• Media type: E-Article
  • Title: Simulations of nonlinear interaction between beta-induced Alfvén eigenmode and tearing mode
  • Contributor: Duan, Sizhe; Wang, Xiaogang; Cai, Huishan; Li, Ding
  • imprint: IOP Publishing, 2023
  • Published in: Nuclear Fusion
  • Language: Not determined
  • DOI: 10.1088/1741-4326/acb802
  • ISSN: 0029-5515; 1741-4326
  • Keywords: Condensed Matter Physics ; Nuclear and High Energy Physics
  • Origination:
  • Footnote:
  • Description: <jats:title>Abstract</jats:title> <jats:p>The nonlinear interaction between the <jats:inline-formula> <jats:tex-math><?CDATA $m/n = 2/1$?></jats:tex-math> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>m</mml:mi> <mml:mrow> <mml:mo>/</mml:mo> </mml:mrow> <mml:mi>n</mml:mi> <mml:mo>=</mml:mo> <mml:mn>2</mml:mn> <mml:mrow> <mml:mo>/</mml:mo> </mml:mrow> <mml:mn>1</mml:mn> </mml:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="nfacb802ieqn1.gif" xlink:type="simple" /> </jats:inline-formula> beta-induced Alfvén eigenmode (BAE) and the <jats:inline-formula> <jats:tex-math><?CDATA $m/n = 2/1$?></jats:tex-math> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>m</mml:mi> <mml:mrow> <mml:mo>/</mml:mo> </mml:mrow> <mml:mi>n</mml:mi> <mml:mo>=</mml:mo> <mml:mn>2</mml:mn> <mml:mrow> <mml:mo>/</mml:mo> </mml:mrow> <mml:mn>1</mml:mn> </mml:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="nfacb802ieqn2.gif" xlink:type="simple" /> </jats:inline-formula> tearing mode (TM) observed in the HL-2A experiment is systematically studied with the hybrid kinetic-magnetohydrodynamic code M3D-K. It is found that the nonlinear growth of TM can lead to a gradient buildup on the magnetic island (MI) edge, and then triggers the destabilization of the linearly-stable BAE. Then, the triggered BAE together with TM can produce a significant redistribution of energetic particles. For BAE linearly-dominant-unstable case, the TM activity results in the inward motion of BAE mode structure, and the BAE can have a delay effect on the MI saturation. Furthermore, a high-frequency axisymmetric <jats:inline-formula> <jats:tex-math><?CDATA $m/n = 0/0$?></jats:tex-math> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>m</mml:mi> <mml:mrow> <mml:mo>/</mml:mo> </mml:mrow> <mml:mi>n</mml:mi> <mml:mo>=</mml:mo> <mml:mn>0</mml:mn> <mml:mrow> <mml:mo>/</mml:mo> </mml:mrow> <mml:mn>0</mml:mn> </mml:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="nfacb802ieqn3.gif" xlink:type="simple" /> </jats:inline-formula> ‘breathing’ mode is generated by the mode coupling of BAE and TM, agreeing well with the experimental observation, and causes the synchronized periodic oscillation of MI width.</jats:p>
  • Access State: Open Access