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CN111736162B - Laser illumination echo detection device and method for complex target - Google Patents

Laser illumination echo detection device and method for complex target Download PDF

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CN111736162B
CN111736162B CN202010769560.9A CN202010769560A CN111736162B CN 111736162 B CN111736162 B CN 111736162B CN 202010769560 A CN202010769560 A CN 202010769560A CN 111736162 B CN111736162 B CN 111736162B
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CN111736162A (en
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韩凯
崔文达
王彦
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National University of Defense Technology
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S17/00Systems using the reflection or reradiation of electromagnetic waves other than radio waves, e.g. lidar systems
    • G01S17/02Systems using the reflection of electromagnetic waves other than radio waves
    • G01S17/06Systems determining position data of a target
    • G01S17/08Systems determining position data of a target for measuring distance only
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
    • G01S7/4802Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00 using analysis of echo signal for target characterisation; Target signature; Target cross-section

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Abstract

本发明公开一种针对复杂目标的激光照明回波探测装置及方法,该装置包括初始光源、空间光调制器、半反半透镜、扩束单元、光场探测单元以及控制单元;该方法包括入射光束调制、照明光斑的调整、回波信号的探测、数据处理以及入射光束调制的优化。本发明提供的装置结构简单,且能够根据不同目标的特性获得最优的激光照明方案,同时本发明的装置具有光场调制和探测能力,给激光照明技术理论研究提供了灵活有效的研究平台;本发明提供的方法可快速获得照明系统极为关心的目标距离、回波辐射强度以及辐射方向分布特性等参数,为研究照明系统中各种因素对照明效果的影响提供试验数据支持。

Figure 202010769560

The invention discloses a laser illumination echo detection device and method for complex targets. The device includes an initial light source, a spatial light modulator, a half mirror, a beam expanding unit, a light field detection unit and a control unit; the method includes an incident Beam modulation, adjustment of illumination spot, detection of echo signals, data processing and optimization of incident beam modulation. The device provided by the present invention has a simple structure, and can obtain the optimal laser illumination scheme according to the characteristics of different targets, and at the same time, the device of the present invention has the capability of light field modulation and detection, and provides a flexible and effective research platform for the theoretical research of laser illumination technology; The method provided by the invention can quickly obtain parameters such as the target distance, echo radiation intensity and radiation direction distribution characteristics that the lighting system is very concerned about, and provide experimental data support for studying the influence of various factors in the lighting system on the lighting effect.

Figure 202010769560

Description

一种针对复杂目标的激光照明回波探测装置及方法A laser illumination echo detection device and method for complex targets

技术领域technical field

本发明涉及激光照明技术领域,尤其是一种针对复杂目标的激光照明回波探测装置及方法。The invention relates to the technical field of laser lighting, in particular to a laser lighting echo detection device and method for complex targets.

背景技术Background technique

激光照明是高能激光武器系统、大型天文望远镜等系统的重要组成部分之一,在可见度较低或者复杂光照条件下,激光照明系统能够照亮目标,提高探测到的目标回波强度和信噪比,为高能激光主发射系统提供较为精确的目标方位和形貌信息。另外,被激光照亮的目标自身可作为大气湍流矫正系统的信标源,显著改善成像质量,提高跟瞄效率。Laser lighting is one of the important components of high-energy laser weapon systems, large astronomical telescopes and other systems. Under low visibility or complex lighting conditions, the laser lighting system can illuminate the target and improve the detected target echo intensity and signal-to-noise ratio. , to provide more accurate target orientation and topography information for the high-energy laser main emission system. In addition, the target illuminated by the laser itself can be used as the beacon source of the atmospheric turbulence correction system, which can significantly improve the imaging quality and improve the tracking and aiming efficiency.

在实际应用中,激光照明是一个十分复杂的系统工程,照明效果与多种因素密切相关。其中,目标多为结构复杂的几何体,而目标特定位置的材质与几何结构可直接影响回波的强度与辐射方向,从而影响回波探测器接收到的回波强度,最终影响探测跟踪系统对目标的探测概率,而现有技术中还没有能够根据不同目标的特性实现最优照明效果的技术方案。In practical applications, laser lighting is a very complex system engineering, and the lighting effect is closely related to many factors. Among them, the targets are mostly geometric bodies with complex structures, and the material and geometric structure of the specific position of the target can directly affect the intensity and radiation direction of the echoes, thereby affecting the echo intensity received by the echo detector, and finally affecting the detection and tracking system. However, in the prior art, there is no technical solution that can realize the optimal lighting effect according to the characteristics of different targets.

此外,受限于试验条件、试验成本等客观因素,目前国内对于激光照明技术中一些具体科学问题的研究仍然不够充分,还没有一种能够快速、便捷地获得目标距离、回波辐射强度与方向特性等与照明效果密切相关的关键参数的技术。而如果通过真实的外场试验研究以上这些问题,不仅成本和费效比令人难以接受,后续的关键技术攻关也将十分困难。In addition, limited by objective factors such as test conditions and test costs, the current domestic research on some specific scientific issues in laser lighting technology is still insufficient, and there is no one that can quickly and easily obtain the target distance, echo radiation intensity and direction. characteristics and other key parameters closely related to lighting effects. If the above problems are studied through real field tests, not only the cost and cost-effectiveness ratio is unacceptable, but the follow-up key technology research will also be very difficult.

发明内容SUMMARY OF THE INVENTION

本发明提供一种针对复杂目标的激光照明回波探测装置及方法,用于克服现有技术中不能根据不同目标的特性实现最优照明效果以及不能快速、便捷地获得照明技术中的关键参数等缺陷。The invention provides a laser illumination echo detection device and method for complex targets, which are used to overcome the inability to achieve optimal illumination effects according to the characteristics of different targets in the prior art, and the inability to quickly and conveniently obtain key parameters in the illumination technology. defect.

为实现上述目的,本发明提出一种针对复杂目标的激光照明回波探测装置,所述激光照明回波探测装置包括初始光源、空间光调制器、半反半透镜、扩束单元、光场探测单元以及控制单元;In order to achieve the above purpose, the present invention proposes a laser illumination echo detection device for complex targets, the laser illumination echo detection device includes an initial light source, a spatial light modulator, a half mirror and a half mirror, a beam expanding unit, and a light field detection device. unit and control unit;

所述初始光源用于提供入射光束;the initial light source is used to provide the incident light beam;

所述空间光调制器接收所述入射光束并对所述入射光束进行强度分布调制,得到具有设定局域强度分布模式的出射光束;The spatial light modulator receives the incident light beam and modulates the intensity distribution of the incident light beam to obtain an outgoing light beam with a set local intensity distribution pattern;

所述扩束单元接收从所述半反半透镜透过的所述出射光束,并对所述出射光束进行扩束,获得覆盖整个目标模型的照明光斑;The beam expanding unit receives the outgoing beam transmitted through the semi-reflective semi-mirror, and expands the outgoing beam to obtain an illumination spot covering the entire target model;

所述扩束单元接收所述照明光斑照射所述目标模型后产生的回波信号,并将所述回波信号射出;The beam expander unit receives an echo signal generated after the illumination spot illuminates the target model, and emits the echo signal;

所述半反半透镜将所述回波信号反射进入所述光场探测单元;The semi-reflective semi-mirror reflects the echo signal into the light field detection unit;

所述光场探测单元对所述回波信号进行探测,并将所述探测获得的数据实时传送至所述控制单元;The light field detection unit detects the echo signal, and transmits the data obtained by the detection to the control unit in real time;

所述控制单元利用光场解码算法对所述探测获得的数据进行解码,获得目标距离、回波辐射强度以及辐射方向分布特性;同时,所述控制单元根据所述回波辐射强度以及所述辐射方向分布特性实时控制所述空间光调制器对所述入射光束的强度分布调制。The control unit decodes the data obtained by the detection by using the light field decoding algorithm to obtain the target distance, echo radiation intensity and radiation direction distribution characteristics; The directional distribution characteristic controls the intensity distribution modulation of the incident light beam by the spatial light modulator in real time.

为实现上述目的,本发明还提出一种针对复杂目标的激光照明回波探测方法,所述激光照明回波探测方法包括:In order to achieve the above object, the present invention also proposes a laser illumination echo detection method for complex targets, the laser illumination echo detection method includes:

利用空间光调制器接收初始光源提供的入射光束,并利用所述空间光调制器对所述入射光束进行强度分布调制,得到具有设定局域强度分布模式的出射光束;Using the spatial light modulator to receive the incident light beam provided by the initial light source, and using the spatial light modulator to perform intensity distribution modulation on the incident light beam to obtain an outgoing light beam with a set local intensity distribution pattern;

利用扩束单元对所述出射光束进行扩束,获得覆盖整个目标模型的照明光斑;The outgoing beam is expanded by a beam expansion unit to obtain an illumination spot covering the entire target model;

利用扩束单元接收所述照明光斑照射所述目标模型后产生的回波信号,并将所述回波信号射出;Using a beam expander unit to receive the echo signal generated by the illumination spot irradiating the target model, and to emit the echo signal;

利用半反半透镜将所述回波信号反射进入光场探测单元;Using a half mirror to reflect the echo signal into the light field detection unit;

利用所述光场探测单元对所述回波信号进行探测,获得探测数据;Use the light field detection unit to detect the echo signal to obtain detection data;

利用控制单元对所述探测数据进行解码,获得目标距离、回波辐射强度以及辐射方向分布特性;Use the control unit to decode the detection data to obtain the target distance, echo radiation intensity and radiation direction distribution characteristics;

根据所述回波辐射强度以及所述辐射方向分布特性,判断所述目标模型的总回波辐射强度是否达到最大,若达到,则输出目标距离、所述空间光调制器的调制相位分布、出射光束的光强分布、所述目标模型的姿态、所述回波辐射强度以及所述辐射方向分布特性;否则通过所述控制单元调整所述空间光调制器的调制相位,直至获得的所述目标模型的总回波辐射强度达到最大。According to the echo radiation intensity and the distribution characteristics of the radiation direction, it is judged whether the total echo radiation intensity of the target model reaches the maximum, and if so, output the target distance, the modulation phase distribution of the spatial light modulator, and the output The light intensity distribution of the light beam, the posture of the target model, the echo radiation intensity, and the distribution characteristics of the radiation direction; otherwise, the modulation phase of the spatial light modulator is adjusted by the control unit until the target is obtained. The total echo radiation intensity of the model is at its maximum.

与现有技术相比,本发明的有益效果有:Compared with the prior art, the beneficial effects of the present invention are:

1、本发明提供的针对复杂目标的激光照明回波探测装置,首先利用空间光调制器对入射光束进行强度分布调制,获得具有设定局域强度分布模式的出射光束;再利用扩束单元对出射光束进行扩束,获得能够覆盖整个目标模型的照明光斑;接着利用光场探测单元对目标模型反射和散射的回波信号进行探测,并将探测获得的数据实时传送至控制单元;最后通过控制单元对探测获得的数据进行解码,获得目标距离、回波辐射强度以及辐射方向分布特性,同时控制单元将根据该回波辐射强度以及辐射方向分布特性实时控制空间光调制器对入射光束的强度分布调制,以使目标模型的总回波辐射强度达到最大。本发明提供的装置结构简单,且能够根据不同目标的特性获得最优的激光照明方案,同时本发明的装置具有光场调制和探测能力,给激光照明技术理论研究提供了灵活有效的研究平台。1. The laser illumination echo detection device for complex targets provided by the present invention firstly uses a spatial light modulator to modulate the intensity distribution of the incident beam to obtain an outgoing beam with a set local intensity distribution pattern; The outgoing beam is expanded to obtain an illumination spot that can cover the entire target model; then, the light field detection unit is used to detect the echo signals reflected and scattered by the target model, and the data obtained from the detection is transmitted to the control unit in real time; finally, through the control The unit decodes the data obtained by the detection to obtain the target distance, echo radiation intensity and radiation direction distribution characteristics. At the same time, the control unit will control the intensity distribution of the incident beam by the spatial light modulator in real time according to the echo radiation intensity and radiation direction distribution characteristics. Modulation to maximize the total echo radiation intensity of the target model. The device provided by the present invention has a simple structure, and can obtain optimal laser illumination schemes according to the characteristics of different targets. Meanwhile, the device of the present invention has light field modulation and detection capabilities, providing a flexible and effective research platform for theoretical research on laser illumination technology.

2、本发明提供的针对复杂目标的激光照明回波探测方法,首先利用光场探测装置实时接收目标模型反射和散射回波信号并对回波信号进行探测;然后利用控制单元对所述探测数据进行数据处理,获得目标距离、回波辐射强度以及辐射方向分布特性,并根据回波辐射强度以及辐射方向分布特性判断所述目标模型的总回波辐射强度是否达到最大,若达到,则输出目标距离、所述空间光调制器的调制相位分布、出射光束的光强分布、所述目标模型的姿态、所述回波辐射强度以及所述辐射方向分布特性;否则通过控制单元调整空间光调制器的调制相位,直至获得的目标模型的总回波辐射强度达到最大。本发明提供的探测方法可快速获得照明系统极为关心的目标距离、回波辐射强度以及辐射方向分布特性等参数,为研究照明系统中各种因素对照明效果的影响提供试验数据支持。2. The laser illumination echo detection method for complex targets provided by the present invention firstly uses a light field detection device to receive the reflected and scattered echo signals of the target model in real time and detect the echo signals; then use a control unit to detect the detection data. Perform data processing to obtain the target distance, echo radiation intensity and radiation direction distribution characteristics, and judge whether the total echo radiation intensity of the target model reaches the maximum according to the echo radiation intensity and radiation direction distribution characteristics, and if so, output the target distance, the modulation phase distribution of the spatial light modulator, the light intensity distribution of the outgoing beam, the attitude of the target model, the echo radiation intensity, and the distribution characteristics of the radiation direction; otherwise, the spatial light modulator is adjusted by the control unit until the total echo radiation intensity of the obtained target model reaches the maximum. The detection method provided by the invention can quickly obtain parameters such as target distance, echo radiation intensity and radiation direction distribution characteristics that the lighting system is very concerned about, and provide experimental data support for studying the influence of various factors in the lighting system on the lighting effect.

附图说明Description of drawings

为了更清楚地说明本发明实施例或现有技术中的技术方案,下面将对实施例或现有技术描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图示出的结构获得其他的附图。In order to explain the embodiments of the present invention or the technical solutions in the prior art more clearly, the following briefly introduces the accompanying drawings that need to be used in the description of the embodiments or the prior art. Obviously, the accompanying drawings in the following description are only These are some embodiments of the present invention, and for those of ordinary skill in the art, other drawings can also be obtained according to the structures shown in these drawings without creative efforts.

图1为本发明提供的针对复杂目标的激光照明回波探测装置的结构图;1 is a structural diagram of a laser illumination echo detection device for complex targets provided by the present invention;

图2为本发明实施例中聚焦型光场相机的结构图;2 is a structural diagram of a focusing light field camera in an embodiment of the present invention;

图3为本发明提供的针对复杂目标的激光照明回波探测方法流程图。FIG. 3 is a flow chart of the method for detecting the echoes of laser illumination for complex targets provided by the present invention.

附图标号说明:1:初始光源;2:起偏器;3:空间光调制器;4:半反半透镜;5:扩束单元;51:次镜;52:主镜;6:目标模型;7:光场探测单元;71:主透镜;72:微透镜阵列;73:窗口;74:成像靶面;8:控制单元。Description of reference numerals: 1: initial light source; 2: polarizer; 3: spatial light modulator; 4: half mirror; 5: beam expander unit; 51: secondary mirror; 52: primary mirror; 6: target model 7: light field detection unit; 71: main lens; 72: microlens array; 73: window; 74: imaging target surface; 8: control unit.

本发明目的的实现、功能特点及优点将结合实施例,参照附图做进一步说明。The realization, functional characteristics and advantages of the present invention will be further described with reference to the accompanying drawings in conjunction with the embodiments.

具体实施方式Detailed ways

下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本发明的一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有作出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。The technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the accompanying drawings in the embodiments of the present invention. Obviously, the described embodiments are only a part of the embodiments of the present invention, not all of the embodiments. Based on the embodiments of the present invention, all other embodiments obtained by those of ordinary skill in the art without creative efforts shall fall within the protection scope of the present invention.

另外,本发明各个实施例之间的技术方案可以相互结合,但是必须是以本领域普通技术人员能够实现为基础,当技术方案的结合出现相互矛盾或无法实现时应当认为这种技术方案的结合不存在,也不在本发明要求的保护范围之内。In addition, the technical solutions between the various embodiments of the present invention can be combined with each other, but must be based on the realization by those of ordinary skill in the art. When the combination of technical solutions is contradictory or cannot be realized, it should be considered that the combination of technical solutions does not exist and is not within the scope of protection claimed by the present invention.

本发明提出一种针对复杂目标的激光照明回波探测装置,如图1所示,该装置包括初始光源1、空间光调制器3、半反半透镜4、扩束单元5、光场探测单元7以及控制单元8;The present invention proposes a laser illumination echo detection device for complex targets, as shown in FIG. 1 , the device includes an initial light source 1, a spatial light modulator 3, a half mirror 4, a beam expanding unit 5, and a light field detection unit 7 and the control unit 8;

初始光源1用于提供入射光束;The initial light source 1 is used to provide the incident light beam;

空间光调制器3接收入射光束并对入射光束进行强度分布调制,得到具有设定局域强度分布模式(经过空间光调制器调制后,照明光强由均匀分布变为设定的特定光强分布)的出射光束;通过空间光调制器3可实现照明光斑强度分布的控制;The spatial light modulator 3 receives the incident light beam and modulates the intensity distribution of the incident light beam to obtain a set local intensity distribution pattern (after modulation by the spatial light modulator, the illumination light intensity changes from a uniform distribution to a set specific light intensity distribution. ) of the outgoing beam; through the spatial light modulator 3, the intensity distribution of the illumination spot can be controlled;

扩束单元5接收从半反半透镜4透过的出射光束,并对出射光束进行扩束,获得覆盖整个目标模型6的照明光斑;The beam expanding unit 5 receives the outgoing beam transmitted from the semi-reflective semi-mirror 4, and expands the outgoing beam to obtain an illumination spot covering the entire target model 6;

扩束单元5接收照明光斑照射目标模型6后产生的回波信号,并将回波信号射出(回波信号经扩束单元5后入射至半反半透镜4);The beam expander unit 5 receives the echo signal generated by the illumination spot irradiating the target model 6, and emits the echo signal (the echo signal is incident on the semi-reflective semi-mirror 4 after passing through the beam expander unit 5);

半反半透镜4将回波信号反射进入光场探测单元7;The half mirror half mirror 4 reflects the echo signal into the light field detection unit 7;

光场探测单元7对回波信号进行探测,并将探测获得的数据(探测获得的数据为回波信号经过光场探测单元7后获得的各个像素值)实时传送至控制单元8;The light field detection unit 7 detects the echo signal, and transmits the data obtained by the detection (the data obtained by the detection is each pixel value obtained after the echo signal passes through the light field detection unit 7) to the control unit 8 in real time;

控制单元8利用光场解码算法对探测获得的数据进行解码,获得目标距离、回波辐射强度以及辐射方向分布特性;同时,控制单元8根据回波辐射强度以及辐射方向分布特性实时控制空间光调制器3对入射光束的强度分布调制。The control unit 8 uses the light field decoding algorithm to decode the data obtained by the detection, and obtains the target distance, the echo radiation intensity and the radiation direction distribution characteristics; meanwhile, the control unit 8 controls the spatial light modulation in real time according to the echo radiation intensity and the radiation direction distribution characteristics. The intensity distribution of the incident beam is modulated by the device 3.

目标距离是指目标模型6与光场探测单元7之间的距离。The target distance refers to the distance between the target model 6 and the light field detection unit 7 .

回波辐射强度是指目标模型的总回波辐射强度

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。The echo radiation intensity refers to the total echo radiation intensity of the target model
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.

辐射方向分布特性是指目标模型6反射和散射的回波信号在各个方向上光线的数量。The radiation direction distribution characteristic refers to the number of rays in various directions of the echo signals reflected and scattered by the target model 6 .

空间光调制器3根据预先输入的调制相位对入射光束进行强度分布调制,输出一束强度分布不均匀的出射光束,该出射光束的光强分布遵循预先设定的光强分布规律。因此,通过该空间光调制器3可实现出射光束强度分布的控制,从而可以调整照明光斑在目标模型6不同部位的辐照强度,可用于研究照明回波与不同强度分布的照明光之间的关系。The spatial light modulator 3 modulates the intensity distribution of the incident light beam according to the pre-input modulation phase, and outputs an outgoing light beam with uneven intensity distribution. The light intensity distribution of the outgoing light beam follows a preset light intensity distribution law. Therefore, the spatial light modulator 3 can realize the control of the intensity distribution of the outgoing beam, so that the irradiation intensity of the illumination spot at different parts of the target model 6 can be adjusted, which can be used to study the relationship between the illumination echo and the illumination light with different intensity distributions. relation.

本发明提供的针对复杂目标的激光照明回波探测装置,首先利用空间光调制器对入射光束进行强度分布调制,获得具有设定局域强度分布模式的出射光束;再利用扩束单元对出射光束进行扩束,获得能够覆盖整个目标模型的照明光斑;接着利用光场探测单元对目标模型反射和散射的回波信号进行探测,并将探测获得的数据实时传送至控制单元;最后通过控制单元对探测获得的数据进行解码,获得目标距离、回波辐射强度以及辐射方向分布特性,同时控制单元将根据该回波辐射强度以及辐射方向分布特性实时控制空间光调制器对入射光束的强度分布调制,以使目标模型的总回波辐射强度达到最大。本发明提供的装置结构简单,且能够根据不同目标的特性获得最优的激光照明方案,同时本发明的装置具有光场调制和探测能力,给激光照明技术理论研究提供了灵活有效的研究平台。The laser illumination echo detection device for complex targets provided by the present invention firstly uses a spatial light modulator to modulate the intensity distribution of the incident beam to obtain an outgoing beam with a set local intensity distribution pattern; Expand the beam to obtain an illumination spot that can cover the entire target model; then use the light field detection unit to detect the echo signals reflected and scattered by the target model, and transmit the detected data to the control unit in real time; The data obtained by the detection is decoded to obtain the target distance, echo radiation intensity and radiation direction distribution characteristics. At the same time, the control unit will control the intensity distribution modulation of the incident beam by the spatial light modulator in real time according to the echo radiation intensity and radiation direction distribution characteristics. In order to maximize the total echo radiation intensity of the target model. The device provided by the present invention has a simple structure, and can obtain optimal laser illumination schemes according to the characteristics of different targets. Meanwhile, the device of the present invention has light field modulation and detection capabilities, providing a flexible and effective research platform for theoretical research on laser illumination technology.

在其中一个实施例中,激光照明回波探测装置还包括起偏器2,起偏器2设置在初始光源1与空间光调制器3之间,用于从初始光源1射出的入射光束中获得偏振光并将该偏振光输入空间光调制器3中。In one of the embodiments, the laser illumination echo detection device further includes a polarizer 2 , and the polarizer 2 is arranged between the initial light source 1 and the spatial light modulator 3 , and is used for obtaining from the incident light beam emitted by the initial light source 1 polarized light and input the polarized light into the spatial light modulator 3 .

起偏器2用于从自然激光中获得偏振光。The polarizer 2 is used to obtain polarized light from natural laser light.

在另一实施例中,扩束单元5包括同轴的次镜51和主镜52,次镜51的半径小于主镜52的半径,次镜51与主镜52之间的距离可调节;In another embodiment, the beam expander unit 5 includes a coaxial secondary mirror 51 and a primary mirror 52, the radius of the secondary mirror 51 is smaller than the radius of the primary mirror 52, and the distance between the secondary mirror 51 and the primary mirror 52 is adjustable;

出射光束经次镜51收集后进入扩束单元5,由主镜51射出并照射目标模型6。The outgoing beam is collected by the secondary mirror 51 and then enters the beam expander unit 5 , and is emitted by the primary mirror 51 to illuminate the target model 6 .

初始光源1、空间光调制器3、半反半透镜4与扩束单元5组成本发明激光照明回波探测装置的照明系统,扩束单元5作为该照明系统的发射终端,能够提高该照明系统的发射口径,控制照明光束在目标模型6处的聚焦状态和光斑尺寸。本发明中扩束单元5采用两级透镜系统,包括次镜51与主镜52。照明光斑的大小由次镜焦距、主镜焦距、主镜与次镜之间的距离以及目标模型与主镜之间的距离共同决定;进一步地,主镜52与次镜51之间的距离可调,以满足不同照明光条件下的实验需求。The initial light source 1, the spatial light modulator 3, the half mirror and the half mirror 4 and the beam expanding unit 5 constitute the lighting system of the laser illumination echo detection device of the present invention, and the beam expanding unit 5 acts as the emission terminal of the lighting system, which can improve the lighting system. The emission aperture of , controls the focus state and spot size of the illumination beam at the target model 6 . In the present invention, the beam expander unit 5 adopts a two-stage lens system, including a secondary mirror 51 and a primary mirror 52 . The size of the illumination spot is determined by the focal length of the secondary mirror, the focal length of the primary mirror, the distance between the primary mirror and the secondary mirror, and the distance between the target model and the primary mirror; further, the distance between the primary mirror 52 and the secondary mirror 51 can be It can be adjusted to meet the experimental needs under different lighting conditions.

在下一个实施例中,光场探测单元7为聚焦型光场相机;In the next embodiment, the light field detection unit 7 is a focusing light field camera;

聚焦型光场相机如图2所示,包括主透镜71和微透镜阵列72,目标模型P通过窗口73在主透镜71下形成一次成像点P’(实质为目标模型产生的回波信号通过窗口73在目标模型),一次成像点P’通过微透镜阵列72并在微透镜阵列72的不同微透镜下在成像靶面74再次成像形成多个二次成像点P”;多个所述二次成像点的像素即为探测获得的数据。As shown in Figure 2, the focusing light field camera includes a main lens 71 and a microlens array 72. The target model P forms a primary imaging point P' under the main lens 71 through a window 73 (essentially, the echo signal generated by the target model passes through the window. 73 in the target model), the primary imaging point P' passes through the microlens array 72 and is imaged again on the imaging target surface 74 under different microlenses of the microlens array 72 to form a plurality of secondary imaging points P"; The pixels of the imaging point are the data obtained by detection.

聚焦型光场相机等效为二次成像系统,目标模型的一次成像通过微透镜阵列72二次成像到红外传感器(即成像靶面74)上,相当于产生了一组“复眼”对同一个目标模型成像,以便探测出回波信号的光场信息。图2中,

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分别为主透镜71的口径、焦距;
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分别为微透镜阵列72中微透镜的口径、焦距;
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分别为主透镜成像空间中的物距、像距;
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分别为微透镜阵列的物距、像距;
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为主透镜到成像靶面的距离。The focusing light field camera is equivalent to a secondary imaging system. The primary imaging of the target model is secondary imaging to the infrared sensor (ie, the imaging target surface 74 ) through the microlens array 72 , which is equivalent to generating a group of "compound eyes" on the same The target model is imaged in order to detect the light field information of the echo signal. In Figure 2,
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,
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are the diameter and focal length of the main lens 71, respectively;
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,
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are the diameter and focal length of the microlenses in the microlens array 72, respectively;
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,
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are the object distance and image distance in the imaging space of the main lens, respectively;
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,
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are the object distance and image distance of the microlens array, respectively;
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The distance from the main lens to the imaging target surface.

在某个实施例中,目标模型6安装在电动云台上,电动云台在控制单元8的控制下带动目标模型6旋转和移动。In a certain embodiment, the target model 6 is installed on an electric pan/tilt head, and the electric pan/tilt head drives the target model 6 to rotate and move under the control of the control unit 8 .

通过电动云台可调节目标模型6的姿态、目标模型6与扩束单元5的距离。电动云台的运动控制参数由控制单元8根据程序预设或人工干预给出。进一步地,根据不同的研究背景,可以采用几种常见的典型目标模型,如飞机、无人机、卫星等,用于研究目标的几何结构、材质以及位姿对照明效果的影响。The posture of the target model 6 and the distance between the target model 6 and the beam expander unit 5 can be adjusted through the electric head. The motion control parameters of the electric pan/tilt head are given by the control unit 8 according to program preset or manual intervention. Further, according to different research backgrounds, several common typical target models can be used, such as airplanes, drones, satellites, etc., to study the influence of the geometric structure, material, and pose of the target on the lighting effect.

在另一个实施例中,空间光调制器3与扩束单元5之间的距离大于

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,其中
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为入射光束的半径,
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为入射光束的波长。In another embodiment, the distance between the spatial light modulator 3 and the beam expander unit 5 is greater than
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,in
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is the radius of the incident beam,
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is the wavelength of the incident beam.

空间光调制器3与扩束单元5之间的距离是指空间光调制器3与扩束单元5中次镜51之间的距离,控制该距离以满足照明光远场传输条件,从而获得所需的光强调制。The distance between the spatial light modulator 3 and the beam expander unit 5 refers to the distance between the spatial light modulator 3 and the secondary mirror 51 in the beam expander unit 5, and the distance is controlled to meet the illumination light far-field transmission conditions, so as to obtain the desired distance. desired intensity control.

在某个实施例中,初始光源1为激光器。In a certain embodiment, the initial light source 1 is a laser.

照明光斑照射目标模型6后,会产生后向反射和散射的回波信号,该回波信号通过扩束单元5入射至半反半透镜4,经半反半透镜4反射后进入光场探测单元7。在实际应用中,目标距离、回波辐射强度以及辐射方向分布特性是照明系统极为关心的三个参数。本发明采用聚焦型光场相机结构作为回波信号的光场探测单元并通过控制单元解算获得以上三个参数。不同于传统的点目标探测技术,聚焦型光场相机具有较大的视场,因而能够一次性得到视场内所有目标模型的距离值、辐射强度以及辐射强度的方向分布,从而大大减小回波探测装置的复杂度。After the illumination spot illuminates the target model 6, a retroreflection and scattering echo signal will be generated. The echo signal is incident on the half mirror 4 through the beam expander unit 5, and then enters the light field detection unit after being reflected by the half mirror 4. 7. In practical applications, the target distance, echo radiation intensity and radiation direction distribution characteristics are the three parameters of great concern to the lighting system. The present invention adopts the focusing light field camera structure as the light field detection unit of the echo signal, and obtains the above three parameters through calculation by the control unit. Different from the traditional point target detection technology, the focusing light field camera has a large field of view, so it can obtain the distance value, radiation intensity and directional distribution of radiation intensity of all target models in the field of view at one time, thereby greatly reducing the return. The complexity of the wave detection device.

控制单元8不仅作为本发明激光照明回波探测装置人机交互的接口,同时也负责控制空间光调制器3和电动云台等设备的工作。另外,由于光场数据解码运算量巨大,光场解码也由控制单元8统完成。The control unit 8 not only serves as an interface for human-computer interaction of the laser illumination echo detection device of the present invention, but also is responsible for controlling the work of the spatial light modulator 3 and the electric pan/tilt and other equipment. In addition, due to the huge computational complexity of the light field data decoding, the light field decoding is also completed by the control unit 8.

在试验过程中,照明光(即入射光束)经调制后照射在目标模型6上,照明回波(即回波信号)由光场探测单元7收集,经控制单元8解算获得目标距离、回波辐射强度及辐射方向分布特性,通过不断调整照明光的光强分布,使得目标模型6在特定目标距离、特定辐射方向的照明回波辐射强度达到最强。During the test, the illumination light (ie the incident beam) is modulated and irradiated on the target model 6, the illumination echo (ie the echo signal) is collected by the light field detection unit 7, and the target distance, echo signal are obtained by the control unit 8 through calculation The wave radiation intensity and radiation direction distribution characteristics, by continuously adjusting the light intensity distribution of the illumination light, make the illumination echo radiation intensity of the target model 6 at a specific target distance and specific radiation direction reach the strongest.

本发明还提出一种针对复杂目标的激光照明回波探测方法,如图3所示,包括:The present invention also proposes a laser illumination echo detection method for complex targets, as shown in FIG. 3 , including:

101:利用空间光调制器接收初始光源提供的入射光束,并利用所述空间光调制器对所述入射光束进行强度分布调制,得到具有设定局域强度分布模式的出射光束;101: Use a spatial light modulator to receive an incident light beam provided by an initial light source, and use the spatial light modulator to perform intensity distribution modulation on the incident light beam to obtain an outgoing light beam having a set local intensity distribution pattern;

102:利用扩束单元对所述出射光束进行扩束,获得覆盖整个目标模型的照明光斑;102: Use a beam expanding unit to expand the outgoing beam to obtain an illumination spot covering the entire target model;

103:利用扩束单元接收所述照明光斑照射所述目标模型后产生的回波信号,并将所述回波信号射出;103: Use a beam expander to receive an echo signal generated after the illumination spot irradiates the target model, and emit the echo signal;

104:利用半反半透镜将所述回波信号反射进入光场探测单元;104: Reflect the echo signal into the light field detection unit by using a half mirror half mirror;

105:利用所述光场探测单元对所述回波信号进行探测,获得探测数据;105: Use the light field detection unit to detect the echo signal to obtain detection data;

光场探测单元对回波信号进行探测获得光强信息,根据这些光强信息可以解码出光场信息。The light field detection unit detects the echo signal to obtain light intensity information, and the light field information can be decoded according to the light intensity information.

106:利用控制单元对所述探测数据进行解码,获得目标距离、回波辐射强度以及辐射方向分布特性;106: Use the control unit to decode the detection data to obtain the target distance, echo radiation intensity, and radiation direction distribution characteristics;

目标距离是指目标模型与扩束单元之间的距离。The target distance is the distance between the target model and the beam expander unit.

107:根据所述回波辐射强度以及所述辐射方向分布特性,判断所述目标模型的总回波辐射强度是否达到最大(总回波辐射强度随着出射光束光强分布的变化而不断改变,多次改变出射光束光强分布,获得多个总回波辐射强度,从中选择最大值),若达到,则输出目标距离、所述空间光调制器的调制相位分布、出射光束的光强分布(入射光束经过空间光调制器的相位调制,出射光束传播一定距离后,光强分布由均匀分布变为设定的特定分布形状)、所述目标模型的姿态、所述回波辐射强度以及所述辐射方向分布特性;否则通过所述控制单元调整所述空间光调制器的调制相位,直至获得的所述目标模型的总回波辐射强度达到最大。107: According to the echo radiation intensity and the radiation direction distribution characteristics, determine whether the total echo radiation intensity of the target model reaches the maximum (the total echo radiation intensity changes continuously with the change of the light intensity distribution of the outgoing beam, Change the light intensity distribution of the outgoing beam multiple times to obtain a plurality of total echo radiation intensities, and select the maximum value), if it is reached, output the target distance, the modulation phase distribution of the spatial light modulator, and the light intensity distribution of the outgoing beam ( The incident beam is phase-modulated by the spatial light modulator, and after the outgoing beam propagates a certain distance, the light intensity distribution changes from a uniform distribution to a set specific distribution shape), the attitude of the target model, the echo radiation intensity, and the Radiation direction distribution characteristics; otherwise, the modulation phase of the spatial light modulator is adjusted by the control unit until the obtained total echo radiation intensity of the target model reaches the maximum.

本发明提供的针对复杂目标的激光照明回波探测方法,首先利用光场探测装置实时接收目标模型反射和散射回波信号并对回波信号进行探测;然后利用控制单元对所述探测数据进行数据处理,获得目标距离、回波辐射强度以及辐射方向分布特性,并根据回波辐射强度以及辐射方向分布特性判断所述目标模型的总回波辐射强度是否达到最大,若达到,则输出目标距离、所述空间光调制器的调制相位分布、出射光束的光强分布、所述目标模型的姿态、所述回波辐射强度以及所述辐射方向分布特性;否则通过控制单元调整空间光调制器的调制相位,直至获得的目标模型的总回波辐射强度达到最大。本发明提供的探测方法可快速获得照明系统极为关心的目标距离、回波辐射强度以及辐射方向分布特性等参数,为研究照明系统中各种因素对照明效果的影响提供试验数据支持。The laser illumination echo detection method for complex targets provided by the present invention firstly utilizes the light field detection device to receive the reflected and scattered echo signals of the target model in real time and detect the echo signals; process, obtain the target distance, echo radiation intensity and radiation direction distribution characteristics, and judge whether the total echo radiation intensity of the target model reaches the maximum according to the echo radiation intensity and radiation direction distribution characteristics, and if so, output the target distance, The modulation phase distribution of the spatial light modulator, the light intensity distribution of the outgoing beam, the attitude of the target model, the echo radiation intensity, and the radiation direction distribution characteristics; otherwise, the modulation of the spatial light modulator is adjusted by the control unit phase until the total echo radiation intensity of the obtained target model reaches the maximum. The detection method provided by the invention can quickly obtain parameters such as target distance, echo radiation intensity and radiation direction distribution characteristics that the lighting system is very concerned about, and provide experimental data support for studying the influence of various factors in the lighting system on the lighting effect.

在其中一个实施例中,对于步骤101,利用空间光调制器接收初始光源提供的入射光束,并利用所述空间光调制器对所述入射光束进行强度分布调制,得到具有设定局域强度分布模式的出射光束,包括:In one embodiment, for step 101, a spatial light modulator is used to receive an incident light beam provided by an initial light source, and the spatial light modulator is used to perform intensity distribution modulation on the incident light beam to obtain a set local intensity distribution. Patterns of outgoing beams, including:

001:利用起偏器从初始光源提供的入射光束获得偏振光并将所述偏振光输入空间光调制器中;001: using a polarizer to obtain polarized light from an incident beam provided by an initial light source and inputting the polarized light into a spatial light modulator;

002:利用所述空间光调制器对所述偏振光进行强度分布调制,得到具有设定局域强度分布模式的出射光束。002: Use the spatial light modulator to perform intensity distribution modulation on the polarized light to obtain an outgoing light beam having a set local intensity distribution pattern.

在另一个实施例中,对于步骤102,利用扩束单元对所述出射光束进行扩束,获得覆盖整个目标模型的照明光斑,包括:In another embodiment, for step 102, using a beam expanding unit to expand the outgoing beam to obtain an illumination spot covering the entire target model, including:

201:调整扩束单元以使从所述扩束单元射出的照明光斑覆盖整个目标模型;201: Adjust the beam expander unit so that the illumination light spot emitted from the beam expander unit covers the entire target model;

调整扩束单元包括调整扩束单元中次镜焦距、主镜焦距、主镜与次镜之间的距离以及目标模型与主镜之间的距离等参数。Adjusting the beam expanding unit includes adjusting parameters such as the focal length of the secondary mirror, the focal length of the primary mirror, the distance between the primary mirror and the secondary mirror, and the distance between the target model and the primary mirror in the beam expanding unit.

202:利用调整好的所述扩束单元对所述出射光束进行扩束,获得覆盖整个目标模型的照明光斑。202 : Use the adjusted beam expanding unit to expand the outgoing beam to obtain an illumination spot covering the entire target model.

在下一个实施例中,光场探测单元为聚焦型光场相机,聚焦型光场相机包括主透镜和微透镜阵列,目标模型在主透镜下形成一次成像点,一次成像点通过微透镜阵列并在微透镜阵列的不同微透镜下再次成像形成多个二次成像点;多个所述二次成像点的像素即为探测获得的数据。In the next embodiment, the light field detection unit is a focusing light field camera, the focusing light field camera includes a main lens and a microlens array, the target model forms a primary imaging point under the main lens, and the primary imaging point passes through the microlens array and is Multiple secondary imaging points are formed by re-imaging under different microlenses of the microlens array; the pixels of the multiple secondary imaging points are the data obtained by detection.

对于步骤104,利用控制单元对所述探测数据进行解码,获得目标距离、回波辐射强度以及辐射方向分布特性,包括:For step 104, use the control unit to decode the detection data to obtain the target distance, echo radiation intensity and radiation direction distribution characteristics, including:

利用控制单元内的光场解码算法对探测数据进行数据处理,光场解码算法用虚深度

Figure 209341DEST_PATH_IMAGE015
描述一次成像点P’与微透镜阵列之间的规范化距离:The detection data is processed by the light field decoding algorithm in the control unit, and the light field decoding algorithm uses the virtual depth
Figure 209341DEST_PATH_IMAGE015
Describe the normalized distance between the primary imaging point P' and the microlens array:

Figure 536417DEST_PATH_IMAGE016
(1)
Figure 536417DEST_PATH_IMAGE016
(1)

式中,

Figure 86347DEST_PATH_IMAGE017
为虚深度;
Figure 498874DEST_PATH_IMAGE018
为微透镜阵列的物距(即一次成像点到微透镜阵列的实际距离);
Figure 589190DEST_PATH_IMAGE019
为微透镜阵列的像距;In the formula,
Figure 86347DEST_PATH_IMAGE017
is the virtual depth;
Figure 498874DEST_PATH_IMAGE018
is the object distance of the microlens array (that is, the actual distance from the primary imaging point to the microlens array);
Figure 589190DEST_PATH_IMAGE019
is the image distance of the microlens array;

目标模型P的一次成像点P’通过微透镜阵列,在不同的微透镜下再次成像为像点P i ”。一次成像点P’在微透镜阵列的投影区域为一个圆域,该圆域的中心为一次成像点P’在微透镜阵列面的投影点,该圆域的半径取决于一次成像点P’的虚深度

Figure 770772DEST_PATH_IMAGE020
,满足关系:The primary imaging point P' of the target model P passes through the microlens array and is re-imaged as an image point P i " under different microlenses. The primary imaging point P' in the projection area of the microlens array is a circular domain, and the The center is the projection point of the primary imaging point P' on the microlens array surface, and the radius of the circle depends on the virtual depth of the primary imaging point P'
Figure 770772DEST_PATH_IMAGE020
, which satisfies the relation:

Figure 507915DEST_PATH_IMAGE021
(2)
Figure 507915DEST_PATH_IMAGE021
(2)

式中,

Figure 407738DEST_PATH_IMAGE022
为一次成像点在微透镜阵列上的投影圆域的半径;
Figure 239428DEST_PATH_IMAGE023
为虚深度;
Figure 275517DEST_PATH_IMAGE024
为微透镜口径;In the formula,
Figure 407738DEST_PATH_IMAGE022
is the radius of the projection circle of the primary imaging point on the microlens array;
Figure 239428DEST_PATH_IMAGE023
is the virtual depth;
Figure 275517DEST_PATH_IMAGE024
is the diameter of the microlens;

每个微透镜阵列中微透镜为一个独立的相机,则虚深度

Figure 432829DEST_PATH_IMAGE025
由双目视觉经典算法计算:The microlens in each microlens array is an independent camera, then the virtual depth
Figure 432829DEST_PATH_IMAGE025
Calculated by the classic binocular vision algorithm:

Figure 397112DEST_PATH_IMAGE026
(3)
Figure 397112DEST_PATH_IMAGE026
(3)

式中,

Figure 501334DEST_PATH_IMAGE027
为虚深度;
Figure 188667DEST_PATH_IMAGE028
为一次成像点在微透镜阵列上的投影圆域中两个最远微透镜之间包含微透镜的数量;
Figure 985722DEST_PATH_IMAGE004
为微透镜口径;
Figure 860137DEST_PATH_IMAGE029
为两个最远微透镜中配准二次成像点间的欧氏距离;In the formula,
Figure 501334DEST_PATH_IMAGE027
is the virtual depth;
Figure 188667DEST_PATH_IMAGE028
is the number of microlenses contained between the two farthest microlenses in the projection circle of the microlens array for one imaging point;
Figure 985722DEST_PATH_IMAGE004
is the diameter of the microlens;
Figure 860137DEST_PATH_IMAGE029
is the Euclidean distance between the registered secondary imaging points in the two most distant microlenses;

由于微透镜口径

Figure 33629DEST_PATH_IMAGE030
是已知的,而一次成像点在微透镜阵列上的投影圆域的半径
Figure 575469DEST_PATH_IMAGE031
可通过聚焦型光场相机探测获得,则根据公式(2)可计算获得虚深度
Figure 543425DEST_PATH_IMAGE020
。Due to the diameter of the microlens
Figure 33629DEST_PATH_IMAGE030
is known, and the radius of the projection circle of the primary imaging point on the microlens array
Figure 575469DEST_PATH_IMAGE031
can be detected by a focusing light field camera, then the virtual depth can be calculated according to formula (2)
Figure 543425DEST_PATH_IMAGE020
.

由于微透镜阵列的像距

Figure 718186DEST_PATH_IMAGE032
是已知的,则根据虚深度
Figure 164211DEST_PATH_IMAGE033
以及公式(1),即可得到一次成像点P’到微透镜阵列的实际距离
Figure 560557DEST_PATH_IMAGE034
。Due to the image distance of the microlens array
Figure 718186DEST_PATH_IMAGE032
is known, then according to the imaginary depth
Figure 164211DEST_PATH_IMAGE033
and formula (1), the actual distance from the primary imaging point P' to the microlens array can be obtained
Figure 560557DEST_PATH_IMAGE034
.

设微透镜阵列到主透镜主面距离为

Figure 699414DEST_PATH_IMAGE035
,则目标模型距离光场探测单元的距离为:The distance from the microlens array to the main surface of the main lens is set as
Figure 699414DEST_PATH_IMAGE035
, the distance between the target model and the light field detection unit is:

Figure 814001DEST_PATH_IMAGE036
(4)
Figure 814001DEST_PATH_IMAGE036
(4)

式中,

Figure 63716DEST_PATH_IMAGE037
为目标模型距离光场探测装置的距离;
Figure 626154DEST_PATH_IMAGE038
为光场探测装置的主透镜焦距;
Figure 935912DEST_PATH_IMAGE039
为光场探测单元的微透镜阵列的物距;
Figure 537795DEST_PATH_IMAGE009
为微透镜阵列的像距;
Figure 591202DEST_PATH_IMAGE040
为微透镜阵列到主透镜主面的距离;In the formula,
Figure 63716DEST_PATH_IMAGE037
is the distance from the target model to the light field detection device;
Figure 626154DEST_PATH_IMAGE038
is the focal length of the main lens of the light field detection device;
Figure 935912DEST_PATH_IMAGE039
is the object distance of the microlens array of the light field detection unit;
Figure 537795DEST_PATH_IMAGE009
is the image distance of the microlens array;
Figure 591202DEST_PATH_IMAGE040
is the distance from the microlens array to the main surface of the main lens;

进一步分析可知,目标模型P的一次像点P’与观测该一次像点P’的某个微透镜

Figure 696561DEST_PATH_IMAGE041
之间的相对位置关系决定一条由P’射向
Figure 177221DEST_PATH_IMAGE042
的光线
Figure 751553DEST_PATH_IMAGE043
(一条光线代表一个方向),而
Figure 608650DEST_PATH_IMAGE044
的子图像中二次成像点P i ”的强度则代表了入射光线(入射光线指入射到聚焦型光场相机内的光线)在
Figure 630833DEST_PATH_IMAGE045
方向的辐射强度,在聚焦型光场相机结构中,一次成像点P’发射的光线可由其投影圆域内的多个微透镜记录,找出一次成像点P’在这些微透镜下的二次成像点P i ”的位置就得到了回波强度在方向上的分布特性。将目标模型P的所有二次成像点P i ”的像素强度相加,则得到了光场探测单元视场内目标模型的总回波辐射强度为:Further analysis shows that the primary image point P' of the target model P and a certain microlens that observes the primary image point P'
Figure 696561DEST_PATH_IMAGE041
The relative positional relationship between determines a line directed by P'
Figure 177221DEST_PATH_IMAGE042
of light
Figure 751553DEST_PATH_IMAGE043
(a ray represents a direction), while
Figure 608650DEST_PATH_IMAGE044
The intensity of the secondary imaging point P i ″ in the sub-image represents the incident light (incident light refers to the light incident into the focusing light field camera)
Figure 630833DEST_PATH_IMAGE045
The radiation intensity in the direction, in the focusing light field camera structure, the light emitted by the primary imaging point P' can be recorded by multiple microlenses in its projection circle, and the secondary imaging of the primary imaging point P' under these microlenses can be found. The position of the point P i ″ can obtain the distribution characteristics of the echo intensity in the direction. The pixel intensities of all the secondary imaging points P i ″ of the target model P are added, and the target model in the field of view of the light field detection unit is obtained. The total echo radiation intensity of is:

Figure 282394DEST_PATH_IMAGE046
(5)
Figure 282394DEST_PATH_IMAGE046
(5)

式中,

Figure 858869DEST_PATH_IMAGE047
为光场探测单元视场内目标模型的总回波辐射强度;
Figure 786503DEST_PATH_IMAGE048
为二次成像点的像素强度;
Figure 335296DEST_PATH_IMAGE050
为一次成像点与微透镜阵列中某个微透镜连线的方向;
Figure 751234DEST_PATH_IMAGE051
为微透镜数量。In the formula,
Figure 858869DEST_PATH_IMAGE047
is the total echo radiation intensity of the target model in the field of view of the light field detection unit;
Figure 786503DEST_PATH_IMAGE048
is the pixel intensity of the secondary imaging point;
Figure 335296DEST_PATH_IMAGE050
is the direction of the connection between the primary imaging point and a microlens in the microlens array;
Figure 751234DEST_PATH_IMAGE051
is the number of microlenses.

本实施例中,步骤104具体包括:In this embodiment, step 104 specifically includes:

401:聚焦型光场相机的数据初始化;401: Data initialization of the focusing light field camera;

数据初始化的目的在于对微透镜渐晕像差进行补偿,然后对初始化后的光场原始数据(原始数据即指原始图像)进行特征点标记,被标记的特征点为目标模型的几何结构特征点或纹理特征点,这些特征点对应了能够计算出回波信息的所有目标模型;The purpose of data initialization is to compensate the vignetting aberration of the microlens, and then mark the feature points of the initialized light field original data (original data refers to the original image), and the marked feature points are the geometric structure feature points of the target model. Or texture feature points, these feature points correspond to all target models that can calculate echo information;

402:根据被标记的特征点,在所述特征点的局部域内进行特征点配准,找出同一目标模型的所有二次成像点及其对应的微透镜;402: According to the marked feature points, perform feature point registration in the local domain of the feature points, and find out all secondary imaging points of the same target model and their corresponding microlenses;

403:利用光场解码算法计算目标模型距离光场探测装置的距离;403: Use the light field decoding algorithm to calculate the distance between the target model and the light field detection device;

根据公式(4)计算目标模型距离光场探测装置的距离

Figure 18267DEST_PATH_IMAGE052
;Calculate the distance between the target model and the light field detection device according to formula (4)
Figure 18267DEST_PATH_IMAGE052
;

404:记录同一目标模型在所有微透镜下的子图像像素强度,并将所有的子图像像素强度相加,得到该目标模型的总回波辐射强度;404: Record the sub-image pixel intensities of the same target model under all microlenses, and add all sub-image pixel intensities to obtain the total echo radiation intensity of the target model;

405:根据目标模型的总回波辐射强度,采用有限域插值法,获得聚焦型光场相机的全视场深度图和目标模型的全局辐亮度分布图。405 : According to the total echo radiation intensity of the target model, a finite field interpolation method is used to obtain a full-field depth map of the focusing light field camera and a global radiance distribution map of the target model.

全局辐亮度分布图即指回波辐射强度以及目标模型的辐射方向分布特性。The global radiance distribution map refers to the echo radiation intensity and the radiation direction distribution characteristics of the target model.

实施例1Example 1

本实施例提供一种针对复杂目标的激光照明回波探测装置,包括激光器、起偏器2、空间光调制器3、半反半透镜4、扩束单元5、目标模型6、聚焦型光场相机以及控制单元8;This embodiment provides a laser illumination echo detection device for complex targets, including a laser, a polarizer 2, a spatial light modulator 3, a half mirror and a half mirror 4, a beam expander 5, a target model 6, and a focusing light field a camera and a control unit 8;

扩束单元5包括同轴的次镜51和主镜52,次镜51的半径小于主镜52的半径,次镜51与主镜52之间的距离可调节;The beam expander unit 5 includes a coaxial secondary mirror 51 and a primary mirror 52, the radius of the secondary mirror 51 is smaller than the radius of the primary mirror 52, and the distance between the secondary mirror 51 and the primary mirror 52 is adjustable;

聚焦型光场相机包括主透镜71和微透镜阵列72。The focusing type light field camera includes a main lens 71 and a microlens array 72 .

空间光调制器3与扩束单元5中次镜51之间的距离远大于

Figure 482747DEST_PATH_IMAGE053
,其中
Figure 151625DEST_PATH_IMAGE054
为激光器提供的入射光束的半径,
Figure 426880DEST_PATH_IMAGE055
为入射光束波长。The distance between the spatial light modulator 3 and the secondary mirror 51 in the beam expander unit 5 is much greater than
Figure 482747DEST_PATH_IMAGE053
,in
Figure 151625DEST_PATH_IMAGE054
the radius of the incident beam provided to the laser,
Figure 426880DEST_PATH_IMAGE055
is the wavelength of the incident beam.

激光器发射直径为2mm的窄束激光(即入射光束),波长为808nm,入射光束经起偏器2入射至空间光调制器3,空间光调制器3在控制单元8控制下对该入射光束进行调制,得到具有特定局域强度分布模式的出射光束,该出射光束传播5m后穿过半反半透镜4,由扩束单元5对该出射光束进行扩束,扩束后获得的照明光斑尺寸约为30cm,目标模型6尺寸为25cm,因此照明光斑能够覆盖目标模型6。目标模型6在电动云台控制下可做位移和旋转运动。目标模型6的反射和散射回波信号经扩束单元5的主镜52收集后,由次镜51出射,再经半反半透镜4反射后进入聚焦型光场相机,聚焦型光场相机对回波信号进行探测,并将探测获得的数据实时传送至控制单元8;The laser emits a narrow beam of laser light with a diameter of 2mm (that is, an incident beam) and a wavelength of 808nm. The incident beam is incident on the spatial light modulator 3 through the polarizer 2, and the spatial light modulator 3 is controlled by the control unit 8. Modulation to obtain an outgoing beam with a specific local intensity distribution pattern, the outgoing beam propagates 5m and passes through the semi-reflective semi-mirror 4, and the outgoing beam is expanded by the beam expanding unit 5, and the illumination spot size obtained after beam expansion is about 30cm, the size of the target model 6 is 25cm, so the illumination spot can cover the target model 6. The target model 6 can perform displacement and rotation movements under the control of the electric PTZ. After the reflected and scattered echo signals of the target model 6 are collected by the primary mirror 52 of the beam expander unit 5, they are emitted by the secondary mirror 51, and then reflected by the half mirror and half mirror 4, and then enter the focusing light field camera. The echo signal is detected, and the data obtained by the detection is transmitted to the control unit 8 in real time;

控制单元8利用光场解码算法对探测获得的数据进行解码,获得目标距离、回波辐射强度以及辐射方向分布特性;同时,控制单元8根据回波辐射强度以及辐射方向分布特性实时控制空间光调制器3对入射光束的强度分布调制。The control unit 8 uses the light field decoding algorithm to decode the data obtained by the detection, and obtains the target distance, the echo radiation intensity and the radiation direction distribution characteristics; meanwhile, the control unit 8 controls the spatial light modulation in real time according to the echo radiation intensity and the radiation direction distribution characteristics. The intensity distribution of the incident beam is modulated by the device 3.

以上所述仅为本发明的优选实施例,并非因此限制本发明的专利范围,凡是在本发明的发明构思下,利用本发明说明书及附图内容所作的等效结构变换,或直接/间接运用在其他相关的技术领域均包括在本发明的专利保护范围内。The above descriptions are only preferred embodiments of the present invention, and are not intended to limit the scope of the present invention. Under the inventive concept of the present invention, any equivalent structural transformations made by the contents of the description and drawings of the present invention, or direct/indirect application Other related technical fields are included in the scope of patent protection of the present invention.

Claims (10)

1.一种针对复杂目标的激光照明回波探测装置,其特征在于,所述激光照明回波探测装置包括初始光源、空间光调制器、半反半透镜、扩束单元、光场探测单元以及控制单元;1. A laser illumination echo detection device for complex targets, characterized in that the laser illumination echo detection device comprises an initial light source, a spatial light modulator, a half mirror, a beam expanding unit, a light field detection unit and control unit; 所述初始光源用于提供入射光束;the initial light source is used to provide the incident light beam; 所述空间光调制器接收所述入射光束并对所述入射光束进行强度分布调制,得到具有设定局域强度分布模式的出射光束;The spatial light modulator receives the incident light beam and modulates the intensity distribution of the incident light beam to obtain an outgoing light beam with a set local intensity distribution pattern; 所述扩束单元接收从所述半反半透镜透过的所述出射光束,并对所述出射光束进行扩束,获得覆盖整个目标模型的照明光斑;The beam expanding unit receives the outgoing beam transmitted through the semi-reflective semi-mirror, and expands the outgoing beam to obtain an illumination spot covering the entire target model; 所述扩束单元接收所述照明光斑照射所述目标模型后产生的回波信号,并将所述回波信号射出;The beam expander unit receives an echo signal generated after the illumination spot illuminates the target model, and emits the echo signal; 所述半反半透镜将所述回波信号反射进入所述光场探测单元;The semi-reflective semi-mirror reflects the echo signal into the light field detection unit; 所述光场探测单元对所述回波信号进行探测,并将所述探测获得的数据实时传送至所述控制单元;The light field detection unit detects the echo signal, and transmits the data obtained by the detection to the control unit in real time; 所述控制单元利用光场解码算法对所述探测获得的数据进行解码,获得目标距离、回波辐射强度以及辐射方向分布特性;同时,所述控制单元根据所述回波辐射强度以及所述辐射方向分布特性实时控制所述空间光调制器对所述入射光束的强度分布调制。The control unit decodes the data obtained by the detection by using the light field decoding algorithm to obtain the target distance, echo radiation intensity and radiation direction distribution characteristics; The directional distribution characteristic controls the intensity distribution modulation of the incident light beam by the spatial light modulator in real time. 2.如权利要求1所述的针对复杂目标的激光照明回波探测装置,其特征在于,所述激光照明回波探测装置还包括起偏器,所述起偏器设置在所述初始光源与所述空间光调制器之间,用于从所述初始光源射出的入射光束中获得偏振光并将所述偏振光输入所述空间光调制器中。2 . The laser illumination echo detection device for complex targets according to claim 1 , wherein the laser illumination echo detection device further comprises a polarizer, and the polarizer is arranged between the initial light source and the initial light source. 3 . between the spatial light modulators, for obtaining polarized light from the incident light beam emitted from the initial light source and inputting the polarized light into the spatial light modulator. 3.如权利要求1所述的针对复杂目标的激光照明回波探测装置,其特征在于,所述扩束单元包括同轴的次镜和主镜,所述次镜的半径小于所述主镜的半径,所述次镜与所述主镜之间的距离可调节;3 . The laser illumination echo detection device for complex targets according to claim 1 , wherein the beam expanding unit comprises a coaxial secondary mirror and a primary mirror, and the radius of the secondary mirror is smaller than that of the primary mirror. 4 . The radius of , the distance between the secondary mirror and the primary mirror can be adjusted; 所述出射光束经所述次镜收集后进入所述扩束单元,由所述主镜射出并照射所述目标模型。The outgoing beam is collected by the secondary mirror and then enters the beam expander unit, and is emitted by the primary mirror to illuminate the target model. 4.如权利要求1所述的针对复杂目标的激光照明回波探测装置,其特征在于,所述光场探测单元为聚焦型光场相机;4. The laser illumination echo detection device for complex targets according to claim 1, wherein the light field detection unit is a focusing light field camera; 所述聚焦型光场相机包括主透镜和微透镜阵列,目标模型在所述主透镜下形成一次成像点,所述一次成像点通过所述微透镜阵列并在所述微透镜阵列的不同微透镜下再次成像形成多个二次成像点;多个所述二次成像点的像素即为探测获得的数据。The focusing light field camera includes a main lens and a microlens array, and the target model forms a primary imaging point under the main lens, and the primary imaging point passes through the microlens array and is located in different microlenses of the microlens array. Next, imaging again forms a plurality of secondary imaging points; the pixels of the plurality of secondary imaging points are the data obtained by detection. 5.如权利要求1所述的针对复杂目标的激光照明回波探测装置,其特征在于,所述目标模型安装在电动云台上,所述电动云台在所述控制单元的控制下带动所述目标模型旋转和移动。5 . The laser illumination echo detection device for complex targets according to claim 1 , wherein the target model is installed on an electric pan/tilt head, and the electric pan/tilt head drives all the objects under the control of the control unit. 6 . Describe the target model rotation and movement. 6.如权利要求1所述的针对复杂目标的激光照明回波探测装置,其特征在于,所述空间光调制器与所述扩束单元之间的距离大于
Figure 584117DEST_PATH_IMAGE001
,其中
Figure 920420DEST_PATH_IMAGE002
为所述入射光束的半径,
Figure 973827DEST_PATH_IMAGE003
为入射光束的波长。
6 . The laser illumination echo detection device for complex targets according to claim 1 , wherein the distance between the spatial light modulator and the beam expanding unit is greater than
Figure 584117DEST_PATH_IMAGE001
,in
Figure 920420DEST_PATH_IMAGE002
is the radius of the incident beam,
Figure 973827DEST_PATH_IMAGE003
is the wavelength of the incident beam.
7.一种针对复杂目标的激光照明回波探测方法,其特征在于,所述激光照明回波探测方法包括:7. A laser illumination echo detection method for complex targets, wherein the laser illumination echo detection method comprises: 利用空间光调制器接收初始光源提供的入射光束,并利用所述空间光调制器对所述入射光束进行强度分布调制,得到具有设定局域强度分布模式的出射光束;Using the spatial light modulator to receive the incident light beam provided by the initial light source, and using the spatial light modulator to perform intensity distribution modulation on the incident light beam to obtain an outgoing light beam with a set local intensity distribution pattern; 利用扩束单元对所述出射光束进行扩束,获得覆盖整个目标模型的照明光斑;The outgoing beam is expanded by a beam expansion unit to obtain an illumination spot covering the entire target model; 利用扩束单元接收所述照明光斑照射所述目标模型后产生的回波信号,并将所述回波信号射出;Using a beam expander unit to receive the echo signal generated by the illumination spot irradiating the target model, and to emit the echo signal; 利用半反半透镜将所述回波信号反射进入光场探测单元;Using a half mirror to reflect the echo signal into the light field detection unit; 利用所述光场探测单元对所述回波信号进行探测,获得探测数据;Use the light field detection unit to detect the echo signal to obtain detection data; 利用控制单元对所述探测数据进行解码,获得目标距离、回波辐射强度以及辐射方向分布特性;Use the control unit to decode the detection data to obtain the target distance, echo radiation intensity and radiation direction distribution characteristics; 根据所述回波辐射强度以及所述辐射方向分布特性,判断所述目标模型的总回波辐射强度是否达到最大,若达到,则输出目标距离、所述空间光调制器的调制相位分布、出射光束的光强分布、所述目标模型的姿态、所述回波辐射强度以及所述辐射方向分布特性;否则通过所述控制单元调整所述空间光调制器的调制相位,直至获得的所述目标模型的总回波辐射强度达到最大。According to the echo radiation intensity and the distribution characteristics of the radiation direction, it is judged whether the total echo radiation intensity of the target model reaches the maximum, and if so, output the target distance, the modulation phase distribution of the spatial light modulator, and the output The light intensity distribution of the beam, the attitude of the target model, the echo radiation intensity, and the radiation direction distribution characteristics; otherwise, the modulation phase of the spatial light modulator is adjusted by the control unit until the target is obtained. The total echo radiation intensity of the model is at its maximum. 8.如权利要求7所述的针对复杂目标的激光照明回波探测方法,其特征在于,利用空间光调制器接收初始光源提供的入射光束,并利用所述空间光调制器对所述入射光束进行强度分布调制,得到具有设定局域强度分布模式的出射光束,包括:8 . The laser illumination echo detection method for complex targets according to claim 7 , wherein a spatial light modulator is used to receive the incident beam provided by the initial light source, and the spatial light modulator is used to detect the incident beam. 9 . Perform intensity distribution modulation to obtain an outgoing beam with a set local intensity distribution pattern, including: 利用起偏器从初始光源提供的入射光束获得偏振光并将所述偏振光输入空间光调制器中;obtaining polarized light from an incident beam provided by an initial light source using a polarizer and inputting the polarized light into a spatial light modulator; 利用所述空间光调制器对所述偏振光进行强度分布调制,得到具有设定局域强度分布模式的出射光束。The intensity distribution of the polarized light is modulated by the spatial light modulator to obtain an outgoing light beam with a set local intensity distribution pattern. 9.如权利要求7所述的针对复杂目标的激光照明回波探测方法,其特征在于,利用扩束单元对所述出射光束进行扩束,获得覆盖整个目标模型的照明光斑,包括:9. The laser illumination echo detection method for complex targets as claimed in claim 7, wherein the beam expanding unit is used to expand the outgoing beam to obtain an illumination spot covering the entire target model, comprising: 调整扩束单元以使从所述扩束单元射出的照明光斑覆盖整个目标模型;Adjusting the beam expander unit so that the illumination spot emitted from the beam expander unit covers the entire target model; 利用调整好的所述扩束单元对所述出射光束进行扩束,获得覆盖整个目标模型的照明光斑。The outgoing beam is expanded by the adjusted beam expanding unit to obtain an illumination spot covering the entire target model. 10.如权利要求7所述的针对复杂目标的激光照明回波探测方法,其特征在于,所述光场探测单元为聚焦型光场相机;所述聚焦型光场相机包括主透镜和微透镜阵列,目标模型在所述主透镜下形成一次成像点,所述一次成像点通过所述微透镜阵列并在所述微透镜阵列的不同微透镜下再次成像形成多个二次成像点;多个所述二次成像点的像素即为探测获得的数据;10. The laser illumination echo detection method for complex targets according to claim 7, wherein the light field detection unit is a focusing light field camera; the focusing light field camera comprises a main lens and a microlens array, the target model forms a primary imaging point under the main lens, and the primary imaging point passes through the microlens array and is imaged again under different microlenses of the microlens array to form a plurality of secondary imaging points; a plurality of secondary imaging points; The pixel of the secondary imaging point is the data obtained by detection; 利用控制单元对所述探测数据进行解码,获得目标距离、回波辐射强度以及辐射方向分布特性,包括:Use the control unit to decode the detection data to obtain the target distance, echo radiation intensity and radiation direction distribution characteristics, including: 利用所述控制单元内的光场解码算法对所述探测数据进行数据处理,所述光场解码算法用虚深度描述所述一次成像点与所述微透镜阵列之间的规范化距离:The detection data is processed by the light field decoding algorithm in the control unit, and the light field decoding algorithm describes the normalized distance between the primary imaging point and the microlens array with virtual depth:
Figure 344766DEST_PATH_IMAGE004
(1)
Figure 344766DEST_PATH_IMAGE004
(1)
式中,
Figure 825426DEST_PATH_IMAGE005
为虚深度;
Figure 196495DEST_PATH_IMAGE006
为微透镜阵列的物距;
Figure 53593DEST_PATH_IMAGE007
为微透镜阵列的像距;
In the formula,
Figure 825426DEST_PATH_IMAGE005
is the virtual depth;
Figure 196495DEST_PATH_IMAGE006
is the object distance of the microlens array;
Figure 53593DEST_PATH_IMAGE007
is the image distance of the microlens array;
所述一次成像点在所述微透镜阵列的投影区域为一个圆域,所述圆域的中心为所述一次成像点在所述微透镜阵列面的投影点,所述圆域的半径取决于所述一次成像点的虚深度,满足关系:The projection area of the primary imaging point on the microlens array is a circular domain, the center of the circular domain is the projection point of the primary imaging point on the microlens array surface, and the radius of the circular domain depends on The virtual depth of the primary imaging point satisfies the relationship:
Figure 13458DEST_PATH_IMAGE008
(2)
Figure 13458DEST_PATH_IMAGE008
(2)
式中,
Figure 665020DEST_PATH_IMAGE009
为一次成像点在微透镜阵列上的投影圆域的半径;
Figure 241494DEST_PATH_IMAGE010
为虚深度;
Figure 213867DEST_PATH_IMAGE011
为微透镜口径;
In the formula,
Figure 665020DEST_PATH_IMAGE009
is the radius of the projection circle of the primary imaging point on the microlens array;
Figure 241494DEST_PATH_IMAGE010
is the virtual depth;
Figure 213867DEST_PATH_IMAGE011
is the diameter of the microlens;
每个所述微透镜阵列中微透镜为一个独立的相机,则所述虚深度由双目视觉经典算法计算:The microlens in each of the microlens arrays is an independent camera, and the virtual depth is calculated by the classic binocular vision algorithm:
Figure 762660DEST_PATH_IMAGE012
(3)
Figure 762660DEST_PATH_IMAGE012
(3)
式中,
Figure 381861DEST_PATH_IMAGE013
为虚深度;
Figure 648894DEST_PATH_IMAGE014
为一次成像点在微透镜阵列上的投影圆域中两个最远微透镜之间包含微透镜的数量;
Figure 113373DEST_PATH_IMAGE015
为微透镜口径;
Figure 516673DEST_PATH_IMAGE016
为两个最远微透镜中配准二次成像点间的欧氏距离;
In the formula,
Figure 381861DEST_PATH_IMAGE013
is the virtual depth;
Figure 648894DEST_PATH_IMAGE014
is the number of microlenses contained between the two farthest microlenses in the projection circle of the microlens array for one imaging point;
Figure 113373DEST_PATH_IMAGE015
is the diameter of the microlens;
Figure 516673DEST_PATH_IMAGE016
is the Euclidean distance between the registered secondary imaging points in the two most distant microlenses;
所述目标模型距离所述光场探测单元的距离为:The distance between the target model and the light field detection unit is:
Figure 57507DEST_PATH_IMAGE017
(4)
Figure 57507DEST_PATH_IMAGE017
(4)
式中,
Figure 811836DEST_PATH_IMAGE018
为目标模型距离光场探测装置的距离;
Figure 876744DEST_PATH_IMAGE019
为光场探测装置的主透镜焦距;
Figure 931288DEST_PATH_IMAGE020
为光场探测单元的微透镜阵列的物距;
Figure 361132DEST_PATH_IMAGE021
为微透镜阵列的像距;
Figure 857884DEST_PATH_IMAGE022
为微透镜阵列到主透镜主面的距离;
In the formula,
Figure 811836DEST_PATH_IMAGE018
is the distance from the target model to the light field detection device;
Figure 876744DEST_PATH_IMAGE019
is the focal length of the main lens of the light field detection device;
Figure 931288DEST_PATH_IMAGE020
is the object distance of the microlens array of the light field detection unit;
Figure 361132DEST_PATH_IMAGE021
is the image distance of the microlens array;
Figure 857884DEST_PATH_IMAGE022
is the distance from the microlens array to the main surface of the main lens;
所述光场探测单元视场内目标模型的总回波辐射强度为:The total echo radiation intensity of the target model in the field of view of the light field detection unit is:
Figure 398587DEST_PATH_IMAGE023
(5)
Figure 398587DEST_PATH_IMAGE023
(5)
式中,
Figure 369954DEST_PATH_IMAGE024
为光场探测单元视场内目标模型的总回波辐射强度;
Figure DEST_PATH_IMAGE025
为二次成像点的像素强度;
Figure 705121DEST_PATH_IMAGE026
为一次成像点与微透镜阵列中某个微透镜连线的方向;
Figure DEST_PATH_IMAGE027
为微透镜数量。
In the formula,
Figure 369954DEST_PATH_IMAGE024
is the total echo radiation intensity of the target model in the field of view of the light field detection unit;
Figure DEST_PATH_IMAGE025
is the pixel intensity of the secondary imaging point;
Figure 705121DEST_PATH_IMAGE026
is the direction of the connection between the primary imaging point and a microlens in the microlens array;
Figure DEST_PATH_IMAGE027
is the number of microlenses.
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