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    • 1. 发明授权
    • Semiconductor laser or array formed by layer intermixing
    • 半导体激光器或由层间混合形成的阵列
    • US5708674A
    • 1998-01-13
    • US367554
    • 1995-01-03
    • Kevin J. BeerninkRobert L. ThorntonDavid P. BourThomas L. PaoliJack Walker
    • Kevin J. BeerninkRobert L. ThorntonDavid P. BourThomas L. PaoliJack Walker
    • H01S5/00H01L21/18H01S5/34H01S5/343H01S5/40H01S3/19
    • B82Y20/00H01L21/182H01S5/34H01S5/4043H01S5/3413H01S5/3414H01S5/3432H01S5/34326H01S5/4087
    • A fabrication process and several structures for an index-guided laser diode formed by IILD or for a multiple wavelength laser array containing stacked semi-conductive active layers with quantum wells. The laser wavelength is varied laterally by effectively inactivating quantum wells which have transition wavelengths longer than that desired in the selected portion of the device. The quantum wells are inactivated by intermixing them with the surrounding high band gap semiconductor layers. To accomplish this intermixing without affecting the active layer in nearby regions, a finite source of impurity inducing or promoting intermixing is located in proximity to the quantum well to be intermixed, and the sample is annealed under conditions which allow for lateral patterning of the impurity-induced intermixing. Alternatively, the body is capped over the quantum well to be inactivated with a material which induces vacancies in semi-conductive material during thermal annealing, thus promoting vacancy-enhanced intermixing of the undesired quantum well. The intermixing can also be brought about by patterned annealing or selective laser heating which produces local annealing, or by use of two different caps. For the index-guided laser diode, the flanking index-guiding regions are formed by IILD from a buried impurity source, in which surface conditions are controlled to promote impurity diffusion to the flanking regions but not to the active stripe region between the flanking regions.
    • 用于由IILD或包含具有量子阱的堆叠半导电有源层的多波长激光器阵列形成的折射率引导激光二极管的制造工艺和若干结构。 通过有效地使具有比器件所选部分中所需要的转换波长更长的量子阱来激活激光波长。 量子阱通过将它们与周围的高带隙半导体层混合而失活。 为了实现这种混合而不影响附近区域中的有源层,杂质诱导或促进混合的有限源位于量子阱附近,以便混合,并且样品在允许杂质 - 诱导混合。 或者,通过在热退火期间在半导电材料中引起空位的材料将物体盖在量子阱上以使其失活,从而促进不期望的量子阱的空位增强的混合。 混合还可以通过图案化退火或选择性激光加热产生局部退火,或通过使用两个不同的盖来实现。 对于折射率引导激光二极管,侧翼引导区域由埋藏杂质源的IILD形成,其中控制表面条件以促进杂质扩散到侧翼区域而不是侧向区域之间的有源条纹区域。
    • 8. 发明授权
    • Apparatus spot position control in an output device employing a linear
array of light sources
    • 在使用光源的线性阵列的输出装置中进行设备点位置控制
    • US5574491A
    • 1996-11-12
    • US195600
    • 1994-02-14
    • Thomas L. Paoli
    • Thomas L. Paoli
    • B41J2/44G01B11/00G02B26/10G05D3/12H04N1/047H04N1/113H04N1/12B41J2/435
    • H04N1/0473H04N1/1135H04N1/12H04N2201/0471H04N2201/04758
    • In a method and apparatus for raster scanning optical output device, such as a laser printer or the like, an array of independently addressable light emitting devices, such as an array of solid state lasers, is used to control spot position on an image plane in the slow scan direction. The array is disposed such that the spots emitted from each element of the array impinge the image plane displaced in the slow scan direction from one another. The total distance between all the spots is less than the distance between fast scan direction scan lines. Only a single element of the array is operated per scan line, thus only a single spot is formed on the image plane per scan line. Control of which of the elements of the array emits a light beam per scan line allows control of the spot position in the slow scan direction for that scan line.
    • 在诸如激光打印机等的光栅扫描光输出装置的方法和装置中,使用诸如固态激光器阵列的可独立寻址的发光装置的阵列来控制图像平面上的光点位置 慢扫描方向。 阵列被布置成使得从阵列的每个元件发射的光斑撞击在慢扫描方向上彼此移位的图像平面。 所有点之间的总距离小于快速扫描方向扫描线之间的距离。 每个扫描线仅对阵列的单个元件进行操作,因此在每个扫描线上的图像平面上仅形成一个点。 控制每个扫描线阵列中的哪个元件发射光束,可以控制该扫描线在慢扫描方向上的光点位置。
    • 10. 发明授权
    • Dynamic control of individual spot exposure in an optical output device
    • 光输出装置中单个点曝光的动态控制
    • US5497181A
    • 1996-03-05
    • US906145
    • 1992-06-29
    • Thomas L. Paoli
    • Thomas L. Paoli
    • B41J2/44G02B26/10G03B27/72G06K15/12H01L21/027G01D15/14
    • G06K15/1214
    • The optical energy per pulse emitted by a laser source is accurately controlled from pulse to pulse by controlling the duration of the pulse according to the integrated value of its amplitude over time. A control signal is formed by converting a portion of the optical output of the laser to an electrical signal with a photodetecting element whose electrical output signal is integrated over time. The laser excitation is terminated when the integrated photocurrent reaches a set threshold level representing the optical energy desired for the pulse. Accurate control of the optical energy in each pulse is maintained in spite of error producing conditions such as unpredictable fluctuations in the laser drive signal, ambient temperature fluctuations, transient heating, and cumulative effects due to sequences of pulses.
    • 通过根据其随时间的幅度的积分值控制脉冲的持续时间,由脉冲到脉冲来精确地控制由激光源发射的每个脉冲的光能。 通过将激光的光输出的一部分转换成具有电输出信号随时间积分的光检测元件的电信号而形成控制信号。 当集成光电流达到表示脉冲所需的光能的设定阈值电平时,激光激发终止。 尽管产生诸如激光驱动信号的不可预测的波动,环境温度波动,瞬态加热以及由于脉冲序列引起的累积效应的错误,仍维持每个脉冲中的光能的精确控制。