Method of making a semiconductor device having a non-alloyed ohmic contact to a buried doped layer
    4.
    发明授权
    Method of making a semiconductor device having a non-alloyed ohmic contact to a buried doped layer 失效
    制造具有与掩埋掺杂层的非合金欧姆接触的半导体器件的方法

    公开(公告)号:US06258616B1

    公开(公告)日:2001-07-10

    申请号:US09083165

    申请日:1998-05-22

    IPC分类号: H01L2100

    摘要: A semiconductor device having a buried doped layer of semiconductor material and a non-alloyed contact to the buried doped layer. The non-alloyed contact is made ohmic by the presence of an underlying delta-doped monolayer. The semiconductor device is made by placing a stop-etch layer on top of a buried doped layer and forming at least one delta-doped monolayer in either the stop-etch layer or the buried doped layer. Layers of semiconductor material disposed above the stop-etch layer are removed with an etchant to define an active region of the semiconductor device. The stop-etch layer prevents the etchant from removing the delta-doped monolayer. A non-alloyed metal film is then deposited over the delta-doped monolayer to form an ohmic contact to the buried doped layer.

    摘要翻译: 一种具有半导体材料的掩埋掺杂层和与该掩埋掺杂层的非合金接触的半导体器件。 通过存在下面的δ-掺杂的单层,非合金化接触是欧姆的。 通过在掩埋掺杂层的顶部放置止蚀蚀刻层并在停止蚀刻层或掩埋掺杂层中形成至少一个δ-掺杂单层来制造半导体器件。 用蚀刻剂去除设置在停止蚀刻层上方的半导体材料层,以限定半导体器件的有源区。 停止蚀刻层防止蚀刻剂去除δ-掺杂的单层。 然后将非合金金属膜沉积在δ掺杂单层上以形成与埋入掺杂层的欧姆接触。

    Method for producing a precise alloy composition from input variables
under nonlinear incorporation conditions
    7.
    发明授权
    Method for producing a precise alloy composition from input variables under nonlinear incorporation conditions 失效
    在非线性掺入条件下从输入变量产生精确合金组成的方法

    公开(公告)号:US5735950A

    公开(公告)日:1998-04-07

    申请号:US653086

    申请日:1996-05-24

    CPC分类号: H01L31/184 Y02E10/544

    摘要: A process for manufacturing precise alloy compositions in nonlinear alloy systems. The invention implements a new quadratic fitting function that relates alloy composition c.sub.A for a variable A to input fluxes f.sub.A and f.sub.B, as c.sub.A =f.sub.A.sup.2 /(f.sub.A.sup.2 +/.beta.f.sub.B.sup.2). .beta. is a parameter that is used to modify the incorporation of the Group V input variable B. This modification is necessary because of different surface populations of Group V dimer species. This new fitting function precisely predicts alloy compositions in nonlinear systems, such as the GaAs.sub.l-y P.sub.y system, where y is set equal to the composition c.sub.A.

    摘要翻译: 一种在非线性合金系统中制造精密合金组成的方法。 本发明实现了一种新的二次拟合函数,其将变量A的合金组成cA与输入通量fA和fB相关联,如cA = fA2 /(fA2 + /βfB2)。 β是用于修改V组输入变量B的并入的参数。由于V族二聚体物种的不同表面积,这种修饰是必需的。 这种新的拟合函数精确地预测非线性系统中的合金组成,例如GaAs1-yPy系统,其中y被设定为等于组成cA。

    Saturable Bragg reflector structure and process for fabricating the same
    8.
    发明授权
    Saturable Bragg reflector structure and process for fabricating the same 失效
    可饱和布拉格反射器结构及其制造方法

    公开(公告)号:US5701327A

    公开(公告)日:1997-12-23

    申请号:US640377

    申请日:1996-04-30

    CPC分类号: H01S3/1118 G02F1/3523

    摘要: Low optical loss and simplified fabrication are achieved by a nonlinear reflector which incorporates one or more semiconductor quantum wells within an n half-wavelengths strain relief layer (where n is an odd integer greater than zero) that is formed on a standard semiconductor quarter wave stack reflector. Growth of the half-wavelength layer is controlled so that dislocations are formed in sufficient concentration at the interface region to act effectively as non-radiative recombination sources. After saturation, these recombination sources remove carriers in the quantum well before the next round trip of the optical pulse arrives in the laser cavity. The nonlinear reflector is suitable for laser modelocking at the high wavelengths associated with many currently contemplated telecommunications applications and provides, at such wavelengths, an intensity dependent response that permits it to be used for saturable absorption directly in a main oscillating cavity of a laser. Saturation intensity of the nonlinear reflector and thereby related laser modelocking properties can be controlled by disposing the quantum well(s) at a particular position within the strain relief layer.

    摘要翻译: 低光损耗和简化制造通过非线性反射器实现,该非线性反射器在n个半波长应变消除层(其中n是大于零的奇整数)中包含一个或多个半导体量子阱,其形成在标准半导体四分之一波长叠层 反射器。 控制半波长层的生长,使得在界面区域以足够的浓度形成位错以有效地作为非辐射复合源起作用。 在饱和之后,这些重组源在光脉冲的下一次往返到达激光腔之前去除量子阱中的载流子。 非线性反射器适用于与许多当前预期的电信应用相关联的高波长处的激光锁模,并且在这样的波长处提供强度依赖性响应,其允许其直接用于激光器的主振荡腔中的可饱和吸收。 可以通过将量子阱设置在应变消除层内的特定位置来控制非线性反射器的饱和强度,从而相关的激光锁模特性。

    Modelocking laser including self-tuning intensity-dependent reflector
for self-starting and stable operation
    9.
    发明授权
    Modelocking laser including self-tuning intensity-dependent reflector for self-starting and stable operation 失效
    模式锁定激光器包括自调谐强度相关反射器,用于自启动和稳定运行

    公开(公告)号:US6141359A

    公开(公告)日:2000-10-31

    申请号:US16622

    申请日:1998-01-30

    摘要: The present invention is an improved modelocked laser comprising an optical gain medium and an optical cavity including a self-tuning saturable reflector incorporating one or more quantum wells. In the improved laser, the self-tuning saturable reflector comprises a first Bragg grating having a reflection spectrum broader than the spectrum of desired lasing and an additional Bragg reflector for light in the spectral region of lasing to provide self-starting and stable operation without mechanical tuning. The Bragg reflectors are preferably semiconductor quarter wave reflector stacks, and the saturable absorber is one or more quantum wells within the outer stack. The invention also encompasses the new saturable reflector used in such lasers.

    摘要翻译: 本发明是一种改进的锁模激光器,其包括光学增益介质和包括具有一个或多个量子阱的自调谐可饱和反射器的光学腔。 在改进的激光器中,自调谐可饱和反射器包括具有比期望的激光的光谱更宽的反射光谱的第一布拉格光栅和用于激光的光谱区域中的光的附加布拉格反射器,以提供自启动和稳定的操作,而不需要机械 调整 布拉格反射器优选地是半导体四分之一波长反射器叠层,并且可饱和吸收体是外部堆叠内的一个或多个量子阱。 本发明还包括在这种激光器中使用的新的可饱和反射器。

    Articles comprising doped semiconductor material
    10.
    发明授权
    Articles comprising doped semiconductor material 失效
    包含掺杂半导体材料的制品

    公开(公告)号:US5834792A

    公开(公告)日:1998-11-10

    申请号:US111765

    申请日:1993-08-25

    摘要: The disclosed novel doping method makes it possible to tailor the effective activation energy of a dopant species in semiconductor material. The method involves formation of very thin layers of .delta.-doped second semiconductor material in first semiconductor material, with the second material chosen to have a bandgap energy that differs from that of the first material. Exemplarily, in a Be-doped GaAs/AlGaAs structure according to the invention the effective activation energy of the dopant was measured to be about 4 meV, and in conventionally Be-doped GaAs it was measured to be about 19 meV. The invention can be advantageously used to dope III-V and II-VI semiconductors. In some cases it may make possible effective doping of a semiconductor for which prior art techniques are not satisfactory.

    摘要翻译: 所公开的新型掺杂方法使得可以调整半导体材料中掺杂剂物质的有效活化能。 该方法包括在第一半导体材料中形成非常薄的δ-掺杂的第二半导体材料层,其中第二材料被选择为具有不同于第一材料的带隙能量。 示例性地,在根据本发明的Be掺杂GaAs / AlGaAs结构中,测量掺杂剂的有效活化能为约4meV,并且在常规的Be掺杂GaAs中,测量其为约19meV。 本发明可有利地用于掺杂III-V和II-VI半导体。 在某些情况下,可能有效地掺杂现有技术不令人满意的半导体。