279 research outputs found
Spin relaxation in -type ZnO quantum wells
We perform an investigation on the spin relaxation for -type ZnO (0001)
quantum wells by numerically solving the kinetic spin Bloch equations with all
the relevant scattering explicitly included. We show the temperature and
electron density dependence of the spin relaxation time under various
conditions such as impurity density, well width, and external electric field.
We find a peak in the temperature dependence of the spin relaxation time at low
impurity density. This peak can survive even at 100 K, much higher than the
prediction and measurement value in GaAs. There also exhibits a peak in the
electron density dependence at low temperature. These two peaks originate from
the nonmonotonic temperature and electron density dependence of the Coulomb
scattering. The spin relaxation time can reach the order of nanosecond at low
temperature and high impurity density.Comment: 6 pages, 4 figure
Theory of laser-induced demagnetization at high temperatures
Laser-induced demagnetization is theoretically studied by explicitly taking
into account interactions among electrons, spins and lattice. Assuming that the
demagnetization processes take place during the thermalization of the
sub-systems, the temperature dynamics is given by the energy transfer between
the thermalized interacting baths. These energy transfers are accounted for
explicitly through electron-magnons and electron-phonons interaction, which
govern the demagnetization time scale. By properly treating the spin system in
a self-consistent random phase approximation, we derive magnetization dynamic
equations for a broad range of temperature. The dependence of demagnetization
on the temperature and pumping laser intensity is calculated in detail. In
particular, we show several salient features for understanding magnetization
dynamics near the Curie temperature. While the critical slowdown in dynamics
occurs, we find that an external magnetic field can restore the fast dynamics.
We discuss the implication of the fast dynamics in the application of heat
assisted magnetic recording.Comment: 11 Pages, 7 Figure
Spin relaxation due to random Rashba spin-orbit coupling in GaAs (110) quantum wells
We investigate the spin relaxation due to the random Rashba spin-orbit
coupling in symmetric GaAs (110) quantum wells from the fully microscopic
kinetic spin Bloch equation approach. All relevant scatterings, such as the
electron-impurity, electron--longitudinal-optical-phonon,
electron--acoustic-phonon, as well as electron-electron Coulomb scatterings are
explicitly included. It is shown that our calculation reproduces the
experimental data by M\"uller {\em et al.} [Phys. Rev. Lett. {\bf 101}, 206601
(2008)] for a reasonable choice of parameter values. We also predict that the
temperature dependence of spin relaxation time presents a peak in the case with
low impurity density, which originates from the electron-electron Coulomb
scattering.Comment: 5 pages, 2 figures, EPL in pres
Crossover to the Anomalous Quantum Regime in the Extrinsic Spin Hall Effect of Graphene
Recent reports of spin-orbit coupling enhancement in chemically modified graphene have opened doors to studies of the spin Hall effect with massless chiral fermions. Here, we theoretically investigate the interaction and impurity density dependence of the extrinsic spin Hall effect in spin-orbit coupled graphene. We present a nonperturbative quantum diagrammatic calculation of the spin Hall response function in the strong-coupling regime that incorporates skew scattering and anomalous impurity density-independent contributions on equal footing. The spin Hall conductivity dependence on Fermi energy and electron-impurity interaction strength reveals the existence of experimentally accessible regions where anomalous quantum processes dominate. Our findings suggest that spin-orbit-coupled graphene is an ideal model system for probing the competition between semiclassical and bona fide quantum scattering mechanisms underlying the spin Hall effect
Current induced local spin polarization due to the spin-orbit coupling in a two dimensional narrow strip
The current induced local spin polarization due to weak Rashba spin-orbit
coupling in narrow strip is studied. In the presence of longitudinal charge
current, local spin polarizations appear in the sample. The spin polarization
perpendicular to the plane has opposite sign near the two edges. The in-plane
spin polarization in the direction perpendicular to the sample edges also
appears, but does not change sign across the sample. From our scaling analysis
based on increasing the strip width, the out-of-plane spin polarization is
important mainly in a system of mesoscopic size, and thus appears not to be
associated with the spin-Hall effect in bulk samples.Comment: 4 pages, 4 figure
Non-Markovian spin relaxation in two-dimensional electron gas
We analyze by Monte-Carlo simulations and analytically spin dynamics of
two-dimensional electron gas (2DEG) interacting with short-range scatterers in
nonquantizing magnetic fields. It is shown that the spin dynamics is
non-Markovian with the exponential spin relaxation followed by the oscillating
tail due to the electrons residing on the closed trajectories. The tail relaxes
on a long time scale due to an additional smooth random potential and inelastic
processes. The developed analytical theory and Monte-Carlo simulations are in
the quantitative agreement with each other.Comment: 6 pages, 3 figure
Electron spin relaxation in graphene with random Rashba field: Comparison of D'yakonov-Perel' and Elliott-Yafet--like mechanisms
Aiming to understand the main spin relaxation mechanism in graphene, we
investigate the spin relaxation with random Rashba field induced by both
adatoms and substrate, by means of the kinetic spin Bloch equation approach.
The charged adatoms on one hand enhance the Rashba spin-orbit coupling locally
and on the other hand serve as Coulomb potential scatterers. Both effects
contribute to spin relaxation limited by the D'yakonov-Perel' mechanism. In
addition, the random Rashba field also causes spin relaxation by spin-flip
scattering, manifesting itself as an Elliott-Yafet--like mechanism. Both
mechanisms are sensitive to the correlation length of the random Rashba field,
which may be affected by the environmental parameters such as electron density
and temperature. By fitting and comparing the experiments from the Groningen
group [J\'ozsa {\it et al.}, Phys. Rev. B {\bf 80}, 241403(R) (2009)] and
Riverside group [Pi {\it et al.}, Phys. Rev. Lett. {\bf 104}, 187201 (2010);
Han and Kawakami, {\it ibid.} {\bf 107}, 047207 (2011)] which show either
D'yakonov-Perel'-- (with the spin relaxation rate being inversely proportional
to the momentum scattering rate) or Elliott-Yafet--like (with the spin
relaxation rate being proportional to the momentum scattering rate) properties,
we suggest that the D'yakonov-Perel' mechanism dominates the spin relaxation in
graphene. The latest experimental finding of a nonmonotonic dependence of spin
relaxation time on diffusion coefficient by Jo {\it et al.} [Phys. Rev. B {\bf
84}, 075453 (2011)] is also well reproduced by our model.Comment: 13 pages, 9 figures, to be published in New J. Phy
Spin Orientation of Holes in Quantum Wells
This paper reviews the spin orientation of spin-3/2 holes in quantum wells.
We discuss the Zeeman and Rashba spin splitting in hole systems that are
qualitatively different from their counterparts in electron systems. We show
how a systematic understanding of the unusual spin-dependent phenomena in hole
systems can be gained using a multipole expansion of the spin density matrix.
As an example we discuss spin precession in hole systems that can give rise to
an alternating spin polarization. Finally, we discuss the qualitatively
different regimes of hole spin polarization decay in clean and dirty samples.Comment: 14 pages, 8 figure
Extrinsic Entwined with Intrinsic Spin Hall Effect in Disordered Mesoscopic Bars
We show that pure spin Hall current, flowing out of a four-terminal
phase-coherent two-dimensional electron gas (2DEG) within inversion asymmetric
semiconductor heterostructure, contains contributions from both the extrinsic
mechanisms (spin-orbit dependent scattering off impurities) and the intrinsic
ones (due to the Rashba coupling). While the extrinsic contribution vanishes in
the weakly and strongly disordered limits, and the intrinsic one dominates in
the quasiballistic limit, in the crossover transport regime the spin Hall
conductance, exhibiting sample-to-sample large fluctuations and sign change, is
not simply reducible to either of the two mechanisms, which can be relevant for
interpretation of experiments on dirty 2DEGs [V. Sih et al., Nature Phys. 1, 31
(2005)].Comment: 5 pages, 3 color EPS figure
Nucleon-nucleon potential in finite nuclei
We consider the spin-isospin-independent central part of the residual
nucleon-nucleon potential in finite spherical nuclei taking into account the
deformation effects of the nucleons within the surrounding nuclear environment.
It is shown that inside the nucleus the short-range repulsive contribution of
the potential is increased and the intermediate attraction is decreased. We
identify the growth of the radial component of the spin-isospin independent
short-range part of the in-medium nucleon-nucleon interaction as the
responsible agent that prevents the radial collapse of the nucleus.Comment: 9 pages, 3 eps figure
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