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Parametric exponential energy decay for dissipative electron-ion plasma waves

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dc.contributor.author Karachalios, NI en
dc.contributor.author Stavrakakis, NM en
dc.contributor.author Xanthopoulos, P en
dc.date.accessioned 2014-03-01T01:22:54Z
dc.date.available 2014-03-01T01:22:54Z
dc.date.issued 2005 en
dc.identifier.issn 0044-2275 en
dc.identifier.uri https://dspace.lib.ntua.gr/xmlui/handle/123456789/16713
dc.subject Dissipation en
dc.subject ECRH plasma heating en
dc.subject Electron-ion plasma waves en
dc.subject Energy decay en
dc.subject Global existence en
dc.subject Klein-Gordon - Schrödinger system en
dc.subject Uniqueness en
dc.subject.classification Mathematics, Applied en
dc.subject.other ZAKHAROV SYSTEM en
dc.subject.other SCHRODINGER en
dc.subject.other ATTRACTORS en
dc.subject.other EQUATIONS en
dc.subject.other CAUCHY en
dc.title Parametric exponential energy decay for dissipative electron-ion plasma waves en
heal.type journalArticle en
heal.identifier.primary 10.1007/s00033-004-2095-2 en
heal.identifier.secondary http://dx.doi.org/10.1007/s00033-004-2095-2 en
heal.language English en
heal.publicationDate 2005 en
heal.abstract We consider the following evolution system of Klein-Gordon-Schrodinger type i psi(t) + kappa psi(xx) + i alpha psi = phi psi, x is an element of Omega, t > 0, phi(tt) - phi(xx) + phi + lambda phi(t) = -Re psi(x), x is an element of Omega, t > 0, satisfying the following initial and boundary conditions psi(x, 0) = psi(0)(x), phi(x, 0) = phi(0)(x), phi(t) (x, 0) = phi(1)(x), x is an element of Omega y(x, t) = phi(x, t) = 0, x is an element of partial derivative Omega, t > 0, with kappa, alpha, lambda positive constants and Omega a bounded subset of R. This system describes the nonlinear interaction between high frequency electron waves and low frequency ion plasma waves in a homogeneous magnetic field, adapted to model the UHH plasma heating scheme. The system focuses on the vital role of collisions, by considering the non-homogeneous polarization drift for the low frequency coupling. In Part I we set up the system, starting from first principles. In Part II we work out global existence and uniqueness of solutions and establish the necessary conditions for the system to manifest energy decay. In Part III the results are physically interpreted, providing a threshold of the effectiveness of UHH, in terms of the plasma variables. en
heal.publisher BIRKHAUSER VERLAG AG en
heal.journalName Zeitschrift fur Angewandte Mathematik und Physik en
dc.identifier.doi 10.1007/s00033-004-2095-2 en
dc.identifier.isi ISI:000228332700004 en
dc.identifier.volume 56 en
dc.identifier.issue 2 en
dc.identifier.spage 218 en
dc.identifier.epage 238 en


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