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Workshop book - Physikzentrum der RWTH Aachen - RWTH Aachen ...

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Posters Monday February 4<br />

Poster 17:<br />

Rashba spin-orbit interaction in a quantum wire superlattice<br />

Sigurdur I. Erlingsson<br />

We study the effects of a longitudinal periodic potential on a parabolic<br />

quantum wire, and long quantum point contacts, defined in a two-dimensional<br />

electron gas with Rashba spin-orbit interaction. For an infinite wire<br />

superlattice we find that the energy gaps are shifted away from the usual<br />

Bragg planes due to the Rashba spin-orbit interaction. We have also calculated<br />

the charge conductance through a periodic potential of a finite length<br />

via the nonequilibrium Green’s function method combined with the Landauer<br />

formalism. We find dips in the conductance that correspond well to<br />

the energy gaps of the infinite wire superlattice. From the infinite wire energy<br />

dispersion, we <strong>der</strong>ive an equation relating the location of the conductance<br />

dips as a function of the Fermi energy to the Rashba spin-orbit coupling<br />

strength. We propose that the strength of the Rashba spin-orbit interaction<br />

can be extracted via a charge conductance measurement.<br />

Poster 18:<br />

Electronic states in a cylindrical nanowire in magnetic and electric fields<br />

Andrei Manolescu<br />

Single particle states of electrons situated on a closed cylindrical surface of<br />

radius 30-100 nm are calculated. The length of the cylin<strong>der</strong> may be either<br />

infinite or finite. In the presence of a magnetic field uniform in space, but perpendicular<br />

to the longitudinal axis of the cylin<strong>der</strong>, the orbital effects depend<br />

on the radial component of the magnetic field. For a sufficiently strong field,<br />

when the magnetic length becomes comparable to the radius of the cylin<strong>der</strong>,<br />

the orbital motion corresponds to closed cyclotron orbits in the regions with<br />

strong radial field, but to open quasi one-dimensional snaking orbits in the<br />

regions where the radial field vanishes and changes sign. The energy of the<br />

cyclotron states increases with the magnetic field relatively to the energy of<br />

the snaking states such that at high magnetic fields the electrons concentrate<br />

around the snaking orbits. The spin of the electron is included via Zeeman<br />

and Rashba spin-orbit effects. A uniform electric field perpendicular to the<br />

cylin<strong>der</strong> is also consi<strong>der</strong>ed, as being produced by a metallic electrode placed<br />

near the cylin<strong>der</strong>. In this case the spin-orbit coupling becomes anisotropic.<br />

Attempts to include Coulomb effects in the Hartree-Fock approximation are<br />

discussed.<br />

69

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