590 research outputs found
User\u27s Guide to MBC3: Multi-Blade Coordinate Transformation Code for 3-Bladed Wind Turbine
The dynamics of wind turbine rotor blades are conventionally expressed in rotating frames attached to the individual blades. The tower-nacelle subsystem though, sees the combined effect of all rotor blades, not the individual blades. Also, the rotor responds as a whole to excitations such as aerodynamic gusts, control inputs, and tower-nacelle motion—all of which occur in a nonrotating frame. Multi-blade coordinate transformation (MBC) helps integrate the dynamics of individual blades and express them in a fixed (nonrotating) frame. MBC involves two steps: transforming the rotating degrees of freedom and transforming the equations of motion. Reference 1 details the MBC operation. This guide summarizes the MBC concept and underlying transformations
Comment on "Froehlich Mass in GaAs-Based Structures"
The results of recent measurements of the cyclotron resonance (CR) spectra
for a GaAs quantum well are interpreted in terms of the resonant magnetopolaron
effect. Owing to this effect, the CR peaks split near the TO-phonon frequency
and also change their positions with respect to those obtained without
electron-phonon interaction. The theoretical peak positions of the CR spectra
calculated within the many-polaron approach compare well with experimental
data, as distinct from the CR energies calculated without electron-phonon
interaction, which show no particular features in the region of the
optical-phonon frequencies. We conclude that the Froehlich polaron concept is
valid and even necessary to interpret the CR spectra of quantum wells.Comment: 1 page, 1 figure, E-mail addresses: [email protected],
[email protected]
Room temperature spin coherence in ZnO
Time-resolved optical techniques are used to explore electron spin dynamics
in bulk and epilayer samples of n-type ZnO as a function of temperature and
magnetic field. The bulk sample yields a spin coherence time T2* of 20 ns at T
= 30 K. Epilayer samples, grown by pulsed laser deposition, show a maximum T2*
of 2 ns at T = 10 K, with spin precession persisting up to T = 280 K.Comment: 3 pages, 3 figure
Strong charge-transfer excitonic effects and Bose-Einstein exciton-condensate in graphane
Using first principles many-body theory methods (GW+BSE) we demonstrate that
optical properties of graphane are dominated by localized charge-transfer
excitations governed by enhanced electron correlations in a two-dimensional
dielectric medium. Strong electron-hole interaction leads to the appearance of
small radius bound excitons with spatially separated electron and hole, which
are localized out-of-plane and in-plane, respectively. The presence of such
bound excitons opens the path on excitonic Bose-Einstein condensate in graphane
that can be observed experimentally.Comment: 8 pages, 6 figure
Imaging spin flows in semiconductors subject to electric, magnetic, and strain fields
Using scanning Kerr microscopy, we directly acquire two-dimensional images of
spin-polarized electrons flowing laterally in bulk epilayers of n:GaAs. Optical
injection provides a local dc source of polarized electrons, whose subsequent
drift and/or diffusion is controlled with electric, magnetic, and - in
particular - strain fields. Spin precession induced by controlled uniaxial
stress along the axes demonstrates the direct k-linear spin-orbit
coupling of electron spin to the shear (off-diagonal) components of the strain
tensor.Comment: 5 pages, 5 color figure
Spin-Hall effect in two-dimensional mesoscopic hole systems
The spin Hall effect in two dimensional hole systems is studied by using the
four-terminal Landauer-B\"{u}ttiker formula with the help of Green functions.
The spin Hall effect exists even when there are {\em not} any correlations
between the spin-up and -down heavy holes (light holes) and when the
-point degeneracy of the heavy hole and light hole bands is lifted by
the confinement or recovered by the strain. When only a heavy hole charge
current without any spin polarization is injected through one lead, under right
choice of lead voltages, one can get a pure heavy (light) hole spin current,
combined with a possible impure light (heavy) hole spin current from another
two leads. The spin Hall coefficients of both heavy and light holes depend on
the Fermi energy, devise size and the disorder strength. It is also shown that
the spin Hall effect of two dimensional hole systems is much more robust than
that of electron systems with the Rashba spin-orbit coupling and the spin Hall
coefficients do not decrease with the system size but tend to some nonzero
values when the disorder strength is smaller than some critical value.Comment: 5 pages, 4 figure
Recommended from our members
User's Guide to PreComp (Pre-Processor for Computing Composite Blade Properties)
PreComp (Pre-processor for computing Composite blade structural properties) was developed to compute the stiffness and inertial properties of a composite blade. The code may also be used to compute the structural properties of a metallic blade by treating it as a special case of an isotropic composite material. This guide provides step-by-step instructions on how to prepare input files (specify blade external geometry and internal structural layup of composite laminates), how to execute the code, and how to interpret the output properties. PreComp performs extensive checks for completeness, range, and viability of input data; these are also discussed in this manual. The code runs fast, usually in a fraction of a second, and requires only a modest knowledge of the composites and laminates schedule typically used in blades
Effective Hamiltonian of Strained Graphene
Based on the symmetry properties of graphene lattice, we derive the effective
Hamiltonian of graphene under spatially non-uniform acoustic and optical
strains. We show that with the proper selection of the parameters, the obtained
Hamiltonian reproduces the results of first-principles spectrum calculations
for acoustic strain up to 10%. The results are generalized for the case of
graphene with broken plane reflection symmetry, which corresponds, for example,
to the case of graphene placed at a substrate. Here, essential modifications to
the Hamiltonian give rise, in particular, to the gap opening in the spectrum in
the presence of the out of plane component of optical strain, which is shown to
be due to the lifting of the sublattice symmetry. The developed effective
Hamiltonian can be used as a convenient tool for analysis of a variety of
strain-related effects, including electron-phonon interaction or
pseudo-magnetic fields induced by the non-uniform strain
Theory of exciton fine structure in semiconductor quantum dots: quantum dot anisotropy and lateral electric field
Theory of exciton fine structure in semiconductor quantum dots and its
dependence on quantum dot anisotropy and external lateral electric field is
presented. The effective exciton Hamiltonian including long range electron-hole
exchange interaction is derived within the k*p effective mass approximation
(EMA). The exchange matrix elements of the Hamiltonian are expressed explicitly
in terms of electron and hole envelope functions. The matrix element
responsible for the "bright" exciton splitting is identified and analyzed. An
excitonic fine structure for a model quantum dot with quasi- two-dimensional
anisotropic harmonic oscillator (2DLAHO) confining potential is analyzed as a
function of the shape anisotropy, size and applied lateral electric field
Exciton spin decay modified by strong electron-hole exchange interaction
We study exciton spin decay in the regime of strong electron-hole exchange
interaction. In this regime the electron spin precession is restricted within a
sector formed by the external magnetic field and the effective exchange fields
triggered by random spin flips of the hole. Using Hanle effect measurements, we
demonstrate that this mechanism dominates our experiments in CdTe/(Cd,Mg)Te
quantum wells. The calculations provide a consistent description of the
experimental results, which is supported by independent measurements of the
parameters entering the model.Comment: 5 pages, 3 figure
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