TJ-II:L-H transition studies: characterization of plasma turbulence using Gas Puff Imaging, Probes, Doppler reflectometry and HIBP diagnostics: Difference between revisions

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== Description of the activity ==
== Description of the activity ==
At TJ-II, spontaneous L-H transitions are achieved in neutral beam injection (NBI) heated plasma. Abrupt as well as gradual transitions are achieved depending, among other plasma parameters, on the heating power and magnetic configuration topology. Doppler reflectometry (DR) measurements show an increase in the negative radial electric field (Er) together with a reduction in plasma turbulence at the transition [1]. These measurements together with measurements obtained using a dual Langmuir probe system [2] show that the trigger of the L-H transition is more correlated with the development of fluctuating radial electric fields than steady-state Er effects. This conclusion is further stressed when operating close to the L-H transition threshold conditions, where pronounced oscillations in both, Er and density turbulence measured by DR show a characteristic predator-prey relation [3]. These experimental observations are consistent with L-H transition models based on turbulence-induced sheared/zonal flows.  In addition, HIBP measurements have shown a reduction in the plasma turbulence and associated flux not only in the plasma edge region but also in the plasma core [4].
At TJ-II, spontaneous L-H transitions are achieved in neutral beam injection (NBI) heated plasma. Abrupt as well as gradual transitions are achieved depending, among other plasma parameters, on the heating power and magnetic configuration topology. Doppler reflectometry (DR) measurements show an increase in the negative radial electric field (Er) together with a reduction in plasma turbulence at the transition [1]. These measurements together with measurements obtained using a dual Langmuir probe system [2] show that the trigger of the L-H transition is more correlated with the development of fluctuating radial electric fields than steady-state Er effects. This conclusion is further stressed when operating close to the L-H transition threshold conditions, where pronounced oscillations in both, Er and density turbulence measured by DR show a characteristic predator-prey relation [3]. These experimental observations are consistent with L-H transition models based on turbulence-induced sheared/zonal flows.  In addition, HIBP measurements show a reduction in the plasma turbulence and associated flux not only in the plasma edge region but also in the plasma core [4].
Recently a Gas Puff Imaging system (GPI) has been installed and tested at TJ-II.  The new gas injection system is used with a camera system that allows 3 simultaneous filtered frames to apply the He I ratio technique, getting 2D measurements of the edge plasma electron density ne and temperature Te with spatial resolution of 3 mm and temporal resolution down to 10 microseconds [5]. This new diagnostic will permit the 2-D characterization of edge and SOL plasma turbulence and is expected to provide additional valuable information on the behaviour of the turbulence during the L-H transition.
Recently a Gas Puff Imaging system (GPI) has been installed and tested at TJ-II.  The new gas injection system is used with a camera system that allows 3 simultaneous filtered frames to apply the He I ratio technique, getting 2D measurements of the edge plasma electron density ne and temperature Te with spatial resolution of 3 mm and temporal resolution down to 10 microseconds [5]. This new diagnostic will permit the 2-D characterization of edge and SOL plasma turbulence and is expected to provide additional valuable information on the behaviour of the turbulence during the L-H transition.
The whole set of diagnostics operating simultaneously will allow the characterization of the plasma turbulence evolution from the SOL (GPI and probes) to the plasma gradient (DR) and plasma core (HIBP) regions at the L-H transition.
The whole set of diagnostics operating simultaneously will allow the characterization of the plasma turbulence evolution from the SOL (GPI and probes) to the plasma gradient (DR) and plasma core (HIBP) regions at the L-H transition.

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