@article{MTMT:34034653, title = {Analysis and expansion of the quasi-continuous exhaust (QCE) regime in ASDEX Upgrade}, url = {https://m2.mtmt.hu/api/publication/34034653}, author = {Faitsch, M. and Eich, T. and Harrer, G.F. and Wolfrum, E. and Brida, D. and David, P. and Dunne, M. and Gil, L. and Labit, B. and Stroth, U.}, doi = {10.1088/1741-4326/acd464}, journal-iso = {NUCL FUSION}, journal = {NUCLEAR FUSION}, volume = {63}, unique-id = {34034653}, issn = {0029-5515}, year = {2023}, eissn = {1741-4326} } @article{MTMT:33856152, title = {Integrated core-SOL simulations for SPARC tokamak with the COREDIV code}, url = {https://m2.mtmt.hu/api/publication/33856152}, author = {Ivanova-Stanik, I and Chmielewski, P and Zagorski, R}, doi = {10.1016/j.fusengdes.2023.113698}, journal-iso = {FUSION ENG DES}, journal = {FUSION ENGINEERING AND DESIGN}, volume = {193}, unique-id = {33856152}, issn = {0920-3796}, year = {2023}, eissn = {1873-7196} } @article{MTMT:34296397, title = {Investigation of helium exhaust dynamics at the ASDEX Upgrade tokamak with full-tungsten wall}, url = {https://m2.mtmt.hu/api/publication/34296397}, author = {Zito, A. and Wischmeier, M. and Kappatou, A. and Kallenbach, A. and Sciortino, F. and Rohde, V. and Schmid, K. and Hinson, E. and Schmitz, O. and Cavedon, M. and McDermott, R. and Dux, R. and Griener, M. and Stroth, U. and the, ASDEX Upgrade Team}, doi = {10.1088/1741-4326/ace26e}, journal-iso = {NUCL FUSION}, journal = {NUCLEAR FUSION}, volume = {63}, unique-id = {34296397}, issn = {0029-5515}, year = {2023}, eissn = {1741-4326} } @article{MTMT:32757673, title = {Healing plasma current ramp-up by nitrogen seeding in the full tungsten environment of WEST}, url = {https://m2.mtmt.hu/api/publication/32757673}, author = {Maget, P. and Manas, P. and Artaud, J.-F. and Bourdelle, C. and Bucalossi, J. and Bufferand, H. and Ciraolo, G. and Desgranges, C. and Devynck, P. and Dumont, R. and Fedorczak, N. and Felici, F. and Goniche, M. and Guillemaut, C. and Guirlet, R. and Gunn, J.P. and Loarer, T. and Morales, J. and Sauter, O. and Van, Mulders S. and Vézinet, D.}, doi = {10.1088/1361-6587/ac4b93}, journal-iso = {PLASMA PHYS CONTR F}, journal = {PLASMA PHYSICS AND CONTROLLED FUSION}, volume = {64}, unique-id = {32757673}, issn = {0741-3335}, year = {2022}, eissn = {1361-6587} } @article{MTMT:33334161, title = {Divertor plasma behaviors with neon seeding at different locations on EAST with ITER-like divertor}, url = {https://m2.mtmt.hu/api/publication/33334161}, author = {Meng, L.Y. and Wang, L. and Wang, H.Q. and Deng, G.Z. and Si, H. and Li, K.D. and Xu, G.S. and Yuan, Q.P. and Guo, H.Y. and Eldon, D. and Garofalo, A.M. and Leonard, A.W. and Hyatt, A. and Humphreys, D. and Gong, X.Z. and Liu, J.B. and Xu, J.C. and Liang, R.R. and Zhong, F.B. and Lin, X. and Duan, Y.M. and Zang, Q. and Zhang, L. and Ding, F. and Yang, Z.S. and Zhang, B. and Zhang, T.}, doi = {10.1088/1741-4326/ac74cf}, journal-iso = {NUCL FUSION}, journal = {NUCLEAR FUSION}, volume = {62}, unique-id = {33334161}, issn = {0029-5515}, year = {2022}, eissn = {1741-4326} } @article{MTMT:32994681, title = {Experimental investigation on divertor tungsten sputtering with neon seeding in ELMy H-mode plasma in EAST tokamak}, url = {https://m2.mtmt.hu/api/publication/32994681}, author = {Ye, DW and Ding, F and Li, KD and Hu, ZH and Zhang, L and Chen, XH and Zhang, Q and Zhao, PA and He, T and Meng, LY and Ye, KX and Zhong, FB and Duan, YM and Ding, R and Wang, L and Xu, GS and Luo, GN}, doi = {10.1088/1674-1056/ac4f58}, journal-iso = {CHINESE PHYS B}, journal = {CHINESE PHYSICS B}, volume = {31}, unique-id = {32994681}, issn = {1674-1056}, year = {2022}, eissn = {1741-4199} } @article{MTMT:33306683, title = {The role of tungsten chemical state and boron on ammonia formation using N-2-H-2 radiofrequency discharges}, url = {https://m2.mtmt.hu/api/publication/33306683}, author = {Antunes, R. and Marot, L. and Romero-Muniz, C. and Steiner, R. and Meyer, E.}, doi = {10.1088/1741-4326/ac33c6}, journal-iso = {NUCL FUSION}, journal = {NUCLEAR FUSION}, volume = {61}, unique-id = {33306683}, issn = {0029-5515}, abstract = {This work aims at investigating the role of tungsten and boron surfaces on ammonia production with N-2-H-2 radiofrequency plasmas at 3 Pa. The experiments combine the analysis of the reaction products and surface chemical environment using mass spectrometry and x-ray photoelectron spectroscopy (XPS). We show that NH3 is formed upon discharges of N-2 or H-2 after having exposed a tungsten (W) foil to H-2 or N-2, respectively. A higher amount of ammonia is formed for the N-2-then-H-2 case, which we explain by the larger number of Eley-Rideal reaction channels for the formation of NH x (s) and the lower surface diffusion barrier for adsorbed hydrogen, calculated using the density functional theory (DFT). As a result, H(s) combines with N(s) or NH x (s) through Langmuir-Hinshelwood at a faster rate than N(s) combines with another N(s). The amount of NH3 formed with N-2-H-2 discharges after conditioning the tungsten foil with H-2, N-2 or O-2 was also investigated. We observed that this pre-conditioning plays no major role on the amount of NH3 detected with the residual gas analyser, albeit a small decrease was observed after H-2 contamination. With DFT, the adsorption energies of H on WO3 and W are found to be similar, while the adsorption of N on WO3 is significantly weaker. The similar NH3 concentrations obtained with a clean and oxidized tungsten surface thus suggest that the adsorption of N does not limit the formation rate of ammonia. The production of NH3 on boron was evaluated as well. The boron surface reduced the amount of detected ammonia almost by half. On the one side, a significant amount of H-2 was removed from the surface during the Ar cleaning that followed, which suggests a strong retention of hydrogen. On the other side, the XPS data reveals that nitrogen forms strong bonds with boron and impurities on the surface, regardless on whether hydrogen is previously present on the surface or in the plasma volume. The presence of hydrogen in the plasma volume, simultaneously with nitrogen or after nitrogen exposure, is nevertheless necessary for the formation of NH(s) and NH2(s). No NH3(s) was however detected with XPS. The increased retention of both hydrogen and nitrogen on the boron surface may thus hinder the formation of NH3.}, keywords = {AMMONIA; boron; tungsten; radiofrequency plasmas}, year = {2021}, eissn = {1741-4326} } @article{MTMT:32832271, title = {Nitrogen retention and ammonia production on tungsten}, url = {https://m2.mtmt.hu/api/publication/32832271}, author = {Ghiorghiu, F and Aissou, T and Minissale, M and Angot, T and De, Temmerman G and Bisson, R}, doi = {10.1088/1741-4326/ac3698}, journal-iso = {NUCL FUSION}, journal = {NUCLEAR FUSION}, volume = {61}, unique-id = {32832271}, issn = {0029-5515}, abstract = {We report a systematic study that quantifies nitrogen retention and ammonia production on tungsten and that sheds light on the mechanism for ammonia formation on ITER's divertor material. Saturation of the nitrogen-implanted layer in polycrystalline tungsten is observed at room temperature for a nitrogen ion fluence in the low 10(21) N+ m(-2) range. Nitrogen desorption from this N-implanted layer occurs in the 800-1100 K temperature range and exhibits a zero-order kinetics with an activation energy of 1.45 eV and a prefactor of 5 x 10(24) m(-2) s(-1). Following nitrogen and deuterium co-implantation, deuterated ammonia production is observed during temperature programmed desorption between 350 K and 650 K in conjunction with deuterium desorption. In contrast, nitrogen desorption still occurs above 800 K. Significant production of ammonia is obtained only when the nitrogen layer created by ion implantation is approaching saturation and the amount of nitrogen lost to ammonia production is only in the percent range. This result is understood by repeating cycles of deuterium implantation and thermo-desorption below the desorption temperature of the nitrogen layer. The exponential decay of the amount of produced ammonia with cycle number demonstrates that nitrogen diffusion to the surface is negligible in the ammonia production temperature range and that ammonia formation occurs at the outermost surface layer. The maximum quantity of ammonia produced from the present N implanted layer is below 2 x 10(18) ND3 m(-2), which is limited by the nitrogen atom surface density. Surface vibrational spectroscopy demonstrates the presence of ammonia precursors on the nitrogen-implanted tungsten surface upon deuterium implantation. These ammonia precursors can be created also at room temperature through the dissociative chemisorption of thermal D-2 catalysed by nitrogen present at the tungsten surface and, more efficiently, by adsorption of deuterium atoms.}, year = {2021}, eissn = {1741-4326} } @article{MTMT:33271671, title = {Parameter dependencies of the experimental nitrogen concentration required for detachment on ASDEX Upgrade and JET}, url = {https://m2.mtmt.hu/api/publication/33271671}, author = {Henderson, S.S. and Bernert, M. and Giroud, C. and Brida, D. and Cavedon, M. and David, P. and Dux, R. and Harrison, J.R. and Huber, A. and Kallenbach, A. and Karhunen, J. and Lomanowski, B. and Matthews, G. and Meigs, A. and Pitts, R.A. and Reimold, F. and Reinke, M.L. and Silburn, S. and Vianello, N. and Wiesen, S. and Wischmeier, M.}, doi = {10.1016/j.nme.2021.101000}, journal-iso = {NUCL MATER ENERGY}, journal = {NUCLEAR MATERIALS AND ENERGY}, volume = {28}, unique-id = {33271671}, year = {2021}, eissn = {2352-1791} } @article{MTMT:32003518, title = {Developments towards an ELM-free pedestal radiative cooling scenario using noble gas seeding in ASDEX Upgrade}, url = {https://m2.mtmt.hu/api/publication/32003518}, author = {Kallenbach, A and Bernert, M and David, P and Dunne, MG and Dux, R and Fable, E and Fischer, R and Gil, L and Gorler, T and Janky, F and McDermott, RM and Suttrop, W and Tardini, G and Wischmeier, M and Plasma, Frigyes}, doi = {10.1088/1741-4326/abbba0}, journal-iso = {NUCL FUSION}, journal = {NUCLEAR FUSION}, volume = {61}, unique-id = {32003518}, issn = {0029-5515}, year = {2021}, eissn = {1741-4326} } @article{MTMT:32056889, title = {Comparison of divertor behavior and plasma confinement between argon and neon seeding in EAST}, url = {https://m2.mtmt.hu/api/publication/32056889}, author = {Li, KD and Yang, ZS and Wang, HQ and Xu, GS and Yuan, QP and Guo, HY and Eldon, D and Hyatt, AL and Humphreys, D and Chen, MW and Wu, K and Liu, JB and He, T and Yang, QQ and Lin, X and Xu, JC and Meng, LY and Ding, F and Chen, XH and Luo, Y and Wu, JH and Duan, YM and Luo, GN and Wang, L}, doi = {10.1088/1741-4326/abf418}, journal-iso = {NUCL FUSION}, journal = {NUCLEAR FUSION}, volume = {61}, unique-id = {32056889}, issn = {0029-5515}, year = {2021}, eissn = {1741-4326} } @article{MTMT:32093281, title = {H-mode plasmas in the pre-fusion power operation 1 phase of the ITER research plan}, url = {https://m2.mtmt.hu/api/publication/32093281}, author = {Loarte, A and Polevoi, AR and Schneider, M and Pinches, SD and Fable, E and Asp, EM and Baranov, Y and Casson, F and Corrigan, G and Garzotti, L and Harting, D and Knight, P and Koechl, F and Parail, V and Farina, D and Figini, L and Nordman, H and Strand, P and Sartori, R}, doi = {10.1088/1741-4326/abfb13}, journal-iso = {NUCL FUSION}, journal = {NUCLEAR FUSION}, volume = {61}, unique-id = {32093281}, issn = {0029-5515}, year = {2021}, eissn = {1741-4326} } @article{MTMT:32404885, title = {Detection of Ammonia and Deuterated Hydrocarbons in Exhaust Gas by Infrared Absorption Spectroscopy duringWall Conditioning}, url = {https://m2.mtmt.hu/api/publication/32404885}, author = {Tanaka, Masahiro and Kato, Hiromi and Suzuki, Naoyuki and Chimura, Hiroki}, doi = {10.1585/pfr.16.2405062}, journal-iso = {PLASMA FUSION RES}, journal = {PLASMA AND FUSION RESEARCH}, volume = {16}, unique-id = {32404885}, issn = {1880-6821}, abstract = {To detect ammonia and deuterated hydrocarbons in exhaust gas from the Large Helical Device (LHD), infrared absorption spectrometry, FTIR with a long optical path gas cell, was applied. Ammonia (NH3) and deuterated hydrocarbons (CxHyDz) could be detected during the first operations of wall baking at 368K and the D-2 glow discharge conducted after vacuum vessel closure. The concentration of ammonia increased with increasing baking temperature, and deuterated ammonia was not detected. Thus, the ammonia, which likely originated from sweat of workers produced during vacuum vessel maintenance activities, was released from the vacuum vessel wall. Hydrocarbons were likely produced by chemical sputtering of carbon tiles and were deuterated by a hydrogen isotope exchange reaction due to D-2 glow discharge, while H2O was released from the vacuum vessel during wall baking. It was confirmed that ammonia and various types of deuterated hydrocarbons could be measured discriminately by an FTIR spectroscopy system using a long optical path gas cell. (C) 2021 The Japan Society of Plasma Science and Nuclear Fusion Research}, keywords = {AMMONIA; FTIR; infrared absorption spectroscopy; exhaust gas monitoring; large fusion test device; deuterated hydrocarbons}, year = {2021} } @article{MTMT:30976340, title = {Plasma-activated catalytic formation of ammonia from N-2?H-2: influence of temperature and noble gas addition}, url = {https://m2.mtmt.hu/api/publication/30976340}, author = {Ben Yaala, M and Scherrer, DF and Saeedi, A and Moser, L and Soni, K and Steiner, R and De, Temmerman G and Oberkofler, M and Marot, L and Meyer, E}, doi = {10.1088/1741-4326/ab519c}, journal-iso = {NUCL FUSION}, journal = {NUCLEAR FUSION}, volume = {60}, unique-id = {30976340}, issn = {0029-5515}, year = {2020}, eissn = {1741-4326} } @article{MTMT:33264723, title = {Long pulse D2and N2seeded discharges on the upper actively cooled tungsten divertor of WEST}, url = {https://m2.mtmt.hu/api/publication/33264723}, author = {Dittmar, T. and Loarer, T. and Drenik, A. and Bourdelle, C. and Brezinsek, S. and Desgranges, C. and Douai, D. and Fedorczak, N. and Guirlet, R. and Gunn, J. and Meyer, O. and Laguardia, L. and Tsitrone, E.}, doi = {10.1088/1402-4896/ab753f}, journal-iso = {PHYS SCR}, journal = {PHYSICA SCRIPTA}, volume = {T171}, unique-id = {33264723}, issn = {0031-8949}, year = {2020}, eissn = {1402-4896} } @article{MTMT:31418133, title = {Impurity transport and divertor retention in Ar and N seeded SOLPS 5.0 simulations for ASDEX Upgrade}, url = {https://m2.mtmt.hu/api/publication/31418133}, author = {Hitzler, F and Wischmeier, M and Reimold, F and Coster, DP}, doi = {10.1088/1361-6587/ab9b00}, journal-iso = {PLASMA PHYS CONTR F}, journal = {PLASMA PHYSICS AND CONTROLLED FUSION}, volume = {62}, unique-id = {31418133}, issn = {0741-3335}, year = {2020}, eissn = {1361-6587} } @article{MTMT:33336276, title = {Long discharges in a steady state with D2and N2on the actively cooled tungsten upper divertor in WEST}, url = {https://m2.mtmt.hu/api/publication/33336276}, author = {Loarer, T. and Dittmar, T. and Tsitrone, E. and Bisson, R. and Bourdelle, C. and Brezinsek, S. and Bucalossi, J. and Corre, Y. and Delpech, L. and Desgranges, C. and De, Temmerman G. and Douai, D. and Ekedahl, A. and Fedorczak, N. and Gallo, A. and Gaspar, J. and Gunn, J. and Houry, M. and Maget, P. and Mitteau, R. and Moreau, P.}, doi = {10.1088/1741-4326/abb919}, journal-iso = {NUCL FUSION}, journal = {NUCLEAR FUSION}, volume = {60}, unique-id = {33336276}, issn = {0029-5515}, year = {2020}, eissn = {1741-4326} } @article{MTMT:30990585, title = {Non-equilibrium characteristics of vibrational and rotational temperatures of N-2-B and C States puffed onto argon arc jet plume}, url = {https://m2.mtmt.hu/api/publication/30990585}, author = {Fukukawa, S and Nezu, A and Akatsuka, H}, doi = {10.7567/1347-4065/ab3c41}, journal-iso = {JPN J APPL PHYS}, journal = {JAPANESE JOURNAL OF APPLIED PHYSICS (2008)}, volume = {58}, unique-id = {30990585}, issn = {0021-4922}, year = {2019}, eissn = {1347-4065} } @article{MTMT:30976862, title = {Active conditioning of ASDEX Upgrade tungsten plasma-facing components and discharge enhancement through boron and boron nitride particulate injection}, url = {https://m2.mtmt.hu/api/publication/30976862}, author = {Lunsford, R and Rohde, V and Bortolon, A and Dux, R and Herrmann, A and Kallenbach, A and McDermott, RM and David, P and Drenik, A and Laggner, F and Maingi, R and Mansfield, DK and Nagy, A and Neu, R and Wolfrum, E}, doi = {10.1088/1741-4326/ab4095}, journal-iso = {NUCL FUSION}, journal = {NUCLEAR FUSION}, volume = {59}, unique-id = {30976862}, issn = {0029-5515}, year = {2019}, eissn = {1741-4326} } @article{MTMT:31813434, title = {Overview of physics studies on ASDEX Upgrade}, url = {https://m2.mtmt.hu/api/publication/31813434}, author = {Meyer, H and Aguiam, D and Angioni, C and Albert, CG and Arden, N and Parra, RA and Asunta, O and de, Baar M and Balden, M and Bandaru, V and Behler, K and Bergmann, A and Bernardo, J and Bernert, M and Biancalani, A and Bilato, R and Birkenmeier, G and Blanken, TC and Bobkov, V and Bock, A and Bolzonella, T and Bortolon, A and Boswirth, B and Bottereau, C and Bottino, A and van, den Brand H and Brezinsek, S and Brida, D and Brochard, F and Bruhn, C and Buchanan, J and Buhler, A and Burckhart, A and Camenen, Y and Carlton, D and Carr, M and Carralero, D and Castaldo, C and Cavedon, M and Cazzaniga, C and Ceccuzzi, S and Challis, C and Chankin, A and Chapman, S and Cianfarani, C and Clairet, F and Coda, S and Coelho, R and Coenen, JW and Colas, L and Conway, GD and Costea, S and Coster, DP and Cote, TB and Creely, A and Croci, G and Cseh, Gábor and Czarnecka, A and Cziegler, I and D'Arcangelo, O and David, P and Day, C and Delogu, R and de, Marne P and Denk, SS and Denner, P and Dibon, M and Di, Siena A and Douai, D and Drenik, A and Drube, R and Dunne, M and Duval, BP and Dux, R and Eich, T and Elgeti, S and Engelhardt, K and Erdős, Boglárka and Erofeev, I and Esposito, B and Fable, E and Faitsch, M and Fantz, U and Faugel, H and Faust, I and Felici, F and Ferreira, J and Fietz, S and Figuereido, A and Fischer, R and Ford, O and Frassinetti, L and Freethy, S and Froschle, M and Fuchert, G and Fuchs, JC and Funfgelder, H and Galazka, K and Galdon-Quiroga, J and Gallo, A and Gao, Y and Garavaglia, S and Garcia-Carrasco, A and Garcia-Munoz, M and Geiger, B and Giannone, L and Gil, L and Giovannozzi, E and Gleason-Gonzalez, C and Gloggler, S and Gobbin, M and Gorler, T and Ortiz, IG and Martin, JG and Goodman, T and Gorini, G and Gradic, D and Grater, A and Granucci, G and Greuner, H and Griener, M and Groth, M and Gude, A and Gunter, S and Guimarais, L and Haas, G and Hakola, AH and Ham, C and Happel, T and den, Harder N and Harrer, GF and Harrison, J and Hauer, V and Hayward-Schneider, T and Hegna, CC and Heinemann, B and Heinzel, S and Hellsten, T and Henderson, S and Hennequin, P and Herrmann, A and Heyn, MF and Heyn, E and Hitzler, F and Hobirk, J and Hofler, K and Holzl, M and Hoschen, T and Holm, JH and Hopf, C and Hornsby, WA and Horvath, L and Houben, A and Huber, A and Igochine, V and Ilkei, Tamás and Ivanova-Stanik, I and Jacob, W and Jacobsen, AS and Janky, F and van, Vuuren AJ and Jardin, A and Jaulmes, F and Jenko, F and Jensen, T and Joffrin, E and Kasemann, CP and Kallenbach, A and Kálvin, Sándor Csaba and Kantor, M and Kappatou, A and Kardaun, O and Karhunen, J and Kasilov, S and Kazakov, Y and Kernbichler, W and Kirk, A and Hansen, SK and Klevarova, V and Kocsis, Lajos Gábor and Kohn, A and Koubiti, M and Krieger, K and Krivska, A and Kramer-Flecken, A and Kudlacek, O and Kurki-Suonio, T and Kurzan, B and Labit, B and Lackner, K and Laggner, F and Lang, PT and Lauber, P and Lebschy, A and Leuthold, N and Li, M and Linder, O and Lipschultz, B and Liu, F and Liu, Y and Lohs, A and Lu, Z and di, Cortemiglia TL and Luhmann, NC and Lunsford, R and Lunt, T and Lyssoivan, A and Maceina, T and Madsen, J and Maggiora, R and Maier, H and Maj, O and Mailloux, J and Maingi, R and Maljaars, E and Manas, P and Mancini, A and Manhard, A and Manso, ME and Mantica, P and Mantsinen, M and Manz, P and Maraschek, M and Martens, C and Martin, P and Marrelli, L and Martitsch, A and Mayer, M and Mazon, D and McCarthy, PJ and McDermott, R and Meister, H and Medvedeva, A and Merkel, R and Merle, A and Mertens, V and Meshcheriakov, D and Meyer, O and Miettunen, J and Milanesio, D and Mink, F and Mlynek, A and Monaco, F and Moon, C and Nabais, F and Nemes-Czopf, A and Neu, G and Neu, R and Nielsen, AH and Nielsen, SK and Nikolaeva, V and Nocente, M and Noterdaeme, JM and Novikau, I and Nowak, S and Oberkofler, M and Oberparleiter, M and Ochoukov, R and Odstrcil, T and Olsen, J and Orain, F and Palermo, F and Pan, O and Papp, G and Perez, IP and Pau, A and Pautasso, G and Penzel, F and Petersson, P and Acosta, JP and Piovesan, P and Piron, C and Pitts, R and Plank, U and Plaum, B and Ploeckl, B and Plyusnin, V and Pokol, G and Poli, E and Porte, L and Potzel, S and Prisiazhniuk, D and Putterich, T and Ramisch, M and Rasmussen, J and Ratt, GA and Ratynskaia, S and Raupp, G and Ravera, GL and Réfy, Dániel and Reich, M and Reimold, F and Reiser, D and Ribeiro, T and Riesch, J and Riedl, R and Rittich, D and Rivero-Rodriguez, JF and Rocchi, G and Rodriguez-Ramos, M and Rohde, V and Ross, A and Rott, M and Rubel, M and Ryan, D and Ryter, F and Saarelma, S and Salewski, M and Salmi, A and Sanchis-Sanchez, L and Santos, J and Sauter, O and Scarabosio, A and Schall, G and Schmid, K and Schmitz, O and Schneider, PA and Schrittwieser, R and Schubert, M and Schwarz-Selinger, T and Schweinzer, J and Scott, B and Sehmer, T and Seliunin, E and Sertoli, M and Shabbir, A and Shalpegin, A and Shao, L and Sharapov, S and Sias, G and Siccinio, M and Sieglin, B and Sigalov, A and Silva, A and Silva, C and Silvagni, D and Simon, P and Simpson, J and Smigelskis, E and Snicker, A and Sommariva, C and Sozzi, C and Spolaore, M and Stegmeir, A and Stejner, M and Stober, J and Stroth, U and Strumberger, E and Suarez, G and Sun, HJ and Suttrop, W and Sytova, E and Szepesi, Tamás Zoltán and Tál, Balázs and Tala, T and Tardini, G and Tardocchi, M and Teschke, M and Terranova, D and Tierens, W and Thoren, E and Told, D and Tolias, P and Tudisco, O and Treutterer, W and Trier, E and Tripsky, M and Valisa, M and Valovic, M and Vanovac, B and van, Vugt D and Varoutis, S and Verdoolaege, G and Vianello, N and Vicente, J and Vierle, T and Viezzer, E and von, Toussaint U and Wagner, D and Wang, N and Wang, X and Weiland, M and White, AE and Wiesen, S and Willensdorfer, M and Wiringer, B and Wischmeier, M and Wolf, R and Wolfrum, E and Xiang, L and Yang, Q and Yang, Z and Yu, Q and Zagorski, R and Zammuto, I and Zhang, W and van, Zeeland M and Zehetbauer, T and Zilker, M and Zoletnik, Sándor and Zohm, H}, doi = {10.1088/1741-4326/ab18b8}, journal-iso = {NUCL FUSION}, journal = {NUCLEAR FUSION}, volume = {59}, unique-id = {31813434}, issn = {0029-5515}, year = {2019}, eissn = {1741-4326} } @article{MTMT:31016928, title = {Physics basis for the first ITER tungsten divertor}, url = {https://m2.mtmt.hu/api/publication/31016928}, author = {Pitts, R. A. and Bonnin, X. and Escourbiac, F. and Frerichs, H. and Gunn, J. P. and Hirai, T. and Kukushkin, A. S. and Kaveeva, E. and Miller, M. A. and Moulton, D. and Rozhansky, V. and Senichenkov, I. and Sytova, E. and Schmitz, O. and Stangeby, P. C. and De Temmerman, G. and Veselova, I. and Wiesen, S.}, doi = {10.1016/j.nme.2019.100696}, journal-iso = {NUCL MATER ENERGY}, journal = {NUCLEAR MATERIALS AND ENERGY}, volume = {20}, unique-id = {31016928}, abstract = {On the eve of component procurement, this paper discusses the present physics basis for the first ITER tungsten (W) divertor, beginning with a reminder of the key elements defining the overall design, and outlining relevant aspects of the Research Plan accompanying the new "staged approach" to ITER nuclear operations which fixes the overall divertor lifetime constraint. The principal focus is on the main design driver, steady state power fluxes in the DT phases, obtained from simulations using the 2-D SOLPS-4.3 and SOLPS-ITER plasma boundary codes, assuming the use of the low Z seeding impurities nitrogen (N) and neon (Ne). A new perspective on the simulation database is adopted, concentrating purely on the divertor physics aspects rather than on the core-edge integration, which has been studied extensively in the course of the divertor design evolution and is published elsewhere. Emphasis is placed on factors which may increase the peak steady state loads: divertor target shaping for component misalignment protection, the influence of fluid drifts, and the consequences of narrow scrape-off layer heat flux channels. All tend to push the divertor into an operating space at higher sub-divertor neutral pressure in order to remain at power flux densities acceptable for the target material. However, a revised criterion for the maximum tolerable loads based on avoidance of W recrystallization, sets an upper limit potentially similar to 50% higher than the previously accepted value of similar to 10 MW m(-2), a consequence both of the choice of material and the finalized component design. Although the simulation database is currently restricted to the 2-D toroidally symmetric situation, considerable progress is now also being made using the EMC3-Eirene 3-D code suite for the assessment of power loading in the presence of magnetic perturbations for ELM control. Some new results for low input power corresponding to the early H-mode operation phases are reported, showing that even if realistic plasma screening is taken into account, significant asymmetric divertor heat fluxes may arise far from the unperturbed strike point. The issue of tolerable limits for transient heat pulses is an open and key question. A new scaling for ELM power deposition has shown that whilst there may be more latitude for operation at higher current without ELM control, the ultimate limit is likely to be set more by material fatigue under large numbers of sub-threshold melting events.}, keywords = {tungsten; ITER; divertor; SOLPS; Heat fluxes}, year = {2019}, eissn = {2352-1791} }