首页> 外文会议>Second Compound Semiconductor Power Transistors and the Thirty-Second State-of-the-Art Program on Compound Semiconductors Symposia, 2nd and 32nd, May 14-19, 2000, Toronto >REDUCTION OF THE BASE-COLLECTOR CAPACITANCE OF HETEROSTRUCTURE BIPOLAR TRANSISTORS USING REGROWTH OVER A PATTERNED SUBCOLLECTOR
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REDUCTION OF THE BASE-COLLECTOR CAPACITANCE OF HETEROSTRUCTURE BIPOLAR TRANSISTORS USING REGROWTH OVER A PATTERNED SUBCOLLECTOR

机译:使用图案化子集合体上的再生减少异质结双极晶体管的基极-电容器容量

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Here we report on the use of regrowth over a patterned subcollector to achieve a reduction in the base-collector capacitance, C_(BC), for InP/InGaAs latticed matched to InP based HBT devices. After patterning the sub-collector, an initial MOCVD regrowth is done followed by MOMBE regrowth of the remainder of the structure. All of the lithography was done using a stepper. We have developed a process to protect the initial alignment features during the regrowth steps to ensure proper realignment. This is a critical issue particularly for the smaller devices where the regrowth technique can have an advantage. Results for devices with a 2X8 urn~2 emitter strip gave maximum f_T and f_(max) values of 105GHz and 130GHz, respectively. These values were limited by a somewhat high collector resistance due to an etching problem near the subcollector which increased the contact resistance. More importantly C _(BC) values of 12.5fF and 9fF for a 2X8um~2 device were extracted from the s-parameter data at I_c = 2mA and 9.5mA, respectively. This seems to indicate that only the area where the initial subcollector was defined contributed to C_(BC). In the layout of the device the actual base area is > l00um~2 which would give about 33fF assuming 0.33fF/um~2 for a 300nm collector thickness. The measured values were closer with to actual patterned subcollector area of about 30um~2.
机译:在这里,我们报告了在带图案的子集电极上使用再生长以减少与基于InP的HBT器件晶格匹配的InP / InGaAs的基极-集电极电容C_(BC)的情况。在对子集电极进行构图之后,首先进行MOCVD再生长,然后再进行其余结构的MOMBE再生长。所有光刻都是使用步进器完成的。我们已经开发了一种在重新生长步骤中保护初始对齐特征的过程,以确保正确地重新对齐。这是一个关键问题,特别是对于再生技术可以占优势的小型设备。具有2X8 urn〜2发射极条的设备的结果分别给出了最大f_T和f_(max)值,分别为105GHz和130GHz。这些值由于子集电极附近的蚀刻问题而受到较高集电极电阻的限制,这会增加接触电阻。更重要的是,分别从I_c = 2mA和9.5mA的s参数数据中提取了2X8um〜2器件的12.5fF和9fF的C_(BC)值。这似乎表明,只有定义了初始子收集器的区域才对C_(BC)起作用。在器件的布局中,实际基极面积> 100um〜2,假设对于300nm的集电极厚度为0.33fF / um〜2,则将提供约33fF的面积。测量值更接近于约30um〜2的实际图案化子收集器面积。

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