CN105184295B - A kind of holoscan space length extracting method based on wavelet transformation and connected domain - Google Patents
A kind of holoscan space length extracting method based on wavelet transformation and connected domain Download PDFInfo
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Abstract
Description
技术领域technical field
本发明涉及光学扫描全息领域与图像重建领域,具体来说,涉及一种基于小波变换与连通域的实现全息扫描空间距离提取方法。The present invention relates to the field of optical scanning holography and image reconstruction, in particular to a method for extracting spatial distance of holographic scanning based on wavelet transform and connected domain.
背景技术Background technique
光学扫描全息技术,简称OSH,是一种数字全息技术,它是由Poon和Korpel最早提出,OSH可以将3维物体的信息存储为2维的全息图。自该项技术提出以来,已经在扫描全息显微镜、3D图像识别以及3D光学遥感等领域得到了广泛的应用。Optical scanning holography technology, referred to as OSH, is a digital holography technology. It was first proposed by Poon and Korpel. OSH can store the information of 3-dimensional objects as 2-dimensional holograms. Since the technology was proposed, it has been widely used in the fields of scanning holographic microscope, 3D image recognition and 3D optical remote sensing.
空间距离提取技术是OSH中一项重要的技术,它可以提取出待测物体的轴向空间信息,而待测物体的轴向空间信息是进行图像重建的重要参数。因此,空间距离提取技术也具有了重要的研究价值。研究证明,在迭代运算中,通过小波分解和连通域算法可以寻找出重建图像边缘的最大值,并抑制离焦图像边缘,当得到边缘的最大值时,即可推测出待测物体的轴向空间信息,从而实现空间距离提取。Spatial distance extraction technology is an important technology in OSH. It can extract the axial spatial information of the object to be measured, and the axial spatial information of the object to be measured is an important parameter for image reconstruction. Therefore, the spatial distance extraction technology also has important research value. The research proves that in the iterative operation, the maximum value of the edge of the reconstructed image can be found through the wavelet decomposition and the connected domain algorithm, and the edge of the out-of-focus image can be suppressed. When the maximum value of the edge is obtained, the axial direction of the object to be measured can be inferred Spatial information, so as to realize spatial distance extraction.
文献《Autofocusing in optical scanning holography》提出了Wigner分布来提取待测物体的轴向空间信息,但是该方法的限制较多并且准确性较低。The document "Autofocusing in optical scanning holography" proposes the Wigner distribution to extract the axial spatial information of the object to be measured, but this method has many limitations and low accuracy.
文献《Blind sectional image reconstruction for optical scanningholography》提出利用Prewitt算子提取重建图像边缘,这种方法具有较好的实用性,但是由于离焦噪声边缘的存在,影响了计算结果的精确度。The document "Blind sectional image reconstruction for optical scanningholography" proposes to use the Prewitt operator to extract the edges of the reconstructed image. This method has good practicability, but due to the existence of defocus noise edges, the accuracy of the calculation results is affected.
发明内容Contents of the invention
本发明的目的在于光学全息扫描自动对焦,提出小波变换与连通域的实现全息扫描空间距离提取方法,该方法通过利用小波变换,提取图像高频成分,去除低频成分,从而提取出图像边缘,同时,利用连通域算法,抑制离焦图像边缘,保留完整的对焦图像边缘。The purpose of the present invention is to automatically focus on optical holographic scanning, and propose a method for extracting space distance of holographic scanning through wavelet transform and connected domain. The method extracts image high-frequency components and removes low-frequency components by using wavelet transform, thereby extracting image edges, and at the same time , using the connected domain algorithm to suppress the edge of the out-of-focus image and retain the complete edge of the in-focus image.
本发明采用的技术方案是:The technical scheme adopted in the present invention is:
一种小波变换与连通域的实现全息扫描空间距离提取方法,其流程如图1所示,包括以下步骤:A method for extracting distance from a holographic scanning space realized by wavelet transform and connected domain, the process of which is shown in Figure 1, including the following steps:
步骤1.将激光通过第一偏振分束器分为两束光路,其中一条光束依次通过一个声光调制器和扩束器,另一条光束依次通过另一个声光调制器、扩束器及凸透镜后,将这两条光束经过第二偏振分束器聚光后干涉形成菲涅尔干涉条纹;Step 1. Divide the laser light into two beam paths through the first polarizing beam splitter, one of which passes through an AOM and a beam expander in sequence, and the other beam passes through another AOM, a beam expander and a convex lens in sequence Finally, the two beams are condensed by the second polarizing beam splitter and then interfered to form Fresnel interference fringes;
步骤2.通过所述菲涅尔干涉条纹对待测物体进行扫描,并利用光电检测器接收扫描后的光信息,从而获得待测物体的全息图;Step 2. Scan the object to be measured through the Fresnel interference fringes, and use the photodetector to receive the scanned light information, so as to obtain a hologram of the object to be measured;
步骤3.设置距离参数的初值及其上限值,设定距离参数的扫描步长,以所述初值作为距离参数的当前值;Step 3. set the initial value and upper limit value of the distance parameter, set the scan step length of the distance parameter, and use the initial value as the current value of the distance parameter;
步骤4.将所得的全息图做傅里叶变换后,与带有所述距离参数的传统光学传递函数的频域表达式的共轭相乘后,再经过逆傅里叶变换,即可得到待测物体的重建图像;Step 4. After performing Fourier transform on the obtained hologram, after multiplying with the conjugate of the frequency domain expression of the traditional optical transfer function with the distance parameter, and then through inverse Fourier transform, you can get A reconstructed image of the object to be tested;
步骤5.将重建图像进行小波分解,即对图像做离焦图像抑制操作去除低频成分信息、保留高频成分信息,得到含有离焦噪声的待测物体边缘图像;Step 5. Perform wavelet decomposition on the reconstructed image, that is, perform a defocused image suppression operation on the image to remove low-frequency component information, retain high-frequency component information, and obtain an edge image of the object to be measured containing defocus noise;
步骤6.采用连通域算法,去除所述待测物体边缘图像的离焦噪声,最后得到无离焦噪声的边缘图像;计算、记录所述无离焦噪声的边缘图像的边缘长度及其对应的距离参数值;Step 6. Use the connected domain algorithm to remove the defocus noise of the edge image of the object to be measured, and finally obtain an edge image without defocus noise; calculate and record the edge length of the edge image without defocus noise and its corresponding distance parameter value;
步骤7.将距离参数的当前值加上一个扫描步长作为距离参数的最新值,并重复执行步骤4至步骤6直至距离参数的当前值已达所设定的上限值时止,由此获得多个边缘长度;提取边缘长度中最大的两个值对应的距离参数值,所述两个距离参数值即为待测物体在轴向空间上所处的位置区间。Step 7. Add a scan step to the current value of the distance parameter as the latest value of the distance parameter, and repeat steps 4 to 6 until the current value of the distance parameter has reached the set upper limit, thus Obtaining a plurality of edge lengths; extracting distance parameter values corresponding to the two largest values of the edge lengths, the two distance parameter values being the position interval of the object to be measured in the axial space.
本发明的有益效果是:The beneficial effects of the present invention are:
(1)本发明使用了光学扫描全息技术,通过小波分解与连通域算法实现对待测物体的轴向空间信息提取,全息扫描空间距离提取技术应用范围包括生物细胞观察、机械控制、光学聚焦等,因此本发明适用于各个领域,应用范围非常广;(1) The present invention uses optical scanning holography technology, and realizes the extraction of axial spatial information of the object to be measured through wavelet decomposition and connected domain algorithm. The application scope of holographic scanning space distance extraction technology includes biological cell observation, mechanical control, optical focusing, etc. Therefore, the present invention is applicable to various fields and has a very wide range of applications;
(2)本发明利用小波分解实现对离焦图像的抑制并提取出对焦图像的边缘,另外通过连通域算法对图像作进一步处理,从而提高了空间距离提取的精确度;(2) The present invention utilizes wavelet decomposition to realize the suppression of the out-of-focus image and extracts the edge of the focus image, and further processes the image through the connected domain algorithm, thereby improving the accuracy of spatial distance extraction;
(3)本发明只需要调节小波分解的细节系数阈值以及连通域阈值,即可实现离焦图像的有效抑制,并准确提取出待测物体的轴向空间信息;(3) The present invention only needs to adjust the detail coefficient threshold and connected domain threshold of wavelet decomposition to realize effective suppression of out-of-focus images and accurately extract the axial spatial information of the object to be measured;
(4)本发明不仅实现方式简单、便于操作,同时具有很强的实用性,适合推广使用。(4) The present invention is not only simple in implementation and easy to operate, but also has strong practicability and is suitable for popularization and use.
附图说明Description of drawings
图1为本发明提供的方法流程示意图;Fig. 1 is the schematic flow chart of the method provided by the present invention;
图2为本发明实施例的基本结构图;Fig. 2 is the basic structural diagram of the embodiment of the present invention;
图3为本发明实施例的待测物体示意图;3 is a schematic diagram of an object to be measured according to an embodiment of the present invention;
图4为本发明实施例的待测物体全息图;FIG. 4 is a hologram of an object to be measured according to an embodiment of the present invention;
图5为本发明实施例的重建图像;Fig. 5 is the reconstruction image of the embodiment of the present invention;
图6为本发明实施例的对焦图像小波分解与连通域算法效果图;Fig. 6 is an effect diagram of wavelet decomposition and connected domain algorithm of the focused image according to the embodiment of the present invention;
图7为本发明实施例的离焦图像小波分解与连通域算法效果图;Fig. 7 is a defocused image wavelet decomposition and connected domain algorithm effect diagram according to an embodiment of the present invention;
图8为本发明实施例的边缘长度双峰函数图。Fig. 8 is a diagram of a bimodal function of edge length according to an embodiment of the present invention.
具体实施方式Detailed ways
下面结合附图与实施例对本发明进一步说明。The present invention will be further described below in conjunction with the accompanying drawings and embodiments.
实施例Example
本发明实施例流程如图1所示,所采用的基本结构如图2所示,其中He-Ne激光器Laser的波长λ=632.8nm,声光调制器(AOFS1,AOFS2)转换频率分别为Ω/2π=79.98MHz和(Ω+ΔΩ)/2π=40MHz,凸透镜L1的焦距为500mm,待测物体如图3所示,XOY平面尺寸为1.5cm×1.5cm,矩阵尺寸为500×500,其轴向位置分别为z1=870mm,z2=1070mm,按照如下步骤即可实现扫描过程:The process flow of the embodiment of the present invention is shown in Figure 1, and the basic structure adopted is shown in Figure 2, wherein the wavelength λ=632.8nm of the He-Ne laser Laser, and the conversion frequency of the acousto-optic modulator (AOFS1, AOFS2) is Ω/ 2π=79.98MHz and (Ω+ΔΩ)/2π=40MHz, the focal length of the convex lens L1 is 500mm, the object to be measured is shown in Figure 3, the XOY plane size is 1.5cm×1.5cm, the matrix size is 500×500, and its axis The positions in the directions are z 1 =870mm, z 2 =1070mm, and the scanning process can be realized according to the following steps:
步骤1.将激光通过第一偏振分束器分为两束光路,其中一条光束依次通过一个声光调制器和扩束器,另一条光束依次通过另一个声光调制器、扩束器及凸透镜后,将这两条光束经过第二偏振分束器聚光后干涉形成菲涅尔干涉条纹;Step 1. Divide the laser light into two beam paths through the first polarizing beam splitter, one of which passes through an AOM and a beam expander in sequence, and the other beam passes through another AOM, a beam expander and a convex lens in sequence Finally, the two beams are condensed by the second polarizing beam splitter and then interfered to form Fresnel interference fringes;
本实施例采用的系统结构如图2所示,由同一光源发出的角频率为ω的光被第一偏振分束器BS1分成两束,其中一束通过声光调制器AOFS1与凸透镜L1,形成球面波;另一束经过声光调制器AOFS2,形成平面波;两束光经第二偏振分束器聚合后在待测物体前干涉形成菲涅尔干涉条纹,其在待测物体所处轴向空间上的表达式如下:The system structure used in this embodiment is shown in Figure 2. The light with angular frequency ω emitted by the same light source is divided into two beams by the first polarizing beam splitter BS1, one of which passes through the acousto-optic modulator AOFS1 and the convex lens L1 to form Spherical wave; the other beam passes through the acousto-optic modulator AOFS2 to form a plane wave; the two beams are aggregated by the second polarizing beam splitter and interfere in front of the object to be measured to form Fresnel interference fringes, which are in the axial direction of the object to be measured The spatial expression is as follows:
其中,待测物体在轴向上划分成n层,zi表示待测物体的第i层所在的轴向位置,NA表示数字孔径,λ表示激光波长,kx和ky表示频域坐标;Among them, the object to be measured is divided into n layers in the axial direction, z i represents the axial position of the i-th layer of the object to be measured, NA represents the numerical aperture, λ represents the laser wavelength, k x and ky represent frequency domain coordinates;
步骤2.通过所述菲涅尔干涉条纹对待测物体进行扫描,并利用光电检测器接收扫描后的光信息,从而获得待测物体的全息图;Step 2. Scan the object to be measured through the Fresnel interference fringes, and use the photodetector to receive the scanned light information, so as to obtain a hologram of the object to be measured;
本实施例利用菲涅尔干涉条纹对物体进行扫描,将形成的全息图存储到计算机里,如图4,具体如下:In this embodiment, Fresnel interference fringes are used to scan the object, and the formed hologram is stored in the computer, as shown in Figure 4, as follows:
其中,g(x,y)表示全息图,F-1、F分别表示傅里叶逆变换和傅里叶变换,i表示待测物体在轴向上的第i层,I(x,y;zi)表示待测物的复振幅函数;Among them, g(x, y) represents the hologram, F -1 and F represent inverse Fourier transform and Fourier transform respectively, i represents the i-th layer of the object to be measured in the axial direction, I(x, y; z i ) represents the complex amplitude function of the object to be measured;
步骤3.设置距离参数的初值及其上限值,设定距离参数的扫描步长,以所述初值作为距离参数的当前值;本实施例中,设置距离参数初值为zo=854.6mm,上限值为zt=1239.6mm;Step 3. Set the initial value of the distance parameter and its upper limit value, set the scan step length of the distance parameter, and use the initial value as the current value of the distance parameter; in this embodiment, set the initial value of the distance parameter to z o = 854.6mm, the upper limit is z t = 1239.6mm;
步骤4.将所得的全息图做傅里叶变换后,与带有所述距离参数的传统光学传递函数的频域表达式的共轭相乘后,再经过逆傅里叶变换,即可得到待测物体的重建图像,如图5所示;Step 4. After performing Fourier transform on the obtained hologram, after multiplying with the conjugate of the frequency domain expression of the traditional optical transfer function with the distance parameter, and then through inverse Fourier transform, you can get The reconstructed image of the object to be measured, as shown in Figure 5;
本实施例中,通过光学传递函数进行图像重建的具体表达如下:In this embodiment, the specific expression of image reconstruction through the optical transfer function is as follows:
其中,Ij(x,y)表示待测物体第j层的重建图像信息,zj表示待测物体重建图像第j层所在的轴向位置,F-1、F分别表示傅里叶逆变换及傅里叶变换,*表示共轭,表示卷积;Among them, I j (x, y) represents the reconstructed image information of the jth layer of the object under test, z j represents the axial position of the jth layer of the reconstructed image of the object under test, and F -1 and F respectively represent the inverse Fourier transform and Fourier transform, * means conjugate, Indicates convolution;
步骤5.将重建图像进行小波分解,即对图像做离焦图像抑制操作去除低频成分信息、保留高频成分信息,得到含有离焦噪声的待测物体边缘图像;Step 5. Perform wavelet decomposition on the reconstructed image, that is, perform a defocused image suppression operation on the image to remove low-frequency component information, retain high-frequency component information, and obtain an edge image of the object to be measured containing defocus noise;
本实施例中,通过小波分解对重建图像进行处理的具体表达式如下:In this embodiment, the specific expression for processing the reconstructed image through wavelet decomposition is as follows:
其中表示细节系数,M×N表示图像规格大小,k1、k2表示x,y轴的转换比;d=H、V、D,分别代表水平方向、垂直方向、对角线方向;的表达式如下:in Represents the detail coefficient, M×N represents the image size, k 1 and k 2 represent the conversion ratio of x and y axes; d=H, V, D, respectively represent the horizontal direction, vertical direction, and diagonal direction; The expression of is as follows:
其中,表示小波函数,ψ表示尺度函数,具体如下:in, represents the wavelet function, and ψ represents the scaling function, as follows:
其中,表示小波函数系数,hψ表示尺度函数系数,且采用哈尔小波,其表达式如下:in, represents the wavelet function coefficient, h ψ represents the scaling function coefficient, and Using Haar wavelet, its expression is as follows:
对图像做初步的离焦图像抑制,其具体操作如下:Perform preliminary out-of-focus image suppression on the image, the specific operation is as follows:
其中,表示所有细节系数中的最大值;对焦图像边缘提取的效果如图6(b)所示;离焦图像边缘提取的效果如图7(b)所示;in, Indicates the maximum value of all detail coefficients; the effect of edge extraction of in-focus images is shown in Figure 6(b); the effect of edge extraction of out-of-focus images is shown in Figure 7(b);
图像边缘提取表达式如下:The image edge extraction expression is as follows:
步骤6.采用连通域算法,去除所述待测物体边缘图像的离焦噪声,最后得到无离焦噪声的边缘图像,其效果如图6(c)、7(c)所示;计算、记录所述无离焦噪声的边缘图像的边缘长度及其对应的距离参数值;Step 6. Adopt the connected domain algorithm to remove the defocus noise of the edge image of the object to be measured, and finally obtain the edge image without defocus noise, as shown in Fig. 6 (c) and 7 (c); calculate and record The edge length of the edge image without defocus noise and its corresponding distance parameter value;
步骤7.将距离参数的当前值加上一个扫描步长作为距离参数的最新值,并重复执行步骤4至步骤6直至距离参数的当前值已达所设定的上限值时止,由此获得多个边缘长度;提取边缘长度最大的两个值对应的距离参数值,所述两个距离参数值构成的范围即为待测物体在轴向空间上所处的位置,如图8所示,两个局部最大峰值所对应的距离就是待测物体所在的轴向距离,可知所得的待测物体轴向空间位置与其实际所处的空间位置吻合。Step 7. Add a scan step to the current value of the distance parameter as the latest value of the distance parameter, and repeat steps 4 to 6 until the current value of the distance parameter has reached the set upper limit, thus Obtain multiple edge lengths; extract the distance parameter values corresponding to the two maximum edge length values, and the range formed by the two distance parameter values is the position of the object to be measured in the axial space, as shown in Figure 8 , the distance corresponding to the two local maximum peaks is the axial distance of the object to be measured. It can be seen that the obtained axial spatial position of the object to be measured is consistent with its actual spatial position.
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CN106228169A (en) * | 2016-08-02 | 2016-12-14 | 电子科技大学 | The distance extracting method in holoscan space based on discrete cosine transform |
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