Low-dimensional phase-locked states in the zakharov equations

Detalhes bibliográficos
Autor(a) principal: Oliveira, Glaucius Iahnke de
Data de Publicação: 1996
Outros Autores: Oliveira, Luiz Paulo Luna de, Rizzato, Felipe Barbedo
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Institucional da UFRGS
Texto Completo: http://hdl.handle.net/10183/103639
Resumo: In this paper we identify phase-locked states among the solutions of the Zakharov equations. Locked states appear as resonant island chains in the appropriate Poincaré plots, with the relevant surface of section obtained by projecting out the full dynamical set on a subspace defined in terms of a pair of center-manifold variables. This pair allows an accurate canonical description of the system immediately after an inverse pitchfork bifurcation destabilizes an initial homogeneous steady state. If one is very close to the bifurcation point, nonlinear saturation of the initial instability is provided by quasistatic integrable ion-acoustic fluctuations, but as one proceeds away from that point, resonant nonintegrable ion-acoustic fluctuations become gradually more important; we show that the phase-locked states result from those resonant fluctuations. If one is not too far from the pitchfork bifurcation, locking is the stable asymptotic state of the interaction. As one moves farther away, locking exists only over long but finite amounts of time. In addition, the resonance separatrix appears to bring the first chaotic activity into the system.
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spelling Oliveira, Glaucius Iahnke deOliveira, Luiz Paulo Luna deRizzato, Felipe Barbedo2014-09-23T02:12:32Z19961063-651Xhttp://hdl.handle.net/10183/103639000179421In this paper we identify phase-locked states among the solutions of the Zakharov equations. Locked states appear as resonant island chains in the appropriate Poincaré plots, with the relevant surface of section obtained by projecting out the full dynamical set on a subspace defined in terms of a pair of center-manifold variables. This pair allows an accurate canonical description of the system immediately after an inverse pitchfork bifurcation destabilizes an initial homogeneous steady state. If one is very close to the bifurcation point, nonlinear saturation of the initial instability is provided by quasistatic integrable ion-acoustic fluctuations, but as one proceeds away from that point, resonant nonintegrable ion-acoustic fluctuations become gradually more important; we show that the phase-locked states result from those resonant fluctuations. If one is not too far from the pitchfork bifurcation, locking is the stable asymptotic state of the interaction. As one moves farther away, locking exists only over long but finite amounts of time. In addition, the resonance separatrix appears to bring the first chaotic activity into the system.application/pdfengPhysical Review. E, Statistical Physics, Plasmas, Fluids and Related Interdisciplinary Topics. New York. Vol. 54, no. 4 (Oct. 1996), p. 3239-3249Sistemas caóticosLow-dimensional phase-locked states in the zakharov equationsEstrangeiroinfo:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/openAccessreponame:Repositório Institucional da UFRGSinstname:Universidade Federal do Rio Grande do Sul (UFRGS)instacron:UFRGSORIGINAL000179421.pdf000179421.pdfTexto completo (inglês)application/pdf283648http://www.lume.ufrgs.br/bitstream/10183/103639/1/000179421.pdfc247b1f267e8cfaa2f49aa87859c6a69MD51TEXT000179421.pdf.txt000179421.pdf.txtExtracted Texttext/plain35140http://www.lume.ufrgs.br/bitstream/10183/103639/2/000179421.pdf.txt447bd2da4bd16e2dd3ec1c8ae14a0779MD52THUMBNAIL000179421.pdf.jpg000179421.pdf.jpgGenerated Thumbnailimage/jpeg2102http://www.lume.ufrgs.br/bitstream/10183/103639/3/000179421.pdf.jpged6df6e1759bfb29687041119c033766MD5310183/1036392023-09-02 03:35:26.779656oai:www.lume.ufrgs.br:10183/103639Repositório de PublicaçõesPUBhttps://lume.ufrgs.br/oai/requestopendoar:2023-09-02T06:35:26Repositório Institucional da UFRGS - Universidade Federal do Rio Grande do Sul (UFRGS)false
dc.title.pt_BR.fl_str_mv Low-dimensional phase-locked states in the zakharov equations
title Low-dimensional phase-locked states in the zakharov equations
spellingShingle Low-dimensional phase-locked states in the zakharov equations
Oliveira, Glaucius Iahnke de
Sistemas caóticos
title_short Low-dimensional phase-locked states in the zakharov equations
title_full Low-dimensional phase-locked states in the zakharov equations
title_fullStr Low-dimensional phase-locked states in the zakharov equations
title_full_unstemmed Low-dimensional phase-locked states in the zakharov equations
title_sort Low-dimensional phase-locked states in the zakharov equations
author Oliveira, Glaucius Iahnke de
author_facet Oliveira, Glaucius Iahnke de
Oliveira, Luiz Paulo Luna de
Rizzato, Felipe Barbedo
author_role author
author2 Oliveira, Luiz Paulo Luna de
Rizzato, Felipe Barbedo
author2_role author
author
dc.contributor.author.fl_str_mv Oliveira, Glaucius Iahnke de
Oliveira, Luiz Paulo Luna de
Rizzato, Felipe Barbedo
dc.subject.por.fl_str_mv Sistemas caóticos
topic Sistemas caóticos
description In this paper we identify phase-locked states among the solutions of the Zakharov equations. Locked states appear as resonant island chains in the appropriate Poincaré plots, with the relevant surface of section obtained by projecting out the full dynamical set on a subspace defined in terms of a pair of center-manifold variables. This pair allows an accurate canonical description of the system immediately after an inverse pitchfork bifurcation destabilizes an initial homogeneous steady state. If one is very close to the bifurcation point, nonlinear saturation of the initial instability is provided by quasistatic integrable ion-acoustic fluctuations, but as one proceeds away from that point, resonant nonintegrable ion-acoustic fluctuations become gradually more important; we show that the phase-locked states result from those resonant fluctuations. If one is not too far from the pitchfork bifurcation, locking is the stable asymptotic state of the interaction. As one moves farther away, locking exists only over long but finite amounts of time. In addition, the resonance separatrix appears to bring the first chaotic activity into the system.
publishDate 1996
dc.date.issued.fl_str_mv 1996
dc.date.accessioned.fl_str_mv 2014-09-23T02:12:32Z
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dc.language.iso.fl_str_mv eng
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dc.relation.ispartof.pt_BR.fl_str_mv Physical Review. E, Statistical Physics, Plasmas, Fluids and Related Interdisciplinary Topics. New York. Vol. 54, no. 4 (Oct. 1996), p. 3239-3249
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