2003
DOI: 10.1103/physrevb.67.195319
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Transport properties in asymmetric InAs/AlSb/GaSb electron-hole hybridized systems

Abstract: Transport properties in asymmetric InAs/GaSb and InAs/AlSb/GaSb heterostructures sandwiched by AlGaSb layers were studied. For the InAs/GaSb structures, partially compensated quantum Hall effects arising from the electron-hole hybridization were observed. By changing the thickness of each layer, the energy positions of the conduction band and the valence band can be controlled independently. In InAs/AlSb/GaSb structures, we tried to control the hybridization strength by varying the AlSb barrier thickness. Magn… Show more

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Cited by 25 publications
(24 citation statements)
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“…As a result, both the electron and hole charges coexist in semimetallic structures with thick GaSb layers, while only negative electron charge exists in the InAs layer of a semiconducting structure with a sufficiently thin GaSb layer. This result agrees with the experimental observation [10]. …”
Section: Introductionsupporting
confidence: 94%
See 1 more Smart Citation
“…As a result, both the electron and hole charges coexist in semimetallic structures with thick GaSb layers, while only negative electron charge exists in the InAs layer of a semiconducting structure with a sufficiently thin GaSb layer. This result agrees with the experimental observation [10]. …”
Section: Introductionsupporting
confidence: 94%
“…Once the electron and hole charge density distributions have been obtained, the Poisson equation is solved taking into account the positive charge of donor defects which are supposed to be ionized. These donor defects as well as the contacts to the InAs/GaSb channel ensure the excess of electrons in the InAs/GaSb quantum wells, observed experimentally [3], [5], [6], [10]. We take the donor defect concentration equal to 2 1 01 1 cm2 at the InAs/GaSb interface for structures investigated experimentally in Ref.…”
Section: Model Descripsionmentioning
confidence: 99%
“…We now show that in this system there is a coexistence of hole and hybridised electron-hole states, resulting in a quantum transport behaviour that deviates from conventional 2D 13 .…”
Section: Introductionmentioning
confidence: 74%
“…The InAs, AlSb, and GaSb layer thicknesses are 30, 3.6, and 18 nm, respectively. This AlSb thickness is sufficient to render the electron-hole hybridization negligible [10]. Strong R xx oscillations as a function of B are observed as horizontal lines on the plot.…”
mentioning
confidence: 90%
“…An InAs=AlSb=GaSb heterostructure sandwiched between Al 0:7 Ga 0:3 Sb barriers is grown on a conductive InAs substrate which acts as a back gate [9]. The inserted AlSb layer takes the role of a barrier between the InAs conduction and GaSb valence bands, controlling the hybridization strength [9,10]. Figure 1(b) shows a contour plot of R xx at 1.6 K as functions of the magnetic field (B) normal to the plane and the gate voltage (V G ) for a sample with a thick AlSb barrier.…”
mentioning
confidence: 99%