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Giruzzi G, Fontana M, Orsitto F, de la Luna E, Dumont R, Figini L, Maslov M, Mazzi S, Schmuck S, Senni L, Sozzi C, Challis C, Frigione D, Garcia J, Garzotti L, Hobirk J, Kappatou A, Keeling D, Lerche E, Maggi C, Mailloux J, Rimini F, Van Eester D. A model of non-Maxwellian electron distribution function for the analysis of ECE data in JET discharges. EPJ Web Conf 2023. [DOI: 10.1051/epjconf/202327703005] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 02/25/2023] Open
Abstract
Recent experiments performed in JET at high level of plasma heating, in preparation of, and during the DT campaign have shown significant discrepancies between electron temperature measurements by Thomson Scattering (TS) and Electron Cyclotron Emission (ECE). In order to perform a systematic analysis of this phenomenon, a simple model of bipolar distortion of the electron distribution function has been developed, allowing analytic calculation of the EC emission and absorption coefficients. Extensive comparisons of the modelled ECE spectra (at both the 2nd and the 3rd harmonic extraordinary mode) with experimental measurements display good agreement when bulk electron distribution distortions around 1-2 times the electron thermal velocity are used and prove useful for a first level of analysis of this effect.
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2
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Fontana M, Giruzzi G, Orsitto FP, de la Luna E, Dumont R, Figini L, Kos D, Maslov M, Schmuck S, Sozzi C, Challis CD, Frigione D, Garcia J, Garzotti L, Hobirk J, Kappatou A, Keeling D, Lerche E, Maggi C, Mailloux J, Rimini F, Van Eester D. Investigation of Te measurements discrepancies between ECE and Thomson diagnostics in high-performance plasmas in JET. EPJ Web Conf 2023. [DOI: 10.1051/epjconf/202327703006] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 02/25/2023] Open
Abstract
For high-temperature JET and TFTR discharges, electron cyclotron emission (ECE) measurements of central electron temperature were systematically found to be up to 20% higher than those taken with Thomson scattering. In recent high-performance JET discharges, central Te measurements, performed with LIDAR Thomson scattering and the X-mode ECE interferometer, have been studied in a large database, including deuterium (DD), and deuterium-tritium plasmas (DT). Discrepancies between Te measurements have been observed outside of the experimental uncertainties. ECE measurements, at high Te, have been found to be higher or lower than those of LIDAR, depending on the specific plasma scenario. In addition, discrepancies between the peaks of the second and third harmonic ranges of the ECE spectrum have been interpreted as evidence for the presence of non-Maxwellian features in the electron distribution function. These comparisons seem to suggest that such features can be found in most of the high-performance scenarios selected in this JET database.
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3
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Bonofiglo PJ, Kiptily V, Goloborodko V, Štancar Ž, Podestà M, Cecil FE, Challis CD, Hobirk J, Kappatou A, Lerche E, Carvalho IS, Garcia J, Mailloux J, Maggi CF, Meigs AG. Lost alpha Faraday cup foil noise characterization during Joint European Torus plasma post-processing analysis. Rev Sci Instrum 2022; 93:093527. [PMID: 36182470 DOI: 10.1063/5.0099314] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/16/2022] [Accepted: 08/18/2022] [Indexed: 06/16/2023]
Abstract
Capacitive plasma pickup is a well-known and difficult problem for plasma-facing edge diagnostics. This problem must be addressed to ensure an accurate and robust interpretation of the real signal measurements vs noise. The Faraday cup fast ion loss detector array of the Joint European Torus (JET) is particularly prone to this issue and can be used as a testbed to prototype solutions. The issue of separation and distinction between warranted fast ion signal and electromagnetic plasma noise has traditionally been solved with hardware modifications, but a more versatile post-processing approach is of great interest. This work presents post-processing techniques to characterize the signal noise. While hardware changes and advancements may be limited, the combination with post-processing procedures allows for more rapid and robust analysis of measurements. The characterization of plasma pickup noise is examined for alpha losses in a discharge from JET's tritium campaign. In addition to highlighting the post-processing methodology, the spatial sensitivity of the detector array is also examined, which presents significant advantages for the physical interpretation of fast ion losses.
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Affiliation(s)
- P J Bonofiglo
- Princeton Plasma Physics Laboratory, Princeton, New Jersey 08540, USA
| | - V Kiptily
- UKAEA, CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom
| | - V Goloborodko
- Kyiv Institute for Nuclear Research, Prospekt Nauky 47, Kyiv 03680, Ukraine
| | - Ž Štancar
- UKAEA, CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom
| | - M Podestà
- Princeton Plasma Physics Laboratory, Princeton, New Jersey 08540, USA
| | - F E Cecil
- Colorado School of Mines, Golden, Colorado 80401, USA
| | - C D Challis
- UKAEA, CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom
| | - J Hobirk
- Max-Planck-Institut für Plasmaphysik, D-85748 Garching, Germany
| | - A Kappatou
- Max-Planck-Institut für Plasmaphysik, D-85748 Garching, Germany
| | - E Lerche
- UKAEA, CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom
| | - I S Carvalho
- Instituto de Plasmas e Fusão Nuclear, Instituto Superior Técnico, Universidade de Lisboa, 1049-001 Lisbon, Portugal
| | - J Garcia
- CEA-IRFM, F-13108 Saint Paul Lez Durance, France
| | - J Mailloux
- UKAEA, CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom
| | - C F Maggi
- UKAEA, CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom
| | - A G Meigs
- UKAEA, CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom
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Ford OP, Vanó L, Alonso JA, Baldzuhn J, Beurskens MNA, Biedermann C, Bozhenkov SA, Fuchert G, Geiger B, Hartmann D, Jaspers RJE, Kappatou A, Langenberg A, Lazerson SA, McDermott RM, McNeely P, Neelis TWC, Pablant NA, Pasch E, Rust N, Schroeder R, Scott ER, Smith HM, Wegner T, Kunkel F, Wolf RC. Charge exchange recombination spectroscopy at Wendelstein 7-X. Rev Sci Instrum 2020; 91:023507. [PMID: 32113444 DOI: 10.1063/1.5132936] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/21/2019] [Accepted: 01/16/2020] [Indexed: 06/10/2023]
Abstract
The Charge Exchange Recombination Spectroscopy (CXRS) diagnostic has become a routine diagnostic on almost all major high temperature fusion experimental devices. For the optimized stellarator Wendelstein 7-X (W7-X), a highly flexible and extensive CXRS diagnostic has been built to provide high-resolution local measurements of several important plasma parameters using the recently commissioned neutral beam heating. This paper outlines the design specifics of the W7-X CXRS system and gives examples of the initial results obtained, including typical ion temperature profiles for several common heating scenarios, toroidal flow and radial electric field derived from velocity measurements, beam attenuation via beam emission spectra, and normalized impurity density profiles under some typical plasma conditions.
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Affiliation(s)
- O P Ford
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - L Vanó
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - J A Alonso
- CIEMAT, Avenida Complutense, 40, 28040 Madrid, Spain
| | - J Baldzuhn
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - M N A Beurskens
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - C Biedermann
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - S A Bozhenkov
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - G Fuchert
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - B Geiger
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - D Hartmann
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - R J E Jaspers
- Eindhoven University of Technology, 5612 AZ Eindhoven, The Netherlands
| | - A Kappatou
- Max-Planck Institut für Plasmaphysik, 85748 Garching, Germany
| | - A Langenberg
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - S A Lazerson
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - R M McDermott
- Eindhoven University of Technology, 5612 AZ Eindhoven, The Netherlands
| | - P McNeely
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - T W C Neelis
- Eindhoven University of Technology, 5612 AZ Eindhoven, The Netherlands
| | - N A Pablant
- Princeton University Plasma Physics Laboratory, Princeton, New Jersey 08544, USA
| | - E Pasch
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - N Rust
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - R Schroeder
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - E R Scott
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - H M Smith
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - Th Wegner
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - F Kunkel
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - R C Wolf
- Max-Planck Institut für Plasmaphysik, 17491 Greifswald, Germany
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McDermott RM, Lebschy A, Geiger B, Bruhn C, Cavedon M, Dunne M, Dux R, Fischer R, Kappatou A, Pütterich T, Viezzer E. Extensions to the charge exchange recombination spectroscopy diagnostic suite at ASDEX Upgrade. Rev Sci Instrum 2017; 88:073508. [PMID: 28764552 DOI: 10.1063/1.4993131] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/07/2023]
Abstract
A new core charge exchange recombination spectroscopy diagnostic has been installed in the ASDEX Upgrade tokamak that is capable of measuring the impurity ion temperature, toroidal rotation, and density on both the low field side (LFS) and high field side (HFS) of the plasma. The new system features 48 lines-of-sight (LOS) with a radial resolution that varies from ±2 cm on the LFS down to ±0.75 cm on the HFS and has sufficient signal to run routinely at 10 ms and for special circumstances down to 2.5 ms integration time. The LFS-HFS ion temperature profiles provide an additional constraint on the magnetic equilibrium reconstruction, and the toroidal rotation frequency profiles are of sufficiently high quality that information on the poloidal velocity can be extracted from the LFS-HFS asymmetry. The diagnostic LOS are coupled to two flexible-wavelength spectrometers such that complete LFS-HFS profiles from two separate impurities can be imaged simultaneously, albeit with reduced radial coverage. More frequently, the systems measure the same impurity providing very detailed information on the chosen species. Care has been taken to calibrate the systems as accurately as possible and to include in the data analysis any effects that could lead to spurious temperatures or rotations.
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Affiliation(s)
- R M McDermott
- Max-Planck-Institut für Plasmaphysik, Boltzmannstr. 2, 85748 Garching, Germany
| | - A Lebschy
- Max-Planck-Institut für Plasmaphysik, Boltzmannstr. 2, 85748 Garching, Germany
| | - B Geiger
- Max-Planck-Institut für Plasmaphysik, Wendelsteinstr. 1, 17491 Greifswald, Germany
| | - C Bruhn
- Max-Planck-Institut für Plasmaphysik, Boltzmannstr. 2, 85748 Garching, Germany
| | - M Cavedon
- Max-Planck-Institut für Plasmaphysik, Boltzmannstr. 2, 85748 Garching, Germany
| | - M Dunne
- Max-Planck-Institut für Plasmaphysik, Boltzmannstr. 2, 85748 Garching, Germany
| | - R Dux
- Max-Planck-Institut für Plasmaphysik, Boltzmannstr. 2, 85748 Garching, Germany
| | - R Fischer
- Max-Planck-Institut für Plasmaphysik, Boltzmannstr. 2, 85748 Garching, Germany
| | - A Kappatou
- Max-Planck-Institut für Plasmaphysik, Boltzmannstr. 2, 85748 Garching, Germany
| | - T Pütterich
- Max-Planck-Institut für Plasmaphysik, Boltzmannstr. 2, 85748 Garching, Germany
| | - E Viezzer
- Department of Atomic, Molecular and Nuclear Physics, University of Seville, Avenida Reina Mercedes, 41012 Seville, Spain
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Griener M, Schmitz O, Bald K, Bösser D, Cavedon M, De Marné P, Eich T, Fuchert G, Herrmann A, Kappatou A, Lunt T, Rohde V, Schweer B, Sochor M, Stroth U, Terra A, Wolfrum E. Fast piezoelectric valve offering controlled gas injection in magnetically confined fusion plasmas for diagnostic and fuelling purposes. Rev Sci Instrum 2017; 88:033509. [PMID: 28372367 DOI: 10.1063/1.4978629] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/07/2023]
Abstract
In magnetically confined fusion plasmas controlled gas injection is crucial for plasma fuelling as well as for various diagnostic applications such as active spectroscopy. We present a new, versatile system for the injection of collimated thermal gas beams into a vacuum chamber. This system consists of a gas pressure chamber, sealed by a custom made piezo valve towards a small capillary for gas injection. The setup can directly be placed inside of the vacuum chamber of fusion devices as it is small and immune against high magnetic fields. This enables gas injection close to the plasma periphery with high duty cycles and fast switch on/off times ≲ 0.5 ms. In this work, we present the design details of this new injection system and a systematic characterization of the beam properties as well as the gas flowrates which can be accomplished. The thin and relatively short capillary yields a small divergence of the injected beam with a half opening angle of 20°. The gas box is designed for pre-fill pressures of 10 mbar up to 100 bars and makes a flowrate accessible from 1018 part/s up to 1023 part/s. It hence is a versatile system for both diagnostic as well as fuelling applications. The implementation of this system in ASDEX Upgrade will be described and its application for line ratio spectroscopy on helium will be demonstrated on a selected example.
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Affiliation(s)
- M Griener
- Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany
| | - O Schmitz
- Department of Engineering Physics, University of Wisconsin-Madison, Madison, Wisconsin 53706, USA
| | - K Bald
- Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany
| | - D Bösser
- Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany
| | - M Cavedon
- Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany
| | - P De Marné
- Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany
| | - T Eich
- Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany
| | - G Fuchert
- Max Planck Institute for Plasma Physics, Wendelsteinstr. 1, 17491 Greifswald, Germany
| | - A Herrmann
- Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany
| | - A Kappatou
- Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany
| | - T Lunt
- Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany
| | - V Rohde
- Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany
| | - B Schweer
- FZ Jülich, Institute for Energy- and Climate Research, 52428 Jülich, Germany
| | - M Sochor
- Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany
| | - U Stroth
- Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany
| | - A Terra
- FZ Jülich, Institute for Energy- and Climate Research, 52428 Jülich, Germany
| | - E Wolfrum
- Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany
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7
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Kappatou A, Jaspers RJE, Delabie E, Marchuk O, Biel W, Jakobs MA. Method to obtain absolute impurity density profiles combining charge exchange and beam emission spectroscopy without absolute intensity calibration. Rev Sci Instrum 2012; 83:10D519. [PMID: 23126860 DOI: 10.1063/1.4732847] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/01/2023]
Abstract
Investigation of impurity transport properties in tokamak plasmas is essential and a diagnostic that can provide information on the impurity content is required. Combining charge exchange recombination spectroscopy (CXRS) and beam emission spectroscopy (BES), absolute radial profiles of impurity densities can be obtained from the CXRS and BES intensities, electron density and CXRS and BES emission rates, without requiring any absolute calibration of the spectra. The technique is demonstrated here with absolute impurity density radial profiles obtained in TEXTOR plasmas, using a high efficiency charge exchange spectrometer with high etendue, that measures the CXRS and BES spectra along the same lines-of-sight, offering an additional advantage for the determination of absolute impurity densities.
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Affiliation(s)
- A Kappatou
- FOM Institute DIFFER - Dutch Institute for Fundamental Energy Research, Association EURATOM-FOM, 3430 BE Nieuwegein, The Netherlands.
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Jaspers RJE, Scheffer M, Kappatou A, van der Valk NCJ, Durkut M, Snijders B, Marchuk O, Biel W, Pokol GI, Erdei G, Zoletnik S, Dunai D. A high etendue spectrometer suitable for core charge eXchange recombination spectroscopy on ITER. Rev Sci Instrum 2012; 83:10D515. [PMID: 23126857 DOI: 10.1063/1.4732058] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/01/2023]
Abstract
A feasibility study for the use of core charge exchange recombination spectroscopy on ITER has shown that accurate measurements on the helium ash require a spectrometer with a high etendue of 1mm(2)sr to comply with the measurement requirements [S. Tugarinov et al., Rev. Sci. Instrum. 74, 2075 (2003)]. To this purpose such an instrument has been developed consisting of three separate wavelength channels (to measure simultaneously He/Be, C/Ne, and H/D/T together with the Doppler shifted direct emission of the diagnostic neutral beam, the beam emission (BES) signal), combining high dispersion (0.02 nm/pixel), sufficient resolution (0.2 nm), high efficiency (55%), and extended wavelength range (14 nm) at high etendue. The combined measurement of the BES along the same sightline within a third wavelength range provides the possibility for in situ calibration of the charge eXchange recombination spectroscopy signals. In addition, the option is included to use the same instrument for measurements of the fast fluctuations of the beam emission intensity up to 2 MHz, with the aim to study MHD activity.
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Affiliation(s)
- R J E Jaspers
- Science and Technology of Nuclear Fusion, Eindhoven University of Technology, Eindhoven, The Netherlands.
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