Chaotic radiation field

The study of electron interaction with a chaotic radiation field is essentially similar to problems in molecular physics. However, because of its significance for cosmology, the papers on this subject have been placed in the next volume (see also Ya.B. s review [12]). 

The variable can be interpreted as being a chaotic radiation field with a bandwidth X. This radiation field can also be supplemented by a proper frequency (see, e.g., ref. 43). This involves an additional virtual variable without implying a conceptual improvement of the problem under study. 

There are three main reasons for presenting the SSE system in this book, (i) Due to its low dimensionality it is a fundamental system. It is described with the help of analytical tools that are widely used in the analysis of Rydberg atoms in strong radiation fields, (ii) The classical version of the SSE system is chaotic, (iii) Surface state electrons possess an ionization continuum, an important feature in all of atomic physics. Since the SSE system is both simple and physical, it is a natmral candidate for research in classically chaotic driven systems that allow ionization to take place. 

The third noise field is at all angles to the jet axis and at higher frequencies. This sound is generated in precisely the same manner as in subsonic flow by the conventional chaotic turbulence. Recent analysis of experimental data by Tam et al. [11] vividly shows the contributions of the distinct components to the total far-field spectrum — that associated with large-scale motions (inclusive of Mach-wave radiation if it exists) and a component to small-scale turbulence. 

The first process prevails at relatively low frequencies. The electric component E of radiation orients dipole moments p along the field direction, while chaotic molecular motions hinder this orientation p and E are the vectors, and the field E is assumed to vary harmonically with time t. Due to inertia of reorienting molecules the time dependence of the polarization lags behind the time dependence E(f), so that heating of the medium occurs (the heating effect is not considered in this work). The dielectric spectrum obeys the Debye relaxation, for which the absorption monotonically increases with frequency. 

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