Fitness voter model: Damped oscillations and anomalous consensus

Autores
Woolcock, Anthony; Connaughton, Colm; Merali, Yasmin; Vazquez, Federico
Año de publicación
2017
Idioma
inglés
Tipo de recurso
artículo
Estado
versión publicada
Descripción
We study the dynamics of opinion formation in a heterogeneous voter model on a complete graph, in which each agent is endowed with an integer fitness parameter k ≥ 0 , in addition to its + or − opinion state. The evolution of the distribution of k -values and the opinion dynamics are coupled together, so as to allow the system to dynamically develop heterogeneity and memory in a simple way. When two agents with different opinions interact, their k -values are compared, and with probability p the agent with the lower value adopts the opinion of the one with the higher value, while with probability 1 − p the opposite happens. The agent that keeps its opinion (winning agent) increments its k -value by one. We study the dynamics of the system in the entire 0 ≤ p ≤ 1 range and compare with the case p = 1 / 2 , in which opinions are decoupled from the k -values and the dynamics is equivalent to that of the standard voter model. When 0 ≤ p < 1 / 2 , agents with higher k -values are less persuasive, and the system approaches exponentially fast to the consensus state of the initial majority opinion. The mean consensus time τ appears to grow logarithmically with the number of agents N , and it is greatly decreased relative to the linear behavior τ ∼ N found in the standard voter model. When 1 / 2 < p ≤ 1 , agents with higher k -values are more persuasive, and the system initially relaxes to a state with an even coexistence of opinions, but eventually reaches consensus by finite-size fluctuations. The approach to the coexistence state is monotonic for 1 / 2 < p < p o ≃ 0.8 , while for p o ≤ p ≤ 1 there are damped oscillations around the coexistence value. The final approach to coexistence is approximately a power law t − b ( p ) in both regimes, where the exponent b increases with p . Also, τ increases respect to the standard voter model, although it still scales linearly with N . The p = 1 case is special, with a relaxation to coexistence that scales as t − 2.73 and a consensus time that scales as τ ∼ N β , with β ≃ 1.45 .
Fil: Woolcock, Anthony. University of Warwick; Reino Unido
Fil: Connaughton, Colm. University of Warwick; Reino Unido. London Mathematical Laboratory; Reino Unido. University of California; Estados Unidos
Fil: Merali, Yasmin. University of Hull; Reino Unido
Fil: Vazquez, Federico. University of Warwick; Reino Unido. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Instituto de Física de Líquidos y Sistemas Biológicos. Universidad Nacional de La Plata. Facultad de Ciencias Exactas. Instituto de Física de Líquidos y Sistemas Biológicos; Argentina
Materia
OPINION FORMATION
HETEROGENEOUS VOTER MODEL
STOCHASTIC PROCESS
INTRINSIC FITNESS
Nivel de accesibilidad
acceso abierto
Condiciones de uso
https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
Repositorio
CONICET Digital (CONICET)
Institución
Consejo Nacional de Investigaciones Científicas y Técnicas
OAI Identificador
oai:ri.conicet.gov.ar:11336/47941

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spelling Fitness voter model: Damped oscillations and anomalous consensusWoolcock, AnthonyConnaughton, ColmMerali, YasminVazquez, FedericoOPINION FORMATIONHETEROGENEOUS VOTER MODELSTOCHASTIC PROCESSINTRINSIC FITNESShttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1We study the dynamics of opinion formation in a heterogeneous voter model on a complete graph, in which each agent is endowed with an integer fitness parameter k ≥ 0 , in addition to its + or − opinion state. The evolution of the distribution of k -values and the opinion dynamics are coupled together, so as to allow the system to dynamically develop heterogeneity and memory in a simple way. When two agents with different opinions interact, their k -values are compared, and with probability p the agent with the lower value adopts the opinion of the one with the higher value, while with probability 1 − p the opposite happens. The agent that keeps its opinion (winning agent) increments its k -value by one. We study the dynamics of the system in the entire 0 ≤ p ≤ 1 range and compare with the case p = 1 / 2 , in which opinions are decoupled from the k -values and the dynamics is equivalent to that of the standard voter model. When 0 ≤ p < 1 / 2 , agents with higher k -values are less persuasive, and the system approaches exponentially fast to the consensus state of the initial majority opinion. The mean consensus time τ appears to grow logarithmically with the number of agents N , and it is greatly decreased relative to the linear behavior τ ∼ N found in the standard voter model. When 1 / 2 < p ≤ 1 , agents with higher k -values are more persuasive, and the system initially relaxes to a state with an even coexistence of opinions, but eventually reaches consensus by finite-size fluctuations. The approach to the coexistence state is monotonic for 1 / 2 < p < p o ≃ 0.8 , while for p o ≤ p ≤ 1 there are damped oscillations around the coexistence value. The final approach to coexistence is approximately a power law t − b ( p ) in both regimes, where the exponent b increases with p . Also, τ increases respect to the standard voter model, although it still scales linearly with N . The p = 1 case is special, with a relaxation to coexistence that scales as t − 2.73 and a consensus time that scales as τ ∼ N β , with β ≃ 1.45 .Fil: Woolcock, Anthony. University of Warwick; Reino UnidoFil: Connaughton, Colm. University of Warwick; Reino Unido. London Mathematical Laboratory; Reino Unido. University of California; Estados UnidosFil: Merali, Yasmin. University of Hull; Reino UnidoFil: Vazquez, Federico. University of Warwick; Reino Unido. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Instituto de Física de Líquidos y Sistemas Biológicos. Universidad Nacional de La Plata. Facultad de Ciencias Exactas. Instituto de Física de Líquidos y Sistemas Biológicos; ArgentinaAmerican Physical Society2017-09info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/47941Woolcock, Anthony; Connaughton, Colm; Merali, Yasmin; Vazquez, Federico; Fitness voter model: Damped oscillations and anomalous consensus; American Physical Society; Physical Review E; 96; 3; 9-2017; 1-142470-0045CONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevE.96.032313info:eu-repo/semantics/altIdentifier/url/https://journals.aps.org/pre/abstract/10.1103/PhysRevE.96.032313info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-10-15T14:25:33Zoai:ri.conicet.gov.ar:11336/47941instacron:CONICETInstitucionalhttp://ri.conicet.gov.ar/Organismo científico-tecnológicoNo correspondehttp://ri.conicet.gov.ar/oai/requestdasensio@conicet.gov.ar; lcarlino@conicet.gov.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:34982025-10-15 14:25:33.647CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse
dc.title.none.fl_str_mv Fitness voter model: Damped oscillations and anomalous consensus
title Fitness voter model: Damped oscillations and anomalous consensus
spellingShingle Fitness voter model: Damped oscillations and anomalous consensus
Woolcock, Anthony
OPINION FORMATION
HETEROGENEOUS VOTER MODEL
STOCHASTIC PROCESS
INTRINSIC FITNESS
title_short Fitness voter model: Damped oscillations and anomalous consensus
title_full Fitness voter model: Damped oscillations and anomalous consensus
title_fullStr Fitness voter model: Damped oscillations and anomalous consensus
title_full_unstemmed Fitness voter model: Damped oscillations and anomalous consensus
title_sort Fitness voter model: Damped oscillations and anomalous consensus
dc.creator.none.fl_str_mv Woolcock, Anthony
Connaughton, Colm
Merali, Yasmin
Vazquez, Federico
author Woolcock, Anthony
author_facet Woolcock, Anthony
Connaughton, Colm
Merali, Yasmin
Vazquez, Federico
author_role author
author2 Connaughton, Colm
Merali, Yasmin
Vazquez, Federico
author2_role author
author
author
dc.subject.none.fl_str_mv OPINION FORMATION
HETEROGENEOUS VOTER MODEL
STOCHASTIC PROCESS
INTRINSIC FITNESS
topic OPINION FORMATION
HETEROGENEOUS VOTER MODEL
STOCHASTIC PROCESS
INTRINSIC FITNESS
purl_subject.fl_str_mv https://purl.org/becyt/ford/1.3
https://purl.org/becyt/ford/1
dc.description.none.fl_txt_mv We study the dynamics of opinion formation in a heterogeneous voter model on a complete graph, in which each agent is endowed with an integer fitness parameter k ≥ 0 , in addition to its + or − opinion state. The evolution of the distribution of k -values and the opinion dynamics are coupled together, so as to allow the system to dynamically develop heterogeneity and memory in a simple way. When two agents with different opinions interact, their k -values are compared, and with probability p the agent with the lower value adopts the opinion of the one with the higher value, while with probability 1 − p the opposite happens. The agent that keeps its opinion (winning agent) increments its k -value by one. We study the dynamics of the system in the entire 0 ≤ p ≤ 1 range and compare with the case p = 1 / 2 , in which opinions are decoupled from the k -values and the dynamics is equivalent to that of the standard voter model. When 0 ≤ p < 1 / 2 , agents with higher k -values are less persuasive, and the system approaches exponentially fast to the consensus state of the initial majority opinion. The mean consensus time τ appears to grow logarithmically with the number of agents N , and it is greatly decreased relative to the linear behavior τ ∼ N found in the standard voter model. When 1 / 2 < p ≤ 1 , agents with higher k -values are more persuasive, and the system initially relaxes to a state with an even coexistence of opinions, but eventually reaches consensus by finite-size fluctuations. The approach to the coexistence state is monotonic for 1 / 2 < p < p o ≃ 0.8 , while for p o ≤ p ≤ 1 there are damped oscillations around the coexistence value. The final approach to coexistence is approximately a power law t − b ( p ) in both regimes, where the exponent b increases with p . Also, τ increases respect to the standard voter model, although it still scales linearly with N . The p = 1 case is special, with a relaxation to coexistence that scales as t − 2.73 and a consensus time that scales as τ ∼ N β , with β ≃ 1.45 .
Fil: Woolcock, Anthony. University of Warwick; Reino Unido
Fil: Connaughton, Colm. University of Warwick; Reino Unido. London Mathematical Laboratory; Reino Unido. University of California; Estados Unidos
Fil: Merali, Yasmin. University of Hull; Reino Unido
Fil: Vazquez, Federico. University of Warwick; Reino Unido. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Instituto de Física de Líquidos y Sistemas Biológicos. Universidad Nacional de La Plata. Facultad de Ciencias Exactas. Instituto de Física de Líquidos y Sistemas Biológicos; Argentina
description We study the dynamics of opinion formation in a heterogeneous voter model on a complete graph, in which each agent is endowed with an integer fitness parameter k ≥ 0 , in addition to its + or − opinion state. The evolution of the distribution of k -values and the opinion dynamics are coupled together, so as to allow the system to dynamically develop heterogeneity and memory in a simple way. When two agents with different opinions interact, their k -values are compared, and with probability p the agent with the lower value adopts the opinion of the one with the higher value, while with probability 1 − p the opposite happens. The agent that keeps its opinion (winning agent) increments its k -value by one. We study the dynamics of the system in the entire 0 ≤ p ≤ 1 range and compare with the case p = 1 / 2 , in which opinions are decoupled from the k -values and the dynamics is equivalent to that of the standard voter model. When 0 ≤ p < 1 / 2 , agents with higher k -values are less persuasive, and the system approaches exponentially fast to the consensus state of the initial majority opinion. The mean consensus time τ appears to grow logarithmically with the number of agents N , and it is greatly decreased relative to the linear behavior τ ∼ N found in the standard voter model. When 1 / 2 < p ≤ 1 , agents with higher k -values are more persuasive, and the system initially relaxes to a state with an even coexistence of opinions, but eventually reaches consensus by finite-size fluctuations. The approach to the coexistence state is monotonic for 1 / 2 < p < p o ≃ 0.8 , while for p o ≤ p ≤ 1 there are damped oscillations around the coexistence value. The final approach to coexistence is approximately a power law t − b ( p ) in both regimes, where the exponent b increases with p . Also, τ increases respect to the standard voter model, although it still scales linearly with N . The p = 1 case is special, with a relaxation to coexistence that scales as t − 2.73 and a consensus time that scales as τ ∼ N β , with β ≃ 1.45 .
publishDate 2017
dc.date.none.fl_str_mv 2017-09
dc.type.none.fl_str_mv info:eu-repo/semantics/article
info:eu-repo/semantics/publishedVersion
http://purl.org/coar/resource_type/c_6501
info:ar-repo/semantics/articulo
format article
status_str publishedVersion
dc.identifier.none.fl_str_mv http://hdl.handle.net/11336/47941
Woolcock, Anthony; Connaughton, Colm; Merali, Yasmin; Vazquez, Federico; Fitness voter model: Damped oscillations and anomalous consensus; American Physical Society; Physical Review E; 96; 3; 9-2017; 1-14
2470-0045
CONICET Digital
CONICET
url http://hdl.handle.net/11336/47941
identifier_str_mv Woolcock, Anthony; Connaughton, Colm; Merali, Yasmin; Vazquez, Federico; Fitness voter model: Damped oscillations and anomalous consensus; American Physical Society; Physical Review E; 96; 3; 9-2017; 1-14
2470-0045
CONICET Digital
CONICET
dc.language.none.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevE.96.032313
info:eu-repo/semantics/altIdentifier/url/https://journals.aps.org/pre/abstract/10.1103/PhysRevE.96.032313
dc.rights.none.fl_str_mv info:eu-repo/semantics/openAccess
https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
eu_rights_str_mv openAccess
rights_invalid_str_mv https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
dc.format.none.fl_str_mv application/pdf
application/pdf
dc.publisher.none.fl_str_mv American Physical Society
publisher.none.fl_str_mv American Physical Society
dc.source.none.fl_str_mv reponame:CONICET Digital (CONICET)
instname:Consejo Nacional de Investigaciones Científicas y Técnicas
reponame_str CONICET Digital (CONICET)
collection CONICET Digital (CONICET)
instname_str Consejo Nacional de Investigaciones Científicas y Técnicas
repository.name.fl_str_mv CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicas
repository.mail.fl_str_mv dasensio@conicet.gov.ar; lcarlino@conicet.gov.ar
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