1992
DOI: 10.1103/physrevlett.68.3563
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Scenarios for the nonlinear evolution of alpha-particle-induced Alfvén wave instability

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Cited by 147 publications
(142 citation statements)
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“…The nonlinear regime The effect of the double-resonance in the nonlinear regime is clearly visible in figure 5 (∆s = 0.2): in the double mode scenario, the modes not only grow faster (in the case of the TAE), but also saturate at a higher level compared to the single mode case (by about a factor of five to ten). This is due to the orbit stochasticization at δB/B ≈ 2 · 10 −3 already discovered in single mode simulations: The stochastic threshold [8] is only reached in the double mode scenario, not in the single mode case. To visualize the effect of stochasticization, an representative particle orbit and the particle's energy evolution before and after the stochasticization sets in is shown in figure 6.…”
Section: Simulation Resultsmentioning
confidence: 75%
See 1 more Smart Citation
“…The nonlinear regime The effect of the double-resonance in the nonlinear regime is clearly visible in figure 5 (∆s = 0.2): in the double mode scenario, the modes not only grow faster (in the case of the TAE), but also saturate at a higher level compared to the single mode case (by about a factor of five to ten). This is due to the orbit stochasticization at δB/B ≈ 2 · 10 −3 already discovered in single mode simulations: The stochastic threshold [8] is only reached in the double mode scenario, not in the single mode case. To visualize the effect of stochasticization, an representative particle orbit and the particle's energy evolution before and after the stochasticization sets in is shown in figure 6.…”
Section: Simulation Resultsmentioning
confidence: 75%
“…[8]) predicts that conversion of free energy to wave energy is enhanced in a multiplemode scenario, i.e., the interaction of multiple modes produces energy conversion rates higher than that which would be achieved with each mode acting independently. This can be partially explained by the principle of gradient (of the radial particle distribution) driven mode growth -according to ‡ γ ∝ ∇ f (s) [9] -which can be extended to multiple modes [8,[10][11][12]. This picture of gradient driven doubleresonance is based on the precondition that modes share resonances in the same phase space area.…”
Section: Theoretical Picture Of Double-resonancementioning
confidence: 99%
“…This chirping was seen in particle simulations to be associated with the dynamics of energetic particles and the formation of coherent structures in the phasespace, moving in the momentum direction 3-5 . Such dynamics in phase space have been studied, not only for the bump-on-tail case, but also for various Energetic Particle Modes (EPMs), be it for specific modes such as the Alfvén waves 6 or in a more general way 7 .…”
Section: Introductionmentioning
confidence: 99%
“…Of particular concern in multiple modes case is whether the TAE amplitudes becomes large enough to cause resonance overlap, which can lead to global particle diffusion and energy loss. As shown previously [23], resonance overlap is greatly facilitated by the simultaneous excitation of multiple modes. In the following simulation we use ITER-like parameters: R = 800cm, a = 300cm, B = 6T, Sr = a / 3 .…”
Section: Nonlinear Particle/mhd Hybrid Simulationsmentioning
confidence: 73%