In particular, we give lower bounds on (rho+partial_{1}), (rho-partial_{n}), (rho+partial_{1}^{L}), (partial_{1}^{L}-rho), (2rho+partial _{1}^{Q}) and (partial_{1}^{Q}-2rho) and the corresponding extremal graphs are characterized.
Meanwhile, models that are equally well represented by both grid and spur graphs are characterized by |K j | = |K d |, which, in Fig. 3, is all of the graphs except I, J, M, N, R and S.
The between-class similarity graph is characterized by Wb,ij = S b (i, j).
In this model, nodes of the graph are characterized by Gabor jets, that is, Gabor wavelet responses at several scales and orientations, all stacked as a vector.
The graph is characterized by a weighted adjacency matrix W = [wkl], k,l = 1.p, and the diagonal degree matrix D with degrees d1 to dp as diagonal elements.
The rPIN network graph is characterized by a relatively short characteristic length (CL) of 3.49 ± 0.01.
The graph of Figure 4 revealed that nanocrystal samples producing similar in vivo effects were characterized by the same zeta potential-pH dependence profile.
Wound tissues were characterized using different algorithms, namely, histogram thresholding, mean shift smoothing, region growing, and graphs [ 10, 11].
Several other important families of graphs may be defined from other values of k and l, and when l ≤ k the (k,l -sparse graphs may be characterized as the graphs formed as the edge-disjoint union of l forests and k − l pseudoforests.
