2004
DOI: 10.1016/j.physe.2003.08.012
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Ballistic transport in InSb quantum wells at high temperature

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Cited by 17 publications
(14 citation statements)
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“…At sufficiently low temperatures, the Al 0. 15 In 0.85 Sb buffer layer is depleted. However, dependent on the doping density of the δ-doped region, the Al 0.2 In 0.8 Sb top cap layer can be occupied and even degenerate, presenting a low-mobility conducting channel in parallel to the high-mobility InSb 2DEG.…”
Section: A Multi-carrier Modelmentioning
confidence: 99%
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“…At sufficiently low temperatures, the Al 0. 15 In 0.85 Sb buffer layer is depleted. However, dependent on the doping density of the δ-doped region, the Al 0.2 In 0.8 Sb top cap layer can be occupied and even degenerate, presenting a low-mobility conducting channel in parallel to the high-mobility InSb 2DEG.…”
Section: A Multi-carrier Modelmentioning
confidence: 99%
“…Due to the nature of the heterostructure, the three layers are spatially separated, but the Al 0.2 In 0.8 Sb layer, the InSb 2DEG, and the top of the Al 0. 15 In 0.85 Sb buffer layer are in intimate contact through the shallow Ohmic contacts. The three layers can therefore be considered to experience the same local electric field, unlike an isolated layer model 25 (this is also reasonable due to the lateral dimensions of the device).…”
Section: A Multi-carrier Modelmentioning
confidence: 99%
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