529 research outputs found
Spin Hall effect in a system of Dirac fermions in the honeycomb lattice with intrinsic and Rashba spin-orbit interaction
We consider spin Hall effect in a system of massless Dirac fermions in a
graphene lattice. Two types of spin-orbit interaction, pertinent to the
graphene lattice, are taken into account - the intrinsic and Rashba terms.
Assuming perfect crystal lattice, we calculate the topological contribution to
spin Hall conductivity. When both interactions are present, their interplay is
shown to lead to some peculiarities in the dependence of spin Hall conductivity
on the Fermi level.Comment: 7 pages, 5 figure
Non-equilibrium spin polarization effects in spin-orbit coupling system and contacting metallic leads
We study theoretically the current-induced spin polarization effect in a
two-terminal mesoscopic structure which is composed of a semiconductor
two-dimensional electron gas (2DEG) bar with Rashba spin-orbit (SO) interaction
and two attached ideal leads. The nonequilibrium spin density is calculated by
solving the scattering wave functions explicitly within the ballistic transport
regime. We found that for a Rashba SO system the electrical current can induce
spin polarization in the SO system as well as in the ideal leads. The induced
polarization in the 2DEG shows some qualitative features of the intrinsic spin
Hall effect. On the other hand, the nonequilibrium spin density in the ideal
leads, after being averaged in the transversal direction, is independent of the
distance measured from the lead/SO system interface, except in the vicinity of
the interface. Such a lead polarization effect can even be enhanced by the
presence of weak impurity scattering in the SO system and may be detectable in
real experiments.Comment: 6 pages,5 figure
Electron spin relaxation in carbon nanotubes
The long standing problem of inexplicably short spin relaxation in carbon
nanotubes (CNTs) is examined. The curvature-mediated spin-orbital interaction
is shown to induce fluctuating electron spin precession causing efficient
relaxation in a manner analogous to the Dyakonov-Perel mechanism. Our
calculation estimates longitudinal (spin-flip) and transversal (decoherence)
relaxation times as short as 150 ps and 110 ps at room temperature,
respectively, along with a pronounced anisotropic dependence. Interference of
electrons originating from different valleys can lead to even faster dephasing.
The results can help clarify the measured data, resolving discrepancies in the
literature.Comment: 9 pages, 3 figure
Phonon-induced decoherence for a quantum dot spin qubit operated by Raman passage
We study single-qubit gates performed via stimulated Raman adiabatic passage
(STIRAP) on a spin qubit implemented in a quantum dot system in the presence of
phonons. We analyze the interplay of various kinds of errors resulting from the
carrier-phonon interaction as well as from quantum jumps related to
nonadiabaticity and calculate the fidelity as a function of the pulse
parameters. We give quantitative estimates for an InAs/GaAs system and identify
the parameter values for which the error is considerably minimized, even to
values below per operation.Comment: Final version; considerable extensions; 18 pages, 7 figure
Detection of spin polarized currents in quantum point contacts via transverse electron focusing
It has been predicted recently that an electron beam can be polarized when it
flows adiabatically through a quantum point contact in a system with spin-orbit
interaction. Here, we show that a simple transverse electron focusing setup can
be used to detect such polarized current. It uses the amplitude's asymmetry of
the spin-split transverse electron focusing peak to extract information about
the electron's spin polarization. On the other hand, and depending on the
quantum point contact geometry, including this one-body effect can be important
when using the focusing setup to study many-body effects in quantum point
contacts.Comment: 5 pages, 5 figure
Spin relaxation of localized electrons in n-type semiconductors
The mechanisms that determine spin relaxation times of localized electrons in
impurity bands of n-type semiconductors are considered theoretically and
compared with available experimental data. The relaxation time of the
non-equilibrium angular momentum is shown to be limited either by hyperfine
interaction, or by spin-orbit interaction in course of exchange-induced spin
diffusion. The energy relaxation time in the spin system is governed by
phonon-assisted hops within pairs of donors with an optimal distance of about 4
Bohr radii. The spin correlation time of the donor-bound electron is determined
either by exchange interaction with other localized electrons, or by spin-flip
scattering of free conduction-band electrons. A possibility of optical cooling
of the spin system of localized electrons is discussed.Comment: Submitted to the special issue "Optical Orientation", Semiconductor
Science and Technolog
Electron Spin Dynamics in Impure Quantum Wells for Arbitrary Spin-Orbit Coupling
Strong interest has arisen recently on low-dimensional systems with strong
spin-orbit interaction due to their peculiar properties of interest for some
spintronic applications. Here, the time evolution of the electron spin
polarization of a disordered two-dimensional electron gas is calculated exactly
within the Boltzmann formalism for arbitrary couplings to a Rashba spin-orbit
field. The classical Dyakonov-Perel mechanism of spin relaxation is shown to
fail for sufficiently strong Rashba fields, in which case new regimes of spin
decay are identified. These results suggest that spin manipulation can be
greatly improved in strong spin-orbit interaction materials.Comment: 5 pages, 2 figures -revised versio
Temperature dependence of D'yakonov-Perel' spin relaxation in zinc blende semiconductor quantum structures
The D'yakonov-Perel' mechanism, intimately related to the spin splitting of
the electronic states, usually dominates the spin relaxation in zinc blende
semiconductor quantum structures. Previously it has been formulated for the two
limiting cases of low and high temperatures. Here we extend the theory to give
an accurate description of the intermediate regime which is often relevant for
room temperature experiments. Employing the self-consistent multiband envelope
function approach, we determine the spin splitting of electron subbands in
n-(001) zinc blende semiconductor quantum structures. Using these results we
calculate spin relaxation rates as a function of temperature and obtain
excellent agreement with experimental data.Comment: 9 pages, 4 figure
Dependence of the intrinsic spin Hall effect on spin-orbit interaction character
We report on a comparative numerical study of the spin Hall conductivity in
two-dimensions for three different spin-orbit interaction models; the standard
k-linear Rashba model, the k-cubic Rashba model that describes two-dimensional
hole systems, and a modified k-linear Rashba model in which the spin-orbit
coupling strength is energy dependent. Numerical finite-size Kubo formula
results indicate that the spin Hall conductivity of the k-linear Rashba model
vanishes for frequency much smaller than the scattering rate
, with order one relative fluctuations surviving out to large system
sizes. For the k-cubic Rashba model case, the spin Hall conductivity does not
depend noticeably on and is finite in the {\em dc} limit, in
agreement with experiment. For the modified k-linear Rashba model the spin Hall
conductivity is noticeably dependent but approaches a finite
value in the {\em dc} limit. We discuss these results in the light of a
spectral decomposition of the spin Hall conductivity and associated sum rules,
and in relation to a proposed separation of the spin Hall conductivity into
skew-scattering, intrinsic, and interband vertex correction contributions.Comment: 10 pages, 4 figure
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