A tomographic algorithm for obtaining the 2D emission of D? and D? in the divertor region of ASDEX Upgrade is developed. It allows for characterizing the time and space evolution of the D emission in the visible range, in particular when the electron density increases during the discharge. At higher Greenwald fraction, the density profile in the scrape-off layer (SOL) becomes flatter, with the formation of a shoulder. With this phenomenon, a change in the SOL transport is observed, with a modification in the behavior of turbulent blobs, which become larger. At the same time, the tomography shows that visible emission, which is localized in the inner divertor target at lower ne, extends in the whole divertor region when density increases, and this effect can be due to a change in ne, Te and neutral profile density. From the measurements of D? and D? emission it is possible to estimate these quantities, and thus studying the role of the divertor neutrals on the shoulder formation. In fact they could lead to density shoulder formation by reducing the flow of ions parallel to the field and by changing the radial electric field affecting SOL turbulence and blobs characteristics [1]. [1] A.Wynn et al., 2018 Nucl. Fusion 58 056001

Reconstruction of visible emission in ASDEX Upgrade divertor

Agostini M;Vianello N;Carraro L;Spolaore M;
2018

Abstract

A tomographic algorithm for obtaining the 2D emission of D? and D? in the divertor region of ASDEX Upgrade is developed. It allows for characterizing the time and space evolution of the D emission in the visible range, in particular when the electron density increases during the discharge. At higher Greenwald fraction, the density profile in the scrape-off layer (SOL) becomes flatter, with the formation of a shoulder. With this phenomenon, a change in the SOL transport is observed, with a modification in the behavior of turbulent blobs, which become larger. At the same time, the tomography shows that visible emission, which is localized in the inner divertor target at lower ne, extends in the whole divertor region when density increases, and this effect can be due to a change in ne, Te and neutral profile density. From the measurements of D? and D? emission it is possible to estimate these quantities, and thus studying the role of the divertor neutrals on the shoulder formation. In fact they could lead to density shoulder formation by reducing the flow of ions parallel to the field and by changing the radial electric field affecting SOL turbulence and blobs characteristics [1]. [1] A.Wynn et al., 2018 Nucl. Fusion 58 056001
2018
Istituto gas ionizzati - IGI - Sede Padova
Inglese
60th Annual Meeting of the APS Division of Plasma Physics
http://meetings.aps.org/Meeting/DPP18/Session/PP11.28
November 5-9, 2018
Portland, Oregon
ASDEX Upgrade
ASDEX Divertor
PP11.00028
12
info:eu-repo/semantics/conferenceObject
none
274
04 Contributo in convegno::04.02 Abstract in Atti di convegno
Agostini, M; Vianello, N; Carralero, D; Carraro, L; Cavedon, M; Dux, R; Lunt, T; Naulin, V; Spolaore, M; Wolfrum, E; the ASDEX Upgrade, Team; the EURO...espandi
   Implementation of activities described in the Roadmap to Fusion during Horizon 2020 through a Joint programme of the members of the EUROfusion consortium
   EUROfusion
   H2020
   633053
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/356133
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