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    • 1. 发明授权
    • Structure and manufacturing method for single-wavelength and multi-wavelength distributed feedback lasers
    • 单波长和多波长分布反馈激光器的结构和制造方法
    • US07012944B2
    • 2006-03-14
    • US10636103
    • 2003-08-07
    • San-Liang LeeIng-Fa Jang
    • San-Liang LeeIng-Fa Jang
    • H01S3/19H01S3/08
    • H01S5/12H01S5/0654H01S5/1203H01S5/1209H01S5/4087H01S2301/173H01S2304/00
    • A single-wavelength distributed feedback (DFB) laser structure is provided. The laser structure having two sections includes an active-material layer for generating a laser having a wavelength in a specific range, two cladding layers respectively covering an upper and a bottom sides of the active-material layer for forming a waveguide structure, a phase shift layer having a specific thickness for controlling a difference between Bragg wavelengths of the two sections, a wet-etching stop layer positioned between the active-material layer and the phase shift layer, and a grating layer having a specific period for determining an illuminating wavelength, wherein a difference between the two sections is an existence of the phase shift layer thereon, and the existence of the phase shift layer causes a difference of the effective refractive indices between the two sections so as to generate a fixed difference between Bragg wavelengths of the two sections.
    • 提供单波长分布反馈(DFB)激光器结构。 具有两个部分的激光器结构包括用于产生具有特定范围波长的激光的活性材料层,分别覆盖用于形成波导结构的活性材料层的上侧和下侧的两个包覆层,相移 具有用于控制两个部分的布拉格波长之间的差异的特定厚度的层,位于活性材料层和相移层之间的湿蚀刻停止层以及具有用于确定照明波长的特定周期的光栅层, 其中两部分之间的差异是其上的相移层的存在,并且相移层的存在导致两部分之间的有效折射率差异,以便产生两个部分的布拉格波长之间的固定差异 部分。
    • 6. 发明授权
    • Semiconductor diode laser, and method of manufacturing thereof
    • 半导体二极管激光器及其制造方法
    • US6078603A
    • 2000-06-20
    • US988597
    • 1997-12-11
    • Leo M. WeegelsHenricus M. De VriezeMaria H. C. Vermeulen-Hartjes
    • Leo M. WeegelsHenricus M. De VriezeMaria H. C. Vermeulen-Hartjes
    • H01S5/065H01S5/02H01S5/028H01S5/062H01S5/10H01S5/32H01S3/19
    • H01S5/06216H01S5/028H01S5/0658H01S5/10H01S5/1082
    • A diode laser is disclosed that is self-pulsating without an increase in the starting current or a decrease in the efficiency. A special coating on an end face of the laser comprises in order a first mirror, a medium having an optical thickness which is at least substantially equal to an integer number of times half the wavelength of the generated electromagnetic radiation, and a second mirror. The coating comprises exclusively materials which have a higher bandgap value than that which corresponds to the wavelength of the generated radiation, while the reflectivities of the mirrors and the deviation of the optical thickness of the medium with respect to an integer number of times half the emission wavelength are chosen such that the group velocity dispersion (GVD) adjacent the wavelength of the generated electromagnetic radiation is negative, and preferably a minimum. Pulse widening owing to pulses arising from automatic mode locking is no longer possible due to a sufficiently negative group velocity dispersion. A laser exhibiting stable self-pulsation is thus provided.
    • 公开了一种二极管激光器,其在不增加启动电流或效率降低的情况下是自脉动的。 激光器端面上的特殊涂层按顺序包括第一反射镜,具有至少基本上等于产生的电磁辐射的波长的一半的光学厚度的介质和第二反射镜。 涂层仅包括具有比对应于所产生的辐射的波长的带隙值更高的带隙值的材料,而反射镜的反射率和介质的光学厚度相对于发射的一半的整数倍的偏差 选择波长,使得与所产生的电磁辐射的波长相邻的群速度色散(GVD)为负,优选为最小。 由于自动模式锁定引起的脉冲,由于充分的负组速度色散,不再可能产生脉冲加宽。 因此提供了表现出稳定的自脉动的激光。
    • 7. 发明授权
    • N-drive or P-drive VCSEL array
    • N驱动或P驱动VCSEL阵列
    • US6069908A
    • 2000-05-30
    • US20724
    • 1998-02-09
    • Albert T. YuenMichael R. T. TanChun Lei
    • Albert T. YuenMichael R. T. TanChun Lei
    • H01S5/00H01S5/02H01S5/042H01S5/183H01S5/187H01S5/42H01S3/19
    • H01S5/183H01S5/423H01S5/0208H01S5/0422
    • A VCSEL that is adapted to the fabrication of an array of VCSELs. A VCSEL array according to the present invention includes first and second VCSELs for generating light of a predetermined wavelength. Each VCSEL includes a bottom reflector comprising an epitaxial layer of a semiconductor of a first conductivity type, a light generation region and a top reflector comprising a semiconductor of a second conductivity type. A bottom electrode is electrically connected to the bottom reflector, and a top electrode is electrically connected to the top reflector. The bottom electrode is grown on top of a buffer layer having an electrical conductivity less than a predetermined value and a crystalline structure that permits epitaxial growth of the bottom reflector on the buffer layer. The buffer layer may be grown on top of a substrate or be the substrate itself in the case in which a substrate having sufficiently low conductivity is utilized. The bottom reflector of each of the VCSELs is in contact with the top of the buffer layer. The first and second VCSELs are electrically isolated from one another by a trench extending into the buffer layer. The buffer layer is constructed from a material having resistivity that is sufficiently low to prevent cross-talk between the first and second VCSELs.
    • 适用于制造VCSEL阵列的VCSEL。 根据本发明的VCSEL阵列包括用于产生预定波长的光的第一和第二VCSEL。 每个VCSEL包括底部反射器,其包括第一导电类型的半导体的外延层,发光区域和包括第二导电类型的半导体的顶部反射器。 底部电极电连接到底部反射器,并且顶部电极电连接到顶部反射器。 底部电极生长在具有小于预定值的电导率的缓冲层的顶部上,并且允许底部反射器在缓冲层上外延生长的晶体结构。 在使用具有足够低的导电性的基板的情况下,可以在衬底的顶部生长缓冲层或者作为衬底本身。 每个VCSEL的底部反射器与缓冲层的顶部接触。 第一和第二VCSEL通过延伸到缓冲层中的沟槽彼此电隔离。 缓冲层由具有足够低的电阻率的材料构成,以防止第一和第二VCSEL之间的串扰。
    • 10. 发明授权
    • Quantum cascade light emitter with pre-biased internal electronic
potential
    • 量子级联发光器具有预偏置内部电子电位
    • US6055254A
    • 2000-04-25
    • US159127
    • 1998-09-23
    • Federico CapassoAlfred Yi ChoClaire F. GmachlAlbert Lee HutchinsonDeborah Lee SivcoAlessandro Tredicucci
    • Federico CapassoAlfred Yi ChoClaire F. GmachlAlbert Lee HutchinsonDeborah Lee SivcoAlessandro Tredicucci
    • H01L29/06H01L29/15H01S5/34H01S5/343H01S3/18H01S3/19
    • B82Y20/00H01S5/3402
    • Instead of trying to keep the SLs of a QC laser field free, we "pre-bias" the actual electronic potential by varying the SL period (and hence average composition) so as to achieve an essentially flat profile, on average, of upper and lower minibands, despite the presence of an applied field in the SLs. In one embodiment, in at least a first subset of the QW layers, the thicknesses of the QW layers are varied from QW layer to QW layer so as to increase in the direction of the applied field. In this embodiment, the upper and lower lasing levels are located, in the absence of an applied electric field, each at different energies from layer to layer within the first subset, so that despite the presence of an applied field, the desired flatband condition of the upper and lower minibands is realized. In a preferred embodiment, the thicknesses of the QW layers within the first subset are varied from QW layer to QW layer so as to increase in the direction of the applied field, and the thicknesses of a second subset of the barrier layers are also varied from barrier layer to barrier layer so as to decrease or increase in the direction of the applied field.
    • 不要试图保持QC激光场的SL不受限制,我们通过改变SL周期(因此平均组成)来“预先偏置”实际的电子电位,以便平均地获得上部和 尽管在SL中存在应用场,但是较低的迷你频段。 在一个实施例中,在QW层的至少第一子集中,QW层的厚度从QW层到QW层变化,以便在施加场的方向上增加。 在该实施例中,在没有所施加的电场的情况下,上和下激光电平各自处于第一子集内的层与层之间的不同能量,使得尽管存在施加的场,但是期望的平带条件 实现上下两个迷你吧。 在优选实施例中,第一子集内的QW层的厚度从QW层到QW层变化,以便在施加的场的方向上增加,并且阻挡层的第二子集的厚度也从 阻挡层到阻挡层,以便在施加的场的方向上减小或增加。