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Absorption length

For concentrated or bulk samples a transmission experiment is both the simplest and the most effective. In essence, one measures the X-ray intensities incident and transmitted through a thin and uniform film of the material. Careful analysis of signal-to-noise ratio considerations indicates that optimal results are obtained when the sample thickness is of the order of 2.5 absorption lengths. Since in this case a simple Beer s law applies, the data are usually plotted as In(7//0) versus E. The intensities are measured using ionization chambers in conjunction with high-gain electrometers (see Fig. 11). [Pg.288]

Liu CY, Bard AJ (1989) Effect of excess charge on band energetics (optical absorption length and carrier redox potential) in small semiconductor particles. Phys Chem 93 3232-3237. [Pg.254]

The spectra shown in Fig. 3.1 appear as unstructured, broad absorption bands, with a maximum of absorption around 200 cm-1 for the lightest system and at lower frequencies for the more massive pairs. Absorption is weak, even at the peaks, and amounts to a mean absorption length of more than 1/a 106 cm (that is 10 km) if both gases are present at partial pressures of just one atmosphere. Absorption of rare gas mixtures increases, however, with increasing densities, with a mean absorption length of centimeters as we approach liquid densities. [Pg.59]

Figure 13. Absorption length La and depletion layer width W of an ideally smooth WSe2 electrode in contact with an electrolyte, assuming e = 9 and n,= X 106... Figure 13. Absorption length La and depletion layer width W of an ideally smooth WSe2 electrode in contact with an electrolyte, assuming e = 9 and n,= X 106...
D0 the optical absorption length is the distance the infrared radiation can travel through the sample (cm), equal to 1/p where P is the optical absorption coefficient... [Pg.51]

Blue, chosen because it s absorption was peaked at 620 nm and because it had a deep absorption minimum around 450 nm. In later work, a thiobarbituric acid derivative in PMMA produced an efficiency of 39 % W 1 cm-2 over an estimated 32 pm absorption length [62]. This was followed recently with new tricyanovi-nylaniline doped polymers in which a net efficiency of nearly 250% W 1 cnr2 was demonstrated over 35 pm. [63] An added bonus was that this approach proved to be the stimulus for many materials to be characterized. Materials with p[3 values as large as 3,800x10 48 esu, coupled with good transparency in the 450-470 nm window, were synthesized and optimistically predicted to satisfy criteria for ADPM SHG with target efficiencies of about 2000% W 1 [64] ... [Pg.105]

Surface recombination reduces the luminescence intensity when the excitation light has a very short absorption length. The effect is weak because of the low carrier mobility and diffusion length, so that although there are many defects at the surface of a-Si H, the effect on the luminescence intensity is only 10-20% (Dunstan 1981). A measure of the surface recombination is the product, aLp, of the optical absorption coefficient and the diffusion length. In most situations in a-Si H, and particularly at low temperature, aLp is less than unity, whereas in crystals it is often much greater. [Pg.307]

Source Brightness (particles cm eV steradian ) Elastic Mean 1 Free Path (A) Absorption Length (A) Minimum Probe Size (A)... [Pg.362]

Radiation groups (2) (Ratio of L to radiation absorption length and blackbody radiation flux to enthalpy convection),... [Pg.278]


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See also in sourсe #XX -- [ Pg.71 ]

See also in sourсe #XX -- [ Pg.1081 ]

See also in sourсe #XX -- [ Pg.134 , Pg.135 , Pg.152 ]




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