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Mathematical analysis of the emergence of communities based on coevolution of social contagion and bonding by homophily
Applied Network Science volume 4, Article number: 39 (2019)
Abstract
In this paper it is analysed how community formation in an adaptive network for bonding based on similarity (homophily) can be related to characteristics of the adaptive network’s structure, which includes the structure of the adaptation principles incorporated. In particular, this is addressed for adaptive social networks for bonding based on homophily. To this end, relevant properties of the network and the adaptation principle have been identified, such as a tipping point for similarity. As one of the results, it has been found how the emergence of communities strongly depends on the value of this tipping point. Moreover, it is shown that some properties of the structure of the network and the adaptation principle entail that the connection weights all converge to 0 (for persons in different communities) or 1 (for persons within one community).
Introduction
In this paper, it is analysed how emerging communities based on the coevolution of social contagion (Levy and Nail 1993) and bonding by homophily (McPherson et al. 2001; Pearson et al. 2006) can be related to characteristics of the adaptive network’s structure. For this adaptive case, this network structure includes the structure of the homophily adaptation principle that is incorporated. The homophily adaptation principle expresses how ‘being alike’ strengthens the connection between two persons (McPherson et al. 2001; Pearson et al. 2006). Social contagion implies that the stronger two persons are connected, the more they will become alike (Levy and Nail 1993). Thus a reciprocal causal relation between the two processes occurs. It is known from simulations (Axelrod 1997; Holme and Newman 2006; Sharpanskykh and Treur 2014; Vazquez 2013; Vazquez et al. 2007) that the emerging behaviour of adaptive network models combining these two processes as a form of coevolution often shows community formation. In the resulting network structure within a community persons have high mutual connection weights and a high extent of ‘being alike’, and persons from different communities have low mutual connection weights and a low extent of ‘being alike’.
Relevant properties of the network and the homophily adaptation principle have been identified, such as a tipping point for homophily. As one of the results, it has been found how the emergence of communities strongly depends on the value of this tipping point. Moreover, it is shown that some properties of the structure of the network and the homophily adaptation principle entail that the connection weights all converge to 0 (for states in different emerging communities) or 1 (for states within one emerging community).
In general, it is a challenging issue for dynamic models to predict what patterns of behaviour will emerge, and how their emergence depends on the structure of the model. This structure includes chosen parameter values used as characteristics of the model’s structure (and settings). This also applies to network models, where behaviour depends in some way on the network structure, defined by network characteristics such as connections and their weights; e.g., (Turnbull et al. 2018). In this context, the issue is how emerging network behaviour relates to network structure. For example, see (Treur, 2018b) it can be an even more challenging issue when coevolution that occurs in adaptive networks is considered, in which case by a mutual causal interaction both the states and the network characteristics change over time. In this case the connections in the network change according to certain adaptation principles which themselves depend on certain adaptation characteristics represented by their own parameters.
In the current paper, the emergence of communities based on the coevolution of social contagion (Levy and Nail 1993) and bonding by homophily (McPherson et al. 2001; Pearson et al. 2006) will be analysed in some depth. By mathematical analysis, it is found out how emerging communities relate to the characteristics of the network and of the specific homophily adaptation principle used in combination with a social contagion principle.
The issue was addressed using the NetworkOriented Modeling approach based on temporalcausal networks (Treur 2016b, Treur 2019) as a vehicle. For temporalcausal networks, parameters characterising the network structure are connection weights, combination functions, and speed factors. For the type of adaptive networks considered, the connection weights are dynamic based on the homophily principle. So they are considered as states themselves and not part of the static characteristics of the network structure anymore. In the research reported here characteristics of the homophily adaptation principle have been identified that play an important role in community formation, among which the tipping point for the difference between two persons This is the point where ‘being alike’ turns into ‘not being alike’, or conversely. In this paper, results are discussed that have been proven mathematically for this relationship between network structure and network behavior for the coevolution process. In particular, for emerging communities what the connections become between persons from one community or persons from different communities, and how different persons from one community or from different communities become. Note that these results have not been proven for one specific model or function, but for whole classes of models with a variety of functions that fulfill certain properties. The technical content has been adopted mostly from the conference paper (Treur 2018c), but extended by more than 50%. One of the additions is the analysis of the relation of the obtained results to the strongly connected components of a network, for example, as defined in (Harary et al. 1965, Ch. 3; Kuich 1970, Section 6).
In this paper, in Section 2 the NetworkOriented Modeling approach used is briefly outlined. In Section 3 adaptive networks based on homophily are described and a number of functions that can be used to model them. Section 4 shows some example simulations. In Section 5 relevant properties are defined that are used in Section 6 to prove results on the relation between network structure and behaviour. In Section 7 it is shown how the obtained results relate to the strongly connected components of a network. Finally, Section 8 is a discussion.
Networkoriented modeling by temporalcausal networks
In order to undertake any mathematical analysis of networks, in the first place, a solid definition of the concept of network is needed, based on welldefined semantics. In the current paper, the interpretation of connections based on causality and dynamics forms a basis of the structure and semantics of the considered networks. It is a deterministic dynamic modeling approach, for example in the line of (Ashby 1960), in contrast to, stochastic modeling approaches as, for example, used in (Axelrod 1997). It can be positioned as a branch in the causal modelling area which has a long tradition in AI; e.g., see (Kuipers and Kassirer 1983; Kuipers 1984; Pearl 2000). It distinguishes itself by a dynamic perspective on causal relations, according to which causal relations exert causal effects over time, and these causal relations themselves can also change over time.
More specifically, the nodes in a network are interpreted here as states (or state variables) that vary over time, and the connections are interpreted as causal relations that define how each state can affect other states over time. This type of network has been called a temporalcausal network (Treur 2016b); note that the word temporal here refers to the causality, not to the network. Temporalcausal networks that themselves change over time as well are called adaptive temporalcausal networks; e.g., (Gross and Sayama 2009). So, in cases of adaptive temporalcausal networks, in addition to the node states also the connections are assumed to change over time and are therefore treated like states as well.
A conceptual representation of a temporalcausal network model by a labeled graph provides a fundamental basis. Such a conceptual representation includes representing in a declarative manner states (also called nodes) and connections between them that represent (causal) impacts of states on each other. This part of a conceptual representation is often depicted in a conceptual picture by a graph with nodes and directed connections. However, a complete conceptual representation of a temporalcausal network model also includes a number of labels for such a graph. A notion of strength of a connection is used as a label for connections, some way to aggregate multiple causal impacts on a state is used, and a notion of speed of change of a state is used for timing of the processes. Note that states have one value; they can relate one by one to states of persons or agents, for example, the strength of their opinion states. It is also possible to model each person by more than one state, for example, an opinion and an emotion state per person. In such a case a person does not relate to a single state but to a subnetwork consisting of multiple states.
The three described notions, called connection weight \( {\boldsymbol{\upomega}}_{X,Y} \), combination function c_{Y}(..), and speed factor η_{Y}, make the graph of states and connections a labeled graph (e.g., see Fig. 1), and form the defining structure of a temporalcausal network model in the form of a conceptual representation; for a summary, see also Table 1, top half: rows 1 to 5. Note that for the current paper all connection weights are assumed nonnegative: \( {\boldsymbol{\upomega}}_{X,Y}\in \left[0,1\right] \) for all X and Y.
The interpretation of a network based on causality and dynamics can be expressed in a formalnumerical way, thus associating semantics to any conceptual temporalcausal network representation in a detailed numericalmathematically defined manner. For a summary, see Table 1, bottom half: rows 6 to 10. This shows how a conceptual representation based on states and connections enriched with labels for connection weights, combination functions, and speed factors, can be transformed into a numerical representation (Treur 2016b), Ch. 2. A more detailed explanation of the difference equation format, taken from (Treur 2016b), Ch 2, p. 60–61, is as follows; see also Fig. 2. The aggregated impact value aggimpact_{Y}(t) at time t pushes the value of Y up or down, depending on how it compares to the current value of Y. So, aggimpact_{Y}(t) is compared to the current value Y(t) of Y at t by taking the difference between them (also see Fig. 2): aggimpact_{Y}(t) – Y(t). If this difference is positive, which means that aggimpact_{Y}(t) at time t is higher than the current value of Y at t, in the time step from t to t + Δt (for some small Δt) the value Y(t) will increase in the direction of the higher value aggimpact_{Y}(t). This increase is done proportionally to the difference, with proportion factor η_{Y} Δt: the increase is η_{Y} [aggimpact_{Y}(t) – Y(t)] Δt; see Fig. 2. By this format, the parameter η_{Y} indeed acts as a speed factor by which it can be specified how fast state Y should change upon causal impact.
There are many different approaches possible to address the issue of combining multiple causal impacts. To provide sufficient flexibility, the NetworkOriented Modelling approach based on temporalcausal networks incorporates for each state a way to specify how multiple causal impacts on this state are aggregated by a combination function. For this aggregation, a library with a number of standard combination functions are available as options (currently 35), but also owndefined functions can be added. The difference equations in Fig. 2 and in the last row in Table 1 constitute the overall numerical representation of the temporalcausal network model and can be used for simulation and mathematical analysis; it can also be written in differential equation format:
For adaptive networks, connection weights are dynamic and therefore handled in the same way as states, with their own combination functions and speed factors; connections of them have weight value 1 by default. This will be shown in more detail in Sections 3 to 5.
Often used examples of combination functions are the identity function id(.) for states with impact from only one other state, the scaled sum function ssum_{λ}(..) with scaling factor λ, and the advanced logistic sum combination function alogistic_{σ,τ}(..) with steepness σ and threshold τ:
Note that for λ = 1, the scaled sum function is just the sum function sum(..), and this sum function can also be used as the identity function in case of one incoming connection. In addition to the above functions, a Euclidean combination function is defined as
where n is the order (which can be any natural number but also any positive real number), and λ is a scaling factor. This can be used when all connection weights are nonnegative, but in the specific case that n is an odd natural number, also negative connection weights can be allowed. A Euclidean combination function is called normalised if the scaling factor λ is chosen in such a way that \( \mathbf{c}\left({\boldsymbol{\upomega}}_{X_1,Y},\dots, {\boldsymbol{\upomega}}_{X_k,Y}\right)=1 \); this is achieved for \( \uplambda ={{{\boldsymbol{\upomega}}_{X_1}}_{,Y}}^n+\dots +{{{\boldsymbol{\upomega}}_{X_k}}_{,Y}}^n \). Note that for n = 1 (first order) the scaled sum function is obtained:
Then \( \uplambda ={\boldsymbol{\upomega}}_{X_1,Y}+\dots +{\boldsymbol{\upomega}}_{X_k,Y} \) makes it normalised. For n = 2 it is the secondorder Euclidean combination function eucl_{2,λ}(..) defined by:
Such a secondorder Euclidean combination function is also often applied in aggregating the error value in optimisation and in parameter tuning using the rootmeansquare deviation (RMSD), based on the Sum of Squared Residuals (SSR).
Adaptive networks based on homophily
The homophily principle addresses bonding between persons. It describes how connections between two persons are strengthened or weakened depending on the extent of similarity between them: more ‘being alike’ will make the persons more ‘like each other’ (McPherson et al. 2001; Pearson et al. 2006). This is modelled by the states X(t) and Y(t) the persons X and Y have at time t, for example, indicating whether at time t they enjoy being physically active (high value) or not (low value), or indicating the extent to which they agree with a certain opinion. According to the homophily principle the weight ω_{X,Y} of the connection from X to Y is changing over time dynamically, depending on how the state levels X(t) and Y(t) differ. As this connection weight ω_{X,Y} is dynamic, in a general setting it is handled as a state with its own combination function \( {\mathbf{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,W\right) \), called homophily combination function. Then the standard difference and differential equation format as shown in Section 2 is applied; here V_{1} stands for X(t), V_{2} stands for Y(t), and W stands for connection weight ω_{X,Y}(t):
The parameter \( {\boldsymbol{\upeta}}_{\upomega_{X,Y}} \) is the speed parameter of connection weight ω_{X,Y}. Note that ω_{X,Y} increases if and only if \( {\mathbf{c}}_{\upomega_{X,Y}}\left(X,Y,{\upomega}_{X,Y}\right)>{\upomega}_{X,Y},{\upomega}_{X,Y} \) decreases if and only if \( {\mathbf{c}}_{\upomega_{X,Y}}\left(X,Y,{\upomega}_{X,Y}\right)<{\upomega}_{X,Y} \), and ω_{X,Y} is stationary if and only if \( {\mathbf{c}}_{\upomega_{X,Y}}\left(X,Y,{\upomega}_{X,Y}\right)={\upomega}_{X,Y} \). Specific adaptation principles formalising bonding by homophily can be obtained by picking specific functions for the homophily combination function \( {\mathbf{c}}_{\upomega_{X,Y}}\left(X,Y,{\upomega}_{X,Y}\right) \) for a given application domain, or even different combination functions \( {\mathbf{c}}_{\upomega_{X,Y}}\left(X,Y,{\upomega}_{X,Y}\right) \) for different persons within a given domain. There are many options for such choices; see, for example, Table 2 and Fig. 3. Therefore it may be more useful to define classes of such homophily combination functions characterised by certain properties of them. Then as shown in Section 6, results can be proven for such a class instead of for each homophily combination function separately. Formal definitions of such properties of the function \( {\mathbf{c}}_{\upomega_{X,Y}}\left(X,Y,{\upomega}_{X,Y}\right) \) will be given in Section 5, but here some examples of homophily combination functions are shown.
A very simple example of a homophily combination function \( {\mathbf{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,W\right) \) is a linear function in D = V_{1}– V_{2} defined as follows:
Here β is a modulation factor that still can be chosen, and τ is a tipping point (or threshold) parameter. This function may have the disadvantage that when W = 0 it may be negative (when D > τ) or when W = 1 it may be higher than 1 (when D < τ), so that it has to be cut off to avoid that the weight value ω_{X,Y} goes outside the interval [0, 1]. This can also be remedied in a smooth manner by choosing β as a function β(W) = α W(1W) of W which can suppress the term τ  D when W comes closer to 0 or 1. This function makes that ω_{X,Y} will not cross the boundaries 0 and 1:
Here α is a modulation or amplification parameter; the higher its value, the stronger the effect (either positive or negative) of homophily on the connection. This combination function for bonding by homophily was considered in (Treur 2017). Using this homophily combination function, the dynamic relations for ω_{X,Y} are:
As a variant of this homophily combination function \( {\mathbf{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,W\right) \) that is linear in D, the following function can be obtained as a quadratic function of D = V_{1}– V_{2}:
Using this combination function, the dynamic relations for ω_{X,Y} are:
In Table 2 and Fig. 3 these linear and quadratic combination function and a number of other examples of homophily combination functions are depicted, with D = V_{1}– V_{2} on the horizontal axis and \( {\mathbf{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,W\right) \) on the vertical axis for τ = 0.2 and W = 0.7. In Section 6 the results that have been proven are general in the sense that they apply to all of such functions, not just one specific function. To this end, in Section 5 relevant properties shared by these functions are defined. The simple linear combination function slhomo_{τ,α}(V_{1}, V_{2}, W) was used in (Blankendaal et al. 2016) and (Treur 2017), and the simple quadratic combination function sqhom_{τ,α}(V_{1}, V_{2}, W) in (van Beukel et al. 2017). A more advanced logistic combination function based on log2homo_{τ,σ,α}(V_{1}, V_{2}, W) was explored in (Boomgaard et al. 2018).
Example simulations for the coevolution of social contagion and bonding by homophily
In this section, a few example simulations for the coevolution of social contagion and bonding based on homophily are described. It will be shown how communities emerge and more specifically how their emergence depends on properties of the chosen functions for homophily. These examples will be used in Section 6 to illustrate the results that have been proven. The examples concern a fully connected social network of 10 states with speed factors η_{Y} = 0.1 for states Y and initial values ω_{X,Y}(0) for the connection weights from state X to state Y as shown in Table 3.
As combination functions for social contagion for the states, the normalised scaled sum functions were used, and as combination functions for the connections the simple linear homophily function slhomo_{τ,α}(V_{1}, V_{2}, W) with tipping point τ = 0.1, speed factor \( {\upeta}_{\upomega_{X,Y}}=0.4 \) for each ω_{X,Y}. The graphs in the lefthand side of Figs. 4 and 5 show time on the horizontal axis and activation values of states at the vertical axis until it ends up in an equilibrium state, i.e., all values become constant. In the same figures on the righthand side matrices with the final connection weights are shown. The homophily modulation factor α is varying from 1 to 10 in Fig. 4, and from 11 to 15 in Fig. 5. More specifically, at the lefthand side of Figs. 4 and 5 graphs of simulations of the state values are shown up to time point 100 (with Δt = 0.05); at the righthand side the connection matrices are shown at time point 500 (with Δt = 0.25), with an accuracy of 3 digits (0 means < 0.001, 1 means > 0.999). It turns out that all connection weights converge to 0 or 1.
Note that the modulation factor α models the strength of the effect of homophily. A higher α makes that connections change earlier in the process (compared to the pace of the social contagion) and due to that more clusters occur, as can be seen in Fig. 4. For α = 1 all states end up in one cluster (all become connected by weights 1), for α = 5 in two clusters (two subgroups of states {X_{1}, X_{2}, X_{8}, X_{9}, X_{10}} and {X_{3}, X_{4}, X_{5}, X_{6}, X_{7}} get connections with weight 1 and form clusters in this way; between these clusters the weights are 0), and for α = 10 in three clusters: {X_{1}, X_{8}}, {X_{2}, X_{9}, X_{10}} and {X_{3}, X_{4}, X_{5}, X_{6}, X_{7}}). Moreover, it can be observed that no clusters emerge with state values at a distance less than tipping point τ = 0.1.
Still increasing the modulation factor α, Fig. 5 zooms in at the birth of a fourth cluster. For α = 11 it can be seen that for the cluster {X_{3}, X_{4}, X_{5}, X_{6}, X_{7}} the states X_{5} and X_{6} join X_{3}, X_{4}, and X_{7} in a very late stage, and (compared to the case α = 10 in Fig. 4) even a slight hesitation for that may be observed from time point 20 to 40 while the values of X_{5} and X_{6} (around 0.7) have distance of about the tipping point τ = 0.1 from the values (around 0.8) for X_{3}, X_{4}, and X_{7}. This hesitation can be confirmed, as increasing the modulation factor α by just 0.4 to 11.4 shows how a fourth separate cluster emerges for {X_{5}, X_{6}}. This fourth cluster converges to state value 0.683 whereas the other cluster {X_{3}, X_{4}, X_{7}} converges to state value 0.796, which is a difference of 0.113: just above the tipping point τ = 0.1. This may suggest that the model keeps the clusters at a distance of at least τ; this is one of the issues that will be analysed further in Section 6. For higher values of α, such as α = 15 no more than these four clusters emerge.
Relevant properties of combination functions for homophily and social contagion
This section addresses definitions for the properties for the network structure and in particular also for the homophily adaptation principle that have been identified as relevant for the adaptive network’s behavior. As adaptation principles are specified by their own combination functions, these properties are described as properties of homophily combination functions. The following are considered plausible assumptions for a homophily combination function; here D = V_{1} – V_{2} :

\( {\mathbf{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,W\right) \) is a function: [0, 1] x [0, 1] x [0, 1] → [0, 1]

\( {\mathbf{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,W\right) \) is a monotonically decreasing function of D

For D close to 0 and W < 1 it holds \( {\mathbf{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,W\right)>W \) (i.e., ω_{X,Y} will increase)

For D close to 1 and W > 0 it holds \( {\mathbf{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,W\right)<W \) (i.e., ω_{X,Y} will decrease)
Note that when the first condition is not fulfilled, usually the function is cut off at 1 (when its value would be above 1) or at 0 (when its value would be below 0); see also in Fig. 3. Relatively simple functions \( {\mathbf{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,W\right) \) that satisfy these requirements are obtained when a tipping point τ (a fixed number between 0 and 1) is assumed such that for 0 < ω_{X,Y} < 1 it holds
• upward change of ω_{X,Y} when D < τ  c_{ωX,Y}(V_{1}, V_{2}, W) > W when D < τ 
• no change of ω_{X,Y} when D = τ  c_{ωX,Y}(V_{1}, V_{2}, W) = W when D = τ 
• downward change of ω_{X,Y} when D > τ  c_{ωX,Y}(V_{1}, V_{2}, W) < W when D > τ 
These criteria are formalised in the following definition of properties of any function c(V_{1}, V_{2}, W), but considered here as properties for homophily combination function in particular. So for the function c(V_{1}, V_{2}, W), keep in mind that this is applied to a homophily combination function \( {\mathbf{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,W\right) \). It will be shown in Section 6 how these properties relate to the equilibrium behaviour of the network.
Definition 1 (Tipping point and strict tipping point)

a)
The function c(V_{1}, V_{2}, W): [0, 1] x [0, 1] x [0, 1] → [0, 1] has tipping point τ for V_{1} and V_{2} if for all W with 0 < W < 1 and all V_{1}, V_{2} it holds

(i)
c(V_{1}, V_{2}, W) > W ⇔ V_{1}– V_{2} < τ

(ii)
c(V_{1}, V_{2}, W) = W ⇔ V_{1}– V_{2} = τ

(iii)
c(V_{1}, V_{2}, W) < W ⇔ V_{1}– V_{2} > τ

(i)

b)
The function c(V_{1}, V_{2}, W) has a strict tipping point τ if it has tipping point τ and in addition it holds:

(i)
If V_{1} – V_{2} < τ then c(V_{1}, V_{2}, 0) > 0

(ii)
If V_{1} – V_{2} > τ then c(V_{1}, V_{2}, 1) < 1

(i)
Note Definition 1a) can be reformulated in the sense that any function c(V_{1}, V_{2}, W) that is monotonically decreasing in D = V_{1}– V_{2} and goes for any W with 0 < W < 1 through the point with D = V_{1}– V_{2} = τ and c(V_{1}, V_{2}, W) = W has tipping point τ. This is illustrated in Fig. 3 by the yellow areas. In particular, this applies to all example functions shown in Table 2 as Fig. 3 shows that they all are monotonically decreasing and go through the point (0.2, 0.7) for which D = 0.2 and c(V_{1}, V_{2}, W) = 0.7.
Note that condition b) of this Definition 1 is not fulfilled when V_{1} – V_{2} < τ and c(V_{1}, V_{2}, 0) = 0 or when V_{1} – V_{2} > τ and c(V_{1}, V_{2}, 1) = 1. For example, for slhomo_{τ,α}(V_{1}, V_{2}, W) and sqhomo_{τ,α}(V1, V2, W) these cases do occur as always slhomo_{τ,α}(V1, V2, 0) = 0 and slhomo_{τ,α}(V_{1}, V_{2}, 1) = 1 due to the factor W(1W), and the same for sqhomo_{τ,α}(V_{1}, V_{2}, W). Therefore they do have a tipping point but they do not have a strict tipping point. In the third paragraph in Section 8 it is discussed how in a practical application having a tipping point but not having a strict tipping point is not a big problem, but some care is needed in not assigning initial values 0 or 1 to connection weights, as these values will never change in such cases. Note that when a function with strict tipping point τ is used, any two nodes X, Y with ω_{X,Y}(t) = 0 (which usually is interpreted as not being connected) can become connected over time: when X(t) – Y(t) < τ, then by Definition 1b)(i) it holds ω_{X,Y}(t’) > 0 for t’ > t.
Some examples of combination functions having a strict tipping point τ have been explored in more detail in (Sharpanskykh and Treur 2014) and (Boomgaard et al. 2018). In the former the advanced quadratic combination function aqhomo_{τ,σ}(V_{1}, V_{2}, W) and in the latter the advanced logistic function alog2homo_{τ,σ,α}(V_{1}, V_{2}, W) has been explored; see also (Treur 2016a, b), Ch 11, p. 309:
Here Pos(x) = (x + x)/2. The following lemma shows some properties of this operator.
Lemma 1

a)
Pos(x) = x when x is positive, else Pos(x) = 0.
So always Pos(x) ≥ 0, and when Pos(x) > 0, then Pos(−x) = 0.

b)
For any numbers α and β the following are equivalent:

(i)
α Pos(x) + β Pos(−x) = 0

(ii)
α Pos(x) = 0 and β Pos(−x) = 0

(iii)
x = 0 or x > 0 and α = 0 or x < 0 and β = 0

(i)
This format using the double Pos(..) function can often be used to create a combination function satisfying the strict tipping point condition as a variation on a combination function satisfying only the tipping point condition. This is shown in the following proposition that assumes any close distance function denoted by d(τ, D). More specifically, the following proposition makes it quite easy to obtain functions with tipping point τ or with strict tipping point τ.
Proposition 1
Suppose for any function d(τ, D) it holds
Then the following hold:

a)
For any α > 0 the function.
satisfies the tipping point condition, but not strict

b)
For any α > 0 the function.
satisfies the strict tipping point condition.
Proof

a)
The proof is mainly based on some algebraic rewriting.
Here as a first step it has to be proven that for any W with 0 < W < 1 and all V_{1}, V_{2} it holds.
This follows from
Similarly the other two cases for V_{1}– V_{2} > τ and V_{1}– V_{2} = τ can be verified.
From c(V_{1}, V_{2}, 0) = 0 for all V_{1}, V_{2} it follows that the strict tipping point requirement is not fulfilled.

b)
Also this proof is mainly based on some algebraic rewriting, thereby using Lemma 1.
First, c’(V_{1}, V_{2}, W) satisfies the tipping point condition; for any W with 0 < W < 1 and all V_{1}, V_{2} by Lemma 1 it holds:
Similarly the other two conditions.
It is strict because
and
Proposition 1 can easily be applied to simple linear or quadratic functions d(τ, D) such as:
but also to functions such as
as is shown in Proposition 2 b) and c).
The following proposition shows for four cases how it can be proven that some homophily combination function satisfies the tipping point or strict tipping point conditions.
Proposition 2

a)
log1hom_{τ,α}(V_{1}, V_{2}, W) has tipping point τ, and is not strict

b)
slog2hom_{τ,α}(V_{1}, V_{2}, W) has tipping point τ, and is not strict

c)
alog2hom_{τ,α}(V_{1}, V_{2}, W) has a strict tipping point τ

d)
exphomo_{τ,σ}(V_{1}, V_{2}, W) has a tipping point τ and is not strict
Proof

a)
This is based on some algebraic rewriting.
For log1hom_{τ,α}(V_{1}, V_{2}, W) suppose 0 < W < 1, then for D = V_{1}– V_{2} it holds
Similarly the other conditions can be verified:
To verify that it has no strict tipping point τ: for any V_{1}, V_{2} it holds

b)
This proof is based on Proposition 1. Applying Proposition 1a) to slog2hom_{τ,α}(V_{1}, V_{2}, W) consider
This function indeed satisfies the conditions of Proposition 1; therefore from Proposition 1a) it follows that it has tipping point τ but not strict tipping point τ.

c)
Also this proof is based on Proposition 1. For alog2hom_{τ,α}(V_{1}, V_{2}, W) it follows from Proposition 1b) with the same d(τ, D) as above that it has strict tipping point τ.

d)
This is based on some algebraic rewriting.
For W with 0 < W < 1 it holds
This shows it has tipping point τ. It has no strict tipping point, as
The following proposition shows that weighted averages of functions with tipping point τ also have a tipping point τ, and the same for having a strict tipping point.
Proposition 3
A weighted average (with positive weights) of homophily combination functions with tipping point τ also has tipping point τ, and with strict tipping point τ, also has strict tipping point τ.
Proof
This can be verified in a straightforward manner.
Suppose
with γ_{1} + … + γ_{m} = 1. Suppose 0 < W < 1. Then V_{1}– V_{2} < τ ⇒ c_{i}(V_{1}, V_{2}, W) > W for all i, and therefore
Similarly
Now suppose c(V_{1}, V_{2}, W) > W, then V_{1}– V_{2} = τ or V_{1}– V_{2} > τ cannot hold as they imply c(V_{1}, V_{2}, W) = W or c(V_{1}, V_{2}, W) < W, therefore V_{1}– V_{2} < τ. The same for the other clauses. Moreover, suppose that the functions c_{i}(V_{1}, V_{2}, W) all have strict tipping point τ. Then
If V_{1} – V_{2} < τ then
If V_{1} – V_{2} > τ then
Therefore also c(V_{1}, V_{2}, W) has a strict tipping point.
When more characteristics on network structure and adaptation combination functions are assumed, more refined results can be found, as will be shown in Section 6. Next, consider the combination functions used for social contagion of the states.
Definition 2 (Properties of combination functions for social contagion)

(a)
A function c(..) is called monotonically increasing if

(b)
A function c(..) is called strictly monotonically increasing if

(c)
A function c(..) is called scalarfree if c(αV_{1}, …, αV_{k}) = α c(V_{1}, …, V_{k}) for all α > 0
Definition 3 (Normalised network)
A network is normalised or uses normalised combination functions if for each state Y it holds \( {\mathrm{c}}_Y\left({\upomega}_{X_1}{,}_Y,\dots, {\upomega}_{X_k}{,}_Y\right)=1 \), where X_{1}, …, X_{k} are the states with outgoing connections to Y.
Note that \( {\mathrm{c}}_Y\left({\upomega}_{X_1}{,}_Y,\dots, {\upomega}_{X_k}{,}_Y\right) \) is an expression in terms of the parameter(s) of the combination function and \( {\upomega}_{X_1}{,}_Y,\dots, {\upomega}_{X_k}{,}_Y \). To require this expression to be equal to 1 provides a constraint on these parameters: an equation relating the parameter value(s) of the combination functions to the parameters \( {\upomega}_{X_1}{,}_Y,\dots, {\upomega}_{X_k}{,}_Y \). To satisfy this property, often the parameter(s) can be given suitable values. For example, for a Euclidean combination function \( {\uplambda}_Y={\upomega}_{X_1}{,_Y}^n+\dots +{\upomega}_{X_k}{,_Y}^n \) will provide a normalised network. This can be done in general:

(1)
normalisation by adjusting the combination functions. If any combination function c_{Y}(..) is replaced by c’_{Y}(..) defined as
then the network becomes normalised: indeed \( \mathrm{c}{'}_A\left({\upomega}_{X_1,Y},\kern0.5em ..,{\upomega}_{X_k,Y}\right)=1 \)

(2)
normalisation by adjusting the connection weights (for scalarfree combination functions). For scalarfree combination functions also normalisation is possible by adapting the connection weights; define:
Then the network becomes normalised; indeed it holds:
Definition 4 (Symmetric network and symmetric combination function)

a)
A network is called weakly symmetric if for all states X, Y it holds ω_{X,Y} > 0 ⇔ ω_{Y,X} > 0. It is fully symmetric if for all states X, Y it holds ω_{X,Y} = ω_{Y,X}.

b)
The homophily combination function \( {\mathrm{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,W\right) \) is called symmetric if \( {\mathrm{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,W\right)={\mathrm{c}}_{\upomega_{Y,X}}\left({V}_2,{V}_1,W\right) \).
If the combination function \( {\mathrm{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,W\right) \) is symmetric, the network is fully symmetric if the initial values for ω_{X,Y} and ω_{Y,X} are equal.
Proposition 4

a)
When the homophily function c(V_{1}, V_{2}, W) is symmetric, and initially the network is fully symmetric, then the network is continually fully symmetric.

b)
For every n > 0 a Euclidean combination function of n^{th} degree is strictly monotonically increasing, scalarfree, and symmetric
Proof

a)
This follows from the fact that in this case the difference equation for ω_{X,Y} is symmetric in X and Y

b)
A Euclidean combination function is composed of strictly monotonic functions as each function \( {V}_i\to {V}_{i^n} \) is monotonic for positive n and positive values V_{i}, and so are W → W/λ and W → W^{1/n}. From
it follows that it is scalarfree. The rest directly follows.
Relating adaptive network structure to bonding behaviour
In this section, an analysis is presented of the asymptotic behaviour of an adaptive network based on the coevolution of social contagion and bonding by homophily. Here it is found out how the network and adaptation properties defined in Section 5 (such as a tipping point τ), affect the emerging behaviour of the adaptive network. In particular, it is addressed how these properties imply that over time the network ends up in certain states (for both the nodes and the connections) that represent community formation. It will turn out that under certain conditions in terms of the properties defined in Section 5, in the end, a number of communities emerge such that:

Nodes within one community have similar state values

Connections between nodes within a community are very strong

Connections between nodes from different communities are very weak
Note that these phenomena were already observed in the simulation examples in Section 4, but now it will be proved why under certain conditions they always have to occur. To formalise this, the following general notions are important; e.g., (Brauer and Nohel 1969; Hirsch 1984; Lotka 1956).
Definition 5 (Stationary point and equilibrium)
A state Y has a stationary point at t if dY(t)/dt = 0, is increasing at t if dY(t)/dt > 0, and is decreasing at t if dY(t)/dt < 0, and similarly for adaptive connection weights ω. The network is in equilibrium a t if every state Y and every connection weight ω in the model has a stationary point at t. The equilibrium is attracting if any small perturbations of its values lead to convergence to the equilibrium values.
Considering the specific differential equation format for a temporalcausal network model shown in Section 2, and assuming nonzero speed factors the following more specific criteria for stationary points, and for increasing and decreasing trends, in terms of the combination functions and connection weights are easily found:
Lemma 2 (Criteria for a stationary, increasing and decreasing)
Let Y be a state and X_{1}, ..., X_{k} the states with outgoing connections to state Y. Then
(i)  Y has a stationary point at t  ⇔  \( {\mathbf{c}}_Y\left({\boldsymbol{\upomega}}_{X_1,Y}{X}_1(t),\dots, {\boldsymbol{\upomega}}_{X_k,Y}{X}_k(t)\right)=Y(t) \) 
(ii)  Y is strictly increasing at t  ⇔  \( {\mathbf{c}}_Y\left({\boldsymbol{\upomega}}_{X_1,Y}{X}_1(t),\dots, {\boldsymbol{\upomega}}_{X_k,Y}{X}_k(t)\right)>Y(t) \) 
(iii)  Y is strictly decreasing at t  ⇔  \( {\mathbf{c}}_Y\left({\boldsymbol{\upomega}}_{X_1,Y}{X}_1(t),\dots, {\boldsymbol{\upomega}}_{X_k,Y}{X}_k(t)\right)<Y(t) \) 
Similarly for connection weights ω.
Theorem 1 presents some of the results found for the relation between the emerging equilibrium values for states and for connection weights. It is shown how the distance of the equilibrium values of two states relates to the equilibrium value of their connections. Note that for now no specific assumption is made on the combination function for social contagion. To prove Theorem 1, the following lemma is a useful means. It shows that when the function c(V_{1}, V_{2}, W) satisfies the tipping point criterion, a connection weight 0 can only be reached for states X and Y when X(t) − Y(t) > τ and a connection weight 1 can only be reached for states X and Y when X(t) − Y(t) < τ.
Lemma 3 Suppose the function c(V_{1}, V_{2}, W) has tipping point τ for V_{1} and V_{2}. Then

(i)
The value 0 for ω_{X,Y} can only be reached from ω_{X,Y}(t) with 0 < ω_{X,Y}(t) < 1 if X(t) − Y(t) > τ

(ii)
The value 1 for ω_{X,Y} can only be reached from ω_{X,Y}(t) with 0 < ω_{X,Y}(t) < 1 if X(t) − Y(t) < τ
Proof

(i)
The proof is by contraposition. Suppose 0 < ω_{X,Y}(t) < 1 holds and X(t) − Y(t) > τ does not hold. Then X(t) − Y(t) ≤ τ, and by Definition 1a)(i) and (ii) it follows that c(V_{1}, V_{2}, W) ≥ W, and therefore from the difference equation it follows that ω_{X,Y}(t + Δt) ≥ ω_{X,Y}(t), so ω_{X,Y}(t) will not become lower and in particular will not reach 0.

(ii)
is similar using Definition 1a)(ii) and (iii).
This lemma already reveals that connection weights ω_{X,Y} converging to 0 have some relation to the state values of X and Y having distance more than τ, and connection weights ω_{X,Y} converging to 1 have some relation to the state values of X and Y having a distance less than τ. These relations between connection weights and state values during a convergence process are made more precise for reaching an equilibrium state in Theorem 1.
Theorem 1 (Relations between equilibrium values for states and for connection weights)
Suppose the function c(V_{1}, V_{2}, W) has tipping point τ for V_{1} and V_{2} and an attracting equilibrium state is given with values \( \underline {\mathbf{X}} \) for the states X and \( {\underline {\boldsymbol{\upomega}}}_{X,Y} \) for the connection weights ω_{X,Y}. Then the following hold:

a)
If \( \left\underline {\mathbf{X}}\underline {\mathbf{Y}}\right<\uptau \), then the equilibrium value \( {\underline {\boldsymbol{\upomega}}}_{X,Y} \) is 1; in particular this holds when \( \underline {\mathbf{X}}=\underline {\mathbf{Y}} \). Therefore, if \( {\underline {\boldsymbol{\upomega}}}_{X,Y}<1 \), then \( \left\underline {\mathbf{X}}\underline {\mathbf{Y}}\right\ge \uptau \), and, in particular, \( \underline {\mathbf{X}}\ne \underline {\mathbf{Y}} \).

b)
If \( \left\underline {\mathbf{X}}\underline {\mathbf{Y}}\right>\uptau \), then the equilibrium value \( {\underline {\boldsymbol{\upomega}}}_{X,Y} \) is 0. Therefore, if \( {\underline {\boldsymbol{\upomega}}}_{X,Y}>0 \), then \( \left\underline {\mathbf{X}}\underline {\mathbf{Y}}\right\le \uptau \).

c)
\( 0<{\underline {\boldsymbol{\upomega}}}_{X,Y}<1 \) implies \( \left\underline {\mathbf{X}}\underline {\mathbf{Y}}\right=\uptau \).
Proof

a)
Suppose two states are given with equilibrium values \( \underline {\mathbf{X}} \) and \( \underline {\mathbf{Y}} \) with distance less than \( \uptau :\left\underline {\mathbf{X}}\underline {\mathbf{Y}}\right<\uptau \). Given this, from the equilibrium equation \( {\mathbf{c}}_{\upomega_{X,Y}}\left(\underline {\mathbf{X}},\underline {\mathbf{Y}},{\underline {\boldsymbol{\upomega}}}_{X,Y}\right)={\underline {\boldsymbol{\upomega}}}_{X,Y} \), by Definition 1(ii) it follows that \( 0<{\underline {\boldsymbol{\upomega}}}_{X,Y}<1 \) cannot be true, and therefore \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=0 \) or \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=1 \). By Lemma 3(i) and the equilibrium being attracting it follows that \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=0 \) can be excluded, so \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=1 \).
The other statement, that if \( {\underline {\boldsymbol{\upomega}}}_{X,Y}<1 \), then \( \left\underline {\mathbf{X}}\underline {\mathbf{Y}}\right\ge \uptau \), follows by logical contraposition.

b)
For \( \left\underline {\mathbf{X}}\underline {\mathbf{Y}}\right>\uptau \) this is similar, using Definition 1(iii). The last statement follows from the contraposition of the previous one.

c)
This immediately follows from a) and b).
This Theorem 1 explains some of the observations made in Section 4, in particular, that in all of these simulations the connection weights all end up either in value 0 (the state equilibrium values differ at least τ) or in value 1 (the state equilibrium values are equal).
When also some assumptions are made for social contagion, for example, as explored in (Treur, 2018b) more refined results can be found. The following is a basic Lemma for normalised networks with social contagion combination functions that are monotonically increasing and scalarfree.
Lemma 4
Let a normalised network with nonnegative connections be given with combination functions that are monotonically increasing and scalarfree; then the following hold:

a) (i) If for some state Y at time t for all nodes X with ω_{X,Y} > 0 it holds X(t) ≤ Y(t), then Y(t) is decreasing at t: dY(t)/dt ≤ 0.
(ii) If, moreover, the combination function is strictly increasing and a state X exists with X(t) < Y(t) and ω_{X,Y} > 0, then Y(t) is strictly decreasing at t: dY(t)(t)/dt < 0.

b) (i) If for some state Y at time t for all nodes X with ω_{X,Y} > 0 it holds X(t) ≥ Y(t), then Y(t) is increasing at t: dY(t)/dt ≥ 0.
(ii) If, moreover, the combination function is strictly increasing and a state X exists with X(t) > Y(t) and ω_{X,Y} > 0, then Y(t) is strictly increasing at t: dY(t)(t)/dt > 0.
Proof
The proofs for a) and b) are similar. Therefore only the proof for a) is given.

a)
(i) This proof shows that lower values of the states with incoming connections can never increase the state value of state Y. More specifically, assume for all states X_{i} with (positive) outgoing connections to Y it holds X_{i}(t) ≤ Y(t). Therefore
and by Lemma 2(i) and (iii) this implies dY(t)/dt ≤ 0.

(ii) This proof shows that a strictly lower values of one of the states with incoming connections will actually decrease the state value of state Y. More specifically, from being strictly monotonous it follows
and by Lemma 2(iii) this implies dY(t)/dt < 0.

b)
This can be proven in a similar manner.
Now the more specific theorem is obtained for the connection weights if the combination functions for social contagion for the states are assumed strictly monotonically increasing and scalarfree. It states that the connection weights in an attracting equilibrium are all 0 or 1, and when τ is a strict tipping point, that depends just on whether they connect states with the same or a different equilibrium state value.
Theorem 2 (Equilibrium values \( {\underline {\boldsymbol{\upomega}}}_{X,Y} \) all 0 or 1)
Suppose the network is weakly symmetric and normalised, and the combination functions for the states are strictly monotonically increasing and scalarfree. Suppose that c(V_{1}, V_{2}, W) has a tipping point τ. Then

a)
In an attracting equilibrium state for any states X, Y from \( \underline {\mathbf{X}}\ne \underline {\mathbf{Y}} \) it follows \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=0 \).

b)
In an attracting equilibrium state for any states X, Y with \( \underline {\mathbf{X}}=\underline {\mathbf{Y}} \) it holds \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=0 \) or \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=1 \).

c)
If c(V_{1}, V_{2}, W) has a strict tipping point τ, then in an equilibrium state for any X, Y with \( \underline {\mathbf{X}}=\underline {\mathbf{Y}} \) it holds \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=1 \).
Proof

a)
The proof goes by reductio ad absurdum (reduce to absurdity); it shows that the opposite of the claimed statement cannot be true by deriving a contradiction from this opposite statement. So, suppose (oppositely) that in an attracting equilibrium state, states X and Y exist such that \( \underline {\mathbf{X}}\ne \underline {\mathbf{Y}} \) and \( {\underline {\boldsymbol{\upomega}}}_{X,Y} \), \( {\underline {\boldsymbol{\upomega}}}_{Y,X}>0 \). Take a state X with this property with highest value \( \underline {\mathbf{X}} \). Then for all states Z with \( \mathbf{Z}>\underline {\mathbf{X}} \) it holds \( {\underline {\boldsymbol{\upomega}}}_{X,Z}={\underline {\boldsymbol{\upomega}}}_{Z,X}=0 \). Therefore all states X_{i} with a nonzero (positive) outgoing connection weight to state X satisfy \( {\underline {\mathbf{X}}}_i\le \underline {\mathbf{X}} \). Moreover, one of these X_{i} is state Y with \( \underline {\mathbf{X}}\ne \underline {\mathbf{Y}} \), so, as X has the highest value, it holds \( \underline {\mathbf{Y}}<\underline {\mathbf{X}} \). Now apply Lemma 4a)(ii) to this state X. It follows that dX(t)/dt < 0; therefore X(t) cannot be not in equilibrium. This contradicts the premise that the network is in equilibrium. Therefore no nodes X and Y exist such that \( \underline {\mathbf{X}}\ne \underline {\mathbf{Y}} \) and \( {\underline {\boldsymbol{\upomega}}}_{X,Y} \), \( {\underline {\boldsymbol{\upomega}}}_{Y,X}>0 \). This implies that \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=0 \) and \( {\underline {\boldsymbol{\upomega}}}_{Y,X}=0 \) for all nodes X and Y with \( \underline {\mathbf{X}}\ne \underline {\mathbf{Y}} \).

b)
Also this proof goes by reductio ad absurdum (reduce to absurdity); also here it is shown that the opposite of the claimed statement cannot be true by deriving a contradiction from this opposite statement. So, suppose (oppositely) \( \underline {\mathbf{X}}=\underline {\mathbf{Y}} \) and 0 < ω_{X,Y}(t) < 1. Then by Definition 1a)(i) from X(t) = Y(t) it follows that \( {\mathrm{c}}_{\upomega_{X,Y}}\left(X(t),Y(t),{\upomega}_{X,Y}(t)\right)>{\upomega}_{X,Y}(t) \). From this by Lemma 2(ii) it follows that dω_{X,Y}(t)/dt > 0: ω_{X,Y}(t) is strictly increasing and is not in equilibrium. This contradicts the premise that the network is in equilibrium. Therefore in the equilibrium state when \( \underline {\mathbf{X}}=\underline {\mathbf{Y}} \) it holds \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=0 \) or \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=1 \).

c)
From b) it is already known that \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=0 \) or \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=1 \). The former option \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=0 \) has to be excluded now. Also this goes by reductio ad absurdum (reduce to absurdity); also here it is shown that the option \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=0 \) cannot be true by deriving a contradiction when this option is assumed. So, suppose \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=0 \). If c(V_{1}, V_{2}, W) is strict, and V_{1} – V_{2} < τ then by Definition 1b)(i) it holds c(V_{1}, V_{2}, 0) > 0, so by Lemma 1(ii) it follows that when \( \underline {\mathbf{X}}=\underline {\mathbf{Y}} \), the value \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=0 \) cannot be an equilibrium value, which contradicts the premisse that the network is in equilibrium. Therefore in an equilibrium for any X, Y with \( \underline {\mathbf{X}}=\underline {\mathbf{Y}} \) it holds \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=1 \).
The following theorem shows the implications for emerging communities or clusters and distances between different equilibrium values for nodes.
Theorem 3 (Partition and equilibrium values of nodes)
Suppose the network is weakly symmetric and normalised, the combination function for the states is strictly monotonically increasing and scalarfree, and the combination function for the connections uses tipping point τ and is strict and symmetric. Then in any attracting equilibrium state a partition of the set of states into disjoint subsets C_{1}, .., C_{p} occurs such that:

(i)
For each C_{i} the equilibrium values for all the states in C_{i} are equal: \( \underline {\mathbf{X}}=\underline {\mathbf{Y}} \) for all X, Y ∈ C_{i}.

(ii)
Every C_{i} forms a fully connected network with weights 1: \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=1 \) for all X, Y ∈ C_{i}.

(iii)
Every two nodes in different C_{i} have connection weight 0: when i ≠ j, then X ∈ C_{i} and Y ∈ C_{j} implies \( {\underline {\boldsymbol{\upomega}}}_{X,Y}=0 \).

(iv)
Any two distinct equilibrium values of states \( \underline {\mathbf{X}}\ne \underline {\mathbf{Y}} \) have distance ≥ τ. Therefore there are at most p ≤ 1 + 1/τ communities C_{i} and equilibrium values \( \underline {\mathbf{X}} \).
Proof
Suppose in the equilibrium there are p distinct state values V_{1}, .., V_{p}; then define the sets
It can easily be verified in a straightforward manner that these sets fulfill what is claimed:

(i)
By definition all state values in one C_{i} are equal

(ii)
From Theorem 2c) it follows that all states with equal values have connections 1, therefore any C_{i} is fully connected.

(iii)
This follows from Theorem 2a).

(iv)
Suppose for some X, Y it holds \( \left\underline {\mathbf{X}}\underline {\mathbf{Y}}\right<\uptau \). Then by Definition 1(i) it follows \( {\mathrm{c}}_{\upomega_{X,Y}}\left({V}_1,{V}_2,0\right)>0 \). Therefore 0 cannot be the equilibrium value \( {\underline {\boldsymbol{\upomega}}}_{X,Y} \); from Theorem 2a) it follows that \( \underline {\mathbf{X}}=\underline {\mathbf{Y}} \), and therefore X and Y are in one C_{i}. This implies that the state values in different C_{i} have distance ≥ τ.
Characterising the attracting equilibrium states in terms of strongly connected components
To analyse connectivity, within Graph Theory the notion of a strongly connected component has been identified. The main parts of the following definitions can be found, for example, in (Harary et al. 1965), Ch. 3, or (Kuich 1970), Section 6. Note that in the current paper only nonnegative connection weights are considered.
Definition 6 (reachability and strongly connected components)

(a)
State Y is forward reachable from state X if there is a directed path from X to Y with nonzero connection weights and speed factors.

(b)
A network N is strongly connected if every two states are mutually forward reachable within N.

(c)
A state is called independent if it is not forward reachable by any other state.

(d)
A subnetwork of a network N is a network whose states and connections are states and connections of N.

(e)
A strongly connected component C of a network N is a strongly connected subnetwork of N such that it is maximal: no larger strongly connected subnetwork of N contains it as a subnetwork.
Strongly connected components C can be identified by choosing any node X of N and adding all nodes that are on any cycle through X. Note also that when a node X is not on any cycle, then it will form a singleton strongly connected component C by itself; this applies in particular to all nodes of N with indegree or outdegree zero. There are efficient algorithms available to determine the strongly connected components of a network or graph; for example, see (Bloem et al. 2006; Chen 2009; Fleischer et al. 2000; Gentilini et al. 2003; Łacki 2013; Li et al. 2014; Tarjan 1972; Wijs et al. 2016).
The strongly connected components form a partition of the nodes of the graph or network. By this partition a more abstract, simpler view of the network can be created, called condensation graph, in which each component becomes one abstract node; this is defined as follows.
Definition 7 (condensation graph)
The condensation graph C(N) of a network N with respect to its strongly connected components is a graph whose nodes are the strongly connected components of N and whose connections are determined as follows: there is a connection from node C_{i} to node C_{j} in C(N) if and only if in N there is at least one connection from a node in the strongly connected component C_{i} to a node in the strongly connected component C_{j}.
An important result is that a condensation graph C(N) is always an acyclic graph. In a sense, all cycles are locked up inside the components, and the connections between these components do not contain any cycles. The following theorem summarizes this; it was adopted from (Harary et al. 1965), Ch. 3, Theorems 3.6 and 3.8, or (Kuich 1970), Section 6.
Theorem 4 (Acyclic condensation graph)

a)
For any network N its condensation graph C(N) is acyclic, and has at least one state of outdegree zero and at least one state of indegree zero.

b)
The network N is acyclic itself if and only if it is graphisomorphic to C(N). In this case, the nodes in C(N) all are singleton sets {X} containing one state X from N.

c)
The network N is strongly connected itself if and only if C(N) only has one node; this node is the set of all states of N.
Note that in an adaptive network, the strongly connected components and the condensation graph usually change over time. For example, connection weights that were 0 can become nonzero, or nonzero connection weights can converge to 0. From Theorem 3 it immediately follows that in the equilibrium state the C_{i} defined there are the strongly connected components of the network. Then the results from Theorem 3 can be rephrased in the above terms in the following way.
Theorem 5 (Strongly connected components in an attracting equilibrium)
Suppose the network is weakly symmetric and normalised, the combination functions for social contagion between the nodes is strictly monotonically increasing and scalarfree, and the homophily combination function for the connections uses tipping point τ and is strict and symmetric. Then in any attracting equilibrium state the following hold:

(i)
There are at most p ≤ 1 + 1/τ strongly connected components.

(ii)
Each strongly connected component is fully connected and all states in it have a common equilibrium state value.

(iii)
There are no nonzero connections between states from different strongly connected components, and the equilibrium values of these states have distance ≥ τ.

(iv)
The condensation graph C(N) is totally disconnected: it has no connections at all.
The following converse holds as well; this shows how equilibrium states can be characterised by specific properties of the strongly connected components.
Theorem 6 (Strongly connected components characterisation)
Suppose the network is weakly symmetric, the combination function for social contagion between the nodes is strictly monotonically increasing, normalised and scalarfree, and the homophily combination function for the connections uses tipping point τ and is strict and symmetric. Suppose at some time point t the following hold:

(i)
Each strongly connected component C is fully connected and all states in C have a common state value.

(ii)
All connections between states from different strongly connected components have weight 0 and the equilibrium values of these states have distance > τ.
Then the network is in an equilibrium state.
Proof
First in a) it is proven that the state values are stationary; next, in b) it is proven that the connection weights are stationary. Having both stationary, the network is in equilibrium.

a)
Consider within any component C any state Y which has only nonzero incoming connections from states X_{1}, …, X_{k}. Due to (ii) these necessarily belong to the same component C. As within C the state values are equal to one value V and each connection has weight 1 the following holds
and therefore by Lemma 2(i) it holds dY(t)/dt = 0, so Y(t) is stationary.

b)
Next, it is proven that the connection weights are stationary. Consider the connection weight ω_{X,Y} for the connection from states X to Y in the same component C. Suppose as a perturbation from 1 it holds ω_{X,Y}(t) < 1. Given that X(t)  Y(t) < τ, from Definition 1(i) it follows that \( {\mathbf{c}}_{\upomega_{X,Y}}\left(X(t),Y(t),{\upomega}_{X,Y}(t)\right)>{\upomega}_{X,Y}(t) \), and therefore dω_{X,Y}(t)/dt > 0, so it would move upward to 1. Therefore ω_{X,Y} is stationary. A similar argument for states X and Y in different components shows that ω_{X,Y} would move downward to 0, and therefore is stationary.
As both the states and the connection weights have been proven stationary, it has been found that the network is in equilibrium.
Note that the situation as characterised is a quite specific situation with trivial condensation graph, if compared, for example, to a general situation as addressed in (Treur 2018d), where usually nontrivial condensation graphs occur.
Overview of simulation experiments
In recent years for a number of the functions from Table 2 simulation experiments have been performed for realworld domains and related to empirical data. An overview of them is shown in Table 4. Some of the experiences are the following.
In general, it was possible to get similar patterns as in the empirical data by using dedicated Parameter Tuning methods such as Simulated Annealing. As may be expected the remaining Root Mean Square error differed with the different studies and domains, and also depends on how finegrained the scoring scales for the data were; for example when a 3 points scale was used for empirical data, already because of that in the [0, 1] interval a variation of 0.15 should be expected within the empirical data themselves, and for a 5 points scale 0.1. Then an average deviation between model and empirical data will be at least in that order of magnitude, not smaller, say 0.15 to 0.25. This indeed was usually the case in the examples discussed in Table 4.
Using the simple linear or simple quadratic functions slhomo_{σ,τ}(..) or sqhomo_{σ,τ}(..) the change of connection weights is very slow when the weights are close to 0 or 1 due to the factor W (1  W) in the function. The advantage of this slowing down effect is that the connection weight values stay within the [0, 1] interval in a natural manner. But the downside of this factor is that when they are exactly 0 or 1 they will even freeze and not be able to change anyway, and the same when 0 or 1 are used as initial values. This is because slhomo_{σ,τ}(..) or sqhomo_{σ,τ}(..) have a tipping point, but no strict tipping point; also see the remark after Definition 1. The same holds for log2homo_{σ,τ}(..). So, when these functions are used, it is better to initialise all connection weight values between 0.1 and 0.9 instead of in the full [0, 1] interval. This is different for the advanced linear and quadratic homophily functions alhomo_{σ,τ}(..) or aqhomo_{σ,τ}(..). For them approaching 0 or 1 is still slow, but leaving 0 or 1 can be fast: they do have a strict tipping point. Note, however, that this is not necessarily always a good property. Maybe when a very strong connection has been formed, even some differences that occur may not affect the connection immediately. So, in some cases, or for some types of persons the slow change close to 0 or 1 as shown by slhomo_{σ,τ}(..) or sqhomo_{σ,τ}(..) may even be more plausible.
Note that in (Kozyreva et al. 2018) a slightly different multicriteria variant of the simple linear homophily function was used that takes into account multiple states in the similarity measure: instead of  V_{1}– V_{2}  for 1 criterion, for k criteria the following Euclidean distance formula is used to measure similarity:
In (Blankendaal et al. 2016) and (van Beukel et al. 2017) for bonding not only a homophily principle was used, but also a ‘more becomes more’ principle which can be considered a variant of what sometimes is called ‘the rich get richer’ (Simon 1955; Bornholdt and Ebel 2001), ‘cumulative advantage’ (Price 1976), ‘the Matthew effect’ (Merton 1968), or ‘preferential attachment’ (Barabási and Albert 1999; Newman 2003). For this ‘more becomes more’ principle, in (Blankendaal et al. 2016) a scaled sum combination function was used for the weights of the connections to a given other person Y with scaling factor the number k of such connections (resulting in the average of these connection weights), and in (van Beukel et al. 2017; van Beukel et al. 2019) and advanced logistic sum:
where W_{1}, …, W_{k} refer to the weights \( {\upomega}_{X_1,Y},\dots, {\upomega}_{X_k,Y} \) of all connections of the other person Y. Note that the first scaled sum option ssum_{k}(..) adapts to the other person’s average connection weight independent of the number of connections, whereas the second alogistic_{σ,τ}(…) option is more additive as more connections of the other person provide higher values. In both approaches, the two combination functions for both the homophily and the more becomes more principle were combined as a weighted sum.
Discussion
In this paper, it was analysed how community formation can be related to characteristics of the adaptive network’s structure, in particular in an adaptive network for bonding based on similarity. Here network structure includes the structure (and settings) of the adaptation principles incorporated. This has been addressed for adaptive social networks for bonding based on homophily (McPherson et al. 2001; Pearson et al. 2006). Relevant properties of the network and the adaptation principle have been identified, such as a tipping point for similarity. As one of the results, it has been found how the emergence of communities strongly depends on the value of this tipping point. It has been shown, for example, that some properties of the structure of the network and the adaptation principle entail that the connection weights all converge to 0 (for persons in different communities) or 1 (for persons within one community). As another main result, it has been found that the formation of communities strongly depends on the value τ of this tipping point; there can be no more communities than 1 + 1/τ within the interval [0, 1].
The presented results do not concern results for just one type of network or function, as more often is found. Instead, they were formulated and proven at a more general level and therefore can be applied not just to specific networks but to classes of networks satisfying the identified relevant properties of network structure and adaptation characteristics. Note, however, that the focus in the current paper is on deterministic behaviour; therefore stochastic models such as, for example, the one reported in a nontechnical manner in (Axelrod 1997), are not covered by this analysis; e.g., see the description here:
For those who prefer symbolic statements, here is a complete description of how the culture, c, at a site can change. Select a random site (s), a random neighbor of that site (n), and a random feature (f). Let G(s,n) be the set of features, g, such that the cultural traits are unequalthat is, c(s,g) ≠ c(n,g). If c(s,f) = c(n,f) and G is not empty, then select a random feature, g, in G(s,n) and set c(s,g) to c(n,g). This implementation of the model takes advantage of that fact that the probability that a random feature, f , will have the same trait at two sites equals the cultural similarity between those two sites. (Axelrod 1997), p. 208, footnote 4
It may be an interesting research focus for the future to explore whether and how the analysis results found here have counterparts for stochastic network models. Besides, in (Axelrod 1997) also regional differences are addressed. In a more extensive application of the models discussed in the current paper, that may be an interesting ingredient to address as well.
The results found also have been related to the strongly connected components of the network (Harary et al. 1965), Ch. 3, or (Kuich 1970), Section 6). A characterisation in terms of properties of the strongly connected components and their relations was found for states of an adaptive network which are attracting equilibrium states.
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Treur, J. Mathematical analysis of the emergence of communities based on coevolution of social contagion and bonding by homophily. Appl Netw Sci 4, 39 (2019). https://doi.org/10.1007/s4110901901307
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DOI: https://doi.org/10.1007/s4110901901307