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240 results on '"Terry, J.L."'

19. Overview of the TCV tokamak experimental programme

Author

Reimerdes, H., primary, Agostini, M., additional, Alessi, E., additional, Alberti, S., additional, Andrebe, Y., additional, Arnichand, H., additional, Balbin, J., additional, Bagnato, F., additional, Baquero-Ruiz, M., additional, Bernert, M., additional, Bin, W., additional, Blanchard, P., additional, Blanken, T.C., additional, Boedo, J.A., additional, Brida, D., additional, Brunner, S., additional, Bogar, C., additional, Bogar, O., additional, Bolzonella, T., additional, Bombarda, F., additional, Bouquey, F., additional, Bowman, C., additional, Brunetti, D., additional, Buermans, J., additional, Bufferand, H., additional, Calacci, L., additional, Camenen, Y., additional, Carli, S., additional, Carnevale, D., additional, Carpanese, F., additional, Causa, F., additional, Cavalier, J., additional, Cavedon, M., additional, Cazabonne, J.A., additional, Cerovsky, J., additional, Chandra, R., additional, Chandrarajan Jayalekshmi, A., additional, Chellaï, O., additional, Chmielewski, P., additional, Choi, D., additional, Ciraolo, G., additional, Classen, I.G.J., additional, Coda, S., additional, Colandrea, C., additional, Dal Molin, A., additional, David, P., additional, de Baar, M.R., additional, Decker, J., additional, Dekeyser, W., additional, de Oliveira, H., additional, Douai, D., additional, Dreval, M., additional, Dunne, M.G., additional, Duval, B.P., additional, Elmore, S., additional, Embreus, O., additional, Eriksson, F., additional, Faitsch, M., additional, Falchetto, G., additional, Farnik, M., additional, Fasoli, A., additional, Fedorczak, N., additional, Felici, F., additional, Février, O., additional, Ficker, O., additional, Fil, A., additional, Fontana, M., additional, Fransson, E., additional, Frassinetti, L., additional, Furno, I., additional, Gahle, D.S., additional, Galassi, D., additional, Galazka, K., additional, Galperti, C., additional, Garavaglia, S., additional, Garcia-Munoz, M., additional, Geiger, B., additional, Giacomin, M., additional, Giruzzi, G., additional, Gobbin, M., additional, Golfinopoulos, T., additional, Goodman, T., additional, Gorno, S., additional, Granucci, G., additional, Graves, J.P., additional, Griener, M., additional, Gruca, M., additional, Gyergyek, T., additional, Haelterman, R., additional, Hakola, A., additional, Han, W., additional, Happel, T., additional, Harrer, G., additional, Harrison, J.R., additional, Henderson, S., additional, Hogeweij, G.M.D., additional, Hogge, J.-P., additional, Hoppe, M., additional, Horacek, J., additional, Huang, Z., additional, Iantchenko, A., additional, Innocente, P., additional, Insulander Björk, K., additional, Ionita-Schrittweiser, C., additional, Isliker, H., additional, Jardin, A., additional, Jaspers, R.J.E., additional, Karimov, R., additional, Karpushov, A.N., additional, Kazakov, Y., additional, Komm, M., additional, Kong, M., additional, Kovacic, J., additional, Krutkin, O., additional, Kudlacek, O., additional, Kumar, U., additional, Kwiatkowski, R., additional, Labit, B., additional, Laguardia, L., additional, Lammers, J.T., additional, Laribi, E., additional, Laszynska, E., additional, Lazaros, A., additional, Linder, O., additional, Linehan, B., additional, Lipschultz, B., additional, Llobet, X., additional, Loizu, J., additional, Lunt, T., additional, Macusova, E., additional, Marandet, Y., additional, Maraschek, M., additional, Marceca, G., additional, Marchetto, C., additional, Marchioni, S., additional, Marmar, E.S., additional, Martin, Y., additional, Martinelli, L., additional, Matos, F., additional, Maurizio, R., additional, Mayoral, M.-L., additional, Mazon, D., additional, Menkovski, V., additional, Merle, A., additional, Merlo, G., additional, Meyer, H., additional, Mikszuta-Michalik, K., additional, Molina Cabrera, P.A., additional, Morales, J., additional, Moret, J.-M., additional, Moro, A., additional, Moulton, D., additional, Muhammed, H., additional, Myatra, O., additional, Mykytchuk, D., additional, Napoli, F., additional, Nem, R.D., additional, Nielsen, A.H., additional, Nocente, M., additional, Nowak, S., additional, Offeddu, N., additional, Olsen, J., additional, Orsitto, F.P., additional, Pan, O., additional, Papp, G., additional, Pau, A., additional, Perek, A., additional, Pesamosca, F., additional, Peysson, Y., additional, Pigatto, L., additional, Piron, C., additional, Poradzinski, M., additional, Porte, L., additional, Pütterich, T., additional, Rabinski, M., additional, Raj, H., additional, Rasmussen, J.J., additional, Rattá, G.A., additional, Ravensbergen, T., additional, Ricci, D., additional, Ricci, P., additional, Rispoli, N., additional, Riva, F., additional, Rivero-Rodriguez, J.F., additional, Salewski, M., additional, Sauter, O., additional, Schmidt, B.S., additional, Schrittweiser, R., additional, Sharapov, S., additional, Sheikh, U.A., additional, Sieglin, B., additional, Silva, M., additional, Smolders, A., additional, Snicker, A., additional, Sozzi, C., additional, Spolaore, M., additional, Stagni, A., additional, Stipani, L., additional, Sun, G., additional, Tala, T., additional, Tamain, P., additional, Tanaka, K., additional, Tema Biwole, A., additional, Terranova, D., additional, Terry, J.L., additional, Testa, D., additional, Theiler, C., additional, Thornton, A., additional, Thrysøe, A., additional, Torreblanca, H., additional, Tsui, C.K., additional, Vaccaro, D., additional, Vallar, M., additional, van Berkel, M., additional, Van Eester, D., additional, van Kampen, R.J.R., additional, Van Mulders, S., additional, Verhaegh, K., additional, Verhaeghe, T., additional, Vianello, N., additional, Villone, F., additional, Viezzer, E., additional, Vincent, B., additional, Voitsekhovitch, I., additional, Vu, N.M.T., additional, Walkden, N., additional, Wauters, T., additional, Weisen, H., additional, Wendler, N., additional, Wensing, M., additional, Widmer, F., additional, Wiesen, S., additional, Wischmeier, M., additional, Wijkamp, T.A., additional, Wünderlich, D., additional, Wüthrich, C., additional, Yanovskiy, V., additional, Zebrowski, J., additional, and EUROfusion MST1 Team, the, additional

Published
2022
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20. Validation of 2D Te and ne measurements made with Helium imaging spectroscopy in the volume of the TCV divertor

Author

Linehan, B., Perek, A., Duval, B.P., Bagnato, F., Blanchard, P., Colandrea, C., de Oliveira, H., Février, O., Flom, E., Wijkamp, T., Gorno, S., Goto, M., Marmar, S., Martinelli, L., Mathews, A., Munoz-Burgos, J.M., Mykytchuk, D., Offeddu, N., Oliveira, D.S., Reimerdes, H., Reiter, D., Schmitz, O., Terry, J.L., Theiler, C., Tsui, C.K., Vincent, B., Wuthrich, C., Zholobenko, W., team, TCV, and TCV Team

Subjects
Nuclear and High Energy Physics, Condensed Matter Physics
Abstract

Multi-spectral imaging of helium atomic emission (HeMSI) has been used to create 2D poloidal maps of T e and n e in TCV’s divertor. To achieve these measurements, TCV’s MANTIS multispectral cameras (Perek et al 2019 Rev. Sci. Instrum. 90 123514) simultaneously imaged four He I lines (two singlet and two triplet) and a He II line (468 nm) from passively present He and He+. The images, which were absolutely calibrated and covered the whole divertor region, were inverted through the assumption of toroidal symmetry to create emissivity profiles and, consequently, line-ratio profiles. A collisional-radiative model (CRM) was applied to the line-ratio profiles to produce 2D poloidal maps of T e and n e . The collisional-radiative modeling was accomplished with the Goto helium CRM code (Zholobenko et al 2018 Nucl. Fusion 58 126006, Zholobenko et al 2018 Technical Report, Goto 2003 J. Quant. Spectrosc. Radiat. Transfer 76 331–44) which accounts for electron-impact excitation (EIE) and deexcitation, and electron–ion recombination (EIR) with He + . The HeMSI T e and n e measurements were compared with co-local Thomson scattering measurements. The two sets of measurements exhibited good agreement for ionizing plasmas: ( 5 eV ⩽ T e ⩽ 60 eV , and 2 × 10 18 m − 3 ⩽ n e ⩽ 3 × 10 19 m − 3 ) in the case of majority helium plasmas, and ( 10 eV ⩽ T e ⩽ 40 eV , 2 × 10 18 m − 3 ⩽ n e ⩽ 3 × 10 19 m − 3 ) in the case of majority deuterium plasmas. However, there were instances where HeMSI measurements diverged from Thomson scattering. When T e ⩽ 10 eV in majority deuterium plasmas, HeMSI deduced inaccurately high values of T e . This disagreement cannot be rectified within the CRM’s EIE and EIR framework. Second, on sporadic occasions within the private flux region, HeMSI produced erroneously high measurements of n e . Multi-spectral imaging of Helium emission has been demonstrated to produce accurate 2D poloidal maps of T e and n e within the divertor of a tokamak for plasma conditions relevant to contemporary divertor studies.

Published
2023
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22. Dynamics and dependencies of the configuration-dependent 1–2 kHz fluctuation in W7-X

Author

Ballinger, S.B., primary, Terry, J.L., additional, Baek, S.G., additional, Beurskens, M., additional, Brunner, K.J., additional, Fuchert, G., additional, Knauer, J., additional, Killer, C., additional, Pasch, E., additional, Rahbarnia, K., additional, Schilling, J., additional, Scott, E., additional, von Stechow, A., additional, Thomsen, H., additional, Grulke, O., additional, Wurden, G., additional, Kocsis, G., additional, Szepesi, T., additional, and Zsuga, L., additional

Published
2021
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29. I-mode pedestal relaxation events in the Alcator C-Mod and ASDEX Upgrade tokamaks.

Author

Silvagni, D., Terry, J.L., McCarthy, W., Hubbard, A.E., Eich, T., Faitsch, M., Gil, L., Golfinopoulos, T., Grenfell, G., Griener, M., Happel, T., Hughes, J.W., Stroth, U., Viezzer, E., the ASDEX Upgrade Team, and the EUROfusion MST1 Team

Subjects
*FUSION reactor divertors, *TOKAMAKS, *PEDESTALS, *FUSION reactors, *ENERGY dissipation, *ELECTRON temperature, *ENERGY futures
Abstract

In some conditions, I-mode plasmas can feature pedestal relaxation events (PREs) that transiently enhance the energy reaching the divertor target plates. To shed light on their appearance, characteristics and energy reaching the divertor targets, a comparative study between two tokamaks â€" Alcator C-Mod and ASDEX Upgrade â€" is carried out. It is found that PREs appear only in a subset of I-mode discharges, mainly when the plasma is close to the H-mode transition. Also, a growing oscillating precursor before the PRE onset is observed in the region close to the separatrix in both devices, and a discussion on a possible triggering mechanism is outlined. The PRE relative energy loss from the confined region is found to increase with decreasing pedestal top collisionality ν ped * . Similarly, also the relative electron temperature drop at the pedestal top, which is related to the conductive energy loss, rises with decreasing ν ped * . Based on these relations, the PRE relative energy loss in future devices such as DEMO and ARC is estimated. Finally, the divertor peak energy fluence due to the PRE is measured on each device. Those values are then compared to the model introduced in Eich et al (2017 Nucl. Mater. Energy 12 84â€"90) for type-I edge localized modes. The model is shown to provide an upper boundary for PRE energy fluence data, while a lower boundary is found by dividing the model by three. These two boundaries are used to make projections of the PRE divertor energy fluence to DEMO and ARC. [ABSTRACT FROM AUTHOR]

Published
2022
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35. Simulation of the SPARC plasma boundary with the UEDGE code.

Author

Ballinger, S.B., Kuang, A.Q., Umansky, M.V., Brunner, D., Canik, J.M., Greenwald, M., Lore, J.D, LaBombard, B., Terry, J.L., Wigram, M., and team, the SPARC

Subjects
SYMMETRY (Physics), HEAT flux, ION temperature, PLASMA boundary layers, ACTINIC flux, FUSION reactor divertors
Abstract

In this work, the UEDGE edge transport code is used to examine conditions in the SPARC divertor and edge plasma for various levels of carbon impurity and power from the core (PSOL). A double-null magnetic configuration is simulated assuming up-down symmetry in geometry and physics. The anomalous heat and particle transport coefficients are tuned to match empirical predictions for SPARC's midplane density profiles, target plate heat flux profiles, and inner/outer divertor power sharing. Convective transport is included on the low-field side, while on the high-field side the transport is modeled as purely diffusive. Hydrogen neutrals are modeled as a fluid with inertial effects, and a carbon impurity is included using the fixed-fraction model. We find that detachment induced by impurity seeding could significantly reduce the heat flux to the divertor surfaces in the SPARC tokamak. At PSOL = 28 MW (the value predicted for SPARC's full-power H-mode scenario) cases with both divertor legs detached were obtained with a carbon impurity fraction between 0.3%–1.4%, far below Zeff limits for SPARC. When the plasma in the outer leg is detached, the peak heat flux density perpendicular to the target plate is below 1 MW m−2, electron and ion temperatures are less than 1.5 eV, and momentum detachment is observed. However, the detachment state is found to be sensitive to the side-wall boundary conditions, the level of neutral pumping, and the target plate tilt. Finally, a broadly similar SOLPS simulation of SPARC is used to assess the appropriateness of the simpler impurity and neutral models used in UEDGE. [ABSTRACT FROM AUTHOR]

Published
2021
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50. Impurity screening behavior of the high-field side scrape-off layer in near-double-null configurations: prospect for mitigating plasma–material interactions on RF actuators and first-wall components

Author

LaBombard, B., primary, Kuang, A.Q., additional, Brunner, D., additional, Faust, I., additional, Mumgaard, R., additional, Reinke, M.L., additional, Terry, J.L., additional, Howard, N., additional, Hughes, J.W., additional, Chilenski, M., additional, Lin, Y., additional, Marmar, E., additional, Rice, J.E., additional, Rodriguez-Fernandez, P., additional, Wallace, G., additional, Whyte, D.G., additional, Wolfe, S., additional, and Wukitch, S., additional

Published
2017
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