TJ-II:Radiation asymmetries and potential variations: Difference between revisions

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* The time evolution of the plasma emissivity along the available lines of sight of the tomography camera systems.
* The time evolution of the plasma emissivity along the available lines of sight of the tomography camera systems.
* The time evolution of the plasma floating potential at the outer core region (<math>r/a\sim 0.9</math>).
* The radial electric field profile using Doppler reflectometry (DR), measured on the right and left side (respect to the normal incidence angle) of the DR measurement plane.
* The time evolution of the line-averaged density <math>\left<n_e(t)\right></math> with interferometry.
* The time evolution of the line-averaged density <math>\left<n_e(t)\right></math> with interferometry.
* The radial profiles of electron density <math>n_{e}(r, t_0)</math> and temperature at one time instant <math>t_0</math> using Thomson Scattering (TS).
* The radial profiles of electron density <math>n_{e}(r, t_0)</math> and temperature at one time instant <math>t_0</math> using Thomson Scattering (TS).
* The time evolution of the electron temperature profile <math>T_{e}(r,t)</math> with Electron Cyclotron Emission (ECE), when available, calibrated with TS.
* The time evolution of the electron temperature profile <math>T_{e}(r,t)</math> with Electron Cyclotron Emission (ECE), when available, calibrated with TS.
* When possible the time evolution of the main ion temperature profile <math>T_{i}(r,t)</math> with the CNPA are four positions that are representative of the inner and mid-core and mid- and far edge.
* When possible the time evolution of the main ion temperature profile <math>T_{i}(r,t)</math> with the CNPA are four positions that are representative of the inner and mid-core and mid- and far edge.
* The time evolution of the radial electric field at the mid-outer resion (<math>r/a\sim 0.7-0.8</math>) with reflectometry.


== Preferred dates and degree of flexibility ==
== Preferred dates and degree of flexibility ==
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