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Faraday rotator

Figure B2.1.1 Femtosecond light source based on an amplified titanium-sapphire laser and an optical parametric amplifier. Symbols used P, Brewster dispersing prism X, titanium-sapphire crystal OC, output coupler B, acousto-optic pulse selector (Bragg cell) FR, Faraday rotator and polarizer assembly DG, diffraction grating BBO, p-barium borate nonlinear crystal. Figure B2.1.1 Femtosecond light source based on an amplified titanium-sapphire laser and an optical parametric amplifier. Symbols used P, Brewster dispersing prism X, titanium-sapphire crystal OC, output coupler B, acousto-optic pulse selector (Bragg cell) FR, Faraday rotator and polarizer assembly DG, diffraction grating BBO, p-barium borate nonlinear crystal.
Figure 10. (a) Two-mode cavity and (b) microwave circuit for Faraday rotation (microwave Hall effect) experiments. [Pg.454]

Metal-solution interface, quantum mechanical calculations for (Kripsonsov), 174 Metal-water affinity, 177 Micro-balance, quartz crystal, 578 Microwave circuit, 446 for Faraday rotation, 454 Microwave conductivity... [Pg.634]

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

Fig. 21. Faraday rotation for a 2- m thick film of Ga Mn.rAs with x = 0.043 measured as a function of the photon energy in a magnetic field of 6 T at 10 and 300 K (a) and as a function of the magnetic field at 10 K, 1.55 eV and at 300 K, 1.49 eV (b). Solid lines show the magnetization determined from magnetotransport measurements at the given temperatures (scaled to match the open symbols) (Kuroiwa et al. 1998). Fig. 21. Faraday rotation for a 2- m thick film of Ga Mn.rAs with x = 0.043 measured as a function of the photon energy in a magnetic field of 6 T at 10 and 300 K (a) and as a function of the magnetic field at 10 K, 1.55 eV and at 300 K, 1.49 eV (b). Solid lines show the magnetization determined from magnetotransport measurements at the given temperatures (scaled to match the open symbols) (Kuroiwa et al. 1998).
Hadronic models deal with secondary electrons (first proposed by Dennison 1980) produced by the decay of collision/annihilation products (mainly 7r=b —> e ) of p-p (Colafrancesco Blasi 1998, Blasi Colafirancesco 1999) or x- X (e.g., Colafrancesco Mele 2001) interactions. The secondary electrons are produced in situ (thus avoiding to invoke re-acceleration) and require values 1 — 10, found to be more consistent with Faraday Rotation data. These models predict a substantial p/e ratio (like that observed in our Galaxy and in SNe remnants) and an extended modest gamma-ray emission with both hadronic and electronic signatures. The in-situ character of these models produce an extended emission both in space and in time (it is actually stationary) and a quite strong feedback on the ICM (Colafrancesco 1999, Miniafi et al. 2001). [Pg.94]

Figure 9.53 shows the essential parts of a Faraday rotation isolator. The electric field of the forward wave is perpendicular to the plane of the resistive card (a thin... [Pg.536]

Unlike the case of the Faraday rotation isolator, even an elementary description of the operational principle of the circulator is not easy, involving as it does the dimensional resonance of the microwave field within the ferrite cylinder. In this context the word resonance does not signify gyromagnetic resonance but a standing-wave resonance determined by the dimensions of the... [Pg.537]

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]

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

D) Faraday rotation spectra of polymer thin films containing Eui Se sample 1 NPs (black line) and sample 2 NPs (red line). Reprinted with permission from Hasegawa et al. (2008). Copyright 2008 American Chemical Society. [Pg.438]

The spectrum of the Eu2+ (4/ ) ion both in aqueous solution [593] and in the solid state [594—598] has been studied by a number of people. In addition to the usual very strong, broad fn - fn 1d transitions, weak, sharp lines are also observed in the ultraviolet region. These weak lines may possibly be due to the transitions from 8 7/2 to the 6P, Z and D terms of the p configuration. The Faraday rotation measurements [549] on Eu2+ in the cubic fluoride lattice showed that the upper level contained some Pj character. [Pg.125]

Figure 3. The influence of oxygen partial pressure on the Faraday rotation values (maxOr) of polarimtion plane of electromagnetic wave passing tlrough the Bii.gYijFesOn-B films. Figure 3. The influence of oxygen partial pressure on the Faraday rotation values (maxOr) of polarimtion plane of electromagnetic wave passing tlrough the Bii.gYijFesOn-B films.
Together with the Faraday rotation of photon polarization (implementing singlequbit rotations) and linear phase-shift, the cphase gate is universal as it can realize arbitrary unitary transformation [Nielsen 2000],... [Pg.90]


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See also in sourсe #XX -- [ Pg.35 ]

See also in sourсe #XX -- [ Pg.259 , Pg.345 ]




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