Graph Spectral Image Processing. Gene Cheung
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[1.50]
where ||·||0 represents the number of non-zero elements, i.e.
[1.51]
With the GFT basis U, it is equivalently represented as
[1.52]
where × represents some possible non-zero elements and
[1.53]
A partial eigendecomposition proposed in literature gives the following approximation of L:
[1.54]
Evaluating only requires K (< N) eigenvectors and eigenvalues, which is significantly less than that obtained using the full eigendecomposition. In general, its computational complexity will be
1.6.5. Polynomial approximation
The previous subsection proposes that we can alleviate the heavy computational burden by assuming the bandlimitedness of the graph signal. However, this requires the assumption on the signal model prior to filtering, but the signal is not bandlimited in general.
In many application scenarios, we often only need the evaluation of x with a given (linear) matrix function h(L). That is, the eigenvalues and eigenvectors themselves are often unnecessary. The polynomial approximation methods introduced here enable us to calculate an approximation of y = h(L)x without the (partial) decomposition of the variation operator.
Another advantage of filtering using a polynomial filter function is the vertex localization. The local filtering could capture local variations of pixel values, which are generally preferable. In contrast, filtering in the graph frequency domain (equation [1.13]) is usually not localized in the vertex domain, because eigenvectors often have global support on the graph. Therefore, localizing graph filter response, both in the vertex and graph frequency domains, has been studied extensively (Shuman et al. 2013; Shuman et al. 2016b; Sakiyama et al. 2016). In fact, the localization of graph spectral filters can be controlled using polynomial filtering.
Polynomial graph filters are defined as follows:
[1.55]
where ck is the kth order coefficient of the polynomial. It is known that each row of Lk collects its k-hop neighborhood; therefore, equation [1.55] is exactly the K-hop localized in the vertex domain. Note that Lk can be represented as
[1.56]
Here, we utilized the orthogonality of U. We can rewrite equation [1.55] by using equation [1.56] as:
[1.57]
Consequently, the polynomial graph filter has the following graph frequency response:
[1.58]
Especially, the output signal in the vertex domain is given by
[1.59]
This indicates that we do not need to compute specific eigenvalues and eigenvectors for just calculating y. Specifically, we need to evaluate Lx, L2x,..., LKx. Calculating Lz, where z is an arbitrary vector, requires
Suppose that a fast computation is required for the spectral response of a graph filter
Any polynomial approximation methods, e.g. Taylor expansion, are possible for the above-mentioned polynomial filtering. In GSP, Chebyshev polynomial approximation is implemented frequently. The Chebyshev expansion gives an approximate minimax polynomial, i.e. the maximum approximation error can be reduced.
The approximated version of h(L)x by the Kth order shifted Chebyshev polynomial, hCheb(L)x, is given by Shuman et al. (2013); Hammond et al. (2011)
[1.60]
and it has the recurrence property:
[1.61]
with
[1.62]