2015
DOI: 10.1017/s0022377815001002
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Nonlinear physics and energetic particle transport features of the beam–plasma instability

Abstract: In this paper we study transport features of a one-dimensional beam-plasma system in the presence of multiple resonances. As a model description of the general problem of a warm energetic particle beam, we assume n cold supra-thermal beams and investigate the self-consistent evolution in the presence of the complete spectrum of nearly degenerate Langmuir modes. A qualitative transport estimation is obtained by computing the Lagrangian Coherent Structures of the system on given temporal scales. This leads to th… Show more

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Cited by 27 publications
(84 citation statements)
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“…As a result, a large number of resonances can be easily described, up to dealing with the so-called quasi-linear limit (Berk et al 1995a;Volokitin & Krafft 2012). The conceptual framework that justifies the implementation of a Hamiltonian approach is the so-called notion of 'quasi-stationary states' (Berk et al 1995b;Elskens & Escande 2003;Carlevaro et al 2014), i.e. transient states of the discrete system, in which a time is spent by the dynamics proportional to the number of considered particles (in practice, charged macroparticles).…”
Section: Hamiltonian Description Of the Beam-plasma Interactionmentioning
confidence: 99%
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“…As a result, a large number of resonances can be easily described, up to dealing with the so-called quasi-linear limit (Berk et al 1995a;Volokitin & Krafft 2012). The conceptual framework that justifies the implementation of a Hamiltonian approach is the so-called notion of 'quasi-stationary states' (Berk et al 1995b;Elskens & Escande 2003;Carlevaro et al 2014), i.e. transient states of the discrete system, in which a time is spent by the dynamics proportional to the number of considered particles (in practice, charged macroparticles).…”
Section: Hamiltonian Description Of the Beam-plasma Interactionmentioning
confidence: 99%
“…In this work, following O' Neil &Malmberg (1968) andO'Neil et al (1971) (see also Carlevaro et al (2015Carlevaro et al ( , 2016a for other reference details), the plasma is addressed as a cold linear dielectric medium represented by longitudinal electrostatic Langmuir waves, whose density n p is assumed much greater that the beam density n B . In this respect, we define η ≡ n B /n p as one of the fundamental parameters of the model.…”
Section: Hamiltonian Description Of the Beam-plasma Interactionmentioning
confidence: 99%
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“…In particular, we adopt the Hamiltonian formulation of the problem described in Ref. [51], where the broad supra-thermal particle beam is discretized as superposition of n ≫ 1 cold beams self-consistently evolving in the presence of m n modes nearly degenerate with Langmuir waves, i.e., with frequency ω k j ≃ ω p for j = 1, ..., m. This ensures that the dielectric function of the cold background plasma is nearly vanishing and allows casting the Poisson equation for each plasma oscillation into the form of a simple evolution equation, while particles trajectories are solved from the equations of motion (2) [9].…”
Section: Numerical Simulations Of Broad Beam Relaxation In Cold Plasmamentioning
confidence: 99%
“…In the following, we first briefly summarize the Hamiltonian formulation of the broad beam relaxation in cold plasma derived in Ref. [51] (Sec.4.1). Then, we discuss the dimensionless parameters that are used to characterize the different nonlinear dynamic regimes (Sec.4.2), which will be studied numerically with four different set-ups of initial conditions (Sec.4.3).…”
Section: Numerical Simulations Of Broad Beam Relaxation In Cold Plasmamentioning
confidence: 99%