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Low‐threshold disorder‐defined buried‐heterostructure AlxGa1-xAs‐GaAs quantum well lasers

机译:低阈值无序埋藏异质结构AlxGa1-xAs-GaAs量子阱激光器

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Two different quantum well heterostructure wafers are used to fabricate buried‐heterostructure AlxGa1-xAs‐GaAs quantum well lasers using Si‐induced layer disordering (via Si diffusion). In contrast to the first wafer (QWH1), the second quantum well wafer (QWH2) utilizes Zn instead of Mg as the p‐type dopant in the top AlxGa1-xAs confining layer and yields, because of concentration mismatch in acceptor and donor doping in the confining layers (nZn≫nSe), inferior laser diodes owing to Zn diffusion from the p‐type to the n‐type confining layer during high temperature processing (850 °C Si diffusion). The first quantum well heterostructure, however, employs a lower concentration Mg doping for its p‐type confining layer (nMg≪nSe) and yields high performance devices when used with the Si‐induced layer‐disordering process. For QWH1 the p‐n junction and injection is not displaced (as for QWH2) from the QW active region during Si‐induced layer disordering (850 °C annealing). A fabrication process is presented in which quantum well laser diodes are built with active regions as narrow in width as 0.6 μm, cw room‐temperature laser threshold currents as low as 3 mA, and pulsed current thresholds as low as 1.5 mA.
机译:使用两种不同的量子阱异质结构晶片,利用Si诱导的层无序(通过Si扩散)来制造掩埋异质结构AlxGa1-xAs-GaAs量子阱激光器。与第一晶圆(QWH1)相比,第二量子阱晶圆(QWH2)在顶部AlxGa1-xAs限制层中使用Zn代替Mg作为p型掺杂剂,并且由于受主和受主掺杂中的浓度不匹配而产生产率。限制层(nZn≫nSe),劣质的激光二极管,这是由于在高温处理期间Zn从p型限制层扩散到n型限制层(850 C的Si扩散)所致。但是,第一个量子阱异质结构在其p型限制层(nMg≪nSe)中采用了较低浓度的Mg掺杂,并在与Si诱导的层无序过程一起使用时产生了高性能的器件。对于QWH1,在Si诱导的层无序(850°C退火)期间,p-n结和注入不会从QW有源区移出(与QWH2一样)。提出了一种制造工艺,其中构造量子阱激光二极管,其有源区的宽度窄至0.6μm,cw室温激光阈值电流低至3 mA,脉冲电流阈值低至1.5 mA。

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    《Journal of Applied Physics》 |1985年第12期|P.4515-4520|共6页
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  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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