1,274 results on '"Dux, R."'
Search Results
2. Inference of Experimental Radial Impurity Transport on Alcator C-Mod: Bayesian Parameter Estimation and Model Selection
- Author
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Sciortino, F., Howard, N. T., Marmar, E. S., Odstrcil, T., Cao, N. M., Dux, R., Hubbard, A. E., Hughes, J. W., Irby, J. H., Marzouk, Y., Milanese, L. M., Reinke, M. L., Rice, J. E., and Rodriguez-Fernandez, P.
- Subjects
Physics - Plasma Physics ,Physics - Applied Physics ,Physics - Computational Physics ,Physics - Data Analysis, Statistics and Probability - Abstract
We present a fully Bayesian approach for the inference of radial profiles of impurity transport coefficients and compare its results to neoclassical, gyrofluid and gyrokinetic modeling. Using nested sampling, the Bayesian Impurity Transport InferencE (BITE) framework can handle complex parameter spaces with multiple possible solutions, offering great advantages in interpretative power and reliability with respect to previously demonstrated methods. BITE employs a forward model based on the pySTRAHL package, built on the success of the well-known STRAHL code [Dux, IPP Report, 2004], to simulate impurity transport in magnetically-confined plasmas. In this paper, we focus on calcium (Ca, Z=20) Laser Blow-Off injections into Alcator C-Mod plasmas. Multiple Ca atomic lines are diagnosed via high-resolution X-ray Imaging Crystal Spectroscopy and Vacuum Ultra-Violet measurements. We analyze a sawtoothing I-mode discharge for which neoclassical and turbulent (quasilinear and nonlinear) predictions are also obtained. We find good agreement in diffusion across the entire radial extent, while turbulent convection and density profile peaking are estimated to be larger in experiment than suggested by theory. Efforts and challenges associated with the inference of experimental pedestal impurity transport are discussed., Comment: 38 pages, 19 figures, submitted for publication in Nuclear Fusion
- Published
- 2020
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3. FIB line marking as a tool for local erosion/deposition/fuzz formation measurements in ASDEX Upgrade during the He campaign
- Author
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Rasiński, M., Brezinsek, S., Kreter, A., Dittmar, T., Krieger, K., Balden, M., de Marne, P., Dux, R., Faitsch, M., Hakola, A., Likonen, J., Tsitrone, E., and Rohde, V.
- Published
- 2023
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4. Performance of a liquid Sn divertor target during ASDEX upgrade L-mode and H-mode operation
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Scholte, J.G.A., Balden, M., Brida, D., Cecrdle, J., Dux, R., Elgeti, S., Faitsch, M., Herrmann, A., Horacek, J., Hunger, K., Krieger, K., Manhard, A., de Marné, P., Rohde, V., and Morgan, T.W.
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- 2023
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5. Admixed pellets for fast and efficient delivery of plasma enhancement gases: Investigations at AUG exploring the option for EU-DEMO
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Lang, P.T., Baylor, L.R., Day, Ch., Dux, R., McDermott, R.M., Giegerich, T., Gleiter, T., Kallenbach, A., Ploeckl, B., Rohde, V., and Zito, A.
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- 2023
- Full Text
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6. The radial localization of the transition from low to high confinement mode in the ASDEX Upgrade tokamak
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Cavedon, M, Happel, T, Hennequin, P, Dux, R, Hofler, K, Plank, U, Putterich, T, Stroth, U, Viezzer, E, Wolfrum, E, Cavedon M., Happel T., Hennequin P., Dux R., Hofler K., Plank U., Putterich T., Stroth U., Viezzer E., Wolfrum E., Cavedon, M, Happel, T, Hennequin, P, Dux, R, Hofler, K, Plank, U, Putterich, T, Stroth, U, Viezzer, E, Wolfrum, E, Cavedon M., Happel T., Hennequin P., Dux R., Hofler K., Plank U., Putterich T., Stroth U., Viezzer E., and Wolfrum E.
- Abstract
A novel experimental method is applied to localize the initial suppression of turbulence, in the form of density fluctuations, at the transition from the low (L-) to the high (H-) confinement mode in toroidal magnetic fusion plasmas. The high radial and temporal resolution, combined with the unprecedented statistical significance, provided the awaited information on a possible dominant E × B shear layer in L-H transition physics. We show, for the first time, that the H-mode turbulence suppression is initiated at the inner E × B shear layer in the ASDEX Upgrade tokamak possibly shedding light on the causality behind the L-H transition process.
- Published
- 2024
7. Comparison of reduced model predictions for divertor detachment onset and reattachment timescales in ASDEX Upgrade and JET experiments
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Henderson, S, Bernert, M, Brida, D, Cavedon, M, David, P, Dux, R, Fevrier, O, Jacquet, P, Jarvinen, A, Kallenbach, A, Karhunen, J, Kirov, K, Komm, M, Lennholm, M, Lomanowski, B, Lowry, C, Mcdermott, R, Meigs, A, Reimerdes, H, Sun, H, Thomas, B, Henderson S. S., Bernert M., Brida D., Cavedon M., David P., Dux R., Fevrier O., Jacquet P., Jarvinen A., Kallenbach A., Karhunen J., Kirov K., Komm M., Lennholm M., Lomanowski B., Lowry C., McDermott R., Meigs A., Reimerdes H., Sun H., Thomas B., Henderson, S, Bernert, M, Brida, D, Cavedon, M, David, P, Dux, R, Fevrier, O, Jacquet, P, Jarvinen, A, Kallenbach, A, Karhunen, J, Kirov, K, Komm, M, Lennholm, M, Lomanowski, B, Lowry, C, Mcdermott, R, Meigs, A, Reimerdes, H, Sun, H, Thomas, B, Henderson S. S., Bernert M., Brida D., Cavedon M., David P., Dux R., Fevrier O., Jacquet P., Jarvinen A., Kallenbach A., Karhunen J., Kirov K., Komm M., Lennholm M., Lomanowski B., Lowry C., McDermott R., Meigs A., Reimerdes H., Sun H., and Thomas B.
- Abstract
Building on prior analysis of ASDEX Upgrade (AUG) experiments (Henderson et al 2023 Nucl. Fusion 63 086024), this study compares simple analytical formula predictions for divertor detachment onset and reattachment timescales in JET experiments. Detachment onset primarily scales with divertor neutral pressure, impurity concentration, power directed to the targets, machine size, and integral perpendicular power decay length. JET experiments, focusing on seeding mixtures of Ne and Ar, align with the detachment onset predictions. Radiation efficiencies among the impurities show good agreement with the model predictions, contrasting with AUG observations which suggested higher efficiency for Ar and lower efficiency for Ne. The time taken to re-ionise the neutral volume in front of the outer target in fully detached divertor conditions was measured following both abrupt increases in injected neutral beam power and, separately, cutting of the impurity gas flow. Re-ionisation of the neutrals occurs within approximately 1 s on JET, which aligns with the simple model prediction derived from AUG data. While the AUG results are not new, their comparison with the JET results enhances understanding, reinforcing confidence in using simple models to predict future reactor scenarios.
- Published
- 2024
8. Poloidal structure of the edge parallel flow in H-mode, L-mode and I-mode confinement regimes
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Cruz-Zabala, D, Viezzer, E, Cano-Megias, P, Cavedon, M, Dux, R, Plank, U, Pütterich, T, Mckay, K, Rodriguez-Gonzalez, A, Garcia-Munoz, M, Cruz-Zabala D. J., Viezzer E., Cano-Megias P., Cavedon M., Dux R., Plank U., Pütterich T., McKay K., Rodriguez-Gonzalez A., Garcia-Munoz M., Cruz-Zabala, D, Viezzer, E, Cano-Megias, P, Cavedon, M, Dux, R, Plank, U, Pütterich, T, Mckay, K, Rodriguez-Gonzalez, A, Garcia-Munoz, M, Cruz-Zabala D. J., Viezzer E., Cano-Megias P., Cavedon M., Dux R., Plank U., Pütterich T., McKay K., Rodriguez-Gonzalez A., and Garcia-Munoz M.
- Abstract
Impurity profiles have been measured with the edge high field side (HFS) and low field side (LFS) charge exchange recombination spectroscopy suite at ASDEX Upgrade enabling the study of the poloidal structure of the edge parallel flow in H-mode, L-mode and I-mode. In H-mode, asymmetries in the impurity density, toroidal and poloidal rotations are found. In I-mode, only toroidal rotation asymmetries have been measured while in L-mode no asymmetries have been observed. The measured parallel flow can be divided in two components, the Pfirsch-Schlüter (PS) flow and the symmetric flow. Two different methods have been followed to determine both contributions to the parallel flow. The first method is based on the calculation of the PS flow at the HFS and LFS from the radial electric field. The second method directly provides the symmetric flow from the flux surface average (FSA) of the parallel flow. In H-mode, the methods provide different results, while in L-mode and I-mode they agree. The differences observed in H-mode between the two methods could be explained by the existence of asymmetries in the impurity density, by the non-negligible particle sources and radial losses, or by the approximations made in the calculation of the FSA of the parallel flow from measurements in two poloidal positions (midplane HFS and LFS) only.
- Published
- 2024
9. Characterization of highly radiating nitrogen-seeded H-mode plasmas in unfavorable B T at ASDEX Upgrade.
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Chen, L., Wolfrum, E., Pan, O., Kurzan, B., Bernert, M., Brida, D., Cavedon, M., Dux, R., Fischer, R., Griener, M., Grover, O., Plank, U., Stieglitz, D., and Zito, A.
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DEUTERIUM ions ,ELECTRON density ,ELECTRON temperature ,PLASMA confinement ,GRANULAR flow ,THOMSON scattering ,NITROGEN plasmas - Abstract
The highly radiating nitrogen-seeded H-mode plasmas in unfavorable B
T has been characterized in the ASDEX Upgrade tokamak (AUG). Three levels of nitrogen puffing rates have been injected into a fully detached H-mode plasma, which is run in lower single null configuration with the ion B × ∇ B drift away from the X-point. A cold ( ∼ 1 − 2 eV) highly radiating ( ∼ 13.0 MW m − 3 ) region forms close to the X-point immediately after nitrogen seeding, as evidenced by measurements of the divertor Thomson scattering (DTS) and the two-dimensional bolometry reconstructions. In addition, the radiator moves further upwards above the X-point along the separatrix at the high-field side (HFS) with increasing nitrogen puffing rates, as evidenced by the Absolute eXtended UltraViolet (AXUV) measurements. The formation of the highly radiating regime is closely correlated to the modifications of the divertor plasma conditions. Along the line of sight of the DTS measurement, the electron temperature reduces down to a few eV, which initials near the X-point and further extends to the HFS scrape-off layer (SOL) simultaneously with the upward movement of the radiator, however, the electron temperature sustains ( ∼ 30 − 50 eV) at the low-field side (LFS) SOL with slightly decreased electron density. The highly radiating regime shows LFS/HFS divertor asymmetry, in contrast to that for H-mode plasmas in favorable BT , suggesting that the drifts play an important role for the formation of the highly radiating X-point regime at AUG. The neutral particle flux increases significantly (factor of ∼ 2 ) in the private flux region, while it increases slightly ( < 20 % ) in the main chamber, thus suggesting an enhanced sub-divertor neutral compression with the formation of the highly radiating regime. Furthermore, a degradation of the pedestal electron density was observed with an enhancement of the electron temperature further inside the pedestal, and complete divertor detachment was achieved by nitrogen seeding with sustained plasma confinement. Finally, particle sources and flow patterns of deuterium and nitrogen ions have been analyzed by SOLPS-ITER modelling, confirming that the E × B drift plays an important role for the formation of the highly radiating regime in unfavorable BT at AUG. [ABSTRACT FROM AUTHOR]- Published
- 2024
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10. Thermal helium beam diagnostic for 2D profile measurements in the divertor of ASDEX Upgrade.
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Hörmann, S., Cavedon, M., Griener, M., Wendler, D., Dux, R., Schmid, K., Kappatou, A., Wischmeier, M., Cruz-Zabala, D. J., Viezzer, E., and Stroth, U.
- Abstract
A new thermal helium beam diagnostic has been implemented in the outer lower divertor of the ASDEX Upgrade tokamak. The purpose of this diagnostic is to measure two-dimensional profiles of electron density (n
e ) and temperature (Te ) with high temporal and spatial resolution. The geometry of the lines of sight is chosen to avoid the influence of prompt recycling and to optimize the resolution without significantly impacting the divertor structure. Moreover, the effect of long-term helium recycling has been analyzed, and its amplitude compared to the active signal is negligible. Finally, the reconstruction of ne and Te is done via a collisional radiative model, while a static and a dynamic model were implemented and compared with SOLPS simulations as well as divertor Thomson scattering data. Furthermore, a new 2D parameterization of the outer divertor volume, which is required for the dynamic model, was developed. Due to its fast and local ne and Te profile measurements, the diagnostic is suitable for investigating fast processes such as divertor transitions and filaments. [ABSTRACT FROM AUTHOR]- Published
- 2024
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11. Design, characterization, and modeling of the Charge eXchange Recombination Spectroscopy (CXRS) suite at the SMall Aspect Ratio Tokamak (SMART)
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Universidad de Sevilla. Departamento de Física Atómica, Molecular y Nuclear, EUROfusion Consortium, Cruz Zabala, Diego José, Viezzer, Eleonora, Rodríguez González, A., Segado Fernández, Jorge, Alvarado Reyes, A., Pérez González, J., García Muñoz, Manuel, Dux, R., Universidad de Sevilla. Departamento de Física Atómica, Molecular y Nuclear, EUROfusion Consortium, Cruz Zabala, Diego José, Viezzer, Eleonora, Rodríguez González, A., Segado Fernández, Jorge, Alvarado Reyes, A., Pérez González, J., García Muñoz, Manuel, and Dux, R.
- Abstract
Ion temperature, rotation, and density are key parameters to evaluate the performance of present and future fusion reactors. These parameters are critical for understanding ion heat, momentum, and particle transport, making it mandatory to properly diagnose them. A common technique to measure these properties is charge exchange recombination spectroscopy (CXRS). For characterizing positive and negative triangularity plasmas at the small aspect ratio tokamak, a poloidal array of gas puff based CXRS diagnostics will be measuring the ion properties in different poloidal positions. In this work, the modeling of the expected signal and spatial coverage using the FIDASIM code is presented. Furthermore, the design and characterization of the low field side midplane CXRS diagnostic are described. Each diagnostic is composed of a gas injection system, an optical system that collects the light emitted by the plasma, and a spectrometer. These systems will provide ion temperature, rotation, and density with a radial resolution of 3.75 mm and a temporal resolution of 2.2 ms.
- Published
- 2024
12. The radial localization of the transition from low to high confinement mode in the ASDEX Upgrade tokamak
- Author
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Universidad de Sevilla. Departamento de Física Atómica, Molecular y Nuclear, Cavedon, M., Happel, T., Hennequin, P., Dux, R., Höfler, K., Plank, U., Pütterich, T., Stroth, U., Viezzer, Eleonora, Wolfrum, E., Universidad de Sevilla. Departamento de Física Atómica, Molecular y Nuclear, Cavedon, M., Happel, T., Hennequin, P., Dux, R., Höfler, K., Plank, U., Pütterich, T., Stroth, U., Viezzer, Eleonora, and Wolfrum, E.
- Abstract
A novel experimental method is applied to localize the initial suppression of turbulence, in the form of density fluctuations, at the transition from the low (L-) to the high (H-) confinement mode in toroidal magnetic fusion plasmas. The high radial and temporal resolution, combined with the unprecedented statistical significance, provided the awaited information on a possible dominant E × B shear layer in L-H transition physics. We show, for the first time, that the H-mode turbulence suppression is initiated at the inner E × B shear layer in the ASDEX Upgrade tokamak possibly shedding light on the causality behind the L-H transition process.
- Published
- 2024
13. First SOLPS‐ITER simulations of ASDEX Upgrade partially detached H‐mode with boron impurity: The missing radiation at the outer strike‐point region.
- Author
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Makarov, S. O., Coster, D. P., Gleiter, T., Brida, D., Muraca, M., Dux, R., David, P., Kurzan, B., Bonnin, X., and O'Mullane, M.
- Subjects
THOMSON scattering ,LANGMUIR probes ,BORON ,SOWING ,RADIATION - Abstract
Partially detached H‐modes are the baseline regime for the future ITER operation. The ASDEX Upgrade partially detached H‐mode is modeled using the SOLPS‐ITER code with drifts enabled and compared with experimental data. For the first time, boron (B) impurity is simulated in the Scrape‐off layer (SOL) and divertor. A comparison between divertor diagnostics and discrepancies between Langmuir probe and Divertor Thomson scattering/Stark broadening diagnostic are discussed. In the modeling, experimental target profiles are reproduced if the experimental level of radiation in the SOL and divertor is achieved using nitrogen (N) impurity seeding. Bolometry measurements detect substantial radiation from the partially detached outer strike point. With B radiation, this maximum in bolometry data is reproduced in the modeling, which is not possible with N alone. [ABSTRACT FROM AUTHOR]
- Published
- 2024
- Full Text
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14. Design, characterization, and modeling of the Charge eXchange Recombination Spectroscopy (CXRS) suite at the SMall Aspect Ratio Tokamak (SMART).
- Author
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Cruz-Zabala, D. J., Viezzer, E., Rodriguez-Gonzalez, A., Segado-Fernandez, J., Alvarado-Reyes, A., Perez-Gonzalez, J., Garcia-Munoz, M., and Dux, R.
- Abstract
Ion temperature, rotation, and density are key parameters to evaluate the performance of present and future fusion reactors. These parameters are critical for understanding ion heat, momentum, and particle transport, making it mandatory to properly diagnose them. A common technique to measure these properties is charge exchange recombination spectroscopy (CXRS). For characterizing positive and negative triangularity plasmas at the small aspect ratio tokamak, a poloidal array of gas puff based CXRS diagnostics will be measuring the ion properties in different poloidal positions. In this work, the modeling of the expected signal and spatial coverage using the FIDASIM code is presented. Furthermore, the design and characterization of the low field side midplane CXRS diagnostic are described. Each diagnostic is composed of a gas injection system, an optical system that collects the light emitted by the plasma, and a spectrometer. These systems will provide ion temperature, rotation, and density with a radial resolution of 3.75 mm and a temporal resolution of 2.2 ms. [ABSTRACT FROM AUTHOR]
- Published
- 2024
- Full Text
- View/download PDF
15. Existence of a detachment cliff at ASDEX Upgrade.
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Scotti, L, Cavedon, M, Bernert, M, Brida, D, Kurzan, B, and Dux, R
- Subjects
POWER density ,BOLOMETERS ,DATABASES ,MANOMETERS ,TOKAMAKS ,CLIFFS - Abstract
The detachment cliff is a bifurcative transition to partial detachment recently discovered at the DIII-D tokamak (McLean et al 2015 J. Nucl. Mater. 463 533–6). This work presents a database analysis of target parameters in L-mode and H-mode discharges to search for a detachment cliff at ASDEX Upgrade (AUG). Most of the transitions from attached to partially detached divertor conditions observed in H- and L-mode discharges in AUG show bifurcative-like characteristics that are consistent with the properties of the detachment cliff if the B × ∇ B drift is directed towards the active X-point. In the operational space of power and density, the bifurcative transitions identified during an L-mode discharge occur at injected power and density higher than a threshold value ( P tot > 0.7 MW and n
e > 1.6 × 10 19 m−3 , respectively). Furthermore, the temperatures at which the transitions start are found to be insensitive to the injected impurity, the injected power and the value of the upstream density. Finally, the study of the evolution of the target parameters, of the intensity of the D α line and of specific manometers and bolometer lines of sights shows that the physical process underlying the detachment cliff and the self-sustained divertor oscillations (Heinrich 2020 Nucl. Fusion 60 076013) might be the same. [ABSTRACT FROM AUTHOR]- Published
- 2024
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16. Development of ECRH-based methods for assisted discharge burn-through: Experiment and simulation
- Author
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Ricci D., Stober J., Dux R., Figini L., Wauters T., Lerche E., and Granucci G.
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Physics ,QC1-999 - Abstract
Electron Cyclotron (EC) waves will be routinely used in future reactors not only for plasma heating and/or non-inductive current drive during the flat top but also to assist the plasma start-up phase in large tokamaks with superconductive coils. In ITER, for example, EC start-up is foreseen since first plasma operation. To limit the level of stray radiation, ECRH can be used after ohmic breakdown, as a robust solution to successfully sustain the plasma burn-through in the presence of pre-filling gas and impurity influx from the wall. On ASDEX Upgrade (AUG), a series of dedicated experiments have been performed using EC heating (X2) with a controlled Ne impurity injection in the prefill phase, to mimic non-favourable burn-through conditions such as would be expected in a discharge following a disruption event. The time for EC heating onset has been optimised to assist the early burn-through and a scan of the Ne concentration has been performed to find the threshold for successful burn-through conditions for two ECH power levels (0.7 and 1.4 MW). The toroidal magnetic field flexibility has been also documented, with the cold resonance position being shifted up to 13% in major radius to match the ITER condition. These experiments showed that optimised settings of ECH power (onset and duration of the pulse) have a key role in making feasible the early Ne burn-through (with Ne concentration up to 14% and EC power of 1.4 MW). Successful pulses will be extended to study stationarity and clean up properties. For an efficient and robust use of such a technique, it is essential to develop appropriate models capable of describing present experiments and of extrapolating (or predicting) to future scenarios. In this work, the predictive 0D model for the burn-though phase BKD0 [1] has been used to reproduce experimental results and estimate the power required for a successful burn-through as a function of the impurity concentration, finding that ECH power of 1.4 MW is required to sustain burn-through with more than 20% of Ne. The scalability of the model has been also tested on TCV [2] and its implication for ITER will be discussed.
- Published
- 2023
- Full Text
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17. Investigation of helium exhaust dynamics at the ASDEX Upgrade tokamak with full-tungsten wall
- Author
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Zito, A, Wischmeier, M, Kappatou, A, Kallenbach, A, Sciortino, F, Rohde, V, Schmid, K, Hinson, E, Schmitz, O, Cavedon, M, Mcdermott, R, Dux, R, Griener, M, Stroth, U, Zito A., Wischmeier M., Kappatou A., Kallenbach A., Sciortino F., Rohde V., Schmid K., Hinson E., Schmitz O., Cavedon M., McDermott R., Dux R., Griener M., Stroth U., Zito, A, Wischmeier, M, Kappatou, A, Kallenbach, A, Sciortino, F, Rohde, V, Schmid, K, Hinson, E, Schmitz, O, Cavedon, M, Mcdermott, R, Dux, R, Griener, M, Stroth, U, Zito A., Wischmeier M., Kappatou A., Kallenbach A., Sciortino F., Rohde V., Schmid K., Hinson E., Schmitz O., Cavedon M., McDermott R., Dux R., Griener M., and Stroth U.
- Abstract
An efficient removal of He ash by active pumping in future fusion devices is necessary to avoid fuel dilution and not degrade the core confinement properties. Therefore, a deep understanding of the underlying physics mechanisms is mandatory. Helium exhaust has been experimentally investigated at the ASDEX Upgrade tokamak. This is an ideal test environment, thanks to the ITER-like divertor geometry, an extensive diagnostics coverage and the presence of plasma-facing components made of tungsten. The exhaust efficiency, characterized by the He compression in the divertor, was found to improve with increasing divertor neutral pressure but to degrade with detachment. A multi-reservoir particle balance model was developed to interpret the observed exhaust dynamics, accounting for plasma transport and wall retention. The limited performance of the pumping system and the efficient helium retention capability of the tungsten wall were identified to have the strongest impact on the exhaust dynamics.
- Published
- 2023
18. Divertor detachment and reattachment with mixed impurity seeding on ASDEX Upgrade
- Author
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Henderson, S, Bernert, M, Brida, D, Cavedon, M, David, P, Dux, R, Fevrier, O, Jarvinen, A, Kallenbach, A, Komm, M, Mcdermott, R, O'Mullane, M, Henderson S. S., Bernert M., Brida D., Cavedon M., David P., Dux R., Fevrier O., Jarvinen A., Kallenbach A., Komm M., McDermott R., O'Mullane M., Henderson, S, Bernert, M, Brida, D, Cavedon, M, David, P, Dux, R, Fevrier, O, Jarvinen, A, Kallenbach, A, Komm, M, Mcdermott, R, O'Mullane, M, Henderson S. S., Bernert M., Brida D., Cavedon M., David P., Dux R., Fevrier O., Jarvinen A., Kallenbach A., Komm M., McDermott R., and O'Mullane M.
- Abstract
Using newly developed spectroscopic models to measure the divertor concentration of Ne and Ar, it is shown that the experimental detachment threshold on ASDEX Upgrade with Ar-only and mixtures of Ar+N or Ne+N scales as expected in comparison with an analytical equation derived by Kallenbach et al (2016 Plasma Phys. Control. Fusion 58 045013). However, it is found that Ar radiates more efficiently and Ne less efficiently in the scrape-off layer than the model predicts. By separately increasing the neutral beam injection power and cutting the impurity gas flow, it is shown that the partially detached and strongly detached X-point radiator scenarios reattach in ≈100 ms and ≈250 ms, respectively. The former timescale is set by the core energy confinement time, whereas the latter has an additional delay caused by the time required for the ionisation front to move from the X-point to the target. A simple equation with scalable geometric terms to predict the ionisation front movement time in future machines is proposed.
- Published
- 2023
19. Experimental study of the edge radial electric field in different drift configurations and its role in the access to H-mode at ASDEX Upgrade
- Author
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Plank, U, Brida, D, Conway, G, Happel, T, Hubbard, A, Putterich, T, Angioni, C, Cavedon, M, Dux, R, Eich, T, Fischer, R, Hennequin, P, Plank U., Brida D., Conway G. D., Happel T., Hubbard A. E., Putterich T., Angioni C., Cavedon M., Dux R., Eich T., Fischer R., Hennequin P., Plank, U, Brida, D, Conway, G, Happel, T, Hubbard, A, Putterich, T, Angioni, C, Cavedon, M, Dux, R, Eich, T, Fischer, R, Hennequin, P, Plank U., Brida D., Conway G. D., Happel T., Hubbard A. E., Putterich T., Angioni C., Cavedon M., Dux R., Eich T., Fischer R., and Hennequin P.
- Abstract
The formation of the equilibrium radial electric field (Er) has been studied experimentally at ASDEX Upgrade (AUG) in L-modes of "favorable"(ion ∇ B-drift toward primary X-point) and "unfavorable"(ion ∇ B-drift away from primary X-point) drift configurations, in view of its impact on H-mode access, which changes with drift configurations. Edge electron and ion kinetic profiles and impurity velocity and mean-field Er profiles across the separatrix are investigated, employing new and improved measurement techniques. The experimental results are compared to local neoclassical theory as well as to a simple 1D scrape-off layer (SOL) model. It is found that in L-modes of matched heating power and plasma density, the upstream SOL Er and the main ion pressure gradient in the plasma edge are the same for either drift configurations, whereas the Er well in the confined plasma is shallower in unfavorable compared to the favorable drift configuration. The contributions of toroidal and poloidal main ion flows to Er, which are inferred from local neoclassical theory and the experiment, cannot account for these observed differences. Furthermore, it is found that in the L-mode, the intrinsic toroidal edge rotation decreases with increasing collisionality and it is co-current in the banana-plateau regime for all different drift configurations at AUG. This gives rise to a possible interaction of parallel Pfirsch-Schlüter flows in the SOL with the confined plasma. Thus, the different H-mode power threshold for the two drift configurations cannot be explained in the same way at AUG as suggested by LaBombard et al. [Phys. Plasmas 12, 056111 (2005)] for Alcator C-Mod. Finally, comparisons of Er profiles in favorable and unfavorable drift configurations at the respective confinement transitions show that also the Er gradients are all different, which indirectly indicates a different type or strength of the characteristic edge turbulence in the two drift configurations.
- Published
- 2023
20. An overview of the in-vessel ICRF-diagnostics in the ASDEX Upgrade tokamak
- Author
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Faugel, H., Ochoukov, R., Bobkov, V., Fünfgelder, H., Noterdaeme, J.M., Aguiam, D., and Dux, R.
- Published
- 2019
- Full Text
- View/download PDF
21. Diagnostics for plasma control – From ITER to DEMO
- Author
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Biel, W., Albanese, R., Ambrosino, R., Ariola, M., Berkel, M.V., Bolshakova, I., Brunner, K.J., Cavazzana, R., Cecconello, M., Conroy, S., Dinklage, A., Duran, I., Dux, R., Eade, T., Entler, S., Ericsson, G., Fable, E., Farina, D., Figini, L., Finotti, C., Franke, Th., Giacomelli, L., Giannone, L., Gonzalez, W., Hjalmarsson, A., Hron, M., Janky, F., Kallenbach, A., Kogoj, J., König, R., Kudlacek, O., Luis, R., Malaquias, A., Marchuk, O., Marchiori, G., Mattei, M., Maviglia, F., De Masi, G., Mazon, D., Meister, H., Meyer, K., Micheletti, D., Nowak, S., Piron, Ch., Pironti, A., Rispoli, N., Rohde, V., Sergienko, G., El Shawish, S., Siccinio, M., Silva, A., da Silva, F., Sozzi, C., Tardocchi, M., Tokar, M., Treutterer, W., and Zohm, H.
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- 2019
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22. Validation of gyrokinetic modelling of light impurity transport including rotation in ASDEX Upgrade
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Casson, F. J., McDermott, R. M., Angioni, C., Camenen, Y., Dux, R., Fable, E., Fischer, R., Geiger, B., Manas, P., Menchero, L., Tardini, G., and team, ASDEX Upgrade
- Subjects
Physics - Plasma Physics - Abstract
Upgraded spectroscopic hardware and an improved impurity concentration calculation allow accurate determination of boron density in the ASDEX Upgrade tokamak. A database of boron measurements is compared to quasilinear and nonlinear gyrokinetic simulations including Coriolis and centrifugal rotational effects over a range of H-mode plasma regimes. The peaking of the measured boron profiles shows a strong anti-correlation with the plasma rotation gradient, via a relationship explained and reproduced by the theory. It is demonstrated that the rotodiffusive impurity flux driven by the rotation gradient is required for the modelling to reproduce the hollow boron profiles at higher rotation gradients. The nonlinear simulations validate the quasilinear approach, and, with the addition of perpendicular flow shear, demonstrate that each symmetry breaking mechanism that causes momentum transport also couples to rotodiffusion. At lower rotation gradients, the parallel compressive convection is required to match the most peaked boron profiles. The sensitivities of both datasets to possible errors is investigated, and quantitative agreement is found within the estimated uncertainties. The approach used can be considered a template for mitigating uncertainty in quantitative comparisons between simulation and experiment., Comment: 19 pages, 11 figures, accepted in Nuclear Fusion
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- 2012
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23. Solitary magnetic perturbations at the ELM onset
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Wenninger, RP, Zohm, H, Boom, JE, Burckhart, A, Dunne, MG, Dux, R, Eich, T, Fischer, R, Fuchs, C, Garcia-Munoz, M, Igochine, V, Hoelzl, M, Luhmann Jr, NC, Lunt, T, Maraschek, M, Mueller, HW, Park, HK, Schneider, PA, Sommer, F, Suttrop, W, Viezzer, E, and Team, the ASDEX Upgrade
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Physics - Plasma Physics - Abstract
Edge localised modes (ELMs) allow maintaining sufficient purity of tokamak H-mode plasmas and thus enable stationary H-mode. On the other hand in a future device ELMs may cause divertor power flux densities far in excess of tolerable material limits. The size of the energy loss per ELM is determined by saturation effects in the non-linear phase of the ELM, which at present is hardly understood. Solitary magnetic perturbations (SMPs) are identified as dominant features in the radial magnetic fluctuations below 100kHz. They are typically observed close (+-0.1ms) to the onset of pedestal erosion. SMPs are field aligned structures rotating in the electron diamagnetic drift direction with perpendicular velocities of about 10km/s. A comparison of perpendicular velocities suggests that the perturbation evoking SMPs is located at or inside the separatrix. Analysis of very pronounced examples showed that the number of peaks per toroidal turn is 1 or 2, which is clearly lower than corresponding numbers in linear stability calculations. In combination with strong peaking of the magnetic signals this results in a solitary appearance resembling modes like palm tree modes, edge snakes or outer modes. This behavior has been quantified as solitariness and correlated to main plasma parameters. SMPs may be considered as a signature of the non-linear ELM-phase originating at the separatrix or further inside. Thus they provide a handle to investigate the transition from linear to non-linear ELM phase. By comparison with data from gas puff imaging processes in the non-linear phase at or inside the separatrix and in the scrape-off-layer (SOL) can be correlated. A connection between the passing of an SMP and the onset of radial filament propagation has been found. Eventually the findings related to SMPs may contribute to a future quantitative understanding of the non-linear ELM evolution., Comment: submitted to Nuclear Fusion
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- 2012
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24. Divertor enrichment of recycling impurity species (He, N2, Ne, Ar, Kr) in ASDEX Upgrade H-modes.
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Kallenbach, A., Dux, R., Henderson, S.S., Tantos, C., Bernert, M., Day, C., McDermott, R.M., Rohde, V., and Zito, A.
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NITROGEN , *IONIZATION energy , *GAS reservoirs , *FLIGHT simulators , *DEUTERIUM , *KRYPTON , *PLASMA density - Abstract
Particle balance calculations are done for the seeding species N2, Ne, Ar, Kr as well as He with the aim of obtaining a realistic description of the divertor and core plasma impurity content. Experimental time traces of main plasma impurity densities are fitted by a single, time-independent parameter v z , in eff . This parameter represents the product of the impurity inward pinch in the pedestal, used for the description of gross fueling here, and the enrichment factor between the sub-divertor gas reservoir and the upstream separatrix. v z , in eff depends strongly on the first ionization energy as well as on the charge Z or mass of the impurity. The prevailing dependence of the enrichment values on the ionization energy suggests the importance of the relative impurity and deuterium ionization lengths in the divertor. Regression analysis of v z , in eff yields an expression for the impurity concentrations in the core and the divertor of ASDEX Upgrade which allows the prediction of the corresponding impurity densities and their divertor enrichment within a factor of 2 with only engineering parameters as input. A simple wall model has been introduced to take into account wall storage and release of impurities, e.g. for conditions of pre-loaded walls due to seeding in previous discharges. Wall effects are observed for all species considered, but wall storage turns out to be more important for N and He compared to Ne, Ar, Kr. Similar enrichment values are obtained for ELMy H-modes and EDA/QCE no-ELM regimes. A factor of approximately 1.4 reduction in enrichment is observed for divertor conditions for pronounced detachment with Ar and N2. The obtained analytical model for the core and sub-divertor impurity densities is well suited for integration into a discharge flight simulator or a real time state observer. [ABSTRACT FROM AUTHOR]
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- 2024
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25. Experimental validation of momentum transport theory in the core of H-mode plasmas in the ASDEX Upgrade tokamak.
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Zimmermann, C. F. B., Angioni, C., McDermott, R. M., Duval, B. P., Dux, R., Fable, E., Salmi, A., Stroth, U., Tala, T., Tardini, G., and Pütterich, T.
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TRANSPORT theory ,TOKAMAKS ,PRANDTL number ,CORE & periphery (Economic theory) ,RESIDUAL stresses - Abstract
This study employs the established momentum transport analysis at ASDEX Upgrade [Zimmermann et al., Nucl. Fusion 63, 124003 (2023)] to investigate the parametric variations of the momentum transport coefficients in the core of H-mode plasmas. These experimental results are compared to a comprehensive database of gyrokinetic calculations. Generally, good agreement between predicted and measured diffusive and convective transport coefficients is found. The predicted and measured Prandtl numbers correlate most dominantly with the magnetically trapped particle fraction. The experimentally inferred pinch numbers strongly depend on the logarithmic density gradient and magnetic shear, consistent with the theoretical predictions of the Coriolis pinch. The intrinsic torque from residual stress in the inner core is small, scales with the local logarithmic density gradient, and the data indicate a possible sign reversal. In the outer periphery of the core, the intrinsic torque is always co-current-directed and scales with the pressure gradient. This is consistent with prior experimental findings and global, non-linear gyrokinetic predictions. It suggests that profile shearing effects generate the intrinsic torque in the inner core. Toward the outer core, most likely, effects from E × B -shearing become more influential. These results offer the first comprehensive picture of this transport channel in the core plasma and contribute to validating the corresponding theoretical understanding. The derived scaling laws are used to construct a reduced momentum transport model, which has been validated against an additional dataset. This demonstrates that the model captures the essential contributions to momentum transport in the core of H-mode plasmas. [ABSTRACT FROM AUTHOR]
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- 2024
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26. Investigation of the fast-ion transport by FIDA spectroscopy at ASDEX Upgrade
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Geiger, B, Garcia-Munoz, M, Dux, R, McDermott, RM, Tardini, G, Hobirk, J, Lunt, T, Heidbrink, WW, and Ryter, F
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- 2012
27. Fast-ion D-alpha measurements at ASDEX Upgrade
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Geiger, B, Garcia-Munoz, M, Heidbrink, WW, McDermott, RM, Tardini, G, Dux, R, Fischer, R, Igochine, V, and Team, the ASDEX Upgrade
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Atomic ,Molecular ,Nuclear ,Particle and Plasma Physics ,Other Physical Sciences ,Fluids & Plasmas - Abstract
A fast-ion D-alpha (FIDA) diagnostic has been developed for the fully tungsten coated ASDEX Upgrade (AUG) tokamak using 25 toroidally viewing lines of sight and featuring a temporal resolution of 10 ms. The diagnostic's toroidal geometry determines a well-defined region in velocity space which significantly overlaps with the typical fast-ion distribution in AUG plasmas. Background subtraction without beam modulation is possible because relevant parts of the FIDA spectra are free from impurity line contamination. Thus, the temporal evolution of the confined fast-ion distribution function can be monitored continuously. FIDA profiles during on- and off-axis neutral beam injection (NBI) heating are presented which show changes in the radial fast-ion distribution with the different NBI geometries. Good agreement has been obtained between measured and simulated FIDA radial profiles in MHD-quiescent plasmas using fast-ion distribution functions provided by TRANSP. In addition, a large fast-ion redistribution with a drop of about 50% in the central fast-ion population has been observed in the presence of a q = 2 sawtooth-like crash, demonstrating the capabilities of the diagnostic. © 2011 IOP Publishing Ltd.
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- 2011
28. Investigation of helium exhaust dynamics at the ASDEX Upgrade tokamak with full-tungsten wall
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Zito, A., primary, Wischmeier, M., additional, Kappatou, A., additional, Kallenbach, A., additional, Sciortino, F., additional, Rohde, V., additional, Schmid, K., additional, Hinson, E.T., additional, Schmitz, O., additional, Cavedon, M., additional, McDermott, R.M., additional, Dux, R., additional, Griener, M., additional, and Stroth, U., additional
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- 2023
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29. Divertor detachment and reattachment with mixed impurity seeding on ASDEX Upgrade
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Henderson, S.S., primary, Bernert, M., additional, Brida, D., additional, Cavedon, M., additional, David, P., additional, Dux, R., additional, Février, O., additional, Järvinen, A., additional, Kallenbach, A., additional, Komm, M., additional, McDermott, R., additional, and O’Mullane, M., additional
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- 2023
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30. Enhanced performance in fusion plasmas through turbulence suppression by megaelectronvolt ions
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Mazzi, S., Garcia, J., Zarzoso, D., Kazakov, Y., Ongena, J., Dreval, M., Nocente, M., Stancar, Z., Szepesi, G., Eriksson, J., Sahlberg, A., Benkadda, S., Abid, N., Abraham, K., Abreu, P., Adabonyan, O., Adrich, P., Afanasev, V., Afzal, M., Ahlgren, T., Aho-Mantila, L., Aiba, N., Airila, M., Akhtar, M., Albanese, R., Alderson-Martin, M., Alegre, D., Aleiferis, S., Aleksa, A., Alekseev, A., Alessi, E., Aleynikov, P., Algualcil, J., Ali, M., Allinson, M., Alper, B., Alves, E., Ambrosino, G., Ambrosino, R., Amosov, V., Andersson Sunden, E., Andrew, P., Angelini, B., Angioni, C., Antoniou, I., Appel, L., Appelbee, C., Aria, S., Ariola, M., Artaserse, G., Arter, W., Artigues, V., Asakura, N., Ash, A., Ashikawa, N., Aslanyan, V., Astrain, M., Asztalos, O., Auld, D., Auriemma, F., Austin, Y., Avotina, L., Aymerich, E., Baciero, A., Bairaktaris, F., Balbin, J., Balbinot, L., Balboa, I., Balden, M., Balshaw, C., Balshaw, N., Bandaru, V., Banks, J., Baranov, Y., Barcellona, C., Barnard, A., Barnard, M., Barnsley, R., Barth, A., Baruzzo, M., Barwell, S., Bassan, M., Batista, A., Batistoni, P., Baumane, L., Bauvir, B., Baylor, L., Beaumont, P., Beckett, D., Begolli, A., Beidler, M., Bekris, N., Beldishevski, M., Belli, E., Belli, F., Belonohy, E., Ben Yaala, M., Benayas, J., Bentley, J., Bergsaker, H., Bernardo, J., Bernert, M., Berry, M., Bertalot, L., Betar, H., Beurskens, M., Bickerton, S., Bieg, B., Bielecki, J., Bierwage, A., Biewer, T., Bilato, R., Bílkova, P., Birkenmeier, G., Bishop, H., Bizarro, J., Blackburn, J., Blanchard, P., Blatchford, P., Bobkov, V., Boboc, A., Bohm, P., Bohm, T., Bolshakova, I., Bolzonella, T., Bonanomi, N., Bonfiglio, D., Bonnin, X., Bonofiglo, P., Boocock, S., Booth, A., Booth, J., Borba, D., Borodin, D., Borodkina, I., Boulbe, C., Bourdelle, C., Bowden, M., Boyd, K., Bozicevic Mihalic, I., Bradnam, S., Braic, V., Brandt, L., Bravanec, R., Breizman, B., Brett, A., Brezinsek, S., Brix, M., Bromley, K., Brown, B., Brunetti, D., Buckingham, R., Buckley, M., Budny, R., Buermans, J., Bufferand, H., Buratti, P., Burgess, A., Buscarino, A., Busse, A., Butcher, D., Cal, E., Calabro, G., Calacci, L., Calado, R., Camenen, Y., Canal, G., Cannas, B., Cappelli, M., Carcangiu, S., Card, P., Cardinali, A., Carman, P., Carnevale, D., Carr, M., Carralero, D., Carraro, L., Carvalho, I., Carvalho, P., Casiraghi, I., Casson, F., Castaldo, C., Catalan, J., Catarino, N., Causa, F., Cavedon, M., Cecconello, M., Challis, C., Chamberlain, B., Chang, C., Chankin, A., Chapman, B., Chernyshova, M., Chiariello, A., Chmielewski, P., Chomiczewska, A., Chone, L., Ciraolo, G., Ciric, D., Citrin, J., Ciupinski, t., Clark, M., Clarkson, R., Clements, C., Cleverly, M., Coad, J., Coates, P., Cobalt, A., Coccorese, V., Coelho, R., Coenen, J., Coffey, I., Colangeli, A., Colas, L., Collins, C., Collins, J., Collins, S., Conka, D., Conroy, S., Conway, B., Conway, N., Coombs, D., Cooper, P., Cooper, S., Corradino, C., Corrigan, G., Coster, D., Cox, P., Craciunescu, T., Cramp, S., Crapper, C., Craven, D., Craven, R., Crialesi Esposito, M., Croci, G., Croft, D., Croitoru, A., Crombe, K., Cronin, T., Cruz, N., Crystal, C., Cseh, G., Cufar, A., Cullen, A., Curuia, M., Czarski, T., Dabirikhah, H., Dal Molin, A., Dale, E., Dalgliesh, P., Dalley, S., Dankowski, J., David, P., Davies, A., Davies, S., Davis, G., Dawson, K., Dawson, S., Day, I., De Bock, M., De Temmerman, G., De Tommasi, G., Deakin, K., Deane, J., Dejarnac, R., Del Sarto, D., Delabie, E., Del-Castillo-Negrete, D., Dempsey, A., Dendy, R., Devynck, P., Di Siena, A., Di Troia, C., Dickson, T., Dinca, P., Dittmar, T., Dobrashian, J., Doerner, R., Donne, A., Dorling, S., Dormido-Canto, S., Douai, D., Dowson, S., Doyle, R., Drewelow, P., Drews, P., Drummond, G., Duckworth, P., Dudding, H., Dumont, R., Dumortier, P., Dunai, D., Dunatov, T., Dunne, M., Duran, I., Durodie, F., Dux, R., Dvornova, A., Eastham, R., Edwards, J., Eich, T., Eichorn, A., Eidietis, N., Eksaeva, A., Haroun, H., Ellwood, G., Elsmore, C., Embreus, O., Emery, S., Ericsson, G., Eriksson, B., Eriksson, F., Eriksson, L., Ertmer, S., Esquembri, S., Esquisabel, A., Estrada, T., Evans, G., Evans, S., Fable, E., Fagan, D., Faitsch, M., Falessi, M., Fanni, A., Farahani, A., Farquhar, I., Fasoli, A., Faugeras, B., Fazinie, S., Felici, F., Felton, R., Fernandes, A., Fernandes, H., Ferrand, J., Ferreira, D., Ferreira, J., Ferro, G., Fessey, J., Ficker, O., Field, A., Figueiredo, A., Figueiredo, J., Fil, A., Fil, N., Finburg, P., Fiorucci, D., Fischer, U., Fishpool, G., Fittill, L., Fitzgerald, M., Flammini, D., Flanagan, J., Flinders, K., Foley, S., Fonnesu, N., Fontana, M., Fontdecaba, J., Forbes, S., Formisano, A., Fornal, T., Fortuna, L., Fortuna-Zalesna, E., Fortune, M., Fowler, C., Fransson, E., Frassinetti, L., Freisinger, M., Fresa, R., Fridstrom, R., Frigione, D., Fülop, T., Furseman, M., Fusco, V., Futatani, S., Gadariya, D., Gal, K., Galassi, D., Gafezka, K., Galeani, S., Gallart, D., Galvao, R., Gao, Y., Garcia-Munoz, M., Gardener, M., Garzotti, L., Gaspar, J., Gatto, R., Gaudio, P., Gear, D., Gebhart, T., Gee, S., Gelfusa, M., George, R., Gerasimov, S., Gervasini, G., Gethins, M., Ghani, Z., Gherendi, M., Ghezzi, F., Giacalone, J., Giacomelli, L., Giacometti, G., Gibson, C., Gibson, K., Gil, L., Gillgren, A., Gin, D., Giovannozzi, E., Giroud, C., Glen, R., Gloggler, S., Goff, J., Gohil, P., Goloborodko, V., Gomes, R., Goncalves, B., Goniche, M., Goodyear, A., Gore, S., Gorini, G., Görler, T., Gotts, N., Goulding, R., Gow, E., Graham, B., Graves, J., Greuner, H., Grierson, B., Griffiths, J., Griph, S., Grist, D., Gromelski, W., Groth, M., Grove, R., Gruca, M., Guard, D., Gupta, N., Gurl, C., Gusarov, A., Hackett, L., Hacquin, S., Hager, R., Hagg, L., Hakola, A., Halitovs, M., Hall, S., Hallworth-Cook, S., Ham, C., Hamaguchi, D., Hamed, M., Hamlyn-Harris, C., Hammond, K., Harford, E., Harrison, J., Harting, D., Hatano, Y., Hatch, D., Haupt, T., Hawes, J., Hawkes, N., Hawkins, J., Hayashi, T., Hazael, S., Hazel, S., Heesterman, P., Heidbrink, B., Helou, W., Hemming, O., Henderson, S., Henriques, R., Hepple, D., Herfindal, J., Hermon, G., Hill, J., Hillesheim, J., Hizanidis, K., Hjalmarsson, A., Ho, A., Hobirk, J., Hoenen, O., Hogben, C., Hollingsworth, A., Hollis, S., Hollmann, E., Hoelzl, M., Homan, B., Hook, M., Hopley, D., Horacek, J., Horsley, D., Horsten, N., Horton, A., Horton, L., Horvath, L., Hotchin, S., Howell, R., Hu, Z., Huber, A., Huber, V., Huddleston, T., Huijsmans, G., Huynh, P., Hynes, A., Iliasova, M., lmrie, D., lmrísek, M., lngleby, J., Innocente, P., Insulander Björk, K., Isernia, N., lvanova-Stanik, I., lvings, E., Jablonski, S., Jachmich, S., Jackson, T., Jacquet, P., Järleblad, H., Jaulmes, F., Jenaro Rodriguez, J., Jepu, I., Joffrin, E., Johnson, R., Johnson, T., Johnston, J., Jones, C., Jones, G., Jones, L., Jones, N., Jones, T., Joyce, A., Juarez, R., Juvonen, M., Kalnina, P., Kaltiaisenaho, T., Kaniewski, J., Kantor, A., Kappatou, A., Karhunen, J., Karkinsky, D., Kashchuk, Y., Kaufman, M., Kaveney, G., Kazantzidis, V., Keeling, D., Kelly, R., Kempenaars, M., Kennedy, C., Kennedy, D., Kent, J., Khan, K., Khilkevich, E., Kiefer, C., Kilpeläinen, J., Kim, C., Kim, H., Kim, S., King, D., King, R., Kinna, D., Kiptily, V., Kirjasuo, A., Kirov, K., Kirschner, A., kiviniemi, T., Kizane, G., Klas, M., Klepper, C., Klix, A., Kneale, G., Knight, M., Knight, P., Knights, R., Knipe, S., Knolker, M., Knott, S., Kocan, M., Kochl, F., Kodeli, I., Kolesnichenko, Y., Kominis, Y., Kong, M., Korovin, V., Kos, B., Kos, D., Koslowski, H., Kotschenreuther, M., Koubiti, M., Kowalska-Strzeciwilk, E., Koziol, K., Krasilnikov, A., Krasilnikov, V., Kresina, M., Krieger, K., Krishnan, N., Krivska, A., Kruezi, U., Ksiezek, I., Kukushkin, A., Kumpulainen, H., Kurki-Suonio, T., Kurotaki, H., Kwak, S., Kwon, O., Laguardia, L., Lagzdina, E., Lahtinen, A., Laing, A., Lam, N., Lambertz, H., Lane, B., Lane, C., Lascas Neto, E., Laszyriska, E., 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., 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moléculaires (PIIM), Aix Marseille Université (AMU)-Centre National de la Recherche Scientifique (CNRS), Institut de Recherche sur la Fusion par confinement Magnétique (IRFM), Commissariat à l'énergie atomique et aux énergies alternatives (CEA), Swiss Plasma Center (SPC), Ecole Polytechnique Fédérale de Lausanne (EPFL), Laboratory for Plasma Physics (LPP), Ecole Royale Militaire / Koninklijke Militaire School (ERM KMS), Kharkiv Institute of Physics and Technology (Ukraine), V.N. Karazin Kharkiv National University (KhNU), Dipartimento di Fisica (Milano), Università degli Studi di Milano = University of Milan (UNIMI), Consiglio Nazionale delle Ricerche [Milano] (CNR), Jozef Stefan Institute [Ljubljana] (IJS), Culham Centre for Fusion Energy (CCFE), Department of Physics and Astronomy [Uppsala], Uppsala University, This work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training programme 2014–2018 and 2019–2020 under Grant agreement No 633053., Mazzi, S, Garcia, J, Zarzoso, D, Kazakov, Y, Ongena, J, Dreval, M, Nocente, M, Stancar, Z, Szepesi, G, Eriksson, J, Sahlberg, A, Benkadda, S, Abid, N, Abraham, K, Abreu, P, Adabonyan, O, Adrich, P, Afzal, M, Ahlgren, T, Aho-Mantila, L, Aiba, N, Airila, M, Akhtar, M, Albanese, R, Alderson-Martin, M, Alegre, D, Aleiferis, S, Aleksa, A, Alessi, E, Aleynikov, P, Algualcil, J, Ali, M, Allinson, M, Alper, B, Alves, E, Ambrosino, G, Ambrosino, R, 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K., Zoulias, I., Zwingmann, W., Zychor, I., JET Contributors, Science and Technology of Nuclear Fusion, EIRES Eng. for Sustainable Energy Systems, Magneto-Hydro-Dynamic Stability of Fusion Plasmas, Applied Physics and Science Education, Kazakov, Yo, VTT Technical Research Centre of Finland, Culham Science Centre, Princeton Plasma Physics Laboratory, Department of Applied Physics, European Commission, Forschungszentrum Jülich, Universidade Lisboa, Fusion and Plasma Physics, University of Milan - Bicocca, Aalto University, General Atomics, ITER, University of Toyama, CEA, Oak Ridge National Laboratory, Technical University of Madrid, Swiss Federal Institute of Technology Lausanne, Dutch Institute for Fundamental Energy Research, Royal Military Academy, Seoul National University, Chalmers University of Technology, Max Planck Institute for Plasma Physics, KTH Royal Institute of Technology, and Aalto-yliopisto
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[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.
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- 2022
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31. Disruption prediction with artificial intelligence techniques in tokamak plasmas
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J., Ratynskaia S., Rebai M., Refy D., Reichle R., Reinke M., Reiser D., Reux C., Reynolds S., Richiusa M. L., Richyal S., Rigamonti D., Rimini F. G., Risner J., Riva M., Rivero-Rodriguez J., Roach C. M., Robins R., Robinson S., Robson D., Rodionov R., Rodrigues P., Ramos M. R., Rodriguez-Fernandez P., Romanelli F., Romanelli M., Romanelli S., Romazanov J., Rossi R., Rowe S., Rowlands D., Rubel M., Rubinacci G., Rubino G., Ruchko L., Ruiz M., Ruiz J. R., Ruset C., Rzadkiewicz J., Saarelma S., Safi E., Sahlberg A., Salewski M., Salmi A., Salmon R., Salzedas F., Sanders I., Sandiford D., Santos B., Santucci A., Sarkimaki K., Sarwar R., Sarychev I., Sauter O., Sauwan P., Scapin N., Schluck F., Schmid K., Schmuck S., Schneider M., Schneider P. A., Schworer D., Scott G., Scott M., Scraggs D., Scully S., Segato M., Seo J., Sergienko G., Sertoli M., Sharapov S. E., Shaw A., Sheikh H., Sheikh U., Shepherd A., Shevelev A., Shigin P., Shinohara K., Shiraiwa S., Shiraki D., Short M., Sias G., Silburn S. A., Silva A., Silva C., Silva J., Silvagni D., Simfukwe D., Simpson J., Sinclair D., Sipila S. K., Sips A. C. C., Siren P., Sirinelli A., Sjostrand H., Skinner N., Slater J., Smith N., Smith P., Snell J., Snoep G., Snoj L., Snyder P., Soare S., Solano E. R., Solokha V., Somers A., Sommariva C., Soni K., Sorokovoy E., Sos M., Sousa J., Sozzi C., Spagnolo S., Spelzini T., Spineanu F., Spong D., Sprada D., Sridhar S., Srinivasan C., Stables G., Staebler G., Stamatelatos I., Stancar Z., Staniec P., Stankunas G., Stead M., Stefanikova E., Stephen A., Stephens J., Stevenson P., Stojanov M., Strand P., Strauss H. R., Strikwerda S., Strom P., Stuart C. I., Studholme W., Subramani M., Suchkov E., Sumida S., Sun H. J., Susts T. E., Svensson J., Svoboda J., Sweeney R., Sytnykov D., Szabolics T., Szepesi G., Tabia B., Tadic T., Tal B., Tala T., Tallargio A., Tamain P., Tan H., Tanaka K., Tang W., Tardocchi M., Taylor D., Teimane A. S., Telesca G., Teplova N., Teplukhina A., Terentyev D., Terra A., Terranova D., Terranova N., Testa D., Tholerus E., Thomas J., Thoren E., Thorman A., Tierens W., Tinguely R. A., Tipton A., Todd H., Tokitani M., Tolias P., Tomes M., Tookey A., Torikai Y., von Toussaint U., Tsavalas P., Tskhakaya D., Turner I., Turner M., Turner M. M., Turnyanskiy M., Tvalashvili G., Tyrrell S., Tyshchenko M., Uccello A., Udintsev V., Urbanczyk G., Vadgama A., Valcarcel D., Valisa M., Olivares P. V., Vallhagen O., Valovic M., Eester D. V., Varje J., Vartanian S., Vasilopoulou T., Vayakis G., Vecsei M., Ventre S., Verdoolaege G., Verona C., Rinati G. V., Veshchev E., Vianello N., Viezzer E., Vignitchouk L., Vila R., Villari R., Villone F., Vincenzi P., Vinyar I., Viola B., Virtanen A. J., Vitins A., Vizvary Z., Vlad G., Vlad M., Vondracek P., de Vries P., Wakeling B., Walkden N. R., Walker M., Walker R., Walsh M., Wang E., Wang N., Warder S., Warren R., Waterhouse J., Watts C., Wauters T., Weckmann A., Maxwell H. W., Weiland M., Weisen H., Weiszflog M., Welch P., Wendler N., West A., Wheatley M., Wheeler S., Whitehead A., Whittaker D., Widdowson A., Wiesen S., Wilkinson J., Williams J. C., Willoughby D., Wilson I., Wilson J., Wilson T., Wischmeier M., Wise P., Withenshaw G., Withycombe A., Witts D., Wojcik-Gargula A., Wolfrum E., Wood R., Woodley C., Woodley R., Woods B., Wright J., Wright J. C., Xu T., Yadikin D., Yajima M., Yakovenko Y., Yang Y., Yanling W., Yanovskiy V., Young I., Young R., Zabolockis R. J., Zacks J., Zagorski R., Zaitsev F. S., Zakharov L., Zarins A., Fernandez D. Z., Zastrow K. -D., Zayachuk Y., Zerbini M., Zhang W., Zhou Y., Zlobinski M., Zocco A., Zohar A., Zoita V., Zoletnik S., Zotta V. 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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
32. Enhanced performance in fusion plasmas through turbulence suppression by megaelectronvolt ions
- Author
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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 L., 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. J., 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., Molin A. D., Dale E., Dalgliesh P., Dalley S., Dankowski J., David P., Davies A., Davies S., Davis G., Dawson K., Dawson S., Day I. E., 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. O., Devynck P., Di Siena A., Di Troia C., Dickson T., Dinca P., Dittmar T., Dobrashian J., Doerner R. P., Donne A. J. H., 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., El Haroun H., Ellwood G., Elsmore C., Embreus O., Emery S., Ericsson G., Eriksson B., Eriksson F., Eriksson L. G., Ertmer S., Esquembri S., Esquisabel A. L., Estrada T., Evans G., Evans S., Fable E., Fagan D., Faitsch M., Falessi M., Fanni A., Farahani A., Farquhar I., Fasoli A., Faugeras B., Fazinic S., Felici F., Felton R., Fernandes A., Fernandes H., Ferrand J., Ferreira D. R., Ferreira J., Ferro G., Fessey J., Ficker O., Field A. R., 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. M., 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., Galazka 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. N., Gervasini G., Gethins M., Ghani Z., Gherendi M., Ghezzi F., Giacalone J. C., Giacomelli L., Giacometti G., Gibson C., Gibson K. J., Gil L., Gillgren A., 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., Gorler T., Gotts N., Goulding R., Gow E., Graham B., Graves J. P., 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., Hall S. A., Hallworth-Cook S., Ham C. J., Hamaguchi D., Hamed M., Hamlyn-Harris C., Hammond K., Harford E., Harrison J. R., Harting D., Hatano Y., Hatch D. R., Haupt T., Hawes J., Hawkes N. C., Hawkins J., Hayashi T., Hazael S., Hazel S., Heesterman P., Heidbrink B., Helou W., Hemming O., Henderson S. S., Henriques R. B., Hepple D., Herfindal J., Hermon G., Hill J., Hillesheim J. C., Hizanidis K., Hjalmarsson A., Ho A., Hobirk J., Hoenen O., Hogben C., Hollingsworth A., Hollis S., Hollmann E., Holzl M., Homan B., Hook M., Hopley D., Horacek J., Horsley D., Horsten N., Horton A., Horton L. D., Horvath L., Hotchin S., Howell R., Hu Z., Huber A., Huber V., Huddleston T., Huijsmans G. T. A., Huynh P., Hynes A., Imrie D., Imrisek M., Ingleby J., Innocente P., Insulander Bjork K., Isernia N., Ivanova-Stanik I., Ivings E., Jablonski S., Jachmich S., Jackson T., Jacquet P., Jarleblad H., Jaulmes F., Rodriguez J. J., Jepu I., Joffrin E., Johnson R., Johnson T., Johnston J., Jones C., Jones G., Jones L., Jones N., Jones T., Joyce A., Juarez R., Juvonen M., Kalnina P., Kaltiaisenaho T., Kaniewski J., Kantor A., Kappatou A., Karhunen J., Karkinsky D., Kaufman M., Kaveney G., Kazantzidis V., Keeling D. L., Kelly R., Kempenaars M., Kennedy C., Kennedy D., Kent J., Khan K., Kiefer C., Kilpelainen J., Kim C., Kim H. -T., Kim S. H., King D. B., King R., Kinna D., Kiptily V. G., Kirjasuo A., Kirov K. K., Kirschner A., Kiviniemi T., Kizane G., Klas M., Klepper C., Klix A., Kneale G., Knight M., Knight P., Knights R., Knipe S., Knolker M., Knott S., Kocan M., Kochl F., Kodeli I., Kolesnichenko Y., Kominis Y., Kong M., Korovin V., Kos B., Kos D., Koslowski H. R., Kotschenreuther M., Koubiti M., Kowalska-Strzeciwilk E., Koziol K., Krasilnikov V., Kresina M., Krieger K., Krishnan N., Krivska A., Kruezi U., Ksiazek I., Kukushkin A. B., Kumpulainen H., Kurki-Suonio T., Kurotaki H., Kwak S., Kwon O. J., Laguardia L., Lagzdina E., Lahtinen A., Laing A., Lam N., Lambertz H. T., Lane B., Lane C., Lascas Neto E., Laszynska E., Lawson K. D., Lazaros A., Lazzaro E., Learoyd G., Lee C., Lee S. E., Leerink S., Leeson T., Lefebvre X., Leggate H. J., Lehmann J., Lehnen M., Leichtle D., Leipold F., Lengar I., Lennholm M., Leon Gutierrez E., Lepiavko B., Leppanen J., Lerche E., Lescinskis A., Lewis J., Leysen W., Li L., Li Y., Likonen J., Linsmeier C., Lipschultz B., Litaudon X., Litherland-Smith E., Liu F., Loarer T., Loarte A., Lobel R., Lomanowski B., Lomas P. J., Lopez J. M., Lorenzini R., Loreti S., Losada U., Loschiavo V. P., Loughlin M., Louka Z., Lovell J., Lowe T., Lowry C., Lubbad S., Luce T., Lucock R., Luna C., de la Luna E., Lungaroni M., Lungu C. P., Lunt T., Lutsenko V., Lyons B., Lyssoivan A., Machielsen M., Macusova E., Maenpaa R., Maggi C. F., Maggiora R., Magness M., Mahesan S., Maier H., Mailloux J., Maingi R., Malinowski K., Manas P., Mantica P., Mantsinen M. J., Manyer J., Manzanares A., Maquet P., Marceca G., Marchetto C., Marchuk O., Mariani A., Mariano G., Marin M., Marinelli M., Markovic T., Marocco D., Marot L., Marsden S., Marsh J., Marshall R., Martellucci L., Martin A., Martin A. J., Martone R., Maruyama S., Maslov M., Masuzaki S., Matejcik S., Mattei M., Matthews G. F., Matveev D., Matveeva E., Mauriya A., Maviglia F., Mayer M., Mayoral M. -L., Mazzotta C., McAdams R., McCarthy P. J., McClements K. G., McClenaghan J., McCullen P., McDonald D. C., McGuckin D., McHugh D., McIntyre G., McKean R., McKehon J., McMillan B., McNamee L., McShee A., Meakins A., Medley S., Meekes C. 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A., Huynh P., Hynes A., Imrie D., Imrisek M., Ingleby J., Innocente P., Insulander Bjork K., Isernia N., Ivanova-Stanik I., Ivings E., Jablonski S., Jachmich S., Jackson T., Jacquet P., Jarleblad H., Jaulmes F., Rodriguez J. J., Jepu I., Joffrin E., Johnson R., Johnson T., Johnston J., Jones C., Jones G., Jones L., Jones N., Jones T., Joyce A., Juarez R., Juvonen M., Kalnina P., Kaltiaisenaho T., Kaniewski J., Kantor A., Kappatou A., Karhunen J., Karkinsky D., Kaufman M., Kaveney G., Kazantzidis V., Keeling D. L., Kelly R., Kempenaars M., Kennedy C., Kennedy D., Kent J., Khan K., Kiefer C., Kilpelainen J., Kim C., Kim H. -T., Kim S. H., King D. B., King R., Kinna D., Kiptily V. G., Kirjasuo A., Kirov K. K., Kirschner A., Kiviniemi T., Kizane G., Klas M., Klepper C., Klix A., Kneale G., Knight M., Knight P., Knights R., Knipe S., Knolker M., Knott S., Kocan M., Kochl F., Kodeli I., Kolesnichenko Y., Kominis Y., Kong M., Korovin V., Kos B., Kos D., Koslowski H. R., Kotschenreuther M., Koubiti M., Kowalska-Strzeciwilk E., Koziol K., Krasilnikov V., Kresina M., Krieger K., Krishnan N., Krivska A., Kruezi U., Ksiazek I., Kukushkin A. B., Kumpulainen H., Kurki-Suonio T., Kurotaki H., Kwak S., Kwon O. J., Laguardia L., Lagzdina E., Lahtinen A., Laing A., Lam N., Lambertz H. T., Lane B., Lane C., Lascas Neto E., Laszynska E., Lawson K. D., Lazaros A., Lazzaro E., Learoyd G., Lee C., Lee S. E., Leerink S., Leeson T., Lefebvre X., Leggate H. J., Lehmann J., Lehnen M., Leichtle D., Leipold F., Lengar I., Lennholm M., Leon Gutierrez E., Lepiavko B., Leppanen J., Lerche E., Lescinskis A., Lewis J., Leysen W., Li L., Li Y., Likonen J., Linsmeier C., Lipschultz B., Litaudon X., Litherland-Smith E., Liu F., Loarer T., Loarte A., Lobel R., Lomanowski B., Lomas P. J., Lopez J. M., Lorenzini R., Loreti S., Losada U., Loschiavo V. P., Loughlin M., Louka Z., Lovell J., Lowe T., Lowry C., Lubbad S., Luce T., Lucock R., Luna C., de la Luna E., Lungaroni M., Lungu C. P., Lunt T., Lutsenko V., Lyons B., Lyssoivan A., Machielsen M., Macusova E., Maenpaa R., Maggi C. F., Maggiora R., Magness M., Mahesan S., Maier H., Mailloux J., Maingi R., Malinowski K., Manas P., Mantica P., Mantsinen M. J., Manyer J., Manzanares A., Maquet P., Marceca G., Marchetto C., Marchuk O., Mariani A., Mariano G., Marin M., Marinelli M., Markovic T., Marocco D., Marot L., Marsden S., Marsh J., Marshall R., Martellucci L., Martin A., Martin A. J., Martone R., Maruyama S., Maslov M., Masuzaki S., Matejcik S., Mattei M., Matthews G. F., Matveev D., Matveeva E., Mauriya A., Maviglia F., Mayer M., Mayoral M. -L., Mazzotta C., McAdams R., McCarthy P. J., McClements K. G., McClenaghan J., McCullen P., McDonald D. C., McGuckin D., McHugh D., McIntyre G., McKean R., McKehon J., McMillan B., McNamee L., McShee A., Meakins A., Medley S., Meekes C. J., Meghani K., Meigs A. G., Meisl G., Meitner S., Menmuir S., Mergia K., Merriman S., Mertens P., Messiaen A., Michling R., Middleton P., Middleton-Gear D., Mietelski J., Milanesio D., Milani E., Militello F., Militello Asp A., Milnes J., Milocco A., Miloshevsky G., Minghao C., Minucci S., Miron I., Miyamoto M., Mlynar J., Moiseenko V., Monaghan P., Monakhov I., Moody T., Moon S., Mooney R., Moradi S., Morales J., Morales R. B., Mordijck S., Moreira L., Morgan L., Moro F., Morris J., Morrison K. -M., Moser L., Moulton D., Mrowetz T., Mundy T., Muraglia M., Murari A., Muraro A., Muthusonai N., N'Konga B., Na Y. -S., Nabais F., Naden M., Naish J., Naish R., Napoli F., Nardon E., Naulin V., Nave M. F. F., Nedzelskiy I., Nestoras I., Neu R., Ng S., Nicassio M., Nielsen A. H., Nina D., Nishijima D., Noble C., Nobs C. R., Nodwell D., Nordlund K., Nordman H., Normanton R., Noterdaeme J. -M., Nowak S., Nunn E., Nystrom H., Oberparleiter M., Obryk B., O'Callaghan J., Odupitan T., Oliver H. J. C., Olney R., O'Mullane M., Organ E., Orsitto F., Orszagh J., Osborne T., Otin R., Otsuka T., Owen A., Oya Y., Oyaizu M., Paccagnella R., Pace N., Packer L. W., Paige S., Pajuste E., Palade D., Pamela S. J. P., Panadero N., Panontin E., Papadopoulos A., Papp G., Papp P., Parail V. V., Pardanaud C., Parisi J., Parra Diaz F., Parsloe A., Parsons M., Parsons N., Passeri M., Patel A., Pau A., Pautasso G., Pavlichenko R., Pavone A., Pawelec E., Soldan C. P., Peacock A., Pearce M., Peluso E., Penot C., Pepperell K., Pereira R., Pereira T., Cippo E. P., Pereslavtsev P., von Thun C. P., Pericoli V., Perry D., Peterka M., Petersson P., Petravich G., Petrella N., Peyman M., Pillon M., Pinches S., Pintsuk G., de Sa W. P., dos Reis A. P., Piron C., Piron L., Pironti A., Pitts R., van de Plassche K. L., Platt N., Plyusnin V., Podesta M., Pokol G., Poli F. M., Pompilian O. G., Popovichev S., Poradzinski M., Porfiri M. T., Porkolab M., Porosnicu C., Porton M., Poulipoulis G., Predebon I., Prestopino G., Price C., Price D., Price M., Primetzhofer D., Prior P., Provatas G., Pucella G., Puglia P., Purahoo K., Pusztai I., Putignano O., Putterich T., Quercia A., Rachlew E., Radulescu G., Radulovic V., Rainford M., Raj P., Ralph G., Ramogida G., Rasmussen D., Rasmussen J. J., Ratta G., Ratynskaia S., Rebai M., Refy D., Reichle R., Reinke M., Reiser D., Reux C., Reynolds S., Richiusa M. L., Richyal S., Rigamonti D., Rimini F. G., Risner J., Riva M., Rivero-Rodriguez J., Roach C. M., Robins R., Robinson S., Robson D., Rodrigues P., Rodriguez Ramos M., Rodriguez-Fernandez P., Romanelli F., Romanelli M., Romanelli S., Romazanov J., Rossi R., Rowe S., Rowlands D., Rubel M., Rubinacci G., Rubino G., Ruchko L., Ruiz M., Ruiz J. R., Ruset C., Rzadkiewicz J., Saarelma S., Safi E., Salewski M., Salmi A., Salmon R., Salzedas F., Sanders I., Sandiford D., Santos B., Santucci A., Sarkimaki K., Sarwar R., Sarychev I., Sauter O., Sauwan P., Scapin N., Schluck F., Schmid K., Schmuck S., Schneider M., Schneider P. A., Schworer D., Scott G., Scott M., Scraggs D., Scully S., Segato M., Seo J., Sergienko G., Sertoli M., Sharapov S. E., Shaw A., Sheikh H., Sheikh U., Shepherd A., Shigin P., Shinohara K., Shiraiwa S., Shiraki D., Short M., Sias G., Silburn S. A., Silva A., Silva C., Silva J., Silvagni D., Simfukwe D., Simpson J., Sinclair D., Sipila S. K., Sips A. C. C., Siren P., Sirinelli A., Sjostrand H., Skinner N., Slater J., Smith N., Smith P., Snell J., Snoep G., Snoj L., Snyder P., Soare S., Solano E. 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.
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- 2022
33. Gyrokinetic analysis of an argon-seeded EDA H-mode in ASDEX Upgrade
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Stimmel, K, Gil, L, Gorler, T, Cavedon, M, David, P, Dunne, M, Dux, R, Fischer, R, Jenko, F, Kallenbach, A, Mcdermott, R, Plank, U, Tardini, G, Told, D, Stimmel K., Gil L., Gorler T., Cavedon M., David P., Dunne M., Dux R., Fischer R., Jenko F., Kallenbach A., McDermott R. M., Plank U., Tardini G., Told D., Stimmel, K, Gil, L, Gorler, T, Cavedon, M, David, P, Dunne, M, Dux, R, Fischer, R, Jenko, F, Kallenbach, A, Mcdermott, R, Plank, U, Tardini, G, Told, D, Stimmel K., Gil L., Gorler T., Cavedon M., David P., Dunne M., Dux R., Fischer R., Jenko F., Kallenbach A., McDermott R. M., Plank U., Tardini G., and Told D.
- Abstract
Understanding edge-localised-mode (ELM)-free high-confinement (H-)mode scenarios is vital for developing practical future demonstration reactor scenarios. An argon-seeded EDA H-mode discharge performed in ASDEX Upgrade is computationally studied in detail for the first time with the gyrokinetic GENE code using experimental profiles and magnetic equilibrium as direct code inputs. Linear scans outline dominant instabilities in the regime and reveal distinct ion- and electron-scale wavenumber growth-rate peaks for two local core and two local pedestal top scenarios. Linear ion-scale growth rates are found to be relatively insensitive to the addition of argon, and collisionality scans demonstrate increased sensitivity in the pedestal top. The addition of an argon impurity profile while keeping the input main ion temperature gradient (ITG) largely unchanged is found to reduce ITG-driven turbulence in the outer core. Nonlinear electromagnetic simulations reveal close agreement with experimentally predicted heat fluxes in the core, outline key sensitivities to electron and background shearing, and reveal gyrokinetic challenges in analysing the quasicoherent mode. Global electrostatic nonlinear simulations reduce local simulated heat transport overpredictions at the pedestal top. A quasilinear analysis finds that there is good core agreement but poor agreement in the pedestal between linear and nonlinear temperature and density fluctuation cross-phases. Local simulation limitations are elucidated and paths forward for future computation are suggested.
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- 2022
34. Non-parametric inference of impurity transport coefficients in the ASDEX Upgrade tokamak
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Nishizawa, T, Dux, R, Mcdermott, R, Sciortino, F, Cavedon, M, Schuster, C, Wolfrum, E, Von Toussaint, U, Van Vuuren, A, Cruz-Zabala, D, Cano-Megias, P, Moon, C, Nishizawa T., Dux R., McDermott R. M., Sciortino F., Cavedon M., Schuster C., Wolfrum E., Von Toussaint U., Van Vuuren A. J., Cruz-Zabala D. J., Cano-Megias P., Moon C., Nishizawa, T, Dux, R, Mcdermott, R, Sciortino, F, Cavedon, M, Schuster, C, Wolfrum, E, Von Toussaint, U, Van Vuuren, A, Cruz-Zabala, D, Cano-Megias, P, Moon, C, Nishizawa T., Dux R., McDermott R. M., Sciortino F., Cavedon M., Schuster C., Wolfrum E., Von Toussaint U., Van Vuuren A. J., Cruz-Zabala D. J., Cano-Megias P., and Moon C.
- Abstract
We present a non-parametric inference of impurity transport coefficients by using charge exchange recombination spectroscopy measurements of Ne X, Ne VIII, O VIII, and C VI lines. Due to their close atomic numbers, neon, oxygen and carbon impurity ions are assumed to have the same diffusion coefficient D and convection velocity v. Unlike conventional techniques that modulate or perturb the impurity contents, we employ a quasi-stationary plasma with static impurity profiles. Since the ratio of v to D only describes the equilibrated profile of the sum of all impurity charge states, steady-state measurements can still decouple D and v if different charge states are simultaneously observed. We have formulated a non-parametric analysis framework based on the Bayesian probability theory and conducted transport coefficient measurements for a Type III ELMy H-mode plasma at ASDEX Upgrade. The charge exchange reactions with the background neutrals, which are known to affect the impurity charge state balance, are taken into account by introducing additional free parameters. While D at the pedestal is close to the neoclassical level ( < 1 m s-2), a large diffusion coefficient and a strong outward convection are inferred right inside the pedestal top.
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- 2022
35. Experimental Investigations of the H-mode Access in Mixed Hydrogen-Deuterium Plasmas at ASDEX Upgrade
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Plank, U, Putterich, T, Angioni, C, Conway, G, Dux, R, Happel, T, Bonanomi, N, Cavedon, M, Gil, L, Mcdermott, R, Schneider, P, Plank U., Putterich T., Angioni C., Conway G. D., Dux R., Happel T., Bonanomi N., Cavedon M., Gil L., McDermott R. M., Schneider P. A., Plank, U, Putterich, T, Angioni, C, Conway, G, Dux, R, Happel, T, Bonanomi, N, Cavedon, M, Gil, L, Mcdermott, R, Schneider, P, Plank U., Putterich T., Angioni C., Conway G. D., Dux R., Happel T., Bonanomi N., Cavedon M., Gil L., McDermott R. M., and Schneider P. A.
- Published
- 2022
36. Physics Exploitation of the new Divertor Thomson Scattering at ASDEX Upgrade
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Cavedon, M, Dux, R, Kurzan, B, Bernert, M, Brida, D, Henderson, S, Nishizawa, T, Lunt, T, Pan, O, Reimold, F, Stroth, U, Wischmeier, M, Wu, H, Cavedon M., Dux R., Kurzan B., Bernert M., Brida D., Henderson S., Nishizawa T., Lunt T., Pan O., Reimold F., Stroth U., Wischmeier M., Wu H., Cavedon, M, Dux, R, Kurzan, B, Bernert, M, Brida, D, Henderson, S, Nishizawa, T, Lunt, T, Pan, O, Reimold, F, Stroth, U, Wischmeier, M, Wu, H, Cavedon M., Dux R., Kurzan B., Bernert M., Brida D., Henderson S., Nishizawa T., Lunt T., Pan O., Reimold F., Stroth U., Wischmeier M., and Wu H.
- Published
- 2022
37. Experimental helium exhaust studies in the full-W ASDEX Upgrade
- Author
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Zito, A, Kappatou, A, Wischmeier, M, Kallenbach, A, Rohde, V, Hinson, E, Schmitz, O, Cavedon, M, Mcdermott, R, Dux, R, Griener, M, Stroth, U, Zito A., Kappatou A., Wischmeier M., Kallenbach A., Rohde V., Hinson E., Schmitz O., Cavedon M., McDermott R. M., Dux R., Griener M., Stroth U., Zito, A, Kappatou, A, Wischmeier, M, Kallenbach, A, Rohde, V, Hinson, E, Schmitz, O, Cavedon, M, Mcdermott, R, Dux, R, Griener, M, Stroth, U, Zito A., Kappatou A., Wischmeier M., Kallenbach A., Rohde V., Hinson E., Schmitz O., Cavedon M., McDermott R. M., Dux R., Griener M., and Stroth U.
- Published
- 2022
38. In-out charge exchange measurements and 3D modelling of diagnostic thermal neutrals to study edge poloidal impurity asymmetries
- Author
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Cruz-Zabala, D, Viezzer, E, Plank, U, Mcdermott, R, Cavedon, M, Fable, E, Dux, R, Cano-Megias, P, Putterich, T, Van Vuuren, A, Garcia-Munoz, M, Garcia Lopez, J, Cruz-Zabala D. J., Viezzer E., Plank U., McDermott R. M., Cavedon M., Fable E., Dux R., Cano-Megias P., Putterich T., Van Vuuren A. J., Garcia-Munoz M., Garcia Lopez J., Cruz-Zabala, D, Viezzer, E, Plank, U, Mcdermott, R, Cavedon, M, Fable, E, Dux, R, Cano-Megias, P, Putterich, T, Van Vuuren, A, Garcia-Munoz, M, Garcia Lopez, J, Cruz-Zabala D. J., Viezzer E., Plank U., McDermott R. M., Cavedon M., Fable E., Dux R., Cano-Megias P., Putterich T., Van Vuuren A. J., Garcia-Munoz M., and Garcia Lopez J.
- Abstract
A new method was developed to model the neutral population produced by the gas puff based charge exchange recombination spectroscopy systems at ASDEX Upgrade (AUG). With this method, the edge impurity density on the high field side (HFS) and low field side (LFS) can be obtained without the need to apply a neutral beam injection system. The neutral penetration needed for the calculation of the impurity density is obtained with a new gas puff module implemented in the FIDASIM code. The LFS impurity density profile evaluated with the new gas puff module matches the impurity density calculated with standard beam-based charge exchange diagnostics. Impurity temperature, rotation and density profiles at the HFS and LFS of an AUG H-mode discharge are presented. Edge impurity toroidal and poloidal flows show asymmetric structures. The impurity density asymmetries obtained with the new gas puff module are consistent with the observed flow structure.
- Published
- 2022
39. Model for access and stability of the X-point radiator and the threshold for marfes in tokamak plasmas
- Author
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Stroth, U, Bernert, M, Brida, D, Cavedon, M, Dux, R, Huett, E, Lunt, T, Pan, O, Wischmeier, M, Stroth U., Bernert M., Brida D., Cavedon M., Dux R., Huett E., Lunt T., Pan O., Wischmeier M., Stroth, U, Bernert, M, Brida, D, Cavedon, M, Dux, R, Huett, E, Lunt, T, Pan, O, Wischmeier, M, Stroth U., Bernert M., Brida D., Cavedon M., Dux R., Huett E., Lunt T., Pan O., and Wischmeier M.
- Abstract
Based on particle and energy balances, a reduced model is derived for the physical mechanisms leading to the occurrence of stable and unstable X-point radiators (XPRs), the latter also known as marfes. The leading roles of the neutral deuterium density in the divertor region for initiating XPRs is highlighted. An access condition is formulated whose parameter dependencies are consistent with experimental observations and which could also apply to the process of divertor detachment. With an exponential increase of the recombination rate at low temperature, the XPR becomes magnetohydrodynamically unstable, leading to a marfe and, possibly, to a disruption. A critical density for marfe occurrence is formulated with the upstream density and safety factor as leading parameters, as in the experiment. Marfes are predicted to be more likely in carbon devices than in impurity-seeded plasmas in tungsten devices. The edge plasma parameter domain where marfes occur resembles that used for active marfe avoidance schemes. Both the XPR and marfe occurrence parameter can be used to guide active discharge control.
- Published
- 2022
40. Experimental investigation of L- and H-mode detachment via the divertor Thomson scattering at ASDEX Upgrade
- Author
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Cavedon, M, Kurzan, B, Bernert, M, Brida, D, Dux, R, Griener, M, Henderson, S, Huett, E, Nishizawa, T, Lunt, T, Pan, O, Stroth, U, Wischmeier, M, Wolfrum, E, Cavedon M., Kurzan B., Bernert M., Brida D., Dux R., Griener M., Henderson S., Huett E., Nishizawa T., Lunt T., Pan O., Stroth U., Wischmeier M., Wolfrum E., Cavedon, M, Kurzan, B, Bernert, M, Brida, D, Dux, R, Griener, M, Henderson, S, Huett, E, Nishizawa, T, Lunt, T, Pan, O, Stroth, U, Wischmeier, M, Wolfrum, E, Cavedon M., Kurzan B., Bernert M., Brida D., Dux R., Griener M., Henderson S., Huett E., Nishizawa T., Lunt T., Pan O., Stroth U., Wischmeier M., and Wolfrum E.
- Abstract
The capabilities of the newly installed divertor Thomson Scattering (DTS) diagnostic (Kurzan et al 2021 J. Inst. 16 C09012) at ASDEX Upgrade (AUG) have been demonstrated by measuring 2D electron densities n e and temperatures T e from attached to fully detached divertor conditions in L- and H-mode. The collected dataset is a breakthrough for divertor studies at AUG in which such measurements have been so far missing. Besides highlighting the strengths and limits of the DTS system, this work provides confirmations and new insights into detachment physics. The transition between partial and pronounced detachment correlates with a 2D redistribution of the electron density from the inner to the outer divertor in both L- and H-mode. In pronounced detachment, a strong parallel pressure gradient could be confirmed throughout the complete SOL. Finally, measurements of n e and T e of a stable X-point radiator revealed local temperatures as low as 1 eV within the confined plasma, whereas the pressure is shown to be constant on closed field lines.
- Published
- 2022
41. Validation of low-Z impurity transport theory using boron perturbation experiments at ASDEX upgrade
- Author
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Mcdermott, R, Angioni, C, Cavedon, M, Kappatou, A, Dux, R, Fischer, R, Manas, P, McDermott R. M., Angioni C., Cavedon M., Kappatou A., Dux R., Fischer R., Manas P., Mcdermott, R, Angioni, C, Cavedon, M, Kappatou, A, Dux, R, Fischer, R, Manas, P, McDermott R. M., Angioni C., Cavedon M., Kappatou A., Dux R., Fischer R., and Manas P.
- Abstract
An experimental technique has been developed at ASDEX upgrade (AUG) to separately identify the diffusive and convective components of the boron particle flux. Using this technique a database of B transport coefficients has been assembled that shows that the normalized ion temperature gradient () is the strongest organizing parameter for both the B diffusion and convection and large is a necessary ingredient to obtain hollow B density profiles in AUG. This database also shows that large changes in the applied neutral beam injection (NBI) have a relatively small impact on impurity transport compared to similar changes in electron cyclotron resonance heating (ECRH). Even low levels of ECRH power dramatically increase both the diffusive and convective fluxes and lead to peaking of the impurity density profile. Comparisons to a combination of neoclassical and quasi-linear gyrokinetic simulations show good agreement in the measured and predicted diffusion coefficients. The outward convection measured in NBI dominated plasmas, however, is not well captured by the simulations, despite the inclusion of fast ions. In contrast, the convection is reasonably well reproduced for plasmas with flat or peaked boron density profiles. This dataset provides an excellent experimental validation of the non-monotonic, predicted, convective-particle-flux created by the combination of pure-pinch, thermo-diffusion, and roto-diffusion. In addition, this dataset demonstrates a non-monotonic dependence of the experimental particle diffusivity to ion heat conductivity (D/? i) in qualitative agreement with theoretical predictions.
- Published
- 2022
42. Wall conditioning effects and boron migration during boron powder injection in ASDEX Upgrade
- Author
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Krieger, K., primary, Balden, M., additional, Bortolon, A., additional, Dux, R., additional, Griener, M., additional, Hegele, K., additional, Laggner, F., additional, Rohde, V., additional, and Wampler, W.R., additional
- Published
- 2023
- Full Text
- View/download PDF
43. Trends of W behavior in ICRF assisted discharges in ASDEX Upgrade
- Author
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Czarnecka, A., Bobkov, V., Dux, R., Pütterich, T., and Sertoli, M.
- Published
- 2015
- Full Text
- View/download PDF
44. Formation of the high density front in the inner far SOL at ASDEX Upgrade and JET
- Author
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Potzel, S., Wischmeier, M., Bernert, M., Dux, R., Reimold, F., Scarabosio, A., Brezinsek, S., Clever, M., Huber, A., Meigs, A., and Stamp, M.
- Published
- 2015
- Full Text
- View/download PDF
45. SOLPS modelling of W arising from repetitive mitigated ELMs in ITER
- Author
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Coster, D.P., Chankin, A.V., Klingshirn, H.-J., Dux, R., Fable, E., Bonnin, X., Kukushkin, A., and Loarte, A.
- Published
- 2015
- Full Text
- View/download PDF
46. Development of ECRH-based methods for assisted discharge burn-through: experiment and simulation
- Author
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Ricci, D., Stober, J., Dux, R., Figini, L., Wauters, T., Lerche, E., Granucci, G., ASDEX Upgrade Team, Max Planck Institute for Plasma Physics, Max Planck Society, and Eurofusion WPTE Team
- Published
- 2023
47. Experimental study of the edge radial electric field in different drift configurations and its role in the access to H-mode at ASDEX Upgrade
- Author
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Plank, U., Brida, D., Conway, G., Happel, T., Hubbard, A., Pütterich, T., Angioni, C., Cavedon, M., Dux, R., Eich, T., Fischer, R., Hennequin, P., and ASDEX Upgrade Team, Max Planck Institute for Plasma Physics, Max Planck Society
- Published
- 2023
48. Design study of an edge current density diagnostic using new high-performance single-channel beam emission spectrometers at DIII-D
- Author
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Albosta, R., primary, Geiger, B., additional, McKee, G., additional, Den Hartog, D., additional, Schellpfeffer, J., additional, Gallenberger, T., additional, Stewart, S., additional, and Dux, R., additional
- Published
- 2022
- Full Text
- View/download PDF
49. Gyrokinetic analysis of an argon-seeded EDA H-mode in ASDEX Upgrade
- Author
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Stimmel K., Gil L., Gorler T., Cavedon M., David P., Dunne M., Dux R., Fischer R., Jenko F., Kallenbach A., McDermott R. M., Plank U., Tardini G., Told D., ASDEX Upgrade Team, Max Planck Institute for Plasma Physics, Max Planck Society, Stimmel, K, Gil, L, Gorler, T, Cavedon, M, David, P, Dunne, M, Dux, R, Fischer, R, Jenko, F, Kallenbach, A, Mcdermott, R, Plank, U, Tardini, G, and Told, D
- Subjects
plasma instabilitie ,plasma simulation ,fusion plasma ,Condensed Matter Physics - Abstract
Understanding edge-localised-mode (ELM)-free high-confinement (H-)mode scenarios is vital for developing practical future demonstration reactor scenarios. An argon-seeded EDA H-mode discharge performed in ASDEX Upgrade is computationally studied in detail for the first time with the gyrokinetic GENE code using experimental profiles and magnetic equilibrium as direct code inputs. Linear scans outline dominant instabilities in the regime and reveal distinct ion- and electron-scale wavenumber growth-rate peaks for two local core and two local pedestal top scenarios. Linear ion-scale growth rates are found to be relatively insensitive to the addition of argon, and collisionality scans demonstrate increased sensitivity in the pedestal top. The addition of an argon impurity profile while keeping the input main ion temperature gradient (ITG) largely unchanged is found to reduce ITG-driven turbulence in the outer core. Nonlinear electromagnetic simulations reveal close agreement with experimentally predicted heat fluxes in the core, outline key sensitivities to electron $\beta$ and background $\boldsymbol{E\times B}$ shearing, and reveal gyrokinetic challenges in analysing the quasicoherent mode. Global electrostatic nonlinear simulations reduce local simulated heat transport overpredictions at the pedestal top. A quasilinear analysis finds that there is good core agreement but poor agreement in the pedestal between linear and nonlinear temperature and density fluctuation cross-phases. Local simulation limitations are elucidated and paths forward for future computation are suggested.
- Published
- 2022
50. Experimental helium exhaust studies in the full-W ASDEX Upgrade
- Author
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Zito A., Kappatou A., Wischmeier M., Kallenbach A., Rohde V., Hinson E., Schmitz O., Cavedon M., McDermott R. M., Dux R., Griener M., Stroth U., ASDEX Upgrade Team, Max Planck Institute for Plasma Physics, Max Planck Society, Zito, A, Kappatou, A, Wischmeier, M, Kallenbach, A, Rohde, V, Hinson, E, Schmitz, O, Cavedon, M, Mcdermott, R, Dux, R, Griener, M, and Stroth, U
- Subjects
plasma - Published
- 2022
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