Sentence examples for electrons subject from inspiring English sources

The principle, formulated by the Danish physicist Niels Bohr about 1920, is an application of the laws of quantum mechanics to the properties of electrons subject to the electric field created by the positive charge on the nucleus of an atom and the negative charge on other electrons that are bound to the nucleus.

We have presented the systematic derivation from the Maximum Entropy Principle of hydrodynamic equations describing a population of electrons subject to spin-orbit interactions.

This paper is devoted to present some results on the derivation of hydrodynamic equations describing electrons subject to spin-orbit-like interactions.

The problem which led Heisenberg to introduce this symmetry (and connect it with the statistical behaviour of quantum particles) in Heisenberg (1926) was to obtain a quantum description of atomic systems seen as ensembles of identical electrons subject to Coulomb interaction in agreement with the spectroscopics results of the time.

Normally the electrons, subjected to a force because of an electric field, accelerate and progressively acquire greater speed.

In this way, electrons subjected to a random potential are not able to move freely through the system if either potential fluctuations due to disorder exceed a critical value or the electron energy is lower than the characteristic potential fluctuation [8, 9].

We consider the energy eigenstates of an electron subject to a harmonic confinement potential V x,y) and a perpendicular magnetic field B where V ( x, y ) = 1 2 m ∗ ω 0 2 ( x 2 + y 2 ) Open image in new window, ω c = eB m ∗ c Open image in new window, and Landau gauge [A=(By,0,0)] has been used.

The dynamics of the single electron subject to the action of the electric potential is now generalized to three dimensions, and the interaction with lattice vibrations is taken into account.

Thin flat dielectric films can be low-macroscopic-field (LMF) electron emitters, able to generate electrons when subject to a macroscopic electric field in the range 1 50 V μm−1.

When materials containing such electrons are subjected to a strong stationary magnetic field, the magnetic axes of the unpaired electrons, or elementary magnets, partially align themselves with the strong external field, and they precess in the field much as the axes of spinning tops often trace cone-shaped surfaces as they precess in the gravitational field of the Earth.

In this work, the edge physics of an Aharonov Bohm interferometer (ABI) defined on a two dimensional electron gas, subject to strong perpendicular magnetic field B, is investigated.