Skip to main content
Advertisement
Browse Subject Areas
?

Click through the PLOS taxonomy to find articles in your field.

For more information about PLOS Subject Areas, click here.

  • Loading metrics

Investigating stronger tolerant network against cascading failures in focusing on changing degree distributions

  • Ryota Kusunoki ,

    Contributed equally to this work with: Ryota Kusunoki, Yukio Hayashi

    Roles Investigation, Methodology, Visualization, Writing – original draft, Writing – review & editing

    ryotakusunoki@hotmail.com

    Affiliation Graduate School of Advanced Science and Technology, Japan Advanced Institute of Science and Technology, Nomi, Ishikawa, Japan

  • Yukio Hayashi

    Contributed equally to this work with: Ryota Kusunoki, Yukio Hayashi

    Roles Conceptualization, Funding acquisition, Investigation, Methodology, Supervision, Writing – review & editing

    Affiliation Graduate School of Advanced Science and Technology, Japan Advanced Institute of Science and Technology, Nomi, Ishikawa, Japan

Abstract

Many real-world networks with Scale-Free structure are significantly vulnerable against both intentional attacks and catastrophic cascading failures. On the other hand, it has been shown that networks with narrower degree distributions have strong robustness of connectivity by enhancing loops. This paper numerically reveals that such networks are also tolerant against cascading failures. Our findings will be useful in designing stronger tolerant network infrastructures.

Introduction

In the early 20th century, Erdős–Rényi (ER) random graphs with homogeneous Poisson degree distributions were widely studied with mathematical interests [1, 2]. After decades, through the progress of techniques for large data analysis, it has been found that Scale-Free (SF) structure with significantly heterogeneous power-low degree distribution exists in many real-world networks such as electric power-grid, actor collaborations, neuronal network [3, 4]. Unfortunately, SF networks are extremely vulnerable against intentional attacks to large degree nodes [5]. On the other hand, by the analysis of generating function and numerical simulations, it has been also revealed that, under a given degree distribution, onion-like structure has the optimal robustness of connectivity when degree-degree correlations increase moderately [6, 7]. However, the robustness of connectivity is decreased for too large positive correlations. Thus, degree-degree correlations may be not essential for improving the robustness.

Recently, it has been suggested that loops are more important than degree-degree correlations for the robustness of connectivity against attacks [8, 9]. Bacause the importance of loops is theoretically supported by the asymptotic equivalence of the dismantling and recycling problems [9], when the second moment of degree is not divergent. Roughly speaking, the worst case attacks for fragmentation is to be loopless. Conversely, the robustness becomes higher as the size of necessary nodes to form loops is larger, although even only measuring of the size is NP-hard in computer science. Actually, by enhancing loops, several rewirings without preserving degrees have been proposed to improve the robustness of connectivity [10]. In particular, even for different rewiring methods, the decreasing the gap between the maximum and the minimum degrees has been found commonly. Thus, narrower degree distribution leads to increase the robustness of connectivity.

As a related study to change degree distributions, growing network (GN) model [11] generates networks with continuously changing degree distributions between power-law and exponential ones, although the robustness of connectivity is not discussed. Moreover, inverse preferential attachment (IPA) model has been recently introduced [12], and generates networks with narrower degree distribution than exponential one. Instead of the gap between the maximum and the minimum degrees, the narrowness can be measured and compared by the variance σ2 = Σk(k− < k >)2P(k) for any degree distribution P(k) with average degree < k > = ΣkkP(k). In particular, it has shown that the robustness of connectivity against attacks increases more as narrower degree distribution [10]. It is also suggested that, the extreme case of the narrowest degree distribution whose width is zero, random regular graphs are the optimal for the robustness [13]. Note that randomization is necessary to investigate the pure effect of the degree distribution, since the IPA model has a chain-like structure [12]. As examples in real networks, exponential and narrower degree distributions appears in growing social networks in which new-comers connect to randomly chosen nodes with encountering and road networks with T-junctions and crossroads, respectively.

On the other hand, even if a network is connected, the malfunction as overload may be occurred through redistribution of flows triggered by the removal of one or a few nodes. Where the flows are corresponded to moving vehicles on road or transferring packets in communication, and the overload means that the node exceeds its capacity. This is called cascading failures and represents a phenomenon of chain reaction to widespread malfunctions in many network systems. Even when links remain intactly, some load exceeded from the capacity for processing or flow passage at nodes results in the loss of connectivity potentially causing severe damage. Excluding their minor differences, this mechanism becomes common for such as power grid collapses, communication congestions, and cascading bankruptcies in infrastructures that widely sustain our contemporary society. Therefore, the problem of cascading failures is very serious. So far cascading failures and defense strategies have been discussed for classical ER random graphs and realistic SF networks, however they are pin-point researches for only Poisson and power-low degree distributions. Note that SF network is significantly vulnerable against cascading failures triggered by intentional attacks [14], and that ER random graph is relatively tolerant compared to SF network [15]. While several defense strategies have been proposed as sacrificial node removal [16], reconnection of links [17], and improving of routing based on degree and load [18], these defense strategies are impractical. Because nodes and links are wasted on the assumption that the network structure can be changed immediately. Furthermore, in recent years, cascading failures have been extendedly studied on interdependent networks, whose infrastructure consists of power-grid, communication, and social networks [1921]. However, even on a single layered network, the stronger tolerant structure is unknown against cascading failures.

Therefore, away from the pin-points of the Poison and power-low degree distributions, we investigate more tolerant topological structures against cascading failures. We focus on changing degree distribution, since a narrower degree distribution leads to enhancing many loops. Therefore, the tolerance against cascading failures is expected because of distributed flows via many bypass routes on loops. Through numerical simulations, we reveal that networks with narrower degree distributions are also higher tolerant against cascading failures.

Continuously changing degree distributions

We consider preferential attachment (PA) [3] and IPA [12] in growing networks. It is well-known that Barabási-Albert (BA) model [3] generates a heterogeneous SF network by PA, whose attachment probability is proportional to degree ki of existing node i. Here, the attachments make m links from a new node to existing nodes in a network at each time step. While in IPA model, the probability is proportional to kβ, β ≥ 0 [12], the generation process is summarized as follows.

  1. Step 1. Start with a complete graph of 2m = 4 nodes as initial configuration.
  2. Step 2. At each time step, a new node is added and attached to existing nodes with m = 2 links.
  3. Step 3. Repeat Steps 1, and 2 until the the network size reaches N.

By IPA model as larger β, network efficiency described in the next subsection is significantly decreased, because a special chain-like structure emerges [12, 22]. Therefore, configuration model [23] is applied as randomization in order to eliminate such a chain-like structure and to investigate the pure effect of degree distributions.

Fig 1 shows the degree distributions in heterogenous SF (dashed black line), homogeneous ER random graphs (dash-dot black line), and more homogeneous (colored lines) networks. The corresponding degree distributions are power-low, Poisson, and narrower ones, respectively. Note that the dashed black line for SF network is straight in log-log plot. As β increases, the maximum degree generated by IPA is decreasing. In particular, networks for β = 50 (orange), and 100 (red) are very homogeneous with narrower degree distributions. The Poisson distribution [1] in ER random graph (dash-dot black line) is similar to that for the case of β = 1 in IPA (light blue line). Note that the case of β = 0 by IPA (blue) is an exponential degree distribution generated by random attachment.

thumbnail
Fig 1. Degree distributions for the network size N = 103 and the total number of links M = 2000.

The dash-doted black line represents a Poisson degree distribution for the network generated by ER random graph, and the dashed black line represents a power-low degree distribution for the network generated by PA. Colored lines represent the narrower degree distributions for networks generated by IPA with different value of β denoted from blue to red.

https://doi.org/10.1371/journal.pone.0297094.g001

In general, cascading failures can be suppressed with many bypass routes in the network. In contrast, the existence of bypass routes is measured by the distribution of link betweenness centrality (BC) [24]. If there are the shortest paths between any nodes as bypass routes, the width of BC distribution becomes narrow. Here, the value of link BC is defined by the ratio of the number of shortest paths through link (i, j) to the total number of shortest paths between source and destination nodes s, di, j. Fig 2 shows the distributions of link BC in heterogeneous SF networks generated by PA (BA model) (dashed black line), homogeneous ER random graphs (dash-dot black line), and more homogeneous networks generated by IPA (colored lines). As changing from SF by PA (dashed black line) to the case of β = 100 by IPA (red line), many links tend to have similar values of link BC with the smaller variance of link BC distribution. In other words, it is suggested that more bypass routes exist in networks with the narrower degree distribution generated by IPA.

thumbnail
Fig 2. Distributions of link betweenness centralities.

The other parameters and the networks represented by lines are the same as in Fig 1.

https://doi.org/10.1371/journal.pone.0297094.g002

It has been shown that, in a modification of IPA model, small amount of random attachment is necessary for the emergence of the average path length 〈Lij〉 ∼ O(log N) as Small-World (SW) property [25] to eliminate chain-like structure for large β. Instead of random attachment, we apply randomization by configuration model [23] to investigate a pure effect of degree distribution. Fig 3 shows the average shortest path length in randomized networks without chain-like structure [12]. In the left of Fig 3, all lines are straights of O(log N) in a semi-log plot as the SW property [25]. However, without the randomization in the right side of Fig 3, the shortest path length increases exponentially as β increases because of the emergence of chain-like structure [12]. Thus, it is expected that networks with narrower degree distributions have both high tolerance and network efficiency against cascading failures as shown later, since the shortest path length is comparable to that in SF networks. The definition of tolerance and network efficiency against cascading failures are explained in the next section.

thumbnail
Fig 3. Average shortest path lengths 〈Lij〉 for the network size N = 104.

(Left) randomized by configuration model, (Right) networks generated by only IPA. The other parameters and the network represented by lines are the same as in Fig 1.

https://doi.org/10.1371/journal.pone.0297094.g003

Cascading failures

We explain a typical procedure of cascading failures [14]. The load Li(t) is defined by node betweenness [26] on the assumption that flows are transmitted along the shortest paths between source s and destination d nodes at where the unit quantity of transmission request is generated in each pair of nodes. (1) where gsd is the total number of shortest paths from s and d nodes, gsd(i) is the number of those paths passing through node i at time step t ≥ 0. Node betweenness means the load as the ratio of flows passing through node i at t and is effectively calculated by Brandes algorithm [27]. Eq (1) implies that the flow is equally distributed to multiple shortest paths with a same length. We remark that link BC is not used to define the load at a node but applied to measure the amount of bypass routes. At each time step t ≥ 1, gsd(i) and gsd are changeable after node removals.

The capacity Ci is defined as proportional to the initial load Li(0). (2) where α > 0 is a tolerance parameter, and Li(0) denotes the initial load at node i in the network at time step t = 0. When Li > Ci: the load Li exceeds the capacity, node i is removed from the network as a malfunction. After such node removals, Eq (1) is recalculated for tt + 1 from t = 0. In other words, the load is redistributed to the remaining nodes after re-routing on the shortest paths. Then, nodes with Lj > Cj are further removed from the network. Such process is repeated until Lk < Ck is satisfied for remaining all nodes.

We consider the following three typical methods [14] and spatial damage methods [28] as triggers of cascading failures, since the damage of cascading failures depends on the types of triggers.

  • Intentional attacks: Max-degree, Max-load attacks [14]
  • Unexpected failures: Random attacks [14]
  • Spatial damages: Localized attacks [28]

Max-degree and max-load attacks choose the nodes with the maximum degrees and loads in all nodes, while random attacks choose nodes uniformly at random as unexpected failures, respectively. As spatial damage by earthquakes or tsunamis [28], localized attacks remove connected nodes based on their hop-distances from a root node. The root node is chosen by three types of triggers: random, max-degree, and max-load attacks, respectively. We set the number of initially removed nodes as AN = N × p, where p is the rate of node removals.

The damage of cascading failures is quantified by the relative size G of the largest connected component (LCC) before and after cascading failures. (3) where N′ is the the network size in the LCC after cascading failures. Furthermore, network efficiency is introduced to measure the efficiency of paths [29]. The average efficiency is defined as, (4) where the efficiency eij between nodes i and j is inversely proportional to the distance dij of the shortest path length eij = 1/dij. For example, dij is calculated by Dijkstra [30] or the preprocessing of Brandes algorithm [27]. If there is no path between the nodes i and j, we set dij = ∞ and eij = 0. Note that the efficiency is defined as the inverse of the harmonic mean, while the average path length is as the arithmetic mean.

We summarise the above process of cascading failures.

  1. Calculate the load Li on each node i by Eq (1).
  2. Remove trigger nodes chosen by random, Max-degree, or Max-load node removals.
  3. Recalculate the load Li on each node i after re-routing.
  4. When Li > Ci, the nodes whose load exceeds their capacity are removed from the network.
  5. Repeat Steps 3, 4 until all nodes are removed or there are no overloaded nodes.

Remember that, after removing either AN = 1 or 50 nodes as triggers, the flows between s and t are equally distributed to the multiple shortest paths with a same length by Eq (1) in the determinant choosing. Therefore, stochastic choosing from the multiple shortest paths is beyond our scope of this study.

Results

As a degree distribution becomes narrow, the network becomes more robust in enhancing loops [10]. Thus, it is expected that many loops potentially lead to increased the tolerance against cascading failures because of distributed flows via many bypass routes on multiple loops. In this section, we will provide a numerical validation of the tolerance against cascade failures. Cascading failures are simulated for the heterogeneous SF networks generated by PA, homogeneous ER random graphs, and the more homogeneous networks generated by IPA for finding more tolerant network structure in changing degree distributions. Remember that the corresponding degree distributions are power-low, Poison, and narrower ones. In order to investigate the pure effect of the degree distributions, networks generated by IPA are rewired at random by configuration model. We set the network size N = 1000, the total number of links M = 2000, β = 0, 1, 5, 10, 20, 50, 100 in IPA, tolerance parameter α = 0, 0.1, 0.2, 0.3, 0.4, 0.5, 0.6, 0.7, 0.8, 0.9, 1.0, and number of removal nodes AN = 1, 50, or 100. The following results are averaged over 100 realizations of randomly generated networks. Note that the results for max-degree and max-load attacks are similar, because the node with the max-degree tends to have the max-load. These similar results are not shown but are presented in supporting information.

Fig 4 shows the relative sizes G after cascading failures. The dash-dotted black line, dashed black line, and colored lines represent the relative sizes G for ER random graph, SF network, and the more homogeneous networks randomized by configuration model after IPA in order to investigate the pure effects of degree distributions. The colored lines represent the relative sizes G for network by configuration model after IPA for different values of β denoted from blue to red in continuously changing degree distributions.

thumbnail
Fig 4. Relative size G for networks with N = 1000 and m = 2 by configuration model.

(Top) random attacks, (Center) max-degree attacks, (Bottom) localized random attacks. (Left) number of initial node removal is AN = 1, (Right) number of initial node removals is AN = 50.

https://doi.org/10.1371/journal.pone.0297094.g004

In Fig 4(a) the relative size G of the network (colored lines) randomized by configuration model after IPA is more highly tolerant than that of SF network (dashed black line) against max-degree attacks for both AN = 1 (a) and 50 (b). The case of larger β from blue to green, yellow, and red suppresses the damage of cascading failures for AN = 50 (b) even with a small value of tolerance parameter. This indicates that the tolerance against cascading failures increases by distributing the load among nodes on the multiple shortest paths, because of many loops between any nodes as the degree distribution becomes narrower.

Against the localized random attacks as shown in Fig 4(d), SF network (dashed black line) has a smaller relative size G than that against random attacks as shown in Fig 4(f) for AN = 50. However, as larger β, the relative size G is larger in the networks (colored lines) by configuration model after IPA. SF network is vulnerable with a high probability that attacked nodes include hubs due to the short path lengths and heterogeneous degree distribution. On the other hand, path lengths between any nodes are short but no hubs exist, if the degree distribution is sufficiently narrow. Therefore, the networks have a higher tolerance against cascading failures. Note that only the root node is removed by localized random attacks for AN = 1, the relative size G is the same as that by random attacks.

On the other hand, in Fig 4(e), the relative size G is almost 1.0, when the number of initial random attacks is AN = 1. It means that there is no major damage against cascading failures except for the case of small α < 0.1. While for AN = 50 in Fig 4(f), SF network (dashed black line) is more tolerant than other networks against cascading failures, as similar to the high robustness of connectivity from the SF network against random attacks [5]. In other words, it is considered that the damage of cascade failures are suppressed as maintaining of connectivity after initial attacks. Furthermore, the relative size G of networks randomized by configuration model after IPA is larger for α ≧ 0.4 than that of SFs network. Note that the relative size G of ER random graph (dash-dot black line) is close to that of the network by configuration model after IPA with β = 1 (light blue line).

Fig 5 shows the network efficiency after a cascading failure by random and localized random attacks for AN = 50. On the right of Fig 5, SF network (dashed black line) is significantly inefficient against localized random attacks, while it is the most efficient against random attacks. However, against random attacks, the efficiency of the SF network is slightly higher than the network randomized after generated by IPA. In these networks with long-tailed and narrower degree distributions, the difference of network efficiency is at most approximately 0.05 on the left of Fig 5. Therefore, more homogeneous networks are not only higher tolerant against cascading failures, but also become efficient for path lengths.

thumbnail
Fig 5. Network efficiency E in networks for N = 1000, m = 2, and AN = 50 by configuration model.

(Left) Random attacks, (Right) Localized random attacks.

https://doi.org/10.1371/journal.pone.0297094.g005

Fig 6 illustrates the network efficiency E before and after cascading failures triggered by localized random, max-degree, and max-load node removals in randomized networks after generations by PA and IPA in changing degree distribution. Before cascading failures (blue line), SF network is the most efficient, while networks by IPA converge to approximately E = 0.195 around β = 10. However, after cascading failures triggered by localized-random node removal (magenta line), the efficiency of SF networks significantly decreases. In contrast, networks by IPA show only a slight reduction in efficiency across any β values. Furthermore, after cascading failures triggered by max-degree and max-load removals (green and dashed red lines), the efficiency shows a remarkable similarity of maintaining a consistent level at approximately E = 0.190 when β ≥ 5. Overall, the homogeneous networks generated by IPA present a decrease in efficiency at most approximately 30%, compared to SF networks before cascading failures which is the most efficient. In addition, at β = 100 when the network achieves sufficient homogeneity, the difference of efficiency between before and after cascading failures is very small.

thumbnail
Fig 6. Network efficiency E before and after cascading failures by localized random, max-degree and max-load nodes removal for N = 1000, m = 2, and AN = 50.

https://doi.org/10.1371/journal.pone.0297094.g006

Conclusion

In this study, we explored the relation between network topology characterized by degree distribution and the tolerance against cascading failures. We consider the cascading failures from various triggers, such as intentional attacks, random failures, and spatial damages. Our results show that narrower degree distributions absorb their cascading failures. Specifically:

  1. The tolerance against cascading failures is significantly improved as the degree distribution narrows. Because flows are distributed to bypass routes in the networks, it mitigates the risk of cascading failures effectively.
  2. In contrast, networks with narrower degree distributions not only have in tolerance cascading failures but also manifested efficiency for their path lengths. SF network is most efficient before cascading failures, but the efficiency is reduced at most approximately 30%. It is also worth to note that the difference between before and after cascading failures by any node removals is negligible for sufficiently homogeneous networks by IPA for β > 10.
  3. While SF network characterized by a power-law degree distribution has tolerance against random attacks, it displayed vulnerability against max-degree and localized random attacks due to the concentration of load at hubs.

This study revealed a tolerant network structure against cascading failures. Such insights will be useful in designing more tolerant infrastructure against natural disasters or damages by intentional conflicts. The reduction of efficiency after cascading failures is the minimum, therefore the networks can be expected to recover rapidly even in cases of malfunction. Further discussions for vulnerabilities and strengths against cascading failures are remaining in other networks with different degree distributions from ours generated by PA or IPA models. Notably, a recent perturbation analysis suggested that the most robust network structure is exhibited by random regular graphs with 0 variance of degree distritubion [13]. Exploring the relationship between efficiency and other network characteristics, such as the clustering coefficient, remains future works.

Supporting information

S1 Fig. Relative size G and network efficiency E against random attacks in randomized networks for N = 1000 and m = 2 by configuration model.

https://doi.org/10.1371/journal.pone.0297094.s001

(EPS)

S2 Fig. Relative size G and network efficiency E against max-degree degree attacks in randomized networks for N = 1000 and m = 2 by configuration model.

https://doi.org/10.1371/journal.pone.0297094.s002

(EPS)

S3 Fig. Relative size G and network efficiency E against max-load degree attacks in randomized networks for N = 1000 and m = 2 by configuration model.

https://doi.org/10.1371/journal.pone.0297094.s003

(EPS)

S4 Fig. Relative size G and network efficiency E against localized random attacks in randomized networks for N = 1000 and m = 2 by configuration model.

https://doi.org/10.1371/journal.pone.0297094.s004

(EPS)

S5 Fig. Relative size G and network efficiency E against localized max-degree degree attacks in randomized networks for N = 1000 and m = 2 by configuration model.

https://doi.org/10.1371/journal.pone.0297094.s005

(EPS)

S6 Fig. Relative size G and network efficiency E against localized max-load degree attacks in randomized networks for N = 1000 and m = 2 by configuration model.

https://doi.org/10.1371/journal.pone.0297094.s006

(EPS)

References

  1. 1. Erdös P. On random graphs. Mathematicae. 1959;6:290–297.
  2. 2. Erdős P, Rényi A, et al. On the evolution of random graphs. Publication of the Mathematical Institute of the Hungarian Academy of Sciences. 1960;5(1):17–60.
  3. 3. Barabási AL, Albert R. Emergence of scaling in random networks. Science. 1999;286(5439):509–512. pmid:10521342
  4. 4. Amaral LAN, Scala A, Barthelemy M, Stanley HE. Classes of small-world networks. Proceedings of National Academy of Science in USA. 2000;97(21):11149–11152. pmid:11005838
  5. 5. Albert R, Jeong H, Barabási AL. Error and attack tolerance of complex networks. Nature. 2000;406(6794):378–382. pmid:10935628
  6. 6. Tanizawa T, Havlin S, Stanley HE. Robustness of onionlike correlated networks against targeted attacks. Physical Review E. 2012;85(4):046109. pmid:22680540
  7. 7. Schneider CM, Moreira AA, Andrade JS Jr, Havlin S, Herrmann HJ. Mitigation of malicious attacks on networks. Proceedings of the National Academy of Sciences in USA. 2011;108(10):3838–3841. pmid:21368159
  8. 8. Hayashi Y, Uchiyama N. Onion-like networks are both robust and resilient. Scientific Reports. 2018;8(1):11241. pmid:30050045
  9. 9. Braunstein A, Dall’Asta L, Semerjian G, Zdeborová L. Network dismantling. Proceedings of the National Academy of Sciences in USA. 2016;113(44):12368–12373. pmid:27791075
  10. 10. Chujyo M, Hayashi Y. A loop enhancement strategy for network robustness. Applied Network Science. 2021;6(1):1–13.
  11. 11. Krapivsky PL, Redner S. Organization of growing random networks. Physical Review E. 2001;63(6):066123. pmid:11415189
  12. 12. Liao F, Hayashi Y. Emergence of robust and efficient networks in a family of attachment models. Physica A: Statistical Mechanics and its Applications. 2022;599:127427.
  13. 13. Chujyo M, Hayashi Y, Hasegawa T. Optimal Network Robustness Against Attacks in Varying Degree Distributions. arXiv. 2023;2301(06291).
  14. 14. Motter AE, Lai YC. Cascade-based attacks on complex networks. Physical Review E. 2002;66(6):065102. pmid:12513335
  15. 15. Xia Y, Fan J, Hill D. Cascading failure in Watts–Strogatz small-world networks. Physica A: Statistical Mechanics and its Applications. 2010;389(6):1281–1285.
  16. 16. Motter AE. Cascade control and defense in complex networks. Physical Review Letters. 2004;93(9):098701. pmid:15447153
  17. 17. Hayashi Y, Miyazaki T. Defence Strategies for Cascading Failures on Scale-Free Networks with Degree-degree Correlations. IPSJ Journal. 2006; p. 47 (3), pp.802–812.
  18. 18. Zhao H, Gao ZY. Cascade defense via navigation in scale free networks. The European Physical Journal B. 2007;57(1):95–101.
  19. 19. Buldyrev SV, Parshani R, Paul G, Stanley HE, Havlin S. Catastrophic cascade of failures in interdependent networks. Nature. 2010;464(7291):1025–1028. pmid:20393559
  20. 20. Cheng Z, Cao J. Cascade of failures in interdependent networks coupled by different type networks. Physica A: Statistical Mechanics and its Applications. 2015;430:193–200.
  21. 21. Duan D, Lv C, Si S, Wang Z, Li D, Gao J, et al. Universal behavior of cascading failures in interdependent networks. Proceedings of the National Academy of Sciences in USA. 2019;116(45):22452–22457. pmid:31624122
  22. 22. Chujyo M, Hayashi Y. Optimal network robustness in continuously changing degree distributions. Proceeding of the 11th Int Complex Networks and their Applications Proc of Complex Networks & Their Applications XI. 2022;.
  23. 23. Newman MEJ. The structure and function of complex networks. SIAM Review. 2003;45(2):167–256.
  24. 24. Brandes U. On variants of shortest-path betweenness centrality and their generic computation. Social Networks. 2008;30(2):136–145.
  25. 25. Watts DJ, Strogatz SH. Collective dynamics of ‘small-world’networks. Nature. 1998;393(6684):440–442. pmid:9623998
  26. 26. Freeman LC. A set of measures of centrality based on betweenness. Sociometry. 1977; p. 35–41.
  27. 27. Brandes U. A faster algorithm for betweenness centrality. Journal of Mathematical Sociology. 2001;25(2):163–177.
  28. 28. Shao S, Huang X, Stanley HE, Havlin S. Percolation of localized attack on complex networks. New Journal of Physics. 2015;17(2):023049.
  29. 29. Latora V, Marchiori M. Efficient behavior of small-world networks. Physical Review Letters. 2001;87(19):198701. pmid:11690461
  30. 30. Dijkstra EW. A note on two problems in connexion with graphs. In: Edsger Wybe Dijkstra: His Life, Work, and Legacy; 2022. p. 287–290.