2021
DOI: 10.1103/physrevb.103.085309
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Emergence of strong tunable linear Rashba spin-orbit coupling in two-dimensional hole gases in semiconductor quantum wells

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Cited by 31 publications
(14 citation statements)
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“…[27] shows that the isotropic approximation describes well the system, but there are special orientations at which the DRSOI is enhanced: the DRSOI is largest when z [110] and y [001] [17,27]. In contrast to other proposals [20] for obtaining DRSOI in Ge heterostructures, in our approach this particular growth direction is convenient but not required. Also, because here the DRSOI originates from the confinement potential and not from the small anisotropies of Ge, the maximal SOI v * is more than 5 times larger than in [20] at comparable electric fields.…”
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confidence: 83%
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“…[27] shows that the isotropic approximation describes well the system, but there are special orientations at which the DRSOI is enhanced: the DRSOI is largest when z [110] and y [001] [17,27]. In contrast to other proposals [20] for obtaining DRSOI in Ge heterostructures, in our approach this particular growth direction is convenient but not required. Also, because here the DRSOI originates from the confinement potential and not from the small anisotropies of Ge, the maximal SOI v * is more than 5 times larger than in [20] at comparable electric fields.…”
mentioning
confidence: 83%
“…In contrast to other proposals [20] for obtaining DRSOI in Ge heterostructures, in our approach this particular growth direction is convenient but not required. Also, because here the DRSOI originates from the confinement potential and not from the small anisotropies of Ge, the maximal SOI v * is more than 5 times larger than in [20] at comparable electric fields.…”
mentioning
confidence: 99%
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“…The parameter β so is material-dependent and depends also in an intricate way on the exact shape of the transverse confining potential. By focusing solely on this Rashba term, we neglect the Dresselhaus contribution stemming from the lack of a crystallographic inversion center (which can contribute to the SOI in materials like GaAs and InAs) and we disregard the "direct" Rashba SOI due to HH-LH mixing [31][32][33][34]68]. With this choice, the analysis that follows is most relevant for quantum dots hosted in materials with a large Rashba coefficient.…”
Section: Confined Heavy Holesmentioning
confidence: 99%
“…We call this orientation direct Rashba axes (DRA) [37] because it guarantees the largest DRSOI in wires [6,7,50]. First, because of the sizeable HH-LH mixing even in planar heterostructures, yielding DRSOI [51], the hyperfine interactions are non-Ising at L x /L y 1. The hyperfine anisotropy is still pronounced in wide Ge wires, but it decreases notably in Si, where the spin decay remains Gaussian with times T i 0 of hundreds of nanoseconds.…”
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confidence: 99%