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Fabry plane

A simple model that makes it possible to describe optical bistability in a variety of systems is a plane nonlinear Fabry-Perot interferometer, filled with a medium whose refractive index is intensity dependent [106]. The slow kinetics of a... [Pg.477]

Figure 8 Frequency interval between the fundamental mode and the first transverse mode of the Fabry-Perot etalon, measured as a function of the orientation of the plane of incidence of the auxiliary He-Ne laser. Similar behaviour has been observed for the dye laser radiation... [Pg.865]

FAB FEA FEB FET FFP FIB FIELO FIR FLAPW FP FP-LMTO FWHM fast atom beam free A exciton free B exciton field effect transistor far field pattern focused ion beam facet-initiated epitaxial lateral overgrowth far infrared reflectance full-potential linearised augmented plane wave Fabry-Perot full-potential linear muffin-tin orbital full wave at half maximum... [Pg.695]

Measurements of the refractive index under pressure are necessary, in addition to the intrinsic refractive index as physical probes of condensed media, to interpret transmission measurements. This is most conveniently done under pressure by measuring Fabry-Perot interference patterns in plane-parallel samples. The position of the interference maxima in transmission is given by... [Pg.85]

The instrument most commonly used to resolve the Brillouin spectrum is the Fabry-Perot interferometer. This device consists of a pair of highly reflective, optically polished mirrors. The transmission function for a plane parallel Fabry-Perot interferometer is ... [Pg.145]

Another approach to MMW spectrometers is based on the Orotron This device, called after the Russian words for an open resonator and a reflection grating, was a semiconfocal Fabry-Perot cavity (Figure 5.1) with the plane mirror having a reflection grating ruled upon it. The cavity, with 0 lO, produced a spectral bandwidth without frequency locking 10-15 kHz and output power was 3-10 mW over 90-150 GHz. [Pg.83]

Fig. 3.5 Experimental arrangement for intracavity Raman spectroscopy with an argon laser CM, multiple reflection four-mirror system for efficient collection of scattered light LM, laser-resonator mirror DP, Dove prism, which turns the image of the horizontal interaction plane by 90° in order to match it to the vertical entrance slit S of the spectrograph FPE, Fabry-Perot etalon to enforce single-mode operation of the argon laser LP, Littrow prism for line selection [315]... Fig. 3.5 Experimental arrangement for intracavity Raman spectroscopy with an argon laser CM, multiple reflection four-mirror system for efficient collection of scattered light LM, laser-resonator mirror DP, Dove prism, which turns the image of the horizontal interaction plane by 90° in order to match it to the vertical entrance slit S of the spectrograph FPE, Fabry-Perot etalon to enforce single-mode operation of the argon laser LP, Littrow prism for line selection [315]...
FIGURE 41 Illustration of nonlinear Fabry-Perot cavity for optical bistability. The end mirrors are plane and parallel, and the medium in the center exhibits either a nonlinear refractive index or saturable absorption. [Pg.192]

The simplest implementation of an interferometric device is that of the so-called Fabry-Perot (FP) etalon. It consists of two plane-parallel, highly reflecting optical surfaces separated by some distance d, to form a wavelength-selective resonator, akin to that in lasers (see Chapter 3). The reflecting surfaces are formed by multilayer dielectric films on the surface of glass plates. [Pg.190]

Fig. 4.39a,b. Two realizations of a Fabry-Perot interferometer (a) solid etalon (b) air-spaced plane-parallel reflecting surfaces... [Pg.138]

More detailed information on the history, theory, practice, and application of plane and spherical Fabry-Perot interferometers may be found in [4.42-4.44]. [Pg.150]

Fig. 5.42a,b. Fabry-Perot interferometer tuned by a piezocylinder (a) two plane-parallel plates with inner reflecting surfaces (b) two Brewster prisms with the outer coated surfaces forming the FPI reflecting planes... [Pg.270]

Fig. 5. Polarized Rayleigh-Brillouin spectrum of amorphous PnHMA taken with a Burleigh plane Fabry-Perot interferometer using a free spectral range of 12.4 GHz at 295 K. The two Brillouin peaks are shifted from the incident frequency by the product of the wave vector q and the sound velocity u. The line width of the Brillouin peaks is related to the attenuation of the sound waves. PnHMA. Fig. 5. Polarized Rayleigh-Brillouin spectrum of amorphous PnHMA taken with a Burleigh plane Fabry-Perot interferometer using a free spectral range of 12.4 GHz at 295 K. The two Brillouin peaks are shifted from the incident frequency by the product of the wave vector q and the sound velocity u. The line width of the Brillouin peaks is related to the attenuation of the sound waves. PnHMA.
A practical realization of the multiple beam-interference discussed in this section may use either a solid plane-parallel glass or fused quartz plate with two coated reflecting surfaces (Fabry-Perot etalon. Fig. 4.41a) or two separate plates, where one... [Pg.160]


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See also in sourсe #XX -- [ Pg.140 ]




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Fabry

Plane Fabry-Perot Interferometer

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