21,566 research outputs found
Dyes removal from water using low cost absorbents
In this study, the removal capacity of low cost adsorbents during the adsorption of Methylene Blue (MB) and Congo Red (CR) at different concentrations (50 and 100mg•L-1) was evaluated. These adsorbents were produced from wood wastes (cedar and teak) by chemical activation (ZnCl2). Both studied materials, Activated Cedar (AC) and activated teak (AT) showed a good fit of their experimental data to the pseudo second order kinetic model and Langmuir isotherms. The maximum adsorption capacities for AC were 2000.0 and 444.4mg•g-1 for MB and CR, respectively, while for AT, maximum adsorption capacities of 1052.6 and 86.4mg•g-1 were found for MB and CR, respectively. © Published under licence by IOP Publishing Ltd
Spin nematics and magnetization plateau transition in anisotropic Kagome magnets
We study S=1 kagome antiferromagnets with isotropic Heisenberg exchange
and strong easy axis single-ion anisotropy . For , the low-energy
physics can be described by an effective model with
antiferromagnetic and ferromagnetic .
Exploiting this connection, we argue that non-trivial ordering into a
"spin-nematic" occurs whenever dominates over , and discuss its
experimental signatures. We also study a magnetic field induced transition to a
magnetization plateau state at magnetization 1/3 which breaks lattice
translation symmetry due to ordering of the and occupies a lobe in the
- phase diagram.Comment: 4pages, two-column format, three .eps figure
Semiclassical ordering in the large-N pyrochlore antiferromagnet
We study the semiclassical limit of the generalization of the
pyrochlore lattice Heisenberg antiferromagnet by expanding about the saddlepoint in powers of a generalized inverse spin. To leading order,
we write down an effective Hamiltonian as a series in loops on the lattice.
Using this as a formula for calculating the energy of any classical ground
state, we perform Monte-Carlo simulations and find a unique collinear ground
state. This state is not a ground state of linear spin-wave theory, and can
therefore not be a physical (N=1) semiclassical ground state.Comment: 4 pages, 4 eps figures; published versio
The symmetry of the spin Hamiltonian in herbertsmithite, a spin-1/2 kagom\'{e} lattice
We present magnetization measurements on oriented powder of
ZnCu(OH)Cl along and perpendicular to the orienting field. We
find a dramatic difference in the magnetization between the two directions. It
is biggest at low measurement fields or high temperatures. We show that the
difference at high temperatures must emerge from Ising-like exchange
anisotropy. This allows us to explain muon spin rotation data at in
terms of an exotic ferromagnetic ground state.Comment: 5 pages, 5 figure
The effect of the lateral interactions on the critical behavior of long straight rigid rods on two-dimensional lattices
Using Monte Carlo simulations and finite-size scaling analysis, the critical
behavior of attractive rigid rods of length k (k-mers) on square lattices at
intermediate density has been studied. A nematic phase, characterized by a big
domain of parallel k-mers, was found. This ordered phase is separated from the
isotropic state by a continuous transition occurring at a intermediate density
\theta_c, which increases linearly with the magnitude of the lateral
interactions.Comment: 7 pages, 6 figure
Perturbative evolution of the static configurations, quasinormal modes and quasi normal ringing in the Apostolatos - Thorne cylindrical shell model
We study the perturbative evolution of the static configurations, quasinormal
modes and quasi normal ringing in the Apostolatos - Thorne cylindrical shell
model. We consider first an expansion in harmonic modes and show that it
provides a complete solution for the characteristic value problem for the
finite perturbations of a static configuration. As a consequence of this
completeness we obtain a proof of the stability of static solutions under this
type of perturbations. The explicit expression for the mode expansion are then
used to obtain numerical values for some of the quasi normal mode complex
frequencies. Some examples involving the numerical evaluation of the integral
mode expansions are described and analyzed, and the quasi normal ringing
displayed by the solutions is found to be in agreement with quasi normal modes
found previously. Going back to the full relativistic equations of motion we
find their general linear form by expanding to first order about a static
solution. We then show that the resulting set of coupled ordinary and partial
differential equations for the dynamical variables of the system can be used to
set an initial plus boundary values problem, and prove that there is an
associated positive definite constant of the motion that puts absolute bounds
on the dynamic variables of the system, establishing the stability of the
motion of the shell under arbitrary, finite perturbations. We also show that
the problem can be solved numerically, and provide some explicit examples that
display the complete agreement between the purely numerical evolution and that
obtained using the mode expansion, in particular regarding the quasi normal
ringing that results in the evolution of the system. We also discuss the
relation of the present work to some recent results on the same model that have
appeared in the literature.Comment: 27 pages, 7 figure
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