Q2. What can be done to estimate the geometrical structure of an image?
The shift and rotation invariance properties of the CWT can also be harnessed to compute accurate and efficient estimates of the geometrical structure in images, namely the strength, orientation, and offset of image edges, ridges, and other singularities.
Q3. What is the property of a truly shift invariant transform?
A truly shift invariant transform has the property that the signal path through any single subband of the transform and its inverse may be characterized by a unique z transfer function, which is unaffected by the down and up sampling within the transform.
Q4. What is the use of finite support for wavelet-based signal processing?
Finite support is extremely useful for wavelet-based signal processing, since it limits the extent to which a signal feature can affect the wavelet coefficients.
Q5. How many complex wavelets can be formed by using the real parts?
a set of six complex wavelet can be formed by using wavelets (43)–(44) as the real parts and wavelets (49)–(50) as the imaginary parts.
Q6. What is the perfect reconstruction condition for the analysis and synthesis FBs?
For the analysis and synthesis FBs to represent a forward and inverse wavelet transform, it is necessary that the perfect reconstruction (PR) condition be satisfied: y(n) = x(n), or more generally y(n) = x(n − no).
Q7. How can the displacement between two images be estimated?
Local displacement (motion) between two images can be estimated from the change of phase of CWT coefficients from one image to the next.
Q8. What is the advantage of the oriented complex 2-D dual-tree wavelet transform?
The oriented complex 2-D dual-tree wavelet transform is four-times expansive, but it has the benefit of being both oriented and approximately analytic.
Q9. Why are the filters for the dual-tree CWT generally longer than real?
It should be noted however, that filters for the dual-tree CWT are generally somewhat longer than filters for real wavelet transforms with similar numbers of vanishing moments, because of the additional constraints (10)–(11) that the filters must approximately satisfy.
Q10. What is the oriented complex 2-D dual-tree wavelet transform?
Note that the oriented 2-D dual-tree CWT (applied to real or complex data) requires four separable wavelet transforms in parallel, and so it is no longer strictly a dual-tree wavelet transform.
Q11. What are the main shortcomings of the wavelet transform?
In spite of its efficient computational algorithm and sparse representation, the wavelet transform suffers from four fundamental, intertwined shortcomings.
Q12. What is the way to illustrate the near shift invariance of the CWT?
One way to illustrate the near shift invariance of the dual-tree CWT is to observe how the projection of a signal onto a certain scale varies as the signal translates.
Q13. Why is the 2-D wavelet transform less efficient for line-and-curve-s?
The reason for this is that while the separable 2-D wavelet transform represents point-singularities efficiently, it is less efficient for line-and curve-singularities (edges).
Q14. What is the oriented real 2-D dual-tree wavelet transform?
Like the 1-D dual-tree CWT, the oriented real 2-D dual-tree wavelet transform is still a dual-tree wavelet transform and is also two-times expansive.
Q15. What is the inverse of the oriented real 2-D dual-tree wavelet transform?
If the two real separable 2-D wavelet transforms are orthonormal transforms, then the transpose of Fhh is its inverse: Fthh · Fhh = I, and similarly Ftgg · Fgg = I.
Q16. How can the authors reduce the width of the bump?
It is possible to reduce the width of the bump by designing H1(z) and Hn(z) so that they have narrower transitions bands, how-[FIG4]
Q17. How can the authors design a pair of filters of equal length?
By jointly designing h0(n) and g0(n), the authors can obtain a pair of filters of equal (or near-equal) length, where both are relatively short.
Q18. What is the spectrum of the complex wavelet h(t) + j?
The spectrum of the complex wavelet ψh(t) + jψg(t) is shown in the figure, and it is clearly nearly analytic (approximately zero on the negative frequency axis).