2019
DOI: 10.1063/1.5100597
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High frequency mode generation by toroidal Alfvén eigenmodes

Abstract: Nonlinear generation of high frequency mode (HFM) by toroidal Alfvén eigenmode (TAE) observed in HL-2A tokamak is analyzed using nonlinear gyrokinetic theory. It is found that, the HFM can be dominated by |nq − m| = 1 perturbations with predominantly ideal magnetohydrodynamic if the two primary TAEs are co-propagating; while the HFM can be characterized by nq − m = 0 electrostatic perturbations if the two primary TAEs are counter-propagating. Here, n and m are respectively the toroidal and poloidal mode number… Show more

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Cited by 4 publications
(4 citation statements)
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“…The highfrequency mode 𝛺 h (𝜔 h , 𝑘 h ) excited by two TAEs, 𝛺 1 (𝜔 1 , 𝑘 1 ) and 𝛺 1 (𝜔 2 , 𝑘 2 ), with opposite toroidal mode numbers can be investigated by nonlinear gyrokinetic theory. [81] In our experiment, 𝜔 1 ≃ 𝜔 2 and 𝑛 1 = −𝑛 2 for the TAEs while the axisymmetric mode with 𝜔 ≈ 𝑉 A /𝑞𝑅. The wave number and frequency matching condition during mode coupling process are…”
Section: Nonlinear Coupling Between Alfvénic Modes and Tearingmentioning
confidence: 61%
“…The highfrequency mode 𝛺 h (𝜔 h , 𝑘 h ) excited by two TAEs, 𝛺 1 (𝜔 1 , 𝑘 1 ) and 𝛺 1 (𝜔 2 , 𝑘 2 ), with opposite toroidal mode numbers can be investigated by nonlinear gyrokinetic theory. [81] In our experiment, 𝜔 1 ≃ 𝜔 2 and 𝑛 1 = −𝑛 2 for the TAEs while the axisymmetric mode with 𝜔 ≈ 𝑉 A /𝑞𝑅. The wave number and frequency matching condition during mode coupling process are…”
Section: Nonlinear Coupling Between Alfvénic Modes and Tearingmentioning
confidence: 61%
“…Meanwhile, various nonideal effects, notably the magnetic geometry, plasma nonuniformity, compressibility and kinetic effects, could break such a 'pure Alfvénic state' [1] and lead to nonlinear spectral energy transfer by coupling with other collective oscillations [2,58,63]. These nonideal effects, which must be accounted for when studying SAW instability nonlinear dynamics and EP transport in burning plasmas, have been intensively investigated using TAE as a paradigm case [51,[120][121][122][123][124][125][126][127], as recently reviewed in [128]. The developed theoretical framework and obtained insights can be straightforwardly applied to other kinds of SAW instabilities, e.g., RSAE, which is the subject of this section, based on the understanding of RSAE linear physics and saturation due to wave-particle interactions as reviewed in section 2.…”
Section: Nonlinear Wave-wave Couplingsmentioning
confidence: 99%
“…Meanwhile, squared bicoherence reveals that the high frequency n = 0 modes are made up of two AMs with (n AM1 , n AM2 ) = (−1, 1)/(−2, 2)/(−3, 3), i.e. the axisymmetric mode in the EAE frequency range is driven by nonlinear coupling of two co-/counter-propagating AMs [26,27], rather than the second harmonic of Alfvénic mode with n = 0 in the TAE frequency range.…”
Section: Nonlinear Mode Coupling Between Tae and Tearing Modementioning
confidence: 99%