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Monochromatic incident radiation

In the microwave and radiowave regions, virtually monochromatic incident radiation is generated and the need for a monochromator is thus obviated. [Pg.280]

Lambert s law, which concerns the thickness of an absorbing medium, states that successive equal thicknesses absorb equal fractions of monochromatic incident radiation. This leads to an exponential decrease in the intensity of the radiation as it passes through the layer. In mathematical terms,... [Pg.357]

At this point, we consider Equation (A3.1), which is only valid for pure monochromatic incident radiation. As we are dealing with blackbody radiation, we simulate the elemental density of radiation Paidco by monochromatic radiation that has the same power. According to Equation (A3.1), the corresponding probability of elemental transition (absorption or stimulated emission) dP is as follows ... [Pg.272]

Figure 20-26 Schematic diagram of Michelson interferometer. Detector response as a function of retardation (= 2[OM - OS]) is shown for monochromatic incident radiation of wavelength X. Figure 20-26 Schematic diagram of Michelson interferometer. Detector response as a function of retardation (= 2[OM - OS]) is shown for monochromatic incident radiation of wavelength X.
For monochromatic incident radiation, these properties are called spectral and when that radiation is polychromatic they are defined as total (Sandu, 1986). Materials may be classified based on their transmissivity, depending on the physical state of the body where the radiation impinges. A body that does not allow the radiation to be transmitted through it is called opaque and is characterized by r = 0. Examples of these are most solids. On the other hand, liquids and some solids like rock salt or glass have a defined transmissivity so they are transparent to radiation. [Pg.406]

Why the crystalline powder does it necessary Being the monochromatic incident radiation (of the fixed wavelength), for a mono-crystal only one or two diffraction beams would be obtain and therefore die dififraction figure would be poorer in the structural information. [Pg.517]

The atoms knocked out of the lattice positions by impinging particles - which are called primary knock-on atoms (PKAs) - can have various energies from zero to Tm, even for monochromatic incident radiation. In addition, the PKA energy spectrum depends on the incident particle type (mass, charge) and energy. Differences in the PKA energy spectrum lead to differences in the damage caused. The formation of a PKA is equivalent to the formation of a vacancy-interstitial defect pair (or Frenkel pair). [Pg.51]

The classical explanation for the Raman effect, also known as the Plac-zeck theory, takes into account a monochromatic incident radiation acting on the matter. During the time that radiation interacts with matter, both are known as a new system, where the total energy is the matter plus radiation... [Pg.328]


See other pages where Monochromatic incident radiation is mentioned: [Pg.226]    [Pg.1418]    [Pg.28]    [Pg.255]    [Pg.102]    [Pg.443]    [Pg.373]    [Pg.469]    [Pg.35]   
See also in sourсe #XX -- [ Pg.259 ]




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