CN110579875B - Laser defense system and method based on Hartmann focusing - Google Patents

Laser defense system and method based on Hartmann focusing Download PDF

Info

Publication number
CN110579875B
CN110579875B CN201910845977.6A CN201910845977A CN110579875B CN 110579875 B CN110579875 B CN 110579875B CN 201910845977 A CN201910845977 A CN 201910845977A CN 110579875 B CN110579875 B CN 110579875B
Authority
CN
China
Prior art keywords
focusing
hartmann
laser
mirror
main
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN201910845977.6A
Other languages
Chinese (zh)
Other versions
CN110579875A (en
Inventor
马晓燠
饶学军
杨奇龙
汪韬
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Chongqing Jiguang Technology Co.,Ltd.
Original Assignee
Chongqing Lianxin Photoelectric Technology Research Institute Co ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Chongqing Lianxin Photoelectric Technology Research Institute Co ltd filed Critical Chongqing Lianxin Photoelectric Technology Research Institute Co ltd
Priority to CN201910845977.6A priority Critical patent/CN110579875B/en
Publication of CN110579875A publication Critical patent/CN110579875A/en
Application granted granted Critical
Publication of CN110579875B publication Critical patent/CN110579875B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F41WEAPONS
    • F41HARMOUR; ARMOURED TURRETS; ARMOURED OR ARMED VEHICLES; MEANS OF ATTACK OR DEFENCE, e.g. CAMOUFLAGE, IN GENERAL
    • F41H11/00Defence installations; Defence devices
    • F41H11/02Anti-aircraft or anti-guided missile or anti-torpedo defence installations or systems
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F41WEAPONS
    • F41HARMOUR; ARMOURED TURRETS; ARMOURED OR ARMED VEHICLES; MEANS OF ATTACK OR DEFENCE, e.g. CAMOUFLAGE, IN GENERAL
    • F41H13/00Means of attack or defence not otherwise provided for
    • F41H13/0043Directed energy weapons, i.e. devices that direct a beam of high energy content toward a target for incapacitating or destroying the target
    • F41H13/005Directed energy weapons, i.e. devices that direct a beam of high energy content toward a target for incapacitating or destroying the target the high-energy beam being a laser beam
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00

Abstract

The invention provides a laser defense system and method based on Hartmann focusing, comprising the following steps: the device comprises a main mirror, a focusing secondary mirror, an inclined mirror, a beam splitter, a Hartmann sensor, a main laser emission system, an illumination system and a controller; the focusing secondary mirror is a part of an optical system and forms an optical receiving and transmitting system with the primary mirror, and the focusing secondary mirror is used as a main focusing executing device; the Hartmann sensor is used for detecting wave front inclination and defocusing, and the measurement result is used for an inclination closed loop and a defocusing correction closed loop. The current common image processing focusing mode is easily affected by ambient light, the focusing deviation and direction cannot be calculated quantitatively, the calculation amount of an algorithm is large, the convergence is poor, stable focusing cannot be achieved, and the target can escape due to long focusing time. The Hartmann sensor is adopted to replace an inclination tracking sensor to detect the wave front aberration, compared with an original image algorithm, the wave front aberration detection method is simple in calculation process and good in stability, and can quantitatively detect the wave front inclination and defocusing, so that rapid focusing is realized.

Description

Laser defense system and method based on Hartmann focusing
Technical Field
The invention relates to the technical field of light beam control in optical instruments, in particular to a laser defense system and a laser defense method based on Hartmann focusing.
Background
The unmanned plane is an unmanned plane controlled by radio remote control equipment and a self-contained program control device. In the 90 s of the 20 th century, western countries fully recognized the role of unmanned aerial vehicles in war, and adopted various new technologies to develop unmanned aerial vehicles vigorously. Nowadays, unmanned aerial vehicles have had multiple functions such as investigation, bullet, interference. Along with the continuous emergence of military and civilian unmanned aerial vehicle, anti-unmanned aerial vehicle consciousness can constantly promote for national security and national soil safety demand, and each country has earlier carried out the research work in this aspect. But adopt traditional means to combat unmanned aerial vehicle, not only the success rate is low, but also probably causes collateral damage to ground and crowd, and laser defense is one of more effective means.
In a laser defense system, the main laser destructive power is in positive correlation with the energy density of a light spot at a target, and the smaller the diameter of the light spot is, the stronger the laser destructive power is. And the accuracy of the focusing of the main laser emission system is a main factor influencing the size of the light spot. The current laser defense system adopts a focusing mode to focus through an image processing mode. The image processing focus is focused based on the size or gray scale of the light spot on the target. The focusing mode is easily influenced by ambient light, and the spot characteristics cannot be accurately extracted under complex light environments such as high contrast and the like; the focusing deviation and direction cannot be calculated quantitatively, and multiple iterations are needed; the algorithm has large calculation amount and poor convergence, which may cause that the focusing cannot be stabilized; the focusing time is long, which may cause the target to escape. Therefore, a new fast focusing method is needed in the laser defense system.
The patents of short-range laser defense system (201721280043.5), unmanned aerial vehicle laser weapon anti-unmanned aerial vehicle system (201811097389.0), laser defense system and high altitude airship (201710296422.1) adopt laser defense, but do not mention a focusing method. The patent 'a defense system of wanting ground based on strong laser of high accuracy dual wavelength' (201820945635.2) adopts the laser rangefinder's method to focus, compares traditional image focusing's mode fast a lot, but the system is complicated, and laser radar is with high costs. In China, a Hartmann sensor is not used for a laser defense focusing case. The invention adopts Hartmann to focus, and simultaneously realizes the inclined tracking, so that the system is more compact and the structure is simpler.
Disclosure of Invention
The technical problem of the invention is solved: the defects of the prior art are overcome, and the laser defense system based on Hartmann focusing is provided. As Hartmann can measure aberrations such as wavefront tilt and defocus, the tilt and defocus aberrations of the target are measured by introducing a low-order Hartmann sensor to replace a traditional position detection sensor, and target tracking and rapid focusing and striking of laser beams are realized.
In a first aspect, an embodiment of the present invention provides a laser defense system based on hartmann focusing, where the system specifically includes: the device comprises a main mirror, a focusing secondary mirror, an inclined mirror, a beam splitter, a Hartmann sensor, a main laser emission system, an illumination system and a controller; the received light is transmitted to a Hartmann sensor through the reflection of a main mirror, the reflection of a focusing secondary mirror, the reflection of an inclined mirror and a beam splitter in sequence; the emitted laser is transmitted out of the system through beam splitter reflection, inclined mirror reflection, focusing secondary mirror reflection and main mirror reflection in sequence;
the primary mirror is a part of the optical system and has a function of converging light beams;
the secondary focusing mirror is a part of an optical system and forms an optical receiving and transmitting system with the primary mirror, the secondary focusing mirror is used as a main focusing executing device, and the focusing amount is measured by the Hartmann;
the tilting mirror plays a role in beam tilt correction in an optical path, tilt correction is carried out on a received optical signal in real time by calculating a correction quantity obtained by calculating a tilt error given by Hartmann, and the tilt correction quantity is measured by the Hartmann;
the beam splitter is used for distinguishing a main laser emission waveband from an illumination waveband, so that the Hartmann sensor is not interfered by the main laser emission and not interfered by the main laser emission;
the Hartmann sensor is used for detecting the inclination and defocusing of the wave front, the measurement result is used for an inclined closed loop and a defocusing correction closed loop, and the Hartmann receiving wave front approaches to a plane wave after closed loop correction;
the Hartmann sensor has a sub-aperture of more than 3 multiplied by 3;
the main laser emission system outputs high-power laser as a main means for target striking, the emission wave surface is designed to be plane wave, and the laser is emitted to be focused on a target point after closed-loop correction;
the illumination system emits laser to illuminate the search area to provide light signals for the Hartmann sensor;
the controller is used for receiving signals of the Hartmann detector, calculating wave front inclination and defocusing, controlling the tilting mirror and the focusing secondary mirror to correct, and controlling the illumination system and the main laser to emit.
With reference to the first aspect, an embodiment of the present invention provides a first possible implementation manner of the first aspect, where the illumination system and the main laser emission are in different wavelength bands, and hartmann responds only to the wavelength band of the illumination system.
With reference to the first possible implementation manner of the first aspect, the embodiment of the present invention provides a second possible implementation manner of the first aspect, and the main laser emission system may manually adjust the beam divergence state and the emission angle for calibration of the initial state.
With reference to the second possible implementation manner of the first aspect, the embodiment of the present invention provides a third possible implementation manner of the first aspect, and the hartmann sensor only needs to reach 3 × 3 or more sub-apertures to measure the tilt and defocus of the incident wavefront.
With reference to the third possible implementation manner of the first aspect, an embodiment of the present invention provides a fourth possible implementation manner of the first aspect, and the focusing secondary mirror includes a secondary mirror and an electric adjustment mechanism.
The secondary mirror is used as a part of the optical system and forms a complete optical transmitting and receiving system with other optical devices.
The electric adjusting mechanism is used for adjusting the relative position of the secondary mirror and the primary mirror, so that the purpose of focusing is achieved.
With reference to the fourth possible implementation manner of the first aspect, an embodiment of the present invention provides a fifth possible implementation manner of the first aspect, where the system further includes a coarse tracking system, which is used for large-range scanning and low-precision tracking, and the coarse tracking system includes a coarse tracking sensor and a coarse tracking actuator.
The coarse tracking sensor is used for searching and position feedback of a target in a 1-5-degree view field range;
the rough tracking actuator is controlled by a rough tracking sensor signal to perform rough tracking on the target, so that the target enters the detection view field of the system.
In a second aspect, an embodiment of the present invention provides a laser defense method based on hartmann focusing, which mainly includes the following steps:
(1) firstly, system calibration is carried out, wave front aberration at a calibration target point is ensured to be received by Hartmann, and at the moment, a main laser emission point is focused on the calibration target point;
(2) emitting illumination laser through an illumination system in a working state after calibration, wherein the illumination laser and the main emission laser are in different wave bands;
(3) the target echo is received by a receiving optical system and then wavefront aberration is measured by a Hartmann sensor;
(4) wherein, the detection signal of the Hartmann sensor 5 can be obtained by calculating a wave front recovery formula, firstly, a facula slope matrix G of the Hartmann sensor is calculated, and the recovery matrix D is used for recovering-The zernike coefficient matrix of the aberration can be found.
A=D-G
Where the elements of G can be calculated from the spot displacement of each sub-aperture.
Figure GDA0003021712300000031
Wherein, Δ xiAnd Δ yi Gx(i) And Gy(i) Respectively representing the spot offsets, G, in the X-and Y-directions of the ith sub-aperturex(i) And Gy(i) Respectively represent the slopes of the ith sub-aperture in the X-direction and the Y-direction, and G can be expressed as:
G=[Gx(1),Gy(1),Gx(2),Gy(2),....Gx(m),Gy(m)]'
wherein D is-The recovery matrix is an inverse matrix of a slope matrix D of each order of Zernike wave surface, and the slope of each order of sub-aperture is:
Figure GDA0003021712300000032
wherein Z isk(x, y) is a k-th order Zernike wave surface, SiNormalizing the area for the ith sub-aperture, Zxk(i) And Zyk(i) Respectively representing the slope corresponding to the ith sub-aperture of the k-th order Zernike wave surface, the n-th order ZernikeThe nicom effective subaperture slope matrix D can be expressed as:
Figure GDA0003021712300000041
(5) the first, second and third order of the Zernike coefficient are the X direction tilt, Y direction tilt and defocus of the wave front aberration, wherein the X direction tilt aberration and the Y direction tilt aberration can be used for controlling the tilt mirror deflection, and the defocus aberration can be used for controlling the focusing secondary mirror.
(6) The controller respectively controls the tilting mirror and the focusing secondary mirror to correct tilting and defocusing aberrations, and the received wavefront of the Hartmann sensor after correction is the same as the calibrated wavefront.
(7) Because the receiving and transmitting light path is common, the corrected target point is conjugated with the laser transmitting point, and the power density at the target is highest.
Compared with the prior art, the invention has the advantages that: according to the laser defense system based on Hartmann focusing, the characteristics of simplicity and high efficiency of detection of a Hartmann sensor are utilized, the inclination and the out-of-focus image difference of an incident wavefront are measured through Hartmann, and then closed-loop correction is carried out through the tilting mirror and the focusing secondary mirror. The existing laser defense system adopts a focusing mode to focus through an image processing mode. The image processing focusing mode is susceptible to ambient light, the focusing deviation and direction cannot be calculated quantitatively, the calculation amount of the algorithm is large, the convergence is poor, stable focusing cannot be achieved, and the target can escape due to long focusing time. And the Hartmann sensor is adopted to replace an oblique tracking sensor to detect the wave front aberration, compared with the original image algorithm, the method has the advantages of simple calculation process and good stability, and can quantitatively detect the wave front defocusing so as to realize quick correction.
In order to make the aforementioned and other objects, features and advantages of the present invention comprehensible, preferred embodiments accompanied with figures are described in detail below.
Drawings
In order to more clearly illustrate the technical solutions of the embodiments of the present invention, the drawings needed to be used in the embodiments will be briefly described below, it should be understood that the following drawings only illustrate some embodiments of the present invention and therefore should not be considered as limiting the scope, and for those skilled in the art, other related drawings can be obtained according to the drawings without inventive efforts.
Fig. 1 is a schematic diagram illustrating a first principle of a hartmann focusing-based laser defense system according to an embodiment of the present invention;
FIG. 2 is a flowchart illustrating a working process of a Hartmann focusing based laser defense system according to an embodiment of the present invention;
FIG. 3 is a second schematic diagram of a Hartmann focusing-based laser defense system according to an embodiment of the present invention;
FIG. 4 is a schematic diagram illustrating a second primary mirror and a secondary mirror of the Hartmann focusing-based laser defense system according to the embodiment of the present invention;
description of the main element symbols:
1. a primary mirror; 2. a focusing secondary mirror; 3. a tilting mirror; 4. a beam splitter; 5. a Hartmann sensor; 6. a main laser emission system; 7. an illumination system; 8. a controller; 9. a coarse tracking sensor; 10. the rack is tracked.
Detailed Description
In order to make the objects, technical solutions and advantages of the embodiments of the present invention clearer, the technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the drawings in the embodiments of the present invention, and it is obvious that the described embodiments are only a part of the embodiments of the present invention, and not all of the embodiments. The components of embodiments of the present invention generally described and illustrated in the figures herein may be arranged and designed in a wide variety of different configurations. Thus, the following detailed description of the embodiments of the present invention, presented in the figures, is not intended to limit the scope of the invention, as claimed, but is merely representative of selected embodiments of the invention. All other embodiments, which can be derived by a person skilled in the art from the embodiments of the present invention without making any creative effort, shall fall within the protection scope of the present invention.
The existing laser defense system adopts a focusing mode to focus through an image processing mode. The image processing focusing mode is susceptible to ambient light, the focusing deviation and direction cannot be calculated quantitatively, the calculation amount of the algorithm is large, the convergence is poor, stable focusing cannot be achieved, and the target can escape due to long focusing time. And the Hartmann sensor is adopted to replace an oblique tracking sensor to detect the wave front aberration, compared with the original image algorithm, the method has the advantages of simple calculation process and good stability, and can quantitatively detect the wave front defocusing so as to realize quick correction.
Example 1: as shown in fig. 1, a laser defense system based on hartmann focusing provided by an embodiment of the present invention includes: the device comprises a main mirror 1, a focusing secondary mirror 2, an inclined mirror 3, a beam splitter 4, a Hartmann sensor 5, a main laser emission system 6, an illumination system 7 and a controller 8. The received light is reflected by the primary mirror 1, reflected by the focusing secondary mirror 2, reflected by the inclined mirror 3 and transmitted to the Hartmann sensor 5 by the beam splitter 4 in sequence; the emitted laser is reflected by a beam splitter 4, a tilting mirror 3, a focusing secondary mirror 2 and a primary mirror 1 in sequence and is emitted out of the system.
The primary mirror 1 is a part of an optical system and has a function of converging light beams;
the focusing secondary mirror 2 is a part of an optical system and forms an optical receiving and transmitting system with the primary mirror 1, and the focusing secondary mirror 2 in the system is used as a main focusing executing device;
the tilting mirror 3 plays a role in beam tilt correction in a light path, and tilt correction is carried out on a received optical signal in real time by calculating a correction quantity given by a tilt error through the Hartmann sensor 5;
the beam splitter 4 is used for distinguishing the main laser emission waveband from the illumination waveband, so that the Hartmann sensor 5 is not interfered by the main laser emission and not interfered by the main laser emission;
the Hartmann sensor 5 is used for detecting wave front inclination and defocusing, and the measurement result is used for an inclination closed loop and a defocusing correction closed loop;
a main laser emission system 6 that outputs high-power laser as a main means of target striking;
the illumination system 7 emits laser light to illuminate the search area to provide light signals for the Hartmann sensor 5;
the controller 8 is used for receiving signals of the Hartmann detector, calculating wave front inclination and defocusing, controlling the inclined mirror and the focusing secondary mirror to correct, and controlling illumination and main laser emission.
Specifically, the main work flow of the laser defense system based on hartmann focusing provided by the embodiment of the present invention is shown in fig. 2:
(1) firstly, system calibration is carried out, wave front aberration at a calibration target point is ensured to be received by Hartmann, and at the moment, a main laser emission point is focused on the calibration target point;
(2) emitting illumination laser through an illumination system in a working state after calibration, wherein the illumination laser and the main emission laser are in different wave bands;
(3) the target echo is received by a receiving optical system and then wavefront aberration is measured by a Hartmann sensor;
(4) wherein, the detection signal of the Hartmann sensor 5 can be obtained by calculating a wave front recovery formula, firstly, a facula slope matrix G of the Hartmann sensor is calculated, and the recovery matrix D is used for recovering-The zernike coefficient matrix of the aberration can be found.
A=D-G
(5) The first, second and third order of the Zernike coefficient are the X direction tilt, Y direction tilt and defocus of the wave front aberration, wherein the X direction tilt aberration and the Y direction tilt aberration can be used for controlling the tilt mirror deflection, and the defocus aberration can be used for controlling the focusing secondary mirror.
(6) The controller respectively controls the tilting mirror and the focusing secondary mirror to correct tilting and defocusing aberrations, and the received wavefront of the Hartmann sensor after correction is the same as the calibrated wavefront.
(7) Because the receiving and transmitting light path is common, the corrected target point is conjugated with the laser transmitting point, and the power density at the target is highest.
Example 2: embodiments of the present invention also include a coarse tracking system, allowing for scanning and tracking of large fields of view, see FIG. 3. The coarse tracking function in the system may be implemented in particular by the coarse tracking sensor 9 and the tracking gantry 10.
The coarse tracking sensor 9 is composed of an imaging lens and a photoelectric detector, the position information of a target can be obtained through the position of a light spot of the photoelectric detector, and the view field can be designed to be 1-5 degrees.
The tracking gantry 10 is used primarily as a load-bearing platform for the system, allowing both horizontal and pitch rotation.
When no suspicious target exists, the tracking rack 10 scans a specific area by a certain scanning path; when a target is found, the tracking frame 10 returns a signal through the coarse tracking sensor 9 to perform closed-loop tracking, so that the target enters a Hartmann 5 view field.
The system working flow after the Hartmann field of view is carried out on the target is the same as that of the embodiment 1.
In addition, the embodiment of the invention also provides another spatial arrangement mode of the primary mirror and the secondary mirror, which can be seen in fig. 4. The optical axes of the primary mirror 1 and the secondary focusing mirror 2 are superposed. This arrangement has the advantage of a larger focus range and less pupil plane translation than in figures 1 and 3.
Finally, it should be noted that: the above-mentioned embodiments are only specific embodiments of the present invention, which are used for illustrating the technical solutions of the present invention and not for limiting the same, and the protection scope of the present invention is not limited thereto, although the present invention is described in detail with reference to the foregoing embodiments, those skilled in the art should understand that: any person skilled in the art can modify or easily conceive the technical solutions described in the foregoing embodiments or equivalent substitutes for some technical features within the technical scope of the present disclosure; such modifications, changes or substitutions do not depart from the spirit and scope of the present invention in its spirit and scope. Are intended to be covered by the scope of the present invention. Therefore, the protection scope of the present invention shall be subject to the protection scope of the claims.

Claims (7)

1. A laser defense system based on Hartmann focusing, comprising: the device comprises a main mirror, a focusing secondary mirror, an inclined mirror, a beam splitter, a Hartmann sensor, a main laser emission system, an illumination system and a controller; the received light is transmitted to a Hartmann sensor through the reflection of a main mirror, the reflection of a focusing secondary mirror, the reflection of an inclined mirror and a beam splitter in sequence; the emitted laser is transmitted out of the system through beam splitter reflection, inclined mirror reflection, focusing secondary mirror reflection and main mirror reflection in sequence;
the illumination system emits laser to illuminate the search area to provide light signals for the Hartmann sensor;
the primary mirror is a part of the optical system and has a function of converging light beams;
the focusing secondary mirror is a part of an optical system and forms an optical receiving and transmitting system with the primary mirror, the focusing secondary mirror is used as a main focusing executing device, and the focusing amount is measured by the Hartmann sensor;
the tilting mirror plays a role in beam tilt correction in an optical path, a Hartmann sensor gives a tilt error, and the tilt error is calculated to obtain a correction quantity to perform tilt correction on a received optical signal in real time, wherein the tilt correction quantity is measured by the Hartmann sensor;
the Hartmann sensor is used for detecting the inclination and defocusing of the wave front, the measurement result is used for an inclined closed loop and a defocusing correction closed loop, and the Hartmann sensor receives the wave front approaching plane wave after closed loop correction;
the main laser emission system outputs high-power laser as a main means of target striking, the wave band is different from that of illumination laser, the emission wave surface is designed into plane wave, and the emission laser is focused on a target point after closed-loop correction;
the beam splitter is used for distinguishing a main laser emission waveband from an illumination waveband, so that the Hartmann sensor is not interfered by the main laser emission light;
the controller is used for receiving Hartmann sensor signals, calculating wave front inclination and defocusing, controlling the inclined mirror and the focusing secondary mirror to correct, and controlling the illumination system and the main laser to emit.
2. The laser defense system based on Hartmann focusing of claim 1, characterized in that: the system also comprises a coarse tracking system, a coarse tracking sensor and a coarse tracking actuator, wherein the coarse tracking system is used for large-range scanning and low-precision tracking; the coarse tracking sensor is used for searching and position feedback of a target in a 1-5-degree view field range; the rough tracking actuator is controlled by a rough tracking sensor signal to perform rough tracking on the target, the tracking precision is superior to a Hartmann view field 1/3, and the target enters the Hartmann view field.
3. The laser defense system based on Hartmann focusing of claim 1, characterized in that: the illumination system and the main laser are emitted in different wave bands, and the Hartmann sensor only responds to the wave band of the illumination system.
4. The laser defense system based on Hartmann focusing of claim 1, characterized in that: the main laser emission system can manually adjust the divergence state and the emission angle of the light beams for calibration of the initial state.
5. The laser defense system based on Hartmann focusing of claim 1, characterized in that: the Hartmann sensor has a sub-aperture of more than 3 x 3.
6. The laser defense system based on Hartmann focusing of claim 1, characterized in that: the focusing secondary mirror comprises a secondary mirror and an electric adjusting mechanism, and the electric adjusting mechanism is used for adjusting the relative position of the secondary mirror and the primary mirror to achieve the purpose of focusing.
7. An implementation method of the Hartmann focusing-based laser defense system of claim 1 is characterized in that the implementation process is as follows:
(1) firstly, system calibration is carried out, the Hartmann sensor is guaranteed to receive no wave front aberration at a calibration target point, and at the moment, a main laser emission point is focused on the calibration target point;
(2) emitting illumination laser through an illumination system in a working state after calibration, wherein the illumination laser and the main emission laser are in different wave bands;
(3) the target echo is received by a receiving optical system and then wavefront aberration is measured by a Hartmann sensor;
(4) it is composed ofIn the method, detection signals of the Hartmann sensor can be obtained by calculating a wave front recovery formula, firstly, a light spot slope matrix G of the Hartmann sensor is calculated, and the light spot slope matrix G passes through a recovery matrix D-A Zernike coefficient matrix A of the aberration can be obtained,
A=D-G
the first order, the second order and the third order of the Zernike coefficient are respectively the X-direction inclination, the Y-direction inclination and the defocusing of the wave front aberration, wherein the X-direction inclination aberration and the Y-direction inclination aberration can be used for controlling the deflection of the inclined mirror, and the defocusing aberration can be used for controlling the focusing secondary mirror;
(5) the controller respectively controls the tilting mirror and the focusing secondary mirror to correct tilting and defocusing aberrations, and the received wavefront of the corrected Hartmann sensor is the same as the calibrated wavefront;
(6) because the receiving and transmitting light path is common, the corrected target point is conjugated with the laser transmitting point, the power density of the target is highest, and then the focusing system is controlled by feedback to realize target tracking and striking.
CN201910845977.6A 2019-09-09 2019-09-09 Laser defense system and method based on Hartmann focusing Active CN110579875B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201910845977.6A CN110579875B (en) 2019-09-09 2019-09-09 Laser defense system and method based on Hartmann focusing

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201910845977.6A CN110579875B (en) 2019-09-09 2019-09-09 Laser defense system and method based on Hartmann focusing

Publications (2)

Publication Number Publication Date
CN110579875A CN110579875A (en) 2019-12-17
CN110579875B true CN110579875B (en) 2021-06-04

Family

ID=68812710

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201910845977.6A Active CN110579875B (en) 2019-09-09 2019-09-09 Laser defense system and method based on Hartmann focusing

Country Status (1)

Country Link
CN (1) CN110579875B (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112596229A (en) * 2020-12-16 2021-04-02 航天科工微电子系统研究院有限公司 Large-caliber off-axis transmitting telescope optical system for directional transmitting equipment
CN112902754B (en) * 2021-01-13 2021-11-16 西安电子科技大学 Infrared camera laser protection device and method based on digital micromirror device
CN115047433B (en) * 2022-08-16 2022-11-01 杭州宇称电子技术有限公司 Optical automatic adjusting method for TOF distance measuring system and application thereof

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1963432A (en) * 2006-12-13 2007-05-16 中国科学院光电技术研究所 Hartman wave front sensor to realize alignment function by light splitter and testing method thereof
AU2009316991A1 (en) * 2008-11-19 2010-05-27 Bae Systems Plc Mirror structure
CN102637994A (en) * 2012-04-18 2012-08-15 清华大学 Device and method for controlling quality of laser beam
EP3098627A1 (en) * 2015-05-27 2016-11-30 MBDA Deutschland GmbH Method and device for capturing an image of a target object
CN107328307A (en) * 2017-08-02 2017-11-07 国蓉科技有限公司 A kind of high light beam quality mid power laser long-range interception system

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108180788B (en) * 2018-02-28 2023-04-25 中国人民武装警察部队工程大学 Portable laser weapon device of anti-small unmanned aerial vehicle and using method thereof
CN108444410B (en) * 2018-06-20 2020-08-14 湖北三江航天红峰控制有限公司 Device and method for measuring parallelism of convergent laser emission optical axis and tracking visual axis

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1963432A (en) * 2006-12-13 2007-05-16 中国科学院光电技术研究所 Hartman wave front sensor to realize alignment function by light splitter and testing method thereof
AU2009316991A1 (en) * 2008-11-19 2010-05-27 Bae Systems Plc Mirror structure
CN102637994A (en) * 2012-04-18 2012-08-15 清华大学 Device and method for controlling quality of laser beam
EP3098627A1 (en) * 2015-05-27 2016-11-30 MBDA Deutschland GmbH Method and device for capturing an image of a target object
CN107328307A (en) * 2017-08-02 2017-11-07 国蓉科技有限公司 A kind of high light beam quality mid power laser long-range interception system

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
"气动光学自适应校正研究进展";谢文科 等;《激光与光电子学进展》;20140814;全文 *
"激光武器系统中的自适应光学技术";姜文汉;《系统工祖与电子技术》;19871231;全文 *

Also Published As

Publication number Publication date
CN110579875A (en) 2019-12-17

Similar Documents

Publication Publication Date Title
CN110579874B (en) Compact structure's self-adaptation laser defense system
CN110579875B (en) Laser defense system and method based on Hartmann focusing
US8451432B2 (en) Laser spot tracking with off-axis angle detection
CN105607074B (en) A kind of beacon adaptive optics system based on pulse laser
CN109313256A (en) Adaptive laser radar receiver
CN110487120B (en) Laser defense system and method for remote illumination
CN104267406A (en) Diffuse reflection laser ranging and high resolution imaging synchronous measurement photoelectric telescope system
US20090225299A1 (en) Laser spot tracker and target identifier
CN110500919B (en) Laser defense system and method for rapid high-precision focusing
CN108845415B (en) Coarse common-phase adjustment method and detection system applied to splicing mirror
CN105954734B (en) Large-caliber laser radar optical axis monitoring device
CN109945743B (en) Active illumination type synchronous monitoring common-caliber tracking and aiming emission system and method
CN109780946B (en) Laser beam-steering guidance angle measurement receiver
CN110864587B (en) Seeker aiming positioning method and aiming positioning system
CN109873253B (en) Active reflecting surface shape adjusting method based on axial gain measurement
CN108955904B (en) Multifunctional wavefront detection device considering point-surface target
CN111102942B (en) Laser emission optical axis and tracking system optical axis parallelism real-time correction system and method
CN111693966B (en) Astronomical positioning field matching device and method for laser radar
CN113534436B (en) Sparse synthetic aperture imaging system based on seven apertures and phase correction method thereof
CN111308685B (en) Artificial multi-color guide star array emission system based on multilayer conjugate adaptive optics
CN112526531B (en) Dual-view-field infrared imaging system with multi-target laser ranging function
Song et al. Design and implementation of infrared/laser dual-mode compound detection system
Adel et al. Design and implementation of a promising optical subsystem with a sky camera for laser warning systems
Vilcheck et al. Miniature lasercomm module for integration into a small unmanned aerial platform
Yang et al. Optimum design for optical antenna of space laser communication system

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant
CP01 Change in the name or title of a patent holder
CP01 Change in the name or title of a patent holder

Address after: 400021 No.7, 23rd floor, No.11, Panxi seventh branch road, Jiangbei District, Chongqing

Patentee after: Chongqing Lianxin Intelligent Technology Research Institute Co.,Ltd.

Address before: 400021 No.7, 23rd floor, No.11, Panxi seventh branch road, Jiangbei District, Chongqing

Patentee before: CHONGQING LIANXIN PHOTOELECTRIC TECHNOLOGY RESEARCH INSTITUTE Co.,Ltd.

TR01 Transfer of patent right

Effective date of registration: 20230625

Address after: Floor 1, No. 141-11 Xingpu Avenue, Huayuan Street, Xinjin County, Chengdu City, Sichuan Province, 611400

Patentee after: Chengdu Xinzhi Ruiguang Technology Co.,Ltd.

Address before: 400021 No.7, 23rd floor, No.11, Panxi seventh branch road, Jiangbei District, Chongqing

Patentee before: Chongqing Lianxin Intelligent Technology Research Institute Co.,Ltd.

TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20230802

Address after: No.6, 23rd floor, No.11, Panxi seventh branch road, Jiangbei District, Chongqing 400021

Patentee after: Chongqing Lianxin Photoelectric Technology Co.,Ltd.

Address before: Floor 1, No. 141-11 Xingpu Avenue, Huayuan Street, Xinjin County, Chengdu City, Sichuan Province, 611400

Patentee before: Chengdu Xinzhi Ruiguang Technology Co.,Ltd.

TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20231007

Address after: 4-1, No. 1-66 Qideng Road, Qijiang District, Chongqing, 400800

Patentee after: Chongqing Jiguang Technology Co.,Ltd.

Address before: No.6, 23rd floor, No.11, Panxi seventh branch road, Jiangbei District, Chongqing 400021

Patentee before: Chongqing Lianxin Photoelectric Technology Co.,Ltd.

TR01 Transfer of patent right