[eng] This thesis studies the effects of the Rashba spin-orbit coupling on the transport properties of electron and hole quantum wires. For each case, a specific
physical system is considered: the first one is a quantum wire with inhomogeneous Rashba coupling while the second is a quantum wire with homogeneous
Rashba intensity and with external magnetic field; they are studied in the
first (electrons) and the second (holes) parts of this work, respectively. Both
systems are examples of the effects of the Rashba spin-orbit coupling on the
physics of transport.
In Part I, for electron systems, we study the conductance and polarization of
the outgoing current for an incident unpolarized electron beam. The electron
conductance of a quantum wire has a staircase dependence with energy, where
each step is a conductance plateau. With the Rashba inhomogeneity a Fano
dip appears at the end of each plateau, at specific energies, and we observe how
the outgoing current is spin polarized. This current polarization occurs only
above the first plateau, since it is due to the interference of two propagating
modes with opposite spin. We also study how two conductance dips, in the
first plateau, interfere when we have two tunable Rashba regions. We show
how this interference evolves from crossing to anticrossing behavior when the
distance between the two regions increases. Transport through evanescent
states is responsible for this behavior, as we will see.
Continuing Part I, we study the generalization of the Datta-Das transistor for
a quasi-one-dimensional system —the original device corresponds to a purely
one-dimensional system with a Rashba region attached to polarized leads and
its main feature is an oscillatory behavior of the conductance with Rashba
strength. In our system we observe how that sinusoidal behavior is strongly affected by the multichannel transport, i.e., transport in a quasi one-dimensional
system having a transverse confinement. As a consequence, increasing the
number of propagating channels the effect of spin precession is destroyed. Finishing this first part, the limit from quasi one-dimensional to two-dimensional
system is considered, when the quantum wire becomes a two-dimensional electron gas with a Rashba stripe.
In the hole-system study, Part II, we present calculations of the g factors for the
lower conductance steps of three dimensional quantum wires. We define the
g factors from the anomalous half-steps appearing in the conductance in the
presence of magnetic field. Our results prove that the anisotropy of g factors
for different magnetic field orientations originates in the Rashba spin-orbit
coupling. We also analyze the relevance of the deformation, as the wire evolves
from 3D towards a flat 2D geometry. For high enough wire deformations, the
perpendicular g factors are greatly quenched by the Rashba interaction. On
the contrary, parallel g factors are rather insensitive to the Rashba interaction,
resulting in a high g factor anisotropy. Finally, we study the purely onedimensional hole system.
[cat] En aquesta tesi s’estudien els efectes de l’acoblament d’esp´ı-`orbita sobre les
propietats de transport de fils qu`antics d’electrons i forats. Per a cada cas s’ha
considerat un sistema f´ısic diferent: per als primers (electrons) ´es un fil qu`antic
amb una zona inhomog`enea d’acoblament de Rashba mentre que en els segons
(forats) l’interacci´o de Rashba ´es homog`enia a l’espai on, a m´es, s’ha aplicat
un camp magn`etic uniforme extern. Aix´ı la tesi est`a separada clarament en
dues parts, la primera pel cas del transport electr`onic i la segona pel transport
fet per forats. Els dos sistemes s´on exemples del efectes que fa l’acoblament
d’esp´ı-`orbita de Rashba sobre el transport.
A la Part I, per al sistema d’electrons, estudiam la conduct`ancia i la polaritzaci´o del corrent resultant quan el feix incident d’electrons ´es no polaritzat. La conduct`ancia per un fil qu`antic t´e una depend`encia escalonada amb
l’energia, on cada gra´o ´es un plateau de conduct`ancia. Amb la inhomogene¨ıtat
de Rashba, apareix un m´ınim de Fano al final de cada plateau a energies
espec´ıfiques i, a m´es, el corrent de sortida est`a polaritzat en esp´ı. Aquest
corrent polaritzat nom´es el trobam a partir d’energies del segon plateau, ja
que ´es la conseq¨u`encia de la interfer`encia de dos modes propagants amb espins oposats. Tamb´e estudiam, en aquesta part, com interfereixen aquests
dos m´ınims de conduct`ancia quan tenim dues zones seguides d’intearcci´o de
Rashba. Observam com els dos deeps passen d’un comportament de creuament a anticreuament quan la dist`ancia entre les dues regions augmenta. Els
responsables d’aquest comportament no s´on m´es que els estats evanescents.
Continuant en aquesta Part I, estudiam la generalitzaci´o del transistor de
Datta i Das per a un sistema quasi-unidimensional –el dispositiu original correspon a un sistema purament 1D amb una regi´o de Rashba acoblada a uns
contactes polaritzats, on la seva principal caracter´ıstica ´es la del comportament oscil·latori de la conduct`ancia en funci´o de la intensitat del Rashba. En
el nostre sistema observam que aquest comportament sinuso¨ıdal es veu fortament afectat pel transport multicanal, ´es a dir, transport en un sistema
quasi-unidimensional el qual t´e un confinament transversal. Conseq¨uentment,
augmentant el nombre de canals propagants, l’efecte de precessi´o d’esp´ı es veu
destruit. Per acabar aquesta part d’electrons, es considera el l´ımit d’un sistema quasi-unidimensional a un de bidimensional, on el fil qu`antic passa a ser
un gas d’electrons bidimensional amb una franja de Rashba.
Per al sistema de forats, Part II, presentam c`alculs dels factors giromagn`etics
per als primers escalons de la conduct`ancia per fils qu`antics tridimensionals.
Definint els factors g com a mitjos escalons “an`omals” que apareixen en la conduct`ancia quan s’hi aplica un camp magn`etic extern, trobam que l’anisotropia
del factors g per a diferents orientacions del camp magn`etic ´es conseq¨u`encia
de l’acoblament de Rashba. Tamb´e analitzam la rellev`ancia de la deformaci´o,
quan el fil passa d’una geometria tridimensional a bidimensional. En un fil molt
deformat, el factor g perpendicular disminueix fortament amb l’increment de
la interacci´o de Rashba. D’altra banda, per un camp magn`etic paral·lel al fil,
els factors g s´on considerablement insensibles al Rashba. Finalment, estudiam
el l´ımit d’un sisema purament unidimensional pel cas de forats.