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Faraday rotation effect

This generalised definition of the / value for autoionising resonances turns out to be useful in describing the Zeeman and Faraday rotation effects for a Beutler-Fano profile. It also yields a more symmetric form... [Pg.206]

Magnetic nanoparticles showing Faraday rotation effect, and/or Kerr effect can be of interest in the fabrication of switches and devices. Size dependant transmittance and Faraday rotation have been found in maghemite ferrofluids and ferrite films." Multilayered assemblies of yttrium garnet nanoparticles show magnetization-induced second harmonic generation (Kerr effect)." In metal/PMMA nanocomposites, the main absorption band narrows and additional peaks appear when decreasing the particle size." ... [Pg.445]

Figure 10. (a) Two-mode cavity and (b) microwave circuit for Faraday rotation (microwave Hall effect) experiments. [Pg.454]

Roland W. Ure, Jr., Thermoelectric Effects in III-V Compounds Herbert Piller, Faraday Rotation... [Pg.648]

R. J. Stim, Band Structure and Galvanomagnetic Effects in III-V Compounds with Indirect Band Gaps R. W. Ure, Jr., Thermoelectric Effects in III-V Compounds H. Piller, Faraday Rotation... [Pg.180]

Natural optical activity is based on the structure of the molecules (optically active centres). Artificial optical rotation is found in magnetic fields the Faraday-Verdet effect or Magneto-Optic Effect, discovered by Michael Faraday in 1845. The theoretical basis for this effect was developed by James Clerk Maxwell in the 1860s and 1870s. From investigations on small molecules we know that the study of magneto-optical rotation offers interesting correlations with the chemical structure and that additive properties of the Verdet constant have been found. [Pg.299]

Faraday effect test. The measured Faraday rotation peak wavelength showed a blue shift tendency with reduced NPs size. [Pg.438]

The use of Faraday rotation spectroscopy to study high Rydberg members and to measure their / values is a recent development. Little early work was done on magneto-optical effects in the vacuum ultraviolet, which can only be explained in terms of technical difficulties, since the subject is not intrinsically new. [Pg.121]

Although all the examples chosen involve singlet states, for which the theory is especially simple, there is no problem in extending the method to more complex Zeeman patterns, or indeed in including the effect of Paschen-Back uncoupling on the MOV spectrum [166]. The influence of -mixing on MOV patterns has also been studied, and is in principle well understood [167], If the experiment is performed with lasers, the influence of laser power on Faraday rotation arises both by population transfer and by the Autler-Townes splitting (section 9.10) [173]. [Pg.130]

Not all systems are time-reversal invariant. In particular, time-reversal invariance is broken by an external magnetic field. This is most easily understood by considering the physical difference between natural rotation and Faraday rotation in naturally occurring rotation (in a crystal or a sugar solution) the plane of polarisation of the radiation comes back onto itself when the light beam is reflected backwards along the same path. This does not occur in Faraday rotation, where the angle of rotation continues to accumulate for the reflected beam. In fact, the Faraday effect is... [Pg.386]

Electron and hole effective masses of various SiC polytypes have been determined by various methods, such as Hall measurements, Faraday rotation, Zeeman splitting of a photoluminescence line, electron cyclotron resonance, and infrared light reflection. There have also been several theoretical studies of the effective masses of 3C-SiC. The effective masses of electrons and holes thus obtained are listed in TABLE 1. [Pg.69]

Dean et al [7] measured the Zeeman splitting of a luminescence line involving the 2p donor state, obtaining the electron effective mass m t=(0.24 0.01)mo and m /m, =0.36 0.01 for n-type cubic crystals. Measurements of infrared Faraday rotation due to free carriers were made by Ellis and Moss [8] at room temperature in a number of n-type hexagonal specimens belonging to the 6H and 15R polytypes of silicon carbide. One component of the total density-of-states effective mass was explicitly determined by this method. A value for the... [Pg.69]

The interaction between a magnetic field and a light wave propagating in a solid or in a liquid gives rise to a rotation of the plane of polarization. This effect is known as Faraday rotation. It results from a difference in propagation velocity for left and right circular polarized light. [Pg.2133]

Fig. 15. X-ray Faraday effect on Fe in Feo,5Nio,5 [71]. The quantities AjS and A5 are proportional to the Faraday ellipticity ep and the Faraday rotation 0p, respectively. Experimental data (symbols) taken at the L edge of Fe are compared with calculated spectra (full lines). The dashed lines are results of model calculations where the exchange splitting of the 2p core states was neglected. Fig. 15. X-ray Faraday effect on Fe in Feo,5Nio,5 [71]. The quantities AjS and A5 are proportional to the Faraday ellipticity ep and the Faraday rotation 0p, respectively. Experimental data (symbols) taken at the L edge of Fe are compared with calculated spectra (full lines). The dashed lines are results of model calculations where the exchange splitting of the 2p core states was neglected.

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See also in sourсe #XX -- [ Pg.445 ]




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