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Spectral continuity

Function continuation procedures are applied to many other problems besides inverse-filtered Fourier spectral continuation and will be discussed in a separate section. [Pg.266]

The researcher may want to combine the computer program used for inverse filtering with that used for spectral continuation so as to perform the complete restoration in one step. The truncation frequency of the inverse-filtered spectrum could be automatically determined from the rms of the noise and the signal, and the amplitude of the spectrum of the impulse response function. [Pg.324]

Plan Apo (plan apochromatic) Corrected for spherical aberration and spectral continuity. These objectives may contain up to 15 separate lenses, as reflected in their price. For black-and-white photography and under the correct lighting conditions, a Plan lens may equal a Plan Apo lens in resolution. However, for color photomicrographs, the latter is preferred. [Pg.751]

For the characterization (compound identification) of the bands eluting from a fast gas chromatographic separation, time-of-flight mass spectrometry (TOFMS) is unsurpassed. The two unique attributes of TOFMS that make it so well suited as a detector for HSGC are very high spectral acquisition rates and spectral continuity across the chromatographic peak profile for a single-component peak (31). [Pg.247]

Spectral continuity refers to the fact that ion abundance ratios for the different masses in the spectrum are the same for all points on the chromatographic peak. Single-ion abundances vary as the vapor pressure in the ion source changes... [Pg.248]

We call the correlation time it is equal to 1/6 Dj, where Dj is the rotational diffusion coefficient. The correlation time increases with increasing molecular size and with increasing solvent viscosity, equation Bl.13.11 and equation B 1.13.12 describe the rotational Brownian motion of a rigid sphere in a continuous and isotropic medium. With the Lorentzian spectral densities of equation B 1.13.12. it is simple to calculate the relevant transition probabilities. In this way, we can use e.g. equation B 1.13.5 to obtain for a carbon-13... [Pg.1504]

Minimizing Spectral Interferences The most important spectral interference is a continuous source of background emission from the flame or plasma and emission bands from molecular species. This background emission is particularly severe for flames in which the temperature is insufficient to break down refractory compounds, such as oxides and hydroxides. Background corrections for flame emission are made by scanning over the emission line and drawing a baseline (Figure 10.51). Because the temperature of a plasma is... [Pg.437]

More pertinent to the present topic is the indirect dissipation mechanism, when the reaction coordinate is coupled to one or several active modes which characterize the reaction complex and, in turn, are damped because of coupling to a continuous bath. The total effect of the active oscillators and bath may be represented by the effective spectral density For instance, in the... [Pg.20]

REELS will continue to be an important surface analytical tool having special features, such as very high surface sensitivity over lateral distances of the order of a few pm and a lateral resolution that is uniquely immune from back scattered electron effects that degrade the lateral resolution of SAM, SEM and EDS. Its universal availability on all types of electron-excited Auger spectrometers is appealing. However in its high-intensity VEELS-form spectral overlap problems prevent widespread application of REELS. [Pg.333]

The chemical and electronic properties of elements at the interfaces between very thin films and bulk substrates are important in several technological areas, particularly microelectronics, sensors, catalysis, metal protection, and solar cells. To study conditions at an interface, depth profiling by ion bombardment is inadvisable, because both composition and chemical state can be altered by interaction with energetic positive ions. The normal procedure is, therefore, to start with a clean or other well-characterized substrate and deposit the thin film on to it slowly at a chosen temperature while XPS is used to monitor the composition and chemical state by recording selected characteristic spectra. The procedure continues until no further spectral changes occur, as a function of film thickness, of time elapsed since deposition, or of changes in substrate temperature. [Pg.30]

A distinction must be made between continuous sources (hydrogen or deuterium lamps, incandescent tungsten lamps, high pressure xenon lamps) and spectral line sources (mercury lamps), which deliver spectrally purer light in the region of their emission lines. [Pg.20]

Continuous sources The sources of choice for measurements in the ultraviolet spectral region are hydrogen or deuterium lamps [1]. When the gas pressure is 30 to 60 X10 Pa they yield a continuous emission spectrum. The maxima of their radiation emission occur at different wavelengths (Hi A = 280 nm Di 2 = 220 nm). This means that the deuterium lamp is superior for measurements in the lower UV region (Fig. 15). [Pg.21]

Dependence of apparent constants on concentration. We continue the consideration of Scheme XXIII by making chemically reasonable tentative selections of the forms of A a and k[. First, consider the acetyl chloride-alcohol reaction. Because the spectral observations show that intermediate formation is essentially complete, this system belongs to the case in which kdk i may be treated as infinite (Scheme XXIV). The observed reaction is then... [Pg.121]

Cole and Davidson s continuous distribution of correlation times [9] has found broad application in the interpretation of relaxation data of viscous liquids and glassy solids. The corresponding spectral density is ... [Pg.170]

Spectral Gamma Ray Log. This log makes use of a very efficient tool that records the individual response to the different radioactive minerals. These minerals include potassium-40 and the elements in the uranium family as well as those in the thorium family. The GR spectrum emitted by each element is made up of easily identifiable lines. As the result of the Compton effect, the counter records a continuous spectrum. The presence of potassium, uranium and thorium can be quantitatively evaluated only with the help of a computer that calculates in real time the amounts present. The counter consists of a crystal optically coupled to a photomultiplier. The radiation level is measured in several energy windows. [Pg.973]

Flame emission spectroscopy - continued evaluation methods, 800 flames, temperature of, 784 general discussion, 779 interferences, 791 chemical, 792 spectral, 792... [Pg.864]

The prediction step for PLS is also slightly different than for PCR. It is also done on a rank-by-rank basis using pairs of special and concentration factors. For each component, the projection of the unknown spectrum onto the first spectral factor is scaled by a response coefficient to become a corresponding projection on the first concentration factor. This yields the contribution to the total concentration for that component that is captured by the first pair of spectral and concentration factors. We then repeat the process for the second pair of factors, adding its concentration contribution to the contribution from the first pair of factors. We continue summing the contributions from each successive factor pair until all of the factors in the basis space have been used. [Pg.132]

PLS finds these factors, W, one-by-one. First, the most significant optimum factor, W, is found. Then, that portion of the variance in the spectral data that is spanned by W is removed from the spectra. Similarly, that portion of the variance in the concentrations that is spanned by W, is removed from the concentrations. Then the next factor, W2, is found for the spectral and concentration residuals that were not spanned by W. The process is continued until all possible factors have been found. [Pg.140]

Fig. 1-17 (Continued). All lines with intensity greater than 1% of the strongest line in the spectral series are shown for the K and L states. As the line is emitted, the electron moves up the arrow the state of the atom moves down. Fig. 1-17 (Continued). All lines with intensity greater than 1% of the strongest line in the spectral series are shown for the K and L states. As the line is emitted, the electron moves up the arrow the state of the atom moves down.
Raman effect (continued) spectral activity, 339-341 terminology of, 295 vibrational wavefunctione, 339-341 Raman lines, 296 weak, 327-330 Raman scattering, 296 classical theory, 297-299 quantum mechanical theory, 296, 297 Raman shift, 296... [Pg.420]

The intensity at the periphery of the line ( Ageneral rule (2.62) [20, 104]. However, the most valuable advantage of general formula (3.34) is its ability to describe continuously the spectral transformation from a static contour to that narrowed by motion (Fig. 3.1). In the process of the spectrum s transformation its maximum is gradually shifted, the asymmetry disappears and it takes the form established by perturbation theory. [Pg.100]


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See also in sourсe #XX -- [ Pg.248 ]




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Spectral density continuous

Spectral relaxation continuous

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