CN104155658A - Image reconstruction method of laser radar imaging system based on compressed sensing - Google Patents
Image reconstruction method of laser radar imaging system based on compressed sensing Download PDFInfo
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Abstract
本发明公开了一种基于压缩感知的激光雷达成像系统的图像重构方法。本方法的激光雷达成像系统采用单元雪崩二极管APD,有效的突破了目前国产线阵雪崩二极管无法大规模集成的瓶颈问题。系统由激光发射模块,望远镜成像模块,数字微反射镜DMD及控制模块,雪崩二极管APD,同步模块,数据采集模块,图像重构模块组成。该发明通过激光发射模块向目标发射脉冲激光,不同距离目标反射回波被数字微反射镜DMD调制,再经过汇聚镜头给单元雪崩二极管APD实现在时间序列上的采样,最后采用后续的图像重构方法重构出目标的三维像。本发明的优点是:无需任何扫描,结构简单,图像重构所需的数据量小,探测灵敏度高。
The invention discloses an image reconstruction method of a lidar imaging system based on compressed sensing. The laser radar imaging system of this method adopts the unit avalanche diode APD, which effectively breaks through the bottleneck problem that the current domestic linear array avalanche diode cannot be integrated on a large scale. The system consists of a laser emitting module, a telescope imaging module, a digital micromirror DMD and a control module, an avalanche diode APD, a synchronization module, a data acquisition module, and an image reconstruction module. The invention emits pulsed lasers to the target through the laser emitting module, and the reflected echoes of targets at different distances are modulated by the digital micro-mirror DMD, and then the unit avalanche diode APD is sampled in time series through the converging lens, and finally the subsequent image reconstruction is adopted The method reconstructs the 3D image of the target. The invention has the advantages of no need for any scanning, simple structure, small amount of data required for image reconstruction, and high detection sensitivity.
Description
技术领域technical field
本发明涉及计算成像技术以及图像重构算法,信号处理、激光雷达。特别涉及一种基于压缩感知的激光雷达成像系统的图像重构方法。The invention relates to computational imaging technology and image reconstruction algorithm, signal processing and laser radar. In particular, it relates to an image reconstruction method of a lidar imaging system based on compressed sensing.
背景技术Background technique
激光雷达是一种主动光电成像技术,与普通的被动光学遥感探测和微波雷达相比具有分辨率高,隐蔽性好,极强的抗干扰能力等;能穿过云雾,植被等探测到真实的地面地形。激光雷达通过向目标发射脉冲激光信号,然后将接收到从目标反射回来的信号(回波信号)与发射信号进行相关的数据处理,从而就可以提取目标的相关信息,比如目标距离,方位,姿态,形状等参数。利用这种激光雷达,在军事上就可以对敌方的飞机,导弹等进行跟踪、探测识别,从而实现精确打击。目前它已经成为我国军事领域中一种不可或缺的技术手段。Lidar is an active photoelectric imaging technology. Compared with ordinary passive optical remote sensing detection and microwave radar, it has high resolution, good concealment, strong anti-interference ability, etc.; it can detect real objects through clouds, vegetation, etc. ground terrain. LiDAR transmits pulsed laser signals to the target, and then processes the received signal (echo signal) reflected from the target and the transmitted signal, so that relevant information of the target can be extracted, such as target distance, orientation, and attitude. , shape and other parameters. Using this kind of laser radar, in the military, it is possible to track, detect and identify enemy aircraft and missiles, so as to achieve precise strikes. At present, it has become an indispensable technical means in the military field of our country.
传统的激光雷达按工作方式可以分为逐点扫描的摆扫式和线阵推扫式。摆扫式激光雷达在技术上已经非常成熟,它最大的优点是原理非常简单。但它也存在很大的缺点,比如难以捕获高速移动的目标;由于存在机械扫描装置,很难做到小型化和轻型化;大量点云数据将对数据采集系统的数据传输与存储以及后续处理带来极大的压力;另外逐点扫描的原理,已及飞行速度和扫描速度的限制将导致距离图像的空间分辨率较低。线阵推扫式激光雷达采用同时发射多束激光和多个探测器的并行探测原理,从而提高覆盖效率和扫描效率,克服逐点扫描式激光雷达的一些缺点。目前,我国推扫式激光雷达的研究才处于起步阶段。而线阵的雪崩二极管APD探测器很难做到大规模集成,就目前的技术手段而言,只能做到25-50单元的APD,线阵APD的工艺瓶颈问题将在很大程度上阻碍推扫式激光雷达的发展。Traditional laser radar can be divided into point-by-point scanning swing-broom type and linear array push-broom type according to the working mode. The swing-sweep lidar is very mature in technology, and its biggest advantage is that the principle is very simple. But it also has great shortcomings, such as it is difficult to capture high-speed moving targets; due to the existence of mechanical scanning devices, it is difficult to achieve miniaturization and light weight; a large amount of point cloud data will affect the data transmission and storage of the data acquisition system and subsequent processing Bring great pressure; in addition, the principle of point-by-point scanning, and the limitation of flight speed and scanning speed will lead to low spatial resolution of distance images. Linear array push-broom lidar adopts the parallel detection principle of emitting multiple laser beams and multiple detectors at the same time, thereby improving coverage efficiency and scanning efficiency, and overcoming some shortcomings of point-by-point scanning lidar. At present, the research on push-broom lidar in my country is just in its infancy. However, it is difficult to achieve large-scale integration of linear array avalanche diode APD detectors. As far as the current technical means are concerned, only 25-50 units of APDs can be achieved. The process bottleneck of linear array APDs will largely hinder Development of pushbroom lidar.
压缩感知(Compressive Sensing,CS)是由美国斯坦福大学数学家Donoho和Candes等人(参见文献1、2、3)在2006年提出的一种采样与压缩同步进行的理论。该理论通过挖掘信号信息的冗余性和稀疏性,在采样过程中,不是获取图像的全部像素采样,而是通过特定的算法,选择合适的调制模板,即:观测矩阵,每次对信号进行全局采样,然后通过这些采样结合相关的恢复算法复原图像。与传统的“先采样、后压缩”不同,CS理论是“边采样、边压缩”的方式,将CS应用于激光雷达成像系统可以显著节省传感器数量,这种“边采样、边压缩”的方式使得信号处理的技术负担从传感器转移到数据处理上来。因此,基于压缩感知理论,发展新型的激光雷达成像系统自然的成为本发明所要研究的内容。Compressive sensing (Compressive Sensing, CS) is a theory that sampling and compression are performed simultaneously by Donoho and Candes, a mathematician at Stanford University in the United States (see documents 1, 2, 3) in 2006. This theory excavates the redundancy and sparsity of signal information. In the sampling process, instead of obtaining all pixel samples of the image, it selects the appropriate modulation template through a specific algorithm, that is, the observation matrix. Global samples are then used to restore the image through these samples combined with related restoration algorithms. Different from the traditional "sampling first, then compression", the CS theory is a "sampling while compression" method. Applying CS to the lidar imaging system can significantly save the number of sensors. This "sampling while compression" method The technical burden of signal processing is transferred from the sensor to the data processing. Therefore, based on the compressed sensing theory, the development of a new type of laser radar imaging system naturally becomes the research content of the present invention.
参考文献:references:
[1]Donoho D L.Compressed sensing[J].IEEE Transactions on InformationTheory,2006,52(4):1289-1306.[1] Donoho D L. Compressed sensing [J]. IEEE Transactions on Information Theory, 2006, 52(4): 1289-1306.
[2]Candès E,Romberg J,Tao T.Robust uncertainty principles:exact signalreconstruction from highly incomplete frequency information[J].IEEETransactions on Information Theory,2006,52(2):489-509.[2] Candès E, Romberg J, Tao T. Robust uncertainty principles: exact signal reconstruction from highly incomplete frequency information [J]. IEEE Transactions on Information Theory, 2006, 52(2): 489-509.
[3]Candès E.Compressive sampling[C].International Congress ofMathematics,2006:1433-1452.[3] Candès E. Compressive sampling [C]. International Congress of Mathematics, 2006: 1433-1452.
发明内容Contents of the invention
本发明的目的是提供一种基于压缩感知的激光雷达成像系统的图像重构方法。在探测器方面,采用单元雪崩二极管APD探测器,克服传统逐点扫描式激光雷达的缺点和避开线阵APD技术工艺的瓶颈问题。在数据获取方面,基于压缩感知理论,采用少量的数据即可重构得到目标的三维图像,在采样的过程中就以经压缩了数据,缓解传统激光雷达成像中大数据量的采集、传输、存储压力。The purpose of the present invention is to provide an image reconstruction method based on a compressive sensing lidar imaging system. In terms of detectors, the unit avalanche diode APD detector is used to overcome the shortcomings of the traditional point-by-point scanning lidar and avoid the bottleneck of the linear array APD technology. In terms of data acquisition, based on the theory of compressed sensing, a small amount of data can be used to reconstruct the 3D image of the target, and the data is compressed during the sampling process, which eases the collection, transmission, and processing of large amounts of data in traditional lidar imaging. Storage pressure.
本发明提出的解决思路如下:The solution proposed by the present invention is as follows:
如图1所示,该新型激光雷达成像系统包括:激光发射模块1;望远镜成像模块2;数字微反射镜DMD及控制模块3;光学汇聚透镜4;雪崩二极管APD5;数据采集模块6;图像重构模块7;同步模块8。其特征在于:激光发射模块1采用波长1064nm的脉冲式激光器,其重复频率100Hz,脉冲能量200mJ;望远镜成像模块2采用焦距为304.8mm,口径为101.6mm的望远镜;数字微反射镜DMD及控制模块3中的数字微反射镜DMD采用1024×768像素,像素大小为13.69μm的DMD;光学汇聚透镜4的焦距为10cm;雪崩二极管APD5的像元尺寸1.5mm,暗电流7nA,上升时间5ns;数据采集模块6采用的采集卡量化位数为10位,采样率5GSPS;同步模块8采用FPGA芯片产生三路同步信号;As shown in Figure 1, the new lidar imaging system includes: laser emission module 1; telescope imaging module 2; digital micro-mirror DMD and control module 3; optical convergence lens 4; avalanche diode APD5; data acquisition module 6; Construction module 7; Synchronization module 8. It is characterized in that: the laser emission module 1 adopts a pulsed laser with a wavelength of 1064nm, its repetition frequency is 100Hz, and the pulse energy is 200mJ; the telescope imaging module 2 adopts a telescope with a focal length of 304.8mm and an aperture of 101.6mm; the digital microreflector DMD and the control module The digital micromirror DMD in 3 adopts a DMD with 1024×768 pixels and a pixel size of 13.69 μm; the focal length of the optical converging lens 4 is 10 cm; the pixel size of the avalanche diode APD5 is 1.5 mm, the dark current is 7 nA, and the rise time is 5 ns; the data The acquisition card quantization digit that acquisition module 6 adopts is 10, and sampling rate is 5GSPS; Synchronization module 8 adopts FPGA chip to generate three synchronous signals;
系统各模块之间的工作流程如下:The workflow between the various modules of the system is as follows:
同步模块8发射同步信号给激光发射模块1和数字微反射镜DMD及控制模块3,激光发射模块1收到同步信号后,开始向场景目标发射脉冲激光,设定场景目标有k个,被目标反射的回波信号依次记为:x1,x2...xk;The synchronization module 8 transmits a synchronization signal to the laser emission module 1 and the digital micro-mirror DMD and the control module 3. After the laser emission module 1 receives the synchronization signal, it starts to emit pulsed laser light to the scene target. The reflected echo signals are sequentially recorded as: x 1 , x 2 ... x k ;
数字微反射镜DMD及控制模块3同时也收到同步信号,然后加载一个调制模板,发送给DMD,调制模板的总数设定为M个。第M次调制时的调制模板记为:θM,具体取值为一个事先设定好的m×n阶矩阵,矩阵元素的取值为0或者1,所有的元素服从高斯随机分布。通过调制模板改变DMD微镜的翻转状态,从而达到调制目标回波的作用。实际上θM就是压缩感知理论中的观测矩阵,M的取值范围为为信号x1的稀疏度;The digital micromirror DMD and the control module 3 also receive the synchronization signal at the same time, then load a modulation template and send it to the DMD, and the total number of modulation templates is set to M. The modulation template during the Mth modulation is recorded as: θ M , the specific value is a pre-set m×n order matrix, the value of the matrix elements is 0 or 1, and all elements obey the Gaussian random distribution. Change the flip state of the DMD micromirror by modulating the template, so as to achieve the effect of modulating the target echo. In fact, θ M is the observation matrix in compressed sensing theory, and the value range of M is is the sparsity of signal x 1 ;
经过DMD调制后的回波信号被光学汇聚透镜4汇聚到雪崩二极管APD5上。在DMD的每一次调制过程中,不同距离的目标回波信号到达APD上的时间不同,将时间依次记为:因此最终在APD探测器上探测到的信号会依次出现多个峰值,如图2所示,每一个峰值对应一个目标;The echo signal modulated by the DMD is converged by the optical converging lens 4 to the avalanche diode APD5. In each modulation process of DMD, the target echo signals at different distances arrive at the APD at different times, and the time is recorded as: Therefore, the signal detected on the APD detector will eventually have multiple peaks in sequence, as shown in Figure 2, each peak corresponds to a target;
雪崩二极管APD5探测到的信号经过数据采集模块6采集后,在时间序列上,依次得到对应的M组数字信号值: After the signal detected by the avalanche diode APD5 is collected by the data acquisition module 6, in the time series , get the corresponding M sets of digital signal values in turn:
图像重构模块7对数据采集模块6采集到的信号进行处理,最终得到每个目标的三维像;The image reconstruction module 7 processes the signal collected by the data acquisition module 6, and finally obtains a three-dimensional image of each target;
图像重构模块7的具体实现步骤如下:The specific implementation steps of the image reconstruction module 7 are as follows:
1)对于第一个目标,数据采集模块6采集到信号写成如下(1)式:1) For the first target, the signal collected by the data acquisition module 6 is written as the following formula (1):
将(1)式改写为如下(2)式的矩阵方程:Rewrite formula (1) as the following matrix equation of formula (2):
F1=Θ·X1 (2)F 1 =Θ·X 1 (2)
上式中,F1是信号构成的M×1矩阵;Θ为M×N矩阵,行数M即为调制模板个数,列数N=m×n为每个调制模板θM的元数总个数,Θ的每一行即由对应的调制模板θM重新排列而成;X1为N×1矩阵;基于压缩感知理论,M的取值远远小于N。因此,(2)式实际上是一个病态方程。直接求解很明显有无穷多个解。但压缩感知理论指出,只要X1是稀疏的,或者在某种正交变换的表示下具有稀疏性,那么求解(2)式将会有特殊的优化求解方法。稀疏性的意思是指其中包含大量的趋于零的数据,只有少量的非零值;In the above formula, F 1 is the signal The formed M×1 matrix; Θ is an M×N matrix, the number of rows M is the number of modulation templates, the number of columns N=m×n is the total number of elements of each modulation template θ M , and each row of Θ is It is rearranged by the corresponding modulation template θ M ; X 1 is an N×1 matrix; based on the theory of compressed sensing, the value of M is much smaller than N. Therefore, (2) is actually an ill-conditioned equation. Direct Solving Clearly there are infinitely many solutions. However, the theory of compressed sensing points out that as long as X 1 is sparse, or has sparseness under the representation of some kind of orthogonal transformation, then there will be a special optimization method for solving equation (2). Sparsity means that it contains a large number of data tending to zero, and only a small number of non-zero values;
对于自然场景目标,一般情况下,可以在一些正交变换的表示下具有稀疏性。例如:傅里叶变换,离散余弦变换等。对于X1,在离散余弦变换下,将其稀疏表示为如下(3)式:For natural scene objects, in general, it is possible to have sparsity under the representation of some orthogonal transformations. For example: Fourier transform, discrete cosine transform, etc. For X 1 , under the discrete cosine transform, it is sparsely expressed as the following formula (3):
X1=Ψ·α1 (3)X 1 =Ψ·α 1 (3)
上式中,α1为X1的稀疏表示,它是一个N×1矩阵;Ψ是N×N阶离散余弦变换矩阵;In the above formula, α 1 is the sparse representation of X 1 , which is an N×1 matrix; Ψ is the N×N order discrete cosine transform matrix;
于是将(2)式重新写为如下(4)式:So the formula (2) is rewritten as the following formula (4):
F1=Θ·X1=Θ·Ψ·α1=T·α1 (4)F 1 =Θ·X 1 =Θ·Ψ·α 1 =T·α 1 (4)
上式中,T为M×N阶的传感矩阵;其中只有α1为未知数;In the above formula, T is the sensing matrix of order M×N; among them, only α 1 is unknown;
图像重构的方法就是求解(4)式中的稀疏系数α1。很明显(4)式实际上是一个病态方程。直接求解有无穷多个解,因此将其转化为如下式(5)的优化问题:The method of image reconstruction is to solve the sparse coefficient α 1 in formula (4). Obviously (4) is actually an ill-conditioned equation. There are infinitely many solutions to the direct solution, so it is transformed into an optimization problem of the following formula (5):
上式中,L1表示1范数,为α1的最优近似解;In the above formula, L 1 represents the 1 norm, is the optimal approximate solution of α 1 ;
(5)式的优化求解算法步骤如下:The optimal solution algorithm steps of formula (5) are as follows:
第一步:初始化一个空矩阵I=[],残差矩阵R=F;Step 1: Initialize an empty matrix I=[], residual matrix R=F;
第二歩:将残差R与T中的每一列分别做内积,并找到内积最大的那一列,将本列取出并添加到矩阵I中;The second step: make the inner product of each column in the residual R and T respectively, and find the column with the largest inner product, take this column out and add it to the matrix I;
第三歩:更新残差,R=F-I·(IT·I)-1·IT·F,其中IT为I的转置矩阵(IT·I)-1为(IT·I)的逆矩阵;The third step: update the residual, R=FI · ( IT · I) -1 · IT · F, wherein IT is the transposition matrix of I ( IT · I) -1 is ( IT · I) the inverse matrix;
第四步:不断顺序循环第二歩和第三步,循环次数为C,它的取值范围为:C≥2M;The 4th step: continuously cycle the second step and the third step in sequence, the number of cycles is C, and its value range is: C≥2M;
第五步:最终(5)式求得的解为如下(6)式:The fifth step: the solution obtained by the final (5) formula is the following (6) formula:
最终求得的第一个目标的图像信息表示为如下(7)式:The finally obtained image information of the first target is expressed as the following formula (7):
将(7)式中的N×1阶矩阵X1重新排列成m×n阶矩阵即可得到目标的二维像;The two-dimensional image of the target can be obtained by rearranging the N × 1 order matrix X 1 in (7) into an m × n order matrix;
2)对于第二个目标,将步骤1)中的(1)式改写为如下(8)式:2) For the second goal, the formula (1) in step 1) is rewritten as the following formula (8):
将(8)式写为如下(9)式的矩阵方程:Write formula (8) as the matrix equation of formula (9):
F2=Θ·X2 (9)F 2 =Θ·X 2 (9)
求解(9)式的方法同步骤1),因此最终求得第二个目标的图像信息表示为如下(10)式:The method of solving formula (9) is the same as step 1), so the image information of the second target is finally obtained as the following formula (10):
3)依次类推,对于第k个目标,将步骤1)中的(1)式改写为如下(11)式:3) By analogy, for the kth target, the formula (1) in step 1) is rewritten as the following formula (11):
将(11)式写为如下(12)式的矩阵方程:Write formula (11) as the matrix equation of formula (12):
Fk=Θ·Xk (12)F k =Θ·X k (12)
求解(12)式的方法同步骤1),因此最终求得第k个目标的图像信息表示为如下(13)式:The method of solving formula (12) is the same as step 1), so the image information of the kth target is finally obtained as the following formula (13):
将(13)式中的N×1阶矩阵Xk重新排列成m×n阶矩阵即可得到目标的二维像;The two-dimensional image of the target can be obtained by rearranging the N × 1 order matrix X k in the formula (13) into an m × n order matrix;
4)对于目标的距离信息,将数据采集模块(6)记录的时间做平均,得到如下(14)式:4) For the distance information of the target, the time recorded by the data acquisition module (6) is averaged to obtain the following formula (14):
上式中,T1为第1个目标的时间信息,依次类推Tk为第k个目标的距离信息;In the above formula, T 1 is the time information of the first target, and by analogy T k is the distance information of the k-th target;
然后得到目标的距离信息为如下(15)式:Then the distance information of the target is obtained as the following formula (15):
上式中,d1为第1个目标的距离信息,依次类推dk为第k个目标的距离信息;In the above formula, d 1 is the distance information of the first target, and d k is the distance information of the k-th target by analogy;
至此,由公式(13)、(15)式,即可得到所有目标的三维像数据。So far, according to formulas (13) and (15), the 3D image data of all targets can be obtained.
本发明的优点在于:The advantages of the present invention are:
(1)本发明采用DMD调制目标的回波信号,与传统的逐点扫描式激光雷达相比,取消机械扫描装置,实现激光雷达系统的小型化和轻量化,具有很强的抗震能力。同时三维图像重构所需的采样数据少。(1) The present invention uses DMD to modulate the echo signal of the target. Compared with the traditional point-by-point scanning laser radar, the mechanical scanning device is eliminated, and the laser radar system is miniaturized and lightweight, and has strong earthquake resistance. At the same time, less sampling data is required for 3D image reconstruction.
(2)本发明系统采用单元雪崩二极管APD作为探测器,与传统的推扫式激光雷达相比,将克服国产线阵大规模雪崩二极管APD在工艺上无法集成的瓶颈问题,同时解决推扫式激光雷达信噪比低,探测灵敏度低等问题。(2) The system of the present invention adopts the unit avalanche diode APD as the detector. Compared with the traditional push-broom laser radar, it will overcome the bottleneck problem that the domestic linear array large-scale avalanche diode APD cannot be integrated in the process, and solve the push-broom laser radar at the same time. Lidar has low signal-to-noise ratio and low detection sensitivity.
附图说明Description of drawings
图1是一种基于压缩感知的激光雷达成像系统及方法,1是激光发射模块;2是望远镜成像模块;3是数字微反射镜DMD及控制模块;4是光学汇聚透镜;5是雪崩二极管APD;6是数据采集模块;7是图像重构模块;8是同步模块;Fig. 1 is a laser radar imaging system and method based on compressed sensing, 1 is the laser emission module; 2 is the telescope imaging module; 3 is the digital micro-mirror DMD and the control module; 4 is the optical convergence lens; 5 is the avalanche diode APD ; 6 is a data acquisition module; 7 is an image reconstruction module; 8 is a synchronization module;
图2是目标回波每次在APD上接收到的信号形式,其中图(a)是第一次调制信号,图(b)是第M次调制信号。Figure 2 is the signal form of the target echo received on the APD each time, where Figure (a) is the first modulation signal, and Figure (b) is the Mth modulation signal.
具体实施方式Detailed ways
下面结合图1给出本发明的一个较好实例,主要作进一步详细说明,而非用来限定本发明的范围。A better example of the present invention is given below in conjunction with FIG. 1 , which is mainly described in further detail, but not used to limit the scope of the present invention.
本发明的具体实施方式主要分为以下几步:The specific embodiment of the present invention is mainly divided into the following steps:
(1)首先确定系统各模块所用元部件的技术参数,具体如下:激光发射模块1采用上海布里渊激光科技有限公司的激光器,技术指标为:工作波长1064nm,重复频率100Hz,脉冲能量200mJ;望远镜成像模块2采用爱蒙特光学(深圳)有限公司的望远镜,选定焦距为304.8mm,口径为101.6mm。数字微反射镜DMD及控制模块3采用美国TI公司生产的DMD,技术指标为1024×768像素,像素大小为13.69μm,控制板采用与之配合的TI-Discovery-4100;光学汇聚透镜4焦距为10cm;雪崩二极管APD5采用美国Pacific Silicon Sensor公司生产的AD1500-10,像元尺寸1.5mm,暗电流7nA,上升时间5ns,响应率36A/w;数据采集模块6采用坤驰科技的QT1230采集卡,技术指标为:量化位数10位,采样率最高为5GSPS;同步模块8采用赛灵思公司的Spartan-6-XC6SLX9芯片产生三路同步信号;(1) First determine the technical parameters of the components used in each module of the system, as follows: Laser emission module 1 adopts the laser of Shanghai Brillouin Laser Technology Co., Ltd., and the technical indicators are: working wavelength 1064nm, repetition frequency 100Hz, pulse energy 200mJ; The telescope imaging module 2 adopts the telescope of Edmund Optics (Shenzhen) Co., Ltd., the selected focal length is 304.8mm, and the aperture is 101.6mm. The digital micromirror DMD and the control module 3 adopt the DMD produced by TI Company of the United States, the technical index is 1024×768 pixels, the pixel size is 13.69 μm, the control board adopts the TI-Discovery-4100 matched with it; the focal length of the optical convergence lens 4 is 10cm; avalanche diode APD5 adopts AD1500-10 produced by Pacific Silicon Sensor Company of the United States, with a pixel size of 1.5mm, dark current of 7nA, rise time of 5ns, and response rate of 36A/w; data acquisition module 6 adopts QT1230 acquisition card of Kunchi Technology, The technical indicators are: 10 quantization digits, the highest sampling rate is 5GSPS; the synchronization module 8 adopts the Spartan-6-XC6SLX9 chip of Xilinx Company to generate three synchronous signals;
(2)系统硬件确定后,首先是同步模块8发射同步信号脉冲,激光发射模块1收到同步信号脉冲以后,向目标发射脉冲激光。(2) After the system hardware is determined, firstly, the synchronization module 8 emits a synchronization signal pulse, and the laser emitting module 1 emits a pulsed laser to the target after receiving the synchronization signal pulse.
(3)同时,数字微反射镜DMD及控制模块3接收到同步脉冲信号以后,加载一个调制模板发送到DMD,调制模板是一个大小为256×192,并且服从高斯随机分布的0,1矩阵,这些调制模板事先生成好,本次实施生成5000个模板。由于步骤(1)所选取的DMD为1024×768像素,为了能让DMD正确识别,实际加载到DMD的模板选取大小为1024×768,超出256×192的元素全部用“0”补全。通过调制,使DMD的微镜处于一定的开关状态,其中“开”用“1”表示,“关”用“0”表示(具体使微镜翻转+12°(开)和-12°(关))。等微镜开关状态稳定以后,即可实现对回波目标的调制,翻转-12°反射的光线被丢弃,翻转+12°反射的光线接着进入后续的光学系统。然后,数据采集模块6进行数据采集。(1)(2)(3)步骤重复5000次,即可完成数据采集。(3) At the same time, after the digital micromirror DMD and the control module 3 receive the synchronous pulse signal, a modulation template is loaded and sent to the DMD. The modulation template is a 0,1 matrix with a size of 256×192 and subject to Gaussian random distribution, These modulation templates are generated in advance, and 5000 templates are generated in this implementation. Since the DMD selected in step (1) is 1024×768 pixels, in order to allow the DMD to be correctly identified, the size of the template actually loaded into the DMD is selected to be 1024×768, and all elements exceeding 256×192 are filled with “0”. Through modulation, the micromirror of the DMD is in a certain switch state, where "on" is represented by "1" and "off" is represented by "0" (specifically, the micromirror is flipped +12° (on) and -12° (off) )). After the state of the micromirror switch is stable, the modulation of the echo target can be realized, the light reflected by flipping -12° is discarded, and the light reflected by flipping +12° then enters the subsequent optical system. Then, the data acquisition module 6 performs data acquisition. (1) (2) (3) steps are repeated 5000 times to complete the data collection.
(4)最后图像重构模块(7)对采样数据进行处理即可得到目标的三维像。为了简要说明,设定场景有5个目标,每个目标的空间分辨率为:256×192像素大小。对每一个目标进行空间二维信息重构,需要求解256×192个未知数,而采样数据只有5000个,相当于数据采集模块6在采样的过程中数据被压缩了256×192-5000=44152个。对每个目标的距离信息重构,求解5个距离信息即可。(4) Finally, the image reconstruction module (7) processes the sampling data to obtain a three-dimensional image of the target. For a brief description, the scene is set to have 5 objects, and the spatial resolution of each object is: 256 × 192 pixel size. To reconstruct the spatial two-dimensional information of each target, 256×192 unknowns need to be solved, and the sampled data is only 5000, which is equivalent to the data being compressed by 256×192-5000=44152 during the sampling process of the data acquisition module 6 . To reconstruct the distance information of each target, it is enough to solve 5 distance information.
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