阅读说明：本技术 一种基于螺旋谱的目标成像方法和装置 (Target imaging method and device based on spiral spectrum ) 是由 任元 陈琳琳 刘通 陈晓岑 于 2020-05-12 设计创作，主要内容包括：本发明涉及一种基于螺旋谱的目标成像方法和装置。它的主要部件包括激光器、单模保偏光纤、准直扩束透镜组、接收光学天线、准直透镜、窄带滤波片、凸透镜、偏振分光棱镜、空间光调制器、螺旋谱测量装置、系统控制器。首先,激光器发射的激光经准直扩束系统出射平面波照射目标；经过目标物体反射后,被接收光学天线接收；其次,接收光学天线接收的回波信号被准直透镜组准直,压缩入射角,然后经窄带滤波片投射到4f成像透镜系统,然后垂直入射反射式空间光调制器；最后,空间光调制器出射光经过偏振分光棱镜入射准直透镜并耦合进入单模保偏光纤,到达螺旋谱测量装置得到强度螺旋谱和相位螺旋谱分布,通过强度螺旋谱和相位螺旋谱的叠加,重构目标物体的形貌。本发明方法通过测量反射光螺旋谱的空间分布,能够实现对目标形貌的瞬时高分辨率成像。(The invention relates to a target imaging method and device based on a spiral spectrum. The main components of the device comprise a laser, a single-mode polarization maintaining optical fiber, a collimation and beam expanding lens group, a receiving optical antenna, a collimating lens, a narrow-band filter, a convex lens, a polarization beam splitting prism, a spatial light modulator, a spiral spectrum measuring device and a system controller. Firstly, emitting plane waves to irradiate a target by laser emitted by a laser through a collimation beam expanding system; after being reflected by the target object, the target object is received by the receiving optical antenna; secondly, the echo signals received by the receiving optical antenna are collimated by a collimating lens group, the incident angle is compressed, then the echo signals are projected to a 4f imaging lens system through a narrow-band filter, and then the echo signals are vertically incident to a reflective spatial light modulator; and finally, emergent light of the spatial light modulator enters the collimating lens through the polarization beam splitter prism and is coupled into the single-mode polarization maintaining fiber, the emergent light reaches the spiral spectrum measuring device to obtain intensity spiral spectrum and phase spiral spectrum distribution, and the appearance of the target object is reconstructed through superposition of the intensity spiral spectrum and the phase spiral spectrum. The method can realize instantaneous high-resolution imaging of the target morphology by measuring the spatial distribution of the spiral spectrum of the reflected light.)

1. The invention relates to a target imaging method and a device based on a spiral spectrum, which comprises the following steps: the device comprises a laser (1), a single-mode polarization-maintaining optical fiber 1(2), a collimation and beam expansion lens group (3), a receiving optical antenna (4), a collimating lens 1(5), a narrow-band filter (6), a convex lens 1(7), a polarization beam splitter prism (8), a convex lens 2(9), a spatial light modulator (10), a collimating lens 2(11), a single-mode polarization-maintaining optical fiber 2(12), a spiral spectrum measuring device (13) and a system controller (14).

2. The method and device for target imaging based on helical spectrum according to claim 1, wherein: firstly, emitting plane waves to irradiate a target by laser emitted by a laser through a collimation beam expanding system; after being reflected by the target object, the target object is received by the receiving optical antenna; secondly, the echo signals received by the receiving optical antenna are collimated by a collimating lens group, the incident angle is compressed, then the echo signals are projected to a 4f imaging lens system through a narrow-band filter, and then the echo signals are vertically incident to a reflective spatial light modulator; and finally, emergent light of the spatial light modulator enters the collimating lens through the polarization beam splitter prism and is coupled into the single-mode polarization maintaining fiber, the emergent light reaches the spiral spectrum measuring device to obtain intensity spiral spectrum and phase spiral spectrum distribution, and the appearance of the object is reconstructed through superposition of the intensity spiral spectrum and the phase spiral spectrum.

3. A method and apparatus for object imaging based on vortex-induced rotation helical spectroscopy according to claim 1 and claim 2, wherein: the echo signal is composed of convex lenses 1 and 7 and convex lenses 2 and 9 through a 4f imaging lens system, then enters a spatial light modulator, phase information and intensity information of the echo signal are obtained through demodulation of the spatial light modulator, and then the intensity spiral spectrum and phase spiral spectrum distribution of the echo signal are obtained through direct analysis of a spiral spectrum measuring device.

Technical Field

The invention mainly relates to the fields of optics, physics, photoelectric conversion, signal detection and optical imaging, in particular to technical methods for modulating and demodulating optical signals and the like.

Background

The terahertz wave band is used as a section of electromagnetic spectrum which is not used on a large scale, and has great application value in the aspects of security inspection and security, space communication, biomedical detection and nondestructive detection of materials. The terahertz imaging technology is one of the most promising technologies in the terahertz technology. The terahertz wave can penetrate most nonpolar materials, so the terahertz wave is particularly suitable for the situations that other electromagnetic waves cannot penetrate and the X-ray contrast is low.

At present, the mainstream development trend of terahertz imaging is to use pulse terahertz imaging of a large-scale array detector to obtain a plurality of pixel points at one time, reduce or get rid of the dependence of an imaging system on a mechanical scanning device, and obtain the intensity and phase information of terahertz waves. Therefore, the imaging speed is a limiting factor of the practical application of the terahertz imaging technology.

Compared with pulse terahertz imaging, the terahertz wave intensity information and phase information can be obtained simultaneously through continuous wave imaging based on the spiral spectrum, the system is simple in structure, the number of required detectors is not high, rapid imaging can be achieved only through a single detector, and the cost of hardware is effectively reduced.

Disclosure of Invention

The invention solves the problems that: the method reconstructs the appearance of a target object by measuring the spatial distribution of a plane wave spiral spectrum, can realize instantaneous and high-resolution imaging, has a simple experimental device structure, can realize integration, and has wide application prospect in the field of instantaneous high-resolution imaging.

The technical solution of the invention is as follows: the invention relates to a target imaging method and a target imaging device based on a spiral spectrum, as shown in figure 1, the main components of the device comprise: the device comprises a laser (1), a single-mode polarization-maintaining optical fiber 1(2), a collimation and beam expansion lens group (3), a receiving optical antenna (4), a collimation lens group 1(5), a narrow-band filter (6), a convex lens 1(7), a polarization beam splitter prism (8), a convex lens 2(9), a spatial light modulator (10), a collimation lens group 2(11), a single-mode polarization-maintaining optical fiber 2(12), a spiral spectrum measuring device (13) and a system controller (14). Firstly, a laser (1) generates a laser beam, the laser beam is incident to a collimation and beam expansion lens group (3) through a single-mode polarization-maintaining optical fiber 1(2) and then is changed into parallel polarized light (plane beam), an imaging target to be detected is irradiated, and an echo signal is received by a receiving optical antenna (4) after being reflected by a target object; then, the echo signal received by the receiving optical antenna (4) is collimated by a collimating lens group (5), the incident angle is compressed, then the echo signal is projected to a 4f imaging lens system (a convex lens 1(7) and a convex lens 2(9)) through a narrow-band filter (6), and then the echo signal is demodulated by a vertical incidence reflective spatial light modulator (10) to obtain spatial information and intensity information; finally, the reflected light enters a collimating lens group 2(11) through a polarization beam splitter prism (8) and a 4f imaging lens system, is coupled into a second single-mode polarization-preserving fiber 2(12), reaches a spiral spectrum measuring device (13), is measured to obtain the intensity spiral spectrum and the phase spiral spectrum distribution of the echo signal, and reconstructs the appearance of the object by overlapping the intensity spiral spectrum and the phase spiral spectrum of the echo signal.

The principle of the invention is as follows:

standard imaging techniques extract information by transforming image features into intensity, phase, and frequency variations by polarization and spatial distribution of the input light. The input light may be gaussian or light having a particular intensity, polarization, or phase distribution. The digital spiral imaging technology is used for extracting information by converting the information into the change of the orbital angular momentum of the light beam.

As incident light, we describe a beam of Orbital Angular Momentum (OAM) as a function U. The transmission function of an object is denoted by T. The wave function of the incident light beam reflected (or transmitted) by the object and corresponding to the outgoing light beam is represented by O, and various information on the surface of the object is represented by a mathematical formula of O ═ T · U. The incident beam is a gaussian beam, OAM is 0, the corresponding orbital angular momentum spectrum only contains a columnar component with the orbital angular momentum quantum number l being 0, after passing through the object, the reflected beam of the orbital angular momentum spectrum does not only contain the component of 0, but also contains other various orbital angular momentum components, because the emergent beam is formed by the reflection or transmission of the object, and carries object information compared with the incident beam. Then, the relationship of each orbital angular momentum component of the emergent light beam is analyzed by the spiral spectrum measuring device in fig. 1, and the difference between the emergent light beam and the incident light beam is combined, so that the object image is restored, and the digital spiral imaging is completed. In this mechanism, it is necessary to obtain each orbital angular momentum component included in the light beam, which corresponds to spreading the light beam into a superposition of the respective orbital angular momentum components. Since orbital angular momentum corresponds to helical phase, this imaging technique is figuratively referred to as digital helical imaging.

In a quantum system, the wave function of any state can be expanded with a set of orthogonal perfect basis vectors, for example, eigenstates of orbital angular momentum can be used as a set of basis vectors. Any wave function can be developed as a sum of the superposition of the various orbital angular momentum components. In a cylindrical coordinate systemThen, the echo signal will be reflectedBased on the laguerre gaussian mode, the following is developed:

wherein A is_l,pThe amplitude of the two parameters with respect to l, p,is a laguerre-gaussian beam eigenstate expansion function.Is a helical spectrum of intensity, phi_l＝arg(A_l,p) Is a phase helical spectrum. The method is based on spatial light modulationThe system directly analyzes to obtain the distribution of the intensity spiral spectrum and the phase spiral spectrum of the echo signal, and reconstructs the appearance of the object by overlapping the intensity spiral spectrum and the phase spiral spectrum of the echo signal.

The invention has the main advantages that:

(1) the method and the device have the advantages of novel technology, simple light path, convenient operation and easy control.

(2) The method and the device enable echo signals to be incident on the spatial light modulator in a reflection mode, then the spatial light modulator is used for directly analyzing to obtain an intensity spiral spectrum and a phase spiral spectrum, and a target morphology is reconstructed.

(3) The method and the device can realize instantaneous and high-resolution imaging and have great application potential in the field of radar staring imaging.

Drawings

FIG. 1 is a schematic diagram of the subject imaging apparatus of the present method and apparatus;

FIG. 2 is a flow chart of the method and apparatus for imaging an object;

FIG. 3 is a schematic representation of an intensity spiral spectrum according to the present method;

FIG. 4 is a schematic diagram of a phase helical spectrum according to the present method.

Detailed Description

The invention takes a spiral spectrum as a detection information carrier, a target imaging flow chart is shown in figure 2, and the specific implementation steps are as follows:

firstly, a laser (1) generates a laser beam with the wavelength of 632.8nm, the laser beam is changed into parallel polarized light after passing through a single-mode polarization-maintaining optical fiber 1(2), and the parallel polarized light is changed into a plane beam with the spot diameter far larger than an object to be imaged after being incident on a collimation and beam expansion lens group (3).

The plane wave irradiates the target to be imaged, after being reflected by the surface of a target object, the target to be imaged is efficiently received by the large-caliber receiving optical antenna (4), and a primary image of the target to be imaged formed by the receiving optical antenna is positioned on a focal plane of the receiving optical antenna; the collimating lens group (5) and the receiving optical antenna (4) form a Kepler telescope system, and primary images of target objects to be imaged on a focal plane of the receiving optical antenna (4) are imaged at infinity.

The image is projected to a 4f imaging lens system (convex lens 1(7) and convex lens 2(9)) through a narrow-band filter (6), and then is demodulated by a vertical incidence reflective spatial light modulator (10) to obtain intensity information and phase information; finally, the reflected light passing through the spatial light modulator is imaged to a collimating lens group 2(11) through a polarization beam splitter prism (8) and a 4f imaging lens system, is coupled to a second single-mode polarization-preserving fiber 2(12), reaches a spiral spectrum measuring device (13) and is analyzed to obtain an echo signal intensity spiral spectrum as shown in fig. 3 and a phase spiral spectrum distribution as shown in fig. 4, and the appearance of the object is reconstructed by overlapping the intensity spiral spectrum and the phase spiral spectrum of the echo signal.

Those skilled in the art will appreciate that the invention may be practiced without these specific details.