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Charged-particle state

Appendix A The Lorentz Condition Appendix B Electron Model of Present Theory B.l. General Equations of the Equilibrium State The Charged-Particle State... [Pg.2]

The present model of charged particle states is connected with two fundamental questions in EM held theory. The first of these concerns the electric charge quantization, partly through its relation with the magnetic flux in non-Abelian... [Pg.63]

For the present theory to result in electrically charged particle states it therefore becomes necessary to look into radial functions R that are divergent at the origin. This leads to the subsequent question whether the corresponding integrals (B.9) would then be able to form the basis of an equilibrium having finite and nonzero values of all the quantities qit, Mo, mo, and, v(1. In the next section we will shown how this question can be answered. [Pg.67]

These fluctuations will affect the motion of charged particles. A major part of the Lamb shift in a hydrogen atom can be understood as the contribution to the energy from the interaction of the electron with these zero point oscillations of the electromagnetic field. The qualitative explanation runs as follows the mean square of the electric and magnetic field intensities in the vacuum state is equal to... [Pg.486]

Inelastic collisions of swift, charged particles with matter are completely described by the distribution of generalized oscillator strengths (GOS s) characterizing the collision. These quantities, characteristic of excitation in the N-electron target (or, in fact, of a dressed projectile as well [1]) from some initial state 0) to a final state n) and concomitant momentum transfer, can be written... [Pg.177]

Real charge is always associated with well-defined physical carriers such as electrons and ions this is not so for the idealized physical charge considered in electrostatics. Each conductor can be characterized by stating the nature and concentration of the free charges. In the present section we consider free charged particles of atomic (or molecular) size, not larger, aggregated entities, such as colloidal particles. [Pg.6]

The condition of equilibrium of the charged particles at the interface between two condnctors can be formulated as the state where their electrochemical potentials are the same in the two phases ... [Pg.24]

The work function of charged particles found for a particular conductor depends not only on its bulk properties (its chemical nature), which govern parameter but also on the state of its surface layer, which influences the parameter (a) xhis has the particular effect that for different single-crystal faces of any given metal, the electron work functions have different values. This experimental fact is one of the pieces of evidence for the existence of surface potentials. The work function also depends on the adsorption of foreign species, since this influences the value of... [Pg.141]

Accelerated electrons in the applied electric field ionize gas molecules, and in these ionization processes extra electrons are created. In the steady state the loss of charged particles is balanced by their production. Due to their much lower mass, electrons move much faster than ions. As a result, charge separation creates... [Pg.28]

Assume, that there are adsorption particles with concentration Nt on the surface of semiconductor which is in adsorption equilibrium with a certain gas. A fraction of adsorption particles is charged with concentration designated as w<. Apart from them, on the surface there are various biographic surface states with concentration of the charged particles ng controlling the degree of an a priori band bending qUso-... [Pg.28]

With charged-particle microprobes, the samples must be stained and thinned to improve both contrast and signal-to-noise ratio coated with a thin conducting layer to reduce charging effects and improve spatial resolution and be in vacuum to maintain the charged-particle beams. Finally, information on the chemical state of the detected elements is difficult to obtain using techniques based on charged particles. [Pg.640]

In contrast to PIXE and RBS, where forces are respectively electromagnetic and electrostatic, this kind of microanalysis uses low range nuclear forces. The analysis is based on the detection of the y-rays emitted from nuclei that are in an excited state following a charged particle induced nuclear reaction. [Pg.106]

Excitation and ionization have a common origin-namely, raising the electronic level of an atom or a molecule from its ground state to a state of higher energy via the impact of charged particles or photons. Nevertheless, their chemical fates can be drastically different. In this chapter, we treat these phenomena descriptively. [Pg.71]


See other pages where Charged-particle state is mentioned: [Pg.65]    [Pg.67]    [Pg.65]    [Pg.67]    [Pg.1419]    [Pg.1436]    [Pg.1625]    [Pg.8]    [Pg.29]    [Pg.402]    [Pg.151]    [Pg.459]    [Pg.665]    [Pg.170]    [Pg.277]    [Pg.374]    [Pg.20]    [Pg.675]    [Pg.703]    [Pg.45]    [Pg.168]    [Pg.138]    [Pg.189]    [Pg.26]    [Pg.89]    [Pg.12]    [Pg.20]    [Pg.283]    [Pg.157]    [Pg.159]    [Pg.886]    [Pg.275]    [Pg.4]    [Pg.7]    [Pg.7]    [Pg.7]   


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