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dc.contributor.authorSharapov, S.E.en_US
dc.contributor.authorOliver, H.J.C.en_US
dc.contributor.authorGarcia, J.en_US
dc.contributor.authorKeeling, D.L.en_US
dc.contributor.authorDreval, M.en_US
dc.contributor.authorGoloborod'ko, V.en_US
dc.contributor.authorKazakov, Ye. O.en_US
dc.contributor.authorKiptily, V.G.en_US
dc.contributor.authorStancar, Z.en_US
dc.contributor.authorBonofiglo, P.J.en_US
dc.contributor.authorCoelho, R.en_US
dc.contributor.authorCraciunescu, T.en_US
dc.contributor.authorFerreira, J.en_US
dc.contributor.authorFigueiredo, A.en_US
dc.contributor.authorFil, N.en_US
dc.contributor.authorFitzgerald, M.en_US
dc.contributor.authorNabais, F.en_US
dc.contributor.authorNocente, M.en_US
dc.contributor.authorPuglia, P.G.en_US
dc.contributor.authorRivero-Rodriguez, J.en_US
dc.contributor.authorRodrigues, P.en_US
dc.contributor.authorSalewski, M.en_US
dc.contributor.authorTinguely, R. Alexen_US
dc.contributor.authorZakharov, L.E.en_US
dc.contributor.authorJET contributorsen_US
dc.date.accessioned2025-03-21T20:13:48Z
dc.date.available2025-03-21T20:13:48Z
dc.date.issued2023-10
dc.identifier23ja030
dc.identifier.urihttps://hdl.handle.net/1721.1/158598
dc.descriptionSubmitted for publication in Nuclear Fusion
dc.description.abstractDedicated experiments were performed in JET DTE2 plasmas for obtaining an α-particle bump-on-tail (BOT) distribution aiming at exciting Alfvén Eigenmodes (AEs). NBI-only heating with modulated power was used so that fusion-born α-particles were the only ions present in the MeV energy range in these DT plasmas. The beam power modulation on a time scale shorter than the α-particle slowing down time was chosen for modulating the α-particle source and thus sustaining a BOT in the α-particle distribution. High-frequency modes in the TAE frequency range and multiple short-lived modes in a wider frequency range have been detected in these DT discharges with interferometry, soft X-ray cameras, and reflectometry. The modes observed were localised close to the magnetic axis, and were not seen in the Mirnov coils. Analysis with the TRANSP and Fokker-Planck FIDIT codes confirms that α-particle distributions with bump-on-tail in energy were achieved during some time intervals in these discharges though no clear correlation was found between the times of the high-frequency mode excitation and the BOT time intervals. The combined MHD and kinetic modelling studies show that the high-frequency mode in the TAE frequency range is best fitted with a TAE of toroidal mode number n= 9. This mode is driven mostly by the on-axis beam ions while the smaller drive due to the pressure gradient of α-particles allows overcoming the marginal stability and exciting the mode [H.J.C. Oliver et al. Toroidal Alfvén eigenmodes observed in low power JET deuterium-tritium plasmas, to be submitted to Nuclear Fusion (2023)]. The observed multiple short-lived modes in a wider frequency range are identified as the on-axis kinetic Alfvén eigenmodes predicted in [M.N. Rosenbluth, P.H. Rutherford, Phys. Rev. Lett. 34 (1975) 1428].
dc.publisherIOPen_US
dc.relation.isversionofdoi.org/10.1088/1741-4326/acee10
dc.sourcePlasma Science and Fusion Centeren_US
dc.titleExperiments on excitation of Alfvén eigenmodes by alpha-particles with bump-on-tail distribution in JET DTE2 plasmasen_US
dc.typeArticleen_US
dc.contributor.departmentMassachusetts Institute of Technology. Plasma Science and Fusion Center
dc.relation.journalNuclear Fusion


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