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Optical density bands

Solid solutions are very common among structurally related compounds. Just as metallic elements of similar structure and atomic properties form alloys, certain chemical compounds can be combined to produce derivative solid solutions, which may permit realization of properties not found in either of the precursors. The combinations of binary compounds with common anion or common cation element, such as the isovalent alloys of IV-VI, III-V, II-VI, or I-VII members, are of considerable scientific and technological interest as their solid-state properties (e.g., electric and optical such as type of conductivity, current carrier density, band gap) modulate regularly over a wide range through variations in composition. A general descriptive scheme for such alloys is as follows [41]. [Pg.22]

Valence Band Spectroscopy. Optical and electronic properties of UPD metal flms on metal electrodes have been studied in situ by means of differential- and electroreflectance spectroscopy [98], Optical absorption bands, however, reflect a combined density of electronic states at a photon energy which is the energetic difference of... [Pg.115]

Figure 14 is a plot of the optical density of the 2890 cm-1 band center versus time for the spectra shown in Fig. 13. At the point labeled A on this graph, the H2 C2H. stream was changed to a H2 He stream. The decrease in intensity of the spectrum due to this species (hereafter called X) is rapid initially but becomes slower as time proceeds. The initial rate of falloff (based on the first two points) is such that if this rate were maintained (dashed line), it would, take about 2 min in pure hydrogen to remove all of X from the surface. Similar conclusions are reached if the integrated intensity in the 2925-2825 cm-1 region is plotted as a function of time. Corresponding runs were also made for C2H4-D2 reactant mixture. Figure 14 is a plot of the optical density of the 2890 cm-1 band center versus time for the spectra shown in Fig. 13. At the point labeled A on this graph, the H2 C2H. stream was changed to a H2 He stream. The decrease in intensity of the spectrum due to this species (hereafter called X) is rapid initially but becomes slower as time proceeds. The initial rate of falloff (based on the first two points) is such that if this rate were maintained (dashed line), it would, take about 2 min in pure hydrogen to remove all of X from the surface. Similar conclusions are reached if the integrated intensity in the 2925-2825 cm-1 region is plotted as a function of time. Corresponding runs were also made for C2H4-D2 reactant mixture.
Figure 2 Variations of optical density of vNH band (3390 cm- ) for ZSM-5 (samples 1 and 2) and ZSM-11 (sample 3) vs the outgassing temperature. Wafers of 4.0 mg. cm 2. Figure 2 Variations of optical density of vNH band (3390 cm- ) for ZSM-5 (samples 1 and 2) and ZSM-11 (sample 3) vs the outgassing temperature. Wafers of 4.0 mg. cm 2.
In order to quantitatively analyze the protein patterns, the gels were scanned, and the relative optical density of the bands was plotted against the distance from the start of the gel. [Pg.111]

Results of electrophoretic analysis of proteins in the allantoic fluid and blood serum before and after photodynamic treatment are presented in Figs. 5.5 and 5.6. Visually, we did not detect any changes in the position and intensity of protein bands. In order to quantitatively analyze these parameters we scanned the gels and measured the relative optical density of the bands (Figs. 5.7 and 5.8). [Pg.114]

Two samples of the same phosphor crystal have quite different thicknesses, so that one of them has a peak optical density of 3 at a frequency of vo. while the other one has a peak optical density of 0.2 at vq. Assume a half width at half maximum of Av = IGHz and a peak wavelength of 600 nm, and draw the absorption spectra (optical density versus frequency) for both samples. Then show the absorbance and transmittance spectra that you expect to obtain for both samples and compare them with the corresponding absorption spectra. (To be more precise, you can suppose that both bands have a Lorentzian profile, and use expression (1.8), or a Gaussian line shape, and then use expression (1.9).)... [Pg.36]

A host material is activated with a certain concentration of Ti + ions. The Huang-Rhys parameter for the absorption band of these ions is 5 = 3 and the electronic levels couple with phonons of 150 cm . (a) If the zero-phonon line is at 522 nm, display the 0 K absorption spectrum (optical density versus wavelength) for a sample with an optical density of 0.3 at this wavelength, (b) If this sample is illuminated with the 514 nm line of a 1 mW Ar+ CW laser, estimate the laser power after the beam has crossed the sample, (c) Determine the peak wavelength of the 0 K emission spectrum, (d) If the quantum efficiency is 0.8, determine the power emitted as spontaneons emission. [Pg.196]

This hydrogen band at 3 = 0.2 was also studied with a diffraction grating spectrometer, and its optical density was found to be 0.1 and its half-width to be 21 cm.- (Fig. 10). Condon (134) showed that infrared spectra were expected to be induced by high electric ffelds and that the selection rules... [Pg.287]

Typical spectra obtained at room temperature are given in Fig. 13. Other spectra were obtained in all cases, but a selection is given only of those that are suitable for calculation of apparent optical density. With such broad bands as those occurring in hydrogen bonding, the absorption spectra obtained directly from the spectrometer give little direct information. [Pg.294]

Fig. 20. Peak optical density of the perturbed OH band produced by the adsorption of acetone at 20, 75, and 135° C. and methyl chloride at 20° C. Peak optical densities of the 2,970-cm. CH stretching band of adsorbed methyl chloride are also given. Value obtained on adsorption 0> after desorption X. Fig. 20. Peak optical density of the perturbed OH band produced by the adsorption of acetone at 20, 75, and 135° C. and methyl chloride at 20° C. Peak optical densities of the 2,970-cm. CH stretching band of adsorbed methyl chloride are also given. Value obtained on adsorption 0> after desorption X.
Figure 7. Temperature dependence of the Q(0,0) longwave bands optical densities of compound 10 NH-tautomers 1 and 2 (T = 77 - 500 K) and schematic diagrams of energies of the two lowest singlet (6o,Si) states of tautomers at 77 K according to experimental data. Figure 7. Temperature dependence of the Q(0,0) longwave bands optical densities of compound 10 NH-tautomers 1 and 2 (T = 77 - 500 K) and schematic diagrams of energies of the two lowest singlet (6o,Si) states of tautomers at 77 K according to experimental data.
The dendrimers were dissolved in a THF solution at room temperature to an optical density of 0.1 OD at 430 nm, and excited into the Soret band with a frequency-doubled femtosecond Ti Sapphire oscillator (Spectra Physics). The intensity of the excitation light was kept at... [Pg.496]

Infrared. The measurements were carried out with a Unicam SP100 spectrophotometer using a 10-cm. gas cell. The concentration of acetylene was estimated by measuring the optical density of the absorption band at 729 cm. 1 and that of hydrogen cyanide from the optical density of the absorption band at 712 cm. 1... [Pg.648]

The bands at 1454 and 1542 cm-1 were chosen to measure the quantities of PyL and PyH+ respectively. In Figure 3, the optical densities plotted are relative to the same number of unit cells of zeolite. This figure shows that the number of Bronsted sites capable of chemisorbing Py at... [Pg.469]


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