1989
DOI: 10.1103/physrevb.39.1411
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Evidence for spin splitting inInxGa1xAs/

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Cited by 285 publications
(173 citation statements)
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“…AlGaN/GaN 2DEG (L) [66] GaSb/InAs 2DEG (L) [67,68] InGaAs/InAlAs 2DEG(L) [69] Ge 2DHG (C) [57] Ge 2DHG (C) [56] Si 2DEG (L) [70] contacts (different sizes) allows switching of one contact in a magnetic field while the other remains fixed. The bottom figure shows a proposed spin FET design utilising a Ge QW as the channel.…”
mentioning
confidence: 99%
“…AlGaN/GaN 2DEG (L) [66] GaSb/InAs 2DEG (L) [67,68] InGaAs/InAlAs 2DEG(L) [69] Ge 2DHG (C) [57] Ge 2DHG (C) [56] Si 2DEG (L) [70] contacts (different sizes) allows switching of one contact in a magnetic field while the other remains fixed. The bottom figure shows a proposed spin FET design utilising a Ge QW as the channel.…”
mentioning
confidence: 99%
“…We have also applied in-plane magnetic field of 0.01 T, small enough to allow the anticrossing close to the bottom of energy dispersion relations (zero slope points). (12) and (13). Although there is a little difference between spin paraboloids, due to the large energy difference between the resonant levels of both wells (∼12 meV) and the splitting of the spin sublevels (∼0.01 meV at p y = 0) it is not possible to distinguish minima behavior.…”
Section: Resultsmentioning
confidence: 99%
“…Several peculiarities for transport phenomena in heterostructures have been also discussed [12][13][14][15]. However, these discussions only consider the mix-ing between Pauli contribution and effective 2D spin-orbit interaction.…”
Section: Introductionmentioning
confidence: 99%
“…In general, there are two different types of symmetry dependent SOI, Rashba 3,4 and Dresselhaus 5 SOIs, in various condensed matter systems. In twodimensional electron gas (2DEG) formed at the III-V semiconductor heterostructures 6 and in various topological insulating systems 7 , the Rashba SOI (RSOI) is linear in momentum and of the form H R = iαk − σ + +h.c., where α is the strength of RSOI, σ ± = σ x ± iσ y with σ x and σ y are the Pauli's spin matrices and k ± = k x ± ik y with k x and k y the components of the wave vector k. Besides, the Rashba SOI in two-dimensional hole gas formed at the interface of p-type GaAs/AlGaAs heterostructures 8,9 , 2DEG on the surface of SrTiO 3 single crystals 10 and in 2D hole gas formed in a strained Ge/SiGe quantum well 11 is cubic in momentum and is of the form H iso R = iαk 3 − σ + + h.c. The spin splitting energy due to this RSOI is always isotropic and hereafter we will mention this as isotropic cubic RSOI.…”
Section: Introductionmentioning
confidence: 99%