June 21, 2013 17:18 PSP Book - 9in x 6in 01-Hedin-c01
Chapter 1
Spin-Polarized Transport in Quantum
Dots System with Rashba Spin–Orbit
Interaction
Xing-Tao An
a
and Jian-Jun Liu
b
a
School of Sciences, Hebei University of Science and Technology,
Shijiazhuang, Hebei 050018, China
b
Physics Department, Shijiazhuang University,
Shijiazhuang, Hebei 050035, China
liujj@mail.hebtu.edu.cn
Recently, spin phenomena in mesoscopic systems have come into
the focus of attention. How to efficiently control and manipulate the
spin in semiconductor mesoscopic structures is the central issue in
spintronics. Quantum dots are among the most studied mesoscopic
systems due to their physical properties as well as their potential
applications in electronic devices. The interplay between spin inter-
ference with spin–orbit interaction or electron interaction gives rise
to a variety of unexpected spin phenomena in mesoscopic systems
and allows moreover to control and engineer the spin of the electron.
In this review, an efficient and flexible numerical algorithm, i.e.,
Keldysh nonequilibrium Green’s function approach is explained and
employed to investigate the spin-dependent transport properties in
multi-quantum dots with spin–orbit interaction and multi-leads.
Spintronics in Nanoscale Devices
Edited by Eric R. Hedin and Yong S. Joe
Copyright
c
2013 Pan Stanford Publishing Pte. Ltd.
ISBN 978-981-4411-69-1 (Hardcover), 978-981-4411-70-7 (eBook)
www.panstanford.com
© 2014 by Taylor & Francis Group, LLC
June 21, 2013 17:18 PSP Book - 9in x 6in 01-Hedin-c01
2 Spin-Polarized Transport in Quantum Dots System
1.1 Introduction
Spintronics is one of the most attractive investigation frontiers
in condensed matter physics and material science due to its
potential application in nanodevices. The generation and detection
of spin-polarized electric currents through a mesoscopic system are
important issues and main goals for spintronics [1]. Electron spin
automatically comprises two levels that is a natural representation
of a qubit [2–4]; moreover the spin has a long decoherence time. The
quantum dot (QD) is an elementary cell of nanoelectronic devices.
The electron spin in the QD is considered as an ideal candidate for
the qubit to realize quantum computing in the future [1]. In order to
utilize the electron spin in the QD as a qubit, one first has to figure
out how to efficiently polarize and manipulate the spin in the QD,
i.e., writing a spin into the QD. For a mesoscopic QD system, it is
a natural idea to couple with ferromagnetic (FM) leads or to use
magnetic field to control and manipulate the spin [2, 3]. However,
these two methods are not feasible in current experiments. First, it is
very difficult to inject the spin from a FM lead into a semiconductor,
and for the second proposal, one has to confine a strong magnetic
field to the small region of a QD [5, 6]. Therefore, it is desirable
to realize spin-polarized transport or the spin accumulation just
by using the intrinsic property of the QD but not with the help of
complex experimental conditions.
More than 10 years ago, Datta and Das proposed a spin
transistor based on the Rashba spin–orbit interactions (RSOIs) in a
semiconductor sandwiched between two FM leads [7]. Since then,
some theoretical and experimental studies have been proposed to
improve the efficiency of spin polarization in transport systems
based on the RSOI [8–15]. The RSOI can couple the spin degree
of freedom of an electron to its orbital motion and vice versa,
thereby giving a useful handle for manipulating and controlling the
electron spin by external electric fields or gate voltages. The RSOI
is a relativistic effect at the low-speed limit, but it is believed to be
substantial in some semiconductors. During the past two decades, a
great number of studies have been drawn to improve the efficiency
of spin polarization in the transport system based on the RSOI
but not under magnetic field or coupled FM leads [1]. Recently,
© 2014 by Taylor & Francis Group, LLC

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