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111.
Bimal P. Singh Jayadev Jena Laxmidhar Besra Sarama Bhattacharjee 《Journal of nanoparticle research》2007,9(5):797-806
The dispersion characteristics of nanosize silicon carbide (SiC) suspension were investigated in terms of surface charge,
particle size, rheological measurement and adsorption study. Ammonium polycarboxylate has been used as dispersant to stabilize
the suspension. It was found that the isoelectric point (iep) of SiC powder was pHiep (4.9). The surface charge of powder changed significantly in presence of the ammonium polycarboxylate dispersant and iep
shifted significantly towards lower acidic pH (3.6). The shift in iep has been quantified in terms of ΔG
0
SP, the specific free energy of adsorption between the surface sites and the adsorbing polyelectrolyte (APC). The values of
ΔG
0
SP (−10.85 RT unit) estimated by the electro kinetic data compare well with those obtained from adsorption isotherms (−9.521 RT unit). The experimentally determined optimum concentration of dispersant required for maximizing the dispersion was found
to be 2.4 mg/g of SiC (corresponding to an adsorbed amount of 1.10 mg/g), at pH 7.5. This is much below the full monolayer
coverage (corresponding to adsorbed amount of 1.75 mg/g) of the particles surface by the dispersant. The surface charge quantity,
rheological, pH, electro kinetic and adsorption isotherm results were used to explain and correlate the stability of the nanosize
silicon carbide in aqueous media. At pH 7.5, where both SiC surface and APC are negatively charged, the adsorption of APC
was low because of limited availability of favourable adsorption sites. In addition, the brush-like configuration of the adsorbed
polymer prevented close approach of any additional dispersant; hence stabilization of the slurry happens at a comparatively
lower concentration than the monolayer coverage. 相似文献
112.
Shigeru Odaka Yoshimasa Kurihara 《The European Physical Journal C - Particles and Fields》2007,51(4):867-873
We are developing a consistent method to combine tree-level event generators for hadron collision interactions with those
including one additional QCD radiation from the initial-state partons, based on the limited leading-log (LLL) subtraction
method, aiming at an application to NLO event generators. In this method, a boundary between non-radiative and radiative processes
necessarily appears at the factorization scale (μF). The radiation effects are simulated using a parton shower (PS) in non-radiative processes. It is therefore crucial in our
method to apply a PS which well reproduces the radiation activities evaluated from the matrix-element (ME) calculations for
radiative processes. The PS activity depends on the applied kinematics model. In this paper we introduce two models for our
simple initial-state leading-log PS: a model similar to the ’old’ PYTHIA-PS and a pT-prefixed model motivated by ME calculations. PS simulations employing these models are tested using W-boson production at
LHC as an example. Both simulations show a smooth matching to the LLL subtracted W+1 jet simulation in the pT distribution of W bosons, and the summed pT spectra are stable against a variation of μF, despite that the pT-prefixed PS results in an apparently harder pT spectrum. 相似文献
113.
114.
Boltzmann-transport equation is analytically solved for two-component magnetoplasma using Chapman-Enskog analysis to include
collisional diffusion transport having anisotropies in both streaming velocity and temperature components. The modified collisional
integrals are analytically solved with flux integrals and perturbed kinetic equation to arrive at drift diffusion velocity
and resulting transport coefficients which are markedly affected by both streaming and temperature anisotropy. The early isotropic
results are recovered in the limit V
0 = 0 and T
‖ = T
⊥ which reduce to eqs (11.30) and (11.31) of [1] and eqs (2.7) and (2.13) of [2]. The electrical resistivity (η⊥) diminishes sharply in fusion temperature limit kT
⊥ = 1 keV. The shape of the curves for both electrical resistivity and thermal conductivity is rectangular hyperbolic. However,
for low thermal ratio (T
‖/T
⊥ < 1), the curves are raised up and for high thermal ratio (T
‖/T
⊥ > 1), they are lowered down the isotropic case (T
‖/T
⊥ > 1), showing comparatively diminished magnitudes of the quantities.
相似文献
115.
We study the adiabatic time evolution of quantum resonances over time scales which are small compared to the lifetime of the
resonances. We consider three typical examples of resonances: The first one is that of shape resonances corresponding, for
example, to the state of a quantum-mechanical particle in a potential well whose shape changes over time scales small compared
to the escape time of the particle from the well. Our approach to studying the adiabatic evolution of shape resonances is
based on a precise form of the time-energy uncertainty relation and the usual adiabatic theorem in quantum mechanics. The
second example concerns resonances that appear as isolated complex eigenvalues of spectrally deformed Hamiltonians, such as
those encountered in the N-body Stark effect. Our approach to study such resonances is based on the Balslev-Combes theory
of dilatation-analytic Hamiltonians and an adiabatic theorem for nonnormal generators of time evolution. Our third example
concerns resonances arising from eigenvalues embedded in the continuous spectrum when a perturbation is turned on, such as
those encountered when a small system is coupled to an infinitely extended, dispersive medium. Our approach to this class
of examples is based on an extension of adiabatic theorems without a spectral gap condition. We finally comment on resonance
crossings, which can be studied using the last approach. 相似文献
116.
Aurelien Drezet 《Pramana》2007,68(3):389-396
In a paper by Home and Agarwal [1], it is claimed that quantum nonlocality can be revealed in a simple interferometry experiment
using only single particles. A critical analysis of the concept of hidden variable used by the authors of [1] shows that the
reasoning is not correct.
相似文献
117.
118.
We use different determinantal Hartree-Fock (HF) wave functions to calculate true variational upper bounds for the ground
state energy of N spin-half fermions in volume V
0, with mass m, electric charge zero, and magnetic moment μ, interacting through magnetic dipole-dipole interaction. We find that at high
densities when the average interparticle distance r
0 becomes small compared to the magnetic length r
m ≡ 2mμ2/ħ2, a ferromagnetic state with spheroidal occupation function n
↑(), involving quadrupolar deformation, gives a lower upper bound compared to the variational energy for the uniform paramagnetic
state or for the state with dipolar deformation. This system is unstable towards infinite density collapse, but we show explicitly
that a suitable short-range repulsive (hard core) interaction of strength U
0 and range a can stop this collapse. The existence of a stable equilibrium high density ferromagnetic state with spheroidal occupation
function is possible as long as the ratio of coupling constants Γcm ≡ (U
0
a
3/μ2) is not very small compared to 1.
相似文献
119.
In this study, nanoparticle emission of TiO2 nanopowder coated on different substrates including wood, polymer, and tile, was evaluated in a simulation box and measured
with a Scanning Mobility Particle Sizer (SMPS) for the first time. The coating process for the substrate followed the instructions
given by the supply company. In the simulation box, UV light, a fan, and a rubber knife were used to simulate the sun light,
wind, and human contacting conditions. Among the three selected substrates, tile coated with TiO2 nanopowder was found to have the highest particle emission (22 #/cm3 at 55 nm) due to nanopowder separation during the simulation process. The UV light was shown to increase the release of particle
below 200 nm from TiO2 nanopowder coating materials. The results show that, under the conditions of UV lamps, a fan and scraping motion, particle
number concentration or average emission rate decreases significantly after 60 and 90 min for TiO2/polymer and TiO2/wood, respectively. However, the emission rate continued to increase after 2 h of testing for TiO2/tile. It is suggested that nanoparticle emission evaluation is necessary for products with nanopowder coating. 相似文献
120.
Václav Štengl Snejana Bakardjieva Natalie Murafa Eva Večerníková Jan Šubrt Vladimír Balek 《Journal of nanoparticle research》2007,9(3):455-470
A new method for preparation of titania nanowires with diameter around 10 nm and length up to 2–3 μm is described. The precursor
was prepared from sodium titanate by adding ethylene glycole (EG) and heating at temperature of 198°C for 6 h under reflux.
The sodium titanate glycolate formed by this way aggregated into 1D nanostructures and was subsequently transformed into titania
glycolate during a chemical treatment with 98% sulfuric acid. Titania nanowires with variable amount of anatase and rutile
were prepared by heating to temperatures in the range 350–1000°C. The precursor as well as titania based samples were characterized
by X-ray diffraction, Infrared spectroscopy, Scanning electron microscopy, High resolution transmission microscopy, Thermogravimetry,
Differential thermal analysis, Evolved gas analysis and Emanation thermal analysis. The nitrogen adsorption/desorption was
used for surface area and porosity determination. The photoactivity of the prepared titania samples was assessed by the photocatalytic
decomposition of 4-chlorophenol in an aqueous slurry under UV irradiation of 365 nm wavelength. 相似文献