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Spin-orbit coupling and electron-phonon scattering - Fachbereich ...

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Chapter 4<br />

Conclusion<br />

In this part of the thesis we have investigated the effect of Rashba spin-<strong>orbit</strong> <strong>coupling</strong><br />

on parabolically confined nanostructures for the example of quantum wires<br />

<strong>and</strong> few-<strong>electron</strong> quantum dots. In these systems the <strong>orbit</strong>al motion is strongly<br />

restricted due to the confinement which leads to characteristic spectral properties.<br />

Since the spin-<strong>orbit</strong> interaction couples spin <strong>and</strong> <strong>orbit</strong>al degrees of freedom, the<br />

question arises, how the confinement induced modification of the <strong>orbit</strong>al motion<br />

affects the spin state of <strong>electron</strong>s in the nanostructure. This is of special interest<br />

in the context of spintronics, where the spin is envisioned as an extension of even<br />

substitute of the <strong>electron</strong> charge in future <strong>electron</strong>ic devices.<br />

In chapter 2, we investigated the combined effect of geometric confinement,<br />

spin-<strong>orbit</strong> <strong>coupling</strong>, <strong>and</strong> magnetic field in quantum wires. In this interplay, the calculated<br />

one-<strong>electron</strong> spectral <strong>and</strong> spin properties show a rich variety of characteristics.<br />

These properties are governed by a compound spin <strong>orbit</strong>al-parity symmetry.<br />

Without magnetic field this spin parity – which is a characteristic property of any<br />

symmetrically confined quasi-1D system with Rashba effect – is shown to replace<br />

the quantum number of spin. It is also responsible for the well-known degeneracy<br />

at k = 0 in symmetrically confined systems with Rashba effect. A non-vanishing<br />

magnetic field breaks the spin-parity symmetry, thus lifting the corresponding degeneracy<br />

at k = 0. We show that this magnetic field induced energy splitting can<br />

become much larger than the Zeeman splitting <strong>and</strong> should be experimentally accessible<br />

by means of optical or transport measurements. In addition, hybridisation<br />

effects of the spin density go along with the symmetry breaking.<br />

The one-<strong>electron</strong> spectrum is shown to be very sensitive to weak magnetic<br />

fields. <strong>Spin</strong>-<strong>orbit</strong> induced modifications of the subb<strong>and</strong> structure of the quantum<br />

wire are strongly altered when the magnetic length becomes comparable to<br />

the confinement. In the context of spintronics, this might imply consequences for<br />

spin-field-effect-transistor designs which depend on spin injection from ferromagnetic<br />

contacts because of magnetic stray fields.<br />

79

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