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Photon absorption spectroscopies, transmission

It is not surprising therefore that the optical properties of small metal particles have received a considerable interest worldwide. Their large range of applications goes from surface sensitive spectroscopic analysis to catalysis and even photonics with microwave polarizers [9-15]. These developments have sparked a renewed interest in the optical characterization of metallic particle suspensions, often routinely carried out by transmission electron microscopy (TEM) and UV-visible photo-absorption spectroscopy. The recent observation of large SP enhancements of the non linear optical response from these particles, initially for third order processes and more recently for second order processes has also initiated a particular attention for non linear optical phenomena [16-18]. Furthermore, the paradox that second order processes should vanish at first order for perfectly spherical particles whereas experimentally large intensities were collected for supposedly near-spherical particle suspensions had to be resolved. It is the purpose of tire present review to describe the current picture on the problem. [Pg.646]

Measurements using extended x-ray absorption fine-structure (EXAFS) spectroscopy were made on the insertion-device beam line of the Materials Research Collaborative Access Team (MRCAT) at the Advanced Photon Source, Argonne National Laboratory. Measurements were made in transmission mode with ionization chambers optimized for the maximum current with linear response ( 10 photons detected/sec). A cryogenically cooled double-crystal Si (111) monochromator with resolution (AE) better than 2.5 eV at 11.564 keV (Pt L3 edge) was used in conjunction with a Rh-coated mirror to minimize the presence of harmonics [9]. The integration time per data point was 1-3 sec, and three scans were obtained for each processing condition. [Pg.473]

Summary For the preparation of photonic crystals, colloid particles with high refractive indices are formed with diameters from a few nanometers up to several hundred nanometers. Whereas the optical density of Ti02 is already given by the titanium atom itself, the incorporation of dyes in these SiOi systems increases the refractive indices (near the absorption wavelength). The colloid particles are characterized by dynamie and static light scattering, SEM, MAS-NMR, UVA is, and optical transmission/reflection spectroscopy. [Pg.785]

Light interacts with solid materials as scattering, absorption, transmission (transmittance), reflectance (both regular and diffuse), and diffraction. The purpose of spectroscopy is to quantify or qualify these interactions by the use of a variety of photon-produdng and photon-detection devices. The physics of these interaction phenomena and devices will be presented in this chapter. [Pg.226]

Basic principles. In Raman spectroscopy, a laser beam (monochromatic light) is directed perpendicularly at the sample. The major part of the light is subject to the common optical laws (absorption, reflection and transmission). A very small part (less than 10 of the incident beam) is reflected via an inelastic scattering of the photons by the lattice phonons. This is the first order Raman scattering. This is the only Raman scattering effect observed for diamond at the excitation energies used. The... [Pg.88]


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