16–21 Sept 2018
Giardini Naxos
Europe/Rome timezone

P4.060 Heavy ion beam probe design and operation on the T-10 tokamak

20 Sept 2018, 11:00
2h
Posters Hall - ATA Hotel Naxos Beach Resort (Giardini Naxos)

Posters Hall - ATA Hotel Naxos Beach Resort

Giardini Naxos

Via Recanati, 26 Giardini Naxos, Messina - Sicily (Italy)
P4

Speaker

Alexander Melnikov (Tokamak Division National Research Centre 'Kurchatov Institute')

Description

Paper describes recent advances in Heavy Ion Beam Probing (HIBP), a unique diagnostics to measure the core plasma potential in the T-10 tokamak (R = 1.5 m, a = 0.3 m, B_tor = 1.5 - 2.5 T). Fine focused (< 1 cm) and intense (<130 mkA) Tl+ beams with energy up to E = 330 keV, equipped by advanced control and data acquisition system provides the measurements in the wide density interval n_e = (0.3 - 5)x10^19 m-3 and the wide range of plasma current 100 < I_pl < 330 kA in Ohmic and ECR-heated plasmas. The multichannel parallel plate electrostatic energy analyzer with a high temporal (≥ 1 ms) and energy (DE / E < 5x10-5) resolution simultaneously provides data on the mean value of plasma potential phi and its oscillations (by the beam extra energy), plasma density oscillations (by the beam current) and poloidal magnetic B_pol oscillations (by the beam toroidal shift) in each of 5 sample volumes (SVs). When SVs are poloidally shifted, we can determine the poloidal electric field E_pol=(phi1- phi2)/x, x~1 cm, and the electrostatic turbulent particle flux G_E×B~n_e E_pol /B_tor. Cross-phase of density oscillations allows us to find the poloidal phase velocity of perturbations, or the plasma turbulence rotation, and the poloidal mode number m. Time evolution of local values of plasma parameters and/or fragments of radial profiles (as long as 2-6 cm) can be measured in a single shot at Low Field Side. The whole profile in the range (0.25 < rho < 1) is available shot by shot for B_tor ≤ 2.2 T. High gain (107 V/A) preamplifiers with 500 kHz bandwidth allows us to study broadband turbulence and various types of quasicoherent modes including tearing MHD modes and Geodesic Acoustic Modes.

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