href="#ulink_6b868a97-803a-531a-ac80-261746a3c357">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]
for k = 0,...,K, where P is the number of sampling points used to compute the Chebyshev coefficients and is usually set to P = K + 1. The approximated filter in equation [1.60] is clearly a Kth order polynomial of λ. As a result, it is K-hop localized in the vertex domain, as previously mentioned (Shuman et al. 2011; Hammond et al. 2011).
The approximation error for the Chebyshev polynomial has been well studied in the context of numerical computation (Vetterli et al. 2014; Phillips 2003):
THEOREM 1.1.– Let K be the polynomial degree of the Chebyshev polynomial and assume that
[1.63]
1.6.6. Krylov subspace method
The Krylov subspace
[1.64]
The Krylov subspace method, in terms of GSP, refers to filtering, i.e. evaluating an arbitrary filtered response h(W)x, realized in a Krylov subspace
[1.65]
where h(HK) is evaluating h(·) for the upper Heisenberg matrix HK, which is obtained by using the Arnoldi process. Furthermore, HK is expected to be much smaller than the original matrix; therefore, evaluating h(HK) using full eigendecomposition will be feasible and light-weighted.
1.7. Conclusion
This chapter introduces the filtering of graph signals performed in the graph frequency domain. This is a key ingredient of graph spectral image processing presented in the following chapters. The design methods of efficient and fast graph filters and filter banks, along with fast GFT (such attempts can be found in Girault et al. (2018); Lu and Ortega (2019)), are still a vibrant area of GSP: the chosen graph filters directly affect the quality of processed images. This chapter only provided a brief overview of graph spectral filtering. Please refer to the references for more details.