«It was very satisfying to see such high resolution
electron densities by the second day of our experiment, but to then also see such strong signals from the changes in the structure was even more exciting,»
Not exact matches
Between 150 and 350 kilometers above Earth's surface, the
density of free - floating
electrons should drop
by a factor of two as they rejoin atoms, the researchers say.
Scientists have worked out the spatial distribution of
electron and positron
density in Ps as given
by the solution of the Schroedinger equation.
The structure of RuO2 (110) and the mechanism for catalytic carbon monoxide oxidation on this surface were studied
by low - energy
electron diffraction, scanning tunneling microscopy, and
density - functional calculations.
By being able to measure
electron density with high accuracy in atmospheric pressure low - temperature plasma, it is no longer necessary to rely solely upon experience and trial and error.
Further,
by being able to precisely measure
electron density, it will now be possible to clarify through computer simulation the important behaviors of active ion species that play important roles in their interaction with living organisms and materials hazardous to the environment.
Last year, along with researchers led
by Brookhaven / Columbia University School of Engineering physicist Simon Billinge, the team established the first firm link between the disappearance of the
density wave within the pseudogap phase and the emergence, as stated
by Davis, of «universally free - flowing
electrons needed for unrestricted superconductivity» [see: https://www.bnl.gov/newsroom/news.php?a=11637].
«We are demonstrating that when the
electrons are no longer hampered
by the «frozen»
density wave state, they become universally free to flow unimpeded,» Davis said.
Electrons traveling through such a narrow path — racing along in what are called charge -
density waves — can be easily reversed
by virtually any obstacle.
By appropriately decorating those graphene sheets with gold nanoparticles, the INRS - EMT team was able to increase significantly the
density of
electron - emitting sites, and thereby improve their FEE performance.
Researchers from The University of Manchester's Jodrell Bank Centre for Astrophysics have developed and demonstrated a process for continuous
electron density measurement of the previously under - explored D region of the ionosphere — a part of the atmosphere that previously could only be sensitively probed
by short - lived rocket - borne instruments.
As a result, we clarified that the influence of the ion mass appeared remarkably in a high -
density plasma and that the detailed physical mechanism in which turbulence is suppressed through an effect caused
by electron - ion collisions.
The study focuses on two perfectly reflecting model plates, separated
by any non-zero
density plasma, i.e. a charged gas which may contain
electrons only or
electrons and positrons.
«
By modelling experimental synchrotron data and comparing it with
density functional theory calculations, we revealed surprising information about the nature of the
electron sharing between layers in these materials.»
The combination of the high
electron density and potent
electron interactions are not seen in other materials and the quantum regime enforced
by the tight passageway, might here be engendering some new kind of
electron transport.
Now, scientists from the research group of Nir Bar - Gill at the Hebrew University of Jerusalem's Racah Institute of Physics and Department of Applied Physics, in cooperation with Prof. Eyal Buks of the Technion — Israel Institute of Technology, have shown that ultra-high
densities of NV centers can be obtained
by a simple process of using
electron beams to kick carbon atoms out of the lattice.
By adjusting various parameters — such as the
density of conduction
electrons in the material or the strength of the DC electric field — it is possible to tune the cutoff wavenumber and, consequently, the frequency of the resulting terahertz radiation.
Proton
density after laser impact on a spherical solid
density target: irradiated
by an ultra-short, high intensity laser (not in picture) the intense electro - magnetic field rips
electrons apart from their ions and creates a plasma.
A neutral oxygen vacancy, a place where an oxygen atom should appear in the lattice but is instead replaced
by two
electrons, is represented
by the yellow shape, which depicts the charge
density of those
electrons.
Electron densities have been extensively monitored
by means of the Mars Express radio science experiment (Pätzold et al. 2009).
They studied how this spontaneous voltage depends on the current direction, temperature, and the chemical composition (the level of doping
by strontium, which controls the
electron density).
Electron densities measured
by radio - occultations (Pätzold et al. 2007) allow one to derive the overall structure of the ionosphere.
They were also able to measure the modulated
electron density caused
by the substitution.
Snapshots of electronic
density change (
electron wake) produced
by H + moving in Cu with a kinetic energy of 81 keV along a [100] channel.
The quiet - time behavior of the ionospheric
electron density peak height of the F2 region, hmF2, has been evaluated from average
electron density profiles and analytically modeled
by the Spherical Harmonic Analysis (SHA) technique following the same methodology as described
by Altadill et al. (2009).
This feature is mainly a consequence of switching off the photo - detachment of negative ions, thus the negative ions created
by attachment remain below 80 km at night and this results in
electron density depletion.
A joint study carried out
by the Finnish Meteorological Institute and the Sodankylä Geophysical Observatory of the University of Oulu has developed ionospheric
electron density imaging techniques.
For example, if I attempt to do an a priori computation of the quantum structure of, say, a carbon atom, I might begin
by solving a single
electron model, treating the
electron -
electron interaction using the probability distribution from the single
electron model to generate a spherically symmetric «
density» of
electrons around the nucleus, and then performing a self - consistent field theory iteration (resolving the single
electron model for the new potential) until it converges.