Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Magneto-optics of the Beutler-Fano resonance

For MOR between bound states, it is in principle possible to determine absolute / values, because the number density N can be eliminated if both a(v) and n(v) are known, as first pointed out by Weingeroff [293]. For a Beutler-Fano profile, this is not possible, essentially because rfano [Pg.208]

The visibility of rotation varies over the profile of a Beutler-Fano res- [Pg.209]

If q — oo, then (a ) — (o /2r) [ x2 — A2)/(x2 + A2)]. For zero or for large detuning, the rotation per unit depth rises to an absolute maximum of a/2T. For q = 0 we note that the rotation per unit absorption depth in the wings does not tend to a constant value (as it does for q — oo), but falls off as aT/2x2 because of continuous absorption, so that any far wing approximation is useless. [Pg.210]

the special case a = T is plotted in fig. 6.6 for different values [Pg.210]

Since autoionising lines narrow down as 1/n 3 in the first autoionisation range, the method can be suitable for high Rydberg states. Sharp autoionising lines do exist and have been known for some time [255, 258, 295]. The first observation of an MOR pattern for an autoionising line is shown in fig. 6.7. The observations agree well with the theory, and a pronounced asymmetry is detected. [Pg.211]


See other pages where Magneto-optics of the Beutler-Fano resonance is mentioned: [Pg.208]   


SEARCH



Beutler

Beutler-Fano resonances

Optical resonance

The resonator

© 2024 chempedia.info