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Multilayer social reinforcement induces bistability on multiplex networks

Longzhao Liu1,2,4,6, Xin Wang1,3,6, Shaoting Tang1,6,7, Hongwei Zheng5,7 and Zhiming Zheng1,5,6 1 LMIB, NLSDE, BDBC, School of Mathematical Sciences, Beihang University, Beijing 100191, China 2 ShenYuan Honor School, Beihang University, Beijing 100191, China 3 Department of Mathematics, Dartmouth College, Hanover, NH 03755, USA 4 Northwestern Institute on Complex Systems, Northwestern University, Evanston, IL 60208, USA 5 Institute of Artificial Intelligence and Blockchain, Guangzhou university, Guangdong province 510006, China 6 PengCheng Laboratory, Shenzhen, 518055 , China 7 Author to whom any correspondence should be addressed [email protected], [email protected]
Abstract

Social reinforcement mechanism, which characterizes the promoting effects when exposing to multiple sources in social contagion process, is ubiquitous in information-technology ecosystem and has aroused great attention in recent years. While the impacts of social reinforcement on single-layer networks are well-documented, extension to multilayer networks is needed to study how reinforcement from different social circles influences the spreading dynamics. To this end, we incorporate multilayer social reinforcement into ignorant-spreader-ignorant (SIS) model on multiplex networks. Our theoretical analysis combines pairwise method and mean-field theory and agrees well with large-scale simulations. Surprisingly, we find this complex social contagion mechanism triggers the emergence of bistability phenomena, where extinction and outbreak states coexist. In particular, the hysteresis loop of stationary prevalence occurs in this bistable region, explaining why the fight towards the spread of rumors is protracted and difficult in modern society. Further, we show that the final state of bistable regions depends on the initial density of adopters, the critical value of which decreases as the contagion transmissibility or the multilayer reinforcement increases. In particular, we highlight two possible conditions for the outbreak of social contagion: to possess large contagion transmissibility, or to possess large initial density of adopters with strong multilayer reinforcement. Our results unveil the non-negligible power of social reinforcement on multiplex networks, which sheds lights on designing efficient strategies in spreading behaviors such as marketing and promoting innovations.

Keywords: complex social contagion, multiplex networks, multilayer social reinforcement, bistability, hysteresis loop.

1 Introduction

Social contagion describes a variety of behavioral imitations caused by social influence and is particularly ubiquitous in the digital age [1, 2, 3]. In order to predict and control the collective contagion phenomena on large-scale social networks, such as the spread of rumors, social norms and online behaviors, scientists have made great efforts on understanding the underlying dynamical mechanisms [4, 5, 6, 7]. Early studies argued that the dynamical processes of social contagion are similar to disease spreading in the sense that a simple contact with a single infected individual can trigger diffusion [8, 9, 10]. Therefore, many epidemic-like models are proposed, which are called simple contagion models. These models provide profound insights into many physical phenomena on social networks, such as the cascading process of information diffusion, the co-contagion dynamics on multiplex networks, and etc [11, 12].

However, simple contagion model can not deal with the spread of more complex social behaviors, especially when the behaviors are risky, costly or polarized, ranging from the spread of public health behaviors (e.g., vaccine, vaping, diet) to social movement [13, 14, 15]. For instance, a well-known complex mechanism of social contagion is called the social reinforcement. It corresponds to the fact that exposure to multiple sources with a same stimuli would give individuals more confidence to participate than multiple exposures to the same source, leading to a significant promotion on social transmission [16, 17]. As McAdam and Paulsen concluded [18], “the fact that we are embedded in many relationships means that any major decision we are contemplating will likely be mediated by a significant subset of those relationships”. Nevertheless, this empirically confirmed phenomenon is fundamentally different from the view of simple contagion model [19, 20]. Hence, more complex mechanisms were further incorporated into dynamical models. These complex contagion models lead to abundant intriguing findings, some of which even conflict with conclusions of simple contagion models [21, 22]. For example, threshold models assumed that social contagion only happens when the number (or fraction) of exposures to multiple sources exceeds a given threshold and suggested the dependence of diffusion results on initial density of adopters [23]. In addition, Centola et al. proved that the clustering network structure suppressed simple contagion while surprisingly facilitated the spread of behaviors that require social reinforcement [24]. Another framework modified epidemic-like models by increasing transmission rate when exposing to multiple sources, and showed the promoting effect of social reinforcement on contagion processes [25, 26]. Another well-known complex mechanism is caused by the interplay between spreading dynamics and network topology. For example, Gross et al. studied contagion process on adaptive networks where the connection between nodes relies on their states, and showed that this dynamics-topology interaction could lead to the emergence of bistable region where healthy and endemic states co-exist [27]. Besides, Iacopini et al. noted that the existence of high-order structures embedded on single-layer networks, such as full triangles, could also induce bistable phenomena [28].

Moreover, complex mechanisms depicting interactions between multiple contagion processes on networked systems, such as the spreading of interacting diseases, were widely investigated [29]. Chen et al. explored cooperative contagion processes where individuals infected by one disease are more susceptible to the other, and showed that large degree of cooperation could lead to the occurrence of abrupt phase transition and bistability [30]. Soriano-Paños et al. described the interaction between cooperative or competitive diseases by increasing or decreasing the susceptibility of individuals infected by one of the diseases, and also found bistability caused by cooperativity between diseases [31]. Sanz et al. proposed a general framework analyzing simultaneous spreading of two interacting diseases and derived complex phase diagrams [32]. Pinotti et al. explored a three-player pathogen system where competition and cooperation coexist, and showed that the presence of cooperative pathogen could lead to some intriguing phenomena including non-monotonic boundaries separating phase diagram and bistability [33]. There were also many works extending the framework from single-layer networks to multilayer networks [34]. For example, Wu et al. studied discrete-time Markov-Chain model depicting the spreading of two diseases in multiplex networks and derived epidemic thresholds [35].

Recently, owing to the development of various social medias, many social behaviors spread in multiple social circles rather than in a single social circle, which are naturally modeled as multilayer networks [36, 37, 38, 39]. Each layer represents a single social circle which could be an online social platform or a network of offline relationships, such as friendships and colleagues. Similar to social reinforcement in a single-layer network, there exists significant difference between exposure to multiple social circles (multilayer reinforcement) and multiple exposures to the same social circle (intra-layer reinforcement)[40]. Specifically, individuals would be more convinced and have higher possibility for diffusion when receiving the same informative stimulus from different social circles. However, previous studies mainly concentrated on simple interactions between nodes and its replicas in different layers [41, 42]. The detailed impacts of multilayer reinforcement mechanism that engineers complex social contagion remain largely unknown.

To fill this gap, here we propose a theoretical framework that incorporates multilayer reinforcement into ignorant-spreader-ignorant (SIS) model to study the spreading dynamics on multiplex networks. We find this complex social contagion mechanism not only expands dissemination, but also results in the emergence of bistable region, within which extinction and outbreak states coexist. Within bistable region, the final state depends on the initial density of adopters. We also detailedly discuss the hysteresis loop and the unstable equilibrium manifolds occurred in the bistable region. Through observing phase diagrams, we highlight two conditions for the outbreak of social contagion: (i) to possess large transmissibility; (ii) to possess large initial density of adopters with strong multilayer reinforcement. As the second condition cannot be obtained by simple contagion model and is less intuitive, our results stress the unneglectable role of complex social contagion and are in line with the findings of previous experimental studies that critical masses are required for establishing collective behaviors such as social changes [43]. In addition, similar phenomena are also observed on finite-size heterogeneous multiplex networks. Our findings provide valuable insights toward dynamical evolutions of complex social contagion on multiplex networks, which are of vital importance for understanding collective online behaviors in the era of social media. In particular, the emerging bistable phenomenon on multiplex networks indicates that the information (truth, ideas, advertisements, etc.) can stride across the trap of extinction and become widespread by selecting a large proportion of initial spreaders on multiple platforms, which implies effective strategies for controlling rumors, promoting innovations and marketing. [44, 45, 46].

2 Model

Consider an undirected multiplex network with two layers, denoted as layer 1 and layer 2. Each layer stands for a social circle, which is an online social platform or an offline relationship network composed of interacting individuals such as friends, families and colleges. Both layers have the same nodes and interlayer edges only connect entities with their replicas, as shown in figure 1(a).

Here we stress that our main purpose is to explore the influence of complex social contagion aroused by multiple social circles, i.e., multilayer reinforcement mechanism. Therefore, we adopt ignorant-spreader-ignorant (SIS) model rather than complex contagion model to characterize the intralayer spreading process, which provides better analytical insights while at expense of being less realistic. In this situation, spreader (SS) represents individuals who adopt norms (information, cognition, attitudes, behaviors and so on) and are willing to spread, while ignorant (II) stands for nodes who do not adopt norms or have no motivation to spread, corresponding to infected and susceptible state in epidemiology, respectively. In each layer kk (k=1,2)(k=1,2), spreader has a probability λk\lambda_{k} to spread norms to its ignorant neighbors and becomes ignorant with probability μk\mu_{k}, as shown in figure 1(b).

Beyond intralayer contagion processes, norms also diffuse across layers, i.e., the interactions between layers. First, complying with previous studies, we utilize interlayer contagion processes where ignorant has a probability pp to become a spreader once its counterpart is in SS state, which depicts the interaction between agents and their replicas, as shown in figure 1(c) [47]. Then, we introduce multilayer reinforcement mechanism to mimic the fact that exposure to multiple social circles is more convincing than multiple exposures to a single social circle. At each time step, if an individual can receive norms from both social circles, i.e. he/she has at least one spreader neighbor in each layer, then with probability γ\gamma the individual would randomly choose one layer to spread the norms (figure 1(d)). The parameter γ\gamma reflects the strength of multilayer reinforcement.

In summary, our model is composed of three processes: intralayer contagion, interlayer contagion and multilayer reinforcement, which is as follows:

  1. 1.

    Intralayer contagion. At each time step, in layer kk, SS makes its neighbors in II state become SS with probability λk\lambda_{k}. Meanwhile, SS turns into II with probability μk\mu_{k}.

  2. 2.

    Interlayer contagion. At each time step, II becomes SS with probability pp if its replica is a spreader.

  3. 3.

    Multilayer reinforcement. At each time step, a node has a probability γ\gamma to randomly choose a layer and become a spreader if there exists at least one spreader in its neighborhood of each layer.

Refer to caption
Figure 1: Schematic of modeling framework. (a) Network structure. The underlying network is composed of two layers with the same nodes, where interlayer edges only connect entities and their replicas. Node’s state is represented by different colors: spreader (red), ignorant (black). (b)-(d) Dynamical model. Our model includes three dynamical processes, whose propagation path is highlighted by red arrows in each subfigure. (b) Intralayer contagion. In each layer, an ignorant has a probability to be infected by its spreader neighbors. (c) Interlayer contagion. An ignorant may change its state to a spreader if its replica is a spreader. (d) Multilayer reinforcement. When node ii is connected to at least one spreader in each layer and is able to receive stimuli from both platforms at the same time, ii randomly chooses a layer and becomes a spreader with a certain probability.

3 Theoretical framework

In this section, we explore dynamical equations of our model on homogeneous multiplex systems, composed of two Erdös-Rényi (ER) networks with average degree k1\langle k_{1}\rangle and k2\langle k_{2}\rangle. The major challenge is the dynamical correlation between two layers caused by interlayer contagion and multilayer reinforcement. Specifically, the counterpart of a spreader is more likely to be a spreader than the counterpart of an ignorant. Classic Mean-field approximation does not consider the dynamical correlation, which leads to the deviation of theoretical predictions from Monte Carlo simulations (see A). To overcome the difficulty, we conduct theoretical analysis by combining pairwise method and mean-field theory.

Here, we define ρX,Y(t)\rho_{X,Y}(t) as the probability that the individual is XX state in layer 1 and YY state in layer 2. Clearly, each individual has four possible states and we have ρS,S(t)+ρS,I(t)+ρI,S(t)+ρI,I(t)=1\rho_{S,S}(t)+\rho_{S,I}(t)+\rho_{I,S}(t)+\rho_{I,I}(t)=1. To begin, we explore intralayer contagion process. Let θk(t)\theta_{k}(t) represent the probability that a node in layer kk is not convinced by its neighbors of the same layer. Utilizing the mean-field theory, θk(t)\theta_{k}(t) can be approximated by

θ1(t)=(1λ1(ρS,S(t)+ρS,I(t)))k1θ2(t)=(1λ2(ρS,S(t)+ρI,S(t)))k2.\eqalign{\theta_{1}(t)&=(1-\lambda_{1}(\rho_{S,S}(t)+\rho_{S,I}(t)))^{\langle k_{1}\rangle}\\ \theta_{2}(t)&=(1-\lambda_{2}(\rho_{S,S}(t)+\rho_{I,S}(t)))^{\langle k_{2}\rangle}.} (1)

Then, we examine the influence of multilayer reinforcement. Denote δk(t)\delta_{k}(t) as the probability that the multilayer reinforcement does not make ignorant turn into a spreader in layer kk. We have δ1(t)=δ2(t)=δ(t)\delta_{1}(t)=\delta_{2}(t)=\delta(t), which can be approximated by

δ(t)=10.5γ(1(1ρS,S(t)ρS,I(t))k1)(1(1ρS,S(t)ρI,S(t))k2),\eqalign{\delta(t)=1-0.5&*\gamma\\ &*(1-(1-\rho_{S,S}(t)-\rho_{S,I}(t))^{\langle k_{1}\rangle})\\ &*(1-(1-\rho_{S,S}(t)-\rho_{I,S}(t))^{\langle k_{2}\rangle}),} (2)

where (1(1ρS,S(t)ρS,I(t))k1)(1-(1-\rho_{S,S}(t)-\rho_{S,I}(t))^{\langle k_{1}\rangle}) and (1(1ρS,S(t)ρI,S(t))k2)(1-(1-\rho_{S,S}(t)-\rho_{I,S}(t))^{\langle k_{2}\rangle}) account for the probabilities that there exists at least one spreader neighbor in layer 1 and in layer 2, respectively.

Furthermore, let gkI(t)g^{I}_{k}(t) and gkS(t)g_{k}^{S}(t) represent the probabilities that ignorant in layer kk is not convinced if its counterpart is in ignorant and spreader state, respectively. The probabilities describe the integrated influence of intralayer contagion, interlayer contagion and multilayer reinforcement. Because the three processes are approximately independent in our model, the probabilities read

gkI(t)=θk(t)δ(t)gkS(t)=θk(t)δ(t)(1p).\eqalign{g^{I}_{k}(t)&=\theta_{k}(t)*\delta(t)\\ g^{S}_{k}(t)&=\theta_{k}(t)*\delta(t)*(1-p).} (3)

Finally, the temporal evolutionary equations of ρS,S(t)\rho_{S,S}(t) can be written as

dρS,Sdt=ρS,S{1(1μ1)(1μ2)}+ρS,I(1μ1)(1g2S)+ρI,S(1μ2)(1g1S)+ρI,I(1g1I)(1g2I),\eqalign{\frac{d\rho_{S,S}}{dt}&=-\rho_{S,S}\{1-(1-\mu_{1})(1-\mu_{2})\}+\rho_{S,I}(1-\mu_{1})(1-g^{S}_{2})\\ &+\rho_{I,S}(1-\mu_{2})(1-g^{S}_{1})+\rho_{I,I}(1-g^{I}_{1})(1-g^{I}_{2}),\\ } (4)

where the first term represents the outflow from the SSS-S class and the last three terms stand for transition from the other states to SSS-S state. Similarly, we can derive the dynamical evolutions of ρS,I(t)\rho_{S,I}(t), ρI,S(t)\rho_{I,S}(t) and ρI,I(t)\rho_{I,I}(t). For the sake of theoretical analysis and readability, ρI,I(t)\rho_{I,I}(t) is automatically substituted for (1ρS,S(t)ρS,I(t)ρI,S(t))(1-\rho_{S,S}(t)-\rho_{S,I}(t)-\rho_{I,S}(t)). Thus, the evolutionary equations of our model read as follows:

dρS,Sdt=ρS,S{1(1μ1)(1μ2)}+ρS,I(1μ1)(1g2S)+ρI,S(1μ2)(1g1S)+(1ρS,SρS,IρI,S)(1g1I)(1g2I)dρS,Idt=ρS,S(1μ1)μ2ρS,I{1(1μ1)g2S}+ρI,S(1g1S)μ2+(1ρS,SρS,IρI,S)(1g1I)g2IdρI,Sdt=ρS,S(1μ2)μ1+ρS,I(1g2S)μ1ρI,S{1(1μ2)g1S}+(1ρS,SρS,IρI,S)g1I(1g2I).\eqalign{\frac{d\rho_{S,S}}{dt}&=-\rho_{S,S}\{1-(1-\mu_{1})(1-\mu_{2})\}+\rho_{S,I}(1-\mu_{1})(1-g^{S}_{2})\\ &+\rho_{I,S}(1-\mu_{2})(1-g^{S}_{1})+(1-\rho_{S,S}-\rho_{S,I}-\rho_{I,S})(1-g^{I}_{1})(1-g^{I}_{2})\\ \frac{d\rho_{S,I}}{dt}&=\rho_{S,S}(1-\mu_{1})\mu_{2}-\rho_{S,I}\{1-(1-\mu_{1})g^{S}_{2}\}\\ &+\rho_{I,S}(1-g^{S}_{1})\mu_{2}+(1-\rho_{S,S}-\rho_{S,I}-\rho_{I,S})(1-g^{I}_{1})g^{I}_{2}\\ \frac{d\rho_{I,S}}{dt}&=\rho_{S,S}(1-\mu_{2})\mu_{1}+\rho_{S,I}(1-g^{S}_{2})\mu_{1}\\ &-\rho_{I,S}\{1-(1-\mu_{2})g^{S}_{1}\}+(1-\rho_{S,S}-\rho_{S,I}-\rho_{I,S})g^{I}_{1}(1-g^{I}_{2}).\\ } (5)

Equation (5) can be simply written as

d𝝆dt=𝒇(𝝆),\frac{d\boldsymbol{\rho}}{dt}=\boldsymbol{f}(\boldsymbol{\rho}), (6)

where 𝝆(t)=(ρS,S(t),ρS,I(t),ρI,S(t))\boldsymbol{\rho}(t)=(\rho_{S,S}(t),\rho_{S,I}(t),\rho_{I,S}(t)). This indicates that the dynamical system is 3-dimension autonomous. Thus, the stability of the fixed points directly determines evolutionary results of the system. We define 𝝆f\boldsymbol{\rho}_{f} as the fixed point of equation (5), which satisfies

𝒇(𝝆f)=𝟎.\boldsymbol{f}(\boldsymbol{\rho}_{f})=\boldsymbol{0}.\\ (7)

In particular, 𝝆f\boldsymbol{\rho}_{f} represents the final state of the system if and only if the fixed point is stable, i.e.,

Λmax(d𝒇d𝝆|𝝆=𝝆f)<0,\Lambda_{max}(\frac{d\boldsymbol{f}}{d\boldsymbol{\rho}}|_{\boldsymbol{\rho}=\boldsymbol{\rho}_{f}})<0,\\ (8)

where Λmax(J)\Lambda_{max}(J) is the largest eigenvalue of matrix JJ.

We notice that there is at least one fixed point (𝝆f=𝟎\boldsymbol{\rho}_{f}=\boldsymbol{0}), which represents that all individuals are in III-I state. When the initial density of spreaders is small, norms go extinct if and only if 𝝆f=𝟎\boldsymbol{\rho}_{f}=\boldsymbol{0} is stable, i.e.,

Λmax(d𝒇d𝝆|𝝆=𝟎)<0.\Lambda_{max}(\frac{d\boldsymbol{f}}{d\boldsymbol{\rho}}|_{\boldsymbol{\rho}=\boldsymbol{0}})<0.\\ (9)

4 Results

4.1 Complex social contagion on homogeneous multiplex networks

Refer to caption
Figure 2: Emergence of bistable phenomena. Prevalence curves are shown against (a)-(b) intralayer transmissibility and (c)-(d) interlayer transmissibility for different values of multilayer reinforcement and initial density of adopters. In each figure, γ=0\gamma=0 (red), γ=0.1\gamma=0.1 (yellow), γ=0.3\gamma=0.3 (blue) and ρ0=0.03\rho_{0}=0.03 (square), ρ0=0.2\rho_{0}=0.2 (diamond). Simulation results are averaged over 30 independent runs, whose standard errors are shown in subplots. In most cases, errors are within 0.01. However, errors can exceed 0.01 when the system is close to the critical points, as the stochastic fluctuation of simulations is relatively large around the thresholds. Theoretical predictions solved by equation (5) are shown by solid lines. Note that for γ=0.3\gamma=0.3 in (a) and γ=0.1\gamma=0.1 or γ=0.3\gamma=0.3 in (c), there emerges bistable region where outbreak and extinction states co-exist. Parameters: μ1=0.6\mu_{1}=0.6, μ2=0.6\mu_{2}=0.6. In addition, (a) λ2=0.02\lambda_{2}=0.02, p=0.1p=0.1, (b) λ2=0.1\lambda_{2}=0.1, p=0.1p=0.1, (c) λ1=0.06\lambda_{1}=0.06, λ2=0.04\lambda_{2}=0.04, and (d) λ1=0.14\lambda_{1}=0.14, λ2=0.06\lambda_{2}=0.06.

In this section, we explore how our model behaves on homogeneous multiplex networks, especially the influence of multilayer reinforcement on the prevalence of norms and the critical properties that separate outbreak and extinction. We start from homogeneous multiplex networks composed of two Erdös-Rényi (ER) graphs with N=10000N=10000 nodes, the average degree of which are k1=6\langle k_{1}\rangle=6 and k2=8\langle k_{2}\rangle=8, respectively. Initially, we randomly set a certain fraction of population as adopters, denoted by ρ0\rho_{0}, who are spreaders in both layers[48]. Here we run 300-step simulations to ensure that the system has reached the dynamic equilibrium.

Refer to caption
Figure 3: Hysteresis phenomena. Shown are the hysteresis loops of the stationary prevalence with respect to changes in (a) intralayer transmissibility and (b) interlayer transmissibility. Two different evolutionary routes arise: prevalence increases from zero to positive values along the ascending path (blue squares) with λ1\lambda_{1} or pp grows, while recovers to zero along the descending path (red triangles) as transmissibility decreases. Theoretical predictions (solid lines) are in good agreement with simulations in most situations. The relatively large stochastic fluctuation of simulations only occurs around the thresholds. Parameters: (a) λ2=0.02\lambda_{2}=0.02,p=0.1p=0.1,γ=0.3\gamma=0.3,μ1=μ2=0.6\mu_{1}=\mu_{2}=0.6; (b) λ1=0.06\lambda_{1}=0.06, λ2=0.04\lambda_{2}=0.04, γ=0.12\gamma=0.12, μ1=μ2=0.6\mu_{1}=\mu_{2}=0.6.
Refer to caption
Figure 4: Effect of initial density of adopters. (a)-(d) Time evolutions for the prevalence are presented under different combinations of transmission parameters. In each figure, a single curve corresponds to one value of different initial densities of adopters. (b) We find that when γ\gamma is relatively large, the initial condition determines the final state of bistable region, either outbreak or extinction. Parameters: μ1=0.6\mu_{1}=0.6, μ2=0.6\mu_{2}=0.6, p=0.1p=0.1. In addition, (a) λ1=0.05\lambda_{1}=0.05, λ2=0.02\lambda_{2}=0.02, γ=0.1\gamma=0.1, (b) λ1=0.05\lambda_{1}=0.05, λ2=0.02\lambda_{2}=0.02, γ=0.3\gamma=0.3, (c) λ1=0.2\lambda_{1}=0.2, λ2=0.02\lambda_{2}=0.02, γ=0.1\gamma=0.1, and (d) λ1=0.05\lambda_{1}=0.05, λ2=0.1\lambda_{2}=0.1, γ=0.1\gamma=0.1.

To begin with, we show prevalence curves as a function of intralayer transmissibility (figure 2(a) and figure 2(b)) and interlayer transmissibility (figure 2(c) and figure 2(d)) under different combinations of multilayer reinforcement and initial density of adopters. All subfigures verify the intuition that multilayer reinforcement promotes social contagion and show that our theoretical predictions agree well with simulation results. The case γ=0\gamma=0 (the red curves) is equivalent to SIS model on multiplex networks , which displays continuous phase transition [41]. Nevertheless, the case γ=0.3\gamma=0.3 (the blue curves) shows large differences in dependence of prevalence on intralayer transmissibility (figure 2(a)) and interlayer transmissibility(figure 2(c)). Phase transition appears at lower value of λ1\lambda_{1} or pp, and becomes discontinuous. Another interesting phenomenon is the emergence of bistable region, where outbreak and extinction states coexist. Specifically, for λ1(0.03,0.08)\lambda_{1}\in(0.03,0.08) in figure 2(a) and p(0,0.12)p\in(0,0.12) in figure 2(c), norms outbreak if ρ0=0.2\rho_{0}=0.2, while go extinct if ρ0=0.03\rho_{0}=0.03. It indicates that the final state in bistable region might depend on the initial density of adopters. Owing to the spontaneous recovery mechanism (μ1\mu_{1} and μ2\mu_{2}), the system would finally reach a dynamic equilibrium. We conduct additional simulations under different μ1\mu_{1} and μ2\mu_{2}, and obtain similar bistable phenomena and discontinuous phase transitions even under weak multilayer reinforcement when μ1\mu_{1} and μ2\mu_{2} are small (see figure 11 in B).

In addition, figure 3 shows the emergence of hysteresis loops of stationary prevalence with respect to changes in intralayer transmissibility and interlayer transmissibility. Here two evolutionary routes can be observed. One is the ascending path (blue squares) describing the stationary prevalence under small initial density of adopters, which corresponds to diffusion processes from few early adopters to global dissemination. For the ascending path, prevalence first remains zero and then rapidly grows to a high level at a large threshold as λ1\lambda_{1} or pp increases. We call the threshold as the diffusion threshold. The other one is the descending path (red triangles) which depicts the final results under large initial density of adopters. It corresponds to the eradication processes that norms transform from a large initial prevalence to a small one. For the descending path, as λ1\lambda_{1} or pp decreases, prevalence remains a high level and would not recover to zero until it mitigates less than a small threshold. We designate the threshold as the eradication threshold. These two paths form hysteresis loops of stationary prevalence, where the diffusion threshold is much larger than the eradication threshold. This indicates that more efforts of reducing transmissibility are required to make the prevalence recover to zero. Our result explains why it is so difficult to eliminate the rumors and misbeliefs from social networks, especially in the modern media environment where different online social platforms interact. Besides, noting the dependence of the system’s final state on its history, we could alter initial density of adopters to realize the mutual transformation of the two evolutionary routes.

To give a more intuitive illustration about how initial density of adopters affects the final state, in figure 4, we further present time evolutions of prevalence for four different combinations of transmission parameters. In each subfigure, a single realization indicates the temporal evolution under a certain value of initial condition (ρ0\rho_{0}), which ranges from 0 to 1 and is represented by different colors. The initial conditions show no influence on the prevalence of norms when γ\gamma is small (γ=0.1\gamma=0.1): either go extinct (figure 4(a)) or outbreak (figure 4(c) and figure 4(d)) no matter what ρ0\rho_{0} is. However, figure 4(b) shows completely different phenomena when γ\gamma is relatively large (γ=0.3\gamma=0.3). There appears a threshold of initial density of adopters (ρ0=0.09\rho_{0}=0.09), below which the prevalence vanishes, while above which the prevalence converges to about 0.3. This indicates that initial density of adopters plays a main role in determining the final state of bistable region. This insight is consistent with empirical studies that critical masses are necessary for initiating social changes, and can not be observed in simple contagion models on multiplex networks [43, 49].

Refer to caption
Figure 5: Conditions of phase transition for bistability. We provide phase diagrams (a) for the joint effects of multilayer reinforcement and intralayer transmissibility and (b) for the joint effects of multilayer reinforcement and interlayer transmissibility. In each subfigure, the phase plane is composed of three regions: outbreak (region 1), bistable where outbreak and extinction states coexist (region 2), extinction (region 3). The separatrixes L1L_{1} and L2L_{2} represent the critical parameters when ρ0\rho_{0} is small and when ρ0=1\rho_{0}=1, and are numerically solved by equation (9) and equation (5). Parameters: (a) λ2=0.02\lambda_{2}=0.02, μ1=0.6\mu_{1}=0.6, μ2=0.6\mu_{2}=0.6, p=0.1p=0.1 and (b) λ1=0.06\lambda_{1}=0.06, λ2=0.04\lambda_{2}=0.04, μ1=0.6\mu_{1}=0.6, μ2=0.6\mu_{2}=0.6.

Note that the emergence of bistable region is an intriguing physical phenomenon arising from multilayer reinforcement. Here, we further explore the detailed conditions of phase transition for bistability. In figure 5, we present phase diagram under different combinations of multilayer reinforcement and intralayer transmissibility (figure 5(a)) or combinations of multilayer reinforcement and interlayer transmissibility. (figure 5(b)). In all subfigures, the phase plane is divided into three regions by two separatrixes (L1L_{1} and L2L_{2}): outbreak, bistable, extinction. The outbreak state means that the prevalence is positive as long as ρ0>0\rho_{0}>0, and the extinction state represents that the prevalence vanishes no matter what ρ0\rho_{0} is. The bistable state means that norms outbreak for large ρ0\rho_{0} while go extinct for small ρ0\rho_{0}. Thus, two separatrixes L1L_{1} and L2L_{2} are critical values of the parameters under very small ρ0\rho_{0} and ρ0=1\rho_{0}=1, which correspond to the diffusion threshold and the eradication threshold of transmissibility, respectively. L1L_{1} and L2L_{2} can be numerically solved by equation (9) and equation (5), respectively. We find that the solution of equation (9) is uncorrelated with multilayer reinforcement (γ\gamma), which is directly reflected by the parallel relationship between L1L_{1} and y-axis. Meanwhile, L2L_{2} is determined by the joint effects of intralayer transmissibility, interlayer transmissibility and multilayer reinforcement. To sum up, region 1 and region 2 highlight two opportunities for outbreak, which are: (i) to own large transmissibilities and (ii) to own large initial density of adopters with strong multilayer reinforcement. These conclusions can be directly applied to many scenarios such as promoting marketing, designing interventions for rumor spreading and establishing new social norms [50, 43]. We also discuss the impacts of system size on the critical value of multilayer reinforcement that leads to bistability, the diffusion threshold of transmissibility as well as the eradication threshold of transmissibility in C. We find that all the critical values first decrease as NN grows when the system is small, and then become stable when NN is large (N>8000N>8000), which also proves the reliability of our large-scale simulations.

Refer to caption
Figure 6: Emergence of unstable manifold in bistable region. The prevalence of multiple equilibriums solved by equation (5) is shown as a function of (a) intralayer transmissibility and (b) interlayer transmissibility for different multilayer reinforcement. For γ=0.3\gamma=0.3 or γ=0.2\gamma=0.2 where bistable region exists, the unstable equilibrium manifold (dashed lines) emerges between the stable equilibrium manifolds (solid lines). Vertical line represents the threshold when the system has no multilayer reinforcement. Parameters: (a) λ2=0.02\lambda_{2}=0.02, p=0.1p=0.1, μ1=μ2=0.6\mu_{1}=\mu_{2}=0.6; (b) λ1=0.06\lambda_{1}=0.06, λ2=0.04\lambda_{2}=0.04, μ1=μ2=0.6\mu_{1}=\mu_{2}=0.6.

Furthermore, we show the existence of unstable equilibrium manifold in bistable region in Figure 6. By solving equation (5), we present the prevalence of multiple equilibriums with respect to changes in intralayer or interlayer transmissibility. Again, our results illustrate that strong multilayer reinforcement can result in the emergence of discontinuous phase transition and bistability. Moreover, we find that the unstable manifold appears between two stable manifolds in bistable region and the prevalence of unstable equilibriums decreases as λ1\lambda_{1} or pp grows.

Refer to caption
Figure 7: Critical density of initial adopters (ρc\rho_{c}) which separates the bistable region into outbreak and extinction. The boxplots present ρc\rho_{c} as a function of (a) intralayer transmissibility, (b) interlayer transmissibility and (c) multilayer reinforcement. Each box contains 30 independent runs. Theoretical predictions are numerically solved by equation (5) and are represented by yellow triangles. Parameters: μ1=0.6\mu_{1}=0.6, μ2=0.6\mu_{2}=0.6. In addition, (a) λ2=0.02\lambda_{2}=0.02, p=0.1p=0.1, γ=0.4\gamma=0.4, (b) λ1=0.06\lambda_{1}=0.06, λ2=0.04\lambda_{2}=0.04, γ=0.3\gamma=0.3, (c) λ1=0.06\lambda_{1}=0.06, λ2=0.04\lambda_{2}=0.04, p=0.1p=0.1.

The bistability phenomenon provides a profound insight that large initial density of adopters could trigger the outbreak even at low values of transmissibility. Here we explore the thresholds of initial conditions (ρc\rho_{c}) under different circumstances, which describe at least how many initial adopters are required for the outbreak of norms in bistable region. In figure 7(a)-(c), we use boxplot to present critical value ρc\rho_{c} as a function of intralayer transmissibility (λ1\lambda_{1}), interlayer transmissibility (pp) and multilayer reinforcement (γ\gamma), respectively. Each box contains 30 independent simulations. We find that the differences among all simulation results in each box are within 0.02, which implies the stability of ρc\rho_{c}. Besides, the critical density of initial adopters (ρc\rho_{c}) decreases as intralayer transmissibility, interlayer transmissibility or multilayer reinforcement increases. Also, our theoretical solutions well predict simulation results. In particular, we notice that all critical values are small (lower than 0.12), which indicates that manipulating initial condition is a powerful and effective way to control social contagions under the existence of multilayer reinforcement.

4.2 Complex social contagion on heterogeneous multiplex networks

Refer to caption
Figure 8: Complex social contagion on heterogeneous multiplex networks. The prevalence is presented as a function of intralayer transmissibility for different combinations of multilayer reinforcement and initial density of adopters on (a) SF-SF multiplex networks, exponent parameters of which are α1=2.7\alpha_{1}=2.7 and α2=2.9\alpha_{2}=2.9, and (b) WS-WS multiplex networks with rewiring probability equal to 0.01. Simulation results are averaged over 30 independent runs, whose standard errors are shown in subplots. Parameters: λ2=0.02\lambda_{2}=0.02, μ1=0.6\mu_{1}=0.6, μ2=0.6\mu_{2}=0.6, p=0.1p=0.1. In addition, γ=0\gamma=0 (red), γ=0.1\gamma=0.1 (yellow), γ=0.3\gamma=0.3 (blue) and ρ0=0.01\rho_{0}=0.01 (square), ρ0=0.3\rho_{0}=0.3 (diamond).

Real-world networks often have power-law degree distribution, i.e, pkkαp_{k}\sim k^{-\alpha}, or small-world characteristics [51, 52]. Studies have revealed that the network structures play an important role in dynamical evolutions [53]. Thus, to mimic real situations, in this section, we examine how our model behaves on multiplex systems composed of two scale-free (SF) networks or two Watts-Strogatz small-world (WS) networks, respectively. All networks have 10000 nodes. The rewiring probability of the two WS networks are both 0.01 and the exponent parameters of the two SF networks are α1=2.7\alpha_{1}=2.7 and α2=2.9\alpha_{2}=2.9.

Figure 8 presents the prevalence as a function of intralayer transmissibility for different values of multilayer reinforcement and initial density of adopters in SF-SF multiplex networks (figure 8(a)) and WS-WS multiplex networks (figure 8(b)). Results show similar phenomena to ER-ER multiplex networks, including promoting effect of multilayer reinforcement and the emergence of bistability when γ\gamma is large (γ=0.3\gamma=0.3).

Refer to caption
Figure 9: Comparison of different strategies for distributing initial seeds. Critical initial density leading to outbreak is presented as a function of intralayer transmissibility when random selection (blue) and target selection (black) are utilized to distribute the initial seeds, respectively. Each box is derived by 30 independent simulations on SF-SF multiplex networks. Parameters: λ2=0.01\lambda_{2}=0.01, p=0.1p=0.1, γ=0.3\gamma=0.3, μ1=μ2=0.6\mu_{1}=\mu_{2}=0.6.

Finally, we explore the influence of strategies for selecting initial seeds on SF-SF multiplex networks. Two strategies are considered: random selection (randomly selecting initial seeds) and target selection (prefer to select those with higher sum of degree as initial seeds). Figure 9 presents the critical density of initial adopters leading to outbreak with respect to changes in intralayer transmissibility when random selection and target selection are adopted, respectively. Results show that a small initial density is enough to result in an outbreak on SF-SF multiplex networks for both strategies. Specifically, the threshold for target selection is much smaller than random selection.

5 Conclusions and Discussions

Complex social contagion describes complicated behavioral evolutions that cannot be characterized by simple contact-contagion models, such as public opinion formation on controversial events, the spread of conspiracies and the establishment of new social norms [54, 55]. These risky or polarized collective behaviors are ubiquitous on various social networks and are largely determined by the high-order interactions regarding to the enhancement effects of multiple exposures, i.e., the social reinforcement [56]. However, it remains unclear how multilayer reinforcement which mimics complex contagion process among multiple social circles influences the final diffusion results.

In this paper, we propose a modified SIS model which incorporates multilayer reinforcement to describe spreading dynamics on multiplex networks. Firstly, we examine how our model behaves on homogeneous multiplex networks. In particular, we stress our efforts on the detailed impact of multilayer reinforcement. A theoretical framework combining pairwise method and mean-field theory is proposed and is verified by large-scale simulations. Interestingly, we find that the multilayer reinforcement induces the emergence of bistability, where extinction and outbreak states coexist. Furthermore, we show that the final state of bistable region is determined by the initial density of adopters whose threshold decreases as intralayer transmissibility, interlayer transmissibility or multilayer reinforcement increases. We also illustrate the hysteresis phenomena where two evolutionary routes occur, known as an ascending path and a descending path, accounting for the phenomenon that rumors are hard to dispel among online social platforms. The detailed conditions of phase transition for bistability are further derived analytically and are shown in phase diagrams. Within the bistable region, we show the existence of unstable manifolds. Results highlight that the chance for the outbreak of social contagion is either to possess large contagion transmissibility or to own large initial density of adopters with strong multilayer reinforcement. Our results are also valid on finite-size heterogeneous multiplex networks.

Our basic yet powerful multilayer reinforcement mechanism reveals the dramatic promoting impacts of complex social contagion on multiplex networks, which indicates the possibility of facilitating spread outbreaks via controlling initial spreaders. These insights are in line with the empirical studies that only large initial density of adopters can successfully initiate social changes [43]. While current results are performed on uncorrelated multiplex networks, further study may extend the framework to partially overlapped multiple networks where edges in different layers are correlated.

This work is supported by Program of National Natural Science Foundation of China Grant No. 11871004, 11922102, and National Key Research and Development Program of China Grant No. 2018AAA0101100.

Appendix A Comparison of Mean-field approximation and simulations

Refer to caption
Figure 10: Comparison of Mean-field approximation and Pairwise approximation as well as simulations. Prevalence is shown (a) against intralayer transmissibility when interlayer interactions are weak and (b) against interlayer transmissibility. Simulation results (blue squares) are averaged over 30 runs, while mean-field approximation (black line) and pairwise approximation (red line) are solved by equation (12) and equation (5), respectively. Parameters: (a) λ2=0.02\lambda_{2}=0.02, p=0.1p=0.1, γ=0.1\gamma=0.1, μ1=μ2=0.6\mu_{1}=\mu_{2}=0.6; (b) λ1=0.06\lambda_{1}=0.06, λ2=0.04\lambda_{2}=0.04, γ=0.1\gamma=0.1, μ1=μ2=0.6\mu_{1}=\mu_{2}=0.6.

Here we consider Mean-field approach to describe the system. Let ρXj(t),(j=1,2)\rho_{X}^{j}(t),(j=1,2) represent the probability that state of node in layer jj is XX. Then we denote θMFj(t)\theta_{MF}^{j}(t) as the probability that ignorant in layer jj is not convinced in intralayer contagion process, which can be written as

θMFj(t)=(1λjρSj(t))kj\theta_{MF}^{j}(t)=(1-\lambda_{j}\rho_{S}^{j}(t))^{\langle k_{j}\rangle} (10)

Next, we denote δMF(t)\delta_{MF}(t) as the probability that ignorant in layer 1 or layer 2 is not affected by multilayer reinforcement. δMF(t)\delta_{MF}(t) can be calculated by

δMF(t)=10.5γ(1(1ρS1(t))k1)(1(1ρS2(t))k2)\delta_{MF}(t)=1-0.5*\gamma*(1-(1-\rho_{S}^{1}(t))^{\langle k_{1}\rangle})*(1-(1-\rho_{S}^{2}(t))^{\langle k_{2}\rangle}) (11)

where (1(1ρSj(t))kj)(1-(1-\rho_{S}^{j}(t))^{\langle k_{j}\rangle}) accounts for the probability that node in layer jj has at least one spreader neighbor.

Thus, the evolutionary equations of our dynamical model can be written as

dρS1dt=μ1ρS1+(1ρS1)(1θMF1(1pρS2)δMF)dρS2dt=μ2ρS2+(1ρS2)(1θMF2(1pρS1)δMF)\eqalign{\frac{d\rho_{S}^{1}}{dt}&=-\mu_{1}\rho_{S}^{1}+(1-\rho_{S}^{1})*(1-\theta_{MF}^{1}(1-p\rho_{S}^{2})\delta_{MF})\\ \frac{d\rho_{S}^{2}}{dt}&=-\mu_{2}\rho_{S}^{2}+(1-\rho_{S}^{2})*(1-\theta_{MF}^{2}(1-p\rho_{S}^{1})\delta_{MF})\\ } (12)

In figure 10, we conduct comparisons of Mean-field approximation and Pairwise approximation as well as simulations. When interlayer interactions are weak, both approximations agree well with simulations (figure 10(a)). Nevertheless, Mean-field approximation would deviate from simulation results when interlayer interactions are strong, while Pairwise approximation is still valid (figure 10(b)). These indicate that considering dynamical correlations of two layers is necessary for an accurate description of the system, especially under strong interlayer interactions.

Appendix B complementary studies for figure 2

Refer to caption
Figure 11: The emergence of bistability under different values of recovery. We set (a) μ1=μ2=0.1\mu_{1}=\mu_{2}=0.1 and (b) μ1=μ2=0.2\mu_{1}=\mu_{2}=0.2, respectively. In each subfigure, the prevalence is shown against intralayer transmissibility under different combinations of multilayer reinforcement and initial density of adopters. Simulation results are averaged over 30 independent runs, whose standard errors are shown in subplots. Parameters: λ2=0.001\lambda_{2}=0.001, p=0.1p=0.1. In addition, γ=0\gamma=0 (red), γ=0.01\gamma=0.01 (yellow), γ=0.1\gamma=0.1 (blue) and ρ0=0.002\rho_{0}=0.002 (square), ρ0=0.1\rho_{0}=0.1 (diamond).

Figure 11 presents the simulation results for different values of spontaneous recovery. In all subfigures, we observe the emergence of bistable phenomena and discontinuous phase transition when multilayer reinforcement is strong (γ=0.1\gamma=0.1). In particular, the case, γ=0.01\gamma=0.01, triggers a small bistable region in figure 11(a), which indicates that even weak multilayer reinforcement could induce bistability on multiplex networks when the value of spontaneous recovery is small.

Appendix C Effect of system size

Refer to caption
Figure 12: Effect of system size. (a) Critical value of multilayer reinforcement (γc\gamma_{c}) inducing bistability is shown with respect to changes in system size. As system size increases, γc\gamma_{c} derived by numerical simulations (blue squares) decreases and finally converges to our theoretical predictions (red line). (b)-(c) Shown are the impacts of system size on the diffusion threshold and the eradication threshold of intralayer transmissibility (λ1\lambda_{1}) and interlayer transmissibility (pp), respectively. In all subplots, simulation results are averaged over 30 independent runs and light blue/red region represents 95% confidence interval. Parameters: k1=6\langle k_{1}\rangle=6, k2=8\langle k_{2}\rangle=8, μ1=μ2=0.6\mu_{1}=\mu_{2}=0.6. In addition, (a) λ1=0.06\lambda_{1}=0.06, λ2=0.02\lambda_{2}=0.02, p=0.1p=0.1; (b) λ2=0.02\lambda_{2}=0.02, p=0.1p=0.1, γ=0.3\gamma=0.3; (c) λ1=0.06\lambda_{1}=0.06, λ2=0.04\lambda_{2}=0.04, γ=0.12\gamma=0.12.

In this section, we first explore how system size affects critical multilayer reinforcement that induces bistability (γc\gamma_{c}) in figure 12(a). When NN is small (N<8000N<8000), γc\gamma_{c} decreases as system size grows. This indicates that small system suppresses the emergence of bistability. When NN is large (N>8000N>8000), γc\gamma_{c} is almost unchanged and is in good agreement with our theoretical prediction. It proves the stability of γc\gamma_{c} and the validity of our theoretical framework when dealing with large-scale systems.

As for the intralayer or interlayer transmissibility, there arise two different thresholds: the diffusion threshold and the eradication threshold. The diffusion threshold is the minimum transmissibility ensuring that few early adopters of rumors could result in global diffusion. The eradication threshold is the maximum transmissibility ensuring that the widespread rumors could be finally eliminated. Here we further study how the diffusion threshold and the eradication threshold change by the system sizes (see figure 12(b)-(c)). When NN is small (N<8000N<8000), both thresholds decrease as the system size increases. When NN is large (N>8000N>8000), both thresholds are almost unchanged. Meanwhile, our theoretical framework well estimates the diffusion threshold as well as the eradication threshold of intralayer and interlayer transmissibility when NN is large.

References

  • [1] Axelrod R 1997 Journal of conflict resolution 41 203–226
  • [2] Del Vicario M, Bessi A, Zollo F, Petroni F, Scala A, Caldarelli G, Stanley H E and Quattrociocchi W 2016 Proceedings of the National Academy of Sciences 113 554–559
  • [3] Stewart A J, Mosleh M, Diakonova M, Arechar A A, Rand D G and Plotkin J B 2019 Nature 573 117–121
  • [4] Zhang Z K, Liu C, Zhan X X, Lu X, Zhang C X and Zhang Y C 2016 Physics Reports 651 1–34
  • [5] Castellano C, Fortunato S and Loreto V 2009 Reviews of modern physics 81 591
  • [6] Pei S and Makse H A 2013 Journal of Statistical Mechanics: Theory and Experiment 2013 P12002
  • [7] Liu L, Wang X, Zheng Y, Fang W, Tang S and Zheng Z 2019 New Journal of Physics
  • [8] Daley D J and Kendall D G 1964 Nature 204 1118–1118
  • [9] Li W, Tang S, Pei S, Yan S, Jiang S, Teng X and Zheng Z 2014 Physica A: Statistical Mechanics and its Applications 397 121–128
  • [10] Vega-Oliveros D A, Da F Costa L and Rodrigues F A 2017 Journal of Statistical Mechanics: Theory and Experiment 2017 023401
  • [11] Wang X, Li W, Liu L, Pei S, Tang S and Zheng Z 2017 Physical Review E 96 032304
  • [12] Moreno Y, Nekovee M and Pacheco A F 2004 Physical Review E 69 066130
  • [13] Centola D 2010 science 329 1194–1197
  • [14] Wang X, Tang S, Zheng Z and Fu F 2020 Physical Review X 10 041042
  • [15] Fu F, Christakis N A and Fowler J H 2017 Scientific reports 7 43634
  • [16] Romero D M, Meeder B and Kleinberg J 2011 Differences in the mechanics of information diffusion across topics: idioms, political hashtags, and complex contagion on twitter Proceedings of the 20th international conference on World wide web pp 695–704
  • [17] Centola D, Eguíluz V M and Macy M W 2007 Physica A: Statistical Mechanics and its Applications 374 449–456
  • [18] McAdam D and Paulsen R 1993 American journal of sociology 99 640–667
  • [19] Hodas N O and Lerman K 2014 Scientific reports 4 4343
  • [20] Aral S and Nicolaides C 2017 Nature communications 8 1–8
  • [21] Granovetter M S 1977 The strength of weak ties Social networks (Elsevier) pp 347–367
  • [22] Melnik S, Ward J A, Gleeson J P and Porter M A 2013 Chaos: An Interdisciplinary Journal of Nonlinear Science 23 013124
  • [23] Watts D J 2002 Proceedings of the National Academy of Sciences 99 5766–5771
  • [24] Centola D and Macy M 2007 American journal of Sociology 113 702–734
  • [25] Zheng M, Lü L, Zhao M et al. 2013 Physical Review E 88 012818
  • [26] Neuhäuser L, Mellor A and Lambiotte R 2020 Physical Review E 101 032310
  • [27] Gross T, D’Lima C J D and Blasius B 2006 Physical review letters 96 208701
  • [28] Iacopini I, Petri G, Barrat A and Latora V 2019 Nature communications 10 1–9
  • [29] Wang W, Liu Q H, Liang J, Hu Y and Zhou T 2019 Physics Reports 820 1–51
  • [30] Chen L, Ghanbarnejad F and Brockmann D 2017 New Journal of Physics 19 103041
  • [31] Soriano-Paños D, Ghanbarnejad F, Meloni S and Gómez-Gardeñes J 2019 Physical Review E 100 062308
  • [32] Sanz J, Xia C Y, Meloni S and Moreno Y 2014 Physical Review X 4 041005
  • [33] Pinotti F, Ghanbarnejad F, Hövel P and Poletto C 2020 Royal Society Open Science 7 190305
  • [34] Bródka P, Musial K and Jankowski J 2020 IEEE Access 8 10316–10341
  • [35] Wu Q and Chen S 2020 Chaos: An Interdisciplinary Journal of Nonlinear Science 30 073115
  • [36] Salehi M, Sharma R, Marzolla M, Magnani M, Siyari P and Montesi D 2015 IEEE Transactions on Network Science and Engineering 2 65–83
  • [37] Soriano-Paños D, Guo Q, Latora V and Gómez-Gardeñes J 2019 Physical Review E 99 062311
  • [38] De Domenico M, Granell C, Porter M A and Arenas A 2016 Nature Physics 12 901–906
  • [39] Bianconi G 2017 Journal of Statistical Mechanics: Theory and Experiment 2017 034001
  • [40] Chen L J, Chen X L, Cai M and Wang W 2018 Physica A: Statistical Mechanics and its Applications 503 516–525
  • [41] Cozzo E, Banos R A, Meloni S and Moreno Y 2013 Physical Review E 88 050801
  • [42] Gomez S, Diaz-Guilera A, Gomez-Gardenes J, Perez-Vicente C J, Moreno Y and Arenas A 2013 Physical review letters 110 028701
  • [43] Centola D, Becker J, Brackbill D and Baronchelli A 2018 Science 360 1116–1119
  • [44] Mønsted B, Sapieżyński P, Ferrara E and Lehmann S 2017 PloS one 12
  • [45] Mahajan V 2010 Wiley International Encyclopedia of Marketing
  • [46] Krapivsky P L, Redner S and Volovik D 2011 Journal of Statistical Mechanics: Theory and Experiment 2011 P12003
  • [47] Li W, Tang S, Fang W, Guo Q, Zhang X and Zheng Z 2015 Physical Review E 92 042810
  • [48] Wang W, Tang M, Stanley H E and Braunstein L A 2018 Physical Review E 98 062320
  • [49] Xie J, Sreenivasan S, Korniss G, Zhang W, Lim C and Szymanski B K 2011 Physical Review E 84 011130
  • [50] Karsai M, Iniguez G, Kaski K and Kertész J 2014 Journal of The Royal Society Interface 11 20140694
  • [51] Barabási A L and Albert R 1999 science 286 509–512
  • [52] Watts D J and Strogatz S H 1998 nature 393 440
  • [53] Moreno Y, Pastor-Satorras R and Vespignani A 2002 The European Physical Journal B-Condensed Matter and Complex Systems 26 521–529
  • [54] Dodds P S and Watts D J 2004 Physical review letters 92 218701
  • [55] Lambiotte R, Rosvall M and Scholtes I 2019 Nature physics 15 313–320
  • [56] Lehmann S and Ahn Y Y 2018 Complex spreading phenomena in social systems (Springer)