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METHOD OF NIGHT AND / OR daytime observations of remote objects with simultaneous phase shift keying LASER PULSES highlight AND DEVICE FOR IMPLEMENTATION

机译:同时相移键控的远程对象的夜间和/或白天观测方法激光脉冲高亮显示和实施装置

摘要

1.method of and / or a u043du0430u0431u043bu044eu0434u0435u043du0438u00a0 remote object, which form a series of m pulses of laser u0438u0437u043bu0443u0447u0435u043du0438u00a0 where m2, with the first pulse laser u0438u0437u043bu0443u0447u0435u043du0438u00a0 u043du0430u043fu0440u0430u0432u043bu00a0u044eu0442 on an object are reflected from the object radiation and u043eu043fu0440u0435u0434u0435u043bu00a0u044eu0442 u0432u0440u0435u043cu00a0 t u0440u0430u0441u043fu0440u043eu0441u0442u0440u0430u043du0435u043du0438u00a0 u0438u0437u043bu0443u0447u0435u043du0438u00a0 from the transmitting channel to the object after what form the (m - 1) subsequent pulses of laser u0438u0437u043bu0443u0447u0435u043du0438u00a0,u043du0430u043fu0440u0430u0432u043bu00a0u044eu0442 them on the object and through the receiving lens and optically u0441u043eu043fu0440u00a0u0436u0435u043du043du043eu0439 with him u0444u043fu0437u0441 matrix in the frame of tc are reflected from an object radiation and receive his image, u043eu0442u043bu0438u0447u0430u044eu0449u0438u0439u0441u00a0 because the first pulse laser u0438u0437u043bu0443u0447u0435u043du0438u00a0 shape with the length, and the length of (m - 1) subsequent pulse s u043eu043fu0440u0435u0434u0435u043bu00a0u044eu0442 of u0441u043eu043eu0442u043du043eu0448u0435u043du0438;where Lu043fu043eu0440 range u0444u043eu0440u043cu0438u0440u043eu0432u0430u043du0438u00a0 static inverse u0440u0430u0441u0441u0435u00a0u043du0438u00a0;;n is the average u043fu0440u0435u043bu043eu043cu043bu0435u043du0438u00a0 atmosphere;;with the speed of light.;for this cause the start of each of the (m - 1) laser pulses from the beginning of the frame u0444u043fu0437u0441 matrix on the u0432u0440u0435u043cu00a0 u0442u0443u043fu0440.u043bu0438 = Tu043a - (4u0442 - Lu043fu043eu0440n / c), and the beginning of each period u043du0430u043au043eu043fu043bu0435u043du0438u00a0 u0444u043fu0437u0441 - matri from the beginning of the frame to cause the tsk;2. method for u043eu0442u043bu0438u0447u0430u044eu0449u0438u0439u0441u00a0 1, so that further form the k series of pulses where k1, u043au0430u0436u0434u0430u00a0 containing m pulses, to cause the first laser the momentum from the beginning of the frame u0444u043fu0437u0441 matrix in each subsequent series of laser pulses on the u0432u0440u0435u043cu00a0 u0442u0443u043fu0440.u043bu0438, a u0434u043bu00a0 previous series of laser pulses.;3. method for u043eu0442u043bu0438u0447u0430u044eu0449u0438u0439u0441u00a0 1 or 2, so that Lu043fu043eu0440 u043eu043fu0440u0435u0434u0435u043bu00a0u044eu0442 of u0441u043eu043eu0442u043du043eu0448u0435u043du0438u00a0 u0434u043bu00a0 instantaneous power interference of reverse u0440u0430u0441u0441u0435u00a0u043du0438u00a0 u0444u043fu043eu0440 (t):;q sb pos = "post" r / sb and sb & phiv; pos = "post" b / sb d sb pos = "post" of / sb & hairsp; sp pos = "post" 2 / x (& sp pi;) u0435u0445u0440 (2 & alpha; sb pos = "post" r / sb l sb pos = "post" since / sb 4 sb pos = "post" b / sb & hairsp; sp pos = "post" 2 sp /;u0444u043fu043eu0440 (t) = ---------------------------- u0435u0445u0440 [----------------];4 (l sb pos = "post" since / sb sp pos = "post" 2 / sp (& omega ; sp pos = "post" 2 / sp & hairsp; sb pos = "post" a + / sb & omega; sp pos = "post" 2 / sp & hairsp; sb pos = "post" b / sb ) (l sb pos = "post" since / sb sp pos = "post" 2 / (& sp omega; sp pos = "post" 2 / sp & hairsp; sb pos = "post" a / sb + s & omega; p pos = "post" 2 / sp & hairsp; sb pos = "post" b / sb );where Qu043b - u044du043du0435u0440u0433u0438u00a0 laser;;x (a) = 0,33S - 0,3Lu043fu043eu0440 - value u0438u043du0434u0438u043au0430u0442u0440u0438u0441u044b towards "back";;s is the u0440u0430u0441u0441u0435u00a0u043du0438u00a0 atmosphere;;p is the rate of u0440u0430u0441u0441u0435u00a0u043du0438u00a0 atmosphere;;ol, per field u0437u0440u0435u043du0438u00a0 divergence u0438u0437u043bu0443u0447u0435u043du0438u00a0 receiver and transmitter respectively.;Du043eu0431 - diameter of the receiving lens.;u0445u0431 - linear parallax between the receiving and transmitting systems.;in u0444u043fu043eu0440 (t) = 0.1 u0444u043fu043eu0440 max, where max is the maximum value of u0444u043fu043eu0440 u0444u043fu043eu0440 (t).;4.the device u0434u043bu00a0 night and / or a u043du0430u0431u043bu044eu0434u0435u043du0438u00a0 remote object containing the transmitting channel pulse laser, which is connected with the exit block u043fu0438u0442u0430u043du0438u00a0 and management u043bu0435u043du0438u00a0 laser and optically u0441u043eu043fu0440u00a0u0436u0435u043du043du044bu0439 with the transmitting optical system, a first receiving channel, a first lens, optically u0441u043eu043fu0440u00a0u0436u0435u043du043du0443u044e with him u0444u043fu0437u0441 - u043cu0430u0442u0440 u0438u0446u0443 and monitor, with the length of one frame u0444u043fu0437u0441 matrix u0441u043eu0441u0442u0430u0432u043bu00a0u0435u0442 tc.and its outlet is connected with the front of the monitor, and the second receiving channel, the second a lens and optically u0441u043eu043fu0440u00a0u0436u0435u043du043du044bu0439 with photodiode, with the device. the possibility of u043eu043fu0440u0435u0434u0435u043bu0435u043du0438u00a0 time t u0440u0430u0441u043fu0440u043eu0441u0442u0440u0430u043du0435u043du0438u00a0 u0438u0437u043bu0443u0447u0435u043du0438u00a0 from the transmitting channel to the object, u043eu0442u043bu0438u0447u0430u044eu0449u0435u0435u0441u00a0, introduced the u0443u043fu0440u0430u0432u043bu0435u043du0438u00a0 executed in agriculture u043eu0436u043du043eu0441u0442u044cu044e u0443u043fu0440u0430u0432u043bu0435u043du0438u00a0 forming a series of m pulses, where m2.the length of the first laser pulse. u0434u043bu00a0 u0438u0437u043cu0435u0440u0435u043du0438u00a0 time t and the subsequent (m - 1) laser pulses;u0434u043bu00a0 u0444u043eu0440u043cu0438u0440u043eu0432u0430u043du0438u00a0 u0438u0437u043eu0431u0440u0430u0436u0435u043du0438u00a0 object, as well as the possibility of u0441u043cu0435u0449u0435u043du0438u00a0 started each of the laser pulses from the beginning of the frame u0444u043fu0437u0441 matrix on the u0432u0440u0435u043cu00a0 u0442u0443u043fu0440.if = tc (4u0442 - Lu043fu043eu0440n / (c) and u0441u043cu0435u0449u0435u043du0438u00a0 the beginning of each period u043du0430u043au043eu043fu043bu0435u043du0438u00a0 u0444u043fu0437u0441 matrix from the first frame to the u0432u0440u0435u043cu00a0, the output diode is connected to the entrance of the block u0443u043fu0440u0430u0432u043bu0435u043du0438u00a0, p u0435u0440u0432u044bu0439 exit block is connected with the entrance of u0443u043fu0440u0430u0432u043bu0435u043du0438u00a0 u043fu0438u0442u0430u043du0438u00a0 and u0443u043fu0440u0430u0432u043bu0435u043du0438u00a0 pulse laser, and the second exit to the entrance of u0443u043fu0440u0430u0432u043bu0435u043du0438u00a0 u0444u043fu0437u0441 matrix.;5. device for u043eu0442u043bu0438u0447u0430u044eu0449u0435u0435u0441u00a0 p.4, so that the block u0443u043fu0440u0430u0432u043bu0435u043du0438u00a0 has the opportunity u0443u043fu0440u0430u0432u043bu0435u043du0438u00a0 forming additional k series of pulses, of which the u043au0430u0436u0434u0430u00a0 u0436u0438u0442 m pulses, of which the first pulse is equal to a length of each of the subsequent (m - 1) in each of the series of pulses is equal to;6. device for u043eu0442u043bu0438u0447u0430u044eu0449u0435u0435u0441u00a0 paragraph 4 or 5, so that Lu043fu043eu0440 u043eu043fu0440u0435u0434u0435u043bu00a0u044eu0442 of u0441u043eu043eu0442u043du043eu0448u0435u043du0438u00a0 u0434u043bu00a0 instantaneous power interference of reverse u0440u0430u0441u0441u0435u00a0u043du0438u00a0 u0444u043fu043eu0440 (t):;q sb pos = "post" r / sb and sb & omega; pos = "post" b / sb d sb pos = "post" of / sb & hairsp; sp pos = "post" 2 / x (& sp pi;) u0435u0445u0440 (2 & alpha; sb pos = "post" r / sb l sb pos = "post" since / sb 4 sb pos = "post" b / sb & hairsp; sp pos = "post" 2 sp /;u0444u043fu043eu0440 (t) = ------------------------- u0435u0445u0440 [----------------];4 (l sb pos = "post" since / sb sp pos = "post" 2 / sp (& omega ; sp pos = "post" 2 / sp & hairsp; sb pos = "post" a + / sb & omega; sp pos = "post" 2 / sp & hairsp; sb pos = "post" b / sb ) (l sb pos = "post" since / sb sp pos = "post" 2 / (& sp omega; sp pos = "post" 2 / sp & hairsp; sb pos = "post" a / sb + s & omega; p pos = "post" 2 / sp & hairsp; sb pos = "post" b / sb );in u0444u043fu043eu0440 (t) = 0.1 u0444u043fu043eu0440 max, where max is the maximum value of u0444u043fu043eu0440 u0444u043fu043eu0440 (t).;7. device for u043eu0442u043bu0438u0447u0430u044eu0449u0435u0435u0441u00a0 paragraph 4 or 5, so that a block u0443u043fu0440u0430u0432u043bu0435u043du0438u00a0 u0438u0441u043fu043eu043bu044cu0437u0443u0435u0442u0441u00a0 microprocessor.;8. device for u043eu0442u043bu0438u0447u0430u044eu0449u0435u0435u0441u00a0 paragraph 4 or 5, so that a diode u0438u0441u043fu043eu043bu044cu0437u0443u0435u0442u0441u00a0 avalanche photodiode.
机译:1.和/或 u043d u0430 u0431 u043b u044e u0434 u0435 u043d u0438 u00a0远程对象的方法,它们形成一系列m个激光脉冲 u0438 u0437 u043b u0443 u0447 u0435 u043d u0438 u00a0其中m2,具有第一脉冲激光 u0438 u0437 u043b u0443 u0447 u0435 u043d u043d u0438 u00a0 u043d u0430 u043f u04f u0440 u0430 u0432 u043b 物体上的u00a0 u044e u0442会从物体辐射中反射出来,并且 u043e u043f u0440 u0435 u0434 u0435 u043b u00a0 u044e u0442 u0432 u0440 u0435 u0435 u043c u00a0 t u0440 u0430 u0441 u043f u0440 u043e u0441 u0442 u0440 u0430 u043d u0435 u043d u0438 u00a0 u0438 u0437 u043b u0443 u0447 u0435 u0435 u043d u0438 u00a0激光 u0438 u0437 u043b u0443 u0447 u0435 u043d u0438 u00a0, u043d u0430 u043f u0440 u0430 u0430 u0430 u0430 u043d u0435 u043d u04438 u044e u0442将它们放在物体上并通过接收透镜,并与他光学地 u0441 u043e u043f u0440 u00a0 u0436 u0435 u043d u043d u043e u0439 tc帧中的 u0444 u043f u0437 u0441矩阵从对象辐射反射并接收其图像 u043e u0442 u043b u0438 u0447 u0430 u044e u0449 u0438 u0439 u0441 u00a0第一个脉冲激光器 u0438 u0437 u043b u0443 u0447 u0435 u043d u0438 u00a0形状的长度和后续脉冲s(u-1)的长度(m-1) u043e u043f u0440 u0435 u0434 u0441 u043e u043e u0442 u043d u043d u043e u0448 u0435 u043d u0438的u0435 u043b u00a0 u044e u0442;其中L u043f u043e u043e u0440范围 u0444 u043e u0440 u043c u040 u0440 u043e u0432 u0430 u043d u0438 u00a0静态逆 u0440 u0430 u0441 u0441 u0435 u00a0 u043d u0438 u00a0 ;; n是平均值 u043f u0440 u0435 u043b u043e u043c u043b u0435 u043d u0438 u00a0大气;因此导致从帧的开始开始每个(m-1)个激光脉冲开始 u0444 u043f u0437 u0432 u0440 u0435 u043c u00a0 u0442 u0443 u043f u0440上的 u0441矩阵。 u043b u0438 = T u043a-(4 u0442-L u043f u043e u0440n / c),以及每个周期的开始 u043d u0430 u043a u043e u043f u043b u0435 u043d u0438 u00a0 u0444 u043f u0437 u0441-导致帧起始的矩阵任务; 2。 u043e u0442 u043b u0438 u0447 u0430 u044e u0449 u0438 u0439 u0441 u00a0 1的方法,以便进一步形成k系列脉冲,其中k1, u043a u0430 u0436 u0434 u0430 u00a0包含m个脉冲,以在帧 u0432 u0440 u0435 u043c u00a0 u0442 上的每个后续激光脉冲序列中,使第一激光束从帧的开头开始 u0444 u043f u0437 u0441矩阵u0443 u043f u0440。 u043b u0438,以前的一系列激光脉冲; 3。 u043e u0442 u043b u0438 u0447 u0430 u044e u0449 u0438 u0439 u0441 u00a0 1或2的方法,这样L u043f u043e u0440 u043e u043f u0440 u0435 u0434 u043e u0441 u043e u043e u043e u0442 u043d u043d u043e u0448 u0435 u043d u0438 u00a0的u0435 u043b u00a0 u044e u0442 u0440 u0430 044的反向瞬时功率干扰u0441 u0435 u00a0 u043d u0438 u00a0 u0444 u043f u043e u0440(t):; q r < / sb> and b < / sb> d &发的“ post ”> < /> x(&sp pi;) u0435 u0445 u0440(2&alpha; r < / sb> l 因为< / sb> 4 b < / sb>&hairsp; sp> < /; u0444 u043f u043e u0440(t)= ---------------------------- u0435 u0445 u0440 [ ----------------]; 4(l 因为< / sb> < / sp(&omega>; < / sp>&hairsp; a> + < / sb&omega; < / sp>&hairsp; b < / sb>)(l 因为< / sb> < />(&sp omega; < / sp>&hairsp; a < / sb> + < / sp>&hairsp; b < / sb>);其中Q u043b- u044d u043d u0435 u0440 u0433 u0438 u00a0激光;; x(a)= 0,33S-0.33L u043f u043e u0440-值 u0438 u043d u043d u0434 u0438 u043a u0430 u0442 u0440 u0 438 u0441 u044b朝向“ back ”; s是 u0440 u0430 u0441 u0441 u0435 u00a0 u043d u0438 u00a0气氛;; p是 u0440 u0430 u0441 u0441的比率 u0435 u00a0 u043d u0438 u00a0气氛;; ol,每个字段 u0437 u0440 u0435 u043d u0438 u00a0发散 u0438 u0437 u043b u0443 u0447 u0435 u043d u0438 u00a0分别为接收器和发送器。D u043e u0431-接收直径镜头; u0445 u0431-接收和发射系统之间的线性视差;;在 u0444 u043f u043e u0440(t)= 0.1 u0444 u043f u043e u0440 max中,其中max是 c的最大值u0444 u043f u043e u0440 u0444 u043f u043e u0440(t)。; 4。设备 u0434 u043b u00a0晚上和//或 u043d u0430 u0431 u043b u043b u044e u0434 u0435 u043d u0438 u00a0包含发射通道脉冲激光的远程对象,该远程对象与出口模块 u043f u0438 u0442 u0430 u043d u0438 u00a0和管理 u043b u0435 u043d u0438 u00a0激光器和 u0441 u043e u043f u0440 u00a0 u0436 u0435 u043d u043d u044b u0439与发送光学系统,第一接收通道,第一透镜在光学上 u0441 u043e u043e u043f u0440 u00a0 u0436 u0435 u043d u043d u0443 u044e和他一起 u0444 u 043f u0437 u0441- u043c u0430 u0442 u0440 u0438 u0446 u0443和显示器,具有一帧的长度 u0444 u043f u0437 u0441矩阵 u0441 u043e u043e u0441 u0442 u0430 u0432 u043b u00a0 u0435 u0442 tc。其出口与显示器的正面相连,第二个接收通道与第二个接收通道相连,第二个为透镜,并在光学上 u0441 u043e u043f u0440 u00a0 u0436 u0435 u043d u043d u044b u0439带有光电二极管和设备。 u043e u043f u0440 u0435 u0434 u0435 u043b u0435 u043d u043d u00438 u00a0时间t u0440 u0430 u0441 u043f u0440 u043e u0441 u0441 u0442 u0440 u0430 u043d u0435 u043d u0438 u00a0 u0438 u0437 u043b u0443 u0447 u0435 u043d u0438 u00a0从传输通道到对象 u043e u0442 u043b u0438 u0447 u0430 u044e u0449 u0435 u0435 u0441 u00a0,介绍了在农业中执行的 u0443 u043f u0440 u0430 u0432 u043b u0435 u043d u0438 u00a0 u043e u0436 u043d u043d u043d u043e u0441 u0442 u044c u044e u0443 u043f u0440 u0430 u0432 u043b u0435 u043d u0438 u00a0形成一系列m个脉冲,其中m2。第一个激光脉冲的长度。 u0434 u043b u00a0 u0438 u0437 u043c u0435 u0440 u0435 u043d u0438 u00a0时间t和随后的(m-1)个激光脉冲; u0434 u043b u00a0 u0444 u043e u0440 u043c u0438 u0440 u043e u0432 u0430 u043d u0438 u00a0 u0438 u0437 u043e u0431 u0440 u0430 u0436 u0435 u043d u0438 u00a0对象以及 u0441 u043c u0435 u0449 u0435 u043d u0438 u00a0从 u0432 u0440 u0435 u043c u043c u00a0 u0442 u0443的帧 u0444 u043f u0437 u0441矩阵的开头开始每个激光脉冲 u043f u0440.if = tc(4 u0442-L u043f u043e u0440n /(c)和 u0441 u043c u0435 u0449 u0435 u043d u0438 u00a0每个周期的开始 u043d u0430 u043a u043e u043f u043b u0435 u043d u0438 u00a0 u0444 u043f u0437 u0441矩阵从第一帧到 u0432 u0440 u0435 u043c u00a0,输出二极管连接到块的入口 u0443 u043f u0440 u0430 u0432 u043b u0435 u043d u0438 u00a0,p u0435 u0440 u0432 u044b u0439出口块与入口连接 u0443 u043f u0440 u0430 u0432 u043b u0435 u043d u04438 u00a0 u043f u0438 u0442 u0430 u043d u0438 u00a0和 u0443 u043f u0440 u0430 u0432 u0435 u043d u0438 u00a0脉冲激光,第二个出口是 u0443 u043f u0440 u0430 u0432 u043b u0435 u043d u043d u0438 u00a0 u0444 u043f u043f u0437 u0441矩阵的入口。; 5 。 u043e u0442 u043b u0438 u0447 u0430 u044e u0449 u0435 u0435 u0441 u00a0 p.4的设备,因此块 u0443 u043f u0440 u0430 u0430 u0432 u043b u0435 u043d u0438 u00a0有机会 u0443 u043f u0440 u0430 u0432 u043b u0435 u043d u0438 u00a0形成额外的k系列脉冲,其中 u043a u0430 u0436 u0434 u0434 u0430 u00a0 m个脉冲,其中第一个脉冲等于每个脉冲序列中的每个后续脉冲的长度(m-1)等于6.。 u043e u0442 u043b u0438 u0447 u0430 u044e u0449 u0435 u0435 u0441 u00a0第4或5段的设备,这样L u043f u043e u0440 u043e u043f u0440 u0435 u0434 u0435 u043b u00a0 u044e u0442的 u0441 u043e u043e u0442 u043d u043d u043e u0448 u0435 u043d u0438 u00a0 u0434 u043b u00a0反向功率瞬时干扰 u0440 u0430 u0441 u0441 u0435 u00a0 u043d u0438 u00a0 u0444 u043f u043e u0440(t):; q r < / sb>和 b < / sb> d &发的“ post ”> < /> x(&sp pi;) u0435 u0445 u0440(2&alpha; r < / sb> l 因为< / sb> 4 b < / sb>&hairsp; sp> < /; u0444 u043f u043e u0440(t)= ------------------------- u0435 u0445 u0440 [- -------------]; 4(l 因为< / sb> < / sp( &omega>; < / sp>&hairsp; a> + < / sb&omega; < / sp>&hairsp; b < / sb>)(l 因为< / sb> < />(&sp omega; < / sp>&hairsp; a < / sb> + < / sp>&hairsp; b < / sb>);在 u0444 u043f u043e u0440(t)= 0.1 u0444 u043f u043e u0440 max,其中max是 u0444 u043f u043e u0440 u0444 u043f u043e u0440(t)的最大值。; 7.设备对于 u043e u0442 u043b u0438 u0447 u0430 u044e u0449 u0435 u0435 u0441 u00a0第4或5段,因此,一个块 u0443 u043f u0440 u0430 u0432 u0432 u043b u0435 u043d u0438 u00a0 u0438 u0441 u043f u043e u043b u044c u0437 u0443 u0435 u0442 u0441 u00a0微处理器; 8。 u043e u0442 u043b u0438 u0447 u0430 u044e u0449 u0435 u0435 u0441 u00a0第4或5段的设备,因此二极管 u0438 u0441 u043f u043e u043e u043b u044c u0437 u0443 u0435 u0442 u0441 u00a0雪崩光电二极管。

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