학술논문

Dependence on plasma shape and plasma fueling for small edge-localized mode regimes in TCV and ASDEX Upgrade
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Labit, B.Eich, T.Harrer, G.F.Wolfrum, E.Bernert, M.Dunne, M.Frassinetti, L.Hennequin, P.Maurizio, R.Merle, A.Meyer, H.F.Saarelma, S.Sheikh, U.Adamek, J.Agostini, M.Aguiam, D.Akers, R.Albanese, R.Albert, C.Alessi, E.Ambrosino, R.Andr be, Y.Angioni, C.Apruzzese, G.Aradi, MatyasArnichand, H.Auriemma, F.Avdeeva, G.Ayllon-Guerola, J.M.Bagnato, F.Bandaru, V.Barnes, M.Barrera Orte, L.Bettini, P.Bilato, R.Biletskyi, O.Bílková, P.Bin, W.Blanchard, P.Blanken, T.C.Bobkov, V.Bock, A.Boeyaert, D.Bogar, K.Bogar, O.Bohm, P.Bolzonella, T.Bombarda, F.Boncagni, L.Bouquey, F.Bowman, C.Brezinsek, S.Brida, D.Brunetti, D.Bucalossi, J.Buchanan, J.Buermans, J.Bufferand, H.Buller, Stefan, 1991; Buratti, P.Burckhart, A.Calabr, G.Calacci, L.Camenen, Y.Cannas, B.Cano Megías, P.Carnevale, D.Carpanese, F.Carr, M.Carralero, D.Carraro, L.Casolari, A.Cathey, A.Causa, F.Cavedon, M.Cecconello, M.Ceccuzzi, S.Cerovsky, J.Chapman, S.Chmielewski, P.Choi, D.Cianfarani, C.Ciraolo, G.Coda, S.Coelho, R.Colas, L.Colette, D.Cordaro, L.Cordella, F.Costea, S.Coster, D.Cruz Zabala, D.J.Cseh, G.Czarnecka, A.Cziegler, I.D'Arcangelo, O.Dal Molin, A.David, P.De Carolis, G.De Oliveira, H.Decker, J.Dejarnac, R.Delogu, R.Den Harder, N.Dimitrova, M.Dolizy, F.Domínguez-Palacios Durán, J.J.Douai, D.Drenik, A.Dreval, M.Dudson, BenjaminDunai, DánielDuval, B.Dux, R.Elmore, S.D.Embréus, Ola, 1991; Erds, B.Fable, E.Faitsch, M.Fanni, A.Farnik, M.Faust, I.Faustin, J.Fedorczak, N.Felici, FFeng, S.Feng, X.Ferreira, JorgeFerr, G.Février, O.Ficker, O.Figini, L.Figueiredo, A.C.A.Fil, A.Fontana, M.Francesco, M.Fuchs, C.Futatani, S.Gabellieri, L.Gadariya, D.Gahle, D.Galassi, D.Galazka, K.Galdon-Quiroga, J.Galeani, S.Gallart, D.Gallo, A.Galperti, C.Garavaglia, S.Garcia, J.Garcia-Lopez, J.Garcia-Mu oz, M.Garzotti, LucaGath, J.Geiger, B.Giacomelli, L.Giannone, L.Gibson, S.Gil, L.Giovannozzi, E.Giruzzi, G.Gobbin, M.Gonzalez Martin, J.Goodman, T.Gorini, G.Gospodarczyk, M.Granucci, G.Grekov, D.Grenfell, G.Griener, M.Groth, M.Grover, O.Gruca, M.Gude, A.Guimarais, L.Gyergyek, T.Hacek, P.Hakola, A.H.Ham, C.Happel, T.Harrison, J.R.Havranek, A.Hawke, J.Henderson, S.S.Hesslow, L.Hitzler, F.Hnat, BogdanHobirk, J.Hoelzl, M.Hogeweij, D.Hopf, C.Hoppe, M.Horáček, J.Hron, M.Huang, Z.Iantchenko, A.Iglesias, D.Igochine, V.Innocente, P.Ionita Schrittwieser, C.Isliker, H.Ivanova-Stanik, I.Jacobsen, A.S.Jakubowski, M.Janky, F.Jardin, A.Jaulmes, F.Jensen, T.Jonsson, T.Kallenbach, A.Kappatou, A.Karpushov, A.Kasilov, S.Kazakov, Yevgen, 1984; Kazantzidis, P.-V.Keeling, D.Kelemen, M.Kendl, A.Kernbichler, W.Kirk, A.Kocsis, G.Komm, M.Kong, M.Korovin, V.Koubiti, M.Kovacic, J.Krawczyk, N.Krieger, K.Kripner, L.Krivska, A.Kudlacek, O.Kulyk, Y.Kurki-Suonio, Taina, 1959; Kwiatkowski, R.Laggner, F.Laguardia, L.Lahtinen, A.Lang, P.T.Likonen, J.Lipschultz, B.Liu, F.Lombroni, R.Lorenzini, R.Loschiavo, V.P.Lunt, T.Macusova, E.Madsen, J.Maggiora, R.Maljaars, B.Manas, P.Mantica, P.Mantsinen, M.Manz, P.Maraschek, MarkMarchenko, V.Marchetto, C.Mariani, A.Marini, C.Markovič, T.Marrelli, L.Martin, P.Martìn-Solìs, J. R.Martitsch, A.Mastrostefano, S.Matos, F.Matthews, G.F.Mayoral, M.L.Mazon, D.Mazzotta, C.Mc Carthy, P.McClements, K.McDermott, R.McMillan, B.Meineri, C.Menkovski, V.Meshcheriakov, D.Messmer, M.Micheletti, D.Milanesio, D.Militello, F.Miron, I.Mlynar, J.Moiseenko, V.Molina Cabrera, P.A.Morales, J.Moret, J.-M.Moro, A.Moulton, D.Nabais, F.Naulin, VNaydenkova, D.Nem, R.D.Nespoli, F.Newton, Sarah, 1981; Nielsen, A.H.Nielsen, S. K.Nikolaeva, V.Nocente, M.Nowak, S.Oberkofler, M.Ochoukov, R.Ollus, P.Olsen, J.Omotani, John, 1985; Ongena, JOrain, F.Orsitto, F.Paccagnella, R.Palha, A.Panaccione, L.Panek, R.Panjan, M.Papp, Gergely, 1985; Paradela Perez, I.Parra, F. I.Passeri, M.Pau, A.Pautasso, GPavlichenko, R.Perek, A.Pericoli Radolfini, V.Pesamosca, F.Peterka, M.Petržilka, V.Piergotti, V.Pigatto, L.Piovesan, P.Piron, C.Piron, L.Plyusnin, V VPokol, G.I.Poli, E.Pölöskei, P.Popov, T.PopovicPór, GáborPorte, L.Pucella, G.Puiatti, M.E.Pütterich, T.Rabinski, M.Juul Rasmussen, J.Rasmussen, J.Rattá, G.A.Ratynskaia, S.Ravensbergen, T.Refy, D.Reich, M.Reimerdes, H.Reimold, F.Reiser, D.Reux, CReznik, S.Ricci, D.Rispoli, N.Rivero-Rodriguez, J.F.Rocchi, G.Rodriguez-Ramos, M.Romano, A.Rosato, J.Rubinacci, G.Rubino, G.Ryan, D.Salewski, M.Salmi, A.Samaddar, D.Sanchis-Sanchez, L.Santos, J.Sarkimaki, K.Sassano, M.Sauter, O.Scannell, R.Scheffer, M.Schneider, B.S.Schneider, P.A.Schrittwieser, R.Schubert, M.Seidl, J.Seliunin, E.Sharapov, S. E.Sheeba, R.R.Sias, G.Sieglin, B.Silva, C.Sipila, S.Smith, S.F.Snicker, A.Solano, E.R.Hansen, S.K.Soria-Hoyo, C.Sorokovoy, E.Sozzi, C.Sperduti, A.Spizzo, G.Spolaore, M.Stejner, M.Stipani, L.Stober, J.Strand, Pär, 1968; Sun, H.-J.Suttrop, W.Sytnykov, D.Szepesi, T.Tál, B.Tala, T.Tardini, G.Tardocchi, M.Teplukhina, A.Terranova, D.Testa, D.Theiler, C.Thorén, E.Thornton, A.J.Tilia, B.Tolias, P.Tomeš, M.Toscano-Jimenez, M.Tsironis, C.Tsui, C.K.Tudisco, O.Urban, J.Valisa, M.Vallar, M.Vallejos Olivares, P.Valovic, MartinVan Vugt, D.Vanovac, B.Varje, J.Varju, J.Varoutis, S.Vartanian, S.Vasilovici, O.Vega, J.Verdoolaege, GeertVerhaegh, K.Vermare, L.Vianello, N.Vicente, J.Viezzer, E.Villone, F.Voitsekhovitch, I.Voltolina, D.Vondráček, P.Vu, N.M.T.Walkden, N. R.Wauters, TWeiland, M.Weinzettl, V.Wensing, M.Wiesen, S.Wiesenberger, M.Wilkie, George, 1983; Willensdorfer, M.Wischmeier, M.Wu, K.Xiang, L.Zagórski, R.Zaloga, D.Zanca, P.Zaplotnik, R.Zebrowski, J.Zhang, W.Zisis, A.Zoletnik, S.Zuin, M.
Source
Nuclear Fusion. 59(8)
Subject
H-mode
type-II ELMs
separatrix density
plasma triangularity
ballooning modes
grassy ELMs
Language
English
ISSN
1741-4326
0029-5515
Abstract
© 2019 Institute of Physics Publishing. All rights reserved. Within the EUROfusion MST1 work package, a series of experiments has been conducted on AUG and TCV devices to disentangle the role of plasma fueling and plasma shape for the onset of small ELM regimes. On both devices, small ELM regimes with high confinement are achieved if and only if two conditions are fulfilled at the same time. Firstly, the plasma density at the separatrix must be large enough (ne,sep/nG ∼ 0.3), leading to a pressure profile flattening at the separatrix, which stabilizes type-I ELMs. Secondly, the magnetic configuration has to be close to a double null (DN), leading to a reduction of the magnetic shear in the extreme vicinity of the separatrix. As a consequence, its stabilizing effect on ballooning modes is weakened.