4,516 research outputs found
Near-Boundary and Bulk Regions of a Semi-Infinite Two-Dimensional Heisenberg Antiferromagnet
Using the spin-wave approximation elementary excitations of a semi-infinite
two-dimensional Heisenberg antiferromagnet are considered. The
spectrum consists of bulk modes -- standing spin waves and a
quasi-one-dimensional mode of boundary spin waves. These latter excitations
eject bulk modes from two boundary rows of sites, thereby dividing the
antiferromagnet into two regions with different dominant excitations. As a
result absolute values of nearest-neighbor spin correlations on the edge exceed
the bulk value.Comment: 8 pages, 3 figure
The t-J model on a semi-infinite lattice
The hole spectral function of the t-J model on a two-dimensional
semi-infinite lattice is calculated using the spin-wave and noncrossing
approximations. In the case of small hole concentration and strong
correlations, , several near-boundary site rows appear to be depleted
of holes. The reason for this depletion is a deformation of the magnon cloud,
which surrounds the hole, near the boundary. The hole depletion in the boundary
region leads to a more complicated spectral function in the boundary row in
comparison with its bulk shape.Comment: 8 pages, 5 figure
Spin current injection by intersubband transitions in quantum wells
We show that a pure spin current can be injected in quantum wells by the
absorption of linearly polarized infrared radiation, leading to transitions
between subbands. The magnitude and the direction of the spin current depend on
the Dresselhaus and Rashba spin-orbit coupling constants and light frequency
and, therefore, can be manipulated by changing the light frequency and/or
applying an external bias across the quantum well. The injected spin current
should be observable either as a voltage generated via the anomalous spin-Hall
effect, or by spatially resolved pump-probe optical spectroscopy.Comment: minor changes, short version publishe
Piezoelectric mechanism of orientation of a bilayer Wigner crystal in a GaAs matrix
A mechanism for orientation of bilayer classical Wigner crystals in a
piezoelectric medium is considered. For the GaAs system the piezoelectric
correction to the electrostatic interaction between electrons is calculated. It
is shown that taking into account the correction due to the piezoelectric
effect leads to a dependence of the total energy of the electron crystal on its
orientation with respect to the crystallographic axes of the surrounding
matrix. A generalization of Ewald's method is obtained for calculating the
anisotropic interaction between electrons in a Wigner crystal. The method is
used to calculate the energy of bilayer Wigner crystals in electron layers
parallel to the crystallographic planes (001), (0-11), and (111) as a function
of their orientation and the distance between layers, and the energetically
most favorable orientation for all types of electron lattices in a bilayer
system is found. It is shown that phase transitions between structures with
different lattice symmetry in a Wigner crystal can be accompanied by a change
of its orientation.Comment: 11 pages, 4 eps figures include
Drift-Diffusion Approach to Spin-Polarized Transport
We develop a drift-diffusion equation that describes electron spin
polarization density in two-dimensional electron systems. In our approach,
superpositions of spin-up and spin-down states are taken into account, what
distinguishes our model from the traditional two-component drift-diffusion
approximation. The Dresselhaus and Rashba spin-orbit coupling mechanisms are
incorporated into consideration, as well as an applied electric field. The
derived equation is applied to the modelling of relaxation of homogeneous spin
polarization. Our results are consistent with previous studies
Dynamic spin susceptibility in the t-J model
A relaxation-function theory for the dynamic spin susceptibility in the
-- model is presented. By a sum-rule-conserving generalized mean-field
approximation (GMFA), the two-spin correlation functions of arbitrary range,
the staggered magnetization, the uniform static susceptibility, and the
antiferromagnetic correlation length are calculated in a wide region of hole
doping and temperaturs. A good agreement with available exact diagonalization
(ED) data is found. The correlation length is in reasonable agreement with
neutron-scattering experiments on La_{2-\delta}Sr_\delta)CuO_4. Going beyond
the GMFA, the self-energy is calculated in the mode-coupling approximation. The
spin dynamics at arbitrary frequencies and wave vectors is studied for various
temperatures and hole doping. At low doping a spin-wave-type behavior is found
as in the Heisenberg model, while at higher doping a strong damping caused by
hole hopping occurs, and a relaxation-type spin dynamics is observed in
agreement with the ED results. The local spin susceptibility and its (\omega/T)
scaling behavior are calculated in a reasonable agreement with experimental and
ED data.Comment: 13 pages, 14 figure
A virtual intersubband spin-flip spin-orbit coupling induced spin relaxation in GaAs (110) quantum wells
A spin relaxation mechanism is proposed based on a second-order spin-flip
intersubband spin-orbit coupling together with the spin-conserving scattering.
The corresponding spin relaxation time is calculated via the Fermi golden rule.
It is shown that this mechanism is important in symmetric GaAs (110) quantum
wells with high impurity density. The dependences of the spin relaxation time
on electron density, temperature and well width are studied with the underlying
physics analyzed.Comment: 4+ pages, 4 figures, to be published in Solid Stat. Commu
Robust to impurity-scattering spin Hall effect in two-dimensional electron gas
We propose a mechanism of spin Hall effect in two-dimensional electron gas
with spatially random Rashba spin-orbit interaction. The calculations based on
the Kubo formalism and kinetic equation show that in contrast to the constant
spin-orbit coupling, spin Hall conductivity in the random spin-orbit field is
not totally suppressed by the potential impurity scattering. Even if the
regular contribution is removed by the vertex corrections, the terms we
consider, remain. Therefore, the intrinsic spin-Hall effect exists being,
however, non-universal.Comment: 4+ pages, 2 figure
Physical Limits of the ballistic and non-ballistic Spin-Field-Effect Transistor: Spin Dynamics in Remote Doped Structures
We investigate the spin dynamics and relaxation in remotely-doped two
dimensional electron systems where the dopants lead to random fluctuations of
the Rashba spin-orbit coupling. Due to the resulting random spin precession,
the spin relaxation time is limited by the strength and spatial scale of the
random contribution to the spin-orbit coupling. We concentrate on the role of
the randomness for two systems where the direction of the spin-orbit field does
not depend on the electron momentum: the spin field-effect transistor with
balanced Rashba and Dresselhaus couplings and the (011) quantum well. Both of
these systems are considered as promising for the spintronics applications
because of the suppression of the Dyakonov-Perel' mechanism there makes the
realization of a spin field effect transistor in the diffusive regime possible.
We demonstrate that the spin relaxation through the randomness of spin-orbit
coupling imposes important physical limitations on the operational properties
of these devices.Comment: 10 pages, 4 figure
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