1998
DOI: 10.1103/physrevb.58.15397
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Spin-dependent electronic tunneling at zero magnetic field

Abstract: The spin-dependent tunneling phenomenon in symmetric and asymmetric semiconductor heterostructures at zero magnetic field is studied theoretically on the base of a single conduction band and spin-dependent boundary conditions approach. It is shown that the spin-orbit splitting in the dispersion relation for the electrons in A III B V semiconductor quantum-tunneling structures can provide a dependence of the tunneling transmission probability on the electron's spin polarization. The dependence is calculated and… Show more

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Cited by 96 publications
(67 citation statements)
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“…Asymmetric nonmagnetic semiconductor barriers are also used in the construction of spin filters [3]. This effect is caused by the interface-induced Rashba spin-orbit coupling [4] and can be quite significant for resonant tunneling through asymmetric double-barrier structure [5].…”
Section: (2004))mentioning
confidence: 99%
See 1 more Smart Citation
“…Asymmetric nonmagnetic semiconductor barriers are also used in the construction of spin filters [3]. This effect is caused by the interface-induced Rashba spin-orbit coupling [4] and can be quite significant for resonant tunneling through asymmetric double-barrier structure [5].…”
Section: (2004))mentioning
confidence: 99%
“…The injection of spin-polarized electrons from ferromagnetic metals into semiconductors has low efficiency, less than 1%, because of a large resistivity mismatch between ferromagnetic and semiconductor materials [1]. Rashba proposed that this problem could be solved by inserting a tunneling barrier at the metal-semiconductor interface [2].Asymmetric nonmagnetic semiconductor barriers are also used in the construction of spin filters [3]. This effect is caused by the interface-induced Rashba spin-orbit coupling [4] and can be quite significant for resonant tunneling through asymmetric double-barrier structure [5].…”
mentioning
confidence: 99%
“…On the other hand, a spin transistor can also be achieved by using only nonmagnetic materials that exploit the unique characteristics of bulk inversion asymmetry in (110)-oriented semiconductor heterostructures, as reported by Hall et al [6][7]. Furthermore, Voskoboynikov et al have proposed that a non-magnetic semiconductor material can be produced by Rashba spin-orbit coupling due to the Dresselhaus effect occurring in zinc-blende [8][9][10].…”
Section: Introductionmentioning
confidence: 94%
“…Here, we mention again that the effective mass is independent of layer. When taking both the transverse motion and the layer-dependent effective mass of the electron into account, the transmission coefficient can have a pronounced dispersion in k space [18]. In this case, one cannot simply reduce the 3D Schrödinger equation to the 1D equation and integrate the k to obtain the current density, as we did here.…”
Section: Introductionmentioning
confidence: 99%