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Wavelet space

Fig. 1. Contour maps for the original ART-P image of the Galactic center field (smoothed with the instrument PSF) and those computed in wavelet space using different vcJues of the wavelet scale, a = 2.5 5 and 10. The contours are shown at the levels of 3, 4, 5, 6, 8, 10,. .. standard deviations. Fig. 1. Contour maps for the original ART-P image of the Galactic center field (smoothed with the instrument PSF) and those computed in wavelet space using different vcJues of the wavelet scale, a = 2.5 5 and 10. The contours are shown at the levels of 3, 4, 5, 6, 8, 10,. .. standard deviations.
Like the FT, the WT converts a signal from its normal time- or property-domain representation into another representation— in wavelet space—which reveals the frequency content of the original signal. A wavelet space representation not only separates frequency components, but unlike the FT, also gives their exact position and identifies their effective domain. It allows WT methods to separate, isolate, and analyze the individual components of a signal. The FTs and WTs are useful when analyzing many different types of chemistry... [Pg.296]

The CWT is compactly described by Eqs. [4] and [6], but this definition allows for infinitely redundant transformations.There is no limit to the number of dilated and translated wavelets (4 (a ), where a and b are real numbers) used in the transform. This unrestricted and unguided use of wavelets to convert a signal into wavelet space often prevents the use of an inverse wavelet transformation because of violations of the conditions required by Eq. [7]. Even though these transforms are redundant and nonreversible, they still reveal information about the character of a particular signal. [Pg.302]

The framework, however, as introduced so far is of little help for our purpose since the shift from any subspace to its immediate in hierarchy would require to change entirely the set of basis functions. Although j x) are all created by the same function, they are different functions and, consequently, the approximation problem has to be solved from scratch with any change of subspace. The theory of wavelets and its relation to multiresolution analysis provides the ladder that allows the transition from one space to the other. [Pg.184]

As approximation schemes, wavelets trivially satisfy the Assumptions 1 and 2 of our framework. Both the Lf and the L°° error of approximation is decreased as we move to higher index spaces. More specifically, recent work (Kon and Raphael, 1993) has proved that the wavelet transform converges uniformly according to the formula... [Pg.185]

The space-frequency localization of wavelets has lead other researchers as well (Pati, 1992 Zhang and Benveniste, 1992) in considering their use in a NN scheme. In their schemes, however, the determination of the network involves the solution of complicated optimization problem where not only the coefficients but also the wavelet scales and positions in the input space are unknown. Such an approach evidently defies the on-line character of the learning problem and renders any structural adaptation procedure impractical. In that case, those networks suffer from all the deficiencies of NNs for which the network structure is a static decision. [Pg.186]

Fig, y. Resolution in scale space of (a) window Fourier transform and (b) wavelet transform. [Pg.231]

In Section II we defined the trend of a measured variable as a strictly ordered sequence of scaling episodes. Since each scaling episode is defined by its bounding inflexion points, it is clear that the extraction of trends necessitates the localization of inflexion points of the measured variable at various scales of the scale-space image. Finally, the interval tree of scale (see Section II) indicates that there is a finite number of distinct sequences of inflexion points, implying a finite number of distinct trends. The question that we will try to answer in this section is, How can you use the wavelet-based decomposition of signals in order to identify the distinct sequences of inflexion points and thus of the signal s trends ... [Pg.237]

The wavelet interval-tree of scale is constructed fi om log 2 N distinct representations, where N is the number of points in the record of measured data. This is a far more efficient representation than that of scale-space filtering with continuous variation of Gaussian a. [Pg.242]

Compression may be achieved if some regions of the time-frequency space in which the data are decomposed do not contain much information. The square of each wavelet coefficient is proportional to the least-squares error of approximation incurred by neglecting that coefficient in the reconstruction ... [Pg.249]

C. Space-Scale Analysis Based on Continuous Wavelet Transform Low-Frequency Rhythms in Human DNA Sequences... [Pg.203]

The continuous wavelet transform (WT) is a space-scale analysis that consists in expanding signals in terms of wavelets that are constructed from a single function, the analyzing wavelet /, by means of dilations and translations [13, 27-29]. When using the successive derivatives of the Gaussian function as analyzing wavelets, namely... [Pg.209]

Until now, the most sensible basic interacting quantum device known to us is the photon. Nevertheless, if the photon possesses an inner structure, as assumed in de Broglie s model, it would imply measurements beyond the photon limit. Since it was assumed that the quantum systems are to be described by local finite wavelets in the derivation of the new uncertainty relations, the measurement space resulting from those general relations must depend on the size of the basic wavelet used. As the width of the analyzing wavelet changes, the measurement scale also changes. This can be seen in the plot in Fig. 20. [Pg.540]

From Fig. 20 one sees that as the width of the basic wavelet Ax0 changes, all the measurement-accessible space is browsed. This space is limited only by Heisenberg s space. The smaller is Axo, the greater is the precision of the measurement of the position, that is, the smaller is the uncertainty Ax, for any value of the error in the momentum. Given that the new relation contains the usual as a particular case, it implies that the measurement space available to the... [Pg.540]

The product of these uncertainties in momentum and in position, lies in the case of the common Fourier microscopes in the Heisenberg uncertainty measurement space, while for the superresolution optical microscope, the same product lies in the more general wavelet uncertainty measurement space. [Pg.554]


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See also in sourсe #XX -- [ Pg.296 , Pg.302 , Pg.303 , Pg.318 ]




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Continuous wavelet transform space-scale analysis

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