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Characterization of the InAsSb/GaSb superlattices by Fourier transform infrared spectroscopy

机译:傅立叶变换红外光谱法表征InAsSb / GaSb超晶格

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The InAsSb/GaSb superlattice structures were sandwiched by the n-InAs or p-GaSb inner and outer bulk layers. The effects of the thickness and doping concentration of inner and outer bulk layers on the interband and intersubband transitions have been studied in detail in this study. The absorption energies for InAsSb/GaSb type Ⅱ superlattices were characterized by Fourier transform infrared (FTIR) spectroscopy. It was found that the intersubband transition hh1-lh1 (first heavy hole to first light hole subband) transition disappeared when the inner bulk layer thickness was smaller than 0.6μm or the outer bulk layer thinner than 0.15μm. The Cl-hhl (first conduction subband to first heavy hole subband) interband transitions of the p-type GaSb sandwiched superlattices were also obtained and characterized in this work. When the superlattices were sandwiched by p~+-GaSb bulk layers, a stronger Cl-hh1 absorption peak (λ = 4μm) was observed obviously. However, the above phenomena were vanished as the superlattices sandwiched by intrinsic GaSb bulk layers. The different long wavelengths of transitions in superlattices can be obtained by utilizing the different type of doping and concentrations of the bulk layers.
机译:InAsSb / GaSb超晶格结构夹在n-InAs或p-GaSb内部和外部本体层之间。本研究详细研究了内部和外部体层的厚度和掺杂浓度对带间和子带间跃迁的影响。用傅立叶变换红外光谱(FTIR)表征了InAsSb / GaSbⅡ型超晶格的吸收能。发现当内部主体层厚度小于0.6μm或外部主体层薄于0.15μm时,子带间过渡hh1-lh1(第一重孔至第一轻孔子带)过渡消失。还获得了p型GaSb夹心超晶格的Cl-hhl(第一导通子带至第一重空穴子带)的带间跃迁,并进行了工作表征。当超晶格被p〜+ GaSb体层夹在中间时,明显观察到了更强的Cl-hh1吸收峰(λ=4μm)。然而,上述现象消失了,因为超晶格被固有的GaSb体层夹在中间。通过使用不同类型的掺杂和体层的浓度,可以获得超晶格中不同的长跃迁波长。

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