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    • 1. 发明授权
    • Method of making fusible spacer for display panel
    • 制作显示面板的易熔垫片的方法
    • US4428764A
    • 1984-01-31
    • US334492
    • 1981-12-28
    • Elias SnitzerRobert E. Wisnieff
    • Elias SnitzerRobert E. Wisnieff
    • C03B23/24C03B37/027H01J9/26C03B37/025
    • C03B23/245C03B37/027H01J9/261
    • A fusible spacer for use in the manufacture of a plasma panel rigidly maintains a preselected spacing between the panel sidewalls. The fusible spacer comprises a core fabricated from a refractory glass, such as R-6 glass, and has a first transverse dimension sized in accordance with the desired spacing between the panel sidewalls. A cladding surrounds the core along and is formed from a material which has a much lower softening point, i.e., 350.degree. C. to 500.degree. C. The separation between the two halves of the panel is set by the first dimension of the core member while the solder glass cladding is fused to rigidly attach to both panel sidewalls bonding the composite structure together. The core and fusible cladding are drawn to size by covering the cladding with a second transitory cladding of the same material as the core material to allow a dimensionally controlled fiber to be drawn even through the fusible cladding has a substantially lower softening point. The core member can have a circular cross section or numerous other cross sections so long as the first transverse dimension defines the panel spacing and the second transverse dimension is not too large to interfere with the discharge sites between row and column electrodes.
    • 用于制造等离子体面板的可熔间隔件在面板侧壁之间刚性地保持预选的间隔。 可熔隔片包括由诸如R-6玻璃的耐火玻璃制成的芯,并且具有根据板侧壁之间的期望间隔尺寸的第一横向尺寸。 芯包层围绕芯并且由具有低得多的软化点,即350℃至500℃的材料形成。板的两个半部之间的间隔由芯部件的第一尺寸 而焊料玻璃包层被熔合以刚性附接到将复合结构粘合在一起的两个面板侧壁。 通过用与芯材料相同的材料的第二短暂包层覆盖包层将核心和可熔覆层拉伸到尺寸,以允许尺寸受控的纤维甚至通过可熔覆层具有较低的软化点。 芯构件可以具有圆形横截面或许多其它横截面,只要第一横向尺寸限定面板间隔,并且第二横向尺寸不会太大而不能干扰行电极和列电极之间的放电位置。
    • 4. 发明授权
    • Optical amplifier
    • 光放大器
    • US4712075A
    • 1987-12-08
    • US802369
    • 1985-11-27
    • Elias Snitzer
    • Elias Snitzer
    • H01S3/05H01L31/14H01S3/06H01S3/067H01S3/083H01S3/094H01S3/131H01S5/00H04B10/00H04B10/16H04B10/17H04B10/22H01S3/00
    • H01S3/083H01S3/06754H01S3/094003H01S3/131
    • An optical amplifier particularly suitable for use in amplifying signals carried on optical fiber in a select communication band. The amplifier comprises a resonant optical waveguide cavity which has a core containing an active gain material with given absorption and fluorescence spectrums. The gain material is of the type that preferably has at least two different emission bands originating from the same energy level with one of the emission bands encompassing the select communication band. The cavity is structured to resonate wavelengths in both emission bands, but with a higher combination of cavity Q and gain coefficient per excited ion for wavelengths in the emission band not corresponding to the select communication band so that, when pumped, the cavity first lases at this band. The lasing action causes the atomic population of the gain material corresponding to the communication band to remain at a stable constant level where it is available to uniformly amplify by stimulated emission optical signals introduced into the cavity.
    • 一种光放大器,特别适用于放大选择通信频带中的光纤上承载的信号。 放大器包括具有包含具有给定吸收和荧光光谱的有源增益材料的芯的谐振光波导腔。 增益材料的类型优选地具有源自与包围选择通信频带的发射频带中的一个相同的能级的至少两个不同的发射带。 空腔被构造成在两个发射频带中谐振波长,但是对于不对应于选择通信频带的发射频带中的波长,腔体Q和每个激发离子的增益系数的组合较高,使得当泵浦时,空腔首先在 这个乐队。 激光作用使得与通信带相对应的增益材料的原子群保持在稳定的恒定水平,其中可用于通过被引入空腔的受激发射光信号均匀放大。
    • 5. 发明授权
    • Super radiant light source
    • 超级光源
    • US4637025A
    • 1987-01-13
    • US663345
    • 1984-10-22
    • Elias SnitzerShaoul Ezekiel
    • Elias SnitzerShaoul Ezekiel
    • G02B6/42G01C19/72G02B6/02H01S3/06H01S3/067H01S3/08H01S3/094H01S5/00H01S3/00
    • H01S3/08059G01C19/721G02B6/02H01S3/06795H01S3/094003
    • A super-radiant light source having an output with a low temporal coherence well suited, for example, to optical inertial sensor applications, includes a single mode optical waveguide such as an optical fiber having its core doped with an active laser material, such as neodymium. Pump light is coupled into the optical fiber at an intensity sufficient to produce a significant amplification of the spontaneous emission. The reflectivity at the exit end of the fiber is low enough so that even with a high gain for the light in one traverse through the fiber, the fiber is operated well below threshold for laser oscillation. The resulting emission is of high intensity, but has a low temporal coherence. In one form, the pump light is coupled into one end of the fiber and a dichroic filter is interposed in the light path between the pump light and the optical fiber to pass pump light into the core and reflect the spontaneous emission of the active material back into the core and toward the output.
    • 具有非常适合于例如光学惯性传感器应用的具有低时间相干性的输出的超辐射光源包括单模光波导,例如其核掺杂有活性激光材料的光纤,例如钕 。 泵浦光以足以产生自发发射的显着放大的强度耦合到光纤中。 光纤出口端的反射率足够低,使得即使在光纤穿过光纤时光的高增益,光纤的运行也远低于激光振荡的阈值。 所产生的发射强度高,但时间一致性较低。 在一种形式中,泵浦光耦合到光纤的一端,并且在泵浦光和光纤之间的光路中插入二向色滤光器,以将泵浦光引导到芯中并将活性材料的自发发射反射回 进入核心并朝向产出。