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Spectroscopic Experiments

In this section we offer some comments based to a large extent on eight years of the study, application, and production use of deconvolution with high-resolution infrared absorption spectra. In Chapter 7, a number of specific examples and test cases are presented that illustrate many of the following comments. [Pg.173]

As a rule of thumb, we have found that, in the range of resolution enhancements from 2 to 5, the minimum required signal-to-noise ratio can be approximately represented by an empirical relationship [Pg.174]

Equation (40) is presented as an approximate guideline, and no physical significance is implied by the form or factors used. A generated data test showing the impact of various signal-to-noise ratios is available (see Blass and Halsey, 1981, Fig. 24) further tests and comments will be found in the next chapter. [Pg.174]

One further comment regarding noise in absorption spectral data, it is the signal-to-noise ratio that affects the quality of the results, not the peak-height -to-noise or information-to-noise ratio. This statement assumes that the data to be deconvolved are principally 10-30% absorbing and that the signal-to-noise ratio satisfies the requirements of Eq. (40). That this is a reasonable observation follows from the physically meaningful constraints that are imposed and the deconvolution process as discussed in Chapters 4 and 7. [Pg.174]

As shown in Section I.E.2 of Chapter 2, the transmitted spectral flux U is given by Eq. (9), and in the case of a pressure-broadened line [Pg.174]


Despite its success in reproducing the hydrogen atom spectmm, the Bolir model of the atom rapidly encountered difficulties. Advances in the resolution obtained in spectroscopic experiments had shown that the spectral features of the hydrogen atom are actually composed of several closely spaced lines these are not accounted for by quantum jumps between Bolir s allowed orbits. However, by modifying the Bolir model to... [Pg.3]

However, the reader may be wondering, what is the connection of all of these classical notions—stable nonnal modes, regular motion on an invariant toms—to the quantum spectmm of a molecule observed in a spectroscopic experiment Recall that in the hannonic nonnal modes approximation, the quantum levels are defined by the set of quantum numbers (Up. . Uyy) giving the number of quanta in each of the nonnal modes. [Pg.62]

The intensity autocorrelation measurement is comparable to all of the spectroscopic experunents discussed in the sections that follow because it exploits the use of a variably delayed, gating pulse in the measurement. In the autocorrelation experiment, the gating pulse is just a replica of the time-fixed pulse. In the spectroscopic experiments, the gating pulse is used to mterrogate the populations and coherences established by the time-fixed pulse. [Pg.1975]

In a conventional spectroscopic experiment, the intensity of a rotational transition within a given vibrational band can be written as... [Pg.2077]

Vanderputten D et al 1996 Angle resolved x-ray photoelectron spectroscopic experiments on the full series of molecular [AUgg(PR3) 2 101 clustered. Chem. See. Dalton Trans. 8 1721... [Pg.2921]

Of course, the guesses above aren t really guesses. They are predicated on many years of Raman and other spectroscopic experience and calculations that are the reverse of the calculation we descr ibed. In spectroscopic studies, one normally calculates the force constants from the stretching frequencies in modeling, one... [Pg.96]

Evidence for the radical anion 3 came from esr spectroscopic experiments, thus supporting this mechanism. The radical anion is protonated by the alcohol to give... [Pg.43]

According to this assignment the differentiating electron, that is, the final electron to enter the atom of lutetium, wss seen as an f electron. This suggested that lutetium should be the final element in the first row of the rare earth elements, in which f electrons are progressively filled, and not a transition element as had been believed by the chemists. As a result of more recent spectroscopic experiments the configuration of ytterbium has been altered to (27)... [Pg.14]

Empirical solvent parameters are determined by thermodynamic or spectroscopic experiments which yield parameters representing ... [Pg.458]

The results of x-ray structure analysis and neutron diffraction, as well as spectroscopic experiments (J(HSi) = 70.8 Hz for 30), can be interpreted in the sense mentioned above. The observed reactivity of 30 is also consistent with this view, the coordinated silanes can be displaced smoothly by phosphines, according to first-order reaction kinetics. [Pg.15]

The components of different frequency or wavelength are called lines because, in the early spectroscopic experiments, the radiation from the sample was passed through a slit and then through a prism the image of the slit was then focused on a photographic plate, where it appeared as a line. [Pg.130]

The number of electrons in an atom affects the properties of the atom. The hydrogen atom, with one electron, has no electron-electron repulsions therefore, all the orbitals of a given shell in the hydrogen atom are degenerate. For instance, the 2s-orbital and all three 2p-orbitaIs have the same energy. In many-electron atoms, however, the results of spectroscopic experiments and calculations show... [Pg.156]

Given the result of an HF or DFT calculation, one aims at calculating molecular properties such as spectroscopic observables. The presumably best way to think about such properties is to regard the spectroscopic experiment as a perturbation of... [Pg.149]

Further spectroscopic experiments were carried out with an operating reactor using a bed of 1-mm catalyst beads [13]. A 3D experiment with one spectral and two spatial coordinates was carried out, yielding NMR spectra for each pixel of a 2D axial slice. Figure 5.4.7 shows several representative spectra selected from the entire data set. The NMR spectra of neat AMS [Figure 5.4.7(d)] and cumene [Figure 5.4.7(f)] are provided for comparison, they were experimentally detected for bulk liquid samples (lower traces with narrow lines) and their lines were then mathematically broadened to 300 Hz (upper traces) to account for the broadening in the... [Pg.583]

The reason for pursuing the reverse program is simply to condense the observed properties into some manageable format consistent with quantum theory. In favourable cases, the model Hamiltonian and wave functions can be used to reliably predict related properties which were not observed. For spectroscopic experiments, the properties that are available are the energies of many different wave functions. One is not so interested in the wave functions themselves, but in the eigenvalue spectrum of the fitted model Hamiltonian. On the other hand, diffraction experiments offer information about the density of a particular property in some coordinate space for one single wave function. In this case, the interest is not so much in the model Hamiltonian, but in the fitted wave function itself. [Pg.264]

Figure 3.7. In-situ reflection-absorption infrared (RAIRS) spectra as a function of catalyst temperature from a Pd(lll) single-crystal surface in the presence of a NO + CO gas mixture (240mbar, Pco/Pno = 1-5) [66]. The data clearly show the appearance of an isocyanate-related band at 2256 cm-1 at temperatures above 500 K. In-situ spectroscopic experiments such as these have proven indispensable to detect and identify key reaction intermediates for the catalytic reduction of NO on metal surfaces. (Figure provided by Professor Goodman and reproduced with permission from the American Chemical Society, Copyright 2003). Figure 3.7. In-situ reflection-absorption infrared (RAIRS) spectra as a function of catalyst temperature from a Pd(lll) single-crystal surface in the presence of a NO + CO gas mixture (240mbar, Pco/Pno = 1-5) [66]. The data clearly show the appearance of an isocyanate-related band at 2256 cm-1 at temperatures above 500 K. In-situ spectroscopic experiments such as these have proven indispensable to detect and identify key reaction intermediates for the catalytic reduction of NO on metal surfaces. (Figure provided by Professor Goodman and reproduced with permission from the American Chemical Society, Copyright 2003).
Fig. 4.1. Current and mass signal during an on-line mass spectroscopic experiment showing the effect of adsorbed tin on platinum upon methanol electrooxidation. 1 M CH3OH/0.5 M H2S04 sweep rate 10 mV/s, 24 °C. Fig. 4.1. Current and mass signal during an on-line mass spectroscopic experiment showing the effect of adsorbed tin on platinum upon methanol electrooxidation. 1 M CH3OH/0.5 M H2S04 sweep rate 10 mV/s, 24 °C.
Before discussing details of their model and others, it is useful to review the two main techniques used to infer the characteristics of chain conformation in unordered polypeptides. One line of evidence came from hydrodynamic experiments—viscosity and sedimentation—from which a statistical end-to-end distance could be estimated and compared with values derived from calculations on polymer chain models (Flory, 1969). The second is based on spectroscopic experiments, in particular CD spectroscopy, from which information is obtained about the local chain conformation rather than global properties such as those derived from hydrodynamics. It is entirely possible for a polypeptide chain to adopt some particular local structure while retaining characteristics of random coils derived from hydrodynamic measurements this was pointed out by Krimm and Tiffany (1974). In support of their proposal, Tiffany and Krimm noted the following points ... [Pg.188]

C5Me5)Rhin(L)Cl]+ complexes present a similar electrocatalytic behavior.21,22,25,26,28,29 However, the corresponding Rh-H complex is less stable and could not be isolated, or even characterized, from spectroscopic experiments. [Pg.476]


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Basic spectroscopic experiments

Classes of Spectroscopic Experiment

Experiment 3.6 Visible Spectroscopic Analysis and Jobs Method for

Experiment 3.8 NMR Spectroscopic Analysis of

Experiment total correlation spectroscop

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