2008
DOI: 10.1134/s1063782608070129
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Exchange enhancement of the g factor in InAs/AlSb heterostructures

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Cited by 35 publications
(38 citation statements)
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“…Previously, we have employed this approximation for a quantitative interpretation of our previous experimental results on CR (Refs. 25 and 33) and magnetotransport [39][40][41][42] in InAs/AlSb QWs as well. Moreover, it can be shown that our approximation for the single-electron states can be reduced to the model proposed by Pfeffer and Zawadzki 43 for the spin splitting in the conduction band in n-type QWs based on narrow-gap materials.…”
Section: A Single-electron Statesmentioning
confidence: 87%
See 1 more Smart Citation
“…Previously, we have employed this approximation for a quantitative interpretation of our previous experimental results on CR (Refs. 25 and 33) and magnetotransport [39][40][41][42] in InAs/AlSb QWs as well. Moreover, it can be shown that our approximation for the single-electron states can be reduced to the model proposed by Pfeffer and Zawadzki 43 for the spin splitting in the conduction band in n-type QWs based on narrow-gap materials.…”
Section: A Single-electron Statesmentioning
confidence: 87%
“…To prevent the interference effects, the substrates of sample structures were wedged with an angle of 2 . Pronounced effect of negative persistent photoconductivity attributed to GaSb cap layer, 31,[39][40][41] allows one to tune electron concentration by using blue LED illumination. In order control a 2DEG concentration in CR experiments, magnetoresistance was measured as well.…”
Section: Methodsmentioning
confidence: 99%
“…[46] for InAs and Ref. [47] for InSb) and are known to have a large spin-orbit interaction strength α as well as large Lande g-factor (g InAs ∼ 10 − 25 [48] and g InSb ∼ 20 − 70 [47]). Furthermore, these materials are known to form interfaces that are highly transparent for electrons, allowing one to induce a large superconducting gap ∆ [49][50][51].…”
Section: Introductionmentioning
confidence: 99%
“…Consequently, previously blocked transitions between the triplet and singlet states are enabled leading to a lifting of the PSB. Note that different g-tensors are caused by different constitutions of the two dots in a DQD due to site-dependent confinement, strain or material composition [22][23][24][25][26][27]. While these differences are expected to occur in any realistic DQD system due to unavoidable imperfections in quantum dot growth or engineering, we expect the difference in the g tensors to be particularly noticeable in materials with a strong SOI.…”
Section: Introductionmentioning
confidence: 97%