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Plasma wall interaction and its implication in an all tungsten divertor tokamak

R Neu et al 2007 Plasma Phys. Control. Fusion 49 B59-B70   doi: 10.1088/0741-3335/49/12B/S04  Help

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R Neu1, M Balden1, V Bobkov1, R Dux1, O Gruber1, A Herrmann1, A Kallenbach1, M Kaufmann1, C F Maggi1, H Maier1, H W Müller1, T Pütterich1, R Pugno1, V Rohde1, A C C Sips1, J Stober1, W Suttrop1, C Angioni1, C V Atanasiu2, W Becker1, K Behler1, K Behringer1, A Bergmann1, T Bertoncelli1, R Bilato1, A Bottino1, M Brambilla1, F Braun1, A Buhler1, A Chankin1, G Conway1, D P Coster1, P de Marné1, S Dietrich1, K Dimova1, R Drube1, T Eich1, K Engelhardt1, H-U Fahrbach1, U Fantz1, L Fattorini3, J Fink1, R Fischer1, A Flaws1, P Franzen1, J C Fuchs1, K Gál4, M García Muñoz1, M Gemisic-Adamov1, L Giannone1, S Gori1, S da Graca3, H Greuner1, A Gude1, S Günter1, G Haas1, J Harhausen1, B Heinemann1, N Hicks1, J Hobirk1, D Holtum1, C Hopf1, L Horton1, M Huart1, V Igochine1, S Kálvin4, O Kardaun1, M Kick1, G Kocsis4, H Kollotzek1, C Konz1, K Krieger1, T Kurki-Suonio5, B Kurzan1, K Lackner1, P T Lang1, P Lauber1, M Laux1, J Likonen5, L Liu1, A Lohs1, K Mank1, A Manini1, M-E Manso3, M Maraschek1, P Martin6, Y Martin7, M Mayer1, P McCarthy8, K McCormick1, H Meister1, F Meo9, P Merkel1, R Merkel1, V Mertens1, F Merz1, H Meyer10, M Mlynek1, F Monaco1, H Murmann1, G Neu1, J Neuhauser1, B Nold11, J-M Noterdaeme1, G Pautasso1, G Pereverzev1, E Poli1, M Püschel1, G Raupp1, M Reich1, B Reiter1, T Ribeiro3, R Riedl1, J Roth1, M Rott1, F Ryter1, W Sandmann1, J Santos3, K Sassenberg1, A Scarabosio1, G Schall1, J Schirmer1, A Schmid1, W Schneider1, G Schramm1, R Schrittwieser12, W Schustereder1, J Schweinzer1, S Schweizer1, B Scott1, U Seidel1, F Serra3, M Sertoli1, A Sigalov1, A Silva3, E Speth1, A Stäbler1, K-H Steuer1, E Strumberger1, G Tardini1, C Tichmann1, W Treutterer1, C Tröster1, L Urso1, E Vainonen-Ahlgren5, P Varela3, L Vermare1, D Wagner1, M Wischmeier1, E Wolfrum1, E Würsching1, D Yadikin1, Q Yu1, D Zasche1, T Zehetbauer1, M Zilker1 and H Zohm1
1 Max Planck Institut für Plasmaphysik, EURATOM Association, 85748 Garching, Germany
2 Institute of Atomic Physics, EURATOM Association-MEdC, Romania
3 CFN, EURATOM Association-IST Lisbon, Portugal
4 KFKI, EURATOM Association-HAS, Budapest, Hungary
5 HUT, EURATOM Association-Tekes, Helsinki, Finland
6 Consorzio RFX, EURATOM Association-ENEA, Padova, Italy
7 CRPP/EPFL, 1015 Lausanne, Switzerland
8 Physics Department University College Cork, Association EURATOM-DCU, Ireland
9 NL Risø, EURATOM Association-RISØ, Roskilde, Denmark
10 UKAEA Culham, EURATOM Association-UKAEA, UK
11 Institut für Plasmaforschung, Stuttgart University, Germany
12 University of Innsbruck, EURATOM Association-ÖAW, Austria

Abstract. ASDEX Upgrade has recently finished its transition towards an all-W divertor tokamak, by the exchange of the last remaining graphite tiles to W-coated ones. The plasma start-up was performed without prior boronization. It was found that the large He content in the plasma, resulting from DC glow discharges for conditioning, leads to a confinement reduction. After the change to D glow for inter-shot conditioning, the He content quickly dropped and, in parallel, the usual H-Mode confinement with H factors close to one was achieved. After the initial conditioning phase, oxygen concentrations similar to that in previous campaigns with boronizations could be achieved. Despite the removal of all macroscopic carbon sources, no strong change in C influxes and C content could be observed so far. The W concentrations are similar to the ones measured previously in discharges with old boronization and only partial coverage of the surfaces with W. Concomitantly it is found that although the W erosion flux in the divertor is larger than the W sources in the main chamber in most of the scenarios, it plays only a minor role for the W content in the main plasma. For large antenna distances and strong gas puffing, ICRH power coupling could be optimized to reduce the W influxes. This allowed a similar increase of stored energy as yielded with comparable beam power. However, a strong increase of radiated power and a loss of H-Mode was observed for conditions with high temperature edge plasma close to the antennas. The use of ECRH allowed keeping the central peaking of the W concentration low and even phases of improved H-modes have already been achieved.

Print publication: Issue 12B (December 2007)
Received 6 July 2007
Published 14 November 2007

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