CN109855558A - Digital hologram three-dimensional method for reconstructing - Google Patents
Digital hologram three-dimensional method for reconstructing Download PDFInfo
- Publication number
- CN109855558A CN109855558A CN201711240115.8A CN201711240115A CN109855558A CN 109855558 A CN109855558 A CN 109855558A CN 201711240115 A CN201711240115 A CN 201711240115A CN 109855558 A CN109855558 A CN 109855558A
- Authority
- CN
- China
- Prior art keywords
- interference
- phase
- positive
- dimensional
- information
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 238000000034 method Methods 0.000 title claims abstract description 33
- 230000003287 optical effect Effects 0.000 claims abstract description 18
- 239000000284 extract Substances 0.000 claims abstract description 10
- 238000005305 interferometry Methods 0.000 claims abstract description 6
- 230000009466 transformation Effects 0.000 claims description 10
- 238000001093 holography Methods 0.000 claims description 7
- 238000005259 measurement Methods 0.000 abstract description 13
- 238000005457 optimization Methods 0.000 description 7
- 238000010586 diagram Methods 0.000 description 6
- 230000010363 phase shift Effects 0.000 description 4
- 238000004458 analytical method Methods 0.000 description 3
- 230000007613 environmental effect Effects 0.000 description 2
- 238000001914 filtration Methods 0.000 description 2
- 238000003384 imaging method Methods 0.000 description 1
- 230000008092 positive effect Effects 0.000 description 1
- 238000006467 substitution reaction Methods 0.000 description 1
Landscapes
- Holo Graphy (AREA)
- Instruments For Measurement Of Length By Optical Means (AREA)
Abstract
本发明提出一种数字全息三维重建方法,该方法包括以下步骤:S0:对一幅干涉条纹图像进行二维傅立叶变换;对傅立叶频域分析处理后进行二维傅立叶逆变换;S1:判断相位衍射平面到干涉条纹图像平面的距离是否为0,如是,则将执行S3;如否,则执行S2;S2:对提取的正的干涉相位信息进行菲涅尔数字衍射计算,提取正的物体光相位信息,并调整菲涅尔数字衍射距离为聚焦位置,以获取聚焦位置的相位;S3:将提取的正的信息代入干涉测量法公式计算,获取物体的立体高度信息,以进行数字全息三维的重建。该方法通过对一幅干涉条纹图像进行频域分析,实现了高速实时且精密稳定的单次曝光数字全息测量。
The present invention provides a digital holographic three-dimensional reconstruction method, which comprises the following steps: S0: performing two-dimensional Fourier transform on an interference fringe image; performing two-dimensional inverse Fourier transform after analyzing and processing the Fourier frequency domain; S1: judging phase diffraction Whether the distance from the plane to the interference fringe image plane is 0, if so, execute S3; if not, execute S2; S2: Perform Fresnel digital diffraction calculation on the extracted positive interference phase information, and extract the positive optical phase of the object information, and adjust the Fresnel digital diffraction distance as the focus position to obtain the phase of the focus position; S3: Substitute the extracted positive information into the interferometry formula for calculation, and obtain the stereo height information of the object for digital holographic three-dimensional reconstruction . The method realizes high-speed, real-time, precise and stable single-exposure digital holographic measurement by analyzing an interference fringe image in the frequency domain.
Description
技术领域technical field
本发明属于数字全息领域,尤其涉及一种利用二维傅立叶干涉条纹分析的数字全息三维重建方法。The invention belongs to the field of digital holography, in particular to a three-dimensional reconstruction method of digital holography using two-dimensional Fourier interference fringe analysis.
背景技术Background technique
数字全息是指利用光学干涉及衍射原理的数字化光场重建的方法,数字全息将反射光的不透明物体表面或者透过光的透明、半透明物体内部结构中每一个三维空间中的点看作为一个点光源,通过数字化光学干涉和衍射的数学公式,利用计算机计算出这些点光源发光时光波相位,根据干涉测量法实现对不透明物体表面或者透明、半透明物体形状进行纳米级超精密的三维测量。Digital holography refers to a method of digital light field reconstruction using the principle of optical interference and diffraction. Digital holography regards each point in the three-dimensional space on the surface of an opaque object that reflects light or the internal structure of transparent and translucent objects that transmit light as a point. The point light source, through the mathematical formula of digital optical interference and diffraction, uses the computer to calculate the light wave phase of these point light sources when they emit light, and realizes the ultra-precise three-dimensional measurement of the surface of opaque objects or the shape of transparent and translucent objects according to the interferometry method.
进行数字全息超精密三维测量时,需要干涉条纹的记录和物体光重建两个步骤。而干涉条纹的记录需要通过搭建干涉光学系统并使用数字相机拍摄干涉条纹完成;物体光重建则需要使用数字菲涅耳变换对干涉条纹图像进行数字化衍射计算从而得到物体光场中光的相位分布,最终使用干涉测量法实现三维重建。When performing ultra-precise 3D measurement of digital holography, two steps are required: the recording of interference fringes and the reconstruction of object light. The recording of interference fringes needs to be completed by building an interference optical system and using a digital camera to photograph the interference fringes; the optical reconstruction of the object needs to use digital Fresnel transform to digitally diffract the interference fringe image to obtain the phase distribution of the light in the light field of the object. Finally, the three-dimensional reconstruction is achieved using interferometry.
现有技术中,其使用的菲涅耳变换的数学公式如下:In the prior art, the mathematical formula of the Fresnel transform used by it is as follows:
上述式(1)中,Γ(ξ′,η′)为菲涅耳衍射平面上的光复数信息,包括光强和相位,(ξ′,η′)表示菲涅耳衍射平面上的平面坐标,A(x,y)为光源透过光圈平面中光圈时的光复数信息,仅含有光强值,也就是干涉条纹图像的灰度值,(x,y)表示光圈平面上的平面坐标,d表示菲涅耳衍射平面和光圈平面之间的垂直距离,ρ′表示光圈上的一点颜射到菲涅耳衍射平面上一点时的衍射距离,λ表示光源的光波长值,i表示复数。In the above formula (1), Γ(ξ', η') is the optical complex information on the Fresnel diffraction plane, including light intensity and phase, and (ξ', η') represents the plane coordinates on the Fresnel diffraction plane , A(x, y) is the complex number information of light when the light source passes through the aperture in the aperture plane, it only contains the light intensity value, that is, the gray value of the interference fringe image, (x, y) represents the plane coordinates on the aperture plane, d represents the vertical distance between the Fresnel diffraction plane and the aperture plane, ρ′ represents the diffraction distance from a point on the aperture to a point on the Fresnel diffraction plane, λ represents the light wavelength value of the light source, and i represents a complex number.
上述中可知,双重积分在计算机计算上不具备速度优势,存在计算机编程烦琐的缺点。另外,使用式(1)进行数字全息三维重建时,通常将数字相机拍摄到的干涉条纹直接代入公式,由于数字相机拍摄到的仅仅是干涉条纹的光强,而干涉条纹呈正弦波的形式,因此通常的三维重建中,如下述式(2)所示,正弦波的正的相位、负的相位以及直流成分将同时被重建出来,其中仅有正的相位精确反映了实际物体的形状信息,负的相位和直流成分作为噪声影响着精确的测量。It can be seen from the above that double integral does not have the advantage of speed in computer calculation, and has the disadvantage of cumbersome computer programming. In addition, when using formula (1) for digital holographic three-dimensional reconstruction, the interference fringes captured by the digital camera are usually directly substituted into the formula. Since the digital camera captures only the light intensity of the interference fringes, and the interference fringes are in the form of sine waves, Therefore, in the usual three-dimensional reconstruction, as shown in the following formula (2), the positive phase, negative phase and DC component of the sine wave will be reconstructed at the same time, and only the positive phase accurately reflects the shape information of the actual object, Negative phase and DC components affect accurate measurements as noise.
其中,A(x,y)表示干涉条纹图像的灰度值,(x,y)表示图像坐标。AR(x,y)表示参照光的复变函数,Ao(x,y)表示物体光的复变函数,表示参照光复变函数的共轭,即相位相反,表示物体光复变函数的共轭。B(x,y)表示干涉条纹中的直流信息,表示干涉条纹中负的物体光相位信息,Ao(x,y)表示三维重建真正需要的物体光正的相位信息。Among them, A(x, y) represents the gray value of the interference fringe image, and (x, y) represents the image coordinates. AR (x, y) represents the complex variable function of the reference light, A o (x, y) represents the complex variable function of the object light, represents the conjugate of the reference light complex function, that is, the phase is opposite, Represents the conjugate of the complex optical function of the object. B(x, y) represents the DC information in the interference fringes, Represents the negative phase information of the object light in the interference fringes, and A o (x, y) represents the positive phase information of the object light that is really needed for 3D reconstruction.
上述现有技术中,虽然利用相移数字全息能够实现从一幅图像中提取正的物体光相位信息,但是却需要2-4幅相移干涉条纹图像,拍摄多幅相移干涉条纹图像耗费时间且拍摄过程中干涉条纹的相移精度极易受到震动、空气对流等环境因素影响,不仅无法实现快速实时的数字全息三维测量而且测量环境要求苛刻,这些因素都导致数字全息测量设备价格昂贵,应用场合受限。In the above-mentioned prior art, although phase-shift digital holography can be used to extract positive object optical phase information from an image, 2-4 phase-shift interference fringe images are required, and it takes time to capture multiple phase-shift interference fringe images. In addition, the phase shift accuracy of interference fringes during the shooting process is easily affected by environmental factors such as vibration and air convection, which not only cannot achieve fast and real-time digital holographic 3D measurement, but also has strict measurement environment requirements. These factors make digital holographic measurement equipment expensive. Occasion limited.
发明内容SUMMARY OF THE INVENTION
为了解决上述问题,本发明提供了一种数字全息三维重建方法,该数字全息三维重建方法,通过对一幅干涉条纹图像进行频域分析,快速实时地从一幅干涉条纹图像中提取三维测量所需的正的物体光相位信息,从而实现高速实时且精密稳定的单次曝光数字全息测量。In order to solve the above problems, the present invention provides a digital holographic three-dimensional reconstruction method. The digital holographic three-dimensional reconstruction method can quickly and real-timely extract the three-dimensional measurement data from an interference fringe image by performing frequency domain analysis on an interference fringe image. The required positive optical phase information of the object can be achieved to achieve high-speed real-time, precise and stable single-exposure digital holographic measurement.
为了达到上述目的,本发明采用的技术方案为:In order to achieve the above object, the technical scheme adopted in the present invention is:
一种数字全息三维重建方法,包括以下步骤:A digital holographic three-dimensional reconstruction method, comprising the following steps:
S0:对一幅干涉条纹图像进行二维傅立叶变换,以将干涉条纹图像转换为傅立叶频域;对傅立叶频域分析处理后进行二维傅立叶逆变换,以形成图像域;并提取正的干涉相位信息;S0: Perform a two-dimensional Fourier transform on an interference fringe image to convert the interference fringe image into the Fourier frequency domain; perform two-dimensional inverse Fourier transform after analyzing and processing the Fourier frequency domain to form the image domain; and extract the positive interference phase information;
S1:判断相位衍射平面到干涉条纹图像平面的距离是否为0,如是,则将执行S3;如否,则执行S2;S1: Determine whether the distance from the phase diffraction plane to the interference fringe image plane is 0, if so, execute S3; if not, execute S2;
S2:对提取的正的干涉相位信息进行菲涅尔数字衍射计算,提取正的物体光相位信息,并调整菲涅尔数字衍射距离为聚焦位置,以获取聚焦位置的相位;S2: perform Fresnel digital diffraction calculation on the extracted positive interference phase information, extract the positive optical phase information of the object, and adjust the Fresnel digital diffraction distance as the focus position to obtain the phase at the focus position;
S3:将提取的正的信息代入干涉测量法公式计算,获取物体的立体高度信息,以进行数字全息三维的重建。S3: Substitute the extracted positive information into the interferometry formula for calculation, and obtain the stereoscopic height information of the object, so as to carry out digital holographic three-dimensional reconstruction.
作为本发明的进一步优化,在步骤S0中,具体包括以下步骤:首先对干涉条纹图像进行二维傅立叶变换,变换后的傅立叶频域空间中,正的干涉相位和负的干涉相位成分对称于位于频域空间中央的直流成分分布;然后通过频域空间带通滤波器提取正的干涉相位的频域信息,并将该正的干涉相位的频域信息频移至频域空间的中央;最后,将平移至频域空间中央的正的干涉相位信息进行傅立叶逆变换,提取正的干涉相位信息。As a further optimization of the present invention, in step S0, it specifically includes the following steps: first, perform a two-dimensional Fourier transform on the interference fringe image, and in the transformed Fourier frequency domain space, the positive interference phase and negative interference phase components are symmetrical to The DC component distribution in the center of the frequency domain space; then, the frequency domain information of the positive interference phase is extracted through the frequency domain space bandpass filter, and the frequency domain information of the positive interference phase is frequency shifted to the center of the frequency domain space; finally, The positive interference phase information shifted to the center of the frequency domain space is subjected to inverse Fourier transform to extract the positive interference phase information.
作为本发明的进一步优化,在步骤S1中,具体包括以下步骤:首先,设定双子菲涅耳衍射平面,即对称于干涉条纹图像平面在正反两个方向分别设定正相位衍射平面以及负相位衍射平面;其次,将正的干涉相位代入欧拉公式获取干涉条纹的复数振幅,将干涉条纹的复数振幅代入二维菲涅尔数字衍射改造公式,调整菲涅尔数字衍射距离,直至获取聚焦位置,得到聚焦位置的物体光复数振幅;最后,根据欧拉公式,从物体光复数振幅获得物体光相位以及振幅分布。As a further optimization of the present invention, in step S1, it specifically includes the following steps: first, set the double Fresnel diffraction plane, that is, set the positive phase diffraction plane and the negative phase diffraction plane in the positive and negative directions symmetrically to the interference fringe image plane, respectively. Phase diffraction plane; secondly, substituting the positive interference phase into Euler's formula to obtain the complex amplitude of the interference fringes, substituting the complex amplitude of the interference fringes into the two-dimensional Fresnel digital diffraction transformation formula, and adjusting the Fresnel digital diffraction distance until the focus is obtained position, the complex amplitude of the object light at the focus position is obtained; finally, according to Euler's formula, the phase and amplitude distribution of the object light are obtained from the complex amplitude of the object light.
作为本发明的进一步优化,在步骤S0中,干涉条纹图像的数学表述公式为As a further optimization of the present invention, in step S0, the mathematical expression formula of the interference fringe image is:
C(x,y)=2AO(x,y)AR(x,y)C(x,y)=2A O (x,y)A R (x,y)
其中,A(x,y)为干涉条纹图像的灰度值,(x,y)为干涉条纹图像坐标;AR(x,y)与分别为参照光复数振幅及其共轭;AO(x,y)与分别为物体光复数振幅及其共轭;B(x,y)为干涉条纹中的直流信息;为干涉条纹中负的干涉光相位信息;为干涉条纹图像中正的干涉光相位信息;干涉条纹图像的二维傅立叶变换的数学表述公式为: A(fx,fy)=B(fx,fy)+C(fx-f0,fy-f0)+C*(fx+fo,fy+fo),Among them, A(x, y) is the gray value of the interference fringe image, (x, y) is the coordinate of the interference fringe image; A R (x, y) and are the reference light complex amplitude and its conjugate, respectively; A O (x, y) and are the complex amplitude of the object light and its conjugate, respectively; B(x, y) is the DC information in the interference fringes; is the negative interference light phase information in the interference fringes; is the positive interference light phase information in the interference fringe image; the mathematical expression formula of the two-dimensional Fourier transform of the interference fringe image is: A(f x , f y )=B(f x , f y )+C(f x -f 0 , f y -f 0 )+C * (f x + fo , f y + fo ),
其中,A(fz,fy)为干涉条纹图像的二维傅立叶变换,(fx,fy)为干涉条纹图像的二维傅立叶频域空间中心坐标,B(fx,fy)为干涉条纹图像中直流信息的二维傅立叶变换,C(fz-fo,fy-fo)为干涉条纹中正的干涉光相位信息的二维傅立叶变换, C*(fx+f0,fy+f0)为干涉条纹中负的干涉光相位信息的二维傅立叶变换,fo为正或负的干涉光相位信息二维傅立叶变换后频域坐标与二维傅立叶频域中间中心坐标的偏离。Among them, A(f z , f y ) is the two-dimensional Fourier transform of the interference fringe image, (f x , f y ) is the center coordinate of the two-dimensional Fourier frequency domain space of the interference fringe image, and B(f x , f y ) is The two-dimensional Fourier transform of the DC information in the interference fringe image, C(f z -f o , f y -f o ) is the two-dimensional Fourier transform of the phase information of the positive interference light in the interference fringe, C * (f x +f 0 , f y +f 0 ) is the two-dimensional Fourier transform of the negative interference light phase information in the interference fringes, f o is the two-dimensional Fourier-transformed frequency domain coordinates of the positive or negative interference light phase information and the two-dimensional Fourier frequency domain intermediate center coordinates deviation.
作为本发明的进一步优化,在步骤S2中,二维菲涅尔数字衍射改造公式为其中,Γ(ξ,η)为正相位衍射平面上的物体光复数振幅,E0(x,y)表示干涉条纹复数振幅; As a further optimization of the present invention, in step S2, the two-dimensional Fresnel digital diffraction transformation formula is: Among them, Γ(ξ, η) is the complex amplitude of the object light on the positive phase diffraction plane, E 0 (x, y) represents the complex amplitude of interference fringes;
作为本发明的进一步优化,在步骤S1中,二维菲涅尔数字衍射改造公式为其中,Γ(ξ′,η′)为负相位衍射平面上的物体光复数振幅,其中,B0(x,y)表示干涉条纹复数振幅; As a further optimization of the present invention, in step S1, the two-dimensional Fresnel digital diffraction transformation formula is: Among them, Γ(ξ', η') is the complex amplitude of the object light on the negative phase diffraction plane, Among them, B 0 (x, y) represents the complex amplitude of interference fringes;
作为本发明的进一步优化,在步骤S1中,所述欧拉公式为:其中,为相位,i表示复数。As a further optimization of the present invention, in step S1, the Euler formula is: in, is the phase, and i is a complex number.
作为本发明的进一步优化,在步骤S0中,所述菲涅尔数字衍射所依据的菲涅尔变换公式为:其中,Γ(ξ′,η′)为菲涅耳衍射平面上的光复数信息,分别为光强和相位;(ξ′,η′)为菲涅耳衍射平面上的平面坐标;A(x,y)为光源透过光圈平面中光圈时的光复数信息;(x,y)为光圈平面上的平面坐标;d为菲涅耳衍射平面和光圈平面之间的垂直距离;ρ‘为光圈上的一点衍射到菲涅耳衍射平面上一点时的衍射距离;λ为光源的光波长值,i表示复数。As a further optimization of the present invention, in step S0, the Fresnel transformation formula on which the Fresnel digital diffraction is based is: Among them, Γ(ξ', η') is the optical complex number information on the Fresnel diffraction plane, which are the light intensity and phase respectively; (ξ', η') are the plane coordinates on the Fresnel diffraction plane; A(x , y) is the complex number information of light when the light source passes through the aperture in the aperture plane; (x, y) is the plane coordinate on the aperture plane; d is the vertical distance between the Fresnel diffraction plane and the aperture plane; ρ' is the aperture Diffraction distance from a point on the Fresnel diffraction plane to a point on the Fresnel diffraction plane; λ is the light wavelength value of the light source, and i is a complex number.
与现有技术相比,本发明的优点和积极效果在于:本发明的数字全息三维重建方法,通过对一幅干涉条纹图像进行频域分析,快速实时地从一幅干涉条纹图像中提取三维测量所需的正的物体光相位信息,从而实现高速实时且精密稳定的单次曝光数字全息测量。Compared with the prior art, the advantages and positive effects of the present invention are as follows: the digital holographic three-dimensional reconstruction method of the present invention can extract three-dimensional measurements from an interference fringe image quickly and in real time by performing frequency domain analysis on an interference fringe image. The required positive optical phase information of the object can achieve high-speed real-time and precise and stable single-exposure digital holographic measurement.
附图说明Description of drawings
图1为本发明数字全息三维重建方法的流程图;Fig. 1 is the flow chart of the digital holographic three-dimensional reconstruction method of the present invention;
图2为本发明方法中干涉条纹图像及其二维傅立叶变换后的频域分布图;Fig. 2 is the frequency domain distribution diagram after interference fringe image and its two-dimensional Fourier transform in the method of the present invention;
图3为本发明方法中双子设定菲涅尔衍射平面图;3 is a plan view of Gemini set Fresnel diffraction in the method of the present invention;
图4为本发明方法中移动带通滤波后的频域信息到整个频域的中心的示意图;4 is a schematic diagram of moving bandpass filtered frequency domain information to the center of the entire frequency domain in the method of the present invention;
图5为本发明方法中二维傅立叶变换后的相位分布图;Fig. 5 is the phase distribution diagram after two-dimensional Fourier transform in the method of the present invention;
图6为本发明方法中二维傅立叶变换后的振幅分布图;6 is an amplitude distribution diagram after two-dimensional Fourier transform in the method of the present invention;
图7为本发明方法中调整衍射距离获得聚焦衍射成像的示意图;7 is a schematic diagram of adjusting the diffraction distance to obtain focused diffraction imaging in the method of the present invention;
图8为本发明方法中数字全息三维重建的结果示意图。FIG. 8 is a schematic diagram of the result of digital holographic three-dimensional reconstruction in the method of the present invention.
具体实施方式Detailed ways
下面,通过示例性的实施方式对本发明进行具体描述。然而应当理解,在没有进一步叙述的情况下,一个实施方式中的元件、结构和特征也可以有益地结合到其他实施方式中。Hereinafter, the present invention will be specifically described through exemplary embodiments. It should be understood, however, that elements, structures and features of one embodiment may be beneficially combined in other embodiments without further recitation.
如图1所示,本发明提供了一种数字全息三维重建方法,该数字全息三维重建方法包括以下步骤:As shown in FIG. 1, the present invention provides a digital holographic three-dimensional reconstruction method, and the digital holographic three-dimensional reconstruction method includes the following steps:
S0:对一幅干涉条纹图像进行二维傅立叶变换,以将干涉条纹图像转换为傅立叶频域;对傅立叶频域分析处理后进行二维傅立叶逆变换,以形成图像域;并提取正的干涉相位信息;S0: Perform a two-dimensional Fourier transform on an interference fringe image to convert the interference fringe image into the Fourier frequency domain; perform two-dimensional inverse Fourier transform after analyzing and processing the Fourier frequency domain to form the image domain; and extract the positive interference phase information;
S1:判断相位衍射平面到干涉条纹图像平面的距离是否为0,如是,则将执行S3;如否,则执行S2;S1: Determine whether the distance from the phase diffraction plane to the interference fringe image plane is 0, if so, execute S3; if not, execute S2;
S2:对提取的正的干涉相位信息进行菲涅尔数字衍射计算,提取正的物体光相位信息,并调整菲涅尔数字衍射距离为聚焦位置,以获取聚焦位置的相位;具体如图7所示,该图中最下方成像即为聚焦位置的相位信息;S2: Perform the Fresnel digital diffraction calculation on the extracted positive interference phase information, extract the positive optical phase information of the object, and adjust the Fresnel digital diffraction distance as the focus position to obtain the phase at the focus position; as shown in Figure 7 The bottom image in the figure is the phase information of the focus position;
S3:将提取的正的信息代入干涉测量法公式计算,获取物体的立体高度信息,以进行数字全息三维的重建。S3: Substitute the extracted positive information into the interferometry formula for calculation, and obtain the stereoscopic height information of the object, so as to carry out digital holographic three-dimensional reconstruction.
进一步,在步骤S0中,具体包括以下步骤:首先对干涉条纹图像进行二维傅立叶变换,变换后的傅立叶频域空间中,正的干涉相位和负的干涉相位成分对称于位于频域空间中央的直流成分分布;然后通过频域空间带通滤波器提取正的干涉相位的频域信息,并将该正的干涉相位的频域信息频移至频域空间的中央;最后,将平移至频域空间中央的正的干涉相位信息进行傅立叶逆变换,提取正的干涉相位信息。Further, in step S0, it specifically includes the following steps: first, perform a two-dimensional Fourier transform on the interference fringe image, and in the transformed Fourier frequency domain space, the positive interference phase and negative interference phase components are symmetrical to the center of the frequency domain space. Then, the frequency domain information of the positive interference phase is extracted by the frequency domain space bandpass filter, and the frequency domain information of the positive interference phase is frequency shifted to the center of the frequency domain space; finally, the frequency domain information is shifted to the frequency domain. The positive interference phase information in the center of the space is subjected to inverse Fourier transform to extract the positive interference phase information.
如图3中所示,二维傅立叶变换后的傅立叶频域空间中,正中心的频域值为干涉条纹的直流成分,左下角的值域为干涉条纹中正的物体光相位成分,右上角的值域为干涉条纹中负的物体光相位成分。通过二维频域带通滤波器可对左下角正的相位成分进行提取而直接滤除直流成分和负的相位成分。具体如图4 所示,带通滤波后的频域信息需要通过二维傅立叶逆变换才能够得到时域中的物体光复变函数,但是带通滤波后的频域信息中已经丢失直流和负的相位信息,需要将带通滤波后的频域成分移动到频域中心,以弥补丢失的直流和负相位成分。As shown in Figure 3, in the Fourier frequency domain space after the two-dimensional Fourier transform, the frequency domain value in the center is the DC component of the interference fringes, the value range in the lower left corner is the positive object light phase component in the interference fringes, and the value in the upper right corner is the positive light phase component of the object in the interference fringes. The value range is the negative object light phase component in the interference fringes. The positive phase component in the lower left corner can be extracted by the two-dimensional frequency domain bandpass filter, and the DC component and the negative phase component can be directly filtered out. Specifically, as shown in Figure 4, the frequency domain information after bandpass filtering needs to pass two-dimensional inverse Fourier transform to obtain the complex optical function of the object in the time domain, but the frequency domain information after bandpass filtering has lost DC and negative. Phase information requires moving the bandpass filtered frequency domain components to the center of the frequency domain to compensate for the missing DC and negative phase components.
继续如图5和图6所示,将图4中右边所示的频域进行二维傅立叶逆变换,能够取得干涉条纹的复变函数,也即式1中的A(x,y),根据欧拉公式可得相位及振幅分布。Continuing as shown in Figure 5 and Figure 6, the two-dimensional inverse Fourier transform of the frequency domain shown on the right in Figure 4 can be used to obtain the complex function of the interference fringes, that is, A(x, y) in Equation 1, according to Euler's formula can get the phase and amplitude distribution.
另外,上述中,在步骤S0中,干涉条纹图像的数学表述公式为In addition, in the above, in step S0, the mathematical expression formula of the interference fringe image is:
C(x,y)=2AO(x,y)AR(x,y)C(x,y)=2A O (x,y)A R (x,y)
其中,A(x,y)为干涉条纹图像的灰度值,(x,y)为干涉条纹图像坐标;AR(x,y)与分别为参照光复数振幅及其共轭;AO(x,y)与分别为物体光复数振幅及其共轭;B(x,y)为干涉条纹中的直流信息;为干涉条纹中负的干涉光相位信息;为干涉条纹图像中正的干涉光相位信息;干涉条纹图像的二维傅立叶变换的数学表述公式为: A(fx,fy)=B(fx,fy)+C(fx-f0,fy-f0)+C*(fx+f0,fy+f0),Among them, A(x, y) is the gray value of the interference fringe image, (x, y) is the coordinate of the interference fringe image; A R (x, y) and are the reference light complex amplitude and its conjugate, respectively; A O (x, y) and are the complex amplitude of the object light and its conjugate, respectively; B(x, y) is the DC information in the interference fringes; is the negative interference light phase information in the interference fringes; is the positive interference light phase information in the interference fringe image; the mathematical expression formula of the two-dimensional Fourier transform of the interference fringe image is: A(f x , f y )=B(f x , f y )+C(f x -f 0 , f y -f 0 )+C * (f x +f 0 , f y +f 0 ),
其中,A(fx,fy)为干涉条纹图像的二维傅立叶变换,(fx,fy)为干涉条纹图像的二维傅立叶频域空间中心坐标,B(fx,fy)为干涉条纹图像中直流信息的二维傅立叶变换,C(fx-fo,fy-fo)为干涉条纹中正的干涉光相位信息的二维傅立叶变换, C*(fx+f0,fy+f0)为干涉条纹中负的干涉光相位信息的二维傅立叶变换,f0为正或负的干涉光相位信息二维傅立叶变换后频域坐标与二维傅立叶频域中间中心坐标的偏离。Among them, A(f x , f y ) is the two-dimensional Fourier transform of the interference fringe image, (f x , f y ) is the center coordinate of the two-dimensional Fourier frequency domain space of the interference fringe image, and B(f x , f y ) is The two-dimensional Fourier transform of the DC information in the interference fringe image, C(f x -f o , f y -f o ) is the two-dimensional Fourier transform of the phase information of the positive interference light in the interference fringe, C * (f x +f 0 , f y +f 0 ) is the two-dimensional Fourier transform of the negative interference light phase information in the interference fringes, f 0 is the two-dimensional Fourier-transformed frequency domain coordinates of the positive or negative interference light phase information and the two-dimensional Fourier frequency domain intermediate center coordinates deviation.
而在步骤S0中,所述菲涅尔数字衍射所依据的菲涅尔变换公式为:其中,Γ(ξ′,η′)为菲涅耳衍射平面上的光复数信息,分别为光强和相位;(ξ′,η′)为菲涅耳衍射平面上的平面坐标;A(x,y)为光源透过光圈平面中光圈时的光复数信息;(x,y)为光圈平面上的平面坐标;d为菲涅耳衍射平面和光圈平面之间的垂直距离;A为光圈上的一点衍射到菲涅耳衍射平面上一点时的衍射距离;λ为光源的光波长值,i表示复数。In step S0, the Fresnel transformation formula on which the Fresnel digital diffraction is based is: Among them, Γ(ξ', η') is the optical complex number information on the Fresnel diffraction plane, which are the light intensity and phase respectively; (ξ', η') are the plane coordinates on the Fresnel diffraction plane; A(x , y) is the complex number information of light when the light source passes through the aperture in the aperture plane; (x, y) is the plane coordinate on the aperture plane; d is the vertical distance between the Fresnel diffraction plane and the aperture plane; A is the aperture on the aperture Diffraction distance when a point is diffracted to a point on the Fresnel diffraction plane; λ is the light wavelength value of the light source, and i is a complex number.
继续如图2所示,在步骤S1中,具体包括以下步骤:首先,设定双子菲涅耳衍射平面,即对称于干涉条纹图像平面1在正反两个方向分别设定正相位衍射平面2以及负相位衍射平面3,则正相位衍射平面2与干涉条纹图像平面1之间的距离即为正的衍射距离4,而负相位衍射平面3与干涉条纹图像平面1之间的距离即为负的衍射距离5;其次,将正的干涉相位代入欧拉公式获取干涉条纹的复数振幅,将干涉条纹的复数振幅代入二维菲涅尔数字衍射改造公式,调整菲涅尔数字衍射距离,直至获取聚焦位置,得到聚焦位置的物体光复数振幅;最后,根据欧拉公式,从物体光复数振幅获得物体光相位以及振幅分布。Continue as shown in FIG. 2 , in step S1 , the following steps are specifically included: First, set the double Fresnel diffraction plane, that is, set the positive phase diffraction plane 2 in the positive and negative directions symmetrical to the interference fringe image plane 1 respectively and the negative phase diffraction plane 3, the distance between the positive phase diffraction plane 2 and the interference fringe image plane 1 is the positive diffraction distance 4, and the distance between the negative phase diffraction plane 3 and the interference fringe image plane 1 is the negative Second, the positive interference phase is substituted into Euler's formula to obtain the complex amplitude of the interference fringes, and the complex amplitude of the interference fringes is substituted into the two-dimensional Fresnel digital diffraction transformation formula, and the Fresnel digital diffraction distance is adjusted until obtaining Focusing position, the object light complex amplitude at the focus position is obtained; finally, according to Euler's formula, the object light phase and amplitude distribution are obtained from the object light complex amplitude.
上述中,在步骤S1中,二维菲涅尔数字衍射改造公式为其中,Γ(ξ′,η′)为负相位衍射平面上的物体光复数振幅,其中,E0(x,y)表示干涉条纹复数振幅;同时,上述在步骤S1中,所述欧拉公式为:其中,为相位,i表示复数。In the above, in step S1, the two-dimensional Fresnel digital diffraction transformation formula is Among them, Γ(ξ', η') is the complex amplitude of the object light on the negative phase diffraction plane, Among them, E 0 (x, y) represents the complex amplitude of interference fringes; Meanwhile, in the above step S1, the Euler formula is: in, is the phase, and i is a complex number.
而在步骤S2中,二维菲涅尔数字衍射改造公式为其中,Γ(ξ,η)为正相位衍射平面上的物体光复数振幅,E0(x,y)表示干涉条纹复数振幅; In step S2, the two-dimensional Fresnel digital diffraction transformation formula is Among them, Γ(ξ, η) is the complex amplitude of the object light on the positive phase diffraction plane, E 0 (x, y) represents the complex amplitude of interference fringes;
通过上述数字全息三维重建方法,其重建结果如图8所示,本发明通过二维傅立叶变换的方法,对一幅干涉条纹图像进行频域分析,快速实时地从一幅干涉条纹图像中提取三维测量所需的正的物体光相位信息,从而实现了高速实时且精密稳定的单次曝光数字全息测量。同时,本发明的数字全息三维重建方法,不需要如现有技术中拍摄多幅相移干涉条纹图像,减少了拍摄耗费的时间,也不会受到震动、空气对流等环境因素影响,从而实现快速实时的数字全息三维测量,应用场合更广泛,降低了成本。Through the above-mentioned digital holographic three-dimensional reconstruction method, the reconstruction result is shown in Figure 8. The present invention analyzes an interference fringe image in the frequency domain by means of a two-dimensional Fourier transform, and extracts three-dimensional images from an interference fringe image in a fast and real-time manner. The required positive optical phase information of the object is measured, thereby realizing high-speed real-time, precise and stable single-exposure digital holographic measurement. At the same time, the digital holographic three-dimensional reconstruction method of the present invention does not need to shoot multiple phase-shifted interference fringe images as in the prior art, which reduces the time spent on shooting, and is not affected by environmental factors such as vibration and air convection, thereby achieving rapid Real-time digital holographic 3D measurement has wider applications and lower costs.
以上所述,仅为本发明的具体实施方式,但本发明的保护范围并不局限于此,任何熟悉本技术领域的技术人员在本发明揭露的技术范围内,可轻易想到变化或替换,都应涵盖在本发明的保护范围之内。因此,本发明的保护范围应以所述权利要求的保护范围为准。The above are only specific embodiments of the present invention, but the protection scope of the present invention is not limited thereto. Any person skilled in the art can easily think of changes or substitutions within the technical scope disclosed by the present invention. should be included within the protection scope of the present invention. Therefore, the protection scope of the present invention should be based on the protection scope of the claims.
Claims (8)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201711240115.8A CN109855558B (en) | 2017-11-30 | 2017-11-30 | Three-dimensional reconstruction method of digital holography |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201711240115.8A CN109855558B (en) | 2017-11-30 | 2017-11-30 | Three-dimensional reconstruction method of digital holography |
Publications (2)
Publication Number | Publication Date |
---|---|
CN109855558A true CN109855558A (en) | 2019-06-07 |
CN109855558B CN109855558B (en) | 2020-09-25 |
Family
ID=66888345
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201711240115.8A Active CN109855558B (en) | 2017-11-30 | 2017-11-30 | Three-dimensional reconstruction method of digital holography |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN109855558B (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN117075739A (en) * | 2023-10-13 | 2023-11-17 | 深圳优立全息科技有限公司 | Holographic sand table-based holographic display method and related device |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20030204325A1 (en) * | 2001-12-04 | 2003-10-30 | Xinhui Niu | Optical profilometry of additional-material deviations in a periodic grating |
CN101681145A (en) * | 2007-05-21 | 2010-03-24 | 视瑞尔技术公司 | Holographic reconstruction system with tracking of the reconstruction |
CN103630086A (en) * | 2013-11-13 | 2014-03-12 | 华南师范大学 | Dual-wavelength simultaneous phase-shift interferometry method based on monochromatic CCD (couple charged device) |
CN105892257A (en) * | 2014-12-10 | 2016-08-24 | 青岛理工大学 | Method and device for recording hologram by sine structured light |
CN106338823A (en) * | 2016-10-27 | 2017-01-18 | 中国科学院光电技术研究所 | Phase inversion method based on mixed focal length Fresnel zone plate |
-
2017
- 2017-11-30 CN CN201711240115.8A patent/CN109855558B/en active Active
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20030204325A1 (en) * | 2001-12-04 | 2003-10-30 | Xinhui Niu | Optical profilometry of additional-material deviations in a periodic grating |
CN101681145A (en) * | 2007-05-21 | 2010-03-24 | 视瑞尔技术公司 | Holographic reconstruction system with tracking of the reconstruction |
CN103630086A (en) * | 2013-11-13 | 2014-03-12 | 华南师范大学 | Dual-wavelength simultaneous phase-shift interferometry method based on monochromatic CCD (couple charged device) |
CN105892257A (en) * | 2014-12-10 | 2016-08-24 | 青岛理工大学 | Method and device for recording hologram by sine structured light |
CN106338823A (en) * | 2016-10-27 | 2017-01-18 | 中国科学院光电技术研究所 | Phase inversion method based on mixed focal length Fresnel zone plate |
Non-Patent Citations (3)
Title |
---|
CHANGHAI LIU: "Modal wavefrontsensoremployingstratified computer-generated holographicelements", 《OPTICSANDLASERSINENGINEERING》 * |
沈川等: "可编程菲涅耳相位透镜应用于多平面全息投影", 《光子学报》 * |
裴闯: "一种三维物体相息图的迭代计算方法", 《光子学报》 * |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN117075739A (en) * | 2023-10-13 | 2023-11-17 | 深圳优立全息科技有限公司 | Holographic sand table-based holographic display method and related device |
CN117075739B (en) * | 2023-10-13 | 2024-01-23 | 深圳优立全息科技有限公司 | Holographic sand table-based holographic display method and related device |
Also Published As
Publication number | Publication date |
---|---|
CN109855558B (en) | 2020-09-25 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
JP5467321B2 (en) | 3D shape measuring method and 3D shape measuring apparatus | |
US9322643B2 (en) | Apparatus and method for 3D surface measurement | |
Karpinsky et al. | High-resolution, real-time 3D imaging with fringe analysis | |
JP5818341B2 (en) | Shape measuring apparatus and shape measuring method | |
CN112697751B (en) | Multi-angle illumination lensless imaging method, system and device | |
CN106054570B (en) | Intensity transmission equation realizes the larger Phase Build Out method of single digital hologram | |
CN104407507A (en) | Hilbert transform based high-precision digital holography phase reconstruction method | |
CN111238403A (en) | Three-dimensional reconstruction method and device based on light field sub-aperture stripe image | |
CN112085793B (en) | A three-dimensional imaging scanning system and point cloud registration method based on combined lens group | |
CN105066906A (en) | Fast high dynamic range three-dimensional measurement method | |
CN103712569B (en) | Based on single image fast phase shift system and the method for detecting phases of deflection angle | |
CN105404128B (en) | Multiframe phase-shifted digital holographic method and device | |
CN103941569A (en) | Method for LED multi-angle holographic three-dimensional data representation | |
CN106557004A (en) | A kind of holographic projection methods and device | |
CN103323938A (en) | Method for acquiring stereo microscopic image | |
KR20150081010A (en) | Apparatus and method for measurement and evaluation of field of view of reconstructed image of hologram | |
CN107144233A (en) | The three dimensional shape measurement system that a kind of projected grating phase is combined with digital hologram | |
JP6867645B2 (en) | Image processing equipment, methods, and programs | |
CN101957171B (en) | A coaxial digital holography method that can effectively suppress zero-order and conjugate images | |
CN109855558B (en) | Three-dimensional reconstruction method of digital holography | |
KR20170079441A (en) | Device and method for recording and reconstructing digital hologram of high step sample with vibrant environment | |
JP2012145361A (en) | Digital holography device | |
CN108254917A (en) | An edge-enhanced imaging device and method based on fractional photon orbital angular momentum | |
CN108182727B (en) | Phase Unwrapping Method Based on Multi-View Geometric Consistency | |
JP6040469B2 (en) | Digital holography device |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant | ||
TR01 | Transfer of patent right |
Effective date of registration: 20250325 Address after: Room 613, 6th Floor, Building 14, No. 9 Linhe South Street, Renhe Town, Shunyi District, Beijing 101300 Patentee after: Beijing Yinuo Heju Digital Technology Co.,Ltd. Country or region after: China Address before: No. 48 Xianxialing Road, Qingdao City, Shandong Province, 266000 Patentee before: QINGDAO QUANWEI MEDICAL TECHNOLOGY CO.,LTD. Country or region before: China |
|
TR01 | Transfer of patent right |