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Power Fourier transform

Developments in two general areas have spurred this progress. Sector and quadrupole mass analysers, the traditional methods of separation of ions in MS, have recently been complemented by the development of powerful Fourier transform (FT-MS) and time-of-flight (TOF-MS) instruments. The TOF analysers are particularly well-suited for detecting higher molar-mass species present in polymers. [Pg.18]

Figure 13. (a) Emission spectra from 5.5 pm thick films containing 0% (solid line) and 20% (dashed line) 8MMAPOSS (b) Emission spectrum from a 5.5 pm film containing 50% 8MMAPOSS and (inset) Power Fourier Transform of spectrum and (c) Edge-on emission from film in (b). [Pg.106]

Polyhedral oligomeric silsesquioxanes Power Fourier transform Pyrromethene Solid-state dye lasers... [Pg.108]

In the early sixties Fourier transform spectroscopy was fully dependent on the access to very large computers. With the evolution towards ever more powerful and smaller computers, even the most powerful Fourier transform spectrometers can now be operated with small dedicated computers. [Pg.45]

As in the case of infrared, progress in computing and the development of powerful algorithms for Fourier transforms has made the development of pulse NMR possible. [Pg.65]

Furthermore, one may need to employ data transformation. For example, sometimes it might be a good idea to use the logarithms of variables instead of the variables themselves. Alternatively, one may take the square roots, or, in contrast, raise variables to the nth power. However, genuine data transformation techniques involve far more sophisticated algorithms. As examples, we shall later consider Fast Fourier Transform (FFT), Wavelet Transform and Singular Value Decomposition (SVD). [Pg.206]

An added consideration is that the TOF instruments are easily and quickly calibrated. As the mass range increases again (m/z 5,000-50,000), magnetic-sector instruments (with added electric sector) and ion cyclotron resonance instruments are very effective, but their prices tend to match the increases in resolving powers. At the top end of these ranges, masses of several million have been analyzed by using Fourier-transform ion cyclotron resonance (FTICR) instruments, but such measurements tend to be isolated rather than targets that can be achieved in everyday use. [Pg.281]

This process is continued until there is only one component. For this reason, the number N is taken as a power of 2. The vector [yj] is filled with zeroes, if need be, to make N = 2 for some p. For the computer program, see Ref. 26. The standard Fourier transform takes N operations to calculation, whereas the fast Fourier transform takes only N log2 N. For large N, the difference is significant at N = 100 it is a factor of 15, but for N = 1000 it is a factor of 100. [Pg.482]

It is a well known fact, called the Wiener-Khintchine Theorem [gardi85], that the correlation function and power spectrum are Fourier Transforms of one another ... [Pg.305]

One of the most common ways of characterizing complexity is by taking Fourier transforms. The spatial power spectrum of a time series of [Pg.394]

Much of the regularity in classical systems can often be best discerned directly by observing their spatial power spectra (see section 6.3). We recall that in the simplest cases, the spectra consist of few isolated discrete peaks in more complex chaotic evolutions, we might get white noise patterns (such as for elementary additive rules). A discrete fourier transform (/ ) of a typical quantum state is defined in the most straightforward manner ... [Pg.418]

The framework we adopted for measuring the scaling behavior from AFM images is the following. The 2-D power spectral density (PSD) of the Fast Fourier Transform of the topography h(x, y) is estimated [541, then averaged over the azimuthal angle

[Pg.413]

In other words, the output power is the area under the product of the Fourier transform of Rx(r) and the squared modulus of the system function H(f). [Pg.183]

Equation (3-317) shows that the power density spectrum of X(t) is related in a very simple way to the Fourier transform of the individual pulses making up the shot noise process. [Pg.186]

It is often useful to deal with the statistics in Fourier space. The Fourier transform of the correlation is called the power spectrum... [Pg.4]

This is the autocorrelation and by the Wiener-Khintchine theorem the power spectrum of the disturbance is given by its Fourier transform,... [Pg.14]

Fourier transform infrared (FTIR) spectroscopy is a powerful analytical tool for characterizing and identifying organic molecules. The IR spectrum of an organic compound serves... [Pg.150]

At the end of the 2D experiment, we will have acquired a set of N FIDs composed of quadrature data points, with N /2 points from channel A and points from channel B, acquired with sequential (alternate) sampling. How the data are processed is critical for a successful outcome. The data processing involves (a) dc (direct current) correction (performed automatically by the instrument software), (b) apodization (window multiplication) of the <2 time-domain data, (c) Fourier transformation and phase correction, (d) window multiplication of the t domain data and phase correction (unless it is a magnitude or a power-mode spectrum, in which case phase correction is not required), (e) complex Fourier transformation in Fu (f) coaddition of real and imaginary data (if phase-sensitive representation is required) to give a magnitude (M) or a power-mode (P) spectrum. Additional steps may be tilting, symmetrization, and calculation of projections. A schematic representation of the steps involved is presented in Fig. 3.5. [Pg.163]


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See also in sourсe #XX -- [ Pg.78 ]




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