Xianli Sun , Linghua Zhang , Qiqing Zhai and Peng ZhengGreen Behavior Diffusion with Positive and Negative Information in Time-varying Multiplex NetworksAbstract: How to comprehend the relationship between information spreading and individual behavior adoption is an essential problem in complex networks. To this end, a novel twolayer model to depict the diffusion of green behavior under the impact of positive and negative information is proposed. Positive information motivates people to adopt green behavior, while negative information reduces the adoption of green behavior. In the model, the physical contact layer describes the green behavior diffusion, and the information layer describes the positive and negative information spreading. Moreover, the social interactions of individuals in two layers change with time and are illustrated by an activity-driven model. Then, we develop the probability transition equations and derive the green behavior threshold. Next, experiments are carried out to confirm the preciseness and theoretical predictions of the new model. It reveals that the prevalence of green behavior can be promoted by restraining the negative information transmission rate and recovery rate of the green nodes while facilitating the positive information transmission rate and green behavior transmission rate. Additionally, reducing the positive information recovery rate and the recovery rate of the green nodes, and increasing the rates of forgetting negative information are beneficial for encouraging the outbreak of green behavior. Furthermore, in the physical contact layer, higher contact capacity and greater activity heterogeneity significantly facilitate green behavior spreading. In the information layer, smaller contact capacity and weaker activity heterogeneity promote diffusion when negative information dominates, whereas larger contact capacity and stronger activity heterogeneity are beneficial when positive information prevails. Keywords: Green behavior diffusion , multiplex network , negative information , positive information , time-varying I. INTRODUCTIONA. Background and MotivationIN the era of global warming, reducing carbon emissions has become an essential issue, capturing worldwide attention [1]. An increasing number of individuals have become conscious of the perilous state of our environment and energy sources, and are strongly advocating green behavior. Green behavior is the activities of individuals or social organizations who embrace the world’s green principles, such as opting for recycling materials, public transportation, efficiently utilizing energy, and safeguarding the species and living environment [2]. Given the critical role that green behavior plays in mitigating environmental degradation, it is essential to understand how these behaviors spread through populations to effectively promote sustainable practices. To understand how green behavior spreads, it is essential to consider the context of complex networks, which are ubiquitous in various systems such as cells, the human brain, ecosystems, and the Internet [3]. Based on the theory of complex networks, researchers can more accurately model the diffusion process, such as information diffusion [4], green behavior diffusion [2], and rumor diffusion [5]. Since green behavior diffusion is often considered to be similar to epidemic diffusion, many researchers simulate the diffusion dynamics of green behavior based on the classical epidemic spreading model [6]. However, real-world systems are frequently associated with each other, complex systems may be made up of several interacting sub-systems [7]. For instance, the power grids frequently rely on the communication systems to transmit the controlling signals, while communication systems typically depend on power grids for their operation [8]. Additionally, offline people persuade their friends to adopt one thing (opinion, product, or service) through word-of-mouth, while online information cascades through social networks can influence offline behavior [9]. As a result, investigating the dynamics and structure on top of multi-layer networks is currently a hot topic in the study of complex systems. As network technology has advanced, online social networks have evolved into a momentous stage for people to communicate, exchange information, and share files [10]. With the growing concern about environmental issues, information related to green behavior propagating through online social networks, may wield considerable influence on the adoption of green behavior [11]. Once individuals acquire information about green behavior from online social networks, they are likely to adopt corresponding green behavior to protect the environment [12]. Actually, plenty of connections among actual individuals take place at different levels and exert mutual effects. Hence, a two-layer network should be considered to depict the dynamic interplay between green behavior spreading and information diffusion [6]. Nowadays, multiplex networks have gained widespread to model the dynamic propagation process among individuals at different layers [13]. In a multiplex network, there are two layers: the information layer and the physical contact layer. These layers interact and influence each other, providing a more comprehensive framework to study the spread of green behavior and the diffusion of information. Even though the previous models properly depict the relationship between information diffusion and green behavior, the spread of green behavior reveals some novel characteristics. Many works focused on the impact of a single type of information on green behavior, for example, all people are likely to receive messages that support green behavior. In practice, individuals may exhibit different attitudes toward green behavior, and individuals’ behavior may display significant heterogeneity [14]. Specifically, when green behaviors propagate in the physical contact layer, some negative information regarding green behavior emerges, which can potentially discourage individuals from adopting green behavior [15]. For example, when it comes to commutes, some people in remote areas contend that car-dependent lifestyles normalize their recreation, work, and residence, and green behavior may reduce the convenience of people’s lives [16]. Moreover, with regard to the purchase of green goods, some people think that the green feature is accompanied by premium pricing which leads to them giving up green goods [17]. In reality, customers will not compromise their requirements or desires for the sake of environmental sustainability. Conversely, in order to reduce carbon emissions and preserve energy, some people actively promote and practice green behavior. Hence, there are typically two forms of information about green behavior that propagate simultaneously on social networks: 1) positive information; and 2) negative information. People can be influenced by different information about green behavior in online social networks to decide whether they adopt green behavior. Therefore, it is imperative to delve into the effect of various information on the dissemination of green behavior. Additionally, many studies focus on the spreading model in static networks. Static connections and interactions are approximations, representing time-aggregated versions of actual interactions [18]. In other words, these models can be characterized as connectivity models, where the connections between individuals are long-lasting elements [19]. This approach completely ignores the time-varying nature of connectivity patterns. Actually, with the prevalence of diverse social networks, interactions among individuals are often rapidly changing and occur within a very short timeframe, such as mobile calls between individuals or the rapid diffusion of information through email [20]. To more accurately understand spreading dynamics in the real world, it is essential to consider the time-dependent interactions between network layers [21]. Therefore, in this paper, we consider the time-varying multiplex networks to describe the dynamic interplay between the information layer and the physical contact layer. B. Main ContributionsFor the sake of getting over the restrictions mentioned above, we develop a new dynamics model called [TeX:] $$U A_1 A_2 U-S G S$$ model, which can precisely depict the process of green behavior propagation. Moreover, we consider time-varying interactions in networks to make the model more grounded in reality. This paper’s main contributions are summarised below. 1) [TeX:] $$U A_1 A_2 U-S G S$$ model: Considering the educational background, the accumulation of knowledge, income, region, etc., individuals have different levels of perceptions, which leads to different attitudes toward green behaviors. Specifically, there exist typically two forms of information about green behavior that propagate in social networks: Positive information and negative information. People can be simultaneously influenced by two types of information about green behavior in online social networks to decide whether they adopt green behavior. Then, we propose the [TeX:] $$U A_1 A_2 U-S G S$$ model for analyzing the interaction between green behavior and information, which utilizes two-layered multiplex networks. 2) Time-varying multiplex networks: Considering interactions among individuals frequently change over time in real-world scenarios, time-varying networks can more accurately capture the fundamental characteristics of complex systems [22]. Thus, we adopt the activity-driven network to describe the physical contact layer and information layer, making both layers time-varying. 3) Green behavior threshold: Predicting the threshold for the propagation of green behavior holds profound significance in safeguarding the environment. Thus, we calculate the green behavior threshold of the [TeX:] $$U A_1 A_2 U-S G S$$ model using the microscopic Markov chain. C. OutlineThe paper is organized as follows. We review the related works in Section II. We develop a novel dynamics model of the green behavior and information propagation in multiplex networks in Section III. In Section IV, we compute the green behavior threshold by the microscopic Markov chain. The extensive simulations are conducted in Section V. Lastly, the conclusions of this paper are clarified in Section VI. II. RELATED WORKA. The Development of Green Behavior ModelThe topic of green sustainable development has grown in prominence as a significant human concern. Understanding the dynamics of how green behavior spreads can significantly enhance the effectiveness of interventions aimed at promoting sustainable practices. In single-layer networks, the green behavior spreading model typically involves analyzing the factors that influence green behavior, such as environmental education [23], energy price [24], environmental activist behavior [25], and transportation [26]. Li et al. [27] combined the game theory with green behavior, and found that people tend to prioritize adopting green behavior when they display a lower activity rate or higher connectivity. Wang et al. [28] investigated the impact of information regarding green attributes and green certification on consumer perceptions. Geng et al. [15] proposed a threecolor theoretical model, exploring motivation and behavior in a two-dimensional context. Kyoi et al. [29] developed a dynamic model in social networks to depict the spread of proenvironmental behaviors and identify promising approaches for supporting them. Moving beyond single-layer networks, researchers have explored the diffusion of green behavior in multiplex networks. Multiplex networks provide a more realistic representation of social systems, capturing the complexity of how individuals interact across various contexts such as family, work, and social circles. The advent of online social networks has witnessed an unparalleled surge in their adoption, profoundly transforming the landscape of interpersonal communication and prompting extensive research into their impacts on offline user behavior [30], such as green behavior [31], voting [32], health behavior [33], and epidemic spreading [34]. Therefore, many studies focused on the coupled diffusion of information on online social networks and green behavior in the physical contact layer. Gao et al. [35] investigated green behavior and knowledge propagation in multiplex networks and found that government policies are critical to green behavior diffusion. According to the Microscopic Markov Chain Approach, Li et al. [11] investigated the influence of information propagation on green behavior spreading in multiplex networks. Li et al. [31] investigated the effects of negative information diffusion on green behaviors employing the HGBS model. Yin et al. [2] developed a dynamic model to depict that green behavior spreading is not only related to green information but also influenced by changes in social relationships. B. The Development of the Time-varying Multiplex NetworksTemporal networks allow information and green behavior propagation along links only when they exist in time, and this leads to considerable influences on propagation efficiency [36]. Currently, the activity-driven model is one of the main timedependent systems, which highlights the structure’s response to its dynamics. The activity-driven model is simple in its basic form and produces a nontrivial temporal structure that affects how dynamical processes develop [37]. Due to its simplicity, the initial activity-driven model is unable to reproduce some common characteristics of social networks, such as memory effects, and assortative mixing [38]. Thanks to these reasons, modifications to the initial model have been implemented and investigated [39]. Chai et al. [40] introduced activity-driven networks to characterize realistic temporal networks, and the node-based SIRS model was used to depict the dissemination dynamics from a microcosmic aspect. Pozzana et al. [41] studied SIS spreading processes using a recently developed extension of the activity-driven modeling framework. Based on the activity-driven model, scholars have extended their work to multiplex networks. Guo et al. [42] considered that the layer of information is an activity-driven network, whereas the layer of physical contact is a static network. Li et al. [43] regarded information spreading network as a static network, while physical contact network is time-varying. Yang et al. [18] depicted information and epidemic diffusion in an activity-driven multiplex network. Huang et al. [44] analyzed the dynamic model of epidemic propagation and resource dissemination in time-varying multiplex networks. Unfortunately, research on green behavior in time-varying multiplex networks is scarce. Therefore, we focus on the diffusion of green behavior in time-varying multiplex networks. III. COUPLED DYNAMIC MODEL OF INFORMATION SPREADING AND GREEN BEHAVIOR DIFFUSIONA. Time-varying Multiplex NetworksGiven that human behavior is generally transmitted through face-to-face interactions, those who live or work in close proximity often have a substantial influence on your behavior. Thus, green behavior propagates through a physical contact network, wherein the connections represent relationships with individuals you encounter daily, such as colleagues, neighbors, and family members. Moreover, messages about green behavior diffuse through an information network, where the connections represent relationships with individuals with whom you share information. Once individuals acquire information about green behavior from an information network, they are likely to adopt corresponding green behavior to protect the environment. Therefore, in addition to regular physical contact, this network should also encompass connections established through digital communication channels [11]. To depict the dynamic interaction between the dissemination of green behavior and information, two-layered multiplex networks are utilized. The lower layer is the physical contact network P, illustrating the spread of green behavior, while the upper layer is the information network V, such as Facebook or WeChat, focusing on the dissemination of information related to green behavior. Specifically, in two-layered networks, the mapping relation between associated individuals is one-toone, which means each individual exists concurrently in the information layer and the physical contact layer [45]. Additionally, each edge in the two-layered network is assumed to be unweighted and undirected. We employ the activity-driven model to create each layer of the networks. Fig. 1 displays the procedures involved in building the time-varying multiplex network. The network consists of N nodes, each with a fixed activity level that determines the chance of the node being activated and establishing new connections with other nodes. Specifically, in the information layer V, the activity level of the node i is [TeX:] $$a_i=\eta_v x_i,$$ and in the physical contact layer P is [TeX:] $$b_i=\eta_p y_i.$$ Parameters of [TeX:] $$x_i \text{ and } y_i$$ represent the activity potentials following power-law distributions [TeX:] $$F_v(x) \propto x^{-\gamma_v} \text { and } F_p(x) \propto y^{-\gamma_p},$$ respectively [46]. Parameters of [TeX:] $$\eta_v \text{ and } \eta_p$$ are the rescaling factors. Moreover, parameters of [TeX:] $$\gamma_v \text { and } \gamma_p$$ refer to activity exponents of the upper and lower layers, respectively [47]. Definition 1: (Activity-driven network) Based on the configurations, the generative steps of the activity-driven network (ADN) are as follows. · At time t, each layer is comprised of N nodes that are separated from each other, and there exists a one-to-one relationship between nodes in two layers. · The node i becomes active with a probability of [TeX:] $$a_i \Delta t(b_i \Delta t),$$ and produces [TeX:] $$m_v\left(m_p\right)$$ connections to other nodes that are chosen at random. · At the next time step [TeX:] $$t+\Delta t$$, we remove all connections and repeat the first and second phases until the diffusion reaches a stationary state or is terminated in both layers. B. The Description of the [TeX:] $$U A_1 A_2 U-S G S$$ ModelIn the upper layer, the [TeX:] $$U A_1 A_2 U$$ model is proposed to depict the green information diffusion. Nodes in this layer are divided into three groups: U (unaware of green information); [TeX:] $$A_1$$ (aware of positive green information); and [TeX:] $$A_2$$ (aware of negative green information). People in state [TeX:] $$A_1$$ receive positive messages and agree on the importance of green behavior which contributes to adopting green behavior. Yet, people in state [TeX:] $$A_2$$ receiving negative information, such as the inconvenience of transport [15], and relatively high expenses of green consumption [48], are not conducive to adopting green behavior. People in states [TeX:] $$A_1 \text{ and } A_2$$ will spread information about the positive and negative information of green behavior to their neighbors in multiplex networks, respectively. In addition, individuals have not received any information on green behavior in the state U, but can get it by communicating with aware neighbors. In the lower layer, the SGS green behavior model is employed to represent the green behavior diffusion. Then, individuals are divided into two groups: 1) S (susceptible) and 2) G (green). On the one hand, the green node encourages the susceptible individuals to follow the green behavior, and on the other hand, they can abandon the green behavior due to price, income, or other reasons and return to the S state. Susceptible nodes have the potential to adopt the green behavior by contacting a green individual. Based on the coupling of information diffusion and green behavior propagation, there exist six states: US, UG, [TeX:] $$A_1 S, A_1 G, A_2 S, \text { and } A_2 G .$$ Moreover, once individuals are in the green state, they must be aware of the information about green behavior and thus UG cannot be included in the model. Additionally, if nodes are in the green state, they will transmit positive information to encourage neighbors to follow green behavior, and thus [TeX:] $$A_2 G$$ is excluded from the model. Therefore, we only consider four potential states in multiplex networks: 1) [TeX:] $$A_1 S$$ (who is susceptible and aware of positive information); 2) [TeX:] $$A_2 S$$ (who is susceptible and aware of negative information); 3) US (who is susceptible and unaware of any information); and 4) [TeX:] $$A_1 G$$ (who is green and aware of positive information). Additionally, we assume that if an individual accepts a specific type of information, they are unlikely to accept any other information. Fig. 2 displays the diagram of the potential state transition for the [TeX:] $$U A_1 A_2 U-S G S$$ model. According to the above description of different states, the propagation rules for the [TeX:] $$U A_1 A_2 U-S G S$$ model can be summarized as follows. · The US nodes will receive the corresponding information disseminated by the spreaders of positive or negative information at rates [TeX:] $$\lambda_1 \text { and } \lambda_2,$$ respectively. · Nodes in states [TeX:] $$A_1 S \text{ or } A_2 S$$ may return to the state US because of forgetting or losing interest in the green information at the recovery rate [TeX:] $$\delta_1 \text { and } \delta_2,$$ respectively. Furthermore, green nodes do not forget the positive information about green behavior before they give up practicing green behavior. · When susceptible nodes come into contact with green nodes, their behaviors receive the influence of a green neighbor and are infected to be green nodes. The green nodes can propagate green behavior to their susceptible neighbors with probability β. · Besides, green nodes will also give up practicing green behavior with a recovery rate μ. Parameters [TeX:] $$\gamma_1 \text { and } \gamma_2\left(1 \leq \gamma_1 \leq 1 / \beta^U, 0 \leq \gamma_2 \leq 1\right)$$ are used to control the impact of positive nodes and negative nodes in the information layer on the physical contact layer, respectively. Compared with unaware nodes, aware nodes whose state is [TeX:] $$A_1 S$$ are more inclined to act in an ecologically beneficial way, and nodes whose state is [TeX:] $$A_2 S$$ are skeptical of green behavior [49]. Thus, we use [TeX:] $$\gamma_1 \text { and } \gamma_2$$ to distinguish the adoption rate among [TeX:] $$A_1 S, A_2 S$$ and US nodes. If an individual is in the state of US, its adoption rate of green behavior is [TeX:] $$\beta^U,$$ while adoption rates of [TeX:] $$A_1 S \text { and } A_2 S$$ nodes are represented by [TeX:] $$\beta^{A_1}=\gamma_1 \beta^U \text { and } \beta^{A_2}=\gamma_2 \beta^U .$$ When the values of [TeX:] $$\gamma_1 \text { and } \gamma_2$$ are bigger, the nodes are more likely to practice green behavior. In particular, when [TeX:] $$\gamma_1=1 \text { and } \gamma_2=1,$$ interactions between two layers disappear, and the configuration is equal to executing the dynamic diffusion in the single-layer network. IV. THEORETICAL ANALYSIS BASED ON THE MICROSCOPIC MARKOV CHAIN APPROACHBased on the microscopic Markov chain (MMC) approach [50], the green behavior threshold [TeX:] $$\beta_c$$ is derived. In our model, there exist four possible states: 1) [TeX:] $$A_1 S$$; 2) [TeX:] $$A_2 S$$; 3) US; and 4) [TeX:] $$A_1 G$$. At time t, the possibility that a node i is in each of the four states can be defined as [TeX:] $$P_i^{A_1 S}(t), P_i^{A_2 S}(t), P_i^{US}(t), \text{ and } P_i^{A_1 G}(t)$$ respectively. Moreover, the normalized condition [TeX:] $$P_i^{A_1 S}(t)+P_i^{A_2 S}(t)+P_i^{A_1 G}(t)+P_i^{US}(t)=1$$ should be satisfied. The notations of all symbols are shown in Table I. TABLE I
In the upper layer, at time t, the probability of the node i is not informed of positive or negative information by [TeX:] $$r_i^{A_1}(t)$$ and [TeX:] $$r_i^{A_2}(t)$$, respectively. Additionally, if the node is not informed of the positive or negative information, at the time step t, the possibility that the node will not affected by neighbors is defined as [TeX:] $$q_i^U(t)$$. Similarly, the possibility that the node i in the physical layer in [TeX:] $$A_1 \text{ or } A_2$$ is not affected by its green neighbors is expressed as [TeX:] $$q_i^{A_1}(t) \text { and } q_i^{A_2}(t),$$ respectively. The expressions of [TeX:] $$r_i^{A_1}(t) \text { and } r_i^{A_2}(t)$$ are described as follows:
(1)[TeX:] $$r_i^{A_1}(t)=\prod_j\left[1-\lambda_1 \frac{m_v}{N} P_j^{A_1}(t)\left(a_i+a_j\right)\right],$$
(2)[TeX:] $$r_i^{A_2}(t)=\prod_j\left[1-\lambda_2 \frac{m_v}{N} P_j^{A_2}(t)\left(a_i+a_j\right)\right],$$where [TeX:] $$P_j^{A_1}(t)=P_j^{A_1 S}(t)+P_j^{A_1 G}(t)$$ and [TeX:] $$P_j^{A_2}(t)=P_j^{A_2 S}(t).$$ According to the theory of the activity-driven model [21], the expression for [TeX:] $$m_v P_j^{A_1}(t)\left(a_i+a_j\right) / N$$ is the possibility that i and j in the information layer are neighbors, where the first part [TeX:] $$m_v a_i P_j^{A_1}(t) / N$$ represents the active node i that establishes a connection with node j that is in the state [TeX:] $$A_1$$ and the other part [TeX:] $$m_v a_j P_j^{A_1}(t) / N$$ represents the individual i receiving a connection from the active individual j in the state [TeX:] $$A_1$$. The expression for [TeX:] $$m_v P_j^{A_2}(t)\left(a_i+a_j\right) / N$$ represents the possibility that the node i and j in the state [TeX:] $$A_2$$ are neighbors in the information layer. Similarly, the expressions of [TeX:] $$q_i^U(t), q_i^{A_1}(t), \text { and } q_i^{A_2}(t)$$ are described as follows:
(3)[TeX:] $$q_i^{A_1}(t)=\prod_j\left[1-\beta^{A_1} \frac{m_p}{N} P_j^{A_1 G}(t)\left(b_i+b_j\right)\right],$$
(4)[TeX:] $$q_i^{A_2}(t)=\prod_j\left[1-\beta^{A_2} \frac{m_p}{N} P_j^{A_1 G}(t)\left(b_i+b_j\right)\right],$$
(5)[TeX:] $$q_i^{U}(t)=\prod_j\left[1-\beta^{U} \frac{m_p}{N} P_j^{A_1 G}(t)\left(b_i+b_j\right)\right],$$where [TeX:] $$m_p P_j^{A_1 G}(t)\left(b_i+b_j\right) / N$$ is the possibility that i and j in the physical contact layer which is in the [TeX:] $$A_1 G$$ state are neighbors. Based on the above definitions, Fig. 3 shows the probability trees of different states in multiplex networks. The features of the asymmetrically interacting diffusion dynamics in time-varying multiplex networks suggest that the microscopic Markov chain approach should be employed for theoretical analysis and prediction. According to (1)–(5) and the probability trees in Fig. 3, the transition equations for different states can be developed by utilizing MMC [51] in (6), where [TeX:] $$P_i^{U S}(t+1), P_i^{A_1 S}(t+1), P_i^{A_2 S}(t+1), \text{ and } P_i^{A_1 G}(t+1)$$ denote the possibility that the node i will be in the state of US, [TeX:] $$A_1 S, A_2 S, \text{ and } A_1 G$$ at the following time step. The system will obtain the stationary solution when t → ∞, and satisfying the following relations.
(6)[TeX:] $$\begin{aligned} P_i^{U S}(t+1)= & P_i^{A_1 S}(t) \delta_1 q_i^U(t)+P_i^{A_2 S}(t) \delta_2 q_i^U(t)+P_i^{A_1 G}(t) \delta_1 \mu+P_i^{U S}(t) r_i^{A_1}(t) r_i^{A_2}(t) q_i^U(t) \\ P_i^{A_1 G}(t+1)= & P_i^{A_1 S}(t)\left\{\delta_1\left[1-q_i^U(t)\right]+\left(1-\delta_1\right)\left[1-q_i^{A_1}(t)\right]\right\}+P_i^{A_1 G}(t)(1-\mu)+P_i^{U S}(t)\left\{r_i^{A_1}(t) r_i^{A_2}(t)\right. \\ & {\left.\left[1-q_i^U(t)\right]+\left[1-r_i^{A_1}(t)-\left(1-r_i^{A_1}(t)\right)\left(1-r_i^{A_2}(t)\right)\right]\left[1-q_i^{A_1}(t)\right]+\left[1-r_i^{A_2}(t)\right]\left[1-q_i^{A_2}(t)\right]\right\} } \\ & +P_i^{A_2 S}(t)\left\{\delta_2\left[1-q_i^U(t)\right]+\left(1-\delta_2\right)\left[1-q_i^{A_2}(t)\right]\right\} \\ P_i^{A_1 S}(t+1)= & P_i^{A_1 S}(t)\left(1-\delta_1\right) q_i^{A_1}(t)+P_i^{U S}(t)\left[1-r_i^{A_1}(t)-\left(1-r_i^{A_1}(t)\right)\left(1-r_i^{A_2}(t)\right)\right] q_i^{A_1}(t) \\ & +P_i^{A_1 G}(t)\left(1-\delta_1\right) \mu \\ P_i^{A_2 S}(t+1)= & P_i^{A_2 S}(t)\left(1-\delta_2\right) q_i^{A_2}(t)+P_i^{U S}(t)\left[1-r_i^{A_2}(t)\right] q_i^{A_2}(t) \end{aligned}$$
(7)[TeX:] $$\begin{aligned} P_i^{U S}(t+1) & =P_i^{U S}(t)=P_i^{U S}, \\ P_i^{A_1 S}(t+1) & =P_i^{A_1 S}(t)=P_i^{A_1 S}, \\ P_i^{A_2 S}(t+1) & =P_i^{A_2 S}(t)=P_i^{A_2 S}, \\ P_i^{A_1 G}(t+1) & =P_i^{A_1 G}(t)=P_i^{A_1 G}, \end{aligned}$$where [TeX:] $$P_i^{U S}, P_i^{A_1 S}, P_i^{A_2 S} \text {, and } P_i^{A_1 G}$$ stand for the proportions of nodes in US, [TeX:] $$A_1 S, A_2 S \text {, and } A_1 G$$ at the steady state. Identifying the extent to which green behavior can be widely adopted is significant. Then, we analyze the green behavior threshold [TeX:] $$\beta_c.$$ If [TeX:] $$\beta^U \gt \beta_c,$$ the green behavior begins to break out, while [TeX:] $$\beta^U \lt \beta_c,$$ a large proportion of the people do not embrace green behavior. Hence, the proportion of green nodes is near 0 when [TeX:] $$\beta^U$$ is close to [TeX:] $$\beta_c$$ at the steady state, and we can assume that [TeX:] $$P_i^{A_1 G}=\epsilon_i \ll 1 .$$ According to (3)–(5), the higher-order terms can be disregarded, yielding the following approximation.
(8)[TeX:] $$\begin{aligned} q_i^{A_1}(t) & \approx 1-\beta^{A_1} m_p\left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right), \\ q_i^{A_2}(t) & \approx 1-\beta^{A_2} m_p\left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right), \\ q_i^U(t) & \approx 1-\beta^U m_p\left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right), \end{aligned}$$where [TeX:] $$\rho^{A_1 G}=\sum_j P_j^{A_1 G}(t) / N, \text { and } \theta_b^{A_1 G}=\sum_j b_j P_j^{A_1 G} / N .$$ For simplicity, we can define that [TeX:] $$\alpha_i^{A_1}=\beta^{A_1} m_p\left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right),$$ [TeX:] $$\alpha_i^{A_2}=\beta^{A_2} m_p\left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right),$$ and [TeX:] $$\alpha_i^U=\beta^U m_p\left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right) .$$ As a result, the expression of (6) can be converted into the subsequent form:
(9)[TeX:] $$\begin{aligned} P_i^{U S}= & P_i^{A_1 S} \delta_1\left(1-\alpha_i^U\right)+P_i^{A_2 S} \delta_2\left(1-\alpha_i^U\right) \\ & +P_i^{A_1 G} \delta_1 \mu+P_i^{U S} r_i^{A_1} r_i^{A_2}\left(1-\alpha_i^U\right), \\ P_i^{A_1 G}= & P_i^{A_1 S}\left[\delta_1 \alpha_i^U+\left(1-\delta_1\right) \alpha_i^{A_1}\right]+P_i^{A_2 S}\left[\delta_2 \alpha_i^U\right. \\ & \left.+\left(1-\delta_2\right) \alpha_i^{A_2}\right]+P_i^{U S}\left[\left(1-r_i^{A_1}\right) r_i^{A_2} \alpha_i^{A_1}\right. \\ & \left.+r_i^{A_1} r_i^{A_2} \alpha_i^U+\left(1-r_i^{A_2}\right) \alpha_i^{A_2}\right]+P_i^{A_1 G}(1-\mu), \\ P_i^{A_1 S}= & P_i^{A_1 S}\left(1-\delta_1\right)\left(1-\alpha_i^{A_1}\right)+P_i^{A_1 G}\left(1-\delta_1\right) \mu \\ & +P_i^{U S}\left(r_i^{A_2}-r_i^{A_1} r_i^{A_2}\right)\left(1-\alpha_i^{A_1}\right), \\ P_i^{A_2 S}= & P_i^{A_2 S}\left(1-\delta_2\right)\left(1-\alpha_i^{A_2}\right)+P_i^{U S}\left(1-r_i^{A_2}\right) \\ & \left(1-\alpha_i^{A_2}\right) . \end{aligned}$$Next, the higher-order components of (9) can be ignored to further simplify the equation.
(10)[TeX:] $$\begin{aligned} P_i^{U S}= & P_i^{A_1 S} \delta_1+P_i^{A_2 S} \delta_2+P_i^{U S} r_i^{A_1} r_i^{A_2}, \\ P_i^{A_1 S}= & P_i^{A_1 S}\left(1-\delta_1\right)+P_i^{U S}\left(r_i^{A_2}-r_i^{A_1} r_i^{A_2}\right), \\ P_i^{A_2 S}= & P_i^{A_2 S}\left(1-\delta_2\right)+P_i^{U S}\left(1-r_i^{A_2}\right), \\ P_i^{A_1 G}= & P_i^{A_1 S}\left[\delta_1 \alpha_i^U+\left(1-\delta_1\right) \alpha_i^{A_1}\right]+P_i^{A_2 S}\left[\delta_2 \alpha_i^U\right. \\ & \left.+\left(1-\delta_2\right) \alpha_i^{A_2}\right]+P_i^{U S}\left[\left(1-r_i^{A_1}\right) r_i^{A_2} \alpha_i^{A_1}\right. \\ & \left.+r_i^{A_1} r_i^{A_2} \alpha_i^U+\left(1-r_i^{A_2}\right) \alpha_i^{A_2}\right]+P_i^{A_1 G}(1-\mu) . \end{aligned}$$Based on the first three equations in (10), the last equation in (10) can be simplified.
(11)[TeX:] $$\begin{aligned} \mu P_i^{A_1 G}= & \beta^U m_p\left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right) P_i^{U S}+\beta^{A_1} m_p \\ & \left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right) P_i^{A_1 S}+\beta^{A_2} m_p\left(b_i \rho^{A_1 G}\right. \\ & \left.+\theta_b^{A_1 G}\right) P_i^{A_2 S} \\ = & \beta m_p\left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right)\left(P_i^{U S}+P_i^{A_1 S} \gamma_1\right. \\ & \left.+P_i^{A_2 S} \gamma_2\right) . \end{aligned}$$Next, (11) can be simplified as:
(12)[TeX:] $$\begin{aligned} \mu P_i^{A_1 G}= & \beta^U m_p\left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right) P_i^{U S}+\beta^{A_1} m_p \\ & \left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right) P_i^{A_1 S}+\beta^{A_2} m_p\left(b_i \rho^{A_1 G}\right. \\ & \left.+\theta_b^{A_1 G}\right) P_i^{A_2 S} \\ = & \beta m_p\left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right)\left(P_i^{U S}+P_i^{A_1 S} \gamma_1\right. \\ & \left.+P_i^{A_2 S} \gamma_2\right) . \end{aligned}$$Meanwhile, the system reaches a steady state when [TeX:] $$P_i^{A_1 S}+P_i^{A_1 G}=P_i^{A_1} \text {, and } P_i^{A_2 S}=P_i^{A_2} .$$ Given that the proportion of green nodes can be negligible when the value of β is close to [TeX:] $$\beta_c$$ at the steady state, we can obtain [TeX:] $$P_i^{A_1 S}+P_i^{A_2 S} \approx P_i^{A_1}+P_i^{A_2},$$ and [TeX:] $$P_i^{U S}=1-P_i^{A_1 S}-P_i^{A_2 S} \approx 1-P_i^{A_2}-P_i^{A_1} .$$ Hence, in accordance with (12), we obtain the following equation:
(13)[TeX:] $$\begin{aligned} \mu P_i^{A_1 G}= & \left(1-P_i^{A_2}-P_i^{A_1}+P_i^{A_1 S} \gamma_1+P_i^{A_2 S} \gamma_2\right) \\ & \beta m_p\left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right) \\ = & \left(1-P_i^{A_2}-P_i^{A_1}+P_i^{A_1} \gamma_1+P_i^{A_2} \gamma_2\right) \\ & \beta m_p\left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right) \\ = & {\left[1-\left(1-\gamma_1\right) P_i^{A_1}-\left(\left(1-\gamma_2\right) P_i^{A_2}\right)\right] } \\ & \beta m_p\left(b_i \rho^{A_1 G}+\theta_b^{A_1 G}\right) . \end{aligned}$$Next, (13) can be further expressed as:
(14)[TeX:] $$\begin{aligned} \mu P_i^{A_1 G}= & \beta m_p\left[b_i \rho^{A_1 G}-\left(1-\gamma_1\right) b_i \rho^{A_1 G} P_i^{A_1}-\right. \\ & \left(1-\gamma_2\right) b_i \rho^{A_1 G} P_i^{A_2}+\theta_b^{A_1 G}-\left(1-\gamma_1\right) P_i^{A_1} \\ & \left.\theta_b^{A_1 G}-\left(1-\gamma_2\right) P_i^{A_2} \theta_b^{A_1 G}\right] . \end{aligned}$$To obtain the proportion of the green node, we can take the average over all nodes, and obtain the next equation:
Combining (14) and (15), we get:
(16)[TeX:] $$\begin{aligned} \mu \rho^{A_1 G}= & \beta m_p\left\{\rho^{A_1 G}\left[\langle b\rangle-\left(1-\gamma_1\right) \theta_b^{A_1}-\left(1-\gamma_2\right) \theta_b^{A_2}\right]\right. \\ & \left.+\theta_b^{A_1 G}\left[1-\left(1-\gamma_1\right) \rho^{A_1}-\left(1-\gamma_2\right) \rho^{A_2}\right]\right\}, \end{aligned}$$where [TeX:] $$\theta_b^{A_2}=\sum_j b_j P_j^{A_2} / N, \text { and } \rho^{A_1}=\sum_i P_i^{A_1} / N .$$ To obtain a closed expression of [TeX:] $$\theta_b^{A_1 G},$$ we multiply [TeX:] $$b_i$$ on two sides of (14) and calculate the average across all nodes.
(17)[TeX:] $$\begin{aligned} \mu \theta_b^{A_1 G}= & \beta m_p\left\{\rho^{A_1 G}\left[\left\langle b^2\right\rangle-\left(1-\gamma_1\right) \theta_{b^2}^{A_1}-\left(1-\gamma_2\right) \theta_{b^2}^{A_2}\right]\right. \\ & \left.+\theta_b^{A_1 G}\left[\langle b\rangle-\left(1-\gamma_1\right) \theta_b^{A_1}-\left(1-\gamma_2\right) \theta_b^{A_2}\right]\right\}, \end{aligned}$$where [TeX:] $$\theta_{b^2}^{A_2}=\sum_j b_j{ }^2 P_j^{A_2} / N.$$ The expressions of (16) and (17) can be as a matrix as follows:
(18)[TeX:] $$H\left[\begin{array}{l} \rho^{A_1 G} \\ \theta_b^{A_1 G} \end{array}\right]=\frac{\mu}{\beta m_p}\left[\begin{array}{l} \rho^{A_1 G} \\ \theta_b^{A_1 G} \end{array}\right] .$$The expression for H is shown in (19) at the bottom of this page.
(19)[TeX:] $$H=\left[\begin{array}{cc} \langle b\rangle-\left(1-\gamma_1\right) \theta_b^{A_1}-\left(1-\gamma_2\right) \theta_b^{A_2} & 1-\left(1-\gamma_1\right) \rho^{A_1}-\left(1-\gamma_2\right) \rho^{A_2} \\ \left\langle b^2\right\rangle-\left(1-\gamma_1\right) \theta_{b^2}^{A_1}-\left(1-\gamma_2\right) \theta_{b^2}^{A_2} & \langle b\rangle-\left(1-\gamma_1\right) \theta_b^{A_1}-\left(1-\gamma_2\right) \theta_b^{A_2} \end{array}\right] .$$As the green behavior begins to spread throughout the network at the steady state, the minimum value of [TeX:] $$\beta \text { is } \beta_c$$ which satisfies (18) with [TeX:] $$\left[\begin{array}{c} \rho^{A_1 G} \\ \theta_b^{A_1 G} \end{array}\right] \neq 0$$[42]. Moreover, the value of f [TeX:] $$\mu /\left(\beta_c m_p\right)$$ is equivalent to the biggest eigenvalue of the matrix H. Then the biggest eigenvalue is: [TeX:] $$\Lambda_{\max }(H)=\sqrt{x}+\langle b\rangle-\left(1-\gamma_1\right) \theta_b^{A_1}-\left(1-\gamma_2\right) \theta_b^{A_2},$$ where [TeX:] $$x=\left[1-\left(1-\gamma_1\right) \rho^{A_1}-\left(1-\gamma_2\right) \rho^{A_2}\right]\left[\left\langle b^2\right\rangle-\right.\left.\left(1-\gamma_1\right) \theta_{b^2}^{A_1}-\left(1-\gamma_2\right) \theta_{b^2}^{A_2}\right].$$ As a result, we can get:
(20)[TeX:] $$\begin{aligned} \beta_c & =\frac{\mu}{m_p \Lambda_{\max }(H)} \\ & =\frac{\mu}{m_p}\left[\sqrt{x}+\langle b\rangle-\left(1-\gamma_1\right) \theta_b^{A_1}-\left(1-\gamma_2\right) \theta_b^{A_2}\right]^{-1} . \end{aligned}$$It is evident from (20) that the green behavior threshold is associated with the spread of two kinds of information. Additionally, the green behavior threshold of the proposed model is influenced by the parameter [TeX:] $$\gamma_1 \text { and } \gamma_2,$$ the recovery probability μ, and the physical network’s topological structure. V. NUMERICAL SIMULATIONSSeveral simulations are performed in this section to validate the proposed model, coupling green behavior diffusion and information spreading. Firstly, we describe the variation of each node over time in synthetic networks and real-world networks. Secondly, the impact of various parameters in the upper and lower networks on green behavior spreading is investigated. Thirdly, the effect of relevant parameters on green behavior thresholds is analyzed. Fourthly, the influence of time-varying properties on the spread of green behavior is examined. For the synthetic network, we construct the multiplex networks with 1,000 nodes by activity-driven model. Referring to [53] and [54], we set the activity exponent of different layers as [TeX:] $$\gamma_p=\gamma_v=2.1,$$ the number of connections that active nodes have produced as [TeX:] $$m_v=m_p=5,$$ and the rescaling factors as [TeX:] $$\eta_v=\eta_p=1.$$ It should be noted that unless certain parameters are chosen as variables, their values remain constant. For the sake of verifying the practicality of the [TeX:] $$U A_1 A_2 U-S G S$$ model, we carry out some simulations on real-world time-varying multiplex networks. We supply the experiments of model propagation on Social Evolution Dataset, which is conducted by the MIT Media Lab [55]. The Social Evolution experiment tracked the everyday life of a whole undergraduate dormitory with mobile phones from October 2008 to May 2009. The data set is represented by a temporal duplex network, constituted by two different layers: A physical layer, formed by face-to-face interactions, and a digital layer built by sharing all tagged Facebook photos, or sharing blog/ live journal/ Twitter activities. Subsequently, we divide the period into independent intervals, extract subgraphs for each raw dataset, and generate four corresponding activity-driven networks. Similar to the method in [53], we measure the activity rate of each node as the number of interactions it performs in a given time interval, divided by the maximum number of interactions performed by all nodes during the same time interval. A. The Trend of Change at Different NodesTo more accurately depict the diffusion of green behavior and the correspondent information, we designate the evolution of green behavior and information diffusion over time in both synthetic networks and real-world networks. Specially, [TeX:] $$\rho^{A_1 G}$$ stands for the percentage of green individuals in the lower layer at the steady state. [TeX:] $$\rho^{U S}$$ stands for the percentage of susceptible individuals who are unaware of the green information at the steady state. [TeX:] $$\rho^{A_1 S} \text { and } \rho^{A_2 S}$$ indicate the proportions of susceptible nodes that are aware of positive and negative green information at the steady state. In each experiment, the initial values of [TeX:] $$\rho^{A_1 G}, \rho^{A_1 S}, \rho^{A_2 S}, \text { and } \rho^{U S}$$ are 0.1, 0, 0.1, and 0.98. According to the processes outlined in Fig. 1 and Fig. 3, we progress the interaction dynamics in the information and physical contact layers. 1) Synthetic networks: Fig. 4 illustrates the evolution of green behavior and information diffusion in synthetic timevarying multiplex networks, with three subplots (a, b, c) representing different parameter settings. In the above three cases, the green nodes increase rapidly, stabilizing at a significant proportion over time. The node that is susceptible and unaware of any information decreases correspondingly, indicating successful diffusion of green behavior. Individuals who are susceptible and aware of positive information initially increase and then stabilize, while [TeX:] $$A_2 S$$ nodes increase and then decrease to 0. Comparing Figs. 4(a), 4(b), and 4(c), the density of green individuals surges in the early stages until it peaks, with the peak value being higher for larger [TeX:] $$\gamma_1 \text { and } \gamma_2$$. This demonstrates that increasing [TeX:] $$\gamma_1 \text { and } \gamma_2$$ enhances the overall 2) Real-world networks: Fig. 5 illustrates the evolution of green behavior and information diffusion in real-world networks. Comparing Fig. 4 with Fig. 5, the results of the real and synthetic data are consistent: the trend of the individual nodes is the same. In the above three cases, the green behavior nodes increase rapidly, reaching a stable proportion as time progresses. The US node decreases over time, indicating that fewer individuals remain susceptible as the green behavior spreads. [TeX:] $$A_2 S$$ nodes will eventually disappear from the system, and the trend for [TeX:] $$A_1 S$$ nodes as well as [TeX:] $$A_1 G$$ nodes is quite similar. Comparing the three subplots in Fig. 5, the greater the values of the parameter [TeX:] $$\gamma_1 \text{ and } \gamma_2$$, the more people adopt green behaviors. B. Validation and Sensitivity AnalysisHere, we conduct experiments to examine the effects of some key parameters of the [TeX:] $$U A_1 A_2 U-S G S$$ model. We designate the density of green nodes in the lower layer at the steady state as [TeX:] $$\rho^G.$$ Moreover, [TeX:] $$\rho^{A_1} \text { and } \rho^{A_2}$$ are employed to depict the percentage of nodes in the upper layer that are aware of positive and negative green information at the steady state. In the computations of the MMC iterative, we define [TeX:] $$\rho^G=\left(\sum_i P_i^{A_1 G}\right) / N, \rho^{A_1}=\left[\sum_i\left(P_i^{A_1 G}+P_i^{A_1 S}\right)\right] / N,$$ and [TeX:] $$\rho^{A_2}=\left(\sum_i P_i^{A_2 S}\right) / N .$$ 1) Influence of parameters in physical contact layer on propagation: In order to verify our MMC theoretical analysis, we supplement the Monte Carlo (MC) simulations and compare them with the theoretical solution. Moreover, for the result of MC simulations, [TeX:] $$\rho^G=N_{A_1 G} / N, \rho^{A_1}=\left(N_{A_1 G}+N_{A_1 S}\right) / N,$$ and [TeX:] $$\rho^{A_2}=N_{A_2 S} / N,$$ where [TeX:] $$N_{A_1 G}, N_{A_1 S}, \text { and } N_{A_2 S}$$ are the number of nodes at the states of [TeX:] $$A_1 G, A_1 S, \text { and } A_2 S$$ in the steady state, respectively. Fig. 6 clearly depicts the changes in three states [TeX:] $$\left(\rho^G, \rho^{A_1}, \rho^{A_2}\right)$$ as functions of the transmission rate β which is obtained by MMC and MC. It is observed that the positive information and the green behavior simultaneously outbreak around the threshold [TeX:] $$\beta_c.$$ Specifically, when [TeX:] $$\beta \lt \beta_c,$$ the value of [TeX:] $$\rho^G \text { and } \rho^{A_1}$$ is 0, and when [TeX:] $$\beta \gt \beta_c,$$ the values of [TeX:] $$\rho^G \text { and } \rho^{A_1}$$ begin to increase. Additionally, the proportion of nodes that disseminate negative information starts to decrease when β approaches the threshold [TeX:] $$\beta_c.$$ Possible explanations for the above phenomenon can be concluded as follows. The proportion of green nodes grows as the transmission rate grows when [TeX:] $$\beta \gt \beta_c.$$ Once the individuals transition into green nodes, they will promptly disseminate positive information. Thus, the positive information and the green behavior outbreak around the threshold [TeX:] $$\beta_c$$ simultaneously. Conversely, when the green behavior transmission rate is high, people are more likely to adopt green behavior. This will lead to more people spreading positive messages, thus suppressing the spread of negative information. Hence, an excellent way to prompt the outbreak of green behavior is by suppressing the transmission of negative information. Additionally, comparing Figs. 6(a), 6(b), and 6(c), the threshold for the green behavior is smaller, and the green behavior prevalence increases. The reason is the greater the values of the parameter [TeX:] $$\gamma_1 \text{ and } \gamma_2,$$ the greater the green behavior transmission rate for [TeX:] $$A_1 \text{ and } A_2$$ nodes. Thus, more effective dissemination of information will help to green behavior outbreaks and expand its prevalence. Fig. 7 effectively illustrates the sensitivity of green behavior density to varying green behavior transmission rates and recovery rates of green nodes. This figure is essential for conducting a sensitivity analysis to understand how varying recovery rates impact the spread and stabilization of green behavior in the time-varying multiplex networks. It is clear to see that for all values of μ, as the propagation rate β increases, the density of green nodes [TeX:] $$\rho^G$$ increases, indicating a higher adoption rate of green behavior. The sensitivity of [TeX:] $$\rho^G$$ to changes in β varies with μ; lower values of μ show a steeper increase in [TeX:] $$\rho^G \text{ and } \beta,$$ while higher values of μ show a more gradual increase. The reason is that individuals who adopt green behavior are less likely to revert with a lower recovery rate μ, allowing the behavior to spread and stabilize quickly. Yet, higher recovery rates μ make it challenging for green behavior to spread and stabilize, as individuals are more likely to revert from green behavior. Hence, lower recovery rates enhance the spread and stabilization of green behavior, while higher recovery rates hinder it. 2) Influence of parameters in information layer on propagation: Subsequently, it is imperative to examine the impact of the rate at which positive or negative information is transmitted on green behavior prevalence. Fig. 8 clearly depicts the prevalence of green behavior within a wide range of [TeX:] $$\lambda_1 \text{ and } \lambda_2.$$ For a fixed [TeX:] $$\lambda_1,$$ when the value of [TeX:] $$\lambda_2$$ is greater than a particular value, the prevalence of green behavior decreases as [TeX:] $$\lambda_2$$ increases. Moreover, as [TeX:] $$\lambda_1$$ gets smaller, the specific value gets smaller and [TeX:] $$A_2$$ can inhibit the spread of green behaviors at a smaller spread rate. The following are explanations that may account for this phenomenon: the role of negative information keeps increasing and the role of positive information keeps being weakened as the increase of negative information transmission, leading to the green behavior prevalence decreases; moreover, when the value of [TeX:] $$\lambda_1$$ is large, the spread of negative information would have to be very high to inhibit the spread of green behavior. Furthermore, comparing panel (a) with panel (b) in Fig. 8, the value of [TeX:] $$\lambda_2$$ must be at least 0.6 to exert a dominant effect of inhibition in panel (b), since a large number of nodes adopt green behavior leads to more positive information in networks, and negative information is hard to propagate based on the high green behavior transmission rate. Generally, it is possible to improve green behavior prevalence by inhibiting the transmission of negative information and promoting the propagation of positive information. Fig. 9 effectively illustrates the sensitivity of green behavior density to varying green behavior transmission rates and positive or negative information recovery rates. This figure is divided into two panels: Panel (a) focuses on five positive information recovery rates, while panel (b) focuses on five negative recovery rates. In panel (a), lower positive recovery rates [TeX:] $$\delta_1$$ result in a rapid increase in the density of green nodes [TeX:] $$\rho^G$$ at lower values of β. Yet, higher positive recovery rates [TeX:] $$\delta_1$$ make it more challenging for green behavior to spread, requiring higher β values to reach similar densities. In panel (b), higher negative recovery rates [TeX:] $$\delta_2$$ also result in a rapid increase in [TeX:] $$\rho^G$$. Contrary to the trend observed with [TeX:] $$\delta_1$$, lower negative recovery rates [TeX:] $$\delta_2$$ hinder the spread of green behavior, requiring higher β values to achieve comparable densities. For both panels, when β is large, the final density of green nodes [TeX:] $$\rho^G$$ shows little variation across different values of [TeX:] $$\delta_1 \text{ and } \delta_2$$, indicating that the transmission rate β plays a dominant role in determining the equilibrium density of green behavior. Therefore, lower positive information recovery rates enhance the spread and stabilization of green behavior, while lower negative information recovery rates hinder it. However, when the green behavior transmission rate β is sufficiently high, the final density of green nodes becomes less sensitive to variations in information recovery rates, emphasizing the critical role of transmission rate in behavior adoption. C. Influence of Related Parameters on Green Behavior ThresholdIn this subsection, we explore different parameters on the green behavior threshold computed by (20). In Fig. 10(a), when the values of [TeX:] $$\delta_1, \delta_2, \mu, \text{ and } \lambda_2$$ are fixed, the threshold [TeX:] $$\beta_c$$ exhibits a progressively decreasing trend as the value of [TeX:] $$\lambda_1$$ is varied from 0.3 to 0.9. Similarly, when [TeX:] $$\delta_1, \delta_2, \mu, \text{ and } \lambda_1$$ are fixed, the threshold [TeX:] $$\beta_c$$ increases as [TeX:] $$\lambda_2$$ increases from 0.1 to 0.6. Therefore, it is possible to prompt the outbreak of green behavior by preventing the diffusion of negative information and facilitating the spread of positive information. In Fig. 10(b), while keeping the parameters [TeX:] $$\lambda_1, \lambda_2, \delta_1 \text{ and } \mu$$ constant, the green behavior threshold [TeX:] $$\beta_c$$ decreases as [TeX:] $$\delta_2$$ increases, whereas it decreases as [TeX:] $$\delta_1$$ decreases when [TeX:] $$\lambda_1, \lambda_2, \delta_2 \text{ and } \mu$$ are fixed. Hence, reducing the rates of forgetting positive information and increasing the rates of forgetting negative information can be considered beneficial approaches to encourage the outbreak of green behavior. Furthermore, the threshold of green behavior also increases as the recovery rate μ increases. Therefore, it is also possible to prompt the outbreak of green behavior by reducing the probability of abandoning green behavior. Additionally, we analyze the impact of the [TeX:] $$\gamma_1 \text{ and } \gamma_2$$ on the green behavior threshold in Fig. 11. It is clear to see that the green behavior threshold gradually decreases as [TeX:] $$\gamma_1$$ increases while other parameters are fixed in Fig. 11(a). This implies that the stronger the influence of positive information, the more people are willing to adopt green behavior and the lower the threshold is. Conversely, in Fig. 11(b), the stronger the inhibitory effect of negative information, the lower the probability of an individual adopting green behavior, and the green behavior threshold increases. As a result, mitigating the influence of negative messages and increasing the impact of positive information can facilitate the outbreak of green behavior. D. Influence of Time-varying Properties on Green Behavior DiffusionSubsequently, we try to figure out how the changing structure of the adaptive network, including the contact capacity and activity heterogeneity, affects the process of coupled dynamics. Since there are two types of information and their roles are opposite in the system, the relationship between green behavior spreading and topological structure is different when different information plays a dominant role. Hence, the simulation will be discussed in the following two aspects. · Positive information is predominant: Positive information plays a bigger role than negative information. · Negative information is predominant: Negative information plays a bigger role than positive information. 1) Influence of nodal activity heterogeneity on green behavior diffusion: Fig. 12 depicts how the green behavior threshold and the final green behavior proportion are affected by the value of [TeX:] $$\gamma_v$$ In Fig. 12(a), there are two types of relationships between the threshold and activity exponent of the information layer. When [TeX:] $$\lambda_1$$ is larger than [TeX:] $$\lambda_2$$, it is visual to see the green behavior threshold increases with the activity exponent of the physical contact layer [TeX:] $$\gamma_v$$. Conversely, when [TeX:] $$\lambda_2$$ is larger than [TeX:] $$\lambda_1$$, the green behavior threshold decreases with [TeX:] $$\gamma_v$$. The principal reason for this phenomenon is that a higher activity exponent results in less heterogeneity of the nodes, and an increase in [TeX:] $$\gamma_v$$ leads to a weakening effect of the node [TeX:] $$A_1$$ when [TeX:] $$\lambda_1$$ is larger than [TeX:] $$\lambda_2.$$ Hence, weakened dissemination of positive messages leads to a higher green behavior threshold. Conversely, when the negative information plays a dominant role in the upper layer, an increase in [TeX:] $$\gamma_v$$ results in a decrease in the weakening effect of negative information in the system. Moreover, to analyze the effect of the final green behavior proportion, we selected one set of parameters from the three sets of parameters for each type. Specifically, we choose [TeX:] $$\lambda_1=0.8, \lambda_2=0.2$$ when positive information plays a bigger role than negative information; and we choose [TeX:] $$\lambda_1=0.2, \lambda_2=0.8$$ when negative information plays a bigger role than positive information. In Fig. 12(b), when β is certain and greater than the propagation threshold, the final green behavior density decreases slightly as [TeX:] $$\gamma_v$$ increases, while the trend is reversed in Fig. 12(c). As a result, when positive information is predominant, we should decrease the activity exponent of the information layer; when negative information is predominant in the system, we should increase the activity exponent of the information layer. Fig. 13 depicts how the green behavior threshold and the final green behavior proportion are affected by the value of [TeX:] $$\gamma_p$$. In Fig. 13(a), it is clear that the green behavior threshold increases monotonically with the activity exponent of the information layer [TeX:] $$\gamma_p$$. When [TeX:] $$\gamma_p$$ is fixed, the larger [TeX:] $$\lambda_1$$ is, the smaller the threshold is. A possible explanation for the above phenomenon is that a lower activity exponent results in more heterogeneity of the nodes. Nodes are highly active when the nodal activities are more heterogeneous. These nodes are capable of sustaining their activities in sequential time steps, which provides the spreading process with constant impetus. Then, the smaller the [TeX:] $$\gamma_p$$, the more conducive the spread of green behavior. Besides, the higher the propagation rate of positive information, the more nodes will become [TeX:] $$A_1$$ and propagate green behavior at a higher rate, thus contributing to the outbreak of green behavior. In Figs. 13(b) and 13(c), regardless of who has a strong role in the upper layer, when β is certain and greater than the propagation threshold, the larger [TeX:] $$\gamma_p$$ is, the smaller the final green behavior density is. That is to say, a smaller activity exponent leads to a greater density of green behavior. Therefore, increasing the heterogeneity of the nodal activities in the physical contact layer can prompt green behavior spreading. 2) Influence of contact capacity on green behavior diffusion: Fig. 14 depicts how the green behavior threshold and the final green behavior density are affected by the value of mv. In Fig. 14(a), when [TeX:] $$\lambda_1$$ is larger than [TeX:] $$\lambda_2$$, the value of green behavior threshold decreases and then increases or stabilizes as [TeX:] $$m_v$$ increases. Additionally, when [TeX:] $$\lambda_2$$ is larger than [TeX:] $$\lambda_1,$$ the value of green behavior threshold increases as [TeX:] $$m_v$$ increases until saturation. The primary cause of this phenomenon is that when [TeX:] $$\lambda_1$$ is larger than [TeX:] $$\lambda_2,$$ [TeX:] $$A_1$$ will connect more nodes as [TeX:] $$m_v$$ increases, leading to more nodes supporting green behavior. At this point, the propagation threshold decreases. However, when [TeX:] $$m_v$$ increases to a certain level, [TeX:] $$A_2$$ also connects more nodes, and the inhibitory effect of [TeX:] $$A_2$$ starts to manifest itself, leading to a rise or stabilization of the threshold value. In addition, when [TeX:] $$\lambda_2$$ is larger than [TeX:] $$\lambda_1$$, negative information plays a dominant role in the upper layer, and the inhibitory effect of negative information increases as [TeX:] $$m_v$$ increases. In Fig. 14(b), when [TeX:] $$\lambda_1 \gt \lambda_2,$$ the density of green behavior increases as [TeX:] $$m_v$$ increases until saturation. In Fig. 14(c), when [TeX:] $$\lambda_1 \lt \lambda_2,$$ the density of green behavior increases and then decreases as [TeX:] $$m_v$$ increases. As a result, when negative information plays a dominant role, we should decrease the contact capacity of the information layer; when positive information plays a dominant role in the system, we should increase the contact capacity of the information layer. Fig. 15 depicts how the green behavior threshold and the final green behavior proportion are affected by the value of [TeX:] $$m_p$$. The threshold for green behavior decreases with the number of links generated by the active nodes increases in the physical contact layer in a time step, regardless of the size relationship between [TeX:] $$\lambda_1 \text{ and } \lambda_2.$$ A possible explanation for the above phenomenon is that when [TeX:] $$m_p$$ is larger, the active nodes will generate more edges and connect more nodes in the physical contact layer, facilitating the propagation of green behavior. Thus, the propagation threshold is smaller and the density of green behaviors is greater. Therefore, enhancing the contact capacity of the nodes in the physical contact layer can prompt green behavior diffusion. VI. CONCLUSIONIn this paper, the [TeX:] $$U A_1 A_2 U-S G S$$ model in time-varying multiplex networks is proposed to investigate the features of green behavior diffusion under the impact of positive and negative information. In time-varying multiplex networks, one layer describes the positive and negative information diffusion and the other represents the green behavior spreading. Based on MMC, we build the probability transition equations and calculate the green behavior threshold of the model. Then, experiments are carried out to confirm the preciseness and theoretical predictions of the new model. It reveals that the prevalence of green behavior can be promoted by restraining the negative information transmission rate and recovery rate of the green nodes while facilitating the positive information transmission rate and green behavior transmission rate. Additionally, reducing the positive information recovery rate and the recovery rate of the green nodes, and increasing the rates of forgetting negative information are beneficial for encouraging the outbreak of green behavior. Moreover, we investigate the structure of the time-varying model that affects green behavior propagation. In the physical contact layer, higher contact capacity and greater activity heterogeneity significantly facilitate green behavior spreading. In the information layer, when negative information plays a dominant role, the smaller contact capacity and the weaker activity heterogeneity can promote green behavior diffusion; when positive information plays a dominant role, the larger contact capacity and the stronger activity heterogeneity of individuals can promote green behavior diffusion. This paper provides a general framework to investigate green behavior diffusion in time-varying multiplex networks, providing some insightful analysis of actual situations and helping develop effective strategies to prompt green behavior spreading. The two-layer approach, which separately analyzes information diffusion and behavior spreading, allows for a detailed examination of the interplay between positive and negative information and green behavior adoption. There are several limitations of this paper, which also casts light on future research directions. Firstly, the analysis is at a generalized level and does not consider the heterogeneity between different green behaviors or individual differences. Further work should focus on a special green behavior, with the consideration of individual heterogeneity. Secondly, the impact of external factors, such as social influence and media effects, is not explicitly considered in our model. Further work should explore the role of external factors to gain a more comprehensive understanding of green behavior adoption and refine intervention strategies. BiographyBiographyLinghua ZhangLinghua Zhang received the M.S. degree in Signal and Information Processing from Southeast University and the Ph.D. degree in Signal and Information Processing from the Nanjing Univer sity of Posts and Telecommunications, Nanjing, China, in 1990 and 2005, respectively, where she is currently a Professor and a Ph.D. Supervisor with the College of Telecommunications and Information Engineering. Her research interests include speech signal processing, voice communication, and signal processing in wireless communication. BiographyBiographyReferences
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