2016
DOI: 10.1103/physrevb.94.245306
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Limits to mobility in InAs quantum wells with nearly lattice-matched barriers

Abstract: The growth and the density dependence of the low temperature mobility of a series of twodimensional electron systems confined to un-intentionally doped, low extended defect density InAs quantum wells with Al 1-x Ga x Sb barriers are reported. The electron mobility limiting scattering mechanisms were determined by utilizing dual-gated devices to study the dependence of mobility on carrier density and electric field independently. Analysis of the possible scattering mechanisms indicate the mobility was limited p… Show more

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Cited by 21 publications
(17 citation statements)
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“…The relative to the vacuum level for changes in film thickness. The level of interface roughness that causes gap misalignments over space is well within the limits of that found in InAs/GaSb/AlSb heterostructures 23,24 .…”
Section: Manuscriptsupporting
confidence: 72%
“…The relative to the vacuum level for changes in film thickness. The level of interface roughness that causes gap misalignments over space is well within the limits of that found in InAs/GaSb/AlSb heterostructures 23,24 .…”
Section: Manuscriptsupporting
confidence: 72%
“…The electron density and mobility measured in an ungated sample are 4.3 × 10 15 m −2 and 118 m 2 /Vs, respectively. This mobility is comparable to those of recently reported state-of-the-art InAs 2DEGs [6][7][8][9], attesting to the high quality of our sample.…”
Section: Methodssupporting
confidence: 89%
“…[23]. For both interfaces, we started with the parameters reported for InAs/AlGaSb QWs [6], roughness height of ∆ = 0.27 nm and correlation length of Λ = 13 nm. We then find that, by increasing the roughness height of the lower interface to ∆ b = 0.64 nm while keeping other parameters the same, the observed asymmetry can be reproduced reasonably well [Fig.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Charge carriers in electronic devices can be scattered (for example, by crystal defects), and the average time between scattering events needs to be long to stabilize these quasiparticles. Yan et al calculate that the charge-carrier scattering time in their devices is impressively long (66 femtoseconds; 1 fs is 10 -15 s), but the scattering times will need to be at least 100 times longer, similar to the scattering time in indium arsenide 12 , to stabilize Majorana fermions. It remains to be seen whether this can be achieved in the authors' devices.…”
Section: Transistors Driven By Superconductorsmentioning
confidence: 99%