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    • 2. 发明授权
    • Scanning laser for a scanning laser radar
    • US4528525A
    • 1985-07-09
    • US296076
    • 1981-08-25
    • Dayton D. EdenWilliam E. Case
    • Dayton D. EdenWilliam E. Case
    • G01S7/481G01S7/491G01S17/42G02F2/00H01S3/086H01S3/10H04N7/18
    • G02F2/002G01S17/42G01S7/4812G01S7/4911G01S7/4917H01S3/086H01S3/10
    • In an optical radar system a coherent signal is transmitted at a variable position and the return signal, that is, the reflected portion of the coherent signal is received and coherently detected. The transmitter utilizes a scanning laser having an electron beam that impinges upon a variable reflectance mirror that terminates one end of an optical cavity. An oscillating mode is generated within the resonant cavity when the electron beam locally heats the surface of the variable reflectance mirror to create a pixel that reflects light in a diffracted pattern. The receiver utilizes a stable single mode laser to illuminate a variable reflectance surface. A receiver electron beam generates a plurality of receiver pixels at various positions. The diffracted light from each pixel generates a plurality of variable angle local oscillator beams that are summed with the return signal at a beamsplitter. The output of the beamsplitter is applied to the surface of a detector array. One of the local oscillator beams is positioned such that the return signal and the local oscillator beam overlap at one of the detectors in the array to provide coherent detection. The frequency of the first coherent signal and the second coherent signal are sampled by a first and second partially reflecting mirror. A frequency detector detects the output of the first and second partially reflecting mirror to detect the frequency difference between the first and second coherent signal and generate a control signal that adjusts the frequency of the first coherent signal. For heterodyne operation a selected frequency difference is generated whereas for homodyne detection a zero frequency difference is generated. An electronic computer coordinates the position of the scanning laser of the transmitter and the position of the local oscillator beams of the receiver such that one of the local oscillator beams will overlap with each of the corresponding return signals at the detector array. A second electronic computer processes the output of the detector array to provide information about the return signal.
    • 4. 发明授权
    • Electronic imaging by encoded image detection
    • 电子成像通过编码图像检测
    • US5737075A
    • 1998-04-07
    • US354669
    • 1994-12-13
    • Mark E. KochWilliam E. Case
    • Mark E. KochWilliam E. Case
    • G01J3/04G01J5/08
    • G01S17/89G01S7/4816H04N5/217H04N5/30
    • A new system for millimeter wave electronic imaging is described. This system utilizes a spatial light modulator in the focal plane of the collection optics. Each pixel of the modulator is driven by a specific high duty cycle modulation function provided by a modulation function generation circuit. Thus the throughput radiation at each pixel is uniquely labeled(encoded). A post modulation detector sums the signal from all the pixels. Subsequent to detection, the appropriate transform of the sum signal yields specific pixel throughput radiation intensity levels. Several configurations are described including one transmittance configuration and two reflectance configurations. Three specific millimeter wave transmittance embodiments and one reflectance embodiment are also described.
    • 描述了一种用于毫米波电子成像的新系统。 该系统在收集光学器件的焦平面中利用空间光调制器。 调制器的每个像素由调制函数生成电路提供的特定高占空比调制功能驱动。 因此,每个像素处的吞吐量辐射被唯一地标记(编码)。 后调制检测器将来自所有像素的信号相加。 在检测之后,和信号的适当变换产生特定像素吞吐量辐射强度水平。 描述了一些配置,包括一个透射率配置和两个反射配置。 还描述了三个具体的毫米波透射率实施例和一个反射率实施例。
    • 5. 发明授权
    • Method and apparatus for population inversion
    • 种群倒置的方法和装置
    • US4477906A
    • 1984-10-16
    • US370174
    • 1982-04-20
    • William E. Case
    • William E. Case
    • H01S3/091H01S3/16
    • H01S3/16H01S3/091
    • Stimulated emission at the approximate wave length of 4.5 microns, 2.25 microns and 1.6 microns is obtained from pumping on an excited energy level. The phenomenon of photon avalanching is utilized to create a population inversion within three lower level states that have a substantially equal energy spacing to provide resonance between neighboring ions. This resonance feeds the photon avalanching process when pump having sufficient power in excess of the critical pump power irradiates a LaCl.sub.3 :Pr.sup.+3 crystal at an excited energy level to maintain a population inversion in an optical cavity.
    • 在激发能级泵浦获得在4.5微米,2.25微米和1.6微米近似波长的受激发射。 利用光子雪崩的现象,在三个较低级别的状态下产生具有基本上相等的能量间隔以提供相邻离子之间共振的群体反演。 当泵具有超过临界泵浦功率的足够功率的泵以激发能级照射LaCl 3 :Pr + 3晶体以维持光腔中的群体反转时,该共振馈送光子雪崩过程。