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Optical systems reflections

A schematic of a PL system layout is shown in Figure 5. This optical system is very similar to that required for absorption, reflectance, modulated reflectance, and Raman scattering measurements. Many custom systems are designed to perform several of these techniques, simultaneously or with only small modifications. [Pg.383]

Nanobeam optics with beam diameters of several nanometers are presently developed at the ESRF. Using a Kirkpatrick-Baez optical system (cf. Fig. 4.9) beam diameters of 80 nm have been achieved. The Kirkpatrick-Baez system is made from two successively reflecting, orthogonal mirrors that are bent into elliptical shape by mechanical benders. The focused flux is strongly increased by deposition of a graded multilayer structure similar to that used with the parabolic Gobel mirror. [Pg.66]

Figure 3. Optical system of instrument of spectral sensitivity measurement (L) Xe arc lamp (Ml) concave mirror (M2, M3) mirror (S) shutter (SI) slit (G) concave reflective grating... Figure 3. Optical system of instrument of spectral sensitivity measurement (L) Xe arc lamp (Ml) concave mirror (M2, M3) mirror (S) shutter (SI) slit (G) concave reflective grating...
Incorrect conclusion 1 above is sometimes said to derive from the reciprocity principle, which states that light waves in any optical system all could be reversed in direction without altering any paths or intensities and remain consistent with physical reality (because Maxwell s equations are invariant under time reversal). Applying this principle here, one notes that an evanescent wave set up by a supercritical ray undergoing total internal reflection can excite a dipole with a power that decays exponentially with z. Then (by the reciprocity principle) an excited dipole should lead to a supercritical emitted beam intensity that also decays exponentially with z. Although this prediction would be true if the fluorophore were a fixed-amplitude dipole in both cases, it cannot be modeled as such in the latter case. [Pg.302]

The optical system comprises a laser, which is reflected by a mirror mounted on the back of the cantilever to another mirror that sends the reflected beam to an array detector. The position of the beam translates in the position of the cantilever in the vertical direction, whereas the lateral position in xy coordinates is inferred from the movement of the xy table. Essentially, AFM uses a feedback system to measure and regulate the force applied on the scanned sample, which allows the acquisition of images using very low forces. [Pg.117]

Figure 1 Optical systems for near-infrared reflectance,... Figure 1 Optical systems for near-infrared reflectance,...
It is inadvisable to mount two or more filters close together in the light path to increase their blocking power. In a miniaturized optical system, the optical densities of the filters will not necessarily add. If the filters are parallel and positioned closely together in parallel uncollimated light be reflected at the second filter will be reflected again at the first. After several reflection... [Pg.32]

An important application for garnets is for isolators in optical communications systems. Reflections from end-faces of components and interconnections in an optical transmission line have a destabilizing effect on the operation of the laser sources and have to be eliminated. This is achieved using an optical isolator , the optical analogue (2 typically in the range 1.30—1.55 /mi) of the microwave isolator described in Section 9.5.5. [Pg.535]

The same fixed optical system can be used for the spectral and topographic option, to provide the required dispersion on the OMA channels. The demagnification of 1/15 mentioned in a preceding section is obtained by a 381 lens (Fig. IB, S, 1C and IE, m) at its focal distance from the slit together with a Dallmeyer Ultrac camera lens, F/0.98 of focal length 25 mm (Fig. 1C, IE, p) in the beam of light diffracted from the grating or reflected from the mirror, 1/15. [Pg.276]


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Optical system reflecting

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