309 results on '"Chomiczewska, A."'
Search Results
2. Microbe cultivation guidelines to optimize rhamnolipid applications
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Ilona E. Kłosowska-Chomiczewska, Adam Macierzanka, Karol Parchem, Pamela Miłosz, Sonia Bladowska, Iga Płaczkowska, Weronika Hewelt-Belka, and Christian Jungnickel
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Biosurfactant design ,Rhamnolipid biosynthesis ,Micellar solubilization ,Microbial cultivation ,QSPR ,Medicine ,Science - Abstract
Abstract In the growing landscape of interest in natural surfactants, selecting the appropriate one for specific applications remains challenging. The extensive, yet often unsystematized, knowledge of microbial surfactants, predominantly represented by rhamnolipids (RLs), typically does not translate beyond the conditions presented in scientific publications. This limitation stems from the numerous variables and their interdependencies that characterize microbial surfactant production. We hypothesized that a computational recipe for biosynthesizing RLs with targeted applicational properties could be developed from existing literature and experimental data. We amassed literature data on RL biosynthesis and micellar solubilization and augmented it with our experimental results on the solubilization of triglycerides (TGs), a topic underrepresented in current literature. Utilizing this data, we constructed mathematical models that can predict RL characteristics and solubilization efficiency, represented as logPRL = f(carbon and nitrogen source, parameters of biosynthesis) and logMSR = f(solubilizate, rhamnolipid (e.g. logPRL), parameters of solubilization), respectively. The models, characterized by robust R2 values of respectively 0.581–0.997 and 0.804, enabled the ranking of descriptors based on their significance and impact—positive or negative—on the predicted values. These models have been translated into ready-to-use calculators, tools designed to streamline the selection process for identifying a biosurfactant optimally suited for intended applications.
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- 2024
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3. Impurity behaviour in JET high-current baseline scenario for Deuterium, Tritium and Deuterium-Tritium plasmas
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N. Wendler, A. Chomiczewska, W. Gromelski, E. Kowalska-Strzęciwilk, G. Telesca, I. Ivanova–Stanik, L. Garzotti, D. Van Eester, V.K. Zotta, D. Frigione, F. Rimini, and G. Pucella
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Deuterium-Tritium plasmas ,JET tokamak ,Plasma impurities ,Plasma radiation ,Nuclear engineering. Atomic power ,TK9001-9401 - Abstract
To support future ITER operation, experimental campaigns at the Joint European Torus (JET) with an ITER-like wall (tungsten divertor and beryllium main chamber) in pure deuterium (D), tritium (T) and Deuterium-Tritium (D-T) were performed. One of the most important challenges in recent years was the development of two main scenarios that investigated different approaches to achieve the high fusion power as well as good plasma confinement (Garzotti et al., 2023). The first one, so-called baseline scenario is relying on high plasma current (Ip≈3.5 MA), normalized beta βN 2 and safety factor q95 ≈ 4.8 (Hobirk et al., 2023).In this paper we focus on the impurity behaviour analysis for the baseline discharges at Ip = 3.5 MA and BT = 3.3 T with D, T and DT plasmas, in which the gas and power waveform were optimized to achieve the best possible performance. In particular, we study the impact of total heating power (Ptot + Palpha), flat-top gas flow and ELM (edge localized modes) frequency on mid-Z (Nickel (Ni), Copper (Cu)) and high-Z (Tungsten (W)) impurities. In addition, we compared the two best performing pulses of the baseline scenario (Ip = 3.5MA, BT = 3.3 T and Pin ≈ 35 MW) in D and DT in order to identify the causes responsible for the increase in radiation during the DT pulse, which led to an early plasma termination. All presented results rely on the data collected by the VUV as well as the bolometry system. Detailed analysis indicates that in the baseline scenario, higher radiation, which is most likely due to the tungsten (W), is observed for T and DT plasmas in comparison to D. Moreover, for the two best performing baseline pulses, tomographic reconstructions show that the radiated power density is mainly emitted from the low field side (LFS) of the plasma and W does not accumulate in the plasma center (Telesca et al., 2024).
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- 2024
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4. Interfacial behaviour of human bile and its substitution for in vitro lipolysis studies
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Dulko, Dorota, Kłosowska-Chomiczewska, Ilona E., del Castillo-Santaella, Teresa, Cabrerizo-Vílchez, Miguel A., Łuczak, Justyna, Staroń, Robert, Krupa, Łukasz, Maldonado-Valderrama, Julia, and Macierzanka, Adam
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- 2024
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5. Impurity behaviour in JET high-current baseline scenario for Deuterium, Tritium and Deuterium-Tritium plasmas
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Wendler, N., Chomiczewska, A., Gromelski, W., Kowalska-Strzęciwilk, E., Telesca, G., Ivanova–Stanik, I., Garzotti, L., Van Eester, D., Zotta, V.K., Frigione, D., Rimini, F., and Pucella, G.
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- 2024
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6. Intelligent service robots for elderly or disabled people and human dignity: legal point of view
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Pfeifer-Chomiczewska, Katarzyna
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- 2023
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7. Effect of oxidation and in vitro intestinal hydrolysis on phospholipid toxicity towards HT29 cell line serving as a model of human intestinal epithelium
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Parchem, Karol, Baranowska, Monika, Kościelak, Anna, Kłosowska-Chomiczewska, Ilona, Domingues, M. Rosário, Macierzanka, Adam, and Bartoszek, Agnieszka
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- 2023
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8. Bivalves Transmissible Neoplasia: Biochemical Aspects of Contagious Cancer in a Clam Macoma Balthica
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Anna Hallmann, Alicja Michnowska, Agnieszka Chomiczewska, Marcin Lipiński, and Katarzyna Smolarz
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Physiology ,QP1-981 ,Biochemistry ,QD415-436 - Published
- 2022
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9. Experimental research on the TCV tokamak
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B.P. Duval, A. Abdolmaleki, M. Agostini, C.J. Ajay, S. Alberti, E. Alessi, G. Anastasiou, Y. Andrèbe, G.M. Apruzzese, F. Auriemma, J. Ayllon-Guerola, F. Bagnato, A. Baillod, F. Bairaktaris, L. Balbinot, A. Balestri, M. Baquero-Ruiz, C. Barcellona, M. Bernert, W. Bin, P. Blanchard, J. Boedo, T. Bolzonella, F. Bombarda, L. Boncagni, M. Bonotto, T.O.S.J. Bosman, D. Brida, D. Brunetti, J. Buchli, J. Buerman, P. Buratti, A. Burckhart, D. Busil, J. Caloud, Y. Camenen, A. Cardinali, S. Carli, D. Carnevale, F. Carpanese, M. Carpita, C. Castaldo, F. Causa, J. Cavalier, M. Cavedon, J.A. Cazabonne, J. Cerovsky, B. Chapman, M. Chernyshova, P. Chmielewski, A. Chomiczewska, G. Ciraolo, S. Coda, C. Colandrea, C. Contré, R. Coosemans, L. Cordaro, S. Costea, T. Craciunescu, K. Crombe, A. Dal Molin, O. D’Arcangelo, D. de Las Casas, J. Decker, J. Degrave, H. de Oliveira, G.L. Derks, L.E. di Grazia, C. Donner, M. Dreval, M.G. Dunne, G. Durr-Legoupil-Nicoud, B. Esposito, T. Ewalds, M. Faitsch, M. Farník, A. Fasoli, F. Felici, J. Ferreira, O. Février, O. Ficker, A. Frank, E. Fransson, L. Frassinetti, L. Fritz, I. Furno, D. Galassi, K. Gałązka, J. Galdon-Quiroga, S. Galeani, C. Galperti, S. Garavaglia, M. Garcia-Munoz, P. Gaudio, M. Gelfusa, J. Genoud, R. Gerrú Miguelanez, G. Ghillardi, M. Giacomin, L. Gil, A. Gillgren, C. Giroud, T. Golfinopoulos, T. Goodman, G. Gorini, S. Gorno, G. Grenfell, M. Griener, M. Gruca, T. Gyergyek, R. Hafner, M. Hamed, D. Hamm, W. Han, G. Harrer, J.R. Harrison, D. Hassabis, S. Henderson, P. Hennequin, J. Hidalgo-Salaverri, J-P. Hogge, M. Hoppe, J. Horacek, A. Huber, E. Huett, A. Iantchenko, P. Innocente, C. Ionita-Schrittwieser, I. Ivanova Stanik, M. Jablczynska, A. Jansen van Vuuren, A. Jardin, H. Järleblad, A.E. Järvinen, J. Kalis, R. Karimov, A.N. Karpushov, K. Kavukcuoglu, J. Kay, Y. Kazakov, J. Keeling, A. Kirjasuo, J.T.W. Koenders, P. Kohli, M. Komm, M. Kong, J. Kovacic, E. Kowalska-Strzeciwilk, O. Krutkin, O. Kudlacek, U. Kumar, R. Kwiatkowski, B. Labit, L. Laguardia, E. Laszynska, A. Lazaros, K. Lee, E. Lerche, B. Linehan, D. Liuzza, T. Lunt, E. Macusova, D. Mancini, P. Mantica, M. Maraschek, G. Marceca, S. Marchioni, A. Mariani, M. Marin, A. Marinoni, L. Martellucci, Y. Martin, P. Martin, L. Martinelli, F. Martinelli, J.R. Martin-Solis, S. Masillo, R. Masocco, V. Masson, A. Mathews, M. Mattei, D. Mazon, S. Mazzi, S.Y. Medvedev, C. Meineri, A. Mele, V. Menkovski, A. Merle, H. Meyer, K. Mikszuta-Michalik, I.G. Miron, P.A. Molina Cabrera, A. Moro, A. Murari, P. Muscente, D. Mykytchuk, F. Nabais, F. Napoli, R.D. Nem, M. Neunert, S.K. Nielsen, A. Nielsen, M. Nocente, S. Noury, S. Nowak, H. Nyström, N. Offeddu, S. Olasz, F. Oliva, D.S. Oliveira, F.P. Orsitto, N. Osborne, P. Oyola Dominguez, O. Pan, E. Panontin, A.D. Papadopoulos, P. Papagiannis, G. Papp, M. Passoni, F. Pastore, A. Pau, R.O. Pavlichenko, A.C. Pedersen, M. Pedrini, G. Pelka, E. Peluso, A. Perek, C. Perez Von Thun, F. Pesamosca, D. Pfau, V. Piergotti, L. Pigatto, C. Piron, L. Piron, A. Pironti, U. Plank, V. Plyusnin, Y.R.J. Poels, G.I. Pokol, J. Poley-Sanjuan, M. Poradzinski, L. Porte, C. Possieri, A. Poulsen, M.J. Pueschel, T. Pütterich, V. Quadri, M. Rabinski, R. Ragona, H. Raj, A. Redl, H. Reimerdes, C. Reux, D. Ricci, M. Riedmiller, S. Rienäcker, D. Rigamonti, N. Rispoli, J.F. Rivero-Rodriguez, C.F. Romero Madrid, J. Rueda Rueda, P.J. Ryan, M. Salewski, A. Salmi, M. Sassano, O. Sauter, N. Schoonheere, R.W. Schrittwieser, F. Sciortino, A. Selce, L. Senni, S. Sharapov, U.A. Sheikh, B. Sieglin, M. Silva, D. Silvagni, B. Simmendefeldt Schmidt, L. Simons, E.R. Solano, C. Sozzi, M. Spolaore, L. Spolladore, A. Stagni, P. Strand, G. Sun, W. Suttrop, J. Svoboda, B. Tal, T. Tala, P. Tamain, M. Tardocchi, A. Tema Biwole, A. Tenaglia, D. Terranova, D. Testa, C. Theiler, A. Thornton, A.S. Thrysoe, M. Tomes, E. Tonello, H. Torreblanca, B. Tracey, M. Tsimpoukelli, C. Tsironis, C.K. Tsui, M. Ugoletti, M. Vallar, M. van Berkel, S. van Mulders, M. van Rossem, C. Venturini, M. Veranda, T. Verdier, K. Verhaegh, L. Vermare, N. Vianello, E. Viezzer, F. Villone, B. Vincent, P. Vincenzi, I. Voitsekhovitch, L. Votta, N.M.T. Vu, Y. Wang, E. Wang, T. Wauters, M. Weiland, H. Weisen, N. Wendler, S. Wiesen, M. Wiesenberger, T. Wijkamp, C. Wüthrich, D. Yadykin, H. Yang, V. Yanovskiy, J. Zebrowski, P. Zestanakis, M. Zuin, and M. Zurita
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TCV ,review ,plasma ,SPC ,EPFL ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
Tokamak à configuration variable (TCV), recently celebrating 30 years of near-continual operation, continues in its missions to advance outstanding key physics and operational scenario issues for ITER and the design of future power plants such as DEMO. The main machine heating systems and operational changes are first described. Then follow five sections: plasma scenarios. ITER Base-Line (IBL) discharges, triangularity studies together with X3 heating and N2 seeding. Edge localised mode suppression, with a high radiation region near the X-point is reported with N _2 injection with and without divertor baffles in a snowflake configuration. Negative triangularity (NT) discharges attained record, albeit transient, β _N ∼ 3 with lower turbulence, higher low-Z impurity transport, vertical stability and density limits and core transport better than the IBL. Positive triangularity L-Mode linear and saturated ohmic confinement confinement saturation, often-correlated with intrinsic toroidal rotation reversals, was probed for D, H and He working gases. H-mode confinement and pedestal studies were extended to low collisionality with electron cyclotron heating obtaining steady state electron iternal transport barrier with neutral beam heating (NBH), and NBH driven H-mode configurations with off-axis co-electron cyclotron current drive. Fast particle physics. The physics of disruptions, runaway electrons and fast ions (FIs) was developed using near-full current conversion at disruption with recombination thresholds characterised for impurity species (Ne, Ar, Kr). Different flushing gases (D2, H2) and pathways to trigger a benign disruption were explored. The 55 kV NBH II generated a rich Alfvénic spectrum modulating the FI fas ion loss detector signal. NT configurations showed less toroidal Alfvén excitation activity preferentially affecting higher FI pitch angles. Scrape-off layer and edge physics. gas puff imaging systems characterised turbulent plasma ejection for several advanced divertor configurations, including NT. Combined diagnostic array divertor state analysis in detachment conditions was compared to modelling revealing an importance for molecular processes. Divertor physics. Internal gas baffles diversified to include shorter/longer structures on the high and/or low field side to probe compressive efficiency. Divertor studies concentrated upon mitigating target power, facilitating detachment and increasing the radiated power fraction employing alternative divertor geometries, optimised X-point radiator regimes and long-legged configurations. Smaller-than-expected improvements with total flux expansion were better modelled when including parallel flows. Peak outer target heat flux reduction was achieved (>50%) for high flux-expansion geometries, maintaining core performance ( H _98 > 1). A reduction in target heat loads and facilitated detachment access at lower core densities is reported. Real-time control. TCV’s real-time control upgrades employed MIMO gas injector control of stable, robust, partial detachment and plasma β feedback control avoiding neoclassical tearing modes with plasma confinement changes. Machine-learning enhancements include trajectory tracking disruption proximity and avoidance as well as a first-of-its-kind reinforcement learning-based controller for the plasma equilibrium trained entirely on a free-boundary simulator. Finally, a short description of TCV’s immediate future plans will be given.
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- 2024
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10. WEST full tungsten operation with an ITER grade divertor
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J. Bucalossi, A. Ekedahl, and the WEST Team, J. Achard, K. Afonin, O. Agullo, T. Alarcon, L. Allegretti, F. Almuhisen, H. Ancher, G. Antar, Y. Anquetin, S. Antusch, V. Anzallo, C. Arnas, J.F. Artaud, M.H. Aumeunier, S.G. Baek, X.Y. Bai, M. Balden, C. Balorin, T. Barbui, A. Barbuti, J. Barlerin, J. Barra, V. Basiuk, T. Batal, O. Baulaigue, A. Bec, M. Becoulet, E. Benoit, E. Bernard, J.M. Bernard, M. Bernert, N. Bertelli, E. Bertrand, P. Beyer, J. Bielecki, P. Bienvenu, R. Bisson, B. Bliewert, G. Bodner, S. Bose, C. Bottereau, C. Bouchand, Y. Boumendjel, F. Bouquey, C. Bourdelle, J. Bourg, S. Brezinsek, F. Brochard, C. Brun, V. Bruno, H. Bufferand, A. Bureau, S. Burles, Y. Camenen, B. Cantone, E. Caprin, M. Carole, S. Carpentier-Chouchana, G. Caulier, F. Causa, N. Cazanave, N. Chanet, O. Chellai, Y. Chen, M. Chernyshova, P. Chmielewski, W. Choe, A. Chomiczewska, G. Ciraolo, F. Clairet, J. Coenen, L. Colas, G. Colledani, J. Colnel, P. Coquillat, E. Corbel, Y. Corre, X. Courtois, T. Czarski, A. Da Ros, R. Daniel, J. Daumas, M. De Combarieu, P. De Vries, C. Dechelle, F. Deguara, R. Dejarnac, J.M. Delaplanche, L.F. Delgado-Aparicio, E. Delmas, L. Delpech, C. Desgranges, P. Devynck, J. Denis, S. Di Genova, R. Diab, A. Diallo, M. Diez, G. Dif-Pradalier, M. Dimitrova, R. Ding, T. Dittmar, L. Doceul, M. Domenes, D. Donovan, D. Douai, L. Dubus, N. Dumas, R. Dumont, F. Durand, A. Durif, F. Durodié, D. Elbeze, S. Ertmer, A. Escarguel, F. Escourbiac, B. Esposito, K. Ezato, F. Faisse, J.L. Farjon, N. Faure, N. Fedorczak, P. Fejoz, F. Felici, C. Fenzi-Bonizec, F. Ferlay, L. Ferrand, L. Fevre, M. Firdaouss, L. Fleury, D. Flouquet, T. Fonghetti, A. Gallo, X. Garbet, J. Garcia, J.L. Gardarein, L. Gargiulo, P. Garibaldi, S. Garitta, J. Gaspar, E. Gauthier, S. Gazzotti, F. Gely, J. Gerardin, G. Gervasini, E. Geulin, M. Geynet, P. Ghendrih, I. Giacalone, C. Gil, S. Ginoux, S. Girard, E. Giroux, G. Giruzzi, M. Goniche, V. Gorse, T. Gray, E. Grelier, C. Grisolia, A. Grosjean, A. Grosman, O. Grover, D. Guibert, D. Guilhem, C. Guillemaut, B. Guillermin, R. Guirlet, J.P. Gunn, Y. Gunsu, T. Gyergyek, S. Hacquin, A. Hakola, J. Harris, J.C. Hatchressian, W. Helou, P. Hennequin, C. Hernandez, L. Hijazi, J. Hillairet, T. Hirai, G.T. Hoang, C. Honoré, M. Houry, A. Huart, G. Huijsmans, P. Huynh, M. Iafrati, F. Imbeaux, N. Imbert, I. Ivanova-Stanik, P. Ivanova, R. Jalageas, A. Jamann, C. Jammes, A. Jardin, L. Jaubert, G. Jiolat, E. Joffrin, C. Johnson, A. Jonas, A. Kirschner, C.C. Klepper, M. Komm, M. Koubiti, S. Kosslow, J. Kovacic, M. Kozeiha, K. Krieger, K. Krol, I. Kudashev, B. Lacroix, L. Laguardia, V. Lamaison, V. Lapleigne, H. Laqua, C. Lau, Y. Lausenaz, R. Lé, M. Le Bohec, N. Lefevre, N. Lemoine, E. Lerche, Y. Lesourd, L. Letellier, M. Lewerentz, Y. Li, A. Liang, P. Linczuk, C. Linsmeier, M. Lipa, X. Litaudon, X. Liu, J. Llorens, T. Loarer, A. Loarte, T. Loewenhoff, G. Lombard, J. Lore, P. Lorenzetto, B. Lu, A. Lumsdaine, R. Lunsford, T. Lunt, G. Luo, P. Magaud, P. Maget, J.F. Mahieu, P. Maini, P. Malard, K. Malinowski, P. Manas, L. Manenc, V. Maquet, Y. Marandet, C. Martin, E.J. Martin, P. Martino, M. Mayer, D. Mazon, S. Mazzi, P. Messina, L. Meunier, D. Midou, G. Miglionico, Y. Mineo, M. Missirlian, R. Mitteau, B. Mitu, D. Moiraf, P. Mollard, G. Momparler, V. Moncada, T. Mondiere, C. Monti, J. Morales, M. Moreau, Ph. Moreau, Y. Moudden, G. Moureau, D. Mouyon, M. Muraglia, T. Nakano, E. Nardon, A. Neff, F. Nespoli, J. Nichols, L. Nicolas, S. Nicollet, R. Nouailletas, M. Ono, V. Ostuni, O. Paillat, C. Parish, H. Park, H. Parrat, J.Y. Pascal, B. Pegourie, F.P. Pellissier, Y. Peneliau, M. Peret, E. Pignoly, G. Pintsuk, R. Pitts, C. Pocheau, A. Podolnik, C. Portafaix, M. Poulos, P. Prochet, A. Puig Sitjes, R. Ragona, M. Rasinski, S. Ratynskaia, G. Raup, X. Regal-Mezin, C. Reux, J. Rice, M. Richou, F. Rigollet, N. Rivals, H. Roche, S. Rodrigues, J. Romazanov, G. Ronchi, C. Ruset, R. Sabot, A. Saille, R. Sakamoto, B. Salamon, F. Samaille, A. Santagiustina, B. Santraine, Y. Sarazin, O. Sauter, Y. Savoie-Peysson, L. Schiesko, M. Scholz, J.L. Schwob, E. Serre, H. Shin, S. Shiraiwa, Ja. Signoret, O. Skalli-Fettachi, P. Sogorb, Y. Song, A. Spring, P. Spuig, S. Sridhar, B. Stratton, C. Talatizi, P. Tamain, R. Tatali, Q. Tichit, A. Torre, L. Toulouse, W. Treutterer, E. Tsitrone, E.A. Unterberg, G. Urbanczyk, G. Van Rooij, N. Varadarajan, S. Vartanian, E. Velly, J.M. Verger, L. Vermare, D. Vezinet, N. Vignal, B. Vincent, S. Vives, D. Volpe, G. Wallace, E. Wang, L. Wang, Y. Wang, Y.S. Wang, T. Wauters, D. Weldon, B. Wirth, M. Wirtz, A. Wojenski, M. Xu, Q.X. Yang, H. Yang, B. Zago, R. Zagorski, B. Zhang, X.J. Zhang, X.L. Zou, and the EUROfusion Tokamak Exploitation Team
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nuclear fusion ,magnetic confinement ,tokamak ,divertor ,WEST ,ITER ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
The mission of WEST (tungsten-W Environment in Steady-state Tokamak) is to explore long pulse operation in a full tungsten (W) environment for preparing next-step fusion devices (ITER and DEMO) with a focus on testing the ITER actively cooled W divertor in tokamak conditions. Following the successful completion of phase 1 (2016-2021), phase 2 started in December 2022 with the lower divertor made entirely of actively cooled ITER-grade tungsten mono-blocks. A boronization prior the first plasma attempt allowed for a smooth startup with the new divertor. Despite the reduced operating window due to tungsten, rapid progress has been made in long pulse operation, resulting in discharges with a pulse length of 100 s and an injected energy of around 300 MJ per discharge. Plasma startup studies were carried out with equatorial boron nitride limiters to compare them with tungsten limiters, while Ion Cyclotron Resonance Heating assisted startup was attempted. High fluence operation in attached regime, which was the main thrust of the first campaigns, already showed the progressive build up of deposits and appearance of dust, impacting the plasma operation as the plasma fluence increased. In total, the cumulated injected energy during the first campaigns reached 43 GJ and the cumulated plasma time exceeded 5 h. Demonstration of controlled X-Point Radiator regime is also reported, opening a promising route for investigating plasma exhaust and plasma-wall interaction issues in more detached regime. This paper summarises the lessons learned from the manufacturing and the first operation of the ITER-grade divertor, describing the progress achieved in optimising operation in a full W environment with a focus on long pulse operation and plasma wall interaction.
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- 2024
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11. Overview of ASDEX upgrade results in view of ITER and DEMO
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H. Zohm, E. Alessi, C. Angioni, N. Arden, V. Artigues, M. Astrain, O. Asunta, M. Balden, V. Bandaru, A. Banon Navarro, M. Bauer, A. Bergmann, M. Bergmann, J. Bernardo, M. Bernert, A. Biancalani, R. Bielajew, R. Bilato, G. Birkenmeier, T. Blanken, V. Bobkov, A. Bock, L. Bock, T. Body, T. Bolzonella, N. Bonanomi, A. Bortolon, B. Böswirth, C. Bottereau, A. Bottino, H. van den Brand, M. Brenzke, S. Brezinsek, D. Brida, F. Brochard, J. Buchanan, A. Buhler, A. Burckhart, Y. Camenen, B. Cannas, P. Cano Megías, D. Carlton, M. Carr, P. Carvalho, C. Castaldo, A. Castillo Castillo, A. Cathey, M. Cavedon, C. Cazzaniga, C. Challis, A. Chankin, A. Chomiczewska, C. Cianfarani, F. Clairet, S. Coda, R. Coelho, J.W. Coenen, L. Colas, G. Conway, S. Costea, D. Coster, T. Cote, A.J. Creely, G. Croci, D.J. Cruz Zabala, G. Cseh, I. Cziegler, O. D’Arcangelo, A. Dal Molin, P. David, C. Day, M. de Baar, P. de Marné, R. Delogu, P. Denner, A. Di Siena, M. Dibon, J.J. Dominguez-Palacios Durán, D. Dunai, M. Dreval, M. Dunne, B.P. Duval, R. Dux, T. Eich, S. Elgeti, A. Encheva, B. Esposito, E. Fable, M. Faitsch, D. Fajardo Jimenez, U. Fantz, M. Farnik, H. Faugel, F. Felici, O. Ficker, A. Figueredo, R. Fischer, O. Ford, L. Frassinetti, M. Fröschle, G. Fuchert, J.C. Fuchs, H. Fünfgelder, S. Futatani, K. Galazka, J. Galdon-Quiroga, D. Gallart Escolà, A. Gallo, Y. Gao, S. Garavaglia, M. Garcia Muñoz, B. Geiger, L. Giannone, S. Gibson, L. Gil, E. Giovannozzi, I. Girka, O. Girka, T. Gleiter, S. Glöggler, M. Gobbin, J.C. Gonzalez, J. Gonzalez Martin, T. Goodman, G. Gorini, T. Görler, D. Gradic, G. Granucci, A. Gräter, G. Grenfell, H. Greuner, M. Griener, M. Groth, O. Grover, A. Gude, L. Guimarais, S. Günter, D. Hachmeister, A.H. Hakola, C. Ham, T. Happel, N. den Harder, G. Harrer, J. Harrison, V. Hauer, T. Hayward-Schneider, B. Heinemann, P. Heinrich, T. Hellsten, S. Henderson, P. Hennequin, M. Herschel, S. Heuraux, A. Herrmann, E. Heyn, F. Hitzler, J. Hobirk, K. Höfler, S. Hörmann, J.H. Holm, M. Hölzl, C. Hopf, L. Horvath, T. Höschen, A. Houben, A. Hubbard, A. Huber, K. Hunger, V. Igochine, M. Iliasova, J. Illerhaus, K. Insulander Björk, C. Ionita-Schrittwieser, I. Ivanova-Stanik, S. Jachmich, W. Jacob, N. Jaksic, A. Jansen van Vuuren, F. Jaulmes, F. Jenko, T. Jensen, E. Joffrin, A. Kallenbach, J. Kalis, A. Kappatou, J. Karhunen, C.-P. Käsemann, S. Kasilov, Y. Kazakov, A. Kendl, W. Kernbichler, E. Khilkevitch, M. Kircher, A. Kirk, S. Kjer Hansen, V. Klevarova, F. Klossek, G. Kocsis, M. Koleva, M. Komm, M. Kong, A. Krämer-Flecken, M. Krause, I. Krebs, A. Kreuzeder, K. Krieger, O. Kudlacek, D. Kulla, T. Kurki-Suonio, B. Kurzan, B. Labit, K. Lackner, F. Laggner, A. Lahtinen, P. Lainer, P.T. Lang, P. Lauber, M. Lehnen, L. Leppin, E. Lerche, N. Leuthold, L. Li, J. Likonen, O. Linder, H. Lindl, B. Lipschultz, Y. Liu, Z. Lu, T. Luda Di Cortemiglia, N.C. Luhmann, T. Lunt, A. Lyssoivan, T. Maceina, J. Madsen, A. Magnanimo, H. Maier, J. Mailloux, R. Maingi, O. Maj, E. Maljaars, V. Maquet, A. Mancini, A. Manhard, P. Mantica, M. Mantsinen, P. Manz, M. Maraschek, C. Marchetto, M. Markl, L. Marrelli, P. Martin, F. Matos, M. Mayer, P.J. McCarthy, R. McDermott, G. Meng, R. Merkel, A. Merle, H. Meyer, M. Michelini, D. Milanesio, V. Mitterauer, P. Molina Cabrera, M. Muraca, F. Nabais, V. Naulin, R. Nazikian, R.D. Nem, R. Neu, A.H. Nielsen, S.K. Nielsen, T. Nishizawa, M. Nocente, I. Novikau, S. Nowak, R. Ochoukov, J. Olsen, P. Oyola, O. Pan, G. Papp, A. Pau, G. Pautasso, C. Paz-Soldan, M. Peglau, E. Peluso, P. Petersson, C. Piron, U. Plank, B. Plaum, B. Plöckl, V. Plyusnin, G. Pokol, E. Poli, A. Popa, L. Porte, J. Puchmayr, T. Pütterich, L. Radovanovic, M. Ramisch, J. Rasmussen, G. Ratta, S. Ratynskaia, G. Raupp, A. Redl, D. Réfy, M. Reich, F. Reimold, D. Reiser, M. Reisner, D. Reiter, B. Rettino, T. Ribeiro, D. Ricci, R. Riedl, J. Riesch, J.F. Rivero Rodriguez, G. Rocchi, P. Rodriguez-Fernandez, V. Rohde, G. Ronchi, M. Rott, M. Rubel, D.A. Ryan, F. Ryter, S. Saarelma, M. Salewski, A. Salmi, O. Samoylov, L. Sanchis Sanchez, J. Santos, O. Sauter, G. Schall, A. Schlüter, J. Scholte, K. Schmid, O. Schmitz, P.A. Schneider, R. Schrittwieser, M. Schubert, C. Schuster, N. Schwarz, T. Schwarz-Selinger, J. Schweinzer, F. Sciortino, O. Seibold-Benjak, A. Shabbir, A. Shalpegin, S. Sharapov, U. Sheikh, A. Shevelev, G. Sias, M. Siccinio, B. Sieglin, A. Sigalov, A. Silva, C. Silva, D. Silvagni, J. Simpson, S. Sipilä, A. Snicker, E. Solano, C. Sommariva, C. Sozzi, M. Spacek, G. Spizzo, M. Spolaore, A. Stegmeir, M. Stejner, D. Stieglitz, J. Stober, U. Stroth, E. Strumberger, G. Suarez Lopez, W. Suttrop, T. Szepesi, B. Tál, T. Tala, W. Tang, G. Tardini, M. Tardocchi, D. Terranova, M. Teschke, E. Thorén, W. Tierens, D. Told, W. Treutterer, G. Trevisan, M. Tripský, P. Ulbl, G. Urbanczyk, M. Usoltseva, M. Valisa, M. Valovic, S. van Mulders, M. van Zeeland, F. Vannini, B. Vanovac, P. Varela, S. Varoutis, T. Verdier, G. Verdoolaege, N. Vianello, J. Vicente, T. Vierle, E. Viezzer, I. Voitsekhovitch, U. von Toussaint, D. Wagner, X. Wang, M. Weiland, D. Wendler, A.E. White, M. Willensdorfer, B. Wiringer, M. Wischmeier, R. Wolf, E. Wolfrum, Q. Yang, C. Yoo, Q. Yu, R. Zagórski, I. Zammuto, T. Zehetbauer, W. Zhang, W. Zholobenko, A. Zibrov, M. Zilker, C.F.B. Zimmermann, A. Zito, S. Zoletnik, the EUROfusion Tokamak Exploitation Team, and the ASDEX Upgrade Team
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tokamak ,MHD stability ,transport modelling ,radiative exhaust ,disruption physics ,ELM free scenarios ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
Experiments on ASDEX Upgrade (AUG) in 2021 and 2022 have addressed a number of critical issues for ITER and EU DEMO. A major objective of the AUG programme is to shed light on the underlying physics of confinement, stability, and plasma exhaust in order to allow reliable extrapolation of results obtained on present day machines to these reactor-grade devices. Concerning pedestal physics, the mitigation of edge localised modes (ELMs) using resonant magnetic perturbations (RMPs) was found to be consistent with a reduction of the linear peeling-ballooning stability threshold due to the helical deformation of the plasma. Conversely, ELM suppression by RMPs is ascribed to an increased pedestal transport that keeps the plasma away from this boundary. Candidates for this increased transport are locally enhanced turbulence and a locked magnetic island in the pedestal. The enhanced D-alpha (EDA) and quasi-continuous exhaust (QCE) regimes have been established as promising ELM-free scenarios. Here, the pressure gradient at the foot of the H-mode pedestal is reduced by a quasi-coherent mode, consistent with violation of the high-n ballooning mode stability limit there. This is suggestive that the EDA and QCE regimes have a common underlying physics origin. In the area of transport physics, full radius models for both L- and H-modes have been developed. These models predict energy confinement in AUG better than the commonly used global scaling laws, representing a large step towards the goal of predictive capability. A new momentum transport analysis framework has been developed that provides access to the intrinsic torque in the plasma core. In the field of exhaust, the X-Point Radiator (XPR), a cold and dense plasma region on closed flux surfaces close to the X-point, was described by an analytical model that provides an understanding of its formation as well as its stability, i.e., the conditions under which it transitions into a deleterious MARFE with the potential to result in a disruptive termination. With the XPR close to the divertor target, a new detached divertor concept, the compact radiative divertor, was developed. Here, the exhaust power is radiated before reaching the target, allowing close proximity of the X-point to the target. No limitations by the shallow field line angle due to the large flux expansion were observed, and sufficient compression of neutral density was demonstrated. With respect to the pumping of non-recycling impurities, the divertor enrichment was found to mainly depend on the ionisation energy of the impurity under consideration. In the area of MHD physics, analysis of the hot plasma core motion in sawtooth crashes showed good agreement with nonlinear 2-fluid simulations. This indicates that the fast reconnection observed in these events is adequately described including the pressure gradient and the electron inertia in the parallel Ohm’s law. Concerning disruption physics, a shattered pellet injection system was installed in collaboration with the ITER International Organisation. Thanks to the ability to vary the shard size distribution independently of the injection velocity, as well as its impurity admixture, it was possible to tailor the current quench rate, which is an important requirement for future large devices such as ITER. Progress was also made modelling the force reduction of VDEs induced by massive gas injection on AUG. The H-mode density limit was characterised in terms of safe operational space with a newly developed active feedback control method that allowed the stability boundary to be probed several times within a single discharge without inducing a disruptive termination. Regarding integrated operation scenarios, the role of density peaking in the confinement of the ITER baseline scenario (high plasma current) was clarified. The usual energy confinement scaling ITER98( p,y ) does not capture this effect, but the more recent H20 scaling does, highlighting again the importance of developing adequate physics based models. Advanced tokamak scenarios, aiming at large non-inductive current fraction due to non-standard profiles of the safety factor in combination with high normalised plasma pressure were studied with a focus on their access conditions. A method to guide the approach of the targeted safety factor profiles was developed, and the conditions for achieving good confinement were clarified. Based on this, two types of advanced scenarios (‘hybrid’ and ‘elevated’ q -profile) were established on AUG and characterised concerning their plasma performance.
- Published
- 2024
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12. Overview of the EUROfusion Tokamak Exploitation programme in support of ITER and DEMO
- Author
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E. Joffrin, M. Wischmeier, M. Baruzzo, A. Hakola, A. Kappatou, D. Keeling, B. Labit, E. Tsitrone, N. Vianello, the ASDEX Upgrade Team, JET Contributors, the MAST-U Team, the TCV Team, the WEST Team, the EUROfusion Tokamak Exploitation Team:, D. Abate, J. Adamek, M. Agostini, C. Albert, F.C.P. Albert Devasagayam, S. Aleiferis, E. Alessi, J. Alhage, S. Allan, J. Allcock, M. Alonzo, G. Anastasiou, E. Andersson Sunden, C. Angioni, Y. Anquetin, L. Appel, G.M. Apruzzese, M. Ariola, C. Arnas, J.F. Artaud, W. Arter, O. Asztalos, L. Aucone, M.H. Aumeunier, F. Auriemma, J. Ayllon, E. Aymerich, A. Baciero, F. Bagnato, L. Bähner, F. Bairaktaris, P. Balázs, L. Balbinot, I. Balboa, M. Balden, A. Balestri, M. Baquero Ruiz, T. Barberis, C. Barcellona, O. Bardsley, S. Benkadda, T. Bensadon, E. Bernard, M. Bernert, H. Betar, R. Bianchetti Morales, J. Bielecki, R. Bilato, P. Bilkova, W. Bin, G. Birkenmeier, R. Bisson, P. Blanchard, A. Bleasdale, V. Bobkov, A. Boboc, A. Bock, K. Bogar, P. Bohm, T. Bolzonella, F. Bombarda, N. Bonanomi, L. Boncagni, D. Bonfiglio, R. Bonifetto, M. Bonotto, D. Borodin, I. Borodkina, T.O.S.J. Bosman, C. Bourdelle, C. Bowman, S. Brezinsek, D. Brida, F. Brochard, R. Brunet, D. Brunetti, V. Bruno, R. Buchholz, J. Buermans, H. Bufferand, P. Buratti, A. Burckhart, J. Cai, R. Calado, J. Caloud, S. Cancelli, F. Cani, B. Cannas, M. Cappelli, S. Carcangiu, A. Cardinali, S. Carli, D. Carnevale, M. Carole, M. Carpita, D. Carralero, F. Caruggi, I.S. Carvalho, I. Casiraghi, A. Casolari, F.J. Casson, C. Castaldo, A. Cathey, F. Causa, J. Cavalier, M. Cavedon, J. Cazabonne, M. Cecconello, L. Ceelen, A. Celora, J. Cerovsky, C.D. Challis, R. Chandra, A. Chankin, B. Chapman, H. Chen, M. Chernyshova, A.G. Chiariello, P. Chmielewski, A. Chomiczewska, C. Cianfarani, G. Ciraolo, J. Citrin, F. Clairet, S. Coda, R. Coelho, J.W. Coenen, I.H. Coffey, C. Colandrea, L. Colas, S. Conroy, C. Contre, N.J. Conway, L. Cordaro, Y. Corre, D. Costa, S. Costea, D. Coster, X. Courtois, C. Cowley, T. Craciunescu, G. Croci, A.M. Croitoru, K. Crombe, D.J. Cruz Zabala, G. Cseh, T. Czarski, A. Da Ros, A. Dal Molin, M. Dalla Rosa, Y. Damizia, O. D’Arcangelo, P. David, M. De Angeli, E. De la Cal, E. De La Luna, G. De Tommasi, J. Decker, R. Dejarnac, D. Del Sarto, G. Derks, C. Desgranges, P. Devynck, S. Di Genova, L.E. di Grazia, A. Di Siena, M. Dicorato, M. Diez, M. Dimitrova, T. Dittmar, L. Dittrich, J.J. Domínguez Palacios Durán, P. Donnel, D. Douai, S. Dowson, S. Doyle, M. Dreval, P. Drews, L. Dubus, R. Dumont, D. Dunai, M. Dunne, A. Durif, F. Durodie, G. Durr Legoupil Nicoud, B. Duval, R. Dux, T. Eich, A. Ekedahl, S. Elmore, G. Ericsson, J. Eriksson, B. Eriksson, F. Eriksson, S. Ertmer, A. Escarguel, B. Esposito, T. Estrada, E. Fable, M. Faitsch, N. Fakhrayi Mofrad, A. Fanni, T. Farley, M. Farník, N. Fedorczak, F. Felici, X. Feng, J. Ferreira, D. Ferreira, N. Ferron, O. Fevrier, O. Ficker, A.R. Field, A. Figueiredo, N. Fil, D. Fiorucci, M. Firdaouss, R. Fischer, M. Fitzgerald, M. Flebbe, M. Fontana, J. Fontdecaba Climent, A. Frank, E. Fransson, L. Frassinetti, D. Frigione, S. Futatani, R. Futtersack, S. Gabriellini, D. Gadariya, D. Galassi, K. Galazka, J. Galdon, S. Galeani, D. Gallart, A. Gallo, C. Galperti, M. Gambrioli, S. Garavaglia, J. Garcia, M. Garcia Munoz, J. Gardarein, L. Garzotti, J. Gaspar, R. Gatto, P. Gaudio, M. Gelfusa, J. Gerardin, S.N. Gerasimov, R. Gerru Miguelanez, G. Gervasini, Z. Ghani, F.M. Ghezzi, G. Ghillardi, L. Giannone, S. Gibson, L. Gil, A. Gillgren, E. Giovannozzi, C. Giroud, G. Giruzzi, T. Gleiter, M. Gobbin, V. Goloborodko, A. González Ganzábal, T. Goodman, V. Gopakumar, G. Gorini, T. Görler, S. Gorno, G. Granucci, D. Greenhouse, G. Grenfell, M. Griener, W. Gromelski, M. Groth, O. Grover, M. Gruca, A. Gude, C. Guillemaut, R. Guirlet, J. Gunn, T. Gyergyek, L. Hagg, J. Hall, C.J. Ham, M. Hamed, T. Happel, G. Harrer, J. Harrison, D. Harting, N.C. Hawkes, P. Heinrich, S. Henderson, P. Hennequin, R. Henriques, S. Heuraux, J. Hidalgo Salaverri, J. Hillairet, J.C. Hillesheim, A. Hjalmarsson, A. Ho, J. Hobirk, E. Hodille, M. Hölzl, M. Hoppe, J. Horacek, N. Horsten, L. Horvath, M. Houry, K. Hromasova, J. Huang, Z. Huang, A. Huber, E. Huett, P. Huynh, A. Iantchenko, M. Imrisek, P. Innocente, C. Ionita Schrittwieser, H. Isliker, P. Ivanova, I. Ivanova Stanik, M. Jablczynska, S. Jachmich, A.S. Jacobsen, P. Jacquet, A. Jansen van Vuuren, A. Jardin, H. Järleblad, A. Järvinen, F. Jaulmes, T. Jensen, I. Jepu, S. Jessica, T. Johnson, A. Juven, J. Kalis, J. Karhunen, R. Karimov, A.N. Karpushov, S. Kasilov, Y. Kazakov, P.V. Kazantzidis, W. Kernbichler, HT. Kim, D.B. King, V.G. Kiptily, A. Kirjasuo, K.K. Kirov, A. Kirschner, A. Kit, T. Kiviniemi, F. Kjær, E. Klinkby, A. Knieps, U. Knoche, M. Kochan, F. Köchl, G. Kocsis, J.T.W. Koenders, L. Kogan, Y. Kolesnichenko, Y. Kominis, M. Komm, M. Kong, B. Kool, S.B. Korsholm, D. Kos, M. Koubiti, J. Kovacic, Y. Kovtun, E. Kowalska Strzeciwilk, K. Koziol, M. Kozulia, A. Krämer Flecken, A. Kreter, K. Krieger, U. Kruezi, O. Krutkin, O. Kudlacek, U. Kumar, H. Kumpulainen, M.H. Kushoro, R. Kwiatkowski, M. La Matina, M. Lacquaniti, L. Laguardia, P. Lainer, P. Lang, M. Larsen, E. Laszynska, K.D. Lawson, A. Lazaros, E. Lazzaro, M.Y.K. Lee, S. Leerink, M. Lehnen, M. Lennholm, E. Lerche, Y. Liang, A. Lier, J. Likonen, O. Linder, B. Lipschultz, A. Listopad, X. Litaudon, E. Litherland Smith, D. Liuzza, T. Loarer, P.J. Lomas, J. Lombardo, N. Lonigro, R. Lorenzini, C. Lowry, T. Luda di Cortemiglia, A. Ludvig Osipov, T. Lunt, V. Lutsenko, E. Macusova, R. Mäenpää, P. Maget, C.F. Maggi, J. Mailloux, S. Makarov, K. Malinowski, P. Manas, A. Mancini, D. Mancini, P. Mantica, M. Mantsinen, J. Manyer, M. Maraschek, G. Marceca, G. Marcer, C. Marchetto, S. Marchioni, A. Mariani, M. Marin, M. Markl, T. Markovic, D. Marocco, S. Marsden, L. Martellucci, P. Martin, C. Martin, F. Martinelli, L. Martinelli, J.R. Martin Solis, R. Martone, M. Maslov, R. Masocco, M. Mattei, G.F. Matthews, D. Matveev, E. Matveeva, M.L. Mayoral, D. Mazon, S. Mazzi, C. Mazzotta, G. McArdle, R. McDermott, K. McKay, A.G. Meigs, C. Meineri, A. Mele, V. Menkovski, S. Menmuir, A. Merle, H. Meyer, K. Mikszuta Michalik, D. Milanesio, F. Militello, A. Milocco, I.G. Miron, J. Mitchell, R. Mitteau, V. Mitterauer, J. Mlynar, V. Moiseenko, P. Molna, F. Mombelli, C. Monti, A. Montisci, J. Morales, P. Moreau, J.M. Moret, A. Moro, D. Moulton, P. Mulholland, M. Muraglia, A. Murari, A. Muraro, P. Muscente, D. Mykytchuk, F. Nabais, Y. Nakeva, F. Napoli, E. Nardon, M.F. Nave, R.D. Nem, A. Nielsen, S.K. Nielsen, M. Nocente, R. Nouailletas, S. Nowak, H. Nyström, R. Ochoukov, N. Offeddu, S. Olasz, C. Olde, F. Oliva, D. Oliveira, H.J.C. Oliver, P. Ollus, J. Ongena, F.P. Orsitto, N. Osborne, R. Otin, P. Oyola Dominguez, D.I. Palade, S. Palomba, O. Pan, N. Panadero, E. Panontin, A. Papadopoulos, P. Papagiannis, G. Papp, V.V. Parail, C. Pardanaud, J. Parisi, A. Parrott, K. Paschalidis, M. Passoni, F. Pastore, A. Patel, B. Patel, A. Pau, G. Pautasso, R. Pavlichenko, E. Pawelec, B. Pegourie, G. Pelka, E. Peluso, A. Perek, E. Perelli Cippo, C. Perez Von Thun, P. Petersson, G. Petravich, Y. Peysson, V. Piergotti, L. Pigatto, C. Piron, L. Piron, A. Pironti, F. Pisano, U. Plank, B. Ploeckl, V. Plyusnin, A. Podolnik, Y. Poels, G. Pokol, J. Poley, G. Por, M. Poradzinski, F. Porcelli, L. Porte, C. Possieri, A. Poulsen, I. Predebon, G. Pucella, M. Pueschel, P. Puglia, O. Putignano, T. Pütterich, V. Quadri, A. Quercia, M. Rabinski, L. Radovanovic, R. Ragona, H. Raj, M. Rasinski, J. Rasmussen, G. Ratta, S. Ratynskaia, R. Rayaprolu, M. Rebai, A. Redl, D. Rees, D. Refy, M. Reich, H. Reimerdes, B.C.G. Reman, O. Renders, C. Reux, D. Ricci, M. Richou, S. Rienacker, D. Rigamonti, F. Rigollet, F.G. Rimini, D. Ripamonti, N. Rispoli, N. Rivals, J.F. Rivero Rodriguez, C. Roach, G. Rocchi, S. Rode, P. Rodrigues, J. Romazanov, C.F. Romero Madrid, J. Rosato, R. Rossi, G. Rubino, J. Rueda Rueda, J. Ruiz Ruiz, P. Ryan, D. Ryan, S. Saarelma, R. Sabot, M. Salewski, A. Salmi, L. Sanchis, A. Sand, J. Santos, K. Särkimäki, M. Sassano, O. Sauter, G. Schettini, S. Schmuck, P. Schneider, N. Schoonheere, R. Schramm, R. Schrittwieser, C. Schuster, N. Schwarz, F. Sciortino, M. Scotto D’Abusco, S. Scully, A. Selce, L. Senni, M. Senstius, G. Sergienko, S.E. Sharapov, R. Sharma, A. Shaw, U. Sheikh, G. Sias, B. Sieglin, S.A. Silburn, C. Silva, A. Silva, D. Silvagni, B. Simmendefeldt Schmidt, L. Simons, J. Simpson, L. Singh, S. Sipilä, Y. Siusko, S. Smith, A. Snicker, E.R. Solano, V. Solokha, M. Sos, C. Sozzi, F. Spineanu, G. Spizzo, M. Spolaore, L. Spolladore, C. Srinivasan, A. Stagni, Z. Stancar, G. Stankunas, J. Stober, P. Strand, C.I. Stuart, F. Subba, G.Y. Sun, H.J. Sun, W. Suttrop, J. Svoboda, T. Szepesi, G. Szepesi, B. Tal, T. Tala, P. Tamain, G. Tardini, M. Tardocchi, D. Taylor, G. Telesca, A. Tenaglia, A. Terra, D. Terranova, D. Testa, C. Theiler, E. Tholerus, B. Thomas, E. Thoren, A. Thornton, A. Thrysoe, Q. TICHIT, W. Tierens, A. Titarenko, P. Tolias, E. Tomasina, M. Tomes, E. Tonello, A. Tookey, M. Toscano Jiménez, C. Tsironis, C. Tsui, A. Tykhyy, M. Ugoletti, M. Usoltseva, D.F. Valcarcel, A. Valentini, M. Valisa, M. Vallar, M. Valovic, SI. Valvis, M. van Berkel, D. Van Eester, S. Van Mulders, M. van Rossem, R. Vann, B. Vanovac, J. Varela Rodriguez, J. Varje, S. Vartanian, M. Vecsei, L. Velarde Gallardo, M. Veranda, T. Verdier, G. Verdoolaege, K. Verhaegh, L. Vermare, G. Verona Rinati, J. Vicente, E. Viezzer, L. Vignitchouk, F. Villone, B. Vincent, P. Vincenzi, M.O. Vlad, G. Vogel, I. Voitsekhovitch, I. Voldiner, P. Vondracek, N.M.T. VU, T. Vuoriheimo, C. Wade, E. Wang, T. Wauters, M. Weiland, H. Weisen, N. Wendler, D. Weston, A. Widdowson, S. Wiesen, M. Wiesenberger, T. Wijkamp, M. Willensdorfer, T. Wilson, A. Wojenski, C. Wuethrich, I. Wyss, L. Xiang, S. Xu, D. Yadykin, Y. Yakovenko, H. Yang, V. Yanovskiy, R. Yi, B. Zaar, G. Zadvitskiy, L. Zakharov, P. Zanca, D. Zarzoso, Y. Zayachuk, J. Zebrowski, M. Zerbini, P. Zestanakis, C. F. B. Zimmermann, M. Zlobinski, A. Zohar, V.K. Zotta, X. Zou, M. Zuin, M. Zurita, and I. Zychor
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JET ,ASDEX Upgrade ,MAST-U ,TCV ,WEST ,Tokamak Exploitation Task Force ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
Within the 9th European Framework programme, since 2021 EUROfusion is operating five tokamaks under the auspices of a single Task Force called ‘Tokamak Exploitation’. The goal is to benefit from the complementary capabilities of each machine in a coordinated way and help in developing a scientific output scalable to future largre machines. The programme of this Task Force ensures that ASDEX Upgrade, MAST-U, TCV, WEST and JET (since 2022) work together to achieve the objectives of Missions 1 and 2 of the EUROfusion Roadmap: i) demonstrate plasma scenarios that increase the success margin of ITER and satisfy the requirements of DEMO and, ii) demonstrate an integrated approach that can handle the large power leaving ITER and DEMO plasmas. The Tokamak Exploitation task force has therefore organized experiments on these two missions with the goal to strengthen the physics and operational basis for the ITER baseline scenario and for exploiting the recent plasma exhaust enhancements in all four devices (PEX: Plasma EXhaust) for exploring the solution for handling heat and particle exhaust in ITER and develop the conceptual solutions for DEMO. The ITER Baseline scenario has been developed in a similar way in ASDEX Upgrade, TCV and JET. Key risks for ITER such as disruptions and run-aways have been also investigated in TCV, ASDEX Upgrade and JET. Experiments have explored successfully different divertor configurations (standard, super-X, snowflakes) in MAST-U and TCV and studied tungsten melting in WEST and ASDEX Upgrade. The input from the smaller devices to JET has also been proven successful to set-up novel control schemes on disruption avoidance and detachment.
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- 2024
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13. COREDIV simulations of D and D–T high current–high power Baseline pulses in JET-ITER like wall
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G. Telesca, A.R. Field, I. Ivanova-Stanik, S. Brezinsek, A. Chomiczewska, D. Frigione, L. Garzotti, E. Kowalska-Strzeciwilk, P. Lomas, J. Mailloux, G. Pucella, F. Rimini, D. Van Eester, R. Zagórski, and JET Contributors
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JET tokamak ,COREDIV ,modelling ,impurity transport ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
The two best performing pulses of the so called ITER-Baseline scenario ( I _p = 3.5 MA and P _in ≈ 35 MW) of JET-ITER like wall, one in deuterium (D) the other in deuterium–tritium (D–T) plasma are examined and compared in this study. Generally, the D–T Baseline pulses exhibit an electron density level higher than the D pulses and the plasma energy is higher than in the comparable D pulses by up to 20%, reaching about 12 MJ in the pulse studied here. In contrast with the D pulses, the D–T pulses are often characterised by the increase in time of the radiated power in the mantle region (0.70 < ρ < 0.95), which may lead to the loss of the edge localised mode activity when the threshold H–L transition power is approached and to the subsequent plasma disruption due to excessive radiation. In this study we try to identify the physical mechanisms responsible for this behaviour using the available experimental data (principally the total radiated power from the bolometry) and the results of the fluid COREDIV model (1D in the core, 2D in the scrape-off-layer (SOL)), self-consistent with respect to core-SOL and also to main plasma-impurities. In fact, the loss of power caused by impurity radiation affects the temperature profile and finally the power to the divertor plate. The electron density and temperature profiles are numerically reconstructed as well as the radiated power density profiles, indicating no major difference in impurity transport in D and D–T. Indeed, the impurity transport coefficients used in COREDIV to match the experimental radiated power profiles are similar in the two pulses. The computed tungsten sources and densities are lower in the D–T pulse and the divertor impurity retention capability is a little better in the D–T pulse, indicatinga stronger collisional drag force in the SOL. The higher electron density and the broadening of its profile are the main cause of the observed increase of the radiated power in the D–T pulse.
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- 2024
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14. Overview of T and D–T results in JET with ITER-like wall
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C.F. Maggi, D. Abate, N. Abid, P. Abreu, O. Adabonyan, M. Afzal, I. Ahmad, M. Akhtar, R. Albanese, S. Aleiferis, E. Alessi, P. Aleynikov, J. Alguacil, J. Alhage, M. Ali, H. Allen, M. Allinson, M. Alonzo, E. Alves, R. Ambrosino, E. Andersson Sundén, P. Andrew, M. Angelone, C. Angioni, I. Antoniou, L. Appel, C. Appelbee, C. Aramunde, M. Ariola, G. Arnoux, G. Artaserse, J.-F. Artaud, W. Arter, V. Artigues, F.J. Artola, A. Ash, O. Asztalos, D. Auld, F. Auriemma, Y. Austin, L. Avotina, J. Ayllón, E. Aymerich, A. Baciero, L. Bähner, F. Bairaktaris, I. Balboa, M. Balden, N. Balshaw, V.K. Bandaru, J. Banks, A. Banon Navarro, C. Barcellona, O. Bardsley, M. Barnes, R. Barnsley, M. Baruzzo, M. Bassan, A. Batista, P. Batistoni, L. Baumane, B. Bauvir, L. Baylor, C. Bearcroft, P. Beaumont, D. Beckett, A. Begolli, M. Beidler, N. Bekris, M. Beldishevski, E. Belli, F. Belli, S. Benkadda, J. Bentley, E. Bernard, J. Bernardo, M. Bernert, M. Berry, L. Bertalot, H. Betar, M. Beurskens, P.G. Bhat, S. Bickerton, J. Bielecki, T. Biewer, R. Bilato, P. Bílková, G. Birkenmeier, R. Bisson, J.P.S. Bizarro, P. Blatchford, A. Bleasdale, V. Bobkov, A. Boboc, A. Bock, G. Bodnar, P. Bohm, L. Bonalumi, N. Bonanomi, D. Bonfiglio, X. Bonnin, P. Bonofiglo, J. Booth, D. Borba, D. Borodin, I. Borodkina, T.O.S.J. Bosman, C. Bourdelle, M. Bowden, I. Božičević Mihalić, S.C. Bradnam, B. Breizman, S. Brezinsek, D. Brida, M. Brix, P. Brown, D. Brunetti, M. Buckley, J. Buermans, H. Bufferand, P. Buratti, A. Burckhart, A. Burgess, A. Buscarino, A. Busse, D. Butcher, G. Calabrò, L. Calacci, R. Calado, R. Canavan, B. Cannas, M. Cannon, M. Cappelli, S. Carcangiu, P. Card, A. Cardinali, S. Carli, P. Carman, D. Carnevale, B. Carvalho, I.S. Carvalho, P. Carvalho, I. Casiraghi, F.J. Casson, C. Castaldo, J.P. Catalan, N. Catarino, F. Causa, M. Cavedon, M. Cecconello, L. Ceelen, C.D. Challis, B. Chamberlain, R. Chandra, C.S. Chang, A. Chankin, B. Chapman, P. Chauhan, M. Chernyshova, A. Chiariello, G.-C. Chira, P. 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Dowson, R. Doyle, M. Dreval, P. Drews, G. Drummond, Ph. Duckworth, H.G. Dudding, R. Dumont, P. Dumortier, D. Dunai, T. Dunatov, M. Dunne, I. Ďuran, F. Durodié, R. Dux, T. Eade, E. Eardley, J. Edwards, T. Eich, A. Eksaeva, H. El-Haroun, R.D. Ellis, G. Ellwood, C. Elsmore, S. Emery, G. Ericsson, B. Eriksson, F. Eriksson, J. Eriksson, L.G. Eriksson, S. Ertmer, G. Evans, S. Evans, E. Fable, D. Fagan, M. Faitsch, D. Fajardo Jimenez, M. Falessi, A. Fanni, T. Farmer, I. Farquhar, B. Faugeras, S. Fazinić, N. Fedorczak, K. Felker, R. Felton, H. Fernandes, D.R. Ferreira, J. Ferreira, G. Ferrò, J. Fessey, O. Février, O. Ficker, A.R. Field, A. Figueiredo, J. Figueiredo, A. Fil, N. Fil, P. Finburg, U. Fischer, G. Fishpool, L. Fittill, M. Fitzgerald, D. Flammini, J. Flanagan, S. Foley, N. Fonnesu, M. Fontana, J.M. Fontdecaba, L. Fortuna, E. Fortuna-Zalesna, M. Fortune, C. Fowler, P. Fox, O. Franklin, E. Fransson, L. Frassinetti, R. Fresa, D. Frigione, T. Fülöp, M. Furseman, S. Gabriellini, D. Gadariya, S. Gadgil, K. Gál, S. Galeani, A. Galkowski, D. Gallart, M. Gambrioli, T. Gans, J. Garcia, M. García-Muñoz, L. Garzotti, J. Gaspar, R. Gatto, P. Gaudio, D. Gear, T. Gebhart, S. Gee, M. Gelfusa, R. George, S.N. Gerasimov, R. Gerru, G. Gervasini, M. Gethins, Z. Ghani, M. Gherendi, P.-I. Gherghina, F. Ghezzi, L. Giacomelli, C. Gibson, L. Gil, M.R. Gilbert, A. Gillgren, E. Giovannozzi, C. Giroud, G. Giruzzi, J. Goff, V. Goloborodko, R. Gomes, J.-F. Gomez, B. Gonçalves, M. Goniche, J. Gonzalez-Martin, A. Goodyear, S. Gore, G. Gorini, T. Görler, N. Gotts, E. Gow, J.P. Graves, J. Green, H. Greuner, E. Grigore, F. Griph, W. Gromelski, M. Groth, C. Grove, R. Grove, N. Gupta, S. Hacquin, L. Hägg, A. Hakola, M. Halitovs, J. Hall, C.J. Ham, M. Hamed, M.R. Hardman, Y. Haresawa, G. Harrer, J.R. Harrison, D. Harting, D.R. Hatch, T. Haupt, J. Hawes, N.C. Hawkes, J. Hawkins, S. Hazael, J. Hearmon, P. Heesterman, P. Heinrich, M. Held, W. Helou, O. Hemming, S.S. Henderson, R. Henriques, R.B. Henriques, D. Hepple, J. Herfindal, G. Hermon, J.C. Hillesheim, K. Hizanidis, A. Hjalmarsson, A. Ho, J. Hobirk, O. Hoenen, C. Hogben, A. Hollingsworth, S. Hollis, E. Hollmann, M. Hölzl, M. Hook, M. Hoppe, J. Horáček, N. Horsten, A. Horton, L.D. Horton, L. Horvath, S. Hotchin, Z. Hu, Z. Huang, E. Hubenov, A. Huber, V. Huber, T. Huddleston, G.T.A. Huijsmans, Y. Husain, P. Huynh, A. Hynes, D. Iglesias, M.V. Iliasova, M. Imríšek, J. Ingleby, P. Innocente, V. Ioannou-Sougleridis, N. Isernia, I. Ivanova-Stanik, E. Ivings, S. Jachmich, T. Jackson, A.S. Jacobsen, P. Jacquet, H. Järleblad, A. Järvinen, F. Jaulmes, N. Jayasekera, F. Jenko, I. Jepu, E. Joffrin, T. Johnson, J. Johnston, C. Jones, E. Jones, G. Jones, L. Jones, T.T.C. Jones, A. Joyce, M. Juvonen, A. Kallenbach, P. Kalnina, D. Kalupin, P. Kanth, A. Kantor, A. Kappatou, O. Kardaun, J. Karhunen, E. Karsakos, Ye.O. Kazakov, V. Kazantzidis, D.L. Keeling, W. Kelly, M. Kempenaars, D. Kennedy, K. Khan, E. Khilkevich, C. Kiefer, H.-T. 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Papadopoulos, G. Papp, V.V. Parail, A. Parsloe, K. Paschalidis, M. Passeri, A. Patel, A. Pau, G. Pautasso, R. Pavlichenko, A. Pavone, E. Pawelec, C. Paz-Soldan, A. Peacock, M. Pearce, I.J. Pearson, E. Peluso, C. Penot, K. Pepperell, A. Perdas, T. Pereira, E. Perelli Cippo, C. Perez von Thun, D. Perry, P. Petersson, G. Petravich, N. Petrella, M. Peyman, L. Pigatto, M. Pillon, S. Pinches, G. Pintsuk, C. Piron, A. Pironti, F. Pisano, R. Pitts, U. Planck, N. Platt, V. Plyusnin, M. Podesta, G. Pokol, F.M. Poli, O.G. Pompilian, M. Poradzinski, M. Porkolab, C. Porosnicu, G. Poulipoulis, A.S. Poulsen, I. Predebon, A. Previti, D. Primetzhofer, G. Provatas, G. Pucella, P. Puglia, K. Purahoo, O. Putignano, T. Pütterich, A. Quercia, G. Radulescu, V. Radulovic, R. Ragona, M. Rainford, P. Raj, M. Rasinski, D. Rasmussen, J. Rasmussen, J.J. Rasmussen, A. Raso, G. Rattá, S. Ratynskaia, R. Rayaprolu, M. Rebai, A. Redl, D. Rees, D. Réfy, R. Reichle, H. Reimerdes, B.C.G. Reman, C. Reux, S. Reynolds, D. Rigamonti, E. Righi, F.G. Rimini, J. Risner, J.F. Rivero-Rodriguez, C.M. Roach, J. Roberts, R. Robins, S. Robinson, D. Robson, S. Rode, P. Rodrigues, P. Rodriguez-Fernandez, S. Romanelli, J. Romazanov, E. Rose, C. Rose-Innes, R. Rossi, S. Rowe, D. Rowlands, C. Rowley, M. Rubel, G. Rubinacci, G. Rubino, M. Rud, J. Ruiz Ruiz, F. Ryter, S. Saarelma, A. Sahlberg, M. Salewski, A. Salmi, R. Salmon, F. Salzedas, F. Sanchez, I. Sanders, D. Sandiford, F. Sanni, O. Sauter, P. Sauvan, G. Schettini, A. Shevelev, A.A. Schekochihin, K. Schmid, B.S. Schmidt, S. Schmuck, M. Schneider, P.A. Schneider, N. Schoonheere, R. Schramm, D. Scoon, S. Scully, M. Segato, J. Seidl, L. Senni, J. Seo, G. Sergienko, M. Sertoli, S.E. Sharapov, R. Sharma, A. Shaw, R. Shaw, H. Sheikh, U. Sheikh, N. Shi, P. Shigin, D. Shiraki, G. Sias, M. Siccinio, B. Sieglin, S.A. Silburn, A. Silva, C. Silva, J. Silva, D. Silvagni, D. Simfukwe, J. Simpson, P. Sirén, A. Sirinelli, H. Sjöstrand, N. Skinner, J. Slater, T. Smart, R.D. Smirnov, N. Smith, P. Smith, T. Smith, J. Snell, L. Snoj, E.R. Solano, V. Solokha, C. Sommariva, K. Soni, M. Sos, J. Sousa, C. Sozzi, T. Spelzini, F. Spineanu, L. Spolladore, D. Spong, C. Srinivasan, G. Staebler, A. Stagni, I. Stamatelatos, M.F. Stamp, Ž. Štancar, P.A. Staniec, G. Stankūnas, M. Stead, B. Stein-Lubrano, A. Stephen, J. Stephens, P. Stevenson, C. Steventon, M. Stojanov, D.A. St-Onge, P. Strand, S. Strikwerda, C.I. Stuart, S. Sturgeon, H.J. Sun, S. Surendran, W. Suttrop, J. Svensson, J. Svoboda, R. Sweeney, G. Szepesi, M. Szoke, T. Tadić, B. Tal, T. Tala, P. Tamain, K. Tanaka, W. Tang, G. Tardini, M. Tardocchi, D. Taylor, A.S. Teimane, G. Telesca, A. Teplukhina, A. Terra, D. Terranova, N. Terranova, D. Testa, B. Thomas, V.K. Thompson, A. Thorman, A.S. Thrysoe, W. Tierens, R.A. Tinguely, A. Tipton, H. Todd, M. Tomeš, A. Tookey, P. Tsavalas, D. Tskhakaya, L.-P. Turică, A. Turner, I. Turner, M. Turner, M.M. Turner, G. Tvalashvili, A. Tykhyy, S. Tyrrell, A. Uccello, V. Udintsev, A. Vadgama, D.F. Valcarcel, A. Valentini, M. Valisa, M. Vallar, M. Valovic, M. Van Berkel, K.L. van de Plassche, M. van Rossem, D. Van Eester, J. Varela, J. Varje, T. Vasilopoulou, G. Vayakis, M. Vecsei, J. Vega, M. Veis, P. Veis, S. Ventre, M. Veranda, G. Verdoolaege, C. Verona, G. Verona Rinati, E. Veshchev, N. Vianello, E. Viezzer, L. Vignitchouk, R. Vila, R. Villari, F. Villone, P. Vincenzi, A. Vitins, Z. Vizvary, M. Vlad, I. Voldiner, U. Von Toussaint, P. Vondráček, B. Wakeling, M. Walker, R. Walker, M. Walsh, R. Walton, E. Wang, F. Warren, R. Warren, J. Waterhouse, C. Watts, T. Webster, M. Weiland, H. Weisen, M. Weiszflog, N. Wendler, A. West, M. Wheatley, S. Whetham, A. Whitehead, D. Whittaker, A. Widdowson, S. Wiesen, M. Willensdorfer, J. Williams, I. Wilson, T. Wilson, M. Wischmeier, A. Withycombe, D. Witts, A. Wojcik-Gargula, E. Wolfrum, R. Wood, R. Woodley, R. Worrall, I. Wyss, T. Xu, D. Yadykin, Y. Yakovenko, Y. Yang, V. Yanovskiy, R. Yi, I. Young, R. Young, B. Zaar, R.J. Zabolockis, L. Zakharov, P. Zanca, A. Zarins, D. Zarzoso Fernandez, K.-D. Zastrow, Y. Zayachuk, M. Zerbini, W. Zhang, B. Zimmermann, M. Zlobinski, A. Zocco, V.K. Zotta, M. Zuin, W. Zwingmann, and I. Zychor
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magnetic fusion ,JET-ILW ,D–T ,tritium ,alpha particles ,fusion prediction ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
In 2021 JET exploited its unique capabilities to operate with T and D–T fuel with an ITER-like Be/W wall (JET-ILW). This second major JET D–T campaign (DTE2), after DTE1 in 1997, represented the culmination of a series of JET enhancements—new fusion diagnostics, new T injection capabilities, refurbishment of the T plant, increased auxiliary heating, in-vessel calibration of 14 MeV neutron yield monitors—as well as significant advances in plasma theory and modelling in the fusion community. DTE2 was complemented by a sequence of isotope physics campaigns encompassing operation in pure tritium at high T-NBI power. Carefully conducted for safe operation with tritium, the new T and D–T experiments used 1 kg of T (vs 100 g in DTE1), yielding the most fusion reactor relevant D–T plasmas to date and expanding our understanding of isotopes and D–T mixture physics. Furthermore, since the JET T and DTE2 campaigns occurred almost 25 years after the last major D–T tokamak experiment, it was also a strategic goal of the European fusion programme to refresh operational experience of a nuclear tokamak to prepare staff for ITER operation. The key physics results of the JET T and DTE2 experiments, carried out within the EUROfusion JET1 work package, are reported in this paper. Progress in the technological exploitation of JET D–T operations, development and validation of nuclear codes, neutronic tools and techniques for ITER operations carried out by EUROfusion (started within the Horizon 2020 Framework Programme and continuing under the Horizon Europe FP) are reported in (Litaudon et al Nucl. Fusion accepted), while JET experience on T and D–T operations is presented in (King et al Nucl. Fusion submitted).
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- 2024
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15. ICRH-related impurity source and control across experiments in H, D, T plasmas at JET-ILW
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A. Chomiczewska, W. Gromelski, I. Ivanova-Stanik, E. Kowalska-Strzęciwilk, N. Wendler, P. Jacquet, A. Meigs, J. Mailloux, S. Menmuir, J. Karhunen, E. Lerche, I. Monakhov, R. Otin, B. Thomas, P. Dumortier, D. Van Eester, M. Barruzo, V. Bobkov, S. Brezinsek, L. Colas, D. Douai, D. Milanesio, E. Pawelec, E. Delabie, B. Lomanowski, and JET Contributors
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fusion ,tokamak ,impurities ,ICRH ,H isotopes ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
The experimental and theoretical analysis were focused on experiments conducted to assess the effect of plasma isotopes, protium (H), deuterium (D), and tritium (T) on ion cyclotron resonance heating (ICRH) related plasma wall interactions. Comparison of L-mode discharges with N = 1 ^3 He and N = 1 H minority ICRH heating scenarios were done for different isotopes. For the selected pulses, the behaviour of high-Z, mid-Z and low-Z intrinsic impurity and radiated power behaviour was investigated based on data from VUV, visible spectroscopy, and bolometry diagnostic at Joint European Torus. It was found that for N = 1 ^3 He scenario during radiofrequency antennas operation, core W, Ni content, Be source and the radiated power are higher for π /2 in comparison to dipole antenna phasing. Lowest core Ni, W content and radiated power is clearly observed for H plasmas in comparison to D and T, where for this ICRH scenario behaviour was similar. However, lower Be photon flux is observed for T in comparison to D plasmas. Be sputtering by He particles is responsible for such an effect. Additionally, several computer simulations were conducted using the COREDIV code. The difference in the electron temperature was due to the difference in the isotope masses. Increased temperature in the central plasma in the case of T plasmas leads to higher radiation in the central plasma in comparison to H plasmas. As a result, the power across separatrix is lower and the temperature on the divertor plate decreases with the increase of the isotope mass. At these temperatures on the divertor plate, W is not sputtered by the main plasma ions H, D and T and by He. For the N = 1 H ICRH scenario clear difference between D and T plasma was observed with higher metallic impurity content for T plasma in comparison to D. Impurity content in the plasmas is found to be sensitive to the power balance between the antenna straps. Its minimum is observed for the maximum of P _cen / P _tot .
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- 2024
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16. Relative quantification of pork and beef in meat products using global and species-specific peptide markers for the authentication of meat composition
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Nalazek-Rudnicka, Katarzyna, Kłosowska-Chomiczewska, Ilona E., Brockmeyer, Jens, Wasik, Andrzej, and Macierzanka, Adam
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- 2022
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17. Effects of different types of primary microplastics on early life stages of rainbow trout (Oncorhynchus mykiss)
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Jakubowska, Magdalena, Białowąs, Marcin, Stankevičiūtė, Milda, Chomiczewska, Agnieszka, Jonko-Sobuś, Karolina, Pažusienė, Janina, Hallmann, Anna, Bučaitė, Agnė, and Urban-Malinga, Barbara
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- 2022
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18. INFOGEST inter-laboratory recommendations for assaying gastric and pancreatic lipases activities prior to in vitro digestion studies
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Grundy, Myriam M.L., Abrahamse, Evan, Almgren, Annette, Alminger, Marie, Andres, Ana, Ariëns, Renata M.C., Bastiaan-Net, Shanna, Bourlieu-Lacanal, Claire, Brodkorb, André, Bronze, Maria R., Comi, Irene, Couëdelo, Leslie, Dupont, Didier, Durand, Annie, El, Sedef N., Grauwet, Tara, Heerup, Christine, Heredia, Ana, Infantes Garcia, Marcos R., Jungnickel, Christian, Kłosowska-Chomiczewska, Ilona E., Létisse, Marion, Macierzanka, Adam, Mackie, Alan R., McClements, David J., Menard, Olivia, Meynier, Anne, Michalski, Marie-Caroline, Mulet-Cabero, Ana-Isabel, Mullertz, Anette, Payeras Perelló, Francina M., Peinado, Irene, Robert, Mélina, Secouard, Sébastien, Serra, Ana T., Silva, Sandra D., Thomassen, Gabriel, Tullberg, Cecilia, Undeland, Ingrid, Vaysse, Carole, Vegarud, Gerd E., Verkempinck, Sarah H.E., Viau, Michelle, Zahir, Mostafa, Zhang, Ruojie, and Carrière, Frédéric
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- 2021
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19. The JET hybrid scenario in Deuterium, Tritium and Deuterium-Tritium
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J. Hobirk, C.D. Challis, A. Kappatou, E. Lerche, D. Keeling, D. King, S. Aleiferis, E. Alessi, C. Angioni, F. Auriemma, M. Baruzzo, É. Belonohy, J. Bernardo, A. Boboc, I.S. Carvalho, P. Carvalho, F.J. Casson, A. Chomiczewska, J. Citrin, I.H. Coffey, N.J. Conway, D. Douai, E. Delabie, B. Eriksson, J. Eriksson, O. Ficker, A.R. Field, M. Fontana, J.M. Fontdecaba, L. Frassinetti, D. Frigione, D. Gallart, J. Garcia, M. Gelfusa, Z. Ghani, L. Giacomelli, E. Giovannozzi, C. Giroud, M. Goniche, W. Gromelski, S. Hacquin, C. Ham, N.C. Hawkes, R.B. Henriques, J.C. Hillesheim, A. Ho, L. Horvath, I. Ivanova-Stanik, P. Jacquet, F. Jaulmes, E. Joffrin, H.T. Kim, V. Kiptily, K. Kirov, D. Kos, E. Kowalska-Strzeciwilk, H. Kumpulainen, K. Lawson, M. Lennholm, X. Litaudon, E. Litherland-Smith, P.J. Lomas, E. de la Luna, C.F. Maggi, J. Mailloux, M.J. Mantsinen, M. Maslov, G. Matthews, K.G. McClements, A.G. Meigs, S. Menmuir, A. Milocco, I.G. Miron, S. Moradi, R.B. Morales, S. Nowak, F. Orsitto, A. Patel, L. Piron, C. Prince, G. Pucella, E. Peluso, C. Perez von Thun, E. Rachlew, C. Reux, F. Rimini, S. Saarelma, P. A Schneider, S. Scully, M. Sertoli, S. Sharapov, A. Shaw, S. Silburn, A. Sips, P. Siren, C. Sozzi, E.R. Solano, Z. Stancar, G. Stankunas, C. Stuart, H.J. Sun, G. Szepesi, D. Valcarcel, M. Valisa, G. Verdoolaege, B. Viola, N. Wendler, M. Zerbini, and JET Contributors
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magnetic fusion ,hybrid scenario ,Tritium ,D-T ,isotope effects ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
The JET hybrid scenario has been developed from low plasma current carbon wall discharges to the record-breaking Deuterium-Tritium plasmas obtained in 2021 with the ITER-like Be/W wall. The development started in pure Deuterium with refinement of the plasma current, and toroidal magnetic field choices and succeeded in solving the heat load challenges arising from 37 MW of injected power in the ITER like wall environment, keeping the radiation in the edge and core controlled, avoiding MHD instabilities and reaching high neutron rates. The Deuterium hybrid plasmas have been re-run in Tritium and methods have been found to keep the radiation controlled but not at high fusion performance probably due to time constraints. For the first time this scenario has been run in Deuterium-Tritium (50:50). These plasmas were re-optimised to have a radiation-stable H-mode entry phase, good impurity control through edge T _i gradient screening and optimised performance with fusion power exceeding 10 MW for longer than three alpha particle slow down times, 8.3 MW averaged over 5 s and fusion energy of 45.8 MJ.
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- 2023
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20. JET D-T scenario with optimized non-thermal fusion
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M. Maslov, E. Lerche, F. Auriemma, E. Belli, C. Bourdelle, C.D. Challis, A. Chomiczewska, A. Dal Molin, J. Eriksson, J. Garcia, J. Hobirk, I. Ivanova-Stanik, Ph. Jacquet, A. Kappatou, Y. Kazakov, D.L. Keeling, D.B. King, V. Kiptily, K. Kirov, D. Kos, R. Lorenzini, E. De La Luna, C.F. Maggi, J. Mailloux, P. Mantica, M. Marin, G. Matthews, I. Monakhov, M. Nocente, G. Pucella, D. Rigamonti, F. Rimini, S. Saarelma, M. Salewski, E.R. Solano, Ž. Štancar, G. Stankunas, H. Sun, M. Tardocchi, D. Van Eester, and JET Contributors
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tokamak ,nuclear fusion ,tritium ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
In JET deuterium-tritium (D-T) plasmas, the fusion power is produced through thermonuclear reactions and reactions between thermal ions and fast particles generated by neutral beam injection (NBI) heating or accelerated by electromagnetic wave heating in the ion cyclotron range of frequencies (ICRFs). To complement the experiments with 50/50 D/T mixtures maximizing thermonuclear reactivity, a scenario with dominant non-thermal reactivity has been developed and successfully demonstrated during the second JET deuterium-tritium campaign DTE2, as it was predicted to generate the highest fusion power in JET with a Be/W wall. It was performed in a 15/85 D/T mixture with pure D-NBI heating combined with ICRF heating at the fundamental deuterium resonance. In steady plasma conditions, a record 59 MJ of fusion energy has been achieved in a single pulse, of which 50.5 MJ were produced in a 5 s time window ( P _fus = 10.1 MW) with average Q = 0.33, confirming predictive modelling in preparation of the experiment. The highest fusion power in these experiments, P _fus = 12.5 MW with average Q = 0.38, was achieved over a shorter 2 s time window, with the period of sustainment limited by high-Z impurity accumulation. This scenario provides unique data for the validation of physics-based models used to predict D-T fusion power.
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- 2023
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21. Isotope mass scaling and transport comparison between JET Deuterium and Tritium L-mode plasmas
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T. Tala, A.E. Järvinen, C.F. Maggi, P. Mantica, A. Mariani, A. Salmi, I.S. Carvalho, A. Chomiczewska, E. Delabie, F. Devasagayam, J. Ferreira, W. Gromelski, N. Hawkes, L. Horvath, J. Karhunen, D. King, A. Kirjasuo, E. Kowalska-Strzeciwilk, S. Leerink, M. Lennholm, B. Lomanowski, M. Maslov, S. Menmuir, R.B. Morales, R. Sharma, H. Sun, K. Tanaka, and JET Contributors
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isotope mass scaling ,Deuterium and Tritium ,confinement and transport ,JET ,dimensionless scaling ,heat and particle transport ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
The dimensionless isotope mass scaling experiment between pure Deuterium and pure Tritium plasmas with matched $\rho^*$ , $\nu^*$ , β _n , q and $T_e/T_i$ has been achieved in JET L-mode with dominant electron heating (NBI+ohmic) conditions. 28% higher scaled energy confinement time $B_t\tau_{E,\mathrm{th}}/A$ is found in favour of the Tritium plasma. This can be cast in the form of the dimensionless energy confinement scaling law as $\Omega_i \tau_{E,\mathrm{th}} \sim A^{0.48 \pm 0.16}$ . This significant isotope mass scaling is consequently seen in the scaled one-fluid heat diffusion coefficient $A \chi_{\mathrm{eff}}/B_t$ which is around 50% lower in the Tritium plasma throughout the whole plasma radius. The isotope mass dependence in the particle transport channel is negligible, supported also by the perturbative particle transport analysis with gas puff modulation. The comparison of the edge particle fuelling or ionisation profiles from the EDGE2D-EIRENE simulations show that the absolute density differences that are necessary for the dimensionless match in the confined plasma dominate over any isotope mass dependencies of particle fuelling and ionization profiles at the plasma edge. Local GENE simulation results indicate a mild anti-gyroBohm effect at $\rho_\mathrm{tor}$ = 0.6 and thereby a small isotope mass dependence in favour of Tritium on heat transport and a negligible effect on particle transport. A significant fraction of the isotope scaling and reduced heat transport observed in the Tritium plasma is not captured in the GENE and ASTRA-TGLF-SAT2 simulations by simply changing the isotope mass for the same input profiles.
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- 2023
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22. L-H transition studies in tritium and deuterium–tritium campaigns at JET with Be wall and W divertor
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E.R. Solano, G. Birkenmeier, C. Silva, E. Delabie, J.C. Hillesheim, A. Baciero, I. Balboa, M. Baruzzo, A. Boboc, M. Brix, J. Bernardo, C. Bourdelle, I.S. Carvalho, P. Carvalho, C.D. Challis, M. Chernyshova, A. Chomiczewska, R. Coelho, I. Coffey, T. Craciunescu, E. de la Cal, E. de la Luna, R. Dumont, P. Dumortier, M. Fontana, J.M. Fontdecaba, L. Frassinetti, D. Gallart, J. Garcia, C. Giroud, W. Gromelski, R.B. Henriques, J. Hall, A. Ho, L.D. Horton, L. Horvath, P. Jacquet, I. Jepu, E. Joffrin, A. Kappatou, D.L. Keeling, D.B. King, V.G. Kiptily, K.K. Kirov, D. Kos, E. Kowalska-Strzęciwilk, M. Lennholm, E. Lerche, E. Litherland-Smith, A. Loarte, B. Lomanowski, P.J. Lomas, C.F. Maggi, J. Mailloux, M.J. Mantsinen, M. Maslov, A.G. Meigs, I. Monakhov, R.B. Morales, A.H. Nielsen, D. Nina, C. Noble, E. Pawelec, M. Poradzinski, G. Pucella, P. Puglia, D. Réfy, J. Juul Rasmussen, E. Righi, F.G. Rimini, T. Robinson, M. Sertoli, S.A. Silburn, G. Sips, P. Sirén, Ž. Štancar, H.J. Sun, G. Szepesi, D. Taylor, E. Tholerus, B. Thomas, G. Verdoolaege, P. Vincenzi, B. Viola, N. Vianello, T. Wilson, and JET Contributors
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L-H transition ,power threshold ,tokamaks ,Tritium ,DT ,JET-ILW ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
The recent deuterium–tritium campaign in JET-ILW (DTE2) has provided a unique opportunity to study the isotope dependence of the L-H power threshold in an ITER-like wall environment (Be wall and W divertor). Here we present results from dedicated L-H transition experiments at JET-ILW, documenting the power threshold in tritium and deuterium–tritium plasmas, comparing them with the matching deuterium and hydrogen datasets. From earlier experiments in JET-ILW it is known that as plasma isotopic composition changes from deuterium, through varying deuterium/hydrogen concentrations, to pure hydrogen, the value of the line averaged density at which the threshold is minimum, ${\bar n_{{\text{e}},{\text{min}}}}$ , increases, leading us to expect that ${\bar n_{{\text{e}},{\text{min}}}}$ (T) < ${\bar n_{{\text{e}},{\text{min}}}}$ (DT) < ${\bar n_{{\text{e}},{\text{min}}}}$ (D) < ${\bar n_{{\text{e}},{\text{min}}}}$ (H). The new power threshold data confirms these expectations in most cases, with the corresponding ordering of the minimum power thresholds. We present a comparison of this data to power threshold scalings, used for extrapolation to future devices such as ITER and DEMO.
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- 2023
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23. Effect of the isotope mass on pedestal structure, transport and stability in D, D/T and T plasmas at similar β N and gas rate in JET-ILW type I ELMy H-modes
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L. Frassinetti, C. Perez von Thun, B. Chapman-Oplopoiou, H. Nyström, M. Poradzinski, J.C. Hillesheim, L. Horvath, C.F. Maggi, S. Saarelma, A. Stagni, G. Szepesi, A. Bleasdale, A. Chomiczewska, R.B. Morales, M. Brix, P. Carvalho, D. Dunai, A.R. Field, J.M. Fontdecaba, H.J. Sun, D.B. King, D. Kos, E. Kowalska, B. Labit, M. Lennholm, S. Menmuir, E. Rachlew, D.I. Refy, P.A. Schneider, E.R. Solano, N. Vianello, M. Vécsei, and JET Contributors
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pedestal ,stability ,tritium ,deuterium/tritium ,JET-ILW ,isotope effect ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
The work describes the pedestal structure, transport and stability in an effective mass ( A _eff ) scan from pure deuterium to pure tritium plasmas using a type I ELMy H-mode dataset in which key parameters that affect the pedestal behaviour (normalized pressure, ratio of the separatrix density to the pedestal density, pedestal ion Larmor radius, pedestal collisionality and rotation) are kept as constant as possible. Experimental results show a significant increase of the density at the pedestal top with increasing A _eff , a modest reduction in the temperature and an increase in the pressure. The variations in the pedestal heights are mainly due to a change in the pedestal gradients while only small differences are observed in the pedestal width. A clear increase in the pedestal density and pressure gradients are observed from deuterium to tritium. The experimental results suggest a reduction of the pedestal inter-edge localized mode (inter-ELM) transport from deuterium to tritium. The reduction is likely in the pedestal inter-ELM particle transport, as suggested by the clear increase of the pedestal density gradients. The experimental results suggest also a possible reduction of the pedestal inter-ELM heat transport, however, the large experimental uncertainties do not allow conclusive claims on the heat diffusivity. The clear experimental reduction of η _e (the ratio between density and temperature gradient lengths) in the middle/top of the pedestal with increasing A _eff suggests that there may be a link between increasing A _eff and the reduction of electron scale turbulent transport. From the modelling point of view, an initial characterization of the behaviour of pedestal microinstabilities shows that the tritium plasma is characterized by growth rates lower than the deuterium plasmas. The pedestal stability of peeling-ballooning modes is assessed with both ideal and resistive magnetohydrodynamics (MHD). No significant effect of the isotope mass on the pedestal stability is observed using ideal MHD. Instead, resistive MHD shows a clear increase of the stability with increasing isotope mass. The resistive MHD results are in reasonable agreement with the experimental results of the normalized pedestal pressure gradient. The experimental and modelling results suggest that the main candidates to explain the change in the pedestal are a reduction in the inter-ELM transport and an improvement of the pedestal stability from deuterium to tritium.
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- 2023
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24. Isotope physics of heat and particle transport with tritium in JET-ILW type-I ELMy H-mode plasmas
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P.A. Schneider, C. Angioni, F. Auriemma, N. Bonanomi, T. Görler, R. Henriques, L. Horvath, D. King, R. Lorenzini, H. Nyström, M. Maslov, J. Ruiz, G. Szepesi, C.D. Challis, A. Chomiczewska, E. Delabie, J.M. Fontdecaba, L. Frassinetti, J. Garcia, C. Giroud, J. Hillesheim, J. Hobirk, A. Kappatou, D.L. Keeling, E. Kowalska-Strzeciwilk, M. Lennholm, B. Lomanowski, T. Luda di Cortemiglia, C.F. Maggi, S. Menmuir, G. Pucella, A. Thorman, and JET Contributors
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H-mode ,tritium ,heat transport ,particle transport ,stability ,isotopes ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
As part the DTE2 campaign in the JET tokamak, we conducted a parameter scan in T and D-T complementing existing pulses in H and D. For the different main ion masses, type-I ELMy H-modes at fixed plasma current and magnetic field can have the pedestal pressure varying by a factor of 4 and the total pressure changing from $\beta_{\mathrm{N}} = 1.0$ to 3.0. We investigated the pedestal and core isotope mass dependencies using this extensive data set. The pedestal shows a strong mass dependence on the density, which influences the core due to the strong coupling between both plasma regions. To better understand the causes for the observed isotope mass dependence in the pedestal, we analysed the interplay between heat and particle transport and the edge localised mode (ELM) stability. For this purpose, we developed a dynamic ELM cycle model with basic transport assumptions and a realistic neutral penetration. The temporal evolution and resulting ELM frequency introduce an additional experimental constraint that conventional quasi-stationary transport analysis cannot provide. Our model shows that a mass dependence in the ELM stability or in the transport alone cannot explain the observations. One requires a mass dependence in the ELM stability as well as one in the particle sources. The core confinement time increases with pedestal pressure for all isotope masses due to profile stiffness and electromagnetic turbulence stabilisation. Interestingly, T and D-T plasmas show an improved core confinement time compared to H and D plasmas even for matched pedestal pressures. For T, this improvement is largely due to the unique pedestal composition of higher densities and lower temperatures than H and D. With a reduced gyroBohm factor at lower temperatures, more turbulent drive in the form of steeper gradients is required to transport the same amount of heat. This picture is supported by quasilinear flux-driven modelling using TGLF -SAT2 within Astra . With the experimental boundary condition TGLF -SAT2 predicts the core profiles well for gyroBohm heat fluxes ${\gt}15$ , however, overestimates the heat and particle transport closer to the turbulent threshold.
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- 2023
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25. Progress with applications of three-ion ICRF scenarios for fusion research: A review
- Author
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Wukitch, SJ, Bertelli, N, Bonoli, P, Kazakov, Y, Ongena, J, Nocente, M, Bobkov, V, Garcia, J, Kiptily, V, Schneider, M, Wukitch, S, Wright, J, Dreval, M, Kirov, K, Mazzi, S, Ochoukov, R, Sharapov, S, Štancar, Weisen, H, Baranov, Y, Baruzzo, M, Bierwage, A, Bilato, R, Chomiczewska, A, Coelho, R, Craciunescu, T, Crombé, K, Delabie, E, Luna, E, Dumont, R, Dumortier, P, Durodié, F, Eriksson, J, Fitzgerald, M, Galdon-Quiroga, J, Gallart, D, Garcia-Munoz, M, Giacomelli, L, Giroud, C, Gonzalez-Martin, J, Hakola, A, Henriques, R, Jacquet, P, Jepu, I, Johnson, T, Kappatou, A, Keeling, D, King, D, Klepper, C, Lauber, P, Lennholm, M, Lerche, E, Lomanowski, B, Lowry, C, Mantsinen, M, Maslov, M, Menmuir, S, Monakhov, I, Nabais, F, Nave, M, Noble, C, Panontin, E, Pinches, S, Polevoi, A, Rigamonti, D, Sahlberg, A, Salewski, M, Schneider, P, Sheikh, H, Shinohara, K, Siren, P, Sumida, S, Thorman, A, Tinguely, R, Valcarcel, D, Van Eester, D, Schoor, M, Varje, J, Weiland, M, Wendler, N, Kazakov Y. O., Ongena J., Nocente M., Bobkov V., Garcia J., Kiptily V. G., Schneider M., Wukitch S., Wright J. C., Dreval M., Kirov K. K., Mazzi S., Ochoukov R., Sharapov S. E., Weisen H., Baranov Y., Baruzzo M., Bierwage A., Bilato R., Chomiczewska A., Coelho R., Craciunescu T., Crombé K., Delabie E., Luna E. D. L., Dumont R., Dumortier P., Durodié F., Eriksson J., Fitzgerald M., Galdon-Quiroga J., Gallart D., Garcia-Munoz M., Giacomelli L., Giroud C., Gonzalez-Martin J., Hakola A., Henriques R., Jacquet P., Jepu I., Johnson T., Kappatou A., Keeling D., King D., Klepper C., Lauber P., Lennholm M., Lerche E., Lomanowski B., Lowry C., Mantsinen M. J., Maslov M., Menmuir S., Monakhov I., Nabais F., Nave M. F. F., Noble C., Panontin E., Pinches S. D., Polevoi A. R., Rigamonti D., Sahlberg A., Salewski M., Schneider P. A., Sheikh H., Shinohara K., Siren P., Sumida S., Thorman A., Tinguely R. A., Valcarcel D., Van Eester D., Schoor M. V., Varje J., Weiland M., Wendler N., Wukitch, SJ, Bertelli, N, Bonoli, P, Kazakov, Y, Ongena, J, Nocente, M, Bobkov, V, Garcia, J, Kiptily, V, Schneider, M, Wukitch, S, Wright, J, Dreval, M, Kirov, K, Mazzi, S, Ochoukov, R, Sharapov, S, Štancar, Weisen, H, Baranov, Y, Baruzzo, M, Bierwage, A, Bilato, R, Chomiczewska, A, Coelho, R, Craciunescu, T, Crombé, K, Delabie, E, Luna, E, Dumont, R, Dumortier, P, Durodié, F, Eriksson, J, Fitzgerald, M, Galdon-Quiroga, J, Gallart, D, Garcia-Munoz, M, Giacomelli, L, Giroud, C, Gonzalez-Martin, J, Hakola, A, Henriques, R, Jacquet, P, Jepu, I, Johnson, T, Kappatou, A, Keeling, D, King, D, Klepper, C, Lauber, P, Lennholm, M, Lerche, E, Lomanowski, B, Lowry, C, Mantsinen, M, Maslov, M, Menmuir, S, Monakhov, I, Nabais, F, Nave, M, Noble, C, Panontin, E, Pinches, S, Polevoi, A, Rigamonti, D, Sahlberg, A, Salewski, M, Schneider, P, Sheikh, H, Shinohara, K, Siren, P, Sumida, S, Thorman, A, Tinguely, R, Valcarcel, D, Van Eester, D, Schoor, M, Varje, J, Weiland, M, Wendler, N, Kazakov Y. O., Ongena J., Nocente M., Bobkov V., Garcia J., Kiptily V. G., Schneider M., Wukitch S., Wright J. C., Dreval M., Kirov K. K., Mazzi S., Ochoukov R., Sharapov S. E., Weisen H., Baranov Y., Baruzzo M., Bierwage A., Bilato R., Chomiczewska A., Coelho R., Craciunescu T., Crombé K., Delabie E., Luna E. D. L., Dumont R., Dumortier P., Durodié F., Eriksson J., Fitzgerald M., Galdon-Quiroga J., Gallart D., Garcia-Munoz M., Giacomelli L., Giroud C., Gonzalez-Martin J., Hakola A., Henriques R., Jacquet P., Jepu I., Johnson T., Kappatou A., Keeling D., King D., Klepper C., Lauber P., Lennholm M., Lerche E., Lomanowski B., Lowry C., Mantsinen M. J., Maslov M., Menmuir S., Monakhov I., Nabais F., Nave M. F. F., Noble C., Panontin E., Pinches S. D., Polevoi A. R., Rigamonti D., Sahlberg A., Salewski M., Schneider P. A., Sheikh H., Shinohara K., Siren P., Sumida S., Thorman A., Tinguely R. A., Valcarcel D., Van Eester D., Schoor M. V., Varje J., Weiland M., and Wendler N.
- Abstract
The viability of magnetic confinement fusion as an energy source depends on achieving the high ion temperatures required for D-T fusion. Among the available techniques, plasma heating with waves in the ion cyclotron range of frequencies (ICRF) is a prominent method for bulk ion heating in fusion plasmas. Furthermore, a detailed understanding of the non-linear physics of alpha heating and the complex impact of MeV-range fast ions on plasma dynamics becomes progressively more important. This paper provides a comprehensive overview of recent developments with the three-ion ICRF scenarios on Alcator C-Mod, ASDEX Upgrade and JET tokamaks. The results demonstrate the flexibility of these novel scenarios for heating bulk ions in D-T ≈ 50%-50% plasmas and efficient generation of MeV-range fast ions in multi-ion species plasmas. Several key results relevant for ITER and future fusion reactors are highlighted.
- Published
- 2023
26. MRM–MS of marker peptides and their abundance as a tool for authentication of meat species and meat cuts in single-cut meat products
- Author
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Nalazek-Rudnicka, Katarzyna, Kłosowska-Chomiczewska, Ilona, Wasik, Andrzej, and Macierzanka, Adam
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- 2019
- Full Text
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27. INFOGEST inter-laboratory recommendations for assaying gastric and pancreatic lipases activities prior to in vitro digestion studies
- Author
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Myriam M.L. Grundy, Evan Abrahamse, Annette Almgren, Marie Alminger, Ana Andres, Renata M.C. Ariëns, Shanna Bastiaan-Net, Claire Bourlieu-Lacanal, André Brodkorb, Maria R. Bronze, Irene Comi, Leslie Couëdelo, Didier Dupont, Annie Durand, Sedef N. El, Tara Grauwet, Christine Heerup, Ana Heredia, Marcos R. Infantes Garcia, Christian Jungnickel, Ilona E. Kłosowska-Chomiczewska, Marion Létisse, Adam Macierzanka, Alan R. Mackie, David J. McClements, Olivia Menard, Anne Meynier, Marie-Caroline Michalski, Ana-Isabel Mulet-Cabero, Anette Mullertz, Francina M. Payeras Perelló, Irene Peinado, Mélina Robert, Sébastien Secouard, Ana T. Serra, Sandra D. Silva, Gabriel Thomassen, Cecilia Tullberg, Ingrid Undeland, Carole Vaysse, Gerd E. Vegarud, Sarah H.E. Verkempinck, Michelle Viau, Mostafa Zahir, Ruojie Zhang, and Frédéric Carrière
- Subjects
Lipases ,Lipolysis ,Enzyme activity ,Titration method ,Inhibitor ,INFOGEST ,Nutrition. Foods and food supply ,TX341-641 - Abstract
In vitro digestion studies often use animal digestive enzyme extracts as substitutes of human gastric and pancreatic secretions. Pancreatin from porcine origin is thus commonly used to provide relevant pancreatic enzymes such as proteases, amylase and lipase. Rabbit gastric extracts (RGE) have been recently introduced to provide gastric lipase in addition to pepsin. Before preparing simulated gastric and pancreatic extracts with targeted enzyme activities as described in in vitro digestion protocols, it is important to determine the activities of enzyme preparations using validated methods. The purpose of this inter-laboratory study within the INFOGEST network was to test the repeatability and reproducibility of lipase assays using the pH-stat technique for measuring the activities of gastric and pancreatic lipases from various sources. Twenty-one laboratories having different pH-stat devices received the same protocol with identical batches of RGE and two pancreatin sources. Lipase assays were performed using tributyrin as a substrate and three different amounts (50, 100 and 200 µg) of each enzyme preparation. The repeatability results within individual laboratories were satisfactory with coefficients of variation (CVs) ranging from 4 to 8% regardless of the enzyme amount tested. However, the inter-laboratory variability was high (CV > 15%) compared to existing standards for bioanalytical assays. We identified and weighted the contributions to inter-laboratory variability of several parameters associated with the various pH-stat equipment used in this study (e.g. reaction vessel volume and shape, stirring mode and rate, burette volume for the automated delivery of sodium hydroxide). Based on this, we established recommendations for improving the reproducibility of lipase assays using the pH-stat technique. Defining accurate and complete recommendations on how to correctly quantify activity levels of enzyme preparations is a gateway to promising comparison of in vitro data obtained from different laboratories following the same in vitro digestion protocol.
- Published
- 2021
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- View/download PDF
28. Study of impurity behavior in JET-ILW hybrid scenario with deuterium, tritium, and deuterium–tritium plasmas.
- Author
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Wendler, N., Chomiczewska, A., Gromelski, W., Kowalska-Strzęciwilk, E., Ivanova-Stanik, I., Challis, C. D., Hobirk, J., Kappatou, A., Lerche, E., Carvalho, P., Coffey, I., Pucella, G., and Giovannozzi, E.
- Subjects
- *
TRITIUM , *DEUTERIUM , *CONTROLLED fusion , *DEUTERIUM plasma , *PLASMA boundary layers , *PLASMA currents , *PLASMA confinement - Abstract
Experimental campaigns at the Joint European Torus with an ITER-like Be/W wall with pure deuterium (D), tritium (T), and deuterium–tritium (DT) were a unique opportunity to explore various aspects related to the ITER operation. One of the most important challenges in recent years was the development of the hybrid scenario for D-T, based on reference deuterium and tritium plasmas. This kind of scenario, one of the foreseen for ITER, is characterized by a low current plasma and a high normalized beta βN factor compared to the parallel optimized baseline scenario [Hobirk et al., Plasma Phys. Controlled Fusion 54, 095001 (2012)]. As the experiments have shown, controlling the plasma edge in the different phases of the hybrid scenario becomes more difficult with higher isotope mass, and therefore, are also in risk of impurity accumulation [Hobirk et al., Nucl. Fusion 63, 112001 (2023)]. For this reason, investigation of the impurity behavior, as well as their control, constituted the crucial issue. The present contribution aims to compare mid-Z and high-Z impurities behavior within H-mode hybrid discharges in D and T plasmas, as well as D and DT plasmas. Detailed analysis shows that in the H-mode regime in the hybrid scenario, higher impurity radiation is observed for DT in comparison to D plasmas, as well as for T compared to D plasmas. Additionally, it was noticed that the most significant contribution to the plasma radiated power comes from W and to a lesser extent from Ni (∼10%). Moreover, it was found that an earlier transition from small edge localized modes (ELMs) to ELM-free phase can result in the earlier increase in impurities. [ABSTRACT FROM AUTHOR]
- Published
- 2024
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- View/download PDF
29. Investigation of triangularity impact on impurity content in JET-ILW H, D, T, and DT plasmas.
- Author
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Gromelski, Wojciech, Angioni, Clemente, Chomiczewska, Agata, Fajardo, Daniel, Ivanova-Stanik, Irena, King, Damian, Kowalska-Strzęciwilk, Ewa, Maslov, Mikhail, Pawelec, Ewa, and Schneider, Philip
- Subjects
PLASMA density ,PLASMA currents ,RADIATION sources ,PLASMA sources ,ELECTRON density ,TOROIDAL plasma - Abstract
The work presents the recent outcome of the research on Joint European Torus with ITER-like wall (JET-ILW) concerning Be, mid-Z (Ni, Cu, Fe), and high-Z (W) impurities for a selection of Neutral Beam Injection-heated, ELMy H-mode pulses using visible and vacuum–ultraviolet spectroscopy together with bolometry diagnostic. The investigation is focused on the evaluation of the plasma triangularity (δ) impact on the impurity radiation in hydrogen (H), deuterium (D), tritium (T), and deuterium–tritium (DT) plasmas for pulses described in [P. A. Schneider, Nucl. Fusion 63, 112010 (2023)]. The variations of δ were in the range of 0.21–0.31 for different time windows with low magnetic toroidal field ( B t = 1.7 T) and plasma current ( I p = 1.4 MA) in the corner–corner configuration, that is with both the inner and outer strike points on the horizontal W-coated divertor target plates. The results confirm the rise in Be flux with plasma isotope and lower δ leading to higher plasma density close to the plasma wall. The dominant role of W as a source of plasma radiation has also been confirmed. For mid-Z impurities and W, the variations in their densities due to δ change are negligible and the rise in their densities is observed with higher isotope mass, although this effect is often masked by the dominant role of ELM frequency on the impurity level. The impurity radiation losses based on bolometry together with the W intensity are ruled by the changes in the electron density and are well correlated when the T
e profiles are conserved. [ABSTRACT FROM AUTHOR]- Published
- 2024
- Full Text
- View/download PDF
30. Rhamnolipid CMC prediction
- Author
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Kłosowska-Chomiczewska, I.E., Mędrzycka, K., Hallmann, E., Karpenko, E., Pokynbroda, T., Macierzanka, A., and Jungnickel, C.
- Published
- 2017
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31. La parole de l’enfant dans l’adoption
- Author
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Pfeifer-Chomiczewska, Katarzyna, primary
- Published
- 2019
- Full Text
- View/download PDF
32. Enhanced performance in fusion plasmas through turbulence suppression by megaelectronvolt ions
- Author
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Mazzi, S., Garcia, J., Zarzoso, D., Kazakov, Y., Ongena, J., Dreval, M., Nocente, M., Stancar, Z., Szepesi, G., Eriksson, J., Sahlberg, A., Benkadda, S., Abid, N., Abraham, K., Abreu, P., Adabonyan, O., Adrich, P., Afanasev, V., Afzal, M., Ahlgren, T., Aho-Mantila, L., Aiba, N., Airila, M., Akhtar, M., Albanese, R., Alderson-Martin, M., Alegre, D., Aleiferis, S., Aleksa, A., Alekseev, A., Alessi, E., Aleynikov, P., Algualcil, J., Ali, M., Allinson, M., Alper, B., Alves, E., Ambrosino, G., Ambrosino, R., Amosov, V., Andersson Sunden, E., Andrew, P., Angelini, B., Angioni, C., Antoniou, I., Appel, L., Appelbee, C., Aria, S., Ariola, M., Artaserse, G., Arter, W., Artigues, V., Asakura, N., Ash, A., Ashikawa, N., Aslanyan, V., Astrain, M., Asztalos, O., Auld, D., Auriemma, F., Austin, Y., Avotina, L., Aymerich, E., Baciero, A., Bairaktaris, F., Balbin, J., Balbinot, L., Balboa, I., Balden, M., Balshaw, C., Balshaw, N., Bandaru, V., Banks, J., Baranov, Y., Barcellona, C., Barnard, A., Barnard, M., Barnsley, R., Barth, A., Baruzzo, M., Barwell, S., Bassan, M., Batista, A., Batistoni, P., Baumane, L., Bauvir, B., Baylor, L., Beaumont, P., Beckett, D., Begolli, A., Beidler, M., Bekris, N., Beldishevski, M., Belli, E., Belli, F., Belonohy, E., Ben Yaala, M., Benayas, J., Bentley, J., Bergsaker, H., Bernardo, J., Bernert, M., Berry, M., Bertalot, L., Betar, H., Beurskens, M., Bickerton, S., Bieg, B., Bielecki, J., Bierwage, A., Biewer, T., Bilato, R., Bílkova, P., Birkenmeier, G., Bishop, H., Bizarro, J., Blackburn, J., Blanchard, P., Blatchford, P., Bobkov, V., Boboc, A., Bohm, P., Bohm, T., Bolshakova, I., Bolzonella, T., Bonanomi, N., Bonfiglio, D., Bonnin, X., Bonofiglo, P., Boocock, S., Booth, A., Booth, J., Borba, D., Borodin, D., Borodkina, I., Boulbe, C., Bourdelle, C., Bowden, M., Boyd, K., Bozicevic Mihalic, I., Bradnam, S., Braic, V., Brandt, L., Bravanec, R., Breizman, B., Brett, A., Brezinsek, S., Brix, M., Bromley, K., Brown, B., Brunetti, D., Buckingham, R., Buckley, M., Budny, R., Buermans, J., Bufferand, H., Buratti, P., Burgess, A., Buscarino, A., Busse, A., Butcher, D., Cal, E., Calabro, G., Calacci, L., Calado, R., Camenen, Y., Canal, G., Cannas, B., Cappelli, M., Carcangiu, S., Card, P., Cardinali, A., Carman, P., Carnevale, D., Carr, M., Carralero, D., Carraro, L., Carvalho, I., Carvalho, P., Casiraghi, I., Casson, F., Castaldo, C., Catalan, J., Catarino, N., Causa, F., Cavedon, M., Cecconello, M., Challis, C., Chamberlain, B., Chang, C., Chankin, A., Chapman, B., Chernyshova, M., Chiariello, A., Chmielewski, P., Chomiczewska, A., Chone, L., Ciraolo, G., Ciric, D., Citrin, J., Ciupinski, t., Clark, M., Clarkson, R., Clements, C., Cleverly, M., Coad, J., Coates, P., Cobalt, A., Coccorese, V., Coelho, R., Coenen, J., Coffey, I., Colangeli, A., Colas, L., Collins, C., Collins, J., Collins, S., Conka, D., Conroy, S., Conway, B., Conway, N., Coombs, D., Cooper, P., Cooper, S., Corradino, C., Corrigan, G., Coster, D., Cox, P., Craciunescu, T., Cramp, S., Crapper, C., Craven, D., Craven, R., Crialesi Esposito, M., Croci, G., Croft, D., Croitoru, A., Crombe, K., Cronin, T., Cruz, N., Crystal, C., Cseh, G., Cufar, A., Cullen, A., Curuia, M., Czarski, T., Dabirikhah, H., Dal Molin, A., Dale, E., Dalgliesh, P., Dalley, S., Dankowski, J., David, P., Davies, A., Davies, S., Davis, G., Dawson, K., Dawson, S., Day, I., De Bock, M., De Temmerman, G., De Tommasi, G., Deakin, K., Deane, J., Dejarnac, R., Del Sarto, D., Delabie, E., Del-Castillo-Negrete, D., Dempsey, A., Dendy, R., Devynck, P., Di Siena, A., Di Troia, C., Dickson, T., Dinca, P., Dittmar, T., Dobrashian, J., Doerner, R., Donne, A., Dorling, S., Dormido-Canto, S., Douai, D., Dowson, S., Doyle, R., Drewelow, P., Drews, P., Drummond, G., Duckworth, P., Dudding, H., Dumont, R., Dumortier, P., Dunai, D., Dunatov, T., Dunne, M., Duran, I., Durodie, F., Dux, R., Dvornova, A., Eastham, R., Edwards, J., Eich, T., Eichorn, A., Eidietis, N., Eksaeva, A., Haroun, H., Ellwood, G., Elsmore, C., Embreus, O., Emery, S., Ericsson, G., Eriksson, B., Eriksson, F., Eriksson, L., Ertmer, S., Esquembri, S., Esquisabel, A., Estrada, T., Evans, G., Evans, S., Fable, E., Fagan, D., Faitsch, M., Falessi, M., Fanni, A., Farahani, A., Farquhar, I., Fasoli, A., Faugeras, B., Fazinie, S., Felici, F., Felton, R., Fernandes, A., Fernandes, H., Ferrand, J., Ferreira, D., Ferreira, J., Ferro, G., Fessey, J., Ficker, O., Field, A., Figueiredo, A., Figueiredo, J., Fil, A., Fil, N., Finburg, P., Fiorucci, D., Fischer, U., Fishpool, G., Fittill, L., Fitzgerald, M., Flammini, D., Flanagan, J., Flinders, K., Foley, S., Fonnesu, N., Fontana, M., Fontdecaba, J., Forbes, S., Formisano, A., Fornal, T., Fortuna, L., Fortuna-Zalesna, E., Fortune, M., Fowler, C., Fransson, E., Frassinetti, L., Freisinger, M., Fresa, R., Fridstrom, R., Frigione, D., Fülop, T., Furseman, M., Fusco, V., Futatani, S., Gadariya, D., Gal, K., Galassi, D., Gafezka, K., Galeani, S., Gallart, D., Galvao, R., Gao, Y., Garcia-Munoz, M., Gardener, M., Garzotti, L., Gaspar, J., Gatto, R., Gaudio, P., Gear, D., Gebhart, T., Gee, S., Gelfusa, M., George, R., Gerasimov, S., Gervasini, G., Gethins, M., Ghani, Z., Gherendi, M., Ghezzi, F., Giacalone, J., Giacomelli, L., Giacometti, G., Gibson, C., Gibson, K., Gil, L., Gillgren, A., Gin, D., Giovannozzi, E., Giroud, C., Glen, R., Gloggler, S., Goff, J., Gohil, P., Goloborodko, V., Gomes, R., Goncalves, B., Goniche, M., Goodyear, A., Gore, S., Gorini, G., Görler, T., Gotts, N., Goulding, R., Gow, E., Graham, B., Graves, J., Greuner, H., Grierson, B., Griffiths, J., Griph, S., Grist, D., Gromelski, W., Groth, M., Grove, R., Gruca, M., Guard, D., Gupta, N., Gurl, C., Gusarov, A., Hackett, L., Hacquin, S., Hager, R., Hagg, L., Hakola, A., Halitovs, M., Hall, S., Hallworth-Cook, S., Ham, C., Hamaguchi, D., Hamed, M., Hamlyn-Harris, C., Hammond, K., Harford, E., Harrison, J., Harting, D., Hatano, Y., Hatch, D., Haupt, T., Hawes, J., Hawkes, N., Hawkins, J., Hayashi, T., Hazael, S., Hazel, S., Heesterman, P., Heidbrink, B., Helou, W., Hemming, O., Henderson, S., Henriques, R., Hepple, D., Herfindal, J., Hermon, G., Hill, J., Hillesheim, J., Hizanidis, K., Hjalmarsson, A., Ho, A., Hobirk, J., Hoenen, O., Hogben, C., Hollingsworth, A., Hollis, S., Hollmann, E., Hoelzl, M., Homan, B., Hook, M., Hopley, D., Horacek, J., Horsley, D., Horsten, N., Horton, A., Horton, L., Horvath, L., Hotchin, S., Howell, R., Hu, Z., Huber, A., Huber, V., Huddleston, T., Huijsmans, G., Huynh, P., Hynes, A., Iliasova, M., lmrie, D., lmrísek, M., lngleby, J., Innocente, P., Insulander Björk, K., Isernia, N., lvanova-Stanik, I., lvings, E., Jablonski, S., Jachmich, S., Jackson, T., Jacquet, P., Järleblad, H., Jaulmes, F., Jenaro Rodriguez, J., Jepu, I., Joffrin, E., Johnson, R., Johnson, T., Johnston, J., Jones, C., Jones, G., Jones, L., Jones, N., Jones, T., Joyce, A., Juarez, R., Juvonen, M., Kalnina, P., Kaltiaisenaho, T., Kaniewski, J., Kantor, A., Kappatou, A., Karhunen, J., Karkinsky, D., Kashchuk, Y., Kaufman, M., Kaveney, G., Kazantzidis, V., Keeling, D., Kelly, R., Kempenaars, M., Kennedy, C., Kennedy, D., Kent, J., Khan, K., Khilkevich, E., Kiefer, C., Kilpeläinen, J., Kim, C., Kim, H., Kim, S., King, D., King, R., Kinna, D., Kiptily, V., Kirjasuo, A., Kirov, K., Kirschner, A., kiviniemi, T., Kizane, G., Klas, M., Klepper, C., Klix, A., Kneale, G., Knight, M., Knight, P., Knights, R., Knipe, S., Knolker, M., Knott, S., Kocan, M., Kochl, F., Kodeli, I., Kolesnichenko, Y., Kominis, Y., Kong, M., Korovin, V., Kos, B., Kos, D., Koslowski, H., Kotschenreuther, M., Koubiti, M., Kowalska-Strzeciwilk, E., Koziol, K., Krasilnikov, A., Krasilnikov, V., Kresina, M., Krieger, K., Krishnan, N., Krivska, A., Kruezi, U., Ksiezek, I., Kukushkin, A., Kumpulainen, H., Kurki-Suonio, T., Kurotaki, H., Kwak, S., Kwon, O., Laguardia, L., Lagzdina, E., Lahtinen, A., Laing, A., Lam, N., Lambertz, H., Lane, B., Lane, C., Lascas Neto, E., Laszyriska, E., 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moléculaires (PIIM), Aix Marseille Université (AMU)-Centre National de la Recherche Scientifique (CNRS), Institut de Recherche sur la Fusion par confinement Magnétique (IRFM), Commissariat à l'énergie atomique et aux énergies alternatives (CEA), Swiss Plasma Center (SPC), Ecole Polytechnique Fédérale de Lausanne (EPFL), Laboratory for Plasma Physics (LPP), Ecole Royale Militaire / Koninklijke Militaire School (ERM KMS), Kharkiv Institute of Physics and Technology (Ukraine), V.N. Karazin Kharkiv National University (KhNU), Dipartimento di Fisica (Milano), Università degli Studi di Milano = University of Milan (UNIMI), Consiglio Nazionale delle Ricerche [Milano] (CNR), Jozef Stefan Institute [Ljubljana] (IJS), Culham Centre for Fusion Energy (CCFE), Department of Physics and Astronomy [Uppsala], Uppsala University, This work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training programme 2014–2018 and 2019–2020 under Grant agreement No 633053., Mazzi, S, Garcia, J, Zarzoso, D, Kazakov, Y, Ongena, J, Dreval, M, Nocente, M, Stancar, Z, Szepesi, G, Eriksson, J, Sahlberg, A, Benkadda, S, Abid, N, Abraham, K, Abreu, P, Adabonyan, O, Adrich, P, Afzal, M, Ahlgren, T, Aho-Mantila, L, Aiba, N, Airila, M, Akhtar, M, Albanese, R, Alderson-Martin, M, Alegre, D, Aleiferis, S, Aleksa, A, Alessi, E, Aleynikov, P, Algualcil, J, Ali, M, Allinson, M, Alper, B, Alves, E, Ambrosino, G, Ambrosino, R, 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K., Zoulias, I., Zwingmann, W., Zychor, I., JET Contributors, Science and Technology of Nuclear Fusion, EIRES Eng. for Sustainable Energy Systems, Magneto-Hydro-Dynamic Stability of Fusion Plasmas, Applied Physics and Science Education, Kazakov, Yo, VTT Technical Research Centre of Finland, Culham Science Centre, Princeton Plasma Physics Laboratory, Department of Applied Physics, European Commission, Forschungszentrum Jülich, Universidade Lisboa, Fusion and Plasma Physics, University of Milan - Bicocca, Aalto University, General Atomics, ITER, University of Toyama, CEA, Oak Ridge National Laboratory, Technical University of Madrid, Swiss Federal Institute of Technology Lausanne, Dutch Institute for Fundamental Energy Research, Royal Military Academy, Seoul National University, Chalmers University of Technology, Max Planck Institute for Plasma Physics, KTH Royal Institute of Technology, and Aalto-yliopisto
- Subjects
[PHYS]Physics [physics] ,Settore FIS/01 ,Settore ING-IND/18 - Fisica dei Reattori Nucleari ,General Physics and Astronomy ,simulation ,magnetically confined plasma ,nuclear fusion ,tokamaks ,turbulence suppression ,Plasma ,[PHYS.PHYS.PHYS-PLASM-PH]Physics [physics]/Physics [physics]/Plasma Physics [physics.plasm-ph] ,confinement ,transport ,Alpha particles ,Fusion reactors ,Turbulence ,physics - Abstract
openaire: EC/H2020/633053/EU//EUROfusion Funding Information: We thank M. Baruzzo and F. Nave for the preparation and execution of JET experiments discussed in this paper; E. de la Luna for support in detailing the experimental diagnostics of JET; A. Ho for assistance in processing the experimental data; T. Görler for providing essential advice to ensure the correct numerical setup for the GENE modelling reported in this paper; Y. Camenen, X. Garbet and A. Bierwage for fruitful discussions about the gyrokinetic analyses; G. Giruzzi for valuable suggestions on the article strategy. The simulations were performed on the IRENE Joliot-Curie HPC system, in the framework of the PRACE projects IONFAST and AFIETC, led by J. Garcia, and on the CINECA Marconi HPC within the project GENE4EP, led by D. Zarzoso. This work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training programme 2014-2018 and 2019-2020 under grant agreement no. 633053. The views and opinions express herein do not necessarily reflect those of the European Commission. Part of the work by Ye. O. Kazakov and J.Ongena was also carried out in the framework of projects done for the ITER Scientist Fellow Network (ISFN). Funding Information: We thank M. Baruzzo and F. Nave for the preparation and execution of JET experiments discussed in this paper; E. de la Luna for support in detailing the experimental diagnostics of JET; A. Ho for assistance in processing the experimental data; T. Görler for providing essential advice to ensure the correct numerical setup for the GENE modelling reported in this paper; Y. Camenen, X. Garbet and A. Bierwage for fruitful discussions about the gyrokinetic analyses; G. Giruzzi for valuable suggestions on the article strategy. The simulations were performed on the IRENE Joliot-Curie HPC system, in the framework of the PRACE projects IONFAST and AFIETC, led by J. Garcia, and on the CINECA Marconi HPC within the project GENE4EP, led by D. Zarzoso. This work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training programme 2014-2018 and 2019-2020 under grant agreement no. 633053. The views and opinions express herein do not necessarily reflect those of the European Commission. Part of the work by Ye. O. Kazakov and J.Ongena was also carried out in the framework of projects done for the ITER Scientist Fellow Network (ISFN). Publisher Copyright: © 2022, The Author(s), under exclusive licence to Springer Nature Limited. Alpha particles with energies on the order of megaelectronvolts will be the main source of plasma heating in future magnetic confinement fusion reactors. Instead of heating fuel ions, most of the energy of alpha particles is transferred to electrons in the plasma. Furthermore, alpha particles can also excite Alfvénic instabilities, which were previously considered to be detrimental to the performance of the fusion device. Here we report improved thermal ion confinement in the presence of megaelectronvolts ions and strong fast ion-driven Alfvénic instabilities in recent experiments on the Joint European Torus. Detailed transport analysis of these experiments reveals turbulence suppression through a complex multi-scale mechanism that generates large-scale zonal flows. This holds promise for more economical operation of fusion reactors with dominant alpha particle heating and ultimately cheaper fusion electricity.
- Published
- 2022
33. Disruption prediction with artificial intelligence techniques in tokamak plasmas
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A., Huynh P., Hynes A., Iliasova M., lmrie D., lmrisek M., lngleby J., Innocente P., Bjork K. I., Isernia N., lvanova-Stanik I., lvings E., Jablonski S., Jachmich S., Jackson T., Jacquet P., Jarleblad H., Jaulmes F., Rodriguez J. J., Jepu I., Joffrin E., Johnson R., Johnson T., Johnston J., Jones C., Jones G., Jones L., Jones N., Jones T., Joyce A., Juarez R., Juvonen M., Kalnina P., Kaltiaisenaho T., Kaniewski J., Kantor A., Kappatou A., Karhunen J., Karkinsky D., Kashchuk Y., Kaufman M., Kaveney G., Kazakov Y. E. O., Kazantzidis V., Keeling D. L., Kelly R., Kempenaars M., Kennedy C., Kennedy D., Kent J., Khan K., Khilkevich E., Kiefer C., Kilpelainen J., Kim C., Kim H. -T., Kim S. H., King D. B., King R., Kinna D., Kiptily V. G., Kirjasuo A., Kirov K. K., Kirschner A., kiviniemi T., Kizane G., Klas M., Klepper C., Klix A., Kneale G., Knight M., Knight P., Knights R., Knipe S., Knolker M., Knott S., Kocan M., Kochl F., Kodeli I., Kolesnichenko Y., Kominis Y., Kong M., Korovin V., Kos B., Kos D., Koslowski H. R., Kotschenreuther M., Koubiti M., Kowalska-Strzeciwilk E., Koziol K., Krasilnikov A., Krasilnikov V., Kresina M., Krieger K., Krishnan N., Krivska A., Kruezi U., Ksiezek I., Kukushkin A. B., Kumpulainen H., Kurki-Suonio T., Kurotaki H., Kwak S., Kwon O. J., Laguardia L., Lagzdina E., Lahtinen A., Laing A., Lam N., Lambertz H. T., Lane B., Lane C., Neto E. L., Laszyriska E., Lawson K. D., Lazaros A., Lazzaro E., Learoyd G., Lee C., Lee S. E., Leerink S., Leeson T., Lefebvre X., Leggate H. J., Lehmann J., Lehnen M., Leichtle D., Leipold F., Lengar I., Lennholm M., Gutierrez E. L., Lepiavko B., Leppanen J., Lerche E., Lescinskis A., Lewis J., Leysen W., Li L., Li Y., Likonen J., Linsmeier C., Lipschultz B., Litaudon X., Litherland-Smith E., Liu F., Loarer T., Loarte A., Lobel R., Lomanowski B., Lomas P. J., Lopez J. M., Lorenzini R., Loreti S., Losada U., Loschiavo V. P., Loughlin M., Louka Z., Lovell J., Lowe T., Lowry C., Lubbad S., Luce T., Lucock R., Lukin A., Luna C., de la Luna E., Lungaroni M., Lungu C. P., Lunt T., Lutsenko V., Lyons B., Lyssoivan A., Machielsen M., Macusova E., Maenpaa R., Maggi C. F., Maggiora R., Magness M., Mahesan S., Maier H., Maingi R., Malinowski K., Manas P., Mantica P., Mantsinen M. J., Manyer J., Manzanares A., Maquet P., Marceca G., Marcenko N., Marchetto C., Marchuk O., Mariani A., Mariano G., Marin M., Marinelli M., Markovic T., Marocco D., Marot L., Marsden S., Marsh J., Marshall R., Martellucci L., Martin A., Martin A. J., Martone R., Maruyama S., Maslov M., Masuzaki S., Matejcik S., Mattei M., Matthews G. F., Matveev D., Matveeva E., Mauriya A., Maviglia F., Mayer M., Mayoral M. -L., Mazzi S., Mazzotta C., McAdams R., McCarthy P. J., McClements K. G., McClenaghan J., McCullen P., McDonald D. C., McGuckin D., McHugh D., Mclntyre G., McKean R., McKehon J., McMillan B., McNamee L., McShee A., Meakins A., Medley S., Meekes C. J., Meghani K., Meigs A. G., Meisl G., Meitner S., Menmuir S., Mergia K., Merriman S., Mertens P., Meshchaninov S., Messiaen A., Michling R., Middleton P., Middleton-Gear D., Mietelski J., Milanesio D., Milani E., Militello F., Asp A. M., Milnes J., Milocco A., Miloshevsky G., Minghao C., Minucci S., Miron I., Miyamoto M., Mlynar J., Moiseenko V., Monaghan P., Monakhov I., Moody T., Moon S., Mooney R., Moradi S., Morales J., Morales R. B., Mordijck S., Moreira L., Morgan L., Moro F., Morris J., Morrison K. -M., Moser L., Moulton D., Mrowetz T., Mundy T., Muraglia M., Muraro A., Muthusonai N., N'Konga B., Na Y. -S., Nabais F., Naden M., Naish J., Naish R., Napoli F., Nardon E., Naulin V., Nave M. F. F., Nedzelskiy I., Nemtsev G., Nesenevich V., Nestoras I., Neu R., Neverov V. S., Ng S., Nicassio M., Nielsen A. H., Nina D., Nishijima D., Noble C., Nobs C. R., Nocente M., Nodwell D., Nordlund K., Nordman H., Normanton R., Noterdaeme J. M., Nowak S., Nunn E., Nystrom H., Oberparleiter M., Obryk B., O'Callaghan J., Odupitan T., Oliver H. J. C., Olney R., O'Mullane M., Ongena J., Organ E., Orsitto F., Orszagh J., Osborne T., Otin R., Otsuka T., Owen A., Oya Y., Oyaizu M., Paccagnella R., Pace N., Packer L. W., Paige S., Pajuste E., Palade D., Pamela S. J. P., Panadero N., Panontin E., Papadopoulos A., Papp G., Papp P., Parail V. V., Pardanaud C., Parisi J., Diaz F. P., Parsloe A., Parsons M., Parsons N., Passeri M., Patel A., Pau A., Pautasso G., Pavlichenko R., Pavone A., Pawelec E., Soldan C. P., Peacock A., Pearce M., Peluso E., Penot C., Pepperell K., Pereira R., Pereira T., Cippo E. P., Pereslavtsev P., Perez von Thun C., Pericoli V., Perry D., Peterka M., Petersson P., Petravich G., Petrella N., Peyman M., Pillon M., Pinches S., Pintsuk G., Pires de Sa W., Pires dos Reis A., Piron C., Piron L., Pironti A., Pitts R., van de Plassche K. L., Platt N., Plyusnin V., Podesta M., Pokol G., Poli F. M., Pompilian O. G., Popovichev S., Poradzinski M., Porfiri M. T., Porkolab M., Porosnicu C., Porton M., Poulipoulis G., Predebon I., Prestopino G., Price C., Price D., Price M., Primetzhofer D., Prior P., Provatas G., Pucella G., Puglia P., Purahoo K., Pusztai I., Putignano O., Putterich T., Quercia A., Rachlew E., Radulescu G., Radulovic V., Rainford M., Raj P., Ralph G., Ramogida G., Rasmussen D., Rasmussen J. J., Ratynskaia S., Rebai M., Refy D., Reichle R., Reinke M., Reiser D., Reux C., Reynolds S., Richiusa M. L., Richyal S., Rigamonti D., Rimini F. G., Risner J., Riva M., Rivero-Rodriguez J., Roach C. M., Robins R., Robinson S., Robson D., Rodionov R., Rodrigues P., Ramos M. R., Rodriguez-Fernandez P., Romanelli F., Romanelli M., Romanelli S., Romazanov J., Rossi R., Rowe S., Rowlands D., Rubel M., Rubinacci G., Rubino G., Ruchko L., Ruiz M., Ruiz J. R., Ruset C., Rzadkiewicz J., Saarelma S., Safi E., Sahlberg A., Salewski M., Salmi A., Salmon R., Salzedas F., Sanders I., Sandiford D., Santos B., Santucci A., Sarkimaki K., Sarwar R., Sarychev I., Sauter O., Sauwan P., Scapin N., Schluck F., Schmid K., Schmuck S., Schneider M., Schneider P. A., Schworer D., Scott G., Scott M., Scraggs D., Scully S., Segato M., Seo J., Sergienko G., Sertoli M., Sharapov S. E., Shaw A., Sheikh H., Sheikh U., Shepherd A., Shevelev A., Shigin P., Shinohara K., Shiraiwa S., Shiraki D., Short M., Sias G., Silburn S. A., Silva A., Silva C., Silva J., Silvagni D., Simfukwe D., Simpson J., Sinclair D., Sipila S. K., Sips A. C. C., Siren P., Sirinelli A., Sjostrand H., Skinner N., Slater J., Smith N., Smith P., Snell J., Snoep G., Snoj L., Snyder P., Soare S., Solano E. R., Solokha V., Somers A., Sommariva C., Soni K., Sorokovoy E., Sos M., Sousa J., Sozzi C., Spagnolo S., Spelzini T., Spineanu F., Spong D., Sprada D., Sridhar S., Srinivasan C., Stables G., Staebler G., Stamatelatos I., Stancar Z., Staniec P., Stankunas G., Stead M., Stefanikova E., Stephen A., Stephens J., Stevenson P., Stojanov M., Strand P., Strauss H. R., Strikwerda S., Strom P., Stuart C. I., Studholme W., Subramani M., Suchkov E., Sumida S., Sun H. J., Susts T. E., Svensson J., Svoboda J., Sweeney R., Sytnykov D., Szabolics T., Szepesi G., Tabia B., Tadic T., Tal B., Tala T., Tallargio A., Tamain P., Tan H., Tanaka K., Tang W., Tardocchi M., Taylor D., Teimane A. S., Telesca G., Teplova N., Teplukhina A., Terentyev D., Terra A., Terranova D., Terranova N., Testa D., Tholerus E., Thomas J., Thoren E., Thorman A., Tierens W., Tinguely R. A., Tipton A., Todd H., Tokitani M., Tolias P., Tomes M., Tookey A., Torikai Y., von Toussaint U., Tsavalas P., Tskhakaya D., Turner I., Turner M., Turner M. M., Turnyanskiy M., Tvalashvili G., Tyrrell S., Tyshchenko M., Uccello A., Udintsev V., Urbanczyk G., Vadgama A., Valcarcel D., Valisa M., Olivares P. V., Vallhagen O., Valovic M., Eester D. V., Varje J., Vartanian S., Vasilopoulou T., Vayakis G., Vecsei M., Ventre S., Verdoolaege G., Verona C., Rinati G. V., Veshchev E., Vianello N., Viezzer E., Vignitchouk L., Vila R., Villari R., Villone F., Vincenzi P., Vinyar I., Viola B., Virtanen A. J., Vitins A., Vizvary Z., Vlad G., Vlad M., Vondracek P., de Vries P., Wakeling B., Walkden N. R., Walker M., Walker R., Walsh M., Wang E., Wang N., Warder S., Warren R., Waterhouse J., Watts C., Wauters T., Weckmann A., Maxwell H. W., Weiland M., Weisen H., Weiszflog M., Welch P., Wendler N., West A., Wheatley M., Wheeler S., Whitehead A., Whittaker D., Widdowson A., Wiesen S., Wilkinson J., Williams J. C., Willoughby D., Wilson I., Wilson J., Wilson T., Wischmeier M., Wise P., Withenshaw G., Withycombe A., Witts D., Wojcik-Gargula A., Wolfrum E., Wood R., Woodley C., Woodley R., Woods B., Wright J., Wright J. C., Xu T., Yadikin D., Yajima M., Yakovenko Y., Yang Y., Yanling W., Yanovskiy V., Young I., Young R., Zabolockis R. J., Zacks J., Zagorski R., Zaitsev F. S., Zakharov L., Zarins A., Fernandez D. Z., Zastrow K. -D., Zayachuk Y., Zerbini M., Zhang W., Zhou Y., Zlobinski M., Zocco A., Zohar A., Zoita V., Zoletnik S., Zotta V. 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J., Ratynskaia S., Rebai M., Refy D., Reichle R., Reinke M., Reiser D., Reux C., Reynolds S., Richiusa M. L., Richyal S., Rigamonti D., Rimini F. G., Risner J., Riva M., Rivero-Rodriguez J., Roach C. M., Robins R., Robinson S., Robson D., Rodionov R., Rodrigues P., Ramos M. R., Rodriguez-Fernandez P., Romanelli F., Romanelli M., Romanelli S., Romazanov J., Rossi R., Rowe S., Rowlands D., Rubel M., Rubinacci G., Rubino G., Ruchko L., Ruiz M., Ruiz J. R., Ruset C., Rzadkiewicz J., Saarelma S., Safi E., Sahlberg A., Salewski M., Salmi A., Salmon R., Salzedas F., Sanders I., Sandiford D., Santos B., Santucci A., Sarkimaki K., Sarwar R., Sarychev I., Sauter O., Sauwan P., Scapin N., Schluck F., Schmid K., Schmuck S., Schneider M., Schneider P. A., Schworer D., Scott G., Scott M., Scraggs D., Scully S., Segato M., Seo J., Sergienko G., Sertoli M., Sharapov S. E., Shaw A., Sheikh H., Sheikh U., Shepherd A., Shevelev A., Shigin P., Shinohara K., Shiraiwa S., Shiraki D., Short M., Sias G., Silburn S. A., Silva A., Silva C., Silva J., Silvagni D., Simfukwe D., Simpson J., Sinclair D., Sipila S. K., Sips A. C. C., Siren P., Sirinelli A., Sjostrand H., Skinner N., Slater J., Smith N., Smith P., Snell J., Snoep G., Snoj L., Snyder P., Soare S., Solano E. R., Solokha V., Somers A., Sommariva C., Soni K., Sorokovoy E., Sos M., Sousa J., Sozzi C., Spagnolo S., Spelzini T., Spineanu F., Spong D., Sprada D., Sridhar S., Srinivasan C., Stables G., Staebler G., Stamatelatos I., Stancar Z., Staniec P., Stankunas G., Stead M., Stefanikova E., Stephen A., Stephens J., Stevenson P., Stojanov M., Strand P., Strauss H. R., Strikwerda S., Strom P., Stuart C. I., Studholme W., Subramani M., Suchkov E., Sumida S., Sun H. J., Susts T. E., Svensson J., Svoboda J., Sweeney R., Sytnykov D., Szabolics T., Szepesi G., Tabia B., Tadic T., Tal B., Tala T., Tallargio A., Tamain P., Tan H., Tanaka K., Tang W., Tardocchi M., Taylor D., Teimane A. S., Telesca G., Teplova N., Teplukhina A., Terentyev D., Terra A., Terranova D., Terranova N., Testa D., Tholerus E., Thomas J., Thoren E., Thorman A., Tierens W., Tinguely R. A., Tipton A., Todd H., Tokitani M., Tolias P., Tomes M., Tookey A., Torikai Y., von Toussaint U., Tsavalas P., Tskhakaya D., Turner I., Turner M., Turner M. M., Turnyanskiy M., Tvalashvili G., Tyrrell S., Tyshchenko M., Uccello A., Udintsev V., Urbanczyk G., Vadgama A., Valcarcel D., Valisa M., Olivares P. V., Vallhagen O., Valovic M., Eester D. V., Varje J., Vartanian S., Vasilopoulou T., Vayakis G., Vecsei M., Ventre S., Verdoolaege G., Verona C., Rinati G. V., Veshchev E., Vianello N., Viezzer E., Vignitchouk L., Vila R., Villari R., Villone F., Vincenzi P., Vinyar I., Viola B., Virtanen A. J., Vitins A., Vizvary Z., Vlad G., Vlad M., Vondracek P., de Vries P., Wakeling B., Walkden N. R., Walker M., Walker R., Walsh M., Wang E., Wang N., Warder S., Warren R., Waterhouse J., Watts C., Wauters T., Weckmann A., Maxwell H. W., Weiland M., Weisen H., Weiszflog M., Welch P., Wendler N., West A., Wheatley M., Wheeler S., Whitehead A., Whittaker D., Widdowson A., Wiesen S., Wilkinson J., Williams J. C., Willoughby D., Wilson I., Wilson J., Wilson T., Wischmeier M., Wise P., Withenshaw G., Withycombe A., Witts D., Wojcik-Gargula A., Wolfrum E., Wood R., Woodley C., Woodley R., Woods B., Wright J., Wright J. C., Xu T., Yadikin D., Yajima M., Yakovenko Y., Yang Y., Yanling W., Yanovskiy V., Young I., Young R., Zabolockis R. J., Zacks J., Zagorski R., Zaitsev F. S., Zakharov L., Zarins A., Fernandez D. Z., Zastrow K. -D., Zayachuk Y., Zerbini M., Zhang W., Zhou Y., Zlobinski M., Zocco A., Zohar A., Zoita V., Zoletnik S., Zotta V. K., Zoulias I., Zwingmann W., and Zychor I.
- Abstract
In nuclear fusion reactors, plasmas are heated to very high temperatures of more than 100 million kelvin and, in so-called tokamaks, they are confined by magnetic fields in the shape of a torus. Light nuclei, such as deuterium and tritium, undergo a fusion reaction that releases energy, making fusion a promising option for a sustainable and clean energy source. Tokamak plasmas, however, are prone to disruptions as a result of a sudden collapse of the system terminating the fusion reactions. As disruptions lead to an abrupt loss of confinement, they can cause irreversible damage to present-day fusion devices and are expected to have a more devastating effect in future devices. Disruptions expected in the next-generation tokamak, ITER, for example, could cause electromagnetic forces larger than the weight of an Airbus A380. Furthermore, the thermal loads in such an event could exceed the melting threshold of the most resistant state-of-the-art materials by more than an order of magnitude. To prevent disruptions or at least mitigate their detrimental effects, empirical models obtained with artificial intelligence methods, of which an overview is given here, are commonly employed to predict their occurrence—and ideally give enough time to introduce counteracting measures.
- Published
- 2022
34. Experimental confirmation of efficient island divertor operation and successful neoclassical transport optimization in Wendelstein 7-X
- Author
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Pedersen, T, Abramovic, I, Agostinetti, P, Torres, M, Akaslompolo, S, Belloso, J, Aleynikov, P, Aleynikova, K, Alhashimi, M, Ali, A, Allen, N, Alonso, A, Anda, G, Andreeva, T, Angioni, C, Arkhipov, A, Arnold, A, Asad, W, Ascasibar, E, Aumeunier, M, Avramidis, K, Aymerich, E, Baek, S, Bahner, J, Baillod, A, Balden, M, Baldzuhn, J, Ballinger, S, Banduch, M, Bannmann, S, Navarro, A, Barbui, T, Beidler, C, Belafdil, C, Bencze, A, Benndorf, A, Beurskens, M, Biedermann, C, Biletskyi, O, Blackwell, B, Blatzheim, M, Bluhm, T, Bockenhoff, D, Bongiovi, G, Borchardt, M, Borodin, D, Boscary, J, Bosch, H, Bosmann, T, Boswirth, B, Bottger, L, Bottino, A, Bozhenkov, S, Brakel, R, Brandt, C, Brauer, T, Braune, H, Brezinsek, S, Brunner, K, Buller, S, Burhenn, R, Bussiahn, R, Buttenschon, B, Buzas, A, Bykov, V, Calvo, I, Mata, K, Caminal, I, Cannas, B, Cappa, A, Carls, A, Carovani, F, Carr, M, Carralero, D, Carvalho, B, Casas, J, Castano-Bardawil, D, Castejon, F, Chaudhary, N, Chelis, I, Chomiczewska, A, Coenen, J, Cole, M, Cordella, F, Corre, Y, Crombe, K, Cseh, G, Csillag, B, Damm, H, Day, C, de Baar, M, De la Cal, E, Degenkolbe, S, Demby, A, Denk, S, Dhard, C, Di Siena, A, Dinklage, A, Dittmar, T, Dreval, M, Drevlak, M, Drewelow, P, Drews, P, Dunai, D, Edlund, E, Effenberg, F, Ehrke, G, Endler, M, Ennis, D, Escoto, F, Estrada, T, Fable, E, Fahrenkamp, N, Fanni, A, Faustin, J, Fellinger, J, Feng, Y, Figacz, W, Flom, E, Ford, O, Fornal, T, Frerichs, H, Freundt, S, Fuchert, G, Fukuyama, M, Fullenbach, F, Gantenbein, G, Gao, Y, Garcia, K, Regana, J, Garcia-Cortes, I, Gaspar, J, Gates, D, Geiger, J, Geiger, B, Giudicotti, L, Gonzalez, A, Goriaev, A, Gradic, D, Grahl, M, Graves, J, Green, J, Grelier, E, Greuner, H, Gross, S, Grote, H, Groth, M, Gruca, M, Grulke, O, Grun, M, Arnaiz, J, Gunter, S, Haak, V, Haas, M, Hacker, P, Hakola, A, Hallenbert, A, Hammond, K, Han, X, Hansen, S, Harris, J, Hartfuss, H, Hartmann, D, Hathiramani, D, Hatzky, R, Hawke, J, Hegedus, S, Hein, B, Heinemann, B, Helander, P, Henneberg, S, Hergenhahn, U, Hidalgo, C, Hindenlang, F, Hirsch, M, Hofel, U, Hollfeld, K, Holtz, A, Hopf, D, Hoschen, D, Houry, M, Howard, J, Huang, X, Hubeny, M, Hudson, S, Ida, K, Igitkhanov, Y, Igochine, V, Illy, S, Ionita-Schrittwieser, C, Isobe, M, Jablczynska, M, Jablonski, S, Jagielski, B, Jakubowski, M, van Vuuren, A, Jelonnek, J, Jenko, F, Jensen, T, Jenzsch, H, Junghanns, P, Kaczmarczyk, J, Kallmeyer, J, Kamionka, U, Kandler, M, Kasilov, S, Kazakov, Y, Kennedy, D, Kharwandikar, A, Khokhlov, M, Kiefer, C, Killer, C, Kirschner, A, Kleiber, R, Klinger, T, Klose, S, Knauer, J, Knieps, A, Kochl, F, Kocsis, G, Kolesnichenko, Y, Konies, A, Konig, R, Kontula, J, Kornejew, P, Koschinsky, J, Kozulia, M, Kramer-Flecken, A, Krampitz, R, Krause, M, Krawczyk, N, Kremeyer, T, Krier, L, Kriete, D, Krychowiak, M, Ksiazek, I, Kubkowska, M, Kuczynski, M, Kuhner, G, Kumar, A, Kurki-Suonio, T, Kwak, S, Landreman, M, Lang, P, Langenberg, A, Laqua, H, Laube, R, Lazerson, S, 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Pechstein, G, Pelka, G, Perseo, V, Peterson, B, Pilopp, D, Pingel, S, Pisano, F, Plockl, B, Plunk, G, Poloskei, P, Pompe, B, Popov, A, Porkolab, M, Proll, J, Pueschel, M, Puiatti, M, Sitjes, A, Purps, F, Rahbarnia, K, Rasinski, M, Rasmussen, J, Reiman, A, Reimold, F, Reisner, M, Reiter, D, Richou, M, Riedl, R, Riemann, J, Risse, K, Roberg-Clark, G, Rohde, V, Romazanov, J, Rondeshagen, D, Rong, P, Rudischhauser, L, Rummel, T, Rummel, K, Runov, A, Rust, N, Ryc, L, Salembier, P, Salewski, M, Sanchez, E, Satake, S, Satheeswaran, G, Schacht, J, Scharff, E, Schauer, F, Schilling, J, Schlisio, G, Schmid, K, Schmitt, J, Schmitz, O, Schneider, W, Schneider, M, Schneider, P, Schrittwieser, R, Schroder, T, Schroder, M, Schroeder, R, Schweer, B, Schworer, D, Scott, E, Shanahan, B, Sias, G, Sichta, P, Singer, M, Sinha, P, Siplia, S, Slaby, C, Sleczka, M, Smith, H, Smoniewski, J, Sonnendrucker, E, Spolaore, M, Spring, A, Stadler, R, Stanczak, D, Stange, T, Stepanov, I, Stephey, L, Stober, J, Stroth, U, Strumberger, E, Suzuki, C, Suzuki, Y, Svensson, J, Szabolics, T, Szepesi, T, Szucs, M, Tabares, F, Tamura, N, Tancetti, A, Tantos, C, Terry, J, Thienpondt, H, Thomsen, H, Thumm, M, Travere, J, Traverso, P, Tretter, J, Trier, E, Mora, H, Tsujimura, T, Turkin, Y, Tykhyi, A, Unterberg, B, van Eeten, P, van Milligen, B, van Schoor, M, Vano, L, Varoutis, S, Vecsei, M, Vela, L, Velasco, J, Vervier, M, Vianello, N, Viebke, H, Vilbrandt, R, Vogel, G, Vogt, N, Volkhausen, C, von Stechow, A, Wagner, F, Wang, E, Wang, H, Warmer, F, Wauters, T, Wegener, L, Wegner, T, Weir, G, Wenzel, U, White, A, Wilde, F, Wilms, F, Windisch, T, Winkler, M, Winter, A, Winters, V, Wolf, R, Wright, A, Wurden, G, Xanthopoulos, P, Xu, S, Yamada, H, Yamaguchi, H, Yokoyama, M, Yoshinuma, M, Yu, Q, Zamanov, M, Zanini, M, Zarnstorff, M, Zhang, D, Zhou, S, Zhu, J, Zhu, C, Zilker, M, Zocco, A, Zohm, H, Zoletnik, S, Zsuga, L, Pedersen T. S., Abramovic I., Agostinetti P., Torres M. A., Akaslompolo S., Belloso J. A., Aleynikov P., Aleynikova K., Alhashimi M., Ali A., Allen N., Alonso A., Anda G., Andreeva T., Angioni C., Arkhipov A., Arnold A., Asad W., Ascasibar E., Aumeunier M. -H., Avramidis K., Aymerich E., Baek S. -G., Bahner J., Baillod A., Balden M., Baldzuhn J., Ballinger S., Banduch M., Bannmann S., Navarro A. B., Barbui T., Beidler C., Belafdil C., Bencze A., Benndorf A., Beurskens M., Biedermann C., Biletskyi O., Blackwell B., Blatzheim M., Bluhm T., Bockenhoff D., Bongiovi G., Borchardt M., Borodin D., Boscary J., Bosch H., Bosmann T., Boswirth B., Bottger L., Bottino A., Bozhenkov S., Brakel R., Brandt C., Brauer T., Braune H., Brezinsek S., Brunner K., Buller S., Burhenn R., Bussiahn R., Buttenschon B., Buzas A., Bykov V., Calvo I., Mata K. C., Caminal I., Cannas B., Cappa A., Carls A., Carovani F., Carr M., Carralero D., Carvalho B., Casas J., Castano-Bardawil D., Castejon F., Chaudhary N., Chelis I., Chomiczewska A., Coenen J. W., Cole M., Cordella F., Corre Y., Crombe K., Cseh G., Csillag B., Damm H., Day C., de Baar M., De la Cal E., Degenkolbe S., Demby A., Denk S., Dhard C., Di Siena A., Dinklage A., Dittmar T., Dreval M., Drevlak M., Drewelow P., Drews P., Dunai D., Edlund E., Effenberg F., Ehrke G., Endler M., Ennis D. A., Escoto F. J., Estrada T., Fable E., Fahrenkamp N., Fanni A., Faustin J., Fellinger J., Feng Y., Figacz W., Flom E., Ford O., Fornal T., Frerichs H., Freundt S., Fuchert G., Fukuyama M., Fullenbach F., Gantenbein G., Gao Y., Garcia K., Regana J. M. G., Garcia-Cortes I., Gaspar J., Gates D. A., Geiger J., Geiger B., Giudicotti L., Gonzalez A., Goriaev A., Gradic D., Grahl M., Graves J. P., Green J., Grelier E., Greuner H., Gross S., Grote H., Groth M., Gruca M., Grulke O., Grun M., Arnaiz J. G., Gunter S., Haak V., Haas M., Hacker P., Hakola A., Hallenbert A., Hammond K., Han X., Hansen S. K., Harris J. H., Hartfuss H., Hartmann D., Hathiramani D., Hatzky R., Hawke J., Hegedus S., Hein B., Heinemann B., Helander P., Henneberg S., Hergenhahn U., Hidalgo C., Hindenlang F., Hirsch M., Hofel U., Hollfeld K. P., Holtz A., Hopf D., Hoschen D., Houry M., Howard J., Huang X., Hubeny M., Hudson S., Ida K., Igitkhanov Y., Igochine V., Illy S., Ionita-Schrittwieser C., Isobe M., Jablczynska M., Jablonski S., Jagielski B., Jakubowski M., van Vuuren A. J., Jelonnek J., Jenko F., Jensen T., Jenzsch H., Junghanns P., Kaczmarczyk J., Kallmeyer J., Kamionka U., Kandler M., Kasilov S., Kazakov Y., Kennedy D., Kharwandikar A., Khokhlov M., Kiefer C., Killer C., Kirschner A., Kleiber R., Klinger T., Klose S., Knauer J., Knieps A., Kochl F., Kocsis G., Kolesnichenko Ya. I., Konies A., Konig R., Kontula J., Kornejew P., Koschinsky J., Kozulia M. M., Kramer-Flecken A., Krampitz R., Krause M., Krawczyk N., Kremeyer T., Krier L., Kriete D. M., Krychowiak M., Ksiazek I., Kubkowska M., Kuczynski M., Kuhner G., Kumar A., Kurki-Suonio T., Kwak S., Landreman M., Lang P. T., Langenberg A., Laqua H. P., Laqua H., Laube R., Lazerson S., Lewerentz M., Li C., Liang Y., Linsmeier Ch., Lion J., Litnovsky A., Liu S., Lobsien J., Loizu J., Lore J., Lorenz A., Losada U., Louche F., Lunsford R., Lutsenko V., Machielsen M., Mackel F., Maisano-Brown J., Maj O., Makowski D., Manduchi G., Maragkoudakis E., Marchuk O., Marsen S., Martines E., Martinez-Fernandez J., Marushchenko M., Masuzaki S., Maurer D., Mayer M., McCarthy K. J., McCormack O., McNeely P., Meister H., Mendelevitch B., Mendes S., Merlo A., Messian A., Mielczarek A., Mishchenko O., Missal B., Mitteau R., Moiseenko V. E., Mollen A., Moncada V., Monnich T., Morisaki T., Moseev D., Motojima G., Mulas S., Mulsow M., Nagel M., Naujoks D., Naulin V., Neelis T., Neilson H., Neu R., Neubauer O., Neuner U., Nicolai D., Nielsen S. K., Niemann H., Nishiza T., Nishizawa T., Nuhrenberg C., Ochoukov R., Oelmann J., Offermanns G., Ogawa K., Okamura S., Olmanns J., Ongena J., Oosterbeek J., Otte M., Pablant N., Alvarez N. P., Pandey A., Pasch E., Pavlichenko R., Pavone A., Pawelec E., Pechstein G., Pelka G., Perseo V., Peterson B., Pilopp D., Pingel S., Pisano F., Plockl B., Plunk G., Poloskei P., Pompe B., Popov A., Porkolab M., Proll J., Pueschel M. J., Puiatti M. -E., Sitjes A. P., Purps F., Rahbarnia K., Rasinski M., Rasmussen J., Reiman A., Reimold F., Reisner M., Reiter D., Richou M., Riedl R., Riemann J., Risse K., Roberg-Clark G., Rohde V., Romazanov J., Rondeshagen D., Rong P., Rudischhauser L., Rummel T., Rummel K., Runov A., Rust N., Ryc L., Salembier P., Salewski M., Sanchez E., Satake S., Satheeswaran G., Schacht J., Scharff E., Schauer F., Schilling J., Schlisio G., Schmid K., Schmitt J., Schmitz O., Schneider W., Schneider M., Schneider P., Schrittwieser R., Schroder T., Schroder M., Schroeder R., Schweer B., Schworer D., Scott E., Shanahan B., Sias G., Sichta P., Singer M., Sinha P., Siplia S., Slaby C., Sleczka M., Smith H., Smoniewski J., Sonnendrucker E., Spolaore M., Spring A., Stadler R., Stanczak D., Stange T., Stepanov I., Stephey L., Stober J., Stroth U., Strumberger E., Suzuki C., Suzuki Y., Svensson J., Szabolics T., Szepesi T., Szucs M., Tabares F. L., Tamura N., Tancetti A., Tantos C., Terry J., Thienpondt H., Thomsen H., Thumm M., Travere J. M., Traverso P., Tretter J., Trier E., Mora H. T., Tsujimura T., Turkin Y., Tykhyi A., Unterberg B., van Eeten P., van Milligen B. Ph., van Schoor M., Vano L., Varoutis S., Vecsei M., Vela L., Velasco J. L., Vervier M., Vianello N., Viebke H., Vilbrandt R., Vogel G., Vogt N., Volkhausen C., von Stechow A., Wagner F., Wang E., Wang H., Warmer F., Wauters T., Wegener L., Wegner T., Weir G., Wenzel U., White A., Wilde F., Wilms F., Windisch T., Winkler M., Winter A., Winters V., Wolf R., Wright A. M., Wurden G. A., Xanthopoulos P., Xu S., Yamada H., Yamaguchi H., Yokoyama M., Yoshinuma M., Yu Q., Zamanov M., Zanini M., Zarnstorff M., Zhang D., Zhou S., Zhu J., Zhu C., Zilker M., Zocco A., Zohm H., Zoletnik S., Zsuga L., Pedersen, T, Abramovic, I, Agostinetti, P, Torres, M, Akaslompolo, S, Belloso, J, Aleynikov, P, Aleynikova, K, Alhashimi, M, Ali, A, Allen, N, Alonso, A, Anda, G, Andreeva, T, Angioni, C, Arkhipov, A, Arnold, A, Asad, W, Ascasibar, E, Aumeunier, M, Avramidis, K, Aymerich, E, Baek, S, Bahner, J, Baillod, A, Balden, M, Baldzuhn, J, Ballinger, S, Banduch, M, Bannmann, S, Navarro, A, Barbui, T, Beidler, C, Belafdil, C, Bencze, A, Benndorf, A, Beurskens, M, Biedermann, C, Biletskyi, O, Blackwell, B, Blatzheim, M, Bluhm, T, Bockenhoff, D, Bongiovi, G, Borchardt, M, Borodin, D, Boscary, J, Bosch, H, Bosmann, T, Boswirth, B, Bottger, L, Bottino, A, Bozhenkov, S, Brakel, R, Brandt, C, Brauer, T, Braune, H, Brezinsek, S, Brunner, K, Buller, S, Burhenn, R, Bussiahn, R, Buttenschon, B, 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- Abstract
We present recent highlights from the most recent operation phases of Wendelstein 7-X, the most advanced stellarator in the world. Stable detachment with good particle exhaust, low impurity content, and energy confinement times exceeding 100 ms, have been maintained for tens of seconds. Pellet fueling allows for plasma phases with reduced ion-temperature-gradient turbulence, and during such phases, the overall confinement is so good (energy confinement times often exceeding 200 ms) that the attained density and temperature profiles would not have been possible in less optimized devices, since they would have had neoclassical transport losses exceeding the heating applied in W7-X. This provides proof that the reduction of neoclassical transport through magnetic field optimization is successful. W7-X plasmas generally show good impurity screening and high plasma purity, but there is evidence of longer impurity confinement times during turbulence-suppressed phases.
- Published
- 2022
35. Enhanced performance in fusion plasmas through turbulence suppression by megaelectronvolt ions
- Author
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A., Huynh P., Hynes A., Imrie D., Imrisek M., Ingleby J., Innocente P., Insulander Bjork K., Isernia N., Ivanova-Stanik I., Ivings E., Jablonski S., Jachmich S., Jackson T., Jacquet P., Jarleblad H., Jaulmes F., Rodriguez J. J., Jepu I., Joffrin E., Johnson R., Johnson T., Johnston J., Jones C., Jones G., Jones L., Jones N., Jones T., Joyce A., Juarez R., Juvonen M., Kalnina P., Kaltiaisenaho T., Kaniewski J., Kantor A., Kappatou A., Karhunen J., Karkinsky D., Kaufman M., Kaveney G., Kazantzidis V., Keeling D. L., Kelly R., Kempenaars M., Kennedy C., Kennedy D., Kent J., Khan K., Kiefer C., Kilpelainen J., Kim C., Kim H. -T., Kim S. H., King D. B., King R., Kinna D., Kiptily V. G., Kirjasuo A., Kirov K. K., Kirschner A., Kiviniemi T., Kizane G., Klas M., Klepper C., Klix A., Kneale G., Knight M., Knight P., Knights R., Knipe S., Knolker M., Knott S., Kocan M., Kochl F., Kodeli I., Kolesnichenko Y., Kominis Y., Kong M., Korovin V., Kos B., Kos D., Koslowski H. R., Kotschenreuther M., Koubiti M., Kowalska-Strzeciwilk E., Koziol K., Krasilnikov V., Kresina M., Krieger K., Krishnan N., Krivska A., Kruezi U., Ksiazek I., Kukushkin A. B., Kumpulainen H., Kurki-Suonio T., Kurotaki H., Kwak S., Kwon O. J., Laguardia L., Lagzdina E., Lahtinen A., Laing A., Lam N., Lambertz H. T., Lane B., Lane C., Lascas Neto E., Laszynska E., Lawson K. D., Lazaros A., Lazzaro E., Learoyd G., Lee C., Lee S. E., Leerink S., Leeson T., Lefebvre X., Leggate H. J., Lehmann J., Lehnen M., Leichtle D., Leipold F., Lengar I., Lennholm M., Leon Gutierrez E., Lepiavko B., Leppanen J., Lerche E., Lescinskis A., Lewis J., Leysen W., Li L., Li Y., Likonen J., Linsmeier C., Lipschultz B., Litaudon X., Litherland-Smith E., Liu F., Loarer T., Loarte A., Lobel R., Lomanowski B., Lomas P. J., Lopez J. M., Lorenzini R., Loreti S., Losada U., Loschiavo V. P., Loughlin M., Louka Z., Lovell J., Lowe T., Lowry C., Lubbad S., Luce T., Lucock R., Luna C., de la Luna E., Lungaroni M., Lungu C. P., Lunt T., Lutsenko V., Lyons B., Lyssoivan A., Machielsen M., Macusova E., Maenpaa R., Maggi C. F., Maggiora R., Magness M., Mahesan S., Maier H., Mailloux J., Maingi R., Malinowski K., Manas P., Mantica P., Mantsinen M. J., Manyer J., Manzanares A., Maquet P., Marceca G., Marchetto C., Marchuk O., Mariani A., Mariano G., Marin M., Marinelli M., Markovic T., Marocco D., Marot L., Marsden S., Marsh J., Marshall R., Martellucci L., Martin A., Martin A. J., Martone R., Maruyama S., Maslov M., Masuzaki S., Matejcik S., Mattei M., Matthews G. F., Matveev D., Matveeva E., Mauriya A., Maviglia F., Mayer M., Mayoral M. -L., Mazzotta C., McAdams R., McCarthy P. J., McClements K. G., McClenaghan J., McCullen P., McDonald D. C., McGuckin D., McHugh D., McIntyre G., McKean R., McKehon J., McMillan B., McNamee L., McShee A., Meakins A., Medley S., Meekes C. J., Meghani K., Meigs A. G., Meisl G., Meitner S., Menmuir S., Mergia K., Merriman S., Mertens P., Messiaen A., Michling R., Middleton P., Middleton-Gear D., Mietelski J., Milanesio D., Milani E., Militello F., Militello Asp A., Milnes J., Milocco A., Miloshevsky G., Minghao C., Minucci S., Miron I., Miyamoto M., Mlynar J., Moiseenko V., Monaghan P., Monakhov I., Moody T., Moon S., Mooney R., Moradi S., Morales J., Morales R. B., Mordijck S., Moreira L., Morgan L., Moro F., Morris J., Morrison K. -M., Moser L., Moulton D., Mrowetz T., Mundy T., Muraglia M., Murari A., Muraro A., Muthusonai N., N'Konga B., Na Y. -S., Nabais F., Naden M., Naish J., Naish R., Napoli F., Nardon E., Naulin V., Nave M. F. F., Nedzelskiy I., Nestoras I., Neu R., Ng S., Nicassio M., Nielsen A. H., Nina D., Nishijima D., Noble C., Nobs C. R., Nodwell D., Nordlund K., Nordman H., Normanton R., Noterdaeme J. -M., Nowak S., Nunn E., Nystrom H., Oberparleiter M., Obryk B., O'Callaghan J., Odupitan T., Oliver H. J. C., Olney R., O'Mullane M., Organ E., Orsitto F., Orszagh J., Osborne T., Otin R., Otsuka T., Owen A., Oya Y., Oyaizu M., Paccagnella R., Pace N., Packer L. W., Paige S., Pajuste E., Palade D., Pamela S. J. P., Panadero N., Panontin E., Papadopoulos A., Papp G., Papp P., Parail V. V., Pardanaud C., Parisi J., Parra Diaz F., Parsloe A., Parsons M., Parsons N., Passeri M., Patel A., Pau A., Pautasso G., Pavlichenko R., Pavone A., Pawelec E., Soldan C. P., Peacock A., Pearce M., Peluso E., Penot C., Pepperell K., Pereira R., Pereira T., Cippo E. P., Pereslavtsev P., von Thun C. P., Pericoli V., Perry D., Peterka M., Petersson P., Petravich G., Petrella N., Peyman M., Pillon M., Pinches S., Pintsuk G., de Sa W. P., dos Reis A. P., Piron C., Piron L., Pironti A., Pitts R., van de Plassche K. L., Platt N., Plyusnin V., Podesta M., Pokol G., Poli F. M., Pompilian O. G., Popovichev S., Poradzinski M., Porfiri M. T., Porkolab M., Porosnicu C., Porton M., Poulipoulis G., Predebon I., Prestopino G., Price C., Price D., Price M., Primetzhofer D., Prior P., Provatas G., Pucella G., Puglia P., Purahoo K., Pusztai I., Putignano O., Putterich T., Quercia A., Rachlew E., Radulescu G., Radulovic V., Rainford M., Raj P., Ralph G., Ramogida G., Rasmussen D., Rasmussen J. J., Ratta G., Ratynskaia S., Rebai M., Refy D., Reichle R., Reinke M., Reiser D., Reux C., Reynolds S., Richiusa M. L., Richyal S., Rigamonti D., Rimini F. G., Risner J., Riva M., Rivero-Rodriguez J., Roach C. M., Robins R., Robinson S., Robson D., Rodrigues P., Rodriguez Ramos M., Rodriguez-Fernandez P., Romanelli F., Romanelli M., Romanelli S., Romazanov J., Rossi R., Rowe S., Rowlands D., Rubel M., Rubinacci G., Rubino G., Ruchko L., Ruiz M., Ruiz J. R., Ruset C., Rzadkiewicz J., Saarelma S., Safi E., Salewski M., Salmi A., Salmon R., Salzedas F., Sanders I., Sandiford D., Santos B., Santucci A., Sarkimaki K., Sarwar R., Sarychev I., Sauter O., Sauwan P., Scapin N., Schluck F., Schmid K., Schmuck S., Schneider M., Schneider P. A., Schworer D., Scott G., Scott M., Scraggs D., Scully S., Segato M., Seo J., Sergienko G., Sertoli M., Sharapov S. E., Shaw A., Sheikh H., Sheikh U., Shepherd A., Shigin P., Shinohara K., Shiraiwa S., Shiraki D., Short M., Sias G., Silburn S. A., Silva A., Silva C., Silva J., Silvagni D., Simfukwe D., Simpson J., Sinclair D., Sipila S. K., Sips A. C. C., Siren P., Sirinelli A., Sjostrand H., Skinner N., Slater J., Smith N., Smith P., Snell J., Snoep G., Snoj L., Snyder P., Soare S., Solano E. 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R., Ruset C., Rzadkiewicz J., Saarelma S., Safi E., Salewski M., Salmi A., Salmon R., Salzedas F., Sanders I., Sandiford D., Santos B., Santucci A., Sarkimaki K., Sarwar R., Sarychev I., Sauter O., Sauwan P., Scapin N., Schluck F., Schmid K., Schmuck S., Schneider M., Schneider P. A., Schworer D., Scott G., Scott M., Scraggs D., Scully S., Segato M., Seo J., Sergienko G., Sertoli M., Sharapov S. E., Shaw A., Sheikh H., Sheikh U., Shepherd A., Shigin P., Shinohara K., Shiraiwa S., Shiraki D., Short M., Sias G., Silburn S. A., Silva A., Silva C., Silva J., Silvagni D., Simfukwe D., Simpson J., Sinclair D., Sipila S. K., Sips A. C. C., Siren P., Sirinelli A., Sjostrand H., Skinner N., Slater J., Smith N., Smith P., Snell J., Snoep G., Snoj L., Snyder P., Soare S., Solano E. R., Solokha V., Somers A., Sommariva C., Soni K., Sorokovoy E., Sos M., Sousa J., Sozzi C., Spagnolo S., Spelzini T., Spineanu F., Spong D., Sprada D., Sridhar S., Srinivasan C., Stables G., Staebler G., Stamatelatos I., Staniec P., Stankunas G., Stead M., Stefanikova E., Stephen A., Stephens J., Stevenson P., Stojanov M., Strand P., Strauss H. R., Strikwerda S., Strom P., Stuart C. I., Studholme W., Subramani M., Suchkov E., Sumida S., Sun H. J., Susts T. E., Svensson J., Svoboda J., Sweeney R., Sytnykov D., Szabolics T., Tabia B., Tadic T., Tal B., Tala T., Tallargio A., Tamain P., Tan H., Tanaka K., Tang W., Tardocchi M., Taylor D., Teimane A. S., Telesca G., Teplukhina A., Terentyev D., Terra A., Terranova D., Terranova N., Testa D., Tholerus E., Thomas J., Thoren E., Thorman A., Tierens W., Tinguely R. A., Tipton A., Todd H., Tokitani M., Tolias P., Tomes M., Tookey A., Torikai Y., von Toussaint U., Tsavalas P., Tskhakaya D., Turner I., Turner M., Turner M. M., Turnyanskiy M., Tvalashvili G., Tyrrell S., Tyshchenko M., Uccello A., Udintsev V., Urbanczyk G., Vadgama A., Valcarcel D., Valisa M., Vallejos Olivares P., Vallhagen O., Valovic M., Van Eester D., Varje J., Vartanian S., Vasilopoulou T., Vayakis G., Vecsei M., Vega J., Ventre S., Verdoolaege G., Verona C., Rinati G. V., Veshchev E., Vianello N., Viezzer E., Vignitchouk L., Vila R., Villari R., Villone F., Vincenzi P., Viola B., Virtanen A. J., Vitins A., Vizvary Z., Vlad G., Vlad M., Vondracek P., de Vries P., Wakeling B., Walkden N. R., Walker M., Walker R., Walsh M., Wang E., Wang N., Warder S., Warren R., Waterhouse J., Watts C., Wauters T., Weckmann A., Wedderburn Maxwell H., Weiland M., Weisen H., Weiszflog M., Welch P., Wendler N., West A., Wheatley M., Wheeler S., Whitehead A., Whittaker D., Widdowson A., Wiesen S., Wilkinson J., Williams J. C., Willoughby D., Wilson I., Wilson J., Wilson T., Wischmeier M., Wise P., Withenshaw G., Withycombe A., Witts D., Wojcik-Gargula A., Wolfrum E., Wood R., Woodley C., Woodley R., Woods B., Wright J., Wright J. C., Xu T., Yadikin D., Yajima M., Yakovenko Y., Yang Y., Yanling W., Yanovskiy V., Young I., Young R., Zabolockis R. J., Zacks J., Zagorski R., Zaitsev F. S., Zakharov L., Zarins A., Zastrow K. -D., Zayachuk Y., Zerbini M., Zhang W., Zhou Y., Zlobinski M., Zocco A., Zohar A., Zoita V., Zoletnik S., Zotta V. K., Zoulias I., Zwingmann W., and Zychor I.
- Abstract
Alpha particles with energies on the order of megaelectronvolts will be the main source of plasma heating in future magnetic confinement fusion reactors. Instead of heating fuel ions, most of the energy of alpha particles is transferred to electrons in the plasma. Furthermore, alpha particles can also excite Alfvénic instabilities, which were previously considered to be detrimental to the performance of the fusion device. Here we report improved thermal ion confinement in the presence of megaelectronvolts ions and strong fast ion-driven Alfvénic instabilities in recent experiments on the Joint European Torus. Detailed transport analysis of these experiments reveals turbulence suppression through a complex multi-scale mechanism that generates large-scale zonal flows. This holds promise for more economical operation of fusion reactors with dominant alpha particle heating and ultimately cheaper fusion electricity.
- Published
- 2022
36. Evidence That the Length of Bile Loop Determines Serum Bile Acid Concentration and Glycemic Control After Bariatric Surgery
- Author
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Mika, Adriana, Kaska, Lukasz, Proczko-Stepaniak, Monika, Chomiczewska, Agnieszka, Swierczynski, Julian, Smolenski, Ryszard T, and Sledzinski, Tomasz
- Published
- 2018
- Full Text
- View/download PDF
37. Screening survey of ocular, nasal, respiratory and skin symptoms in manicurists in Poland
- Author
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Marta Kieć-Świerczyńska, Dominika Świerczyńska-Machura, Dorota Chomiczewska-Skóra, Beata Kręcisz, and Jolanta Walusiak-Skorupa
- Subjects
manicurists ,beauty salons ,occupational exposure ,screening ,allergy symptoms ,acrylates ,Medicine - Abstract
Objectives: Manicurists are exposed to various chemicals in nail and skin care products and may develop ocular, nasal, respiratory or skin adverse reactions to them. To investigate the occurrence of ocular, nasal, respiratory and skin problems among manicurists and to identify their causal factors, particularly allergic etiology and occupational origin. Material and Methods: Manicurists employed in beauty salons in the central region of Poland were invited to fill in the questionnaire and undergo medical examination, skin prick tests with common aeroallergens, patch tests with European Baseline Series and (Meth)Acrylates Series-Nails and spirometry. Results: In the questionnaire adverse nasal symptoms were reported by 70%, ocular – by 58%, respiratory – by 42%, hand eczema – by 43% of manicurists. In the medical interview, the frequency of those complaints was lower: nasal ones – 41%, ocular – 24%, cough – 18%, hand skin dryness – 20%, hand eczema – 6%. Cough and hand skin dryness occurred significantly more frequently than in the case of controls. Contact allergy was found for 41% of manicurists and 35% of controls. The prevalence of nickel sensitization was high in both groups (38% and 27%, respectively). Only 3 manicurists reacted to (meth)acrylates. The frequency of atopic diseases was similar in compared groups. Irritant nasal and respiratory reactions were significantly more prevalent among manicurists (nasal – 18% vs. 2%, p < 0.01; respiratory – 18% vs. 1%, p < 0.001). Work-related nasal irritant reactions were finally diagnosed for 19%, ocular ones – for 13%, respiratory – for 18% and within hand skin – for 23% of manicurists. Conclusions: The frequency of workattributed irritant mucosal and skin symptoms among manicurists is high. Exposure to acrylates is an important source of mucosal irritant reactions while occlusive gloves cause irritation of hand skin. The prevalence of nickel allergy among Polish females is high. Int J Occup Med Environ Health 2017;30(6):887–896
- Published
- 2017
- Full Text
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38. The JET hybrid scenario in Deuterium, Tritium and Deuterium-Tritium
- Author
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Hobirk, J., Challis, C. D., Kappatou, A., Lerche, E., Keeling, D., King, D., Aleiferis, S., Alessi, E., Angioni, C., Auriemma, F., Baruzzo, M., Belonohy, E., Bernardo, J., Boboc, A., Carvalho, I. S., Carvalho, P., Casson, F. J., Chomiczewska, A., Citrin, J., Coffey, I. H., Conway, N. J., Douai, D., Delabie, E., Eriksson, Benjamin, Eriksson, Jacob, Ficker, O., Field, A. R., Fontana, M., Fontdecaba, J. M., Frassinetti, L., Frigione, D., Gallart, D., Garcia, J., Gelfusa, M., Ghani, Z., Giacomelli, L., Giovannozzi, E., Giroud, C., Goniche, M., Gromelski, W., Hacquin, S., Ham, C., Hawkes, N. C., Henriques, R. B., Hillesheim, J. C., Ho, A., Horvath, L., Ivanova-Stanik, I., Jacquet, P., Jaulmes, F., Joffrin, E., Kim, H. T., Kiptily, V., Kirov, K., Kos, D., Kowalska-Strzeciwilk, E., Kumpulainen, H., Lawson, K., Lennholm, M., Litaudon, X., Litherland-Smith, E., Lomas, P. J., de la Luna, E., Maggi, C. F., Mailloux, J., Mantsinen, M. J., Maslov, M., Matthews, G., Mcclements, K. G., Meigs, A. G., Menmuir, S., Milocco, A., Miron, I. G., Moradi, S., Morales, R. B., Nowak, S., Orsitto, F., Patel, A., Piron, L., Prince, C., Pucella, G., Peluso, E., von Thun, C. Perez, Rachlew, E., Reux, C., Rimini, F., Saarelma, S., Schneider, P. A., Scully, S., Sertoli, M., Sharapov, S., Shaw, A., Silburn, S., Sips, A., Siren, P., Sozzi, C., Solano, E. R., Stancar, Z., Stankunas, G., Stuart, C., Sun, H. J., Szepesi, G., Valcarcel, D., Valisa, M., Verdoolaege, G., Viola, B., Wendler, N., Zerbini, M., Hobirk, J., Challis, C. D., Kappatou, A., Lerche, E., Keeling, D., King, D., Aleiferis, S., Alessi, E., Angioni, C., Auriemma, F., Baruzzo, M., Belonohy, E., Bernardo, J., Boboc, A., Carvalho, I. S., Carvalho, P., Casson, F. J., Chomiczewska, A., Citrin, J., Coffey, I. H., Conway, N. J., Douai, D., Delabie, E., Eriksson, Benjamin, Eriksson, Jacob, Ficker, O., Field, A. R., Fontana, M., Fontdecaba, J. M., Frassinetti, L., Frigione, D., Gallart, D., Garcia, J., Gelfusa, M., Ghani, Z., Giacomelli, L., Giovannozzi, E., Giroud, C., Goniche, M., Gromelski, W., Hacquin, S., Ham, C., Hawkes, N. C., Henriques, R. B., Hillesheim, J. C., Ho, A., Horvath, L., Ivanova-Stanik, I., Jacquet, P., Jaulmes, F., Joffrin, E., Kim, H. T., Kiptily, V., Kirov, K., Kos, D., Kowalska-Strzeciwilk, E., Kumpulainen, H., Lawson, K., Lennholm, M., Litaudon, X., Litherland-Smith, E., Lomas, P. J., de la Luna, E., Maggi, C. F., Mailloux, J., Mantsinen, M. J., Maslov, M., Matthews, G., Mcclements, K. G., Meigs, A. G., Menmuir, S., Milocco, A., Miron, I. G., Moradi, S., Morales, R. B., Nowak, S., Orsitto, F., Patel, A., Piron, L., Prince, C., Pucella, G., Peluso, E., von Thun, C. Perez, Rachlew, E., Reux, C., Rimini, F., Saarelma, S., Schneider, P. A., Scully, S., Sertoli, M., Sharapov, S., Shaw, A., Silburn, S., Sips, A., Siren, P., Sozzi, C., Solano, E. R., Stancar, Z., Stankunas, G., Stuart, C., Sun, H. J., Szepesi, G., Valcarcel, D., Valisa, M., Verdoolaege, G., Viola, B., Wendler, N., and Zerbini, M.
- Abstract
The JET hybrid scenario has been developed from low plasma current carbon wall discharges to the record-breaking Deuterium-Tritium plasmas obtained in 2021 with the ITER-like Be/W wall. The development started in pure Deuterium with refinement of the plasma current, and toroidal magnetic field choices and succeeded in solving the heat load challenges arising from 37 MW of injected power in the ITER like wall environment, keeping the radiation in the edge and core controlled, avoiding MHD instabilities and reaching high neutron rates. The Deuterium hybrid plasmas have been re-run in Tritium and methods have been found to keep the radiation controlled but not at high fusion performance probably due to time constraints. For the first time this scenario has been run in Deuterium-Tritium (50:50). These plasmas were re-optimised to have a radiation-stable H-mode entry phase, good impurity control through edge Ti gradient screening and optimised performance with fusion power exceeding 10 MW for longer than three alpha particle slow down times, 8.3 MW averaged over 5 s and fusion energy of 45.8 MJ.
- Published
- 2023
- Full Text
- View/download PDF
39. JET D-T scenario with optimized non-thermal fusion
- Author
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Maslov, M., Lerche, E., Auriemma, F., Belli, E., Bourdelle, C., Challis, C. D., Chomiczewska, A., Dal Molin, A., Eriksson, Jacob, Garcia, J., Hobirk, J., Ivanova-Stanik, I., Jacquet, Ph., Kappatou, A., Kazakov, Y., Keeling, D. L., King, D. B., Kiptily, V., Kirov, K., Kos, D., Lorenzini, R., de la Luna, E., Maggi, C. F., Mailloux, J., Mantica, P., Marin, M., Matthews, G., Monakhov, I., Nocente, M., Pucella, G., Rigamonti, D., Rimini, F., Saarelma, S., Salewski, M., Solano, E. R., Stancar, Z., Stankunas, G., Sun, H., Tardocchi, M., Van Eester, D., Maslov, M., Lerche, E., Auriemma, F., Belli, E., Bourdelle, C., Challis, C. D., Chomiczewska, A., Dal Molin, A., Eriksson, Jacob, Garcia, J., Hobirk, J., Ivanova-Stanik, I., Jacquet, Ph., Kappatou, A., Kazakov, Y., Keeling, D. L., King, D. B., Kiptily, V., Kirov, K., Kos, D., Lorenzini, R., de la Luna, E., Maggi, C. F., Mailloux, J., Mantica, P., Marin, M., Matthews, G., Monakhov, I., Nocente, M., Pucella, G., Rigamonti, D., Rimini, F., Saarelma, S., Salewski, M., Solano, E. R., Stancar, Z., Stankunas, G., Sun, H., Tardocchi, M., and Van Eester, D.
- Abstract
In JET deuterium-tritium (D-T) plasmas, the fusion power is produced through thermonuclear reactions and reactions between thermal ions and fast particles generated by neutral beam injection (NBI) heating or accelerated by electromagnetic wave heating in the ion cyclotron range of frequencies (ICRFs). To complement the experiments with 50/50 D/T mixtures maximizing thermonuclear reactivity, a scenario with dominant non-thermal reactivity has been developed and successfully demonstrated during the second JET deuterium-tritium campaign DTE2, as it was predicted to generate the highest fusion power in JET with a Be/W wall. It was performed in a 15/85 D/T mixture with pure D-NBI heating combined with ICRF heating at the fundamental deuterium resonance. In steady plasma conditions, a record 59 MJ of fusion energy has been achieved in a single pulse, of which 50.5 MJ were produced in a 5 s time window (P fus = 10.1 MW) with average Q = 0.33, confirming predictive modelling in preparation of the experiment. The highest fusion power in these experiments, P fus = 12.5 MW with average Q = 0.38, was achieved over a shorter 2 s time window, with the period of sustainment limited by high-Z impurity accumulation. This scenario provides unique data for the validation of physics-based models used to predict D-T fusion power.
- Published
- 2023
- Full Text
- View/download PDF
40. JET D-T scenario with optimized non-thermal fusion
- Author
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Maslov, M, Lerche, E, Auriemma, F, Belli, E, Bourdelle, C, Challis, C, Chomiczewska, A, Dal Molin, A, Eriksson, J, Garcia, J, Hobirk, J, Ivanova-Stanik, I, Jacquet, P, Kappatou, A, Kazakov, Y, Keeling, D, King, D, Kiptily, V, Kirov, K, Kos, D, Lorenzini, R, de la Luna, E, Maggi, C, Mailloux, J, Mantica, P, Marin, M, Matthews, G, Monakhov, I, Nocente, M, Pucella, G, Rigamonti, D, Rimini, F, Saarelma, S, Salewski, M, Solano, E, Stancar, Z, Stankunas, G, Sun, H, Tardocchi, M, Van Eester, D, Challis, CD, Keeling, DL, King, DB, Maggi, CF, Solano, ER, Maslov, M, Lerche, E, Auriemma, F, Belli, E, Bourdelle, C, Challis, C, Chomiczewska, A, Dal Molin, A, Eriksson, J, Garcia, J, Hobirk, J, Ivanova-Stanik, I, Jacquet, P, Kappatou, A, Kazakov, Y, Keeling, D, King, D, Kiptily, V, Kirov, K, Kos, D, Lorenzini, R, de la Luna, E, Maggi, C, Mailloux, J, Mantica, P, Marin, M, Matthews, G, Monakhov, I, Nocente, M, Pucella, G, Rigamonti, D, Rimini, F, Saarelma, S, Salewski, M, Solano, E, Stancar, Z, Stankunas, G, Sun, H, Tardocchi, M, Van Eester, D, Challis, CD, Keeling, DL, King, DB, Maggi, CF, and Solano, ER
- Abstract
In JET deuterium-tritium (D-T) plasmas, the fusion power is produced through thermonuclear reactions and reactions between thermal ions and fast particles generated by neutral beam injection (NBI) heating or accelerated by electromagnetic wave heating in the ion cyclotron range of frequencies (ICRFs). To complement the experiments with 50/50 D/T mixtures maximizing thermonuclear reactivity, a scenario with dominant non-thermal reactivity has been developed and successfully demonstrated during the second JET deuterium-tritium campaign DTE2, as it was predicted to generate the highest fusion power in JET with a Be/W wall. It was performed in a 15/85 D/T mixture with pure D-NBI heating combined with ICRF heating at the fundamental deuterium resonance. In steady plasma conditions, a record 59 MJ of fusion energy has been achieved in a single pulse, of which 50.5 MJ were produced in a 5 s time window (P fus = 10.1 MW) with average Q = 0.33, confirming predictive modelling in preparation of the experiment. The highest fusion power in these experiments, P fus = 12.5 MW with average Q = 0.38, was achieved over a shorter 2 s time window, with the period of sustainment limited by high-Z impurity accumulation. This scenario provides unique data for the validation of physics-based models used to predict D-T fusion power.
- Published
- 2023
41. L-H transition studies in tritium and deuterium-tritium campaigns at JET with Be wall and W divertor
- Author
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Solano, E., Birkenmeier, G., Silva, C., Delabie, E., Hillesheim, J., Baciero, A., Balboa, I., Baruzzo, M., Boboc, A., Brix, M., Bernardo, J., Bourdelle, C., Carvalho, I., Carvalho, P., Challis, C., Chernyshova, M., Chomiczewska, A., Coelho, R., Coffey, I., Craciunescu, T., de la Cal, E., de la Luna, E., Dumont, R., Dumortier, P., Fontana, M., Fontdecaba, J., Frassinetti, L., Gallart, D., Garcia, J., Giroud, C., Gromelski, W., Henriques, R., Hall, J., Ho, A., Horton, L.D., Horvath, L., Jacquet, P., Jepu, I., Joffrin, E., Kappatou, A., Keeling, D., King, D., Kiptily, V., Kirov, K., Kos, D., Kowalska-Strzęciwilk, E., Lennholm, M., Lerche, E., Litherland-Smith, E., Loarte, A., Lomanowski, B., Lomas, P.J., Maggi, C.F., Mailloux, J., Mantsinen, M.J., Maslov, M., Meigs, A.G., Monakhov, I., Morales, R.B., Nielsen, Anders Henry, Nina, D., Noble, C., Pawelec, E., Poradzinski, M., Pucella, Gianluca, Puglia, P., Réfy, D., Rasmussen, Jens Juul, Righi, E., Rimini, F.G., Robinson, T., Sertoli, M., Silburn, S. A., Sips, G., Sirén, P., Štancar, Žiga, Sun, H. J., Szepesi, G., Taylor, D., Tholerus, E., Thomas, Beth, Verdoolaege, G., Vincenzi, P., Viola, Bruno, Vianello, N, Wilson, Thomas, Solano, E., Birkenmeier, G., Silva, C., Delabie, E., Hillesheim, J., Baciero, A., Balboa, I., Baruzzo, M., Boboc, A., Brix, M., Bernardo, J., Bourdelle, C., Carvalho, I., Carvalho, P., Challis, C., Chernyshova, M., Chomiczewska, A., Coelho, R., Coffey, I., Craciunescu, T., de la Cal, E., de la Luna, E., Dumont, R., Dumortier, P., Fontana, M., Fontdecaba, J., Frassinetti, L., Gallart, D., Garcia, J., Giroud, C., Gromelski, W., Henriques, R., Hall, J., Ho, A., Horton, L.D., Horvath, L., Jacquet, P., Jepu, I., Joffrin, E., Kappatou, A., Keeling, D., King, D., Kiptily, V., Kirov, K., Kos, D., Kowalska-Strzęciwilk, E., Lennholm, M., Lerche, E., Litherland-Smith, E., Loarte, A., Lomanowski, B., Lomas, P.J., Maggi, C.F., Mailloux, J., Mantsinen, M.J., Maslov, M., Meigs, A.G., Monakhov, I., Morales, R.B., Nielsen, Anders Henry, Nina, D., Noble, C., Pawelec, E., Poradzinski, M., Pucella, Gianluca, Puglia, P., Réfy, D., Rasmussen, Jens Juul, Righi, E., Rimini, F.G., Robinson, T., Sertoli, M., Silburn, S. A., Sips, G., Sirén, P., Štancar, Žiga, Sun, H. J., Szepesi, G., Taylor, D., Tholerus, E., Thomas, Beth, Verdoolaege, G., Vincenzi, P., Viola, Bruno, Vianello, N, and Wilson, Thomas
- Abstract
The recent deuterium-tritium campaign in JET-ILW (DTE2) has provided a unique opportunity to study the isotope dependence of the L-H power threshold in an ITER-like wall environment (Be wall and W divertor). Here we present results from dedicated L-H transition experiments at JET-ILW, documenting the power threshold in tritium and deuterium-tritium plasmas, comparing them with the matching deuterium and hydrogen datasets. From earlier experiments in JET-ILW it is known that as plasma isotopic composition changes from deuterium, through varying deuterium/hydrogen concentrations, to pure hydrogen, the value of the line averaged density at which the threshold is minimum, n̄e,min, increases, leading us to expect that n̄e,min(T) < n̄e,min(DT) < n̄e,min(D) < n̄e,min(H). The new power threshold data confirms these expectations in most cases, with the corresponding ordering of the minimum power thresholds. We present a comparison of this data to power threshold scalings, used for extrapolation to future devices such as ITER and DEMO.
- Published
- 2023
42. Towards Rational Biosurfactant Design—Predicting Solubilization in Rhamnolipid Solutions
- Author
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Ilona E. Kłosowska-Chomiczewska, Adrianna Kotewicz-Siudowska, Wojciech Artichowicz, Adam Macierzanka, Agnieszka Głowacz-Różyńska, Patrycja Szumała, Krystyna Mędrzycka, Elżbieta Hallmann, Elena Karpenko, and Christian Jungnickel
- Subjects
rhamnolipid ,biosurfactant ,micellar solubilization ,efficiency ,MSR ,QSAR ,Organic chemistry ,QD241-441 - Abstract
The efficiency of micellar solubilization is dictated inter alia by the properties of the solubilizate, the type of surfactant, and environmental conditions of the process. We, therefore, hypothesized that using the descriptors of the aforementioned features we can predict the solubilization efficiency, expressed as molar solubilization ratio (MSR). In other words, we aimed at creating a model to find the optimal surfactant and environmental conditions in order to solubilize the substance of interest (oil, drug, etc.). We focused specifically on the solubilization in biosurfactant solutions. We collected data from literature covering the last 38 years and supplemented them with our experimental data for different biosurfactant preparations. Evolutionary algorithm (EA) and kernel support vector machines (KSVM) were used to create predictive relationships. The descriptors of biosurfactant (logPBS, measure of purity), solubilizate (logPsol, molecular volume), and descriptors of conditions of the measurement (T and pH) were used for modelling. We have shown that the MSR can be successfully predicted using EAs, with a mean R2val of 0.773 ± 0.052. The parameters influencing the solubilization efficiency were ranked upon their significance. This represents the first attempt in literature to predict the MSR with the MSR calculator delivered as a result of our research.
- Published
- 2021
- Full Text
- View/download PDF
43. Fundamental ICRF heating of deuterium ions in JET-DTE2.
- Author
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Lerche, E., Maslov, M., Jacquet, Ph., Monakhov, I., King, D., Keeling, D., Challis, C. D., Eester, D. Van, Mantica, P., Maggi, C., Garcia, J., Auriemma, F., Coelho, R., Coffey, I., Chomiczewska, A., Delabie, E., Dumont, R., Dumortier, P., Eriksson, J., and Ferreira, J.
- Subjects
DEUTERIUM ions ,HEATING ,FAST ions ,ION energy ,ION temperature ,TRITIUM - Abstract
Beam-target reactions are responsible for a substantial fraction of the fusion power generated in D-T plasmas in JET-ILW (Be/W-wall), with ion temperatures of 10-12keV and large neutral-beam injection (NBI) power. It is known that injecting D beam ions with energies of ∼100-150keV in T-rich plasmas has a larger potential for beam-target fusion than in 50:50 D:T plasmas, but such a scenario was never developed in the past D-T experiments performed in JET-C (Carbon-wall) and in TFTR in the 90's. On top of the intrinsic advantages of using D beams in T-rich plasmas for D-T neutron production, simulations have shown that fundamental ion-cyclotron resonance heating (ICRH) of the D ions can significantly boost the net fusion reactivity, since both the thermalized D ions and the fast D-NBI ions are accelerated to energy ranges that are optimal for the D-T reaction cross-section. The beneficial effect of fundamental D ICRH on thermal D minorities in tritium plasmas (without NBI) was identified in the JET-C D-T experiments, but was not tested in high performance H-mode discharges with D-NBI heating. In 2021, dedicated JET-ILW DTE2 [1] experiments confirmed - for the first time - the improved fusion performance of T-rich plasmas with high D-NBI power and highlighted the key impact of fundamental D ICRH on the fusion reactivity. This new scenario lead to the world-wide 5s averaged fusion power (and energy) record in D-T tokamak plasmas with dominant beam-target reactions. A brief experimental overview followed by detailed RF wave / Fokker-Planck simulations including NBI-ICRH synergy will be presented, to disentangle the different components contributing to the high neutron yield achieved in these experiments. [ABSTRACT FROM AUTHOR]
- Published
- 2023
- Full Text
- View/download PDF
44. RF power as key contributor to high performance "baseline" scenario experiments in JET DD and DT plasmas in preparation for ITER.
- Author
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Eester, D. Van, Frigione, D., Garzotti, L., Lomas, P., Lowry, C., Rimini, F., Aleiferis, S., Alessi, A., Auriemma, F., Baruzzo, M., Boboc, A., Carvalho, I., Chomiczewska, A., Luna, E. de la, Dreval, M., Ferreira, D., Ferreira, J., Field, A. R., Frassinetti, L., and Garcia, J.
- Subjects
DEUTERIUM plasma ,PLASMA currents ,PLASMA density ,TOROIDAL plasma ,RADIO frequency ,FAST ions ,INERTIAL confinement fusion - Abstract
Experimental studies of Deuterium and Tritium plasmas have been carried out at JET in the last years, yielding precious information for the next generation of fusion devices. Among the various approaches taken, JET's "Baseline" scenario experiments are pushing the machine towards its engineering limits by operating in a high-confinement H-mode at high toroidal field, plasma current and fuel density, as planned for ITER. The present paper provides a brief sketch of the Baseline scenario philosophy and discusses a number of RF-related results obtained in the preparation of the DT campaign as well as its preparations. Fusion powers of almost 9MW and energies of 12MJ have been reached in DT "Baseline" scenario plasmas. The differing role of radio frequency and beam heating is highlighted, the former allowing peaked core temperature profiles instrumental e.g. for core high-Z impurity chasing and the "landing" of high performance discharges while the latter is the main overall heating source in JET. Synergistic effects from the simultaneous use of wave and beam heating are responsible for a modest but noticeable increase in fusion power. One of the differences between D and DT plasmas is the plasma density, which impacts on the beam deposition as well as fast ion generation. [ABSTRACT FROM AUTHOR]
- Published
- 2023
- Full Text
- View/download PDF
45. Role of NBI fuelling in contributing to density peaking between the ICRH and NBI identity plasmas on JET
- Author
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T. Tala, F. Eriksson, P. Mantica, A. Mariani, A. Salmi, E.R. Solano, I.S. Carvalho, A. Chomiczewska, E. Delabie, J. Ferreira, E. Fransson, L. Horvath, P. Jacquet, D. King, A. Kirjasuo, S. Leerink, E. Lerche, C. Maggi, M. Marin, M. Maslov, S. Menmuir, R.B. Morales, V. Naulin, M.F.F. Nave, H. Nordman, C. Perez von Thun, P.A. Schneider, M. Sertoli, K. Tanaka, JET Contributors, VTT Technical Research Centre of Finland, JET, CNR-ENEA-EURATOM Association, University of Milan - Bicocca, CIEMAT, University of Lisbon, IPPLM, Chalmers University of Technology, Department of Applied Physics, Royal Military Academy, Dutch Institute for Fundamental Energy Research, Technical University of Denmark, Max-Planck-Institut für Plasmaphysik, Tokamak Energy Ltd, National Institute for Fusion Science, Aalto-yliopisto, Aalto University, Tala, T, Eriksson, F, Mantica, P, Mariani, A, Salmi, A, Solano, E, Carvalho, I, Chomiczewska, A, Delabie, E, Ferreira, J, Fransson, E, Horvath, L, Jacquet, P, King, D, Kirjasuo, A, Leerink, S, Lerche, E, Maggi, C, Marin, M, Maslov, M, Menmuir, S, Morales, R, Naulin, V, Nave, M, Nordman, H, Perez Von Thun, C, Schneider, P, Sertoli, M, Tanaka, K, Contributors, J, and JET Contributors
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Nuclear and High Energy Physics ,Other Physics Topics ,dimensioness identity plasma ,particle transport ,NBI fuelling ,particle transport modelling ,Energy Engineering ,Condensed Matter Physics ,Fusion, Plasma and Space Physics ,density peaking - Abstract
Density peaking has been studied between an ICRH and NBI identity plasma in JET. The comparison shows that 8 MW of NBI heating/fueling increases the density peaking by a factor of two, being R/L n = 0.45 for the ICRH pulse and R/L n = 0.93 for the NBI one averaged radially over ρ tor = 0.4, 0.8. The dimensionless profiles of q, ρ *, υ *, β n and T i/T e ≈ 1 were matched within 5% difference except in the central part of the plasma (ρ tor < 0.3). The difference in the curvature pinch (same q-profile) and thermo-pinch (T i = T e) between the ICRH and NBI discharges is virtually zero. Both the gyro-kinetic simulations and integrated modelling strongly support the experimental result where the NBI fuelling is the main contributor to the density peaking for this identity pair. It is to be noted here that the integrated modeling does not reproduce the measured electron density profiles, but approximately reproduces the difference in the density profiles between the ICRH and NBI discharge. Based on these modelling results and the analyses, the differences between the two pulses in impurities, fast ions (FIs), toroidal rotation and radiation do not cause any such changes in the background transport that would invalidate the experimental result where the NBI fuelling is the main contributor to the density peaking. This result of R/L n increasing by a factor of 2 per 8 MW of NBI power is valid for the ion temperature gradient dominated low power H-mode plasmas. However, some of the physics processes influencing particle transport, like rotation, turbulence and FI content scale with power, and therefore, the simple scaling on the role of the NBI fuelling in JET is not necessarily the same under higher power conditions or in larger devices.
- Published
- 2022
46. Isotope mass scaling and transport comparison between JET Deuterium and Tritium L-mode plasmas.
- Author
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Tala, T., Järvinen, A.E., Maggi, C.F., Mantica, P., Mariani, A., Salmi, A., Carvalho, I.S., Chomiczewska, A., Delabie, E., Devasagayam, F., Ferreira, J., Gromelski, W., Hawkes, N., Horvath, L., Karhunen, J., King, D., Kirjasuo, A., Kowalska-Strzeciwilk, E., Leerink, S., and Lennholm, M.
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TRITIUM ,DEUTERIUM ,ISOTOPES ,PARTICLE analysis ,PLASMA boundary layers ,PLASMA confinement ,DIFFUSION coefficients - Abstract
The dimensionless isotope mass scaling experiment between pure Deuterium and pure Tritium plasmas with matched ρ ∗ , ν ∗ , β
n , q and T e / T i has been achieved in JET L-mode with dominant electron heating (NBI+ohmic) conditions. 28% higher scaled energy confinement time B t τ E , t h / A is found in favour of the Tritium plasma. This can be cast in the form of the dimensionless energy confinement scaling law as Ω i τ E , t h ∼ A 0.48 ± 0.16 . This significant isotope mass scaling is consequently seen in the scaled one-fluid heat diffusion coefficient A χ e f f / B t which is around 50% lower in the Tritium plasma throughout the whole plasma radius. The isotope mass dependence in the particle transport channel is negligible, supported also by the perturbative particle transport analysis with gas puff modulation. The comparison of the edge particle fuelling or ionisation profiles from the EDGE2D-EIRENE simulations show that the absolute density differences that are necessary for the dimensionless match in the confined plasma dominate over any isotope mass dependencies of particle fuelling and ionization profiles at the plasma edge. Local GENE simulation results indicate a mild anti-gyroBohm effect at ρ t o r = 0.6 and thereby a small isotope mass dependence in favour of Tritium on heat transport and a negligible effect on particle transport. A significant fraction of the isotope scaling and reduced heat transport observed in the Tritium plasma is not captured in the GENE and ASTRA-TGLF-SAT2 simulations by simply changing the isotope mass for the same input profiles. [ABSTRACT FROM AUTHOR]- Published
- 2023
- Full Text
- View/download PDF
47. L-H transition studies in tritium and deuterium–tritium campaigns at JET with Be wall and W divertor.
- Author
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Solano, E.R., Birkenmeier, G., Silva, C., Delabie, E., Hillesheim, J.C., Baciero, A., Balboa, I., Baruzzo, M., Boboc, A., Brix, M., Bernardo, J., Bourdelle, C., Carvalho, I.S., Carvalho, P., Challis, C.D., Chernyshova, M., Chomiczewska, A., Coelho, R., Coffey, I., and Craciunescu, T.
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TRITIUM ,DEUTERIUM ,HYDROGEN ,ISOTOPES ,EXTRAPOLATION ,TOKAMAKS ,DENSITY - Abstract
The recent deuterium–tritium campaign in JET-ILW (DTE2) has provided a unique opportunity to study the isotope dependence of the L-H power threshold in an ITER-like wall environment (Be wall and W divertor). Here we present results from dedicated L-H transition experiments at JET-ILW, documenting the power threshold in tritium and deuterium–tritium plasmas, comparing them with the matching deuterium and hydrogen datasets. From earlier experiments in JET-ILW it is known that as plasma isotopic composition changes from deuterium, through varying deuterium/hydrogen concentrations, to pure hydrogen, the value of the line averaged density at which the threshold is minimum, n ˉ e , min , increases, leading us to expect that n ˉ e , min (T) < n ˉ e , min (DT) < n ˉ e , min (D) < n ˉ e , min (H). The new power threshold data confirms these expectations in most cases, with the corresponding ordering of the minimum power thresholds. We present a comparison of this data to power threshold scalings, used for extrapolation to future devices such as ITER and DEMO. [ABSTRACT FROM AUTHOR]
- Published
- 2023
- Full Text
- View/download PDF
48. Isotope physics of heat and particle transport with tritium in JET-ILW type-I ELMy H-mode plasmas.
- Author
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Schneider, P.A., Angioni, C., Auriemma, F., Bonanomi, N., Görler, T., Henriques, R., Horvath, L., King, D., Lorenzini, R., Nyström, H., Maslov, M., Ruiz, J., Szepesi, G., Challis, C.D., Chomiczewska, A., Delabie, E., Fontdecaba, J.M., Frassinetti, L., Garcia, J., and Giroud, C.
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PARTICLE physics ,ISOTOPES ,PLASMA currents ,HEAT flux ,PEDESTALS ,TRITIUM ,PLASMA confinement - Abstract
As part the DTE2 campaign in the JET tokamak, we conducted a parameter scan in T and D-T complementing existing pulses in H and D. For the different main ion masses, type-I ELMy H-modes at fixed plasma current and magnetic field can have the pedestal pressure varying by a factor of 4 and the total pressure changing from β N = 1.0 to 3.0. We investigated the pedestal and core isotope mass dependencies using this extensive data set. The pedestal shows a strong mass dependence on the density, which influences the core due to the strong coupling between both plasma regions. To better understand the causes for the observed isotope mass dependence in the pedestal, we analysed the interplay between heat and particle transport and the edge localised mode (ELM) stability. For this purpose, we developed a dynamic ELM cycle model with basic transport assumptions and a realistic neutral penetration. The temporal evolution and resulting ELM frequency introduce an additional experimental constraint that conventional quasi-stationary transport analysis cannot provide. Our model shows that a mass dependence in the ELM stability or in the transport alone cannot explain the observations. One requires a mass dependence in the ELM stability as well as one in the particle sources. The core confinement time increases with pedestal pressure for all isotope masses due to profile stiffness and electromagnetic turbulence stabilisation. Interestingly, T and D-T plasmas show an improved core confinement time compared to H and D plasmas even for matched pedestal pressures. For T, this improvement is largely due to the unique pedestal composition of higher densities and lower temperatures than H and D. With a reduced gyroBohm factor at lower temperatures, more turbulent drive in the form of steeper gradients is required to transport the same amount of heat. This picture is supported by quasilinear flux-driven modelling using TGLF -SAT2 within Astra. With the experimental boundary condition TGLF -SAT2 predicts the core profiles well for gyroBohm heat fluxes > 15 , however, overestimates the heat and particle transport closer to the turbulent threshold. [ABSTRACT FROM AUTHOR]
- Published
- 2023
- Full Text
- View/download PDF
49. Effect of the isotope mass on pedestal structure, transport and stability in D, D/T and T plasmas at similar β N and gas rate in JET-ILW type I ELMy H-modes.
- Author
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Frassinetti, L., Perez von Thun, C., Chapman-Oplopoiou, B., Nyström, H., Poradzinski, M., Hillesheim, J.C., Horvath, L., Maggi, C.F., Saarelma, S., Stagni, A., Szepesi, G., Bleasdale, A., Chomiczewska, A., Morales, R.B., Brix, M., Carvalho, P., Dunai, D., Field, A.R., Fontdecaba, J.M., and Sun, H.J.
- Subjects
TRITIUM ,PEDESTALS ,DEUTERIUM plasma ,LARMOR radius ,ISOTOPES ,DEUTERIUM - Abstract
The work describes the pedestal structure, transport and stability in an effective mass (A
eff ) scan from pure deuterium to pure tritium plasmas using a type I ELMy H-mode dataset in which key parameters that affect the pedestal behaviour (normalized pressure, ratio of the separatrix density to the pedestal density, pedestal ion Larmor radius, pedestal collisionality and rotation) are kept as constant as possible. Experimental results show a significant increase of the density at the pedestal top with increasing Aeff , a modest reduction in the temperature and an increase in the pressure. The variations in the pedestal heights are mainly due to a change in the pedestal gradients while only small differences are observed in the pedestal width. A clear increase in the pedestal density and pressure gradients are observed from deuterium to tritium. The experimental results suggest a reduction of the pedestal inter-edge localized mode (inter-ELM) transport from deuterium to tritium. The reduction is likely in the pedestal inter-ELM particle transport, as suggested by the clear increase of the pedestal density gradients. The experimental results suggest also a possible reduction of the pedestal inter-ELM heat transport, however, the large experimental uncertainties do not allow conclusive claims on the heat diffusivity. The clear experimental reduction of ηe (the ratio between density and temperature gradient lengths) in the middle/top of the pedestal with increasing Aeff suggests that there may be a link between increasing Aeff and the reduction of electron scale turbulent transport. From the modelling point of view, an initial characterization of the behaviour of pedestal microinstabilities shows that the tritium plasma is characterized by growth rates lower than the deuterium plasmas. The pedestal stability of peeling-ballooning modes is assessed with both ideal and resistive magnetohydrodynamics (MHD). No significant effect of the isotope mass on the pedestal stability is observed using ideal MHD. Instead, resistive MHD shows a clear increase of the stability with increasing isotope mass. The resistive MHD results are in reasonable agreement with the experimental results of the normalized pedestal pressure gradient. The experimental and modelling results suggest that the main candidates to explain the change in the pedestal are a reduction in the inter-ELM transport and an improvement of the pedestal stability from deuterium to tritium. [ABSTRACT FROM AUTHOR]- Published
- 2023
- Full Text
- View/download PDF
50. Preservatives as important etiologic factors of allergic contact dermatitis
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Beata Kręcisz, Dorota Chomiczewska-Skóra, and Marta Kieć-Świerczyńska
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methylisothiazolinone ,allergic contact dermatitis ,preservatives ,patch tests ,occupational dermatitis ,Public aspects of medicine ,RA1-1270 - Abstract
Background: Preservatives present in cosmetics and other industrial products can cause allergic contact dermatitis. The aim of the study was to assess the frequency of allergy to selected preservatives in consecutive patients examined due to contact dermatitis in the Nofer Institute of Occupational Medicine, Łódź, and to establish whether individuals sensitized to formaldehyde react simultaneously to formaldehyde releasers. Material and Methods: A group of 405 patients (308 females and 97 males) was examined in 2011–2013. In all participants patch tests with a series of 13 preservatives (paraben mix, formaldehyde, Quaternium 15, chloromethylisothiazolinone/methylisothiazolinone mix, methyldibromoglutaronitrile, diazolidinyl urea, imidazolidinyl urea, DMDM hydantoin, 2-bromo-2-nitropropane-1,3-diol, iodopropynyl butylcarbamate, benzalkonium chloride, sodium metabisulfite, produced by Chemotechnique Diagnostics, Sweden) were performed. Results: Of the 405 patients 74 (including 52 females) showed positive results of patch tests. Contact allergy to at least 1 preservative was noted in 47 (11.6%) patients, including 34 (11%) females and 13 (13.4%) males. Methylisothiazolinone proved to be the most frequent sensitizer – 4.7% (5.2% females, 3.1% males) while parabens, 2-bromo-2-nitropropane-1,3-diol and imidazolidinyl urea (0.2%) were found to be the least frequent. Fourteen (3.4%) participants, 10 women and 4 men, were allergic to formaldehyde and/or formaldehyde releasers. In 11 (78.6%) of them monovalent hypersensitivity was observed. In 13 (3.2% of the examined group) patients allergy to preservatives might have been of occupational origin. Conclusions: Preservatives, particularly isothiazolinones, are significant causal factors of allergic contact dermatitis, including occupational cases. Individuals sensitized to formaldehyde may react simultaneously to formaldehyde releasers, however, such reactions are relatively rare. Med Pr 2015;66(3):327–332
- Published
- 2015
- Full Text
- View/download PDF
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