Literature DB >> 35701528

Identifying influential spreaders by gravity model considering multi-characteristics of nodes.

Zhe Li1, Xinyu Huang2.   

Abstract

How to identify influential spreaders in complex networks is a topic of general interest in the field of network science. Therefore, it wins an increasing attention and many influential spreaders identification methods have been proposed so far. A significant number of experiments indicate that depending on a single characteristic of nodes to reliably identify influential spreaders is inadequate. As a result, a series of methods integrating multi-characteristics of nodes have been proposed. In this paper, we propose a gravity model that effectively integrates multi-characteristics of nodes. The number of neighbors, the influence of neighbors, the location of nodes, and the path information between nodes are all taken into consideration in our model. Compared with well-known state-of-the-art methods, empirical analyses of the Susceptible-Infected-Recovered (SIR) spreading dynamics on ten real networks suggest that our model generally performs best. Furthermore, the empirical results suggest that even if our model only considers the second-order neighborhood of nodes, it still performs very competitively.
© 2022. The Author(s).

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Year:  2022        PMID: 35701528      PMCID: PMC9197977          DOI: 10.1038/s41598-022-14005-3

Source DB:  PubMed          Journal:  Sci Rep        ISSN: 2045-2322            Impact factor:   4.996


Introduction

The focus of network science has been shifting from discovering macroscopic statistical regularities to microscopic elements, vital nodes identification has received a huge amount of attention from researchers of network science in recent years. Vital nodes identification can be widely used in disease analysis[1,2], rumor analysis[3], information propagation[4], power grid protection[5], discovery of candidate drug targets and essential proteins[6], discovery of important species[7,8], and so on. So far, most known methods only use structural information[9], which can be classified into neighborhood-based centralities and path-based centralities roughly. Typical representatives of neighborhood-based centralities are degree centrality[10] (DC), H-index[11] and k-shell decomposition method[12] (KS). For DC, the more neighbors a node has, the greater its influence. For H-index, the more large-degree neighbors a node has, the greater its influence. For KS, the more central a node locates in the network, the greater its influence. Besides, eigenvector centrality[13] (EC) is the representative neighborhood-based iterative method, suggesting that the influence of a node is not only determined by the number of its neighbors, but also determined by the influence of each neighbor. Typical representatives of path-based centralities are betweenness centrality[14] (BC) and closeness centrality[15] (CC). For BC, the more a node is located in shortest paths, the greater its influence. For CC, the closer a node is to other nodes, the greater its influence. However, a significant number of experiments indicate that depending on a single characteristic of nodes to reliably identify influential spreaders is inadequate[9]. As a result, the methods integrating multi-characteristics of nodes have been proposed. In particular, the methods based on gravity law seem very promising. As several laws behind phenomena in life are similar to the gravity law, the gravity model, which derives from the gravity law, is also favored and exhibited in many real-life scenarios. Representative examples include predicting the population migration between regions in demography[16] and forecasting the trade flows throughout countries in economics[17]. In network science, the gravity model is utilized to evaluate the influence[18-20] of nodes, and so on. Recently, a series of gravity-law-based algorithms[18-30] considering both neighborhood information and path information have been proposed, and their performance is much better than the above well-known state-of-the-art methods. Typical representatives are gravity centrality[18] (GC), improved gravity centrality[19] (IGC) and local gravity model[20] (LGM). For GC, the k-shell value of a node is regarded as its mass. For IGC, the focal node uses the k-shell value as its mass while its neighbors view the degree value as their masses. For LGM, the degree value of a node is regarded as its mass. However, whether the degree or k-shell is regarded as mass, the influence of neighbors is not taken into consideration. In view of this, we propose a gravity model that effectively integrates multi-characteristics of nodes to measure the influence of nodes in spreading dynamics. In our model, the number of neighbors, the influence of neighbors, the location of nodes, and the path information between nodes are all taken into consideration.

Preliminaries

Well-known state-of-the-art methods

Denote an undirected and unweighted simple network, where V and E are the sets of nodes and links. Denote and , then the network has N nodes and M links. The adjacent matrix of G is denoted by , if node i links to node j, , otherwise, . The degree centrality[10] (DC) of node i is measured bywhere . The H-index[11] of node i, denoted by H(i), is defined as the maximal integer satisfying that there are at least H(i) neighbors of node i whose degrees are all greater than or equal to H(i). The k-shell decomposition method[12] (KS) works by iterative decomposition of the network into different shells. The first step of KS is to remove the nodes whose degrees are equal to 1 from the network, which will cause a reduction of the degree value to the remaining nodes. Continually remove all the nodes whose residual degrees are less than or equal to 1, until all the remaining nodes’ residual degrees are greater than 1. All the removed nodes in the first step form the 1-shell and their k-shell values are all equal to 1. Repeat this process to obtain 2-shell, 3-shell, , and so on. The decomposition process will continue until there are no more nodes in the network. The eigenvector centrality[13] (EC) of node i is measured bywhere c is a constant, generally speaking, c is set to the reciprocal of the largest eigenvalue of A. The betweenness centrality[14] (BC) of node i is measured bywhere is the number of shortest paths between node s and node t, and is the number of shortest paths via node i between node s and node t. The closeness centrality[15] (CC) of node i is measured bywhere d(i, j) is the shortest distance from node i to node j. The gravity centrality[18] (GC) of node i is measured bywhere is the k-shell value of node i, and is the neighborhood set whose distance to node i is not greater than 3. An extended version of GC, denoted by GC+, GC+ of node i is measured bywhere is the neighborhood set whose distance to node i equals to 1. The improved gravity centrality[19] (IGC) of node i is measured by An extended version of IGC, denoted by IGC+, IGC+ of node i is measured by The local gravity model[20] (LGM) of node i is measured bywhere R is the truncation radius, and the optimal truncation radius can be estimated bywhere is the average distance of the network.

The SIR model

The SIR model[31] initially considers all the nodes as in the susceptible (S) state except the source node in the infected (I) state. At each time step, each infected node can infect its susceptible neighbors with probability . Then, each infected node enters the recovered (R) state with probability . The propagation process continues until there are no more nodes in the infected state. The influence of node i can be estimated bywhere is the number of recovered nodes when dynamic process achieves steady state. For simplicity, is set to 1, then the corresponding epidemic threshold[32] can be calculated bywhere is the average degree, and is the second-order moment of the degree distribution.

The Kendall’s Tau

The Kendall’s Tau[33] is an index describing the strength of correlation between two sequences. Denote and are two sequences with N elements. For any pair of two-tuples and , if both and or both and , the pair is concordant. If both and or both and , the pair is discordant. If or , the pair is neither concordant nor discordant. The Kendall’s Tau of X and Y can be calculated bywhere is the number of concordant pairs, and is the number of discordant pairs.

The monotonicity

The monotonicity[34] M of ranking list L is used to quantitatively measure the resolution of different indices, and it can be calculated bywhere U is the size of L, and is the number of ties with the same rank r.

Results

Algorithms

According to previous studies, the degree value of a node indicates the number of its neighbors, the k-shell value of a node reflects where it locates in the network, the eigenvector centrality value of a node can reflect both the number of its neighbors and the influence of each neighbor, and the distance between two nodes can describe the path information. Individually speaking, nodes with large degree value, k-shell value and eigenvector centrality value are likely to be more influential. Furthermore, a node is of higher impacts on nearby nodes. According to the above issues and inspired by the gravity law, we regard the sum of degree value, k-shell value and eigenvector centrality value of a node as its mass, and the shortest distance between two nodes as their distance. Therefore, the influence of node i can be estimated as Such method is named as multi-characteristics gravity model (MCGM) as it considers multi-characteristics of nodes and adopts the gravity law. It is not difficult to find that these three indices (DC, KS, EC) are not in the same order of magnitude, so normalization is required. As a result, Eq. (15) can be rewritten aswhere , and denote the maximum of degree value, k-shell value and eigenvector centrality value, respectively. However, since the k-shell index has smaller value space, the normalized k-shell index is still larger than the other two indices. Therefore, it is necessary to lower the impact of the k-shell index. Given an index, due to the scale-free property of networks, the index values of most nodes are relatively small. Therefore, the index with larger value space generally has a smaller ratio between the median and the maximum. In our model, it is obvious that the value space of degree centrality and eigenvector centrality is larger than that of k-shell index. In view of this, we can lower the impact of k-shell index bywhere , and denote the median of degree value, k-shell value and eigenvector centrality value, respectively. The purpose of taking the maximum value of is to prevent the function of k-shell index from being excessively weakened. Finally, Eq. (15) can be rewritten asThe Algorithmic description of MCGM is provided in Algorithm 1. We take a toy network shown in Fig. 1 to illustrate the calculation process of Algorithm 1.
Figure 1

A toy network. The red nodes are in 1-shell, the green nodes are in 2-shell and the purple nodes are in 3-shell.

A toy network. The red nodes are in 1-shell, the green nodes are in 2-shell and the purple nodes are in 3-shell. Firstly, calculate the degree value, k-shell value and eigenvector centrality value of each node in the toy network, the results are shown in Table 1.
Table 1

The degree value, k-shell value and eigenvector centrality value of each node in the toy network.

NodeDCKSEC
1110.0259
2320.0943
3320.1256
4430.1714
5430.1534
6430.1534
7530.1917
8110.0421
9110.0421
The degree value, k-shell value and eigenvector centrality value of each node in the toy network. Secondly, calculate , , , , and , furthermore, calculate . Finally, the result of MCGM with of the toy network is shown in Table 2. Take node 3 as an example, the 1-order neighbors of node 3 are node 2, node 4 and node 7, the 2-order neighbors of node 3 are node 1, node 5 and node 6, so .
Table 2

The result of MCGM with of the toy network.

Node1-order neighbors2-order neighborsMCGM
123,71.9679
21,3,74,5,613.1293
32,4,71,5,616.9320
43,5,6,72,8,929.0955
54,6,7,82,3,926.0652
64,5,7,92,3,826.0652
72,3,4,5,61,8,935.9099
854,6,73.4704
964,5,73.4704
The result of MCGM with of the toy network.

Data description

In this paper, we apply ten real networks from six fields to test the performance of MCGM, including one transportation network (USAir[35]), one communication network (Email[36]), one infrastructure network (Power[37]), one technological network (Router[38]), two collaboration networks (Jazz[39] and NS[40]) and four social networks (PB[41], Facebook[42], WV[43] and Sex[44]). Table 3 shows these networks’ topological features, including the number of nodes, the number of links, the average degree, the average distance, the clustering coefficient[37], denoted by C, the assortative coefficient[45], denoted by r, the degree heterogeneity[46], denoted by H, and the epidemic threshold[32] of SIR model[31].
Table 3

The topological features of ten real networks.

NetworksNM\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\langle k \rangle $$\end{document}k\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\langle d \rangle $$\end{document}dCrH\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta _c$$\end{document}βc
USAir332212612.80722.73810.7494− 0.20793.46390.0231
Email113354519.62223.60600.25400.07821.94210.0565
Power494165942.669118.98920.10650.00351.45040.3483
Router502262582.49226.44880.0329− 0.13845.50310.0786
Jazz198274227.69702.23500.63340.02021.39510.0266
NS3799144.82326.04190.7981− 0.08171.66300.1424
PB12221671427.35522.73750.3600− 0.22132.97070.0125
Facebook40398823443.69103.69250.61700.06362.43920.0095
WV706610073628.51293.24750.2090− 0.08335.09920.0069
Sex15810385404.87545.78460.0000− 0.11455.82760.0365
The topological features of ten real networks.

Empirical results

Based on the above real networks, the well-known SIR model[31] is used to compare the influential rankings produced by algorithms and simulations. Given the network and the transmission probability , in order to guarantee the reliability of the results, 1000 independent realizations are executed and averaged to obtain the standard ranking of the influence of nodes (see details about SIR model in Preliminaries). In each realization, every node is selected once as the seed once. We apply the Kendall’s Tau () between the standard ranking and the ranking produced by the algorithm to measure the accuracy of an algorithm. Since , the closer the is to 1, the better the performance of the algorithm. The benchmark algorithms include degree centrality[10] (DC), H-index[11], k-shell decomposition method[12] (KS), eigenvector centrality[13] (EC), betweenness centrality[14] (BC), closeness centrality[15] (CC), DynamicRank[47] (DR), the extended version of gravity centrality[18] (GC+), the extended version of improved gravity centrality[19] (IGC+) and local gravity model[20] (LGM). Table 4 compares the accuracies of MCGM and the ten benchmark algorithms for . Furthermore, the accuracies of different values (not too far from ) are shown in Fig. 2.
Table 4

The algorithms’ accuracies of MCGM and the benchmark algorithms measured by Kendall’s Tau for .

NetworksDCH-indexKSECBCCCDRGC+IGC+LGMMCGM
USAir0.73700.75680.75290.89460.51710.80270.90960.89850.90060.88750.9145
Email0.76530.78830.77020.88320.62430.81630.89910.91190.91330.86970.9091
Power0.42640.40090.31220.28180.32540.38380.75700.79060.83870.74420.7639
Router0.31390.19280.18100.59240.30960.63830.82150.78960.78230.78940.8324
Jazz0.81500.85130.76380.88540.46410.70080.87610.91580.92440.86660.9333
NS0.57900.56100.51060.36600.30030.33970.73770.85110.87220.83720.8736
PB0.85240.86940.85950.87380.67710.78520.90600.91890.91760.90300.9184
Facebook0.67980.70660.70750.62260.45290.39400.78650.84140.83720.82750.8639
WV0.76190.76620.76570.83340.69780.81270.83600.82980.83050.82760.8379
Sex0.46640.48550.49250.74040.41180.76770.81390.80380.80760.77890.8448

The parameters in the related algorithms (i.e., LGM and MCGM) are adjusted to their optimal values subject to the largest , that is, we need to search the optimal truncation radius which can maximize by traversing the truncation radius. Obviously, searching the optimal truncation radius in this way is very time-consuming, fortunately, in subsequent experiments, we find that MCGM still performs very competitively even if the truncation radius is just set to 2. For each network, the best algorithm is emphasized by bold.

Figure 2

The algorithms’ accuracies measured by Kendall’s Tau for different . The six classic algorithms (DC, H-index, KS, EC, BC and CC) are represented by black symbols, DR is represented by green symbols, the typical algorithms based on the gravity law (GC+, IGC+ and LGM) are represented by blue symbols, MCGM is represented by red symbols.

The algorithms’ accuracies of MCGM and the benchmark algorithms measured by Kendall’s Tau for . The parameters in the related algorithms (i.e., LGM and MCGM) are adjusted to their optimal values subject to the largest , that is, we need to search the optimal truncation radius which can maximize by traversing the truncation radius. Obviously, searching the optimal truncation radius in this way is very time-consuming, fortunately, in subsequent experiments, we find that MCGM still performs very competitively even if the truncation radius is just set to 2. For each network, the best algorithm is emphasized by bold. The algorithms’ accuracies measured by Kendall’s Tau for different . The six classic algorithms (DC, H-index, KS, EC, BC and CC) are represented by black symbols, DR is represented by green symbols, the typical algorithms based on the gravity law (GC+, IGC+ and LGM) are represented by blue symbols, MCGM is represented by red symbols. As shown in Table 4, the methods based on gravity law (GC+, IGC+, LGM and MCGM) show great advantages over the classic methods (DC, H-index, KS, EC, BC, CC), especially in Power, Router and NS, the advantage of the methods based on gravity law are extremely obvious. Notice that, except the above three networks, the performance of EC is significantly better than other classic methods, and even performs competitively in comparison with the methods based on gravity law, which indirectly shows that the stability of the method based on the gravity law is better and their performance will not decline precipitously due to the differences of networks. Furthermore, for the methods based on gravity law, MCGM generally performs best since it effectively considers more characteristics of nodes. As shown in Fig. 2, MCGM still performs very competitively compared with the ten benchmark algorithms for different not too far from , suggesting the robustness of our findings. Figure 3 shows the optimal truncation radius of MCGM in the ten real networks. It is not difficult to find that the optimal truncation radius of most networks is concentrated at . Therefore, we may simply set to test the performance of MCGM. Table 5 compares the accuracies of MCGM with and the benchmark algorithms.
Figure 3

The of MCGM for . Ten pentagrams represent ten networks and the blue line is . The of MCGM in USAir, Jazz and PB is 1, the of MCGM in Email, Router, NS, Facebook, WV and Sex is 2, and the of MCGM in Power is 6.

Table 5

The algorithms’ accuracies of MCGM with and the benchmark algorithms measured by Kendall’s Tau for .

NetworksDCH-indexKSECBCCCDRGC+IGC+LGMMCGM (\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$R=2$$\end{document}R=2)
USAir0.73700.75680.75290.89460.51710.80270.90960.89850.90060.88750.9092
Email0.76530.78830.77020.88320.62430.81630.89910.91190.91330.86970.9091
Power0.42640.40090.31220.28180.32540.38380.75700.79060.83870.74420.6616
Router0.31390.19280.18100.59240.30960.63830.82150.78960.78230.78940.8324
Jazz0.81500.85130.76380.88540.46410.70080.87610.91580.92440.86660.9255
NS0.57900.56100.51060.36600.30030.33970.73770.85110.87220.83720.8736
PB0.85240.86940.85950.87380.67710.78520.90600.91890.91760.90300.9123
Facebook0.67980.70660.70750.62260.45290.39400.78650.84140.83720.82750.8639
WV0.76190.76620.76570.83340.69780.81270.83600.82980.83050.82760.8379
Sex0.46640.48550.49250.74040.41180.76770.81390.80380.80760.77890.8448

For each network, the best algorithm is emphasized by bold.

The of MCGM for . Ten pentagrams represent ten networks and the blue line is . The of MCGM in USAir, Jazz and PB is 1, the of MCGM in Email, Router, NS, Facebook, WV and Sex is 2, and the of MCGM in Power is 6. The algorithms’ accuracies of MCGM with and the benchmark algorithms measured by Kendall’s Tau for . For each network, the best algorithm is emphasized by bold. As shown in Table 5, MCGM with generally performs best in comparison with the benchmark algorithms, it still obtains the best results in six of the ten real networks. Since the optimal truncation radius approximately scales linearly with the average distance[20], if the average distance of the network is relatively large, setting will have a significant impact on the performance of MCGM, such as Power whose average distance is 18.9892. Fortunately, most real networks have small-world property, tends to be small in most cases. Furthermore, we need to compare MCGM and MCGM without normalization to illustrate the importance of normalization. Table 6 compares the accuracies of MCGM using Eq. (15), MCGM using Eq. (16) and MCGM using Eq. (18). As shown in Table 6, MCGM has been gradually improved by normalization, suggesting the importance of normalization and the effectiveness of our normalization strategy.
Table 6

The algorithms’ accuracies of MCGM using Eq. (15), MCGM using Eq. (16) and MCGM using Eq. (18) measured by Kendall’s Tau for .

NetworksMCGM (Eq. 15)MCGM (Eq. 16)MCGM (Eq. 18)
USAir0.89460.90600.9145
Email0.87820.89860.9091
Power0.75570.75690.7639
Router0.79920.79830.8324
Jazz0.88880.92120.9333
NS0.84280.87100.8736
PB0.90470.91100.9184
Facebook0.83810.85470.8639
WV0.82990.83410.8379
Sex0.78770.79960.8448

The parameters are adjusted to their optimal values subject to the largest . For each network, the best algorithm is emphasized by bold.

The algorithms’ accuracies of MCGM using Eq. (15), MCGM using Eq. (16) and MCGM using Eq. (18) measured by Kendall’s Tau for . The parameters are adjusted to their optimal values subject to the largest . For each network, the best algorithm is emphasized by bold. Finally, we apply the monotonicity[34] to measure the resolution of different algorithms. As shown in Table 7, MCGM generally performs best even if it only considers 1-order neighbors or 2-order neighbors in most cases. The results reported in Table 7 demonstrate MCGM is a remarkably high-resolution algorithm.
Table 7

The monotonicity of different algorithms. The parameters in the related algorithms (i.e., LGM and MCGM) are adjusted to their optimal values subject to the largest .

NetworksDCH-indexKSECBCCCDRGC+IGC+LGMMCGM
USAir0.85860.83550.81140.99510.69700.98920.99510.99510.99510.99330.9951
Email0.88740.85830.80880.99990.94000.99880.99990.99990.99990.99980.9999
Power0.59270.39300.24600.99990.83140.99980.99620.99960.99970.99990.9999
Router0.28860.08760.06910.99640.29850.99610.99560.99650.99650.99640.9966
Jazz0.96590.93830.79440.99940.98850.98780.99930.99950.99930.99910.9994
NS0.76420.68250.64210.99550.33880.99280.99500.99540.99560.99330.9955
PB0.93280.92680.90640.99930.94890.99800.99930.99930.99930.99910.9993
Facebook0.97390.96650.94190.99990.98550.99670.99990.99990.99990.99990.9999
WV0.77610.77320.76730.99960.77040.99940.99960.99960.99960.99960.9996
Sex0.60020.54570.52880.99970.67570.99960.99960.99970.99970.99970.9997

For each network, the best algorithm is emphasized by bold.

The monotonicity of different algorithms. The parameters in the related algorithms (i.e., LGM and MCGM) are adjusted to their optimal values subject to the largest . For each network, the best algorithm is emphasized by bold.

Computational complexity

The computational complexity of the methods used in this paper is shown in Table 8. The computational complexity of DC, KS and EC is O(N), O(M) and , respectively. Therefore, it is obvious that the part with the highest computational complexity of MCGM is computing the R-order neighbors of each node, it needs times operations. Hence the computational complexity of MCGM is . Since most real networks have small-world property, in most cases (see Fig. 3), so the computational complexity of MCGM is generally not more than , where .
Table 8

The computational complexity of MCGM and the benchmark algorithms.

MethodsTopologyComplexity
DCLocalO(N)
H-indexSemi-local\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$O(N+M)$$\end{document}O(N+M)
KSGlobalO(M)
ECGlobal\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$O(N+M)$$\end{document}O(N+M)
BCGlobal\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$O(NM+N^{2}logN)$$\end{document}O(NM+N2logN)
CCGlobal\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$O(NM+N^{2}logN)$$\end{document}O(NM+N2logN)
DRSemi-local\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$O(N\langle k \rangle ^{3})$$\end{document}O(Nk3)
GC+Global\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$O(N\langle k \rangle ^{3})$$\end{document}O(Nk3)
IGC+Global\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$O(N\langle k \rangle ^{3})$$\end{document}O(Nk3)
LGMSemi-local\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$O(N\langle k \rangle ^{R})$$\end{document}O(NkR)
MCGMGlobal\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$O(N\langle k \rangle ^{R})$$\end{document}O(NkR)
The computational complexity of MCGM and the benchmark algorithms.

Discussion

In summary, we propose a novel gravity model that effectively integrates multi-characteristics of nodes, named as multi-characteristics gravity model (MCGM). The number of neighbors, the influence of neighbors, the location of nodes, and the path information between nodes are all taken into consideration in our model. In addition, we propose a normalization strategy to solve the problem that different indices are not in the same order of magnitude, Table 6 suggests the importance of normalization and the effectiveness of our normalization strategy. Compared with well-known state-of-the-art methods, empirical analyses of the SIR spreading dynamics on ten real networks suggest that our model always performs very competitively, as shown in Table 4. However, MCGM needs to find the optimal truncation radius by traversing the truncation radius and it is very time-consuming. Fortunately, the optimal truncation radius approximately scales linearly with the average distance[20], and most real networks have small-world property[37,48], so even if the truncation radius is just set to 2, MCGM still performs very competitively in most cases, as shown in Table 5. Therefore, without increasing the computational complexity, MCGM effectively considers more characteristics of nodes and obtains more accurate results. Although the computational complexity of MCGM is not high, it needs the global topological structure, same as GC+ and IGC+. While LGM can work under the case where the global topology is not known. As a result, our suggestions for practical use are as follows: if the network’s global topology is known, apply MCGM and set R to 2, otherwise, apply LGM and set R to 2 or 3. Of course, there are still some potential problems in the future. First of all, the gravity law is symmetrical, but due to the different effects of different nodes or the inherent asymmetry of dynamics[49,50], an asymmetric form of the gravity law may be relevant. Secondly, in weighted complex networks, the heterogeneity of links greatly changes nodes’ importance[51], a weighted form of the gravity law may be relevant. Finally, in order to establish a unified research framework, a unified gravity model is needed to be proposed. Although GC+, IGC+ and LGM are proposed from different perspectives, a unified form of expression exists. We propose a rough model which intends to start further discussion on this issue. The rough unified gravity model is described aswhere a and b are adjustable parameters. If and , the unified gravity model degenerates to LGM. If and , the unified gravity model degenerates to GC (GC+ can be obtained by Eq. (6)). If and , the unified gravity model degenerates to IGC (IGC+ can be obtained by Eq. (8)).
  20 in total

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2.  Assortative mixing in networks.

Authors:  M E J Newman
Journal:  Phys Rev Lett       Date:  2002-10-28       Impact factor: 9.161

3.  Absence of influential spreaders in rumor dynamics.

Authors:  Javier Borge-Holthoefer; Yamir Moreno
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4.  Collective dynamics of 'small-world' networks.

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5.  Identifying influential spreaders in complex networks by propagation probability dynamics.

Authors:  Duan-Bing Chen; Hong-Liang Sun; Qing Tang; Sheng-Zhao Tian; Mei Xie
Journal:  Chaos       Date:  2019-03       Impact factor: 3.642

Review 6.  Network medicine: a network-based approach to human disease.

Authors:  Albert-László Barabási; Natali Gulbahce; Joseph Loscalzo
Journal:  Nat Rev Genet       Date:  2011-01       Impact factor: 53.242

7.  Comprehensive influence of topological location and neighbor information on identifying influential nodes in complex networks.

Authors:  Xiaohua Wang; Qing Yang; Meizhen Liu; Xiaojian Ma
Journal:  PLoS One       Date:  2021-05-21       Impact factor: 3.240

8.  The H-index of a network node and its relation to degree and coreness.

Authors:  Linyuan Lü; Tao Zhou; Qian-Ming Zhang; H Eugene Stanley
Journal:  Nat Commun       Date:  2016-01-12       Impact factor: 14.919

9.  Identifying influential spreaders by gravity model.

Authors:  Zhe Li; Tao Ren; Xiaoqi Ma; Simiao Liu; Yixin Zhang; Tao Zhou
Journal:  Sci Rep       Date:  2019-06-10       Impact factor: 4.379

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