CN107655659A - Laser communication terminal vacuum test system and test method thereof - Google Patents
Laser communication terminal vacuum test system and test method thereof Download PDFInfo
- Publication number
- CN107655659A CN107655659A CN201710861450.3A CN201710861450A CN107655659A CN 107655659 A CN107655659 A CN 107655659A CN 201710861450 A CN201710861450 A CN 201710861450A CN 107655659 A CN107655659 A CN 107655659A
- Authority
- CN
- China
- Prior art keywords
- communication terminal
- laser communication
- mrow
- vacuum
- laser
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/02—Testing optical properties
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/07—Arrangements for monitoring or testing transmission systems; Arrangements for fault measurement of transmission systems
- H04B10/075—Arrangements for monitoring or testing transmission systems; Arrangements for fault measurement of transmission systems using an in-service signal
- H04B10/079—Arrangements for monitoring or testing transmission systems; Arrangements for fault measurement of transmission systems using an in-service signal using measurements of the data signal
- H04B10/0795—Performance monitoring; Measurement of transmission parameters
- H04B10/07955—Monitoring or measuring power
Landscapes
- Physics & Mathematics (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Testing Of Optical Devices Or Fibers (AREA)
Abstract
本发明涉及激光通信终端真空测试系统及其测试方法,包括发散角测试系统、功率测试系统及波相差测试系统;调整激光通信终端,使得激光通信终端指向并对准平行光管;平行光管接收激光通信终端发射的光束,并汇聚成像在发散角测试模块的光电耦合器上;调整激光通信终端,使激光通信终端发射与缩束系统同轴的光束,发射光束经过缩束系统后形成缩束平行光束,缩束平行光束经第一分光镜分光,分别传输至功率计与第二分光镜上,第二分光镜将光束再次进行分光后由第一哈特曼波前传感器与第二哈特曼波前传感器接收。可完成单端激光通信终端的热真空试验,验证真空高低温过程中,激光通信终端的稳定性,是激光通信终端热真空试验过程中必不可少的测试系统。
The invention relates to a laser communication terminal vacuum test system and a test method thereof, including a divergence angle test system, a power test system and a wave phase difference test system; the laser communication terminal is adjusted so that the laser communication terminal points to and aligns with a collimator; the collimator receives The beam emitted by the laser communication terminal is converged and imaged on the photocoupler of the divergence angle test module; the laser communication terminal is adjusted so that the laser communication terminal emits a beam coaxial with the beam reduction system, and the emitted beam passes through the beam reduction system to form a beam reduction Parallel beams, narrowed parallel beams are split by the first beam splitter and transmitted to the power meter and the second beam splitter respectively. The second beam splitter splits the beam again and then the first Hartmann wavefront sensor and the second Hart Mambo front sensor reception. It can complete the thermal vacuum test of the single-ended laser communication terminal, verify the stability of the laser communication terminal during the high and low temperature vacuum process, and is an indispensable test system for the thermal vacuum test of the laser communication terminal.
Description
技术领域technical field
本发明属于光学检测领域,涉及激光通信终端真空测试系统及其测试方法,尤其涉及一种空间激光通信终端真空条件下发散角、波相差、发射功率等参数的测试系统及其测量方法。The invention belongs to the field of optical detection, and relates to a vacuum test system and a test method for a laser communication terminal, in particular to a test system and a test method for parameters such as divergence angle, wave phase difference, and emission power of a space laser communication terminal under vacuum conditions.
背景技术Background technique
激光通信尤其是空间激光通信与传统微波空间通信的方式相比,具有高速、保密、抗干扰和轻小型等优势。随着空间遥感技术的发展,各类有效载荷将获取大量空间探测数据,这些数据需要实时传送至地面,供相关技术人员分析。目前卫星上常用的微波带宽约为百兆级别,已接近微波通信的理论极限,而实际的光纤激光通信传输速率高达40G/s,目前已经得到了实际应用,利用密集型光波复原技术(Densewavelength DivisionMultiplexing,DWDM)等光放大技术还可实现更高传输速率,地面上百吉级别光纤激光通信系统都已经商业化,因此采用激光进行通信将会大大减小数据传输压力。随着5.65G/s空间激光通信终端(Laser Communication Terminal,LCT)的成功实验,国外的几十吉比特率空间LCT也正处于研究和规划中,这些都充分证明了激光通信实际应用中的优势,所以以激光作为媒质进行通信可以很好的解决通信带宽瓶颈问题。Compared with traditional microwave space communication, laser communication, especially space laser communication, has the advantages of high speed, confidentiality, anti-interference and small size. With the development of space remote sensing technology, various payloads will obtain a large amount of space detection data, which needs to be transmitted to the ground in real time for analysis by relevant technical personnel. At present, the microwave bandwidth commonly used on satellites is about 100 megabytes, which is close to the theoretical limit of microwave communication, while the actual optical fiber laser communication transmission rate is as high as 40G/s, which has been practically applied at present. , DWDM) and other optical amplification technologies can also achieve higher transmission rates. The Baiji-level fiber laser communication system on the ground has been commercialized, so the use of lasers for communication will greatly reduce the pressure on data transmission. With the successful experiment of 5.65G/s space laser communication terminal (Laser Communication Terminal, LCT), dozens of gigabit rate space LCTs abroad are also under research and planning, which fully proves the advantages of laser communication in practical applications , so using laser as a medium for communication can solve the communication bandwidth bottleneck problem very well.
空间激光通信系统作为一种有效载荷,无论是在研制完成后,还是在发射之前,都要对其主要的技术指标进行严格的测试。在热真空环境下,考核空间激光通信系统的关键指标,成为空间激光通信系统环境试验中的重中之重。As a payload, the space laser communication system must be strictly tested for its main technical indicators no matter after the development is completed or before launch. In a thermal vacuum environment, evaluating the key indicators of the space laser communication system has become the top priority in the environmental test of the space laser communication system.
由于空间激光通信终端信息传输时需要至少台终端方能完成,而双终端对接信息传输测试需要的测试系统非常复杂,在热真空试验中想完成双终端对接测试的难度很大,因此,选择真空条件下对单端空间激光通信终端的关键指标进行测试。Since the information transmission of the space laser communication terminal requires at least one terminal to complete, and the test system required for the dual-terminal docking information transmission test is very complicated, it is very difficult to complete the dual-terminal docking test in the thermal vacuum test. Therefore, vacuum The key indicators of the single-ended space laser communication terminal are tested under these conditions.
单端激光通信终端的关键指标包括波相差、发散角和发射功率,如何在热真空条件下完成上述三项指标的测量,是验证单端激光通信终端热真空稳定性的难题。The key indicators of a single-ended laser communication terminal include wave phase difference, divergence angle, and transmission power. How to complete the measurement of the above three indicators under thermal vacuum conditions is a difficult problem in verifying the thermal vacuum stability of a single-ended laser communication terminal.
发明内容Contents of the invention
本发明的目的是提供一种激光通信终端真空测试系统及其测试方法,实现单端激光通信终端热真空条件下波相差、发散角和发射功率等关键指标的测试。The purpose of the present invention is to provide a laser communication terminal vacuum testing system and its testing method, to realize the testing of key indicators such as wave phase difference, divergence angle and transmission power under thermal vacuum conditions of a single-ended laser communication terminal.
本发明的技术解决方案是提供一种激光通信终端真空测试系统,其特殊之处在于:包括发散角测试系统、功率测试系统及波相差测试系统;The technical solution of the present invention is to provide a vacuum test system for laser communication terminals, which is special in that it includes a divergence angle test system, a power test system and a wave phase difference test system;
激光通信终端发射角度能够调节;The launch angle of the laser communication terminal can be adjusted;
上述发散角测试系统包括沿激光通信终端一路出射光路依次设置的平行光管1与发散角测试模块2;上述发散角测试模块2包括三维平移台及设置在三维平移台上的光电耦合器;The above-mentioned divergence angle testing system includes a collimator 1 and a divergence angle testing module 2 arranged sequentially along one outgoing optical path of the laser communication terminal; the above-mentioned divergence angle testing module 2 includes a three-dimensional translation platform and a photocoupler arranged on the three-dimensional translation platform;
上述激光通信终端发射与平行光管1同轴的光束;上述平行光管1接收激光通信终端发射的光束,并汇聚成像在发散角测试模块2的光电耦合器上;The above-mentioned laser communication terminal emits a light beam coaxial with the collimator 1; the above-mentioned collimator 1 receives the light beam emitted by the laser communication terminal, and converges the image on the photocoupler of the divergence angle test module 2;
上述激光通信终端与平行光管1位于真空环境中;The above-mentioned laser communication terminal and collimator 1 are located in a vacuum environment;
上述功率测试系统包括沿激光通信终端另一路出射光路依次设置的缩束系统6、第一分光镜8及位于第一分光镜8一路出射光路中的功率计12;The above-mentioned power test system includes a beam shrinking system 6 arranged sequentially along the other outgoing optical path of the laser communication terminal, a first beam splitter 8 and a power meter 12 located in one outgoing optical path of the first beam splitter 8;
上述波相差测试系统包括位于第一分光镜8另一路出射光路中的第二分光镜9及分别位于第二分光镜9出射光路中的第二哈特曼波前传感器11与第一哈特曼波前传感器10;The above-mentioned wave phase difference testing system includes a second beam splitter 9 located in the other outgoing light path of the first beam splitter 8, and a second Hartmann wavefront sensor 11 and the first Hartmann wavefront sensor 11 respectively located in the outgoing light path of the second beam splitter 9. Terman wavefront sensor 10;
上述激光通信终端发射与缩束系统6同轴的光束,发射光束经过缩束系统6后形成缩束平行光束,缩束平行光束经第一分光镜8分光,分别传输至功率计12与第二分光镜9上,第二分光镜9将光束再次进行分光后由第一哈特曼波前传感器10与第二哈特曼波前传感器11接收。The above-mentioned laser communication terminal emits a beam coaxial with the beam reduction system 6, and the emitted beam passes through the beam reduction system 6 to form a reduced beam parallel beam, which is split by the first beam splitter 8 and transmitted to the power meter 12 and the second On the beam splitter 9 , the second beam splitter 9 splits the beam again and receives it by the first Hartmann wavefront sensor 10 and the second Hartmann wavefront sensor 11 .
优选地,该测试系统还包括具有光学窗口5的真空罐3上述激光通信终端4位于真空罐3中,激光通信终端的出射光通过光学窗口5入射至缩束系统6;Preferably, the test system also includes a vacuum tank 3 with an optical window 5. The above-mentioned laser communication terminal 4 is located in the vacuum tank 3, and the outgoing light of the laser communication terminal enters the beam reduction system 6 through the optical window 5;
上述平行光管1与真空罐3固连,平行光管1与真空罐3形成密闭的真空空间,该空间内可模拟真空环境。The above-mentioned collimator 1 is fixedly connected with the vacuum tank 3, and the collimator 1 and the vacuum tank 3 form a closed vacuum space in which a vacuum environment can be simulated.
优选地,为了提高发散角的测量精度,上述平行光管1为长焦距离轴抛物面反射式平行光管。一般认为焦距大于10m的平行光管为长焦距平行光管。Preferably, in order to improve the measurement accuracy of the divergence angle, the above-mentioned collimator 1 is a parabolic reflective collimator with a long focal length axis. It is generally considered that a collimator with a focal length greater than 10 m is a long focal length collimator.
优选地,上述发散角测试模块2的感光面位于平行光管1的焦面处。Preferably, the photosensitive surface of the divergence angle testing module 2 is located at the focal plane of the collimator 1 .
优选地,上述发散角测试模块2中的感光器件包括至少一个光谱范围为800nm~1600nm的CCD或CMOS器件;上述发散角测试模块2还包括位于感光器件前端的衰减片组,通过加入不同衰减倍率的衰减片组调整进入感光器件的能量。Preferably, the photosensitive device in the above-mentioned divergence angle test module 2 includes at least one CCD or CMOS device with a spectral range of 800nm to 1600nm; the above-mentioned divergence angle test module 2 also includes an attenuation sheet group positioned at the front end of the photosensitive device. The attenuation film set adjusts the energy entering the photosensitive device.
优选地,上述缩束系统6由沿光路依次设置的离轴抛物面镜和目镜7组成,缩束倍率Γ的计算公式如公式(1)所示;Preferably, the above-mentioned attenuation system 6 is composed of off-axis parabolic mirrors and eyepieces 7 sequentially arranged along the optical path, and the calculation formula of the attenuation magnification Γ is shown in formula (1);
其中:L为激光通信终端4的出瞳直径;Wherein: L is the exit pupil diameter of the laser communication terminal 4;
a为两个哈特曼波前传感器的靶面的内切圆直径。a is the diameter of the inscribed circle of the target surface of the two Hartmann wavefront sensors.
优选地,上述第一哈特曼波前传感器10与第二哈特曼波前传感器11的特征波长与空间激光通信的特征波长匹配。Preferably, the characteristic wavelengths of the first Hartmann wavefront sensor 10 and the second Hartmann wavefront sensor 11 match the characteristic wavelength of space laser communication.
优选地,上述真空罐3的直径为3m、长为5m,内部真空度可达1×10-6Pa;Preferably, the above-mentioned vacuum tank 3 has a diameter of 3 m and a length of 5 m, and the internal vacuum degree can reach 1×10 -6 Pa;
上述光学窗口5为Φ500mm直径窗口,窗口玻璃的材料为石英或微晶;The above-mentioned optical window 5 is a Φ500mm diameter window, and the material of the window glass is quartz or microcrystalline;
上述平行光管1为30m焦距、Φ1m口径的离轴抛物面反射式平行光管;The above-mentioned collimator 1 is an off-axis parabolic reflective collimator with a focal length of 30 m and a diameter of Φ1 m;
上述第一哈特曼波前传感器10的特征波长为808nm、830nm,上述第二哈特曼波前传感器11的特征波长为1541nm、1550nm;The characteristic wavelengths of the above-mentioned first Hartmann wavefront sensor 10 are 808nm and 830nm, and the characteristic wavelengths of the above-mentioned second Hartmann wavefront sensor 11 are 1541nm and 1550nm;
缩束系统6的离轴抛物面镜为Φ250mm离轴抛物面镜;The off-axis parabolic mirror of the attenuator system 6 is a Φ250mm off-axis parabolic mirror;
上述参数并不仅仅限于所给的数据。The above parameters are not limited to the data given.
优选地,上述功率计12为积分球式功率计12,波长响应范围为800nm~1700nm,动态范围0.01W~10W。Preferably, the aforementioned power meter 12 is an integrating sphere power meter 12 with a wavelength response range of 800nm-1700nm and a dynamic range of 0.01W-10W.
本发明还提供一种基于上述的一种激光通信终端真空测试系统的激光通信终端真空测试方法,包括以下步骤:The present invention also provides a laser communication terminal vacuum test method based on the above-mentioned laser communication terminal vacuum test system, including the following steps:
步骤一:真空罐与平行光管内部同时抽真空,真空度达到1×10-5Pa以内后,开始激光通信终端性能测试;Step 1: Simultaneously evacuate the interior of the vacuum tank and the collimator, and start the performance test of the laser communication terminal after the vacuum degree reaches within 1×10 -5 Pa;
步骤二:调整激光通信终端,使得激光通信终端指向并对准平行光管;Step 2: Adjust the laser communication terminal so that the laser communication terminal points to and aligns with the collimator;
步骤三:选择衰减片组,装入发散角测试模块中,打开激光通信终端发射激光光束;Step 3: Select the attenuation sheet group, install it into the divergence angle test module, and turn on the laser communication terminal to emit the laser beam;
步骤四:发散角测试模块根据所成光斑图像调整曝光时间;Step 4: The divergence angle test module adjusts the exposure time according to the formed spot image;
步骤五:发散角测试模块连续采集六幅图像,计算不同图像对应的光斑直径Di,根据公式(2)计算焦面处光斑直径单位为mm,根据公式(3)计算不同波长对应的发散角θ,单位为rad;Step 5: The divergence angle test module continuously collects six images, calculates the spot diameter D i corresponding to different images, and calculates the spot diameter at the focal plane according to formula (2) The unit is mm, and the divergence angle θ corresponding to different wavelengths is calculated according to formula (3), and the unit is rad;
步骤六:调整激光通信终端的角度,使得激光通信终端指向并对准缩束系统;Step 6: Adjust the angle of the laser communication terminal so that the laser communication terminal points to and aligns with the beam reduction system;
步骤七:选择两组衰减片组,分别装入第一哈特曼波前传感器与第二哈特曼波前传感器前端,打开激光通信终端发射激光光束;Step 7: Select two sets of attenuation sheets, install them into the front end of the first Hartmann wavefront sensor and the second Hartmann wavefront sensor respectively, and turn on the laser communication terminal to emit the laser beam;
步骤八:功率计测量出射功率P2,按照公式(4)计算激光通信终端发射光功率P1;Step 8: The power meter measures the outgoing power P 2 , and calculates the emitted optical power P 1 of the laser communication terminal according to formula (4);
其中,τ1为缩束系统的透过率;τ2为第一分光镜的反射率;Wherein, τ 1 is the transmittance of the reduced beam system; τ 2 is the reflectivity of the first beam splitter;
步骤九:第一哈特曼波前传感器接收808nm激光,通过调整其姿态得到出射光束波相差,第二哈特曼波前传感器接收1541nm激光,通过调整其姿态得到出射光束波相差。Step 9: The first Hartmann wavefront sensor receives the 808nm laser, and obtains the wave phase difference of the outgoing beam by adjusting its attitude; the second Hartmann wavefront sensor receives the 1541nm laser, and obtains the wave phase difference of the outgoing beam by adjusting its attitude.
本发明的有益效果是:The beneficial effects of the present invention are:
1、本发明可完成单端激光通信终端的热真空试验,验证真空高低温过程中,激光通信终端的稳定性,是激光通信终端热真空试验过程中必不可少的测试系统;1. The present invention can complete the thermal vacuum test of a single-ended laser communication terminal, verify the stability of the laser communication terminal in the process of vacuum high and low temperature, and is an indispensable test system for the thermal vacuum test of the laser communication terminal;
2、本发明的激光通信终端真空测试系统,使用了两路分光,可使同时获取激光通信终端波相差和发射功率,测试过程稳定、可靠,能极大的提高测试效率,非常适合在工程测试中应用,该系统将测试的模块均置于真空环境之外,方便后续进行其余指标测试的扩张,其被改造功能很强大;2. The laser communication terminal vacuum test system of the present invention uses two-way splitting, which can simultaneously obtain the wave phase difference and transmission power of the laser communication terminal. The test process is stable and reliable, and the test efficiency can be greatly improved. It is very suitable for engineering testing In the middle application, the system puts the tested modules outside the vacuum environment, which is convenient for the subsequent expansion of other index tests, and its transformation function is very powerful;
3、本发明使用长焦距平行光管进行发散角的测量,激光通信终端的发散角在微弧度量级,可以大大提高发散角的测量精度;3. The present invention uses a long focal length collimator to measure the divergence angle, and the divergence angle of the laser communication terminal is on the micro-arc scale, which can greatly improve the measurement accuracy of the divergence angle;
4、本发明使用了缩束系统和分光镜的设计,可以同时测量激光通信终端的两个波长的波相差,可实现激光通信终端波相差和输出功率的同时测量,系统结构稳定、重复性高,满足热真空试验的测试需求。4. The present invention uses the design of the beam shrinking system and the beam splitter, which can simultaneously measure the wave phase difference of two wavelengths of the laser communication terminal, and can realize the simultaneous measurement of the wave phase difference and output power of the laser communication terminal. The system structure is stable and repeatable. , to meet the test requirements of thermal vacuum test.
附图说明Description of drawings
图1是本发明所提供的一种激光通信终端真空测试系统发散角测试模块的结构示意图;Fig. 1 is a schematic structural view of a divergence angle test module of a laser communication terminal vacuum test system provided by the present invention;
图2是本发明所提供的一种激光通信终端真空测试系统波相差和发射光功率测试模块的结构示意图;Fig. 2 is a schematic structural diagram of a wave phase difference and emission optical power test module of a laser communication terminal vacuum test system provided by the present invention;
图3是本发明所提供的一种激光通信终端真空测试系统波相差和发射光功率测试模块的放大图;3 is an enlarged view of a wave phase difference and emitted light power test module of a laser communication terminal vacuum test system provided by the present invention;
图中:1-平行光管;2-发散角测试模块;3-真空罐;4-激光通信终端;5-光学窗口;6-缩束系统;7-目镜;8-第一分光镜;9-第二分光镜;10-第一哈特曼波前传感器;11-第二哈特曼波前传感器;12-功率计。In the figure: 1-collimator; 2-divergence angle test module; 3-vacuum tank; 4-laser communication terminal; 5-optical window; 6-beam reduction system; 7-eyepiece; 8-first beam splitter; 9 - second beam splitter; 10 - first Hartmann wavefront sensor; 11 - second Hartmann wavefront sensor; 12 - power meter.
具体实施方式Detailed ways
以下结合附图及具体实施方式对本发明做进一步的描述。The present invention will be further described below in conjunction with the accompanying drawings and specific embodiments.
从图1及图2可以看出,本实施例测试系统包括用于放置激光通信终端4的真空罐3,真空罐3的尺寸为3m直径、5m长,内部真空度可达1×10-6Pa;真空罐3的一侧具有能够使光透过的石英或微晶光学窗口5,光学窗口5的直径为Φ500mm;其中激光通信终端4的出射光方向可调。It can be seen from Figures 1 and 2 that the test system of this embodiment includes a vacuum tank 3 for placing the laser communication terminal 4. The size of the vacuum tank 3 is 3m in diameter and 5m in length, and the internal vacuum degree can reach 1×10 -6 Pa; one side of the vacuum tank 3 has a quartz or microcrystalline optical window 5 capable of transmitting light, and the diameter of the optical window 5 is Φ500 mm; the direction of the outgoing light of the laser communication terminal 4 is adjustable.
还包括位于激光通信终端4出射光路中的发散角测试系统、功率测试系统及波相差测试系统。It also includes a divergence angle test system, a power test system and a wave phase difference test system located in the outgoing light path of the laser communication terminal 4 .
发散角测试系统包括沿光路设置的平行光管1及发散角测试模块2,平行光管1、激光通信终端4在同一个密闭空间中,该空间内可模拟真空环境,由于平行光管1的焦距和口径大,光学窗口5玻璃很难做到Φ1m口径,因此,将平行光管1与真空罐3连接在一起,做成一个密闭的空间,方便模拟真空环境;发散角测试模块2及功率测试系统与波相差测试系统均位于真空环境外,方便的进行位置的调整;本实施例中平行光管1是焦距为30m、Φ1m口径的离轴抛物面反射式平行光管1,其他实施例中不仅限于此参数;发散角测试模块2的感光面位于平行光管1的焦面处,发散角测试模块2中的感光器件为CCD或CMOS器件,光谱范围为800nm~1600nm,可以由一片感光器件完成,也可以通过更换不同波长范围的器件来满足整个测试光谱范围的需要;发散角模块的感光器件前端可加入衰减片组,通过加入不同衰减倍率的衰减片组来调整进入感光器件的能量。The divergence angle test system includes a collimator 1 and a divergence angle test module 2 arranged along the optical path. The collimator 1 and the laser communication terminal 4 are in the same closed space, which can simulate a vacuum environment. The focal length and aperture are large, and it is difficult for the optical window 5 glass to achieve a diameter of Φ1m. Therefore, the collimator 1 and the vacuum tank 3 are connected together to form a closed space, which is convenient for simulating the vacuum environment; the divergence angle test module 2 and the power Both the test system and the wave phase difference test system are located outside the vacuum environment, and it is convenient to adjust the position; in this embodiment, the collimator 1 is an off-axis parabolic reflective collimator 1 with a focal length of 30 m and a diameter of Φ1 m. Not limited to this parameter; the photosensitive surface of the divergence angle test module 2 is located at the focal plane of the collimator 1, and the photosensitive device in the divergence angle test module 2 is a CCD or CMOS device with a spectral range of 800nm to 1600nm. It is also possible to meet the needs of the entire test spectrum range by replacing devices with different wavelength ranges; the front end of the photosensitive device of the divergence angle module can be added with an attenuating film group, and the energy entering the photosensitive device can be adjusted by adding attenuating film groups with different attenuation ratios.
激光通信终端4发射光束与平行光管1同轴,平行光管1接收激光通信终端4发射光束,经过会聚后成像在发散角测试模块2上。The light beam emitted by the laser communication terminal 4 is coaxial with the collimator 1 , and the collimator 1 receives the light beam emitted by the laser communication terminal 4 and is imaged on the divergence angle test module 2 after convergence.
功率测试系统包括沿光路设置的缩束系统6、第一分光镜8及功率计12,在本实施例中功率计12位于第一分光镜8的反射光路中,在其他实施例中功率计12也可以位于第一分光镜8的透射光路中,只要满足功率计12与波相差测试系统分别位于第一分光镜8不同的光路中即可。缩束系统6由Φ250mm离轴抛物面镜和目镜7组成,缩束倍率Γ的计算公式如公式(1)所示;The power test system includes a beam shrinking system 6 arranged along the optical path, a first beam splitter 8 and a power meter 12. In this embodiment, the power meter 12 is located in the reflected light path of the first beam splitter 8. In other embodiments, the power meter 12 It can also be located in the transmission light path of the first beam splitter 8, as long as the power meter 12 and the wave phase difference testing system are respectively located in different light paths of the first beam splitter 8. The beam reduction system 6 is composed of a Φ250mm off-axis parabolic mirror and an eyepiece 7, and the calculation formula of the beam reduction magnification Γ is shown in formula (1);
其中:L为激光通信终端4的出瞳直径;a为哈特曼波前传感器的靶面尺寸;Where: L is the exit pupil diameter of the laser communication terminal 4; a is the target surface size of the Hartmann wavefront sensor;
功率计12为积分球式功率计12,波长响应范围为800nm~1700nm,动态范围0.01W~10W;The power meter 12 is an integrating sphere power meter 12 with a wavelength response range of 800nm to 1700nm and a dynamic range of 0.01W to 10W;
波相差测试系统包括位于第一分光镜8透射光路中的第二分光镜9、位于第二分光镜9透射光路中的第一哈特曼波前传感器10及位于第二分光镜9透射光路中的第二哈特曼波前传感器11,在其他实施例中第一哈特曼波前传感器10及第二哈特曼波前传感器11位置可以互换;第一哈特曼波前传感器10的特征波长为808nm、830nm,第二哈特曼波前传感器11的特征波长为1541nm、1550nm;这些波长为空间激光通信的特征波长,但不仅限于这些波长;The wave phase difference test system includes a second beam splitter 9 located in the transmission light path of the first beam splitter 8, a first Hartmann wavefront sensor 10 located in the transmission light path of the second beam splitter 9, and a first Hartmann wavefront sensor 10 located in the transmission light path of the second beam splitter 9. The second Hartmann wavefront sensor 11, in other embodiments the first Hartmann wavefront sensor 10 and the second Hartmann wavefront sensor 11 positions can be interchanged; The first Hartmann wavefront sensor 10 The characteristic wavelengths are 808nm and 830nm, and the characteristic wavelengths of the second Hartmann wavefront sensor 11 are 1541nm and 1550nm; these wavelengths are the characteristic wavelengths of space laser communication, but not limited to these wavelengths;
激光通信终端4调整方位角后,发射光束与缩束系统6同轴,发射光束经过光学窗口5、缩束系统6后,形成缩束平行光束,经过第一分光镜8分光,分别传输到功率计12和第二分光镜9上,经过第二分光镜9分光后,分别由第一哈特曼波前传感器10和第二哈特曼波前传感器11接收。After the laser communication terminal 4 adjusts the azimuth angle, the emission beam is coaxial with the beam reduction system 6, and the emission beam passes through the optical window 5 and the beam reduction system 6 to form a parallel beam reduction beam, which is split by the first beam splitter 8 and transmitted to the power On the meter 12 and the second beam splitter 9, after being split by the second beam splitter 9, the light is received by the first Hartmann wavefront sensor 10 and the second Hartmann wavefront sensor 11 respectively.
同时,本发明还提供了一种基于如上所述的激光通信终端4真空测试方法,该方法包括以下步骤:At the same time, the present invention also provides a vacuum test method based on the laser communication terminal 4 as described above, the method includes the following steps:
1)真空罐3与平行光管1内部同时抽真空,真空度达到1×10-5Pa以内后,开始激光通信终端性能测试;1) The inside of the vacuum tank 3 and the collimator 1 are evacuated at the same time, and after the vacuum degree reaches within 1×10 -5 Pa, the performance test of the laser communication terminal is started;
2)激光通信终端4调整指向与平行光管1对准;2) The laser communication terminal 4 adjusts the pointing to align with the collimator 1;
3)根据事先计算选择合适的衰减片组装入发散角测试模块2中,打开激光通信终端4发射激光光束;3) According to the calculation in advance, select a suitable attenuator to assemble into the divergence angle test module 2, and turn on the laser communication terminal 4 to emit the laser beam;
4)发散角测试模块2根据所成光斑图像调整合适的曝光时间,一般使所成像的灰度值不超过总的量化位数的80%为宜;4) The divergence angle test module 2 adjusts a suitable exposure time according to the formed spot image, generally making the imaged gray value not exceed 80% of the total number of quantized digits;
5)连续采集6幅图像,根据程序计算不同图像对应的光斑直径Di,根据公式(2)计算通过公式(3)计算得到不同波长的发散角θ。5) Continuously collect 6 images, calculate the spot diameter D i corresponding to different images according to the program, and calculate according to formula (2) The divergence angle θ of different wavelengths is calculated by formula (3).
其中:θ为信号光发散角,单位:rad;Where: θ is the signal light divergence angle, unit: rad;
为焦面处的光斑直径,单位:mm; is the spot diameter at the focal plane, unit: mm;
6)激光通信终端4调整指向与缩束系统6对准;6) The laser communication terminal 4 adjusts the pointing and aligns with the beam reduction system 6;
7)根据事先计算选择合适的衰减片组装入哈特曼波前传感器前端,打开激光通信终端4发射激光光束;7) According to the calculation in advance, select a suitable attenuator to assemble into the front end of the Hartmann wavefront sensor, and open the laser communication terminal 4 to emit the laser beam;
8)功率计12测量出射功率P2,按照公式(4)计算激光通信终端4发射光功率P1;8) The power meter 12 measures the outgoing power P 2 , and calculates the transmitted optical power P 1 of the laser communication terminal 4 according to formula (4);
其中:P1为激光通信终端4发射光功率;Where: P 1 is the optical power emitted by the laser communication terminal 4;
P2为功率计12测得的出射功率;P 2 is the output power measured by the power meter 12;
τ1为缩束系统6的透过率;τ2为第一分光镜8的反射率;τ 1 is the transmittance of the beam reduction system 6; τ 2 is the reflectivity of the first beam splitter 8;
9)第一哈特曼波前传感器10接收808nm激光,通过调整其姿态得到出射光束波相差,第二哈特曼波前传感器11接收1541nm激光,通过调整其姿态得到出射光束波相差。9) The first Hartmann wavefront sensor 10 receives the 808nm laser, and obtains the wave phase difference of the outgoing beam by adjusting its attitude. The second Hartmann wavefront sensor 11 receives the 1541nm laser, and obtains the wave phase difference of the outgoing beam by adjusting its attitude.
本发明的激光通信终端真空测试系统,可以满足单端激光通信终端主要光学参数的测量,验证真空高低温过程中,激光通信终端的稳定性,是激光通信终端热真空试验过程中必不可少的测试系统。The laser communication terminal vacuum test system of the present invention can meet the measurement of the main optical parameters of the single-ended laser communication terminal, and verify the stability of the laser communication terminal in the process of vacuum high and low temperature, which is indispensable in the thermal vacuum test process of the laser communication terminal test system.
本发明的激光通信终端真空测试系统,使用了两路分光,可使同时获取激光通信终端波相差和发射功率,测试过程稳定、可靠,能极大的提高测试效率,非常适合在工程测试中应用,该系统将测试的模块均置于真空环境之外,方便后续进行其余指标测试的扩张,其被改造功能很强大。The laser communication terminal vacuum test system of the present invention uses two beam splitters, which can simultaneously obtain the wave phase difference and emission power of the laser communication terminal. The test process is stable and reliable, and can greatly improve the test efficiency. It is very suitable for application in engineering testing. , the system puts the tested modules out of the vacuum environment, which facilitates the subsequent expansion of other index tests, and its transformation function is very powerful.
本发明的激光通信终端真空测试系统,选用了焦距较长的平行光管来完成发散角的测量,可以大大提高发散角的测量精度。The laser communication terminal vacuum test system of the present invention selects a collimator with a longer focal length to measure the divergence angle, which can greatly improve the measurement accuracy of the divergence angle.
Claims (10)
- A kind of 1. laser communication terminal vacuum test system, it is characterised in that:Including angle of divergence test system, power test system And ripple difference test system;Laser communication terminal transmission angle can be adjusted;The angle of divergence test system is included along the laser communication terminal parallel light tube (1) that emitting light path is set gradually all the way and hair Dissipate angle test module (2);The angle of divergence test module (2) includes D translation platform and the photoelectricity being arranged on D translation platform Coupler;The laser communication terminal transmission light beam coaxial with parallel light tube (1);It is whole that the parallel light tube (1) receives laser communication The light beam of transmitting is held, and converges and is imaged on the photoelectrical coupler of angle of divergence test module (2);The laser communication terminal is located in vacuum environment with parallel light tube (1);Shrink beam system (6) that the power test system includes setting gradually along laser communication terminal another way emitting light path, the One spectroscope (8) and the power meter (12) in the first spectroscope (8) all the way emitting light path;Ripple difference test system include the second spectroscope (9) being located in the first spectroscope (8) another way emitting light path and The second Hartmann wave front sensor (11) and first Hartmann's wavefront sensing being located at respectively in the second spectroscope (9) emitting light path Device (10);The laser communication terminal transmission light beam coaxial with shrink beam system (6), transmitting light beam are formed after shrink beam system (6) Shrink beam collimated light beam, shrink beam collimated light beam are divided through the first spectroscope (8), are transmitted separately to power meter (12) and the second spectroscope (9) on, the second spectroscope (9) light beam is divided again after by the first Hartmann wave front sensor (10) and the second Hartmann Wavefront sensor (11) receives.
- A kind of 2. laser communication terminal vacuum test system according to claim 1, it is characterised in that:Also include that there is light The vacuum tank (3) of window (5) is learned, the laser communication terminal (4) is located in vacuum tank (3), the emergent light of laser communication terminal Shrink beam system (6) is incident to by optical window (5);The parallel light tube (1) is connected with vacuum tank (3), and parallel light tube (1) forms closed vacuum space with vacuum tank (3).
- A kind of 3. laser communication terminal vacuum test system according to claim 2, it is characterised in that:The parallel light tube (1) it is long-focus off-axis parabolic collimator.
- A kind of 4. laser communication terminal vacuum test system according to claim 3, it is characterised in that:The angle of divergence is surveyed The photosurface of die trial block (2) is located at the focal plane of parallel light tube (1).
- A kind of 5. laser communication terminal vacuum test system according to claim 4, it is characterised in that:The angle of divergence is surveyed Sensor devices in die trial block (2) include the CCD or cmos device that at least one spectral region is 800nm~1600nm;It is described Angle of divergence test module (2) also includes the attenuator group positioned at sensor devices front end, by the decay for adding differential declines multiplying power Piece group is adjusted into the energy of sensor devices.
- 6. according to a kind of any described laser communication terminal vacuum test systems of claim 1-5, it is characterised in that:The contracting Beam system (6) is made up of the off axis paraboloidal mirror and eyepiece (7) set gradually along light path, shrink beam multiplying power Γ calculation formula such as public affairs Shown in formula (1);<mrow> <mi>&Gamma;</mi> <mo>=</mo> <mfrac> <mi>L</mi> <mi>a</mi> </mfrac> <mo>-</mo> <mo>-</mo> <mo>-</mo> <mrow> <mo>(</mo> <mn>1</mn> <mo>)</mo> </mrow> </mrow>Wherein:L is the exit pupil diameter of laser communication terminal (4);A is the inscribed circle diameter of the target surface of two Hartmann wave front sensors.
- A kind of 7. laser communication terminal vacuum test system according to claim 6, it is characterised in that:First Hart Graceful Wavefront sensor (10) and the characteristic wavelength of the second Hartmann wave front sensor (11) and the characteristic wavelength of laser space communication Matching.
- A kind of 8. laser communication terminal vacuum test system according to claim 7, it is characterised in that:A diameter of 3m, a length of 5m of the vacuum tank (3), internal vacuum is up to 1 × 10-6Pa;The optical window (5) is Φ 500mm diameter windows, and the material of window glass is quartz or crystallite;The parallel light tube (1) is 30m focal lengths, the off-axis parabolic collimator of Φ 1m bores;The characteristic wavelength of first Hartmann wave front sensor (10) is 808nm, 830nm, and the second Hartmann wavefront passes The characteristic wavelength of sensor (11) is 1541nm, 1550nm;The off axis paraboloidal mirror of shrink beam system (6) is Φ 250mm off axis paraboloidal mirrors.
- A kind of 9. laser communication terminal vacuum test system according to claim 7, it is characterised in that:The power meter (12) it is integrating sphere type power meter, wavelength response range is 800nm~1700nm, dynamic range 0.01W~10W.
- 10. a kind of laser communication based on a kind of any described laser communication terminal vacuum test systems of claim 1-9 is whole Hold vacuum test method, it is characterised in that comprise the following steps:Step 1:For vacuum tank with being vacuumized inside parallel light tube simultaneously, vacuum reaches 1 × 10-5After within Pa, start laser and lead to Believe terminal capabilities test;Step 2:Adjust laser communication terminal so that laser communication terminal is pointed to and is directed at parallel light tube;Step 3:Attenuator group is selected, is fitted into angle of divergence test module, opens laser communication terminal transmission laser beam;Step 4:Angle of divergence test module adjusts the time for exposure according to institute into light spot image;Step 5:The width image of angle of divergence test module continuous acquisition six, calculate spot diameter D corresponding to different imagesi, according to public affairs Formula (2) calculates spot diameter at focal planeUnit is mm, the angle of divergence θ according to corresponding to formula (3) calculates different wave length, unit For rad;<mrow> <mover> <mi>D</mi> <mo>&OverBar;</mo> </mover> <mo>=</mo> <mfrac> <mrow> <munderover> <mo>&Sigma;</mo> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> </mrow> <mn>6</mn> </munderover> <mrow> <mo>(</mo> <msub> <mi>D</mi> <mn>1</mn> </msub> <mo>+</mo> <msub> <mi>D</mi> <mn>2</mn> </msub> <mo>+</mo> <mn>...</mn> <mo>+</mo> <msub> <mi>D</mi> <mn>6</mn> </msub> <mo>)</mo> </mrow> </mrow> <mn>6</mn> </mfrac> <mo>-</mo> <mo>-</mo> <mo>-</mo> <mrow> <mo>(</mo> <mn>2</mn> <mo>)</mo> </mrow> </mrow><mrow> <mi>&theta;</mi> <mo>=</mo> <mfrac> <mover> <mi>D</mi> <mo>&OverBar;</mo> </mover> <mi>f</mi> </mfrac> <mo>-</mo> <mo>-</mo> <mo>-</mo> <mrow> <mo>(</mo> <mn>3</mn> <mo>)</mo> </mrow> </mrow>Step 6:Adjust the angle of laser communication terminal so that laser communication terminal is pointed to and is directed at shrink beam system;Step 7:Two groups of attenuator groups are selected, are respectively charged into the first Hartmann wave front sensor and second Hartmann's wavefront sensing Device front end, open laser communication terminal transmission laser beam;Step 8:Power meter measurement outgoing power P2, laser communication terminal transmission luminous power P is calculated according to formula (4)1;<mrow> <msub> <mi>P</mi> <mn>1</mn> </msub> <mo>=</mo> <mfrac> <msub> <mi>P</mi> <mn>2</mn> </msub> <mrow> <msub> <mi>&tau;</mi> <mn>1</mn> </msub> <mo>&times;</mo> <msub> <mi>&tau;</mi> <mn>2</mn> </msub> </mrow> </mfrac> <mo>-</mo> <mo>-</mo> <mo>-</mo> <mrow> <mo>(</mo> <mn>4</mn> <mo>)</mo> </mrow> </mrow>Wherein, τ1For the transmitance of shrink beam system;τ2For first spectroscopical reflectivity;Step 9:First Hartmann wave front sensor receives 808nm laser, and outgoing beam ripple phase is obtained by adjusting its posture Difference, the second Hartmann wave front sensor receive 1541nm laser, and outgoing beam ripple difference is obtained by adjusting its posture.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201710861450.3A CN107655659B (en) | 2017-09-21 | 2017-09-21 | Laser communication terminal vacuum test system and test method thereof |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201710861450.3A CN107655659B (en) | 2017-09-21 | 2017-09-21 | Laser communication terminal vacuum test system and test method thereof |
Publications (2)
Publication Number | Publication Date |
---|---|
CN107655659A true CN107655659A (en) | 2018-02-02 |
CN107655659B CN107655659B (en) | 2024-01-05 |
Family
ID=61130788
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201710861450.3A Active CN107655659B (en) | 2017-09-21 | 2017-09-21 | Laser communication terminal vacuum test system and test method thereof |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN107655659B (en) |
Cited By (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108507687A (en) * | 2018-02-09 | 2018-09-07 | 中国科学院长春光学精密机械与物理研究所 | A kind of infrared Hartmann wave front sensor |
CN109450562A (en) * | 2018-11-23 | 2019-03-08 | 长春理工大学 | Off-axis two waveband laser communication comprehensive performance testing system and method |
CN110611533A (en) * | 2019-09-24 | 2019-12-24 | 四川天邑康和通信股份有限公司 | Method for filtering defective optical modules of ONU (optical network Unit) in production line |
CN110672304A (en) * | 2019-08-16 | 2020-01-10 | 中国科学院西安光学精密机械研究所 | Laser communication terminal relay optical path performance testing system, method and calibration method |
CN111426448A (en) * | 2020-03-27 | 2020-07-17 | 中国科学院西安光学精密机械研究所 | Optical assembly performance test platform |
CN111811430A (en) * | 2020-07-22 | 2020-10-23 | 中国科学院西安光学精密机械研究所 | A device and method for measuring the surface shape of an optical element in a low temperature environment |
CN112713932A (en) * | 2020-12-21 | 2021-04-27 | 中国科学院西安光学精密机械研究所 | Laser communication terminal optical path relay unit assembling and detecting system and detecting method based on same |
CN113162690A (en) * | 2021-06-01 | 2021-07-23 | 中国科学院微小卫星创新研究院 | Space laser communication detection device and method |
CN113452437A (en) * | 2021-06-25 | 2021-09-28 | 中国科学院上海光学精密机械研究所 | Inter-satellite laser link test simulation system and method for space optical communication |
CN113967608A (en) * | 2021-12-22 | 2022-01-25 | 南京英田光学工程股份有限公司 | Ground screening test device and method for satellite-borne MEMS beam control swing mirror |
CN118549094A (en) * | 2024-07-26 | 2024-08-27 | 北京融为科技有限公司 | Test method and device for measuring laser load index |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20010028462A1 (en) * | 1998-09-22 | 2001-10-11 | Nikon Corporation | Interferometer system and method of manufacturing projection optical system using same |
CN103033261A (en) * | 2012-12-26 | 2013-04-10 | 中国科学院上海光学精密机械研究所 | On-line detection method of focal spot energy distribution |
CN106840610A (en) * | 2017-01-06 | 2017-06-13 | 中国科学院上海光学精密机械研究所 | The measurement apparatus and measuring method of optic element damage threshold value under vacuum environment |
CN207423494U (en) * | 2017-09-21 | 2018-05-29 | 中国科学院西安光学精密机械研究所 | Laser communication terminal vacuum test system |
-
2017
- 2017-09-21 CN CN201710861450.3A patent/CN107655659B/en active Active
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20010028462A1 (en) * | 1998-09-22 | 2001-10-11 | Nikon Corporation | Interferometer system and method of manufacturing projection optical system using same |
CN103033261A (en) * | 2012-12-26 | 2013-04-10 | 中国科学院上海光学精密机械研究所 | On-line detection method of focal spot energy distribution |
CN106840610A (en) * | 2017-01-06 | 2017-06-13 | 中国科学院上海光学精密机械研究所 | The measurement apparatus and measuring method of optic element damage threshold value under vacuum environment |
CN207423494U (en) * | 2017-09-21 | 2018-05-29 | 中国科学院西安光学精密机械研究所 | Laser communication terminal vacuum test system |
Non-Patent Citations (1)
Title |
---|
刘敏时;王晓曼;景文博;王斌;: "用于激光光束检测的夏克-哈特曼传感器参量设计", 光学学报, no. 03 * |
Cited By (17)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108507687A (en) * | 2018-02-09 | 2018-09-07 | 中国科学院长春光学精密机械与物理研究所 | A kind of infrared Hartmann wave front sensor |
CN109450562A (en) * | 2018-11-23 | 2019-03-08 | 长春理工大学 | Off-axis two waveband laser communication comprehensive performance testing system and method |
CN109450562B (en) * | 2018-11-23 | 2021-02-05 | 长春理工大学 | Off-axis dual-band laser communication comprehensive performance testing system and method |
CN110672304A (en) * | 2019-08-16 | 2020-01-10 | 中国科学院西安光学精密机械研究所 | Laser communication terminal relay optical path performance testing system, method and calibration method |
CN110611533A (en) * | 2019-09-24 | 2019-12-24 | 四川天邑康和通信股份有限公司 | Method for filtering defective optical modules of ONU (optical network Unit) in production line |
CN110611533B (en) * | 2019-09-24 | 2021-01-01 | 四川天邑康和通信股份有限公司 | Method for filtering defective optical modules of ONU (optical network Unit) in production line |
CN111426448A (en) * | 2020-03-27 | 2020-07-17 | 中国科学院西安光学精密机械研究所 | Optical assembly performance test platform |
CN111426448B (en) * | 2020-03-27 | 2021-06-22 | 中国科学院西安光学精密机械研究所 | An optical component performance test platform |
CN111811430B (en) * | 2020-07-22 | 2021-09-14 | 中国科学院西安光学精密机械研究所 | Optical element surface shape measuring device and method in low-temperature environment |
CN111811430A (en) * | 2020-07-22 | 2020-10-23 | 中国科学院西安光学精密机械研究所 | A device and method for measuring the surface shape of an optical element in a low temperature environment |
CN112713932A (en) * | 2020-12-21 | 2021-04-27 | 中国科学院西安光学精密机械研究所 | Laser communication terminal optical path relay unit assembling and detecting system and detecting method based on same |
CN113162690A (en) * | 2021-06-01 | 2021-07-23 | 中国科学院微小卫星创新研究院 | Space laser communication detection device and method |
CN113162690B (en) * | 2021-06-01 | 2023-10-27 | 中国科学院微小卫星创新研究院 | Space laser communication detection device and method |
CN113452437A (en) * | 2021-06-25 | 2021-09-28 | 中国科学院上海光学精密机械研究所 | Inter-satellite laser link test simulation system and method for space optical communication |
CN113967608A (en) * | 2021-12-22 | 2022-01-25 | 南京英田光学工程股份有限公司 | Ground screening test device and method for satellite-borne MEMS beam control swing mirror |
CN118549094A (en) * | 2024-07-26 | 2024-08-27 | 北京融为科技有限公司 | Test method and device for measuring laser load index |
CN118549094B (en) * | 2024-07-26 | 2024-11-19 | 北京融为科技有限公司 | Test method and device for measuring laser load index |
Also Published As
Publication number | Publication date |
---|---|
CN107655659B (en) | 2024-01-05 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN107655659A (en) | Laser communication terminal vacuum test system and test method thereof | |
CN101782435B (en) | Laser parameter comprehensive test system | |
CN207423494U (en) | Laser communication terminal vacuum test system | |
CN110672304B (en) | Laser communication terminal relay optical path performance testing system, method and calibration method | |
CN104865576B (en) | A kind of compact ultra-short pulse laser long-distance ranging system and its distance-finding method | |
CN104539350B (en) | Space laser communication terminal level system testing method | |
CN110146259A (en) | A kind of reflective multi-light axis consistency quantitative test of large-caliber off-axis and calibrating installation | |
CN105444991B (en) | Optical coupling efficiency test device in a kind of atmospheric turbulance | |
CN104539349B (en) | Multifunctional laser space communication ground test system and static parameter test method | |
CN101651496A (en) | Beacon optical axis precision positioning system in atmosphere laser communication system | |
CN109738160B (en) | Multi-optical-axis consistency testing device and method based on laser communication system | |
CN202522516U (en) | Optical transmissivity test device | |
CN114200687B (en) | Optical self-calibration device and method for laser communication system | |
CN103471820A (en) | Real-time revising tester for portable multi-spectral optoelectronic device | |
CN201203707Y (en) | Precise Optical Axis Positioning Device in Atmospheric Laser Communication System | |
CN110823527A (en) | Calibration method for optical axis of multi-sensor containing laser | |
CN209927419U (en) | Large-caliber off-axis reflection type multi-optical-axis consistency quantitative test and calibration device | |
CN108287059A (en) | High-precision near-infrared laser beam quality measurement analysis device | |
CN116519136B (en) | Same-optical-axis adjustment system and method for moon direct spectrum irradiance instrument | |
CN111769870B (en) | Space laser communication terminal relay optical path assembly detection device and detection method | |
CN106643668A (en) | Atmosphere laser occultation signal generation and detection equipment | |
CN106443638A (en) | Analysis method, verification system and verification method of laser echo transmission characteristic | |
CN207600598U (en) | The atmospheric parameter monitoring device of the big visual field sky imaging technique of multiband | |
CN107764521A (en) | Device and method for measuring isolation of optical antenna of laser communication system | |
CN107515044A (en) | Atmospheric parameter monitoring device and method for multi-band large field of view sky imaging technology |
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 |