会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 4. 发明授权
    • Article comprising a strain-compensated QC laser
    • 文章包括应变补偿QC激光
    • US6023482A
    • 2000-02-08
    • US12300
    • 1998-01-23
    • Federico CapassoAlfred Yi ChoSung-Nee George ChuJerome FaistAlbert Lee HutchinsonDeborah Lee Sivco
    • Federico CapassoAlfred Yi ChoSung-Nee George ChuJerome FaistAlbert Lee HutchinsonDeborah Lee Sivco
    • H01S5/00H01S5/06H01S5/12H01S5/34H01S3/19
    • B82Y20/00H01S5/3402H01S5/0612H01S5/12H01S5/3403H01S5/3406
    • A quantum cascade (QC) laser has a multilayer core region comprising alternating layers of a first and a second semiconductor material, with lattice constants a.sub.1 and a.sub.2, respectively. The first material is selected such that a.sub.1 >a.sub.0, where a, is the lattice constant of the substrate (typically InP), and the second material is selected such that a.sub.2 >a.sub.0. The materials are also selected such that the conduction band discontinuity .DELTA.E.sub.c between the first and second materials is greater than 520 meV in absolute value. The multilayer core comprises a multiplicity of essentially identical multilayer repeat units. The layer thicknesses and materials of the repeat units are selected to substantially provide strain compensation over a repeat unit. QC lasers according to this invention preferably comprise a distributed feedback feature, (e.g., a Bragg grating) selected to ensure single mode laser emission, and can be designed for operation at a wavelength in the first atmospheric window, typically about 3-5 .mu.m. Such lasers can advantageously be used for absorption spectroscopy, e.g., for emission monitoring.
    • 量子级联(QC)激光器具有包括第一和第二半导体材料的交替层的多层芯区域,分别具有晶格常数a1和a2。 选择第一材料使得a1> a0,其中a是衬底的晶格常数(通常为InP),并且选择第二材料使得a2> a0。 这些材料也被选择成使得第一和第二材料之间的导带不连续性DELTA Ec绝对值大于520meV。 多层芯包括多个基本相同的多层重复单元。 选择重复单元的层厚度和材料以在重复单元上基本上提供应变补偿。 根据本发明的QC激光器优选地包括被选择用于确保单模激光发射的分布反馈特征(例如,布拉格光栅),并且可以设计成在第一大气窗口中的波长下操作,通常为约3-5μm 。 这种激光器可以有利地用于吸收光谱,例如用于发射监测。
    • 6. 发明授权
    • Mounting technology for intersubband light emitters
    • 子带发射器的安装技术
    • US06326646B1
    • 2001-12-04
    • US09448929
    • 1999-11-24
    • James Nelson BaillargeonFederico CapassoAlfred Yi ChoGeorge Sung-Nee ChuClaire GmachlAlbert Lee HutchinsonArthur Mike SergentDeborah Lee SivcoAlessandro Tredicucci
    • James Nelson BaillargeonFederico CapassoAlfred Yi ChoGeorge Sung-Nee ChuClaire GmachlAlbert Lee HutchinsonArthur Mike SergentDeborah Lee SivcoAlessandro Tredicucci
    • H01L3300
    • B82Y20/00H01S5/0202H01S5/02268H01S5/02272H01S5/02469H01S5/0425H01S5/2275H01S5/3402
    • A mounting technology that increases the cw operating temperature of intersubband lasers, without increasing the risk of hot spots near the facets and short circuits near the perimeter of the laser chip, is described. In accordance with one embodiment of our invention, a method of fabricating a intersubband semiconductor laser comprises the steps of providing a single crystal semiconductor substrate, forming on the substrate an epitaxial region that includes a core region and an intersubband active region in the core region, forming front and back facets that define an optical cavity resonator, forming a metal electrode on the epitaxial region so as to provide an electrical connection to said active region, and mounting said laser on a heat sink, characterized in that the mounting step includes the steps of (i) soldering the electrode to the heat sink so that the front facet overhangs an edge of the heat sink and (ii) cleaving off the overhanging portion of the laser so as to form a new front facet that is essentially flush with the edge of said heat sink. In accordance with another embodiment, our invention is further characterized in that metal electrode to the epitaxial region is recessed from the edges of the laser chip. In accordance with yet another embodiment, our invention is further characterized in that the back facet of the laser is coated so that any solder that might tend to creep onto the back facet contacts the coating and not semiconductor material (in particular the ends of the active region).
    • 描述了增加带间激光器的cw工作温度的安装技术,而不增加靠近激光芯片周边的面和短路附近的热点的风险。 根据本发明的一个实施例,一种制造子带间半导体激光器的方法包括以下步骤:提供单晶半导体衬底,在衬底上形成包含核心区域和芯区域中的子带间有源区域的外延区域, 形成限定光腔谐振器的前和后刻面,在所述外延区域上形成金属电极,以提供与所述有源区域的电连接,以及将所述激光器安装在散热器上,其特征在于,所述安装步骤包括步骤 (i)将电极焊接到散热器,使得前刻面突出于散热器的边缘,并且(ii)从激光器的悬垂部分分离,以形成基本上与边缘齐平的新的前刻面 的所述散热器。 根据另一个实施例,本发明的特征还在于,到外延区域的金属电极从激光芯片的边缘凹进。 根据又一个实施例,本发明的特征还在于,激光器的后面被涂覆,使得任何可能趋于蠕变到背面上的焊料与涂层接触而不是半导体材料(特别是活性物质的端部) 地区)。
    • 9. 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。