Neil F. Johnson’s research while affiliated with University of Washington and other places

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Publications (281)


Multispecies Cohesion: Humans, Machinery, AI, and Beyond
  • Article
  • Full-text available

December 2024

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11 Reads

Physical Review Letters

Frank Yingjie Huo

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Neil F. Johnson

The global chaos caused by the July 19, 2024 technology meltdown highlights the need for a theory of what large-scale cohesive behaviors—dangerous or desirable—could suddenly emerge from future systems of interacting humans, machinery, and software, including artificial intelligence; when they will emerge; and how they will evolve and be controlled. Here, we offer answers by introducing an aggregation model that accounts for the interacting entities’ inter- and intraspecies diversities. It yields a novel multidimensional generalization of existing aggregation physics. We derive exact analytic solutions for the time to cohesion and growth of cohesion for two species, and some generalizations for an arbitrary number of species. These solutions reproduce—and offer a microscopic explanation for—an anomalous nonlinear growth feature observed in various current real-world systems. Our theory suggests good and bad “surprises” will appear sooner and more strongly as humans, machinery, artificial intelligence, and so on interact more, but it also offers a rigorous approach for understanding and controlling this.

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How U.S. Presidential elections strengthen global hate networks

October 2024

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32 Reads

Local or national politics can be a catalyst for potentially dangerous hate speech. But with a third of the world’s population eligible to vote in 2024 elections, we need an understanding of how individual-level hate multiplies up to the collective global scale. We show, based on the most recent U.S. presidential election, that offline events are associated with rapid adaptations of the global online hate universe that strengthens both its network-of-networks structure and the types of hate content that it collectively produces. Approximately 50 million accounts in hate communities are drawn closer to each other and to a broad mainstream of billions. The election triggered new hate content at scale around immigration, ethnicity, and antisemitism that aligns with conspiracy theories about Jewish-led replacement. Telegram acts as a key hardening agent; yet, it is overlooked by U.S. Congressional hearings and new E.U. legislation. Because the hate universe has remained robust since 2020, anti-hate messaging surrounding global events (e.g., upcoming elections or the war in Gaza) should pivot to blending multiple hate types while targeting previously untouched social media structures.


Multi-species framework. A Schematics of the system, interactions and dynamics of 4 co-evolving species of different sizes, interaction rates, and properties: I (green), II (brown), III (red) and IV (blue). Within species heterogeneity is enabled by the function y(j)(t)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$y^{(j)}(t)$$\end{document} for species j, which ranges from 0 to 1 and it could change over time. The central panel illustrates the state of the system at three specific times. Species I and II co-evolve without mixing, i.e., they form pure clusters, while species III and IV form mixed clusters. Clusters occasionally experience total fragmentation (i.e., fission). The bottom panel shows the size of the Giant Connected Component (GCC) of the pure and the mixed sub-systems pointing to large scale events such as the onset and total fission. B Dynamics of monomers in a system of k=4\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$k=4$$\end{document} species as a function of time, where the theoretical results are compared with those from microscopic simulations. The parameters are: N1=700\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$N_1=700$$\end{document} (magenta), N2=600\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$N_2=600$$\end{document} (cyan), N3=400\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$N_3=400$$\end{document} (orange), N4=300\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$N_4=300$$\end{document} (gray), the elements of the F-matrix are f11=f44=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{11}=f_{44}=1$$\end{document}, f22=1/2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{22}=1/2$$\end{document}, f33=2/3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{33}=2/3$$\end{document}, fij=(1/3)δ2,3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{ij}=(1/3)\delta _{2,3}$$\end{document}, where δi,j\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\delta _{i,j}$$\end{document} is the Kronecker delta with i,j=1,...,k\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$i,j=1,...,k$$\end{document} for all i≠j\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$i\ne j$$\end{document}. C. Onset time as a function of the ratio of cross-species interaction ε\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\varepsilon $$\end{document} to the same-species interaction f, for a system of k species for the cases shown.
Fusion mechanisms in the two-species system. GCC onset time ton\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$t_{on}$$\end{document} and occupancy ηj\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\eta _j$$\end{document} for a 2-species system as a function of the cross-species interaction ε\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\varepsilon $$\end{document}, and the species concentration ratio N1/N2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$N_1/N_2$$\end{document} (N2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$N_2$$\end{document} is kept fixed at 500 objects). Each panel shows a large plot of the onset time for the cases of weak (solid curve) and strong (dashed curve) ε\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\varepsilon $$\end{document}. In addition, two smaller plots indicate the GCC composition for each species (red and blue are species 1 and 2, respectively) these two values of ε\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\varepsilon $$\end{document} (top plot), and the full landscape of the onset time as a function of ε\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\varepsilon $$\end{document} and the concentration ratio (bottom plot). Af1>f2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_1>f_2$$\end{document} (f1=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_1=1$$\end{document}, f2=1/3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_2=1/3$$\end{document}). Bf1<f2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_1<f_2$$\end{document} ( f1=2/3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_1=2/3$$\end{document}, f2=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_2=1$$\end{document}). In all cases the solid curve indicates ε=0.1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\varepsilon =0.1$$\end{document}, and the dashed curve ε=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\varepsilon =1$$\end{document}.
Fibrils formation in a biomolecular condensate. A Schematics of the dynamical phases of the amyloid peptide aggregation process. Starting from a dilute solution of monomeric peptides (left panel), dimers, trimers and higher order oligomers form through a first nucleation process yielding an oligomeric state (central panel). Resultant oligomers fuse with each other through a second nucleation yielding the solid β\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta $$\end{document}-rich aggregated phase akin to the emergence of the GCC in a dynamical network. B Experimental aggregation profiles (squares) of 3.5 μ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mu $$\end{document}M Aβ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta $$\end{document}-42 peptide solution in different concentrations of LCD Dpb1N-AK-Dpb1N as reported in ref.⁶, and our two-species theory (curves). The LCD concentrations are: 0μ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0\,\mu $$\end{document}M (magenta), 2μ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$2\,\mu $$\end{document}M (orange), 5μ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$5\,\mu $$\end{document}M (blue), and 10μ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$10\,\mu $$\end{document}M (black). Accordingly, the theory uses values of concentration of species 1 (i.e., biomolecular condensate) following identical proportions (respectively, N1=0,400,1000,2000\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$N_1=0, 400, 1000, 2000$$\end{document}), while species 2 (i.e., the amyloid system) is kept constant (N2=500\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$N_2=500$$\end{document} objects). C Fitting parameters (ε\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\varepsilon $$\end{document} and f1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_1$$\end{document}) for the different concentrations. Dashed and dotted lines are exponential and linear fits, respectively. Error bars are the associated standard errors. D Impact of dynamical changes in the concentration of the condensates in the phases of the fibril formation. The concentration increases/decreases at a constant rate q (q≈-10,0,+10\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$q\approx -10,0,+10$$\end{document} nM/min). Arrows point the direction the amyloid sub-system takes due to the perturbation: orange is q>0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$q>0$$\end{document}, and green is q<0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$q<0$$\end{document}. E Theoretical prediction of the impact of dynamical variations in the condensates’ concentration on the fibril onset. If the concentration growth rate reaches a threshold q∗≥110\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$q*\ge 110$$\end{document}nM/min, the fibril will not be formed.
Emergence of vaccines distrust in online networks. A Online vaccination views network according to public Facebook pages identified in December 2020. The color of the nodes indicates the views of the specific page: ’pro’ (blue), ’anti’ (red), and ’neutral’ (green). B Model system constructed with our 3 species theory with parameters estimated from the real network system in A and using the same color code. C GCC composition of the model system at the onset time (η(ton)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\eta (t_{on})$$\end{document}) showing the dominance of the ’anti’ category from the early stage. D Impact in the GCC composition at the onset by altering the cohesiveness (i.e., fii\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{ii}$$\end{document}) of the pro (top panel) and the anti (bottom panel). Orange vertical line in all panels of D and E point to the unperturbed parameter value for each case. E Impact in the GCC composition at the onset by altering the number of active fronts (i.e., Nj\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$N_{j}$$\end{document}) of the pro (top panel) and the anti (bottom panel). F Impact in the GCC composition at the onset by altering the level of engagement for all sides of the debate: pro (left), anti (center), and neutral (right), as a function of different sets of interaction parameters: fPA\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{\mathcal{P}\mathcal{A}}$$\end{document} versus fPN\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{\mathcal{P}\mathcal{N}}$$\end{document} (top row), fPA\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{\mathcal{P}\mathcal{A}}$$\end{document} versus fAN\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{\mathcal{A}\mathcal{N}}$$\end{document} (central row), fAN\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{\mathcal{A}\mathcal{N}}$$\end{document} versus fPN\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{\mathcal{P}\mathcal{N}}$$\end{document} (bottom row). The star on each panel points to the real values of fPA\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{\mathcal{P}\mathcal{A}}$$\end{document}, fPN\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{\mathcal{P}\mathcal{N}}$$\end{document}, and fAN\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f_{\mathcal{A}\mathcal{N}}$$\end{document} estimated from the real data in A as shown in Table 1.
Non-equilibrium physics of multi-species assembly applied to fibrils inhibition in biomolecular condensates and growth of online distrust

September 2024

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21 Reads

Self-assembly is a key process in living systems—from the microscopic biological level (e.g. assembly of proteins into fibrils within biomolecular condensates in a human cell) through to the macroscopic societal level (e.g. assembly of humans into common-interest communities across online social media platforms). The components in such systems (e.g. macromolecules, humans) are highly diverse, and so are the self-assembled structures that they form. However, there is no simple theory of how such structures assemble from a multi-species pool of components. Here we provide a very simple model which trades myriad chemical and human details for a transparent analysis, and yields results in good agreement with recent empirical data. It reveals a new inhibitory role for biomolecular condensates in the formation of dangerous amyloid fibrils, as well as a kinetic explanation of why so many diverse distrust movements are now emerging across social media. The nonlinear dependencies that we uncover suggest new real-world control strategies for such multi-species assembly.


Simple fusion-fission quantifies Israel-Palestine violence and suggests multi-adversary solution

September 2024

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40 Reads

Frank Yingjie Huo

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Dylan J. Restrepo

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[...]

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Neil F. Johnson

Why humans fight has no easy answer. However, understanding better how humans fight could inform future interventions, hidden shifts and casualty risk. Fusion-fission describes the well-known grouping behavior of fish etc. fighting for survival in the face of strong opponents: they form clusters ('fusion') which provide collective benefits and a cluster scatters when it senses danger ('fission'). Here we show how similar clustering (fusion-fission) of human fighters provides a unified quantitative explanation for complex casualty patterns across decades of Israel-Palestine region violence, as well as the October 7 surprise attack -- and uncovers a hidden post-October 7 shift. State-of-the-art data shows this fighter fusion-fission in action. It also predicts future 'super-shock' attacks that will be more lethal than October 7 and will arrive earlier. It offers a multi-adversary solution. Our results -- which include testable formulae and a plug-and-play simulation -- enable concrete risk assessments of future casualties and policy-making grounded by fighter behavior.


Nonlinear spreading behavior across multi-platform social media universe

April 2024

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27 Reads

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1 Citation

Understanding how harmful content (mis/disinformation, hate, etc.) manages to spread among online communities within and across social media platforms represents an urgent societal challenge. We develop a non-linear dynamical model for such viral spreading, which accounts for the fact that online communities dynamically interconnect across multiple social media platforms. Our mean-field theory (Effective Medium Theory) compares well to detailed numerical simulations and provides a specific analytic condition for the onset of outbreaks (i.e., system-wide spreading). Even if the infection rate is significantly lower than the recovery rate, it predicts system-wide spreading if online communities create links between them at high rates and the loss of such links (e.g., due to moderator pressure) is low. Policymakers should, therefore, account for these multi-community dynamics when shaping policies against system-wide spreading.


Fig. 2 | Empirical data (symbols) vs. mathematical solutions of the deterministic governing equations (curves, derivation SI Sec. 4.1). a Relative number of links created at time t from hate communities on a given platform (source). b Relative number of links created at time t to other communities on a given platform (target). Approximately 80% of targets are hate-vulnerable mainstream communities. Only the largest curves are shown, the rest are aggregated as 'Other' (black curves). c, d Same as plots a and b but applied to Jan 4-5 data using different time points.
Fig. 3 | Simulations with context of a network map. a Dynamical network aggregated over 2.5 years' worth of social media data. Each colored node is a hate community. Each white node is a hate-vulnerable mainstream community to which a hate node has a direct link. Edges are colored the same color as their source node. Generally, the areas of color visible in this network are space between nodes filled by dense edges. Side panels compare platforms' involvement by only highlighting edges that originate from hate nodes on a given platform. 2023 Texas shooter's YouTube community is shown, so too is a major Wagner mercenary community on Telegram (Reverse Side of the Medal). See SI for others and an example zoom-in (dotted box, Suppl. Fig. 15). Network layout is generated by the ForceAtlas2 algorithm 68 : sets of communities appear closer together when they share more links. b Comparing mitigation schemes' effects on network topology, modeled after robustness tests
Adaptive link dynamics drive online hate networks and their mainstream influence

April 2024

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29 Reads

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2 Citations

Online hate is dynamic, adaptive— and may soon surge with new AI/GPT tools. Establishing how hate operates at scale is key to overcoming it. We provide insights that challenge existing policies. Rather than large social media platforms being the key drivers, waves of adaptive links across smaller platforms connect the hate user base over time, fortifying hate networks, bypassing mitigations, and extending their direct influence into the massive neighboring mainstream. Data indicates that hundreds of thousands of people globally, including children, have been exposed. We present governing equations derived from first principles and a tipping-point condition predicting future surges in content transmission. Using the U.S. Capitol attack and a 2023 mass shooting as case studies, our findings offer actionable insights and quantitative predictions down to the hourly scale. The efficacy of proposed mitigations can now be predicted using these equations.


Vulnerability of Quantum Information Systems to Collective Manipulation

April 2024

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53 Reads

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1 Citation

The highly specialist terms ‘quantum computing’ and ‘quantum information’, together with the broader term ‘quantum technologies’, now appear regularly in the mainstream media. While this is undoubtedly highly exciting for physicists and investors alike, a key question for society concerns such systems’ vulnerabilities – and in particular, their vulnerability to collective manipulation. Here we present and discuss a new form of vulnerability in such systems, that we have identified based on detailed many-body quantum mechanical calculations. The impact of this new vulnerability is that groups of adversaries can maximally disrupt these systems’ global quantum state which will then jeopardize their quantum functionality. It will be almost impossible to detect these attacks since they do not change the Hamiltonian and the purity remains the same; they do not entail any real-time communication between the attackers; and they can last less than a second. We also argue that there can be an implicit amplification of such attacks because of the statistical character of modern non-state actor groups. A countermeasure could be to embed future quantum technologies within redundant classical networks. We purposely structure the discussion in this chapter so that the first sections are self-contained and can be read by non-specialists.


Multi-Species Cohesion: Humans, machinery, AI and beyond

February 2024

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44 Reads

What large-scale cohesive behaviors-desirable or dangerous-can suddenly emerge from systems with interacting humans, machinery and software including AI? When will they emerge? How will they evolve and be controlled? Here we offer some answers to these urgent questions by introducing an aggregation model that accounts for entities' inter-and intra-species diversities. It yields a novel multi-dimensional generalization of existing aggregation physics. We derive exact analytic solutions for the time-to-cohesion and growth-of-cohesion for two species, and some generalizations for an arbitrary number of species. These solutions reproduce-and offer a microscopic explanation for-an anomalous nonlinear growth feature observed in related real-world systems, e.g. Hamas-Hezbollah online support, human-machine team interactions, AI-determined topic coherence. A key takeaway is that good and bad 'surprises' will appear increasingly quickly as humans-machinery-AI etc. mix more-but the theory offers a rigorous approach for understanding and controlling this.


Controlling bad-actor-artificial intelligence activity at scale across online battlefields

January 2024

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69 Reads

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2 Citations

PNAS Nexus

We consider the looming threat of bad actors using artificial intelligence (AI)/Generative Pretrained Transformer to generate harms across social media globally. Guided by our detailed mapping of the online multiplatform battlefield, we offer answers to the key questions of what bad-actor-AI activity will likely dominate, where, when—and what might be done to control it at scale. Applying a dynamical Red Queen analysis from prior studies of cyber and automated algorithm attacks, predicts an escalation to daily bad-actor-AI activity by mid-2024—just ahead of United States and other global elections. We then use an exactly solvable mathematical model of the observed bad-actor community clustering dynamics, to build a Policy Matrix which quantifies the outcomes and trade-offs between two potentially desirable outcomes: containment of future bad-actor-AI activity vs. its complete removal. We also give explicit plug-and-play formulae for associated risk measures.


Network Composition Across Different Softening Scenarios
Softening Online Extremes Using Network Engineering

January 2024

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18 Reads

IEEE Access

The prevalence of dangerous misinformation and extreme views online has intensified since the onset of Israel-Hamas war on 7 October 2023. Social media platforms have long grappled with the challenge of providing effective mitigation schemes that can scale to the 5 billion-strong online population. Here, we introduce a novel solution grounded in online network engineering and demonstrate its potential through small pilot studies. We begin by outlining the characteristics of the online social network infrastructure that have rendered previous approaches to mitigating extremes ineffective. We then present our new online engineering scheme and explain how it circumvents these issues. The efficacy of this scheme is demonstrated through a pilot empirical study, which reveals that automatically assembling groups of users online with diverse opinions, guided by a map of the online social media infrastructure, and facilitating their anonymous interactions, can lead to a softening of extreme views. We then employ computer simulations to explore the potential for implementing this scheme online at scale and in an automated manner, without necessitating the contentious removal of specific communities, imposing censorship, relying on preventative messaging, or requiring consensus within the online groups. These pilot studies provide preliminary insights into the effectiveness and feasibility of this approach in online social media settings.


Citations (53)


... The rapid spread of deepfakes through social media and digital platforms poses significant challenges due to the interconnected nature of online communities and the persuasive power of multimedia content. Deepfakes proliferate across multiple platforms, with interconnected online communities facilitating rapid sharing, even when the initial "infection" rate is low (Xia & Johnson, 2024). The decentralized nature of social media allows personal accounts, rather than automated bots, to be primary spreaders of fake content, including deepfakes (Dourado, 2023). ...

Reference:

The Relationship of Digital Literacy, Exposure to AI-Generated Deepfake Videos, and the Ability to Identify Deepfakes in Generation XHubungan Literasi Digital, Paparan Video Deepfake yang Dihasilkan AI, dan Kemampuan untuk Mengidentifikasi Deepfake pada Generasi X
Nonlinear spreading behavior across multi-platform social media universe

... This would open the use of photons and topological matter-connected states for new strategies to harness non-classical aspects of both matter and radiation ranging from fundamental physics aspects to potential applications in quantum information/computation issues. This becomes even more relevant in powerful platforms with novel quantum materials strongly coupled to optical and microwave cavities [13][14][15][16][17][18] where photon quantum states, specifically coherent and squeezed states, show great promise in this regard due to the ease of availability and well-established control techniques. ...

Vulnerability of Quantum Information Systems to Collective Manipulation

... Thus, a recent study from Mexico argues that "political speeches frequently use fallacies to sway voters during electoral campaigns" (Nieto-Benitez et al., 2023). Analysing the use of AI for malicious political purposes, a number of researchers characterize them as "bad actors" and express fears that they will "generate harms across social media globally" (Johnson, Sear, & Illari, 2023) and their influence will grow. However, the use of generated false or misleading information is already a legal and ethical issue. ...

Controlling bad-actor-artificial intelligence activity at scale across online battlefields

PNAS Nexus

... In much of this work, there is a binary classification for coordinated and non-coordinated users by choosing a high cosine similarity or Jaccard coefficient as a threshold beyond which users are considered coordinated [15,16,13,11]. This approach has been demonstrated with respect to the promotion of influencers, hashtags, websites, and account handle swapping, to name some of the most prominent behavior dimensions considered [16,10,11,20]. ...

Inductive detection of influence operations via graph learning

... The COVID-19 pandemic exacerbated existing global health issues including health inequities, mental health, social isolation, and addictions [17,18]. Additionally, declining trust in public health resulted from ineffective crisis communication and management [19], and a complex information ecosystem where mis/disinformation is widely circulating [20]. More than ever, public health needs competency frameworks that reflect the current multifaceted and overlapping public health challenges to ensure the workforce is adequately equipped to address them. ...

Rise of post-pandemic resilience across the distrust ecosystem

... Each entity p within a given species α can have an arbitrary number of additional intraspecies traits that could in principle change over time, denoted as ⃗ y p;α ðtÞ. Each component (trait value) lies between 0 and 1 [41,[51][52][53][54][55][56][57][58]. ...

Shockwavelike Behavior across Social Media

Physical Review Letters

... The recovery of historical weather observations from paper archives is informing our knowledge and understanding of the risks from extreme weather. Any approach to estimating risk by identifying plausible worst-case outcomes (Thompson et al., 2017) or developing storylines of severe weather events (Shepherd et al., 2018) would benefit from longer sampling of real-world behaviour and improved historical knowledge (Woo and Johnson, 2018;Pinto et al., 2019). ...

Stochastic Modeling of Possible Pasts to Illuminate Future Risk
  • Citing Chapter
  • March 2023

... This difficulty arises because the data, deeply embedded in platform interactions, complicate separating intrinsic human behavior from the influences exerted by the platform's design and algorithms. Research has delved deeply into issues such as polarization, misinformation, and antisocial behaviors in digital spaces [9][10][11][12][13], highlighting the intricate and multifaceted effects of social networks on public discourse. ...

Offline events and online hate

... In this paper, we simulate a networked system, where thousands of agents, solely driven by LLMs, freely establish social relationships, communicate, and form opinions on political issues. We discover that these free-form social interactions among LLM agents result in the emergence of opinion polarization, a phenomenon widely observed in human society [28,[33][34][35][36][37][38]. Meanwhile, LLM agents spontaneously organize their own social network of human-like properties: agents with homophilic opinions tend to cluster, while those with opposing opinions tend to avoid interactions /citelaiposition. ...

Emergence of Polarization in Coevolving Networks

Physical Review Letters