| Literature DB >> 31242270 |
Michael T Gastner1,2, Károly Takács2,3, Máté Gulyás2,4, Zsuzsanna Szvetelszky2, Beáta Oborny4,5.
Abstract
Humans have a demonstrated tendency to copy or imitate the behavior and attitude of others and actively influence each other's opinions. In plenty of empirical contexts, publicly revealed opinions are not necessarily in line with internal opinions, causing complex social influence dynamics. We study to what extent hypocrisy is sustained during opinion formation and how hidden opinions change the convergence to consensus in a group. We build and analyze a modified version of the voter model with hypocrisy in a complete graph with a neutral competition between two alternatives. We compare the process from various initial conditions, varying the proportions between the two opinions in the external (revealed) and internal (hidden) layer. According to our results, hypocrisy always prolongs the time needed for reaching a consensus. In a complete graph, this time span increases linearly with group size. We find that the group-level opinion emerges in two steps: (1) a fast and directional process, during which the number of the two kinds of hypocrites equalizes; and (2) a slower, random drift of opinions. During stage (2), the ratio of opinions in the external layer is approximately equal to the ratio in the internal layer; that is, the hidden opinions do not differ significantly from the revealed ones at the group level. We furthermore find that the initial abundances of opinions, but not the initial prevalence of hypocrisy, predicts the mean consensus time and determines the opinions' probabilities of winning. These insights highlight the unimportance of hypocrisy in consensus formation under neutral conditions. Our results have important societal implications in relation to hidden voter preferences in polls and improve our understanding of opinion formation in a more realistic setting than that of conventional voter models.Entities:
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Year: 2019 PMID: 31242270 PMCID: PMC6594623 DOI: 10.1371/journal.pone.0218729
Source DB: PubMed Journal: PLoS One ISSN: 1932-6203 Impact factor: 3.240
Fig 3Changes in the composition of the group over time in four realizations of the CVM.
Each point belongs to one “snapshot” between the initial state (large, filled symbols) and the consensus (large, open symbols). The parameters for all simulations are N = 400, c = 1, e = 1/4, i = 1/16. We show only a single simulation for each initial condition, but we note that repeated simulations from the same initial state can end in either of the absorbing states unless the initial state is already a consensus. The time intervals between the plotted points change along the trajectories: during the transient, we plot every 100th time step until the 2000th time step. Afterwards we plot only every 10000th time step because the spatial density of data points is higher along the attractor. (A) Abundances of the two kinds of hypocrites (ρRb and ρBr) and the proportion of frank red individuals (ρRr). These variables completely describe the state of the system. The theoretical attractor ( is shown as a black curve. (B) Equalization of the two kinds of hypocrites in the same realizations. In a consensus, there are no hypocrites (i.e., ρRb = ρBr = 0). Therefore, the open symbols at the consensus overlap. The attractor appears as a straight line because it is a two-dimensional projection of the curve embedded in three dimensions. The line is exactly on the diagonal. (C) Equalization of the abundance of the red opinion in the external (ρR = ρRb+ρRr) and internal layer (ρr = ρBr+ρRr). The attractor (black line) is exactly on the diagonal.
Contingency table showing the fraction of individuals with different combinations of external and internal opinions.
| External opinion | ||||
|---|---|---|---|---|
| sum | ||||
| Internal opinion | ||||
| sum | 1 | |||
The four cases of CVM simulations that are displayed in Figs 3 and 4.
| Symbol & Color | ■ | ▲ | ◆ | ▼ | |
|---|---|---|---|---|---|
| 0.00 | 0.25 | 0.50 | 0.75 | ||
| 1.00 | 0.75 | 0.25 | 0.00 | ||
| 0.00 | 0.00 | 0.25 | 0.00 | ||
| 0.81±0.02 | 0.65±0.03 | 0.57±0.03 | 0.17±0.02 | ||
| 0.80 | 0.65 | 0.55 | 0.15 | ||
| 2630±160 | 3270±160 | 3470±150 | 2090±140 | ||
| 2563.0 | 3316.2 | 3524.6 | 2165.1 | ||
| 3.23±0.05 | 3.23±0.11 | 3.14±0.23 | 3.15±0.07 | ||
| 3.2 | |||||
The top row shows the symbols and colors used in the figures. The next three rows show the initial conditions. The remaining rows compare measurements from simulations (N = 400, c = 1, e = 1/4, i = 1/16) with theoretical values. Each measurement is the sample mean of 1000 simulations. Uncertainties are given as 95% confidence intervals. It is noteworthy that the time until consensus is much longer than the equalization time Tequal. (See Section 4.2 for the definition of Tequal.)