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    • 7. 发明申请
    • IMPROVEMENTS IN OR RELATING TO LIGHT BEAM MODULATION
    • 改进或涉及光束调制
    • WO1988008998A1
    • 1988-11-17
    • PCT/US1988001451
    • 1988-05-03
    • EASTMAN KODAK COMPANY
    • EASTMAN KODAK COMPANYMAUER, Paul, BernardNARAYAN, BadhriRODDY, James, Edward
    • G02F01/21
    • H01S5/06213G02F1/21G02F2001/213H01S5/0622
    • Method and apparatus for modulating the collimated output beam (62) of a laser diode (56) whose emission frequency changes with the magnitude of the current supplied to the diode. The frequency changes occur by jumps (26), in which a relatively high rate of change of frequency occurs, and by drifts (28) between jumps (26). In the drifts (28), relatively low rates of change of frequency per unit variation in magnitude of current occur. The beam (38, 58) is directed onto an interferometer (30) for converting frequency modulation to amplitude modulation. The current to the diode (56) is varied by an amount less than the current needed to cause the drift (28) between successive jumps, whereby the frequency may be shifted by drifting between a frequency at which destructive interference occurs in the interferometer (30) and another frequency at which constructive interference occurs, without causing a jump in frequency.
    • 用于调制激光二极管(56)的准直输出光束(62)的方法和装置,其发射频率随提供给二极管的电流的大小而变化。 频率变化通过跳跃(26)发生,其中发生频率变化的相对较高的频率以及跳跃(26)之间的漂移(28)。 在漂移(28)中,电流幅度的单位变化频率变化率相对较低。 光束(38,58)被引导到用于将频率调制转换成幅度调制的干涉仪(30)。 到二极管(56)的电流的变化量小于在连续跳跃之间引起漂移(28)所需的电流,借此通过在干涉仪(30)中发生相消干涉的频率之间的漂移来移动频率 )和发生相长干扰的另一个频率,而不会引起频率的跳跃。
    • 9. 发明申请
    • SCANNING APPARATUS
    • 扫描仪
    • WO1987006016A1
    • 1987-10-08
    • PCT/US1987000670
    • 1987-03-30
    • EASTMAN KODAK COMPANY
    • EASTMAN KODAK COMPANYNARAYAN, BadhriRODDY, James, EdwardSTARK, Richard, AlanTHOMPSON, Dennis, Allen
    • G02B26/10
    • H04N1/1265G02B13/0005G02B13/10G02B26/106G06K7/10594H04N1/12
    • A scanner including a source (24) of coherent or substantially coherent light, a radial hologon (48), a f theta lens (60) and a target (64). Between the light source and the hologon there are means (32) for forming light from the source into a collimated beam having an oblong cross-sectional shape and for directing the beam onto the hologon at a predetermined incident angle and with the long axis of the oblong cross-sectional shape of the beam radial of the axis of rotation of the hologon. Prismatic means (36) are provided between the halogon and the lens means for so modifying the cross-sectional shape of the beam that the spot at the target station has a selected shape and orientation. This allows the shape, orientation and size of the beam on the hologon to be optimum for duty cycle of the hologon and for spot size on the target. The prismatic means (36) allows the spot shape and orientation on target to be optimized. The prismatic means tends to introduce undesirable bow into the scan line, therefore the wavelength of the light and the grating factor n lambda /d of the hologon are selected to produce an approximately equivalent opposite bow.
    • 一种扫描器,包括相干或基本上相干的光的源(24),径向hologon(48),fθ透镜(60)和目标(64)。 在光源和hologon之间存在用于将来自源的光形成为具有长方形横截面形状的准直光束并用于以预定入射角将光束引导到hologon上的装置(32) 长圆形横截面形状的梁的径向旋转轴的旋转。 棱镜装置(36)设置在卤素和透镜装置之间,以便改变目标台上的光斑具有所选形状和取向的横截面形状。 这允许hologon上的梁的形状,取向和尺寸对于hologon的占空比和目标上的点尺寸是最佳的。 棱镜装置(36)允许优化目标上的斑点形状和取向。 棱镜装置倾向于将不想要的弓引入扫描线,因此选择光的波长和hologon的光栅因子nλ/ d以产生大致相当的相对的弓。