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1. Isotope effects and Alfven eigenmode stability in JET H, D, T, DT, and He plasmas

Author: Tinguely, R. A., Puglia, P. G., Dowson, S., Porkolab, M., Douai, D., Fasoli, A., Frassinetti, L., King, D., Schneider, P., and Contributors, JET
Subjects: Physics - Plasma Physics
Abstract: While much about Alfven eigenmode (AE) stability has been explored in previous and current tokamaks, open questions remain for future burning plasma experiments, especially regarding exact stability threshold conditions and related isotope effects; the latter, of course, requiring good knowledge of the plasma ion composition. In the JET tokamak, eight in-vessel antennas actively excite stable AEs, from which their frequencies, toroidal mode numbers, and net damping rates are assessed. The effective ion mass can also be inferred using measurements of the plasma density and magnetic geometry. Thousands of AE stability measurements have been collected by the Alfven Eigenmode Active Diagnostic in hundreds of JET plasmas during the recent Hydrogen, Deuterium, Tritium, DT, and Helium-4 campaigns. In this novel AE stability database, spanning all four main ion species, damping is observed to decrease with increasing Hydrogenic mass, but increase for Helium, a trend consistent with radiative damping as the dominant damping mechanism. These data are important for confident predictions of AE stability in both non-nuclear (H/He) and nuclear (D/T) operations in future devices. In particular, if radiative damping plays a significant role in overall stability, some AEs could be more easily destabilized in D/T plasmas than their H/He reference pulses, even before considering fast ion and alpha particle drive. Active MHD spectroscopy is also employed on select HD, HT, and DT plasmas to infer the effective ion mass, thereby closing the loop on isotope analysis and demonstrating a complementary method to typical diagnosis of the isotope ratio.
Published: 2024

2. The JET hybrid H-mode scenario from a pedestal turbulence perspective

Author: Leppin, L. A., Görler, T., Frassinetti, L., Saarelma, S., Hobirk, J., Jenko, F., and contributors, JET
Subjects: Physics - Plasma Physics
Abstract: Turbulent transport is a decisive factor in determining the pedestal structure of H-modes. Here, we present the first comprehensive characterization of gyrokinetic turbulent transport in a JET hybrid H-mode pedestal. Local, linear simulations are performed to identify instabilities and global, nonlinear electromagnetic simulations reveal the turbulent heat and particle flux structure of the pedestal. Our analysis focuses on the Deuterium reference discharge \#97781 performed in the scenario development for the Deuterium-Tritium campaign. We find the pedestal top transport to be dominated by ion temperature gradient (ITG) modes. In the pedestal center turbulent ion transport is suppressed and electron transport is driven by multi-faceted electron temperature gradient (ETG) modes, which extend down to ion-gyroradius scales. A strong impact of $E\times B$ shear on the absolute turbulence level is confirmed by the global, nonlinear simulations. Furthermore, impurities are shown to reduce the main ion transport. Dedicated density and ion temperature profile variations test the sensitivity of the results and do not find strong differences in the turbulent transport in more reactor-like conditions.
Published: 2024

3. Developing Deep Learning Algorithms for Inferring Upstream Separatrix Density at JET

Author: Kit, A., Jaervinen, A., Wiesen, S., Poels, Y., and Frassinetti, L.
Subjects: Physics - Plasma Physics
Abstract: Predictive and real-time inference capability for the upstream separatrix electron density, $n_\text{e, sep}$, is essential for design and control of core-edge integrated plasma scenarios. In this study, both supervised and semi-supervised machine learning algorithms are explored to establish direct mapping as well as indirect compressed representation of the pedestal profiles for predictions and inference of $n_{\text{e, sep}}$. Based on the EUROfusion pedestal database for JET, a tabular dataset was created, consisting of machine parameters, fraction of ELM cycle, high resolution Thomson scattering profiles of electron density and temperature, and $n_{\text{e, sep}}$ for 608 JET shots. Using the tabular dataset, the direct mapping approach provides a mapping of machine parameters and ELM percentage to $n_{\text{e, sep}}$. Through representation learning, a compressed representation of the experimental pedestal electron density and temperature profiles is established. By conditioning the representation with machine control parameters, a probabilistic generative predictive model is established. For prediction, the machine parameters can be used to establish a conditional distribution of the compressed pedestal profiles, and the decoder that is trained as part of the algorithm can be used to decode the compressed representation back to full pedestal profiles. Although, in this work, a proof-of-principle for predicting and inferring $n_{\text{e, sep}}$ is given, such a representation learning can be used also for many other applications as the full pedestal profile is predicted. An implementation of this work can be found at https://github.com/fusionby2030/moxie., Comment: 6 pages, 5 figures, accepted contribution to the 25th International Conference on Plasma Surface Interaction in Controlled Fusion Devices(PSI-25)
Published: 2022
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4. Innovative dud detection based on JET DT experience

Author: Piron, L., Aleiferis, S., Garzotti, L., Sauter, O., Solano, E.R., Baruzzo, M., Cicioni, R., Van Eester, D., Frassinetti, L., Frigione, D., Lennholm, M., Lomas, P.J., Martin, P., Pau, A., Rimini, F., and Valcarcel, D.F.
Published: 2024
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5. Microtearing modes as the source of magnetic fluctuations in the JET pedestal

Author: Hatch, D. R., Kotschenreuther, M., Mahajan, S. M., Pueschel, M. J., Michoski, C., Merlo, G., Hassan, E., Field, A. R., Frassinetti, L., Giroud, C., Hillesheim, J. C., Maggi, C. F., von Thun, C. Perez, Roach, C. M., Saarelma, S., Jarema, D., Jenko, F., and contributors, JET
Subjects: Physics - Plasma Physics
Abstract: We report on a detailed study of magnetic fluctuations in the JET pedestal, employing basic theoretical considerations, gyrokinetic simulations, and experimental fluctuation data, to establish the physical basis for their origin, role, and distinctive characteristics. We demonstrate quantitative agreement between gyrokinetic simulations of microtearing modes (MTMs) and two magnetic frequency bands with corresponding toroidal mode numbers n=4 and 8. Such disparate fluctuation scales, with substantial gaps between toroidal mode numbers, are commonly observed in pedestal fluctuations. Here we provide a clear explanation, namely the alignment of the relevant rational surfaces (and not others) with the peak in the omega star profile, which is localized in the steep gradient region of the pedestal. We demonstrate that a global treatment is required to capture this effect. Nonlinear simulations suggest that the MTM fluctuations produce experimentally-relevant transport levels and saturate by relaxing the background electron temperature gradient, slightly downshifting the fluctuation frequencies from the linear predictions. Scans in collisionality are compared with simple MTM dispersion relations. At the experimental points considered, MTM growth rates can either increase or decrease with collision frequency depending on the parameters thus defying any simple characterization of collisionality dependence.
Published: 2020
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6. ELM and inter-ELM tungsten erosion sources in high-power, JET ITER-like wall H-mode plasmas

Author: Kumpulainen, H.A., Groth, M., Brezinsek, S., Corrigan, G., Frassinetti, L., Harting, D., Koechl, F., Karhunen, J., Meigs, A.G., O'Mullane, M., and Romazanov, J.
Published: 2022
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7. Improved accuracy and robustness of electron density profiles from JET’s X-mode frequency-modulated continuous-wave reflectometers

Author: Morales, R. B., primary, Salmi, A., additional, Abreu, P., additional, Amador, C. H. S., additional, Appel, L., additional, Carman, P., additional, Fessey, J., additional, Flanagan, J., additional, Fontana, M., additional, Frassinetti, L., additional, Giroud, C., additional, Hacquin, S., additional, Heuraux, S., additional, Meneses, L., additional, Ronchi, G., additional, Sabot, R., additional, Silva, A., additional, Sirinelli, A., additional, Szepesi, G., additional, Taylor, D., additional, and Terranova, D., additional
Published: 2024
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8. Local measurement of error field using naturally rotating tearing mode dynamics in EXTRAP T2R

Author: Sweeney, R. M., Frassinetti, L., Brunsell, P., Fridström, R., and Volpe, F. A.
Subjects: Physics - Plasma Physics, Nuclear Experiment
Abstract: An error field (EF) detection technique using the amplitude modulation of a naturally rotating tearing mode (TM) is developed and validated in the EXTRAP T2R reversed field pinch. The technique was used to identify intrinsic EFs of $m/n = 1/-12$, where $m$ and $n$ are the poloidal and toroidal mode numbers. The effect of the EF and of a resonant magnetic perturbation (RMP) on the TM, in particular on amplitude modulation, is modeled with a first-order solution of the Modified Rutherford Equation. In the experiment, the TM amplitude is measured as a function of the toroidal angle as the TM rotates rapidly in the presence of an unknown EF and a known, deliberately applied RMP. The RMP amplitude is fixed while the toroidal phase is varied from one discharge to the other, completing a full toroidal scan. Using three such scans with different RMP amplitudes, the EF amplitude and phase are inferred from the phases at which the TM amplitude maximizes. The estimated EF amplitude is consistent with other estimates (e.g. based on the best EF-cancelling RMP, resulting in the fastest TM rotation). A passive variant of this technique is also presented, where no RMPs are applied, and the EF phase is deduced., Comment: Submitted for publication in Plasma Physics and Controlled Fusion
Published: 2016
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9. EUROfusion contributions to ITER nuclear operation

Author: Litaudon, X., Fantz, U., Villari, R., Toigo, V., Aumeunier, M. -H, Autran, J. -L, Batistoni, P., Belonohy, E., Bradnam, S., Cecchetto, M., Colangeli, A., Dacquait, F., Dal Bello, S., Dentan, M., De Pietri, M., Eriksson, Jacob, Fabbri, M., Falchetto, G., Figini, L., Figueiredo, J., Flammini, D., Fonnesu, N., Frassinetti, L., Galdon-Quiroga, J., Garcia-Alia, R., Garcia-Munoz, M., Ghani, Z., Gonzalez-Martin, J., Grelier, E., Di Grazia, L., Grove, B., Grove, C. L., Gusarov, A., Heinemann, B., Hjalmarsson, Anders, Hyvarinen, O., Ioannou-Sougleridis, V., Jones, L., Kim, H. -T, Klosowski, M., Kocan, M., Kos, B., Kos, L., Kotnik, D., Laszynska, E., Leichtle, D., Lengar, I., Leon-Gutierrez, E., Lopez-Revelles, A. J., Loreti, S., Loughlin, M., Marcuzzi, D., Mcclements, K. G., Mariano, G., Mattei, M., Mergia, K., Mietelski, J., Mitteau, R., Moindjie, S., Munteanu, D., Naish, R., Noce, S., Packer, L. W., Pamela, S., Pampin, R., Pau, A., Peacock, A., Peluso, E., Peneliau, Y., Peric, J., Radulovic, V., Ricci, D., Rimini, F., Sanchis-Sanchez, L., Sauvan, P., Savva, M. I., Serianni, G., Shand, C. R., Snicker, A., Snoj, L., Stamatelatos, I. E., Stancar, Z., Terranova, N., Vasilopoulou, T., Vila, R., Waterhouse, J., Wimmer, C., Wuenderlich, D., Zohar, A., Litaudon, X., Fantz, U., Villari, R., Toigo, V., Aumeunier, M. -H, Autran, J. -L, Batistoni, P., Belonohy, E., Bradnam, S., Cecchetto, M., Colangeli, A., Dacquait, F., Dal Bello, S., Dentan, M., De Pietri, M., Eriksson, Jacob, Fabbri, M., Falchetto, G., Figini, L., Figueiredo, J., Flammini, D., Fonnesu, N., Frassinetti, L., Galdon-Quiroga, J., Garcia-Alia, R., Garcia-Munoz, M., Ghani, Z., Gonzalez-Martin, J., Grelier, E., Di Grazia, L., Grove, B., Grove, C. L., Gusarov, A., Heinemann, B., Hjalmarsson, Anders, Hyvarinen, O., Ioannou-Sougleridis, V., Jones, L., Kim, H. -T, Klosowski, M., Kocan, M., Kos, B., Kos, L., Kotnik, D., Laszynska, E., Leichtle, D., Lengar, I., Leon-Gutierrez, E., Lopez-Revelles, A. J., Loreti, S., Loughlin, M., Marcuzzi, D., Mcclements, K. G., Mariano, G., Mattei, M., Mergia, K., Mietelski, J., Mitteau, R., Moindjie, S., Munteanu, D., Naish, R., Noce, S., Packer, L. W., Pamela, S., Pampin, R., Pau, A., Peacock, A., Peluso, E., Peneliau, Y., Peric, J., Radulovic, V., Ricci, D., Rimini, F., Sanchis-Sanchez, L., Sauvan, P., Savva, M. I., Serianni, G., Shand, C. R., Snicker, A., Snoj, L., Stamatelatos, I. E., Stancar, Z., Terranova, N., Vasilopoulou, T., Vila, R., Waterhouse, J., Wimmer, C., Wuenderlich, D., and Zohar, A.
Abstract: ITER is of key importance in the European fusion roadmap as it aims to prove the scientific and technological feasibility of fusion as a future energy source. The EUROfusion consortium of labs within Europe is contributing to the preparation of ITER scientific exploitation and operation and aspires to exploit ITER outcomes in view of DEMO. The paper provides an overview of the major progress obtained recently, carried out in the frame of the new (initiated in 2021) EUROfusion work-package called 'Preparation of ITER Operation' (PrIO). The overview paper is directly supported by the eleven EUROfusion PrIO contributions given at the 29th Fusion Energy Conference (16-21 October 2023) London, UK [www.iaea.org/events/fec2023]. The paper covers the following topics: (i) development and validation of tools in support to ITER operation (plasma breakdown/burn-through with evolving plasma volume, new infra-red synthetic diagnostic for off-line analysis and wall monitoring using Artificial Intelligence techniques, synthetic diagnostics development, development and exploitation of multi-machine databases); (ii) R&D for the radio-frequency ITER neutral beam sources leading to long duration of negative deuterium/hydrogen ions current extraction at ELISE and participation in the neutral beam test facility with progress on the ITER source SPIDER, and, the commissioning of the 1 MV high voltage accelerator (MITICA) with lessons learned for ITER; (iii) validation of neutronic tools for ITER nuclear operation following the second JET deuterium-tritium experimental campaigns carried out in 2021 and in 2023 (neutron streaming and shutdown dose rate calculation, water activation and activated corrosion products with advanced fluid dynamic simulation; irradiation of several materials under 14.1 MeV neutron flux etc).
Published: 2024
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10. Improved Confinement in JET High {beta} Plasmas with an ITER-Like Wall

Author: Challis, C. D., Garcia, J., Beurskens, M., Buratti, P., Delabie, E., Drewelow, P., Frassinetti, L., Giroud, C., Hawkes, N., Hobirk, J., Joffrin, E., Keeling, D., King, D. B., Maggi, C. F., Mailloux, J., Marchetto, C., McDonald, D., Nunes, I., Pucella, G., Saarelma, S., and Simpson, J.
Subjects: Physics - Plasma Physics
Abstract: The replacement of the JET carbon wall (C-wall) by a Be/W ITER-like wall (ILW) has affected the plasma energy confinement. To investigate this, experiments have been performed with both the C-wall and ILW to vary the heating power over a wide range for plasmas with different shapes., Comment: 50 pages, 32 figures. This is an author-created, un-copyedited version of an article submitted for publication in Nuclear Fusion. IoP Publishing Ltd is not responsible for any errors or omissions in this version of the manuscript or any version derived from it
Published: 2015
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11. Contrasting H-mode behaviour with deuterium fuelling and nitrogen seeding in the all-carbon and metallic versions of JET

Author: Maddison, G. P., Giroud, C., Alper, B., Arnoux, G., Balboa, I., Beurskens, M. N. A., Boboc, A., Brezinsek, S., Brix, M., Clever, M., Coelho, R., Coenen, J. W., Coffey, I., Belo, P. C. da Silva Aresta, Devaux, S., Devynck, P., Eich, T., Felton, R. C., Flanagan, J., Frassinetti, L., Garzotti, L., Groth, M., Jachmich, S., Järvinen, A., Joffrin, E., Kempenaars, M. A. H., Kruezi, U., Lawson, K. D., Lehnen, M., Leyland, M. J., Liu, Y., Lomas, P. J., Lowry, C. G., Marsen, S., Matthews, G. F., McCormick, G. K., Meigs, A. G., Morris, A. W., Neu, R., Nunes, I. M., Oberkofler, M., Rimini, F. G., Saarelma, S., Sieglin, B., Sips, A. C. C., Sirinelli, A., Stamp, M. F., van Rooij, G. J., Ward, D. J., Wischmeier, M., and contributors, JET EFDA
Subjects: Physics - Plasma Physics
Abstract: The former all-carbon wall on JET has been replaced with beryllium in the main torus and tungsten in the divertor to mimic the surface materials envisaged for ITER. Comparisons are presented between Type I H-mode characteristics in each design by examining respective scans over deuterium fuelling and impurity seeding, required to ameliorate exhaust loads both in JET at full capability and in ITER., Comment: 55 pages, 15 figures
Published: 2014
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12. Core integrated simulations for the Divertor Tokamak Test facility scenarios towards consistent core-pedestal-SOL modelling

Author: Casiraghi, I, Mantica, P, Ambrosino, R, Aucone, L, Baiocchi, B, Balbinot, L, Barberis, T, Castaldo, A, Cavedon, M, Frassinetti, L, Innocente, P, Koechl, F, Nowak, S, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Vincenzi, P, Casiraghi I., Mantica P., Ambrosino R., Aucone L., Baiocchi B., Balbinot L., Barberis T., Castaldo A., Cavedon M., Frassinetti L., Innocente P., Koechl F., Nowak S., Agostinetti P., Ceccuzzi S., Figini L., Granucci G., Vincenzi P., Casiraghi, I, Mantica, P, Ambrosino, R, Aucone, L, Baiocchi, B, Balbinot, L, Barberis, T, Castaldo, A, Cavedon, M, Frassinetti, L, Innocente, P, Koechl, F, Nowak, S, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Vincenzi, P, Casiraghi I., Mantica P., Ambrosino R., Aucone L., Baiocchi B., Balbinot L., Barberis T., Castaldo A., Cavedon M., Frassinetti L., Innocente P., Koechl F., Nowak S., Agostinetti P., Ceccuzzi S., Figini L., Granucci G., and Vincenzi P.
Abstract: Deuterium plasma discharges of the Divertor Tokamak Test facility (DTT) in different operational scenarios have been predicted by a comprehensive first-principle based integrated modelling activity using state-of-art quasi-linear transport models. The results of this work refer to the updated DTT configuration, which includes a device size optimisation (enlargement to R 0 = 2.19 m and a = 0.70 m) and upgrades in the heating systems. The focus of this paper is on the core modelling, but special attention was paid to the consistency with the scrape-off layer parameters required to achieve divertor plasma detachment. The compatibility of these physics-based predicted scenarios with the electromagnetic coil system capabilities was then verified. In addition, first estimates of DTT sawteeth and of DTT edge localised modes were achieved.
Published: 2023

13. Impact of nitrogen seeding on confinement and power load control of a high-triangularity JET ELMy H-mode plasma with a metal wall

Author: Giroud, C, Maddison, G P, Jachmich, S, Rimini, F, Beurskens, M N A, Balboa, I, Brezinsek, S, Coelho, R, Coenen, J W, Frassinetti, L, Joffrin, E, Oberkofler, M, Lehnen, M, Liu, Y, Marsen, S, K, K McCormick, Meigs, A, Neu, R, Sieglin, B, van Rooij, G, Arnoux, G, Belo, P, Brix, M, Clever, M, Coffey, I, Devaux, S, Douai, D, Eich, T, Flanagan, J, Grunhagen, S, Huber, A, Kempenaars, M, Kruezi, U, Lawson, K, Lomas, P, Lowry, C, Nunes, I, Sirinnelli, A, Sips, A C C, Stamp, M, Wiesen, S, and contributors, JET-EFDA
Subjects: Physics - Plasma Physics
Abstract: This paper reports the impact on confinement and power load of the high-shape 2.5MA ELMy H-mode scenario at JET of a change from an all carbon plasma facing components to an all metal wall. In preparation to this change, systematic studies of power load reduction and impact on confinement as a result of fuelling in combination with nitrogen seeding were carried out in JET-C and are compared to their counterpart in JET with a metallic wall. An unexpected and significant change is reported on the decrease of the pedestal confinement but is partially recovered with the injection of nitrogen., Comment: 30 pages, 16 figures
Published: 2013
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14. Error Field Assessment from Driven Rotation of Stable External Kinks at EXTRAP-T2R Reversed Field Pinch

Author: Volpe, F. A., Frassinetti, L., Brunsell, P. R., Drake, J. R., and Olofsson, K. E. J.
Subjects: Physics - Plasma Physics
Abstract: A new non-disruptive error field (EF) assessment technique not restricted to low density and thus low beta was demonstrated at the EXTRAP-T2R reversed field pinch. Stable and marginally stable external kink modes of toroidal mode number n=10 and n=8, respectively, were generated, and their rotation sustained, by means of rotating magnetic perturbations of the same n. Due to finite EFs, and in spite of the applied perturbations rotating uniformly and having constant amplitude, the kink modes were observed to rotate non-uniformly and be modulated in amplitude. This behavior was used to precisely infer the amplitude and approximately estimate the toroidal phase of the EF. A subsequent scan permitted to optimize the toroidal phase. The technique was tested against deliberately applied as well as intrinsic error fields of n=8 and 10. Corrections equal and opposite to the estimated error fields were applied. The efficacy of the error compensation was indicated by the increased discharge duration and more uniform mode rotation in response to a uniformly rotating perturbation. The results are in good agreement with theory, and the extension to lower n, to tearing modes and to tokamaks, including ITER, is discussed., Comment: 21 pages, 16 figures
Published: 2013
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15. MHD and Gyro-kinetic Stability of JET Pedestals

Author: Saarelma, S., Beurskens, M. N. A., Dickinson, D., Frassinetti, L., Leyland, M. J., Roach, C. M., and contributors, EFDA-JET
Subjects: Physics - Plasma Physics
Abstract: The pedestal profile measurements in high triangularity JET plasmas show that with low fuelling the pedestal width decreases during the ELM cycle and with high fuelling it stays constant. In the low fuelling case the pedestal pressure gradient keeps increasing until the ELM crash and in the high fuelling case it initially increases then saturates during the ELM cycle. Stability analysis reveals that both JET plasmas become unstable to finite-n ideal MHD peeling-ballooning modes at the end of the ELM cycle. During the ELM cycle, infinite-n ideal MHD ballooning modes and kinetic ballooning modes are found to be locally stable in most of the steep pressure gradient region of the pedestal owing to the large bootstrap current, but to be locally unstable in a narrow region of plasma at the extreme edge. Unstable micro-tearing modes are found at the JET pedestal top, but they are sub-dominant to ion temperature gradient modes. They are insensitive to collisionality and stabilised by increasing density gradient., Comment: submitted to Nuclear Fusion, 23 pages, for EFDA-JET contributors see the Appendix of F. Romanelli et al., Proceedings of the 24th IAEA Fusion Energy Conference 2012, San Diego, USA
Published: 2013
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16. Representation learning algorithms for inferring machine independent latent features in pedestals in JET and AUG.

Author: Järvinen, A. E., Kit, A., Poels, Y. R. J., Wiesen, S., Menkovski, V., Frassinetti, L., and Dunne, M.
Subjects: MACHINE learning, ELECTRON distribution, PEDESTALS, MAGNETIC confinement, LATENT variables
Abstract: Variational autoencoder (VAE)-based representation learning algorithms are explored for their capability to disentangle tokamak size dependence from other dependencies in a dataset of thousands of observed pedestal electron density and temperature profiles from JET and ASDEX Upgrade tokamaks. Representation learning aims to establish a useful representation that characterizes the dataset. In the context of magnetic confinement fusion devices, a useful representation could be considered to map the high-dimensional observations to a manifold that represents the actual degrees of freedom of the plasma scenario. A desired property for these representations is organization of the information into disentangled variables, enabling interpretation of the latent variables as representations of semantically meaningful characteristics of the data. The representation learning algorithms in this work are based on VAE that encodes the pedestal profile information into a reduced dimensionality latent space and learns to reconstruct the full profile information given the latent representation. Attaching an auxiliary regression objective for the machine control parameter configuration, broadly following the architecture of the domain invariant variational autoencoder (DIVA), the model learns to associate device control parameters with the latent representation. With this multimachine dataset, the representation does encode density scaling with device size that is qualitatively consistent with Greenwald density limit scaling. However, if the major radius of the device is given through a common regression objective with the other machine control parameters, the latent state of the representation struggles to clearly disentangle the device size from changes of the other machine control parameters. When separating the device size as an independent latent variable with dedicated regression objectives, similar to separation of domain and class labels in the original DIVA publication, the latent space becomes well organized as a function of the device size. [ABSTRACT FROM AUTHOR]
Published: 2024
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17. The see-saw mechanism and heavy Majorana neutrino masses in an SO(10) model

Author: Alles, W. and Frassinetti, L.
Subjects: High Energy Physics - Phenomenology
Abstract: We apply the see-saw mechanism and an SO(10) model to neutrino masses and mixing in order to estimate the heavy Majorana masses. We discuss shortly the decay modes of heavy Majorana neutrinos and calculate their contribution to the lepton number violating processes \mu\to e\gamma, \tau\to\mu\gamma and \tau\to e\gamma., Comment: 7 pages
Published: 2000

18. Gray-box modeling of resistive wall modes with vacuum-plasma separation and optimal control design for EXTRAP T2R

Author: Setiadi, A.C., Brunsell, P.R., Villone, F., Mastrostefano, S., and Frassinetti, L.
Published: 2017
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19. Enhanced performance in fusion plasmas through turbulence suppression by megaelectronvolt ions

Author: 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., Lawson, K., Lazaros, A., Lazzaro, E., Learoyd, G., Lee, C., Lee, S., Leerink, S., Leeson, T., Lefebvre, X., Leggate, H., 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., Lopez, J., Lorenzini, R., Loreti, S., Losada, U., Loschiavo, V., Loughlin, M., Louka, Z., Lovell, J., Lowe, T., Lowry, C., Lubbad, S., Luce, T., Lucock, R., Lukin, A., Luna, C., Luna, E., Lungaroni, M., Lungu, C., Lunt, T., Lutsenko, V., Lyons, B., Lyssoivan, A., Machielsen, M., Macusova, E., Mäenpää, R., Maggi, C., Maggiora, R., Magness, M., Mahesan, S., Maier, H., Maingi, R., Malinowski, K., Manas, P., Mantica, P., Mantsinen, M., 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., Martone, R., Maruyama, S., Maslov, M., Masuzaki, S., Matejcik, S., Mattei, M., Matthews, G., Matveev, D., Matveeva, E., Mauriya, A., Maviglia, F., Mayer, M., Mayoral, M., Mazzotta, C., McAdams, R., McCarthy, P., McClements, K., McClenaghan, J., McCullen, P., McDonald, D., McGuckin, D., McHugh, D., Mclntyre, G., McKean, R., McKehon, J., McMillan, B., McNamee, L., McShee, A., Meakins, A., Medley, S., Meekes, C., Meghani, K., Meigs, A., 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., 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., Mordijck, S., Moreira, L., Morgan, L., Moro, F., Morris, J., Morrison, K., Moser, L., Moulton, D., Mrowetz, T., Mundy, T., Muraglia, M., Murari, A., Muraro, A., Muthusonai, N., N'Konga, B., Na, Y., Nabais, F., Naden, M., Naish, J., Naish, R., Napoli, F., Nardon, E., Naulin, V., Nave, M., Nedzelskiy, I., Nemtsev, G., Nesenevich, V., Nestoras, I., Neu, R., Neverov, V., Ng, S., Nicassio, M., Nielsen, A., Nina, D., Nishijima, D., Noble, C., Nobs, C., Nodwell, D., Nordlund, K., Nordman, H., Normanton, R., Noterdaeme, J., Nowak, S., Nunn, E., Nystrom, H., Oberparleiter, M., Obryk, B., O'Callaghan, J., Odupitan, T., Oliver, H., 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., Paige, S., Pajuste, E., Palade, D., Pamela, S., Panadero, N., Panontin, E., Papadopoulos, A., Papp, G., Papp, P., Parail, 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., Paz Soldan, C., Peacock, A., Pearce, M., Peluso, E., Penot, C., Pepperell, K., Pereira, R., Pereira, T., Perelli Cippo, E., 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., Plassche, K., Platt, N., Plyusnin, V., Podesta, M., Pokol, G., Poli, F., Pompilian, O., Popovichev, S., Poradzinski, M., Porfiri, M., 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., Pütterich, T., Quercia, A., Rachlew, E., Radulescu, G., Radulovic, V., Rainford, M., Raj, P., Ralph, G., Ramogida, G., Rasmussen, D., Rasmussen, J., Ratta, G., Ratynskaia, S., Rebai, M., Refy, D., Reichle, R., Reinke, M., Reiser, D., Reux, C., Reynolds, S., Richiusa, M., Richyal, S., Rigamonti, D., Rimini, F., Risner, J., Riva, M., Rivero-Rodriguez, J., Roach, C., Robins, R., Robinson, S., Robson, D., Rodionov, R., 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 Ruiz, J., 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., Schworer, D., Scott, G., Scott, M., Scraggs, D., Scully, S., Segato, M., Seo, J., Sergienko, G., Sertoli, M., Sharapov, S., Shaw, A., Sheikh, H., Sheikh, U., Shepherd, A., Shevelev, A., Shigin, P., Shinohara, K., Shiraiwa, S., Shiraki, D., Short, M., Sias, G., Silburn, S., Silva, A., Silva, C., Silva, J., Silvagni, D., Simfukwe, D., Simpson, J., Sinclair, D., Sipilä, S., Sips, A., Siren, P., Sirinelli, A., Sjöstrand, H., Skinner, N., Slater, J., Smith, N., Smith, P., Snell, J., Snoep, G., Snoj, L., Snyder, P., Soare, S., Solano, E., 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., Strikwerda, S., Ström, P., Stuart, C., Studholme, W., Subramani, M., Suchkov, E., Sumida, S., Sun, H., Susts, T., 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., 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., Tipton, A., Todd, H., Tokitani, M., Tolias, P., Tomes, M., Tookey, A., Torikai, Y., Toussaint, U., Tsavalas, P., Tskhakaya, D., Turner, I., Turner, 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., Verona Rinati, G., Veshchev, E., Vianello, N., Viezzer, E., Vignitchouk, L., Vila, R., Villari, R., Villone, F., Vincenzi, P., Vinyar, I., Viola, B., Virtanen, A., Vitins, A., Vizvary, Z., Vlad, G., Vlad, M., Vondracek, P., de Vries, P., Wakeling, B., Walkden, N., 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., 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., Xu, T., Yadikin, D., Yajima, M., Yakovenko, Y., Yang, Y., Yanling, W., Yanovskiy, V., Young, I., Young, R., Zabolockis, R., Zacks, J., Zagorski, R., Zaitsev, F., Zakharov, L., Zarins, A., Zarzoso Fernandez, D., Zastrow, K., Zayachuk, Y., Zerbini, M., Zhang, W., Zhou, Y., Zlobinski, M., Zocco, A., Zohar, A., Zoita, V., Zoletnik, S., Zotta, V., Zoulias, I., Zwingmann, W., Zychor, I., Physique des interactions ioniques et 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

20. Pedestal particle balance studies in JET-ILW H-mode plasmas

Author: Horvath, L, Lomanowski, B, Karhunen, J, Maslov, M, Schneider, PA, Simpson, J, Brix, M, Chapman-Oplopoiou, B, Corrigan, G, Frassinetti, L, Groth, M, Lawson, K, Maggi, CF, Menmuir, S, Morales, RB, Moulton, D, Myatra, O, Nina, D, Pereira, T, Refy, DI, Saarelma, S, Vecsei, M, Chiariello, A, Formisano, A, Horvath, L, Lomanowski, B, Karhunen, J, Maslov, M, Schneider, Pa, Simpson, J, Brix, M, Chapman-Oplopoiou, B, Corrigan, G, Frassinetti, L, Groth, M, Lawson, K, Maggi, Cf, Menmuir, S, Morales, Rb, Moulton, D, Myatra, O, Nina, D, Pereira, T, Refy, Di, Saarelma, S, Vecsei, M, Chiariello, A, Formisano, A, JET, Oak Ridge National Laboratory, Max-Planck-Institut für Plasmaphysik, Department of Applied Physics, KTH Royal Institute of Technology, Fusion and Plasma Physics, Universidade Lisboa, Center for Energy Research, Aalto-yliopisto, Aalto University, and JET Contributors
Subjects: H-mode, Nuclear Energy and Engineering, particle transport, EDGE2D-EIRENE, JET-ILW, fuelling, EIRENE, Condensed Matter Physics, pedestal
Abstract: JET-ILW type I ELMy H-modes at 2.5 MA/2.8 T with constant NBI heating (23 MW) and gas fuelling rate were performed, utilising edge localised mode (ELM) pacing by vertical kicks and plasma shaping (triangularity, δ) as tools to disentangle the effects of ELMs, inter-ELM transport and edge stability on the pedestal particle balance. In agreement with previous studies, the pedestal confinement improves with increasing δ, mostly due to a significant increase in pedestal density while the ELM frequency ( f E L M ) is decreased. Improved pedestal confinement with increasing δ was observed even when the pedestal MHD stability was degraded artificially by vertical kicks, implying that increased triangularity may favourably affect the inter-ELM pedestal recovery. The workflow developed to quantify the pedestal particle balance uses high time-resolution profile reflectometry to characterise the inter-ELM evolution of the plasma particle content ( d N / d t ), the NEO drift-kinetic solver to evaluate the neoclassical fluxes and interpretative EDGE2D-EIRENE simulations to estimate the edge particle source. The edge particle source is then constrained by deuterium Balmer-α line intensity measurements in the main chamber, which are, however, strongly affected by reflections from the metal walls. The reflections are accounted for by the CHERAB code taking the divertor emission (the brightest light source in the torus) distribution from imaging spectroscopy measurements as input. Our analysis shows that in the second half of the ELM cycle, the volume-integrated particle source is larger than d N / d t , indicating that transport plays a key role in the inter-ELM pedestal recovery.
Published: 2023

21. Disruption prediction with artificial intelligence techniques in tokamak plasmas

Author: Vega, J, Murari, A, Dormido-Canto, S, Ratta, G, Gelfusa, M, Mailloux, J, 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, 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, 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, Bilkova, 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, de la 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, 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, Douai, D, Dowson, S, Doyle, R, Dreval, M, 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, El Haroun, H, Ellwood, G, Elsmore, C, Embreus, O, Emery, S, Ericsson, G, Eriksson, B, Eriksson, F, Eriksson, J, 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, Fulop, T, Furseman, M, Fusco, V, Futatani, S, Gadariya, D, Gal, K, Galassi, D, Gafezka, K, Galeani, S, Gallart, D, Galvao, R, Gao, Y, Garcia, J, Garcia-Munoz, M, Gardener, M, Garzotti, L, Gaspar, J, Gatto, R, Gaudio, P, Gear, D, Gebhart, T, Gee, S, 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, 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Lngleby, J, Innocente, P, Bjork, K, Isernia, N, lvanova-Stanik, I, Lvings, E, Jablonski, S, Jachmich, S, Jackson, T, Jacquet, P, Jarleblad, H, Jaulmes, F, 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, Kazakov, Y, Kazantzidis, V, Keeling, D, Kelly, R, Kempenaars, M, Kennedy, C, Kennedy, D, Kent, J, Khan, K, Khilkevich, E, Kiefer, C, Kilpelainen, 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, Neto, E, Laszyriska, E, Lawson, K, Lazaros, A, Lazzaro, E, Learoyd, G, Lee, C, Lee, S, Leerink, S, Leeson, T, Lefebvre, X, Leggate, H, Lehmann, J, Lehnen, M, Leichtle, D, Leipold, F, Lengar, I, Lennholm, M, 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, Lopez, J, Lorenzini, R, Loreti, S, Losada, U, Loschiavo, V, 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, Lunt, T, Lutsenko, V, Lyons, B, Lyssoivan, A, Machielsen, M, Macusova, E, Maenpaa, R, Maggi, C, Maggiora, R, Magness, M, Mahesan, S, Maier, H, Maingi, R, Malinowski, K, Manas, P, Mantica, P, Mantsinen, M, 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, Martone, R, Maruyama, S, Maslov, M, Masuzaki, S, Matejcik, S, Mattei, M, Matthews, G, Matveev, D, Matveeva, E, Mauriya, A, Maviglia, F, Mayer, M, Mayoral, M, Mazzi, S, Mazzotta, C, Mcadams, R, Mccarthy, P, Mcclements, K, Mcclenaghan, J, Mccullen, P, Mcdonald, D, Mcguckin, D, Mchugh, D, Mclntyre, G, Mckean, R, Mckehon, J, Mcmillan, B, Mcnamee, L, Mcshee, A, Meakins, A, Medley, S, Meekes, C, Meghani, K, Meigs, A, 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, Milnes, J, 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Terranova, N, Testa, D, Tholerus, E, Thomas, J, Thoren, E, Thorman, A, Tierens, W, Tinguely, R, 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, Turnyanskiy, M, Tvalashvili, G, Tyrrell, S, Tyshchenko, M, Uccello, A, Udintsev, V, Urbanczyk, G, Vadgama, A, Valcarcel, D, Valisa, M, Olivares, P, Vallhagen, O, Valovic, M, Eester, D, Varje, J, Vartanian, S, Vasilopoulou, T, Vayakis, G, Vecsei, M, Ventre, S, Verdoolaege, G, Verona, C, Rinati, G, Veshchev, E, Vianello, N, Viezzer, E, Vignitchouk, L, Vila, R, Villari, R, Villone, F, Vincenzi, P, Vinyar, I, Viola, B, Virtanen, A, Vitins, A, Vizvary, Z, Vlad, G, Vlad, M, Vondracek, P, de Vries, P, Wakeling, B, Walkden, N, Walker, M, Walker, R, Walsh, M, Wang, E, Wang, N, Warder, S, Warren, R, Waterhouse, J, Watts, C, Wauters, T, Weckmann, A, Maxwell, H, Weiland, M, Weisen, H, Weiszflog, M, Welch, P, Wendler, N, West, A, Wheatley, M, Wheeler, S, 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A., Gelfusa M., Mailloux J., 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. G., Alessi E., Aleynikov P., Algualcil J., Ali M., Allinson M., Alper B., Alves E., Ambrosino G., Ambrosino R., Amosov V., Sunden E. A., Andrew P., Angelini B. M., Angioni C., Antoniou I., Appel L. C., 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. K., Banks J., Baranov Y. F., 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. 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C., 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., de la 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. S., Carvalho P., Casiraghi I., Casson F. J., Castaldo C., Catalan J. P., Catarino N., Causa F., Cavedon M., Cecconello M., Challis C. D., Chamberlain B., Chang C. S., 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. P., Coates P., Cobalt A., Coccorese V., Coelho R., Coenen J. W., Coffey I. H., Colangeli A., Colas L., Collins C., Collins J., Collins S., Conka D., Conroy S., Conway B., Conway N. 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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

22. Enhanced performance in fusion plasmas through turbulence suppression by megaelectronvolt ions

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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. 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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

23. Predict–first scenario modelling in support of the design of the Divertor Tokamak Test facility

Author: Casiraghi, I, Mantica, P, Ambrosino, R, Aucone, L, Auriemma, F, Baiocchi, B, Balbinot, L, Barberis, T, Bonanomi, N, Castaldo, A, Citrin, J, Frassinetti, L, Innocente, P, Koechl, F, Mariani, A, Nowak, S, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Valisa, M, Casiraghi I., Mantica P., Ambrosino R., Aucone L., Auriemma F., Baiocchi B., Balbinot L., Barberis T., Bonanomi N., Castaldo A., Citrin J., Frassinetti L., Innocente P., Koechl F., Mariani A., Nowak S., Agostinetti P., Ceccuzzi S., Figini L., Granucci G., Valisa M., Casiraghi, I, Mantica, P, Ambrosino, R, Aucone, L, Auriemma, F, Baiocchi, B, Balbinot, L, Barberis, T, Bonanomi, N, Castaldo, A, Citrin, J, Frassinetti, L, Innocente, P, Koechl, F, Mariani, A, Nowak, S, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Valisa, M, Casiraghi I., Mantica P., Ambrosino R., Aucone L., Auriemma F., Baiocchi B., Balbinot L., Barberis T., Bonanomi N., Castaldo A., Citrin J., Frassinetti L., Innocente P., Koechl F., Mariani A., Nowak S., Agostinetti P., Ceccuzzi S., Figini L., Granucci G., and Valisa M.
Published: 2022

24. Overview of the TCV tokamak experimental programme

Author: Reimerdes, H, Agostini, M, Alessi, E, Alberti, S, Andrebe, Y, Arnichand, H, Balbin, J, Bagnato, F, Baquero-Ruiz, M, Bernert, M, Bin, W, Blanchard, P, Blanken, T, Boedo, J, Brida, D, Brunner, S, Bogar, C, Bogar, O, Bolzonella, T, Bombarda, F, Bouquey, F, Bowman, C, Brunetti, D, Buermans, J, Bufferand, H, Calacci, L, Camenen, Y, Carli, S, Carnevale, D, Carpanese, F, Causa, F, Cavalier, J, Cavedon, M, Cazabonne, J, Cerovsky, J, Chandra, R, Chandrarajan Jayalekshmi, A, Chellai, O, Chmielewski, P, Choi, D, Ciraolo, G, Classen, I, Coda, S, Colandrea, C, Dal Molin, A, David, P, De Baar, M, Decker, J, Dekeyser, W, De Oliveira, H, Douai, D, Dreval, M, Dunne, M, Duval, B, Elmore, S, Embreus, O, Eriksson, F, Faitsch, M, Falchetto, G, Farnik, M, Fasoli, A, Fedorczak, N, Felici, F, Fevrier, O, Ficker, O, Fil, A, Fontana, M, Fransson, E, Frassinetti, L, Furno, I, Gahle, D, Galassi, D, Galazka, K, Galperti, C, Garavaglia, S, Garcia-Munoz, M, Geiger, B, Giacomin, M, Giruzzi, G, Gobbin, M, Golfinopoulos, T, Goodman, T, Gorno, S, Granucci, G, Graves, J, Griener, M, Gruca, M, Gyergyek, T, Haelterman, R, Hakola, A, Han, W, Happel, T, Harrer, G, Harrison, J, Henderson, S, Hogeweij, G, Hogge, J, Hoppe, M, Horacek, J, Huang, Z, Iantchenko, A, Innocente, P, Insulander Bjork, K, Ionita-Schrittweiser, C, Isliker, H, Jardin, A, Jaspers, R, Karimov, R, Karpushov, A, Kazakov, Y, Komm, M, Kong, M, Kovacic, J, Krutkin, O, Kudlacek, O, Kumar, U, Kwiatkowski, R, Labit, B, Laguardia, L, Lammers, J, Laribi, E, Laszynska, E, Lazaros, A, Linder, O, Linehan, B, Lipschultz, B, Llobet, X, Loizu, J, Lunt, T, Macusova, E, Marandet, Y, Maraschek, M, Marceca, G, Marchetto, C, Marchioni, S, Marmar, E, Martin, Y, Martinelli, L, Matos, F, Maurizio, R, Mayoral, M, Mazon, D, Menkovski, V, Merle, A, Merlo, G, Meyer, H, Mikszuta-Michalik, K, Molina Cabrera, P, Morales, J, Moret, J, Moro, A, Moulton, D, Muhammed, H, Myatra, O, Mykytchuk, D, Napoli, F, Nem, R, Nielsen, A, Nocente, M, Nowak, S, Offeddu, N, Olsen, J, Orsitto, F, Pan, O, Papp, G, Pau, A, Perek, A, Pesamosca, F, Peysson, Y, Pigatto, L, Piron, C, Poradzinski, M, Porte, L, Putterich, T, Rabinski, M, Raj, H, Rasmussen, J, Ratta, G, Ravensbergen, T, Ricci, D, Ricci, P, Rispoli, N, Riva, F, Rivero-Rodriguez, J, Salewski, M, Sauter, O, Schmidt, B, Schrittweiser, R, Sharapov, S, Sheikh, U, Sieglin, B, Silva, M, Smolders, A, Snicker, A, Sozzi, C, Spolaore, M, Stagni, A, Stipani, L, Sun, G, Tala, T, Tamain, P, Tanaka, K, Tema Biwole, A, Terranova, D, Terry, J, Testa, D, Theiler, C, Thornton, A, Thrysoe, A, Torreblanca, H, Tsui, C, Vaccaro, D, Vallar, M, Van Berkel, M, Van Eester, D, Van Kampen, R, Van Mulders, S, Verhaegh, K, Verhaeghe, T, Vianello, N, Villone, F, Viezzer, E, Vincent, B, Voitsekhovitch, I, Vu, N, Walkden, N, Wauters, T, Weisen, H, Wendler, N, Wensing, M, Widmer, F, Wiesen, S, Wischmeier, M, Wijkamp, T, Wunderlich, D, Wuthrich, C, Yanovskiy, V, Zebrowski, J, Reimerdes H., Agostini M., Alessi E., Alberti S., Andrebe Y., Arnichand H., Balbin J., Bagnato F., Baquero-Ruiz M., Bernert M., Bin W., Blanchard P., Blanken T. C., Boedo J. A., Brida D., Brunner S., Bogar C., Bogar O., Bolzonella T., Bombarda F., Bouquey F., Bowman C., Brunetti D., Buermans J., Bufferand H., Calacci L., Camenen Y., Carli S., Carnevale D., Carpanese F., Causa F., Cavalier J., Cavedon M., Cazabonne J. A., Cerovsky J., Chandra R., Chandrarajan Jayalekshmi A., Chellai O., Chmielewski P., Choi D., Ciraolo G., Classen I. G. J., Coda S., Colandrea C., Dal Molin A., David P., De Baar M. R., Decker J., Dekeyser W., De Oliveira H., Douai D., Dreval M., Dunne M. G., Duval B. P., Elmore S., Embreus O., Eriksson F., Faitsch M., Falchetto G., Farnik M., Fasoli A., Fedorczak N., Felici F., Fevrier O., Ficker O., Fil A., Fontana M., Fransson E., Frassinetti L., Furno I., Gahle D. S., Galassi D., Galazka K., Galperti C., Garavaglia S., Garcia-Munoz M., Geiger B., Giacomin M., Giruzzi G., Gobbin M., Golfinopoulos T., Goodman T., Gorno S., Granucci G., Graves J. P., Griener M., Gruca M., Gyergyek T., Haelterman R., Hakola A., Han W., Happel T., Harrer G., Harrison J. R., Henderson S., Hogeweij G. M. D., Hogge J. -P., Hoppe M., Horacek J., Huang Z., Iantchenko A., Innocente P., Insulander Bjork K., Ionita-Schrittweiser C., Isliker H., Jardin A., Jaspers R. J. E., Karimov R., Karpushov A. N., Kazakov Y., Komm M., Kong M., Kovacic J., Krutkin O., Kudlacek O., Kumar U., Kwiatkowski R., Labit B., Laguardia L., Lammers J. T., Laribi E., Laszynska E., Lazaros A., Linder O., Linehan B., Lipschultz B., Llobet X., Loizu J., Lunt T., Macusova E., Marandet Y., Maraschek M., Marceca G., Marchetto C., Marchioni S., Marmar E. S., Martin Y., Martinelli L., Matos F., Maurizio R., Mayoral M. -L., Mazon D., Menkovski V., Merle A., Merlo G., Meyer H., Mikszuta-Michalik K., Molina Cabrera P. A., Morales J., Moret J. -M., Moro A., Moulton D., Muhammed H., Myatra O., Mykytchuk D., Napoli F., Nem R. D., Nielsen A. H., Nocente M., Nowak S., Offeddu N., Olsen J., Orsitto F. P., Pan O., Papp G., Pau A., Perek A., Pesamosca F., Peysson Y., Pigatto L., Piron C., Poradzinski M., Porte L., Putterich T., Rabinski M., Raj H., Rasmussen J. J., Ratta G. A., Ravensbergen T., Ricci D., Ricci P., Rispoli N., Riva F., Rivero-Rodriguez J. F., Salewski M., Sauter O., Schmidt B. S., Schrittweiser R., Sharapov S., Sheikh U. A., Sieglin B., Silva M., Smolders A., Snicker A., Sozzi C., Spolaore M., Stagni A., Stipani L., Sun G., Tala T., Tamain P., Tanaka K., Tema Biwole A., Terranova D., Terry J. L., Testa D., Theiler C., Thornton A., Thrysoe A., Torreblanca H., Tsui C. K., Vaccaro D., Vallar M., Van Berkel M., Van Eester D., Van Kampen R. J. R., Van Mulders S., Verhaegh K., Verhaeghe T., Vianello N., Villone F., Viezzer E., Vincent B., Voitsekhovitch I., Vu N. M. T., Walkden N., Wauters T., Weisen H., Wendler N., Wensing M., Widmer F., Wiesen S., Wischmeier M., Wijkamp T. A., Wunderlich D., Wuthrich C., Yanovskiy V., Zebrowski J., Reimerdes, H, Agostini, M, Alessi, E, Alberti, S, Andrebe, Y, Arnichand, H, Balbin, J, Bagnato, F, Baquero-Ruiz, M, Bernert, M, Bin, W, Blanchard, P, Blanken, T, Boedo, J, Brida, D, Brunner, S, Bogar, C, Bogar, O, Bolzonella, T, Bombarda, F, Bouquey, F, Bowman, C, Brunetti, D, Buermans, J, Bufferand, H, Calacci, L, Camenen, Y, Carli, S, Carnevale, D, Carpanese, F, Causa, F, Cavalier, J, Cavedon, M, Cazabonne, J, Cerovsky, J, Chandra, R, Chandrarajan Jayalekshmi, A, Chellai, O, Chmielewski, P, Choi, D, Ciraolo, G, Classen, I, Coda, S, Colandrea, C, Dal Molin, A, David, P, De Baar, M, Decker, J, Dekeyser, W, De Oliveira, H, Douai, D, Dreval, M, Dunne, M, Duval, B, Elmore, S, Embreus, O, Eriksson, F, Faitsch, M, Falchetto, G, Farnik, M, Fasoli, A, Fedorczak, N, Felici, F, Fevrier, O, Ficker, O, Fil, A, Fontana, M, Fransson, E, Frassinetti, L, Furno, I, Gahle, D, Galassi, D, Galazka, K, Galperti, C, Garavaglia, S, Garcia-Munoz, M, Geiger, B, Giacomin, M, Giruzzi, G, Gobbin, M, Golfinopoulos, T, Goodman, T, Gorno, S, Granucci, G, Graves, J, Griener, M, Gruca, M, Gyergyek, T, Haelterman, R, Hakola, A, Han, W, Happel, T, Harrer, G, Harrison, J, Henderson, S, Hogeweij, G, Hogge, J, Hoppe, M, Horacek, J, Huang, Z, Iantchenko, A, Innocente, P, Insulander Bjork, K, Ionita-Schrittweiser, C, Isliker, H, Jardin, A, Jaspers, R, Karimov, R, Karpushov, A, Kazakov, Y, Komm, M, Kong, M, Kovacic, J, Krutkin, O, Kudlacek, O, Kumar, U, Kwiatkowski, R, Labit, B, Laguardia, L, Lammers, J, Laribi, E, Laszynska, E, Lazaros, A, Linder, O, Linehan, B, Lipschultz, B, Llobet, X, Loizu, J, Lunt, T, Macusova, E, Marandet, Y, Maraschek, M, Marceca, G, Marchetto, C, Marchioni, S, Marmar, E, Martin, Y, Martinelli, L, Matos, F, Maurizio, R, Mayoral, M, Mazon, D, Menkovski, V, Merle, A, Merlo, G, Meyer, H, Mikszuta-Michalik, K, Molina Cabrera, P, Morales, J, Moret, J, Moro, A, Moulton, D, Muhammed, H, Myatra, O, Mykytchuk, D, Napoli, F, Nem, R, Nielsen, A, Nocente, M, Nowak, S, Offeddu, N, Olsen, J, Orsitto, F, Pan, O, Papp, G, Pau, A, Perek, A, Pesamosca, F, Peysson, Y, Pigatto, L, Piron, C, Poradzinski, M, Porte, L, Putterich, T, Rabinski, M, Raj, H, Rasmussen, J, Ratta, G, Ravensbergen, T, Ricci, D, Ricci, P, Rispoli, N, Riva, F, Rivero-Rodriguez, J, Salewski, M, Sauter, O, Schmidt, B, Schrittweiser, R, Sharapov, S, Sheikh, U, Sieglin, B, Silva, M, Smolders, A, Snicker, A, Sozzi, C, Spolaore, M, Stagni, A, Stipani, L, Sun, G, Tala, T, Tamain, P, Tanaka, K, Tema Biwole, A, Terranova, D, Terry, J, Testa, D, Theiler, C, Thornton, A, Thrysoe, A, Torreblanca, H, Tsui, C, Vaccaro, D, Vallar, M, Van Berkel, M, Van Eester, D, Van Kampen, R, Van Mulders, S, Verhaegh, K, Verhaeghe, T, Vianello, N, Villone, F, Viezzer, E, Vincent, B, Voitsekhovitch, I, Vu, N, Walkden, N, Wauters, T, Weisen, H, Wendler, N, Wensing, M, Widmer, F, Wiesen, S, Wischmeier, M, Wijkamp, T, Wunderlich, D, Wuthrich, C, Yanovskiy, V, Zebrowski, J, Reimerdes H., Agostini M., Alessi E., Alberti S., Andrebe Y., Arnichand H., Balbin J., Bagnato F., Baquero-Ruiz M., Bernert M., Bin W., Blanchard P., Blanken T. C., Boedo J. A., Brida D., Brunner S., Bogar C., Bogar O., Bolzonella T., Bombarda F., Bouquey F., Bowman C., Brunetti D., Buermans J., Bufferand H., Calacci L., Camenen Y., Carli S., Carnevale D., Carpanese F., Causa F., Cavalier J., Cavedon M., Cazabonne J. A., Cerovsky J., Chandra R., Chandrarajan Jayalekshmi A., Chellai O., Chmielewski P., Choi D., Ciraolo G., Classen I. G. J., Coda S., Colandrea C., Dal Molin A., David P., De Baar M. R., Decker J., Dekeyser W., De Oliveira H., Douai D., Dreval M., Dunne M. G., Duval B. P., Elmore S., Embreus O., Eriksson F., Faitsch M., Falchetto G., Farnik M., Fasoli A., Fedorczak N., Felici F., Fevrier O., Ficker O., Fil A., Fontana M., Fransson E., Frassinetti L., Furno I., Gahle D. S., Galassi D., Galazka K., Galperti C., Garavaglia S., Garcia-Munoz M., Geiger B., Giacomin M., Giruzzi G., Gobbin M., Golfinopoulos T., Goodman T., Gorno S., Granucci G., Graves J. P., Griener M., Gruca M., Gyergyek T., Haelterman R., Hakola A., Han W., Happel T., Harrer G., Harrison J. R., Henderson S., Hogeweij G. M. D., Hogge J. -P., Hoppe M., Horacek J., Huang Z., Iantchenko A., Innocente P., Insulander Bjork K., Ionita-Schrittweiser C., Isliker H., Jardin A., Jaspers R. J. E., Karimov R., Karpushov A. N., Kazakov Y., Komm M., Kong M., Kovacic J., Krutkin O., Kudlacek O., Kumar U., Kwiatkowski R., Labit B., Laguardia L., Lammers J. T., Laribi E., Laszynska E., Lazaros A., Linder O., Linehan B., Lipschultz B., Llobet X., Loizu J., Lunt T., Macusova E., Marandet Y., Maraschek M., Marceca G., Marchetto C., Marchioni S., Marmar E. S., Martin Y., Martinelli L., Matos F., Maurizio R., Mayoral M. -L., Mazon D., Menkovski V., Merle A., Merlo G., Meyer H., Mikszuta-Michalik K., Molina Cabrera P. A., Morales J., Moret J. -M., Moro A., Moulton D., Muhammed H., Myatra O., Mykytchuk D., Napoli F., Nem R. D., Nielsen A. H., Nocente M., Nowak S., Offeddu N., Olsen J., Orsitto F. P., Pan O., Papp G., Pau A., Perek A., Pesamosca F., Peysson Y., Pigatto L., Piron C., Poradzinski M., Porte L., Putterich T., Rabinski M., Raj H., Rasmussen J. J., Ratta G. A., Ravensbergen T., Ricci D., Ricci P., Rispoli N., Riva F., Rivero-Rodriguez J. F., Salewski M., Sauter O., Schmidt B. S., Schrittweiser R., Sharapov S., Sheikh U. A., Sieglin B., Silva M., Smolders A., Snicker A., Sozzi C., Spolaore M., Stagni A., Stipani L., Sun G., Tala T., Tamain P., Tanaka K., Tema Biwole A., Terranova D., Terry J. L., Testa D., Theiler C., Thornton A., Thrysoe A., Torreblanca H., Tsui C. K., Vaccaro D., Vallar M., Van Berkel M., Van Eester D., Van Kampen R. J. R., Van Mulders S., Verhaegh K., Verhaeghe T., Vianello N., Villone F., Viezzer E., Vincent B., Voitsekhovitch I., Vu N. M. T., Walkden N., Wauters T., Weisen H., Wendler N., Wensing M., Widmer F., Wiesen S., Wischmeier M., Wijkamp T. A., Wunderlich D., Wuthrich C., Yanovskiy V., and Zebrowski J.
Abstract: The tokamak à configuration variable (TCV) continues to leverage its unique shaping capabilities, flexible heating systems and modern control system to address critical issues in preparation for ITER and a fusion power plant. For the 2019-20 campaign its configurational flexibility has been enhanced with the installation of removable divertor gas baffles, its diagnostic capabilities with an extensive set of upgrades and its heating systems with new dual frequency gyrotrons. The gas baffles reduce coupling between the divertor and the main chamber and allow for detailed investigations on the role of fuelling in general and, together with upgraded boundary diagnostics, test divertor and edge models in particular. The increased heating capabilities broaden the operational regime to include Te/Ti ∼1 and have stimulated refocussing studies from L-mode to H-mode across a range of research topics. ITER baseline parameters were reached in type-I ELMy H-modes and alternative regimes with 'small' (or no) ELMs explored. Most prominently, negative triangularity was investigated in detail and confirmed as an attractive scenario with H-mode level core confinement but an L-mode edge. Emphasis was also placed on control, where an increased number of observers, actuators and control solutions became available and are now integrated into a generic control framework as will be needed in future devices. The quantity and quality of results of the 2019-20 TCV campaign are a testament to its successful integration within the European research effort alongside a vibrant domestic programme and international collaborations.
Published: 2022

25. The dependence of confinement on the isotope mass in the core and the edge of AUG and JET-ILW H-mode plasmas

Author: Schneider, P, Angioni, C, Frassinetti, L, Horvath, L, Maslov, M, Auriemma, F, Cavedon, M, Challis, C, Delabie, E, Dunne, M, Climent, J, Hobirk, J, Kappatou, A, Keeling, D, Kurzan, B, Lennholm, M, Lomanowski, B, Maggi, C, Mcdermott, R, Putterich, T, Thorman, A, Willensdorfer, M, Schneider P. A., Angioni C., Frassinetti L., Horvath L., Maslov M., Auriemma F., Cavedon M., Challis C. D., Delabie E., Dunne M. G., Climent J. M. F., Hobirk J., Kappatou A., Keeling D. L., Kurzan B., Lennholm M., Lomanowski B., Maggi C. F., McDermott R. M., Putterich T., Thorman A., Willensdorfer M., Schneider, P, Angioni, C, Frassinetti, L, Horvath, L, Maslov, M, Auriemma, F, Cavedon, M, Challis, C, Delabie, E, Dunne, M, Climent, J, Hobirk, J, Kappatou, A, Keeling, D, Kurzan, B, Lennholm, M, Lomanowski, B, Maggi, C, Mcdermott, R, Putterich, T, Thorman, A, Willensdorfer, M, Schneider P. A., Angioni C., Frassinetti L., Horvath L., Maslov M., Auriemma F., Cavedon M., Challis C. D., Delabie E., Dunne M. G., Climent J. M. F., Hobirk J., Kappatou A., Keeling D. L., Kurzan B., Lennholm M., Lomanowski B., Maggi C. F., McDermott R. M., Putterich T., Thorman A., and Willensdorfer M.
Abstract: Experiments in ASDEX Upgrade (AUG) and JET with the ITER-like wall (JET-ILW) are performed to separate the pedestal and core contributions to confinement in H-modes with different main ion masses. A strong isotope mass dependence in the pedestal is found which is enhanced at high gas puffing. This is because the ELM type changes when going from D to H for matched engineering parameters, which is likely due to differences in the inter ELM transport with isotope mass. The pedestal can be matched in H and D plasmas by varying only the triangularity and keeping the engineering parameters relevant for core transport the same. With matched pedestals Astra/TGLF (Sat1geo) core transport simulations predict the experimental profiles equally well for H and D. These core transport simulations show a negligible mass dependence and no gyro-Bohm scaling is observed. However, to match the experimental observations at medium ß it is required to take the fast-ion dilution and rotation into account. This is not enough for high ß plasmas where for the first time a profile match between H and D plasmas was achieved experimentally. Under these conditions quasilinear modelling with TGLF over predicts the transport in the core of H and D plasmas alike.
Published: 2022

26. Testing a prediction model for the H-mode density pedestal against JET-ILW pedestals

Author: Saarelma, S., primary, Connor, J.W., additional, Bilkova, P., additional, Bohm, P., additional, Field, A.R., additional, Frassinetti, L., additional, Fridstrom, R., additional, and Kirk, A., additional
Published: 2023
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27. Pedestal particle balance studies in JET-ILW H-mode plasmas

Author: Horvath, L, primary, Lomanowski, B, additional, Karhunen, J, additional, Maslov, M, additional, Schneider, P A, additional, Simpson, J, additional, Brix, M, additional, Chapman-Oplopoiou, B, additional, Corrigan, G, additional, Frassinetti, L, additional, Groth, M, additional, Lawson, K, additional, Maggi, C F, additional, Menmuir, S, additional, Morales, R B, additional, Moulton, D, additional, Myatra, O, additional, Nina, D, additional, Pereira, T, additional, Réfy, D I, additional, Saarelma, S, additional, and Vécsei, M, additional
Published: 2023
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28. Investigation of the dependence of pe,ped on ne,sep in JET H-Mode plasmas using integrated JETTO-MISHKA-FRANTIC simulations

Author: Simpson, J., primary, Moulton, D., additional, Giroud, C., additional, Groth, M., additional, Horvath, L., additional, Casson, F.J., additional, Kochl, F., additional, Frassinetti, L., additional, Corrigan, G., additional, Saarelma, S., additional, Garzotti, L., additional, Gahle, D.S., additional, and Chankin, A., additional
Published: 2023
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29. Multi-code estimation of DTT edge transport parameters

Author: Balbinot, L., primary, Rubino, G., additional, Casiraghi, I., additional, Meineri, C., additional, Frassinetti, L., additional, Aucone, L., additional, Mantica, P., additional, Innocente, P., additional, and Wigram, M., additional
Published: 2023
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30. Developing deep learning algorithms for inferring upstream separatrix density at JET

Author: Kit, A., primary, Järvinen, A.E., additional, Wiesen, S., additional, Poels, Y., additional, and Frassinetti, L., additional
Published: 2023
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31. The JET hybrid scenario in Deuterium, Tritium and Deuterium-Tritium

Author: 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
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32. Modelling performed for predictions of fusion power in JET DTE2: overview and lessons learnt

Author: Garcia, J, Casson, F, Frassinetti, L, Gallart, D, Garzotti, L, Kim, H, Nocente, M, Saarelma, S, Auriemma, F, Ferreira, J, Gabriellini, S, Ho, A, Huynh, P, Kirov, K, Lerche, E, Mantsinen, M, Zotta, V, Stancar, Z, Taylor, D, Van Eester, D, Challis, C, Casson, FJ, Kim, HT, Kirov, KK, Mantsinen, MJ, Zotta, VK, Taylor, DMA, Challis, CD, Garcia, J, Casson, F, Frassinetti, L, Gallart, D, Garzotti, L, Kim, H, Nocente, M, Saarelma, S, Auriemma, F, Ferreira, J, Gabriellini, S, Ho, A, Huynh, P, Kirov, K, Lerche, E, Mantsinen, M, Zotta, V, Stancar, Z, Taylor, D, Van Eester, D, Challis, C, Casson, FJ, Kim, HT, Kirov, KK, Mantsinen, MJ, Zotta, VK, Taylor, DMA, and Challis, CD
Abstract: For more than a decade, an unprecedented predict-first activity has been carried in order to predict the fusion power and provide guidance to the second Deuterium-Tritium (D-T) campaign performed at JET in 2021 (DTE2). Such an activity has provided a framework for a broad model validation and development towards the D-T operation. It is shown that it is necessary to go beyond projections using scaling laws in order to obtain detailed physics based predictions. Furthermore, mixing different modelling complexity and promoting an extended interplay between modelling and experiment are essential towards reliable predictions of D-T plasmas. The fusion power obtained in this predict-first activity is in broad agreement with the one finally measured in DTE2. Implications for the prediction of fusion power in future devices, such as ITER, are discussed.
Published: 2023

33. L-H transition studies in tritium and deuterium-tritium campaigns at JET with Be wall and W divertor

Author: 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

34. Developing deep learning algorithms for inferring upstream separatrix density at JET

Author: Kit, A., Järvinen, A.E., Wiesen, S., Poels, Y., Frassinetti, L., JET Contributors, Kit, A., Järvinen, A.E., Wiesen, S., Poels, Y., Frassinetti, L., and JET Contributors
Abstract: Predictive and real-time inference capability for the upstream separatrix electron density, ne, sep, is essential for design and control of core-edge integrated plasma scenarios. In this study, both supervised and semi-supervised machine learning algorithms are explored to establish direct mapping as well as indirect compressed representation of the pedestal profiles for predictions and inference of ne, sep. Based on the EUROfusion pedestal database for JET (Frassinetti et al., 2021), a tabular dataset was created, consisting of machine parameters, fraction of ELM cycle, high resolution Thomson scattering profiles of electron density and temperature, and ne, sep for 608 JET shots. Using the tabular dataset, the direct mapping approach provides a mapping of machine parameters and ELM percentage to ne, sep. Through representation learning, a compressed representation of the experimental pedestal electron density and temperature profiles is established. By conditioning the representation with machine control parameters, a probabilistic generative predictive model is established. For prediction, the machine parameters can be used to establish a conditional distribution of the compressed pedestal profiles, and the decoder that is trained as part of the algorithm can be used to decode the compressed representation back to full pedestal profiles. Although, in this work, a proof-of-principle for predicting and inferring ne, sep is given, such a representation learning can be used also for many other applications as the full pedestal profile is predicted. An implementation of this work can be found at https://github.com/fusionby2030/psi_2022.
Published: 2023

35. RF power as key contributor to high performance "baseline" scenario experiments in JET DD and DT plasmas in preparation for ITER.

Author: 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
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36. 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: 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 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. [ABSTRACT FROM AUTHOR]
Published: 2023
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37. Isotope physics of heat and particle transport with tritium in JET-ILW type-I ELMy H-mode plasmas.

Author: 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.
Subjects: 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
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38. Modelling performed for predictions of fusion power in JET DTE2: overview and lessons learnt.

Author: Garcia, J., Casson, F.J., Frassinetti, L., Gallart, D., Garzotti, L., Kim, H.-T., Nocente, M., Saarelma, S., Auriemma, F., Ferreira, J., Gabriellini, S., Ho, A., Huynh, P., Kirov, K.K., Lerche, E., Mantsinen, M.J., Zotta, V.K., Stancar, Z., Taylor, D.M.A., and Van Eester, D.
Subjects: PREDICTION models, MODEL validation
Abstract: For more than a decade, an unprecedented predict-first activity has been carried in order to predict the fusion power and provide guidance to the second Deuterium–Tritium (D–T) campaign performed at JET in 2021 (DTE2). Such an activity has provided a framework for a broad model validation and development towards the D–T operation. It is shown that it is necessary to go beyond projections using scaling laws in order to obtain detailed physics based predictions. Furthermore, mixing different modelling complexity and promoting an extended interplay between modelling and experiment are essential towards reliable predictions of D–T plasmas. The fusion power obtained in this predict-first activity is in broad agreement with the one finally measured in DTE2. Implications for the prediction of fusion power in future devices, such as ITER, are discussed. [ABSTRACT FROM AUTHOR]
Published: 2023
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39. Supervised learning approaches to modeling pedestal density

Author: Kit, A, primary, Järvinen, A E, additional, Frassinetti, L, additional, and Wiesen, S, additional
Published: 2023
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40. Parameter dependencies of the separatrix density in low triangularity L-mode and H-mode JET-ILW plasmas

Author: Lomanowski, B., primary, Rubino, G., additional, Uccello, A., additional, Dunne, M., additional, Vianello, N., additional, Aleiferis, S., additional, Canik, J., additional, Carvalho, I., additional, Corrigan, G., additional, Frassinetti, L., additional, Frigione, D., additional, Garzotti, L., additional, Groth, M., additional, Meigs, A., additional, Maslov, M., additional, von Thun, C. Perez, additional, Rimini, F., additional, Schneider, P.A., additional, Sergienko, G., additional, Simpson, J., additional, and Van Eester, D., additional
Published: 2023
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41. Isotope mass dependence of pedestal transport in JET H-mode plasmas

Author: Predebon, I., primary, Hatch, D.R., additional, Frassinetti, L., additional, Horvath, L., additional, Saarelma, S., additional, Chapman-Oplopoiou, B., additional, Görler, T., additional, and Maggi, C.F., additional
Published: 2023
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42. Validation of IMEP on Alcator C-Mod and JET-ILW ELMy H-mode plasmas

Author: Luda, T, primary, Angioni, C, additional, Dunne, M G, additional, Fable, E, additional, Kallenbach, A, additional, Bonanomi, N, additional, Schneider, P A, additional, Siccinio, M, additional, Tardini, G, additional, Rodriguez-Fernandez, P, additional, Hughes, J W, additional, Howard, N, additional, Frassinetti, L, additional, Saarelma, S, additional, Upgrade Team, The ASDEX, additional, MST1 Team, The EUROfusion, additional, C-Mod Team, The Alcator, additional, and contributors, JET, additional
Published: 2023
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43. Investigation of the influence of divertor recycling on global plasma confinement in JET ITER-like wall

Author: Tamain, P., Joffrin, E., Bufferand, H., Järvinen, A., Brezinsek, S., Ciraolo, G., Delabie, E., Frassinetti, L., Giroud, C., Groth, M., Lipschultz, B., Lomas, P., Marsen, S., Menmuir, S., Oberkofler, M., Stamp, M., Wiesen, S., and JET EFDA contributors
Published: 2015
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44. Thermal analysis of an exposed tungsten edge in the JET divertor

Author: Arnoux, G., Coenen, J., Bazylev, B., Corre, Y., Matthews, G.F., Balboa, I., Clever, M., Dejarnac, R., Devaux, S., Eich, T., Gauthier, E., Frassinetti, L., Horacek, J., Jachmich, S., Kinna, D., Marsen, S., Mertens, Ph., Pitts, R.A., Rack, M., Sergienko, G., Sieglin, B., Stamp, M., and Thompson, V.
Published: 2015
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45. ELM induced tungsten melting and its impact on tokamak operation

Author: Coenen, J.W., Arnoux, G., Bazylev, B., Matthews, G.F., Jachmich, S., Balboa, I., Clever, M., Dejarnac, R., Coffey, I., Corre, Y., Devaux, S., Frassinetti, L., Gauthier, E., Horacek, J., Knaup, M., Komm, M., Krieger, K., Marsen, S., Meigs, A., Mertens, Ph., Pitts, R.A., Puetterich, T., Rack, M., Stamp, M., Sergienko, G., Tamain, P., and Thompson, V.
Published: 2015
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46. Investigation of the dependence of pe,ped on ne,sep in JET H-Mode plasmas using integrated JETTO-MISHKA-FRANTIC simulations

Author: Simpson, J., Moulton, D., Giroud, C., Groth, M., Horvath, L., Casson, F., Kochl, F., Frassinetti, L., Corrigan, G., Saarelma, S., Garzotti, L., Gahle, D., Chankin, A., and JET Contributors
Published: 2023

47. ELM and inter-ELM tungsten erosion sources in high-power, JET ITER-like wall H-mode plasmas

Author: Kumpulainen, H. A., Groth, M., Brezinsek, S., Corrigan, G., Frassinetti, L., Harting, D., Koechl, F., Karhunen, J., Meigs, A. G., O'Mullane, M., Romazanov, J., JET Contributors, Department of Applied Physics, Fusion and Plasma Physics, Forschungszentrum Jülich, Culham Science Centre, KTH Royal Institute of Technology, Aalto-yliopisto, and Aalto University
Subjects: Erosion, JET, JINTRAC, ERO2.0, Edge-localised mode, Spectroscopy, Tungsten
Abstract: Funding Information: This work has been carried out within the framework of the EUROfusion Consortium, funded by the European Union via the Euratom Research and Training Programme (Grant Agreement No 101052200 — EUROfusion). Views and opinions expressed are however those of the author(s) only and do not necessarily reflect those of the European Union or the European Commission. Neither the European Union nor the European Commission can be held responsible for them. The ERO2.0 simulations utilised computing resources provided by the Science-IT project at Aalto University. Funding Information: This work has been carried out within the framework of the EUROfusion Consortium, funded by the European Union via the Euratom Research and Training Programme (Grant Agreement No 101052200 — EUROfusion). Views and opinions expressed are however those of the author(s) only and do not necessarily reflect those of the European Union or the European Commission. Neither the European Union nor the European Commission can be held responsible for them. The ERO2.0 simulations utilised computing resources provided by the Science-IT project at Aalto University. Publisher Copyright: © 2022 The Author(s) Simulations of JET ITER-like wall high-confinement mode plasmas, including type-I edge-localised modes (ELMs), using JINTRAC for the background plasmas and ERO2.0 for tungsten erosion and transport, predict virtually perfect screening of the primary W erosion sources at the divertor targets during both the ELM and inter-ELM phases. The largest source of W influx to the main plasma is predicted to be the outer vertical divertor due to sputtering by energetic fuel (D, T) atoms from charge-exchange reactions. ERO2.0 predictions accurately reproduce the measured W I emission in the low-field side divertor, but underpredict the W II emission by a factor of 10. Potential reasons for the W II discrepancy include uncertainties in the atomic data, assumptions on the sheath properties and the sputtering angle distribution, and the impact of metastable states.
Published: 2022

48. Effect of resistivity on the pedestal MHD stability in JET

Author: Nyström, H., primary, Frassinetti, L., additional, Saarelma, S., additional, Huijsmans, G.T.A., additional, Perez von Thun, C., additional, Maggi, C.F., additional, Hillesheim, J.C., additional, and contributors, JET, additional
Published: 2022
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49. Scenario modelling for the Divertor Tokamak Test facility

Author: Casiraghi, I., Mantica, P., Ambrosino, R., Aucone, L., Baiocchi, B., Balbinot, L., Castaldo, A., Citrin, J., Frassinetti, L., Innocente, P., Kochl, F., Mariani, A., Agostinetti, P., Ceccuzzi, S., Figini, L., Granucci, G., Valisa, M., Casiraghi, I, Mantica, P, Ambrosino, R, Aucone, L, Baiocchi, B, Balbinot, L, Castaldo, A, Citrin, J, Frassinetti, L, Innocente, P, Koechl, F, Mariani, A, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, and Valisa, M
Subjects: integrated modelling, Divertor Tokamak Test facility, DTT, quasi-linear transport models
Abstract: The scenario integrated modelling is a top priority work during the design of a new tokamak, as the Divertor Tokamak Test facility (DTT) under construction at the ENEA Research Center in Frascati. The first simulations of the main baseline scenarios contributed to the optimization of the DTT project, particularly with regard to the machine size and heating systems, besides serving as reference for diagnostics design. In this paper we report the first simulations of the full power baseline scenario in the final configuration of the machine and heating mix.
Published: 2022

50. Predict–first scenario modelling in support of the design of the Divertor Tokamak Test facility

Author: Casiraghi I., Mantica P., Ambrosino R., Aucone L., Auriemma F., Baiocchi B., Balbinot L., Barberis T., Bonanomi N., Castaldo A., Citrin J., Frassinetti L., Innocente P., Koechl F., Mariani A., Nowak S., Agostinetti P., Ceccuzzi S., Figini L., Granucci G., Valisa M., Casiraghi, I, Mantica, P, Ambrosino, R, Aucone, L, Auriemma, F, Baiocchi, B, Balbinot, L, Barberis, T, Bonanomi, N, Castaldo, A, Citrin, J, Frassinetti, L, Innocente, P, Koechl, F, Mariani, A, Nowak, S, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, and Valisa, M
Subjects: Predict–first scenario modelling, Divertor Tokamak Test facility, DTT, quasi-linear trasnport models
Published: 2022

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