{"data":{"id":"10.6084/m9.figshare.2060595.v1","type":"dois","attributes":{"doi":"10.6084/m9.figshare.2060595.v1","prefix":"10.6084","suffix":"m9.figshare.2060595.v1","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Mellor, Andrew","nameType":"Personal","givenName":"Andrew","familyName":"Mellor","affiliation":[],"nameIdentifiers":[]},{"name":"Mobilia, Mauro","nameType":"Personal","givenName":"Mauro","familyName":"Mobilia","affiliation":[],"nameIdentifiers":[]},{"name":"R.K.P. Zia","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Characterization of the Nonequilibrium Steady State of a Heteogeneous Nonlinear q-Voter Model with Zealotry (Supplimentary Material)"}],"publisher":"figshare","container":{},"publicationYear":2016,"subjects":[{"subject":"20304 Thermodynamics and Statistical Physics","subjectScheme":"FOR"},{"subject":"FOS: Mechanical engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Mechanical engineering","subjectScheme":"Fields of Science and Technology (FOS)"}],"contributors":[],"dates":[{"date":"2016-01-14","dateType":"Created"},{"date":"2016-01-14","dateType":"Updated"},{"date":"2016","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsPreviousVersionOf","relatedIdentifier":"10.6084/m9.figshare.2060595","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["662424 Bytes"],"formats":[],"version":null,"rightsList":[{"rights":"Creative Commons Attribution 4.0 International","rightsUri":"https://creativecommons.org/licenses/by/4.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc-by-4.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"Supplementary material for \u003cem\u003eCharacterization of the Nonequilibrium Steady State of a Heteogeneous Nonlinear q-Voter Model with Zealotry\u003c/em\u003e.Authors: \u003cem\u003eAndrew Mellor, Mauro Mobilia, R.K.P. Zia\u003c/em\u003e\u003cb\u003eItems include:\u003c/b\u003eStationary state evolution as a function of z.Explicit expressions of LGA matrices, F and D.Vorticity and Stream Function: Definitions and Figure 3.Comparisons between precision numerical results and simulation data.Comparisons between LGA predictions and simulation results.\u003cb\u003eAbstract:\u003c/b\u003eWe introduce an heterogeneous nonlinear q-voter model with two types of susceptible voters and zealots, and study its non-equilibrium properties when the population is finite and well mixed. In this two-opinion model, each individual supports one of two parties and is either a susceptible voter of type q\u003csub\u003e1\u003c/sub\u003e or q\u003csub\u003e2\u003c/sub\u003e, or is an inflexible zealot. At each time step, a q\u003csub\u003ei\u003c/sub\u003e-susceptible voter (i=1,2) consults a group of q\u003csub\u003ei\u003c/sub\u003e neighbors and adopts their opinion if all group members agree, while zealots are inflexible and never change their opinion. We show that this model violates the detailed balance whenever q\u003csub\u003e1\u003c/sub\u003e≠q\u003csub\u003e2\u003c/sub\u003eand has surprisingly rich properties. Here, we focus on the characterization of the model’s non-equilibrium stationary state (NESS) in terms of its probability distribution and currents in the distinct regimes of low and high density of zealotry. We unveil the NESS properties in each of these phases by computing the opinion distribution and the circulation of probability currents, as well as the two-point correlation functions at unequal times (formally related to a “probability angular momentum”). Our analytical calculations obtained in the realm of a linear Gaussian approximation are compared with numerical results.\u003cb\u003eViewing Notes:\u003c/b\u003eTo view the supplementary materials, download all files and run index.html in a web browser (preferably Chrome).\u003cbr\u003e","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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