premise of maintaining the compact structure of the original optical fiber confocal scanning microscope 9 beam splitters form a new quasi-confocal microscope with a small field of view, which enables it to have the function of a positioning microscope. The localization microscope itself is also a quasi-confocal high-resolution microscope with submicron lateral resolution. It is organically combined with the fiber confocal scanning microscope. The optical fiber confocal scanning microscope in the prior art uses the point scanning imaging form and cannot image at one time, so it does not have the function of direct observation and positioning of the observation screen 11 . The utility model includes A, B, and C small-field microscopes with a primary imaging structure, which can be directly observed with human eyes on the observation screen 11, and is pre-positioned for the optical fiber confocal scanning microscope for point scanning imaging. In operation, in order to image the sample 7 under test, it must move some distance in the axial direction, that is, move to a position away from the focal plane P and leave the Fraunhofer diffraction area. Otherwise, what is observed on the observation screen 11 is the Fraunhofer diffraction pattern instead of the image of the sample surface. The optical fiber confocal scanning microscope of the utility model has the measurement and positioning part C, just as the person who launches the shell has a telescope. He can select targets in the wide field of vision he sees. Conversely speaking, without a telescope, it will be difficult to determine the target. The utility model adds this important function to the optical fiber confocal scanning microscope without destroying its compact and light structure. This will further develop its application in material science, biomedicine and even life science and other disciplines.

上述作为光源的激光器1是固体激光器,或者是气体激光器,或者是半导体激光器,或者是其他的相干光源。The above-mentioned laser 1 as a light source is a solid-state laser, or a gas laser, or a semiconductor laser, or other coherent light sources.

上述的样品调节架17是三维调节架。The above-mentioned sample adjusting rack 17 is a three-dimensional adjusting rack.

本实用新型的优点是:The utility model has the advantages of:

1.由于在本实用新型的显微镜中与光纤扫描部分B交错置放有测量定位部分C,这就使得本实用新型的一台显微镜同时具有两种显微镜的功能。既具有光纤扫描显微镜的优点,又具有准共焦小视场显微镜为其定位的功能。因此本实用新型的显微镜既具有结构紧凑轻巧的特点,又具有自定位的功能,操作方便,稳定可靠,实用,便于推广。1. Since the measurement and positioning part C is interlaced with the optical fiber scanning part B in the microscope of the present invention, this makes a microscope of the present invention have the functions of two microscopes simultaneously. It not only has the advantages of fiber scanning microscope, but also has the function of quasi-confocal small field microscope for its positioning. Therefore, the microscope of the utility model not only has the characteristics of compact and light structure, but also has the function of self-positioning, and is easy to operate, stable and reliable, practical and easy to popularize.

2.本实用新型光纤扫描部分B,可以拓扑超高分辨率图像,又可以利用C部分进行准共焦一次成像。小视场准共焦显微镜一方面为光纤共焦扫描显微镜的测定范围定位,另一方面也可以利用它来直接进行亚微米级的微结构检测。该结构的优点如①由于这两种显微镜大部分是共光路的结构,所以光路具有抗干扰性强,适用于各种环境。②一次成像区域围绕在光纤共焦扫描显微镜的探测点附近,视场小,定位准确。③一次成像显微镜是利用相干光照明的,图像清晰,且便于图像边沿定位。2. The optical fiber scanning part B of the utility model can topologically super-high-resolution images, and can use part C to perform quasi-confocal primary imaging. On the one hand, the small-field quasi-confocal microscope positions the measurement range of the fiber-optic confocal scanning microscope, and on the other hand, it can also be used to directly detect submicron microstructures. The advantages of this structure are as follows: ① Since most of these two microscopes have a common optical path structure, the optical path has strong anti-interference and is suitable for various environments. ②The primary imaging area surrounds the detection point of the fiber optic confocal scanning microscope, with a small field of view and accurate positioning. ③Primary imaging microscope is illuminated by coherent light, the image is clear, and it is easy to locate the edge of the image.

3.在探测器15前加入放大目镜16的优点是增加了探测信号细度。假如利用600~800nm的激光为探测光,光纤射出光斑仅有5μm左右的直径。而一般探测器15的分辨率等于或大于这个量级。把光斑放大10多倍成像在探测器15的接收面上,会使探测器15的分辨率相对增加了10~20倍。增加了探测细度。提高了整体仪器的分辨率。3. The advantage of adding the magnifying eyepiece 16 in front of the detector 15 is to increase the fineness of the detection signal. If a 600-800nm laser is used as the probe light, the diameter of the light spot emitted by the fiber is only about 5 μm. However, the resolution of the general detector 15 is equal to or greater than this order of magnitude. Magnifying the light spot by more than 10 times and imaging it on the receiving surface of the detector 15 will relatively increase the resolution of the detector 15 by 10 to 20 times. Increased probing granularity. Improved overall instrument resolution.

附图说明:Description of drawings:

图1为本实用新型的光纤共焦扫描显微镜的光路示意图。FIG. 1 is a schematic diagram of the optical path of the fiber optic confocal scanning microscope of the present invention.

图2为实施例1,利用本实用新型显微镜对被测样品7是闪耀光栅检测结果的曲线图。Fig. 2 is a graph showing the results of the blazed grating detection of the tested sample 7 by using the microscope of the utility model in embodiment 1.

图3为实施例2,利用本实用新型的显微镜对被测样品7是镀膜光盘预刻槽检测结果与已有技术检测结果比较的二维曲线图。图中实线—表示利用本实用新型显微镜的检测结果,虚线———表示利用已有技术的扫描近场光学显微镜的检测结果。点划线—·—表示利用已有技术原子力显微镜检测的结果。Fig. 3 is embodiment 2, utilizes the microscope of the present utility model to test sample 7 is the two-dimensional curve chart of the pregroove detection result of coated optical disc and the prior art detection result comparison. In the figure, the solid line—represents the detection result using the microscope of the utility model, and the dotted line——represents the detection result using the scanning near-field optical microscope of the prior art. The dotted line—·—indicates the results detected by the prior art atomic force microscope.

实施例1:Example 1:

如图1所示结构,激光器1为氦氖激光器,探测器15为CCD探测器(像无间隔为10μm),采样物镜6的参数为40×,NA为0.65,光束准直镜5的参数4×,NA为0.1,光纤耦合器4是与氦氖激光束匹配的单模光纤。其压电陶瓷驱动器PZT8移动分辨率为5nm。被测样品7为闪耀光栅。对其刻线形状及刻线角度进行检测。它的细度为1200线/毫米,其闪耀角为22.3度。利用本实用新型的检测结果:其细度是:1200±50线/mm,该检测数据中包括了光栅的制作和损伤造成的误差。其闪耀角为22.5±0.5度。本实用新型还检测了刻线的高度,结果为350±55nm。测试结果表明这块是被淘汰的光栅,其表面损伤严重。测量结果的截面如图2所示。The structure shown in Figure 1, the laser 1 is a helium-neon laser, the detector 15 is a CCD detector (the distance between images is 10 μm), the parameter of the sampling objective lens 6 is 40×, the NA is 0.65, and the parameter of the beam collimator 5 is 4 ×, NA is 0.1, and the fiber coupler 4 is a single-mode fiber matched with the He-Ne laser beam. Its piezoelectric ceramic driver PZT8 moves with a resolution of 5nm. Test sample 7 is a blazed grating. Detect the shape and angle of the reticle. Its fineness is 1200 lines/mm, and its blaze angle is 22.3 degrees. Utilize the detection result of the utility model: its fineness is: 1200±50 lines/mm, the detection data includes the error caused by the manufacture and damage of the grating. Its blaze angle is 22.5±0.5 degrees. The utility model also detects the height of the reticle, and the result is 350±55nm. The test results showed that this grating was eliminated, and its surface was severely damaged. A cross-section of the measurement results is shown in Figure 2.

实施例2:Example 2:

仍然利用上述结构及各光学元件的参数,被测样品7是镀了膜层的光盘对其预刻槽进行了检测。其被测样品7制作数据为:槽宽为0.4μm,槽间距为1.64±0.05μm,槽高为92±3nm。该检测结果(图3中实线)好于利用已有技术的原子力显微镜(图3中点划线)和近场扫描光学显微镜(图3中虚线)的检测结果。由图3示出。Still using the above-mentioned structure and parameters of each optical element, the tested sample 7 is an optical disc coated with a film layer, and its pre-groove is tested. The production data of the tested sample 7 are: the groove width is 0.4 μm, the groove spacing is 1.64±0.05 μm, and the groove height is 92±3 nm. The detection result (solid line in FIG. 3 ) is better than the detection results of the prior art atomic force microscope (dotted line in FIG. 3 ) and near-field scanning optical microscope (dashed line in FIG. 3 ). Shown in Figure 3.

Claims (3)

1.一种光纤共焦扫描显微镜,包括照明光束输入部分(A),光纤扫描部分(B),探测采样部分(D)和控制数据采集处理部分(E),其中照明光束输入部分(A)包括沿着激光器(1)出射光束前进的方向上依次置有耦合物镜(2),光纤耦合器(4),在光纤耦合器(4)的第一输出端(O1)上置有盛放折射率匹配液的容器(3);光纤扫描部分B包括沿光纤耦合器(4)第二输出端(O2)输出光束前进方向上,依次置有光束准直镜(5),采样物镜(6)和置于采样物镜(6)焦面(f)上的被测样品(7);探测采样部分(D)包括在光纤耦合器(4)第三输出端(O3)出射光束的前进方向上置有带探测器电源(14)的探测器(15);控制数据采集处理部分E包括置放被测样品(7)的带压电陶瓷驱动器(8)的由压电陶瓷构成的样品调节架(17),压电陶瓷驱动器(8)通过带平衡器的电源(13)与计算机(12)相联,计算机(12)同时还与探测采样部分(D)中的探测器(15)相联,其特征在于与光纤扫描部分(B)交错置放的有测量定位部分(C),测量定位部分(C)包括沿着置于样品调节架(17)上,在采样物镜(6)的离焦面(P)上的被测样品(7)反射回来的光束前进方向上,依次有采样物镜(6),分光板(9),在分光板(9)反射光束前进的方向上,依次有放大目镜(10)和观察屏(11);在探测采样部分(D)中,在光纤耦合器(4)的第三输出端(O3)与探测器(15)的接收面之间置有放大目镜(16)。1. A fiber optic confocal scanning microscope, comprising an illumination beam input part (A), an optical fiber scanning part (B), a detection sampling part (D) and a control data acquisition processing part (E), wherein the illumination beam input part (A) Including a coupling objective lens (2) and a fiber coupler (4) arranged sequentially along the direction in which the light beam emitted by the laser (1) advances, and a container placed on the first output end (O 1 ) of the fiber coupler (4) The container (3) of the refractive index matching liquid; the optical fiber scanning part B includes a beam collimating mirror ( 5 ) and a sampling objective lens ( 6) and the measured sample (7) placed on the focal plane (f) of the sampling objective lens (6); the detection sampling part (D) includes the advancement of the outgoing light beam at the third output end (O 3 ) of the fiber coupler (4) A detector (15) with a detector power supply (14) is placed in the direction; the control data acquisition and processing part E includes a sample made of piezoelectric ceramics with a piezoelectric ceramic driver (8) for placing the measured sample (7) The adjustment frame (17), the piezoelectric ceramic driver (8) is connected with the computer (12) through the power supply (13) with a balancer, and the computer (12) is also connected with the detector (15) in the detection sampling part (D) Connected, it is characterized in that there is a measurement positioning part (C) interlaced with the optical fiber scanning part (B), and the measurement positioning part (C) includes placing on the sample adjustment frame (17) along the sampling objective lens (6) On the out-of-focus surface (P) of the measured sample (7) in the direction of the light beam reflected back, there are in turn a sampling objective lens (6), a beam splitter (9), and in the direction of the light beam reflected by the beam splitter (9), There are magnifying eyepieces (10) and observation screens (11) in sequence; in the detection sampling part (D), between the third output end (O 3 ) of the fiber optic coupler (4) and the receiving surface of the detector (15) A magnifying eyepiece (16) is provided. 2.按照权利要求1所述的光纤共焦扫描显微镜,其特征在于测量定位部分(C)中的分光板(9)的反射率小于10%。2. The optical fiber confocal scanning microscope according to claim 1, characterized in that the reflectance of the beam splitter (9) in the measurement positioning part (C) is less than 10%. 3.按照权利要求1所述的光纤共焦扫描显微镜,其特征在于测量定位部分(C)中的观察屏(11)是直接观察屏面,或者是探测器的接收面。3. The optical fiber confocal scanning microscope according to claim 1, characterized in that the observation screen (11) in the measurement positioning part (C) is a direct observation screen, or a receiving surface of a detector.
CN 99240337 1999-11-16 1999-11-16 Optical fiber confocal scanning microscope Expired - Fee Related CN2397505Y (en)

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Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101776791B (en) * 2010-01-08 2012-09-26 华中科技大学 Light stimulation device
CN103926228A (en) * 2014-04-28 2014-07-16 江苏天宁光子科技有限公司 Laser scanning fluorescence confocal microscopic endoscopic imaging system
CN109443241A (en) * 2018-12-07 2019-03-08 哈尔滨工业大学 A kind of high speed axial direction scanning confocal micro-measurement apparatus and method based on tuning fork driving
CN109443240A (en) * 2018-12-07 2019-03-08 哈尔滨工业大学 A kind of laser triangulation optical measurement instrument and method based on intermediary layer scattering
CN109458950A (en) * 2018-12-07 2019-03-12 哈尔滨工业大学 A kind of servo-actuated confocal microscopy device and method of pin hole based on intermediary layer scattering
CN118882501A (en) * 2024-09-26 2024-11-01 中国科学院长春光学精密机械与物理研究所 Linear differential confocal displacement sensor system based on lateral encoding

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101776791B (en) * 2010-01-08 2012-09-26 华中科技大学 Light stimulation device
CN103926228A (en) * 2014-04-28 2014-07-16 江苏天宁光子科技有限公司 Laser scanning fluorescence confocal microscopic endoscopic imaging system
CN109443241A (en) * 2018-12-07 2019-03-08 哈尔滨工业大学 A kind of high speed axial direction scanning confocal micro-measurement apparatus and method based on tuning fork driving
CN109443240A (en) * 2018-12-07 2019-03-08 哈尔滨工业大学 A kind of laser triangulation optical measurement instrument and method based on intermediary layer scattering
CN109458950A (en) * 2018-12-07 2019-03-12 哈尔滨工业大学 A kind of servo-actuated confocal microscopy device and method of pin hole based on intermediary layer scattering
CN118882501A (en) * 2024-09-26 2024-11-01 中国科学院长春光学精密机械与物理研究所 Linear differential confocal displacement sensor system based on lateral encoding

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