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Fourier transforms for

Besides the intrinsic usefulness of Fourier series and Fourier transforms for chemists (e.g., in FTIR spectroscopy), we have developed these ideas to illustrate a point that is important in quantum chemistry. Much of quantum chemistry is involved with basis sets and expansions. This has nothing in particular to do with quantum mechanics. Any time one is dealing with linear differential equations like those that govern light (e.g. spectroscopy) or matter (e.g. molecules), the solution can be written as linear combinations of complete sets of solutions. [Pg.555]

The breakdown of a given signal into a sum of oscillatory functions is accomplished by application of Fourier series techniques or by Fourier transforms. For a periodic function F t) with a period t, a Fourier series may be expressed as... [Pg.560]

Lam, R. B., Wieboldt, R. C., and Isenhour, T. L., Practical Computation with Fourier Transforms for Data Analysis, Anal. Chem. 53, 1981, 889A-901A. [Pg.413]

In contrast to MoSx/NaY, the Fourier transform for MoSj/NaY clearly showed Mo-O bondings as well as Mo-S and Mo-Mo bondings as summarized in Table 1. It is evident that Mo oxide species in calcined MoOj/NaY are only partially sulfided. XPS results corroborated the EXAFS results. The incomplete sulfidation of the Mo species in MoS /NaY may explain in part the relatively low HDS and HYD activities of the cat ysts in Figs.l and 2. [Pg.506]

The Fourier transforms for both films are again quite similar, but as for the ex situ measurements, the chromate-passivated films appear to have a more glassy structure. It should be mentioned that these studies employed a rather limited data range which makes spectral differentiation difficult. [Pg.294]

The evaluation of the contribution of cycle diagrams to the activity coefficient is formally complete once the eigenvalues of SI have been found. Let us write the result explicitly in terms of the Fourier transforms for the important case of two defects a and / each of which is allowed to occupy a particular one of the two positions in the unit cell. In this simple system the labelling of positions in the unit cell by superscripts on Fourier transforms becomes redundant and can be omitted. The result is... [Pg.53]

J = The discrete Fourier transform for that case. x = actual data. i = increment in the series. w = frequency. t = time. [Pg.950]

An alternative approach involves integrating out the elastic degrees of freedom located above the top layer in the simulation.76 The elimination of the degrees of freedom can be done within the context of Kubo theory, or more precisely the Zwanzig formalism, which leads to effective (potentially time-dependent) interactions between the atoms in the top layer.77-80 These effective interactions include those mediated by the degrees of freedom that have been integrated out. For periodic solids, a description in reciprocal space decouples different wave vectors q at least as far as the static properties are concerned. This description in turn implies that the computational effort also remains in the order of L2 InL, provided that use is made of the fast Fourier transform for the transformation between real and reciprocal space. The description is exact for purely harmonic solids, so that one can mimic the static contact mechanics between a purely elastic lattice and a substrate with one single layer only.81... [Pg.104]

Wangen, L. E., Frew, B. M., Isenhour, T. L., Jurs, P. C. Appl. Spectros. 25, 1971, 203-207. Investigation of the fourier transform for analyzing spectroscopic data by computerized learning machines. [Pg.43]

Fig. 12 Moduli of the Fourier transform for CojcAl at Co K-edge (x = 2 (black circle) and X = 3 (empty square)). The distances are not corrected from phase shifts... Fig. 12 Moduli of the Fourier transform for CojcAl at Co K-edge (x = 2 (black circle) and X = 3 (empty square)). The distances are not corrected from phase shifts...
The effects of particle size on the EXAFS region of the XAS spectra are reflected in the coordination numbers obtained in the fits to the EXAFS data. Figure 15 shows the EXAFS or xi ) data and corresponding Fourier transforms for a Pt foil, a Pt02... [Pg.381]

Figure 31. Ru K EXAFS data (insets) and correspmding Fourier transforms for Ru tSej particles on a Sn02 F support in (a) nitrogen and (b) oxygen saturated 0.5 i ol dm H2SO4 experimental data (thin lines) and fits hicK lines).(Reproduced with permission from ref 149. Copyright 2000 Elsevier Sequoia S.A., Lausanne.)... Figure 31. Ru K EXAFS data (insets) and correspmding Fourier transforms for Ru tSej particles on a Sn02 F support in (a) nitrogen and (b) oxygen saturated 0.5 i ol dm H2SO4 experimental data (thin lines) and fits hicK lines).(Reproduced with permission from ref 149. Copyright 2000 Elsevier Sequoia S.A., Lausanne.)...
Any modification of the magnetization thus arises from relaxation phenomena. The transverse magnetization spin-locked along must end up at its thermal equilibrium value, that is zero. The corresponding evolution is exponential with a time constant denoted by Tip (relaxation time in the rotating frame), very close (if not identical) to T. In practice, the signal is measured (and subsequently Fourier transformed) for a set of x values, in successive experiments, and obeys the equation... [Pg.13]

Fourier transform for different, chemically very similar halomethanes and a mixture thereof. The time-domain data in Figure 7.11 can be directly interpreted as an observation of molecular motion in real time, made possible by the compressed ultrashort pulses in the microscope. From the presence of different oscillatory patterns and beatings, it already becomes clear that the different molecules can be discriminated with high resolution. Correspondingly, the Fourier spectra in Figure 7.11 show markedly different vibrational resonances, which can also be discriminated in the ternary mixture of all components. [Pg.185]

P.D. Welch, The use of fast Fourier transform for the estimation of power spectra A method based an time averaging over short, modified periodigrams. IEEE Trans. Audio and Electroacustics. AU-15 (1967) 70-73. [Pg.260]

The proof is a straightforward application of the fundamental properties of the Fourier transform, namely, its linearity, and how it intertwines differentiation, multiplication and convolution. This material is available in any introduction to Fourier transforms for example, see [DyM, Chapter 2]. The only tricky part is the calculation of the Fourier transform of the Coulomb potential. See Exercise 9.3. [Pg.284]

Figure 9.9 Fourier transform for Fe K-edge EXAFS of FeN0 9I... Figure 9.9 Fourier transform for Fe K-edge EXAFS of FeN0 9I...
Figure 9.12 Schematic crystal structure of Ni2N and Fourier transform for Fe K-edge EXAFS of (Ni(l 7-,FC 27)2N. O, transition metal , nitrogen. Figure 9.12 Schematic crystal structure of Ni2N and Fourier transform for Fe K-edge EXAFS of (Ni(l 7-,FC 27)2N. O, transition metal , nitrogen.
Figure 7. Corresponding time (kx,ky) and frequency (x,y) domain data in two-dimensional image using Fourier transform for two uniform circular objects. The time domain S(kx,ky) is successively one- and two-dimensionally Fourier transformed to arise the spectra S (kx,y) and S"(x,y). Figure 7. Corresponding time (kx,ky) and frequency (x,y) domain data in two-dimensional image using Fourier transform for two uniform circular objects. The time domain S(kx,ky) is successively one- and two-dimensionally Fourier transformed to arise the spectra S (kx,y) and S"(x,y).
Fourier channel k. The phase is known up to a multiple of 27t(since only exp /( ),(/")) is known). Time-scale modifications also require the knowledge of the instantaneous frequency G) (f ). 0), Uua) can also be estimated from successive short-time Fourier transforms for a given value of k, computing the backward difference of the short-time Fourier transform phase yields... [Pg.160]

We obtain the well known result that off-diagonal elements oscillate in time. Now define Fourier-transform for lesser function (r = t —12)... [Pg.265]

FT/ICR experiments have conventionally been carried out with pulsed or frequency-sweep excitation. Because the cyclotron experiment connects mass to frequency, one can construct ("tailor") any desired frequency-domain excitation pattern by computing its inverse Fourier transform for use as a time-domain waveform. Even better results are obtained when phase-modulation and time-domain apodization are used. Applications include dynamic range extension via multiple-ion ejection, high-resolution MS/MS, multiple-ion simultaneous monitoring, and flatter excitation power (for isotope-ratio measurements). [Pg.21]

Kwok, Y.C., Manz, A., Shah convolution differentiation Fourier transform for rear analysis in microchip capillary electrophoresis../. Chromatogr. A 2001, 924(1-2), 177-186. [Pg.445]

Figure 2.26. Quantum beat-modulated fluorescence decay and its Fourier transform for the l W level of Sj thiophosgene. (Reprinted with permission from Ref. [42].)... Figure 2.26. Quantum beat-modulated fluorescence decay and its Fourier transform for the l W level of Sj thiophosgene. (Reprinted with permission from Ref. [42].)...
Gutjhar AL (1989) Fast Fourier transform for random field generation. Los Alamos Report 4-R58-2690R, New Mexico Institute of Mining and Technology, Socorro, NM... [Pg.131]


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