بسمه تعالی

1. بسمه تعالی Fast Imaging of turbulent plasmas in the GyM device D.Iraji, D.Ricci, G.Granucci, S.Garavaglia, A.Cremona IFP-CNR-Milan 7th Workshop on Fusion Data Processing Validation and Analysis Frascati-March 2012

2. Outlines Motivations Fast imaging of GyM plasmas Reconstruction of the emissivity profiles Fluctuations profiles CAS for detection and visualization of plasma structures (a comparison with probe measurements) Summary

3. Motivations A non perturbative approach is fast visible imaging of plasma turbulence. An ultimate goal of plasma imaging is extracting plasma characteristics as much as possible from images. We need to reconstruct the plasma emissivity profiles in order to analyze plasma structures.

4. Fast Visible Imaging system Camera Characteristics: Photron ultima APX-RS Full, 1024 by 1024 pixel resolution, up to 3,000 fps, 10-bit monochrome CMOS sensor with pixels in dimension of 17×17µm Top recording speed is 250,000 fps Image memory can be expanded to facilitate 6 second recordings at 1,000 fps And 4.2 seconds at 250,000 fps. Capability of synchronization with the Other diagnostics such as probes (error < 100nsec)

5. Fast visible plasma imaging CSDX, G.Antar TORPEX D.Iraji NSTX, S.Zweben Camera + GP Camera +Image Intensifier • ELMs • Blobs/Filaments • Modes

6. High Speed gated Image Intensifier Hamamatsu C10880-03 Max. gain 10000 Spectral response 185-900 nm Gating 10ns-10ms Repetition rate 200kHz Resolution 38 lp/mm

7. GyM Electron density profile Electron Temperature profile Modular device in which the magnetic field configuration can be easily modified. # of Coils 10 Max current 1000 A Max magnetic field 0.13 T Cooling water rate 22 l/min Power supply (d.c.) 1000A/50V Vacuum chamber (m): Length 2.11 Diameter 0.25 B average ~ 80 mT Langmuir probe 2.45 GHz source Hot filament source

8. Line integrated images (raw data)H2, RF power: 1500 W I(t): Camera image frame at time (t) 75000 fps, 4 us exposure time

9. Reconstruction of the emissivity profile Z r B and g >=0 1cm×1cm I =T g Solving least square using SVD approach N M MN

10. Reconstruction • Calculation of the Transformer Matrix T : • Triangulation of reference images to find the camera pixels positions related to the machine coordinates (P) • Length of the intersection of LOS corresponding to each camera pixel (i) with plasma pixel (j) is Tij I ref P T Triangulation LOS g Reconstruction NR < 5% I exp

11. Reconstructed emissivity profilesH2, RF power: 1500 W g(t): Reconstructed emissivity profile at time (t) 75000 fps, 4 us exposure time Each frame Cnsums ~ 2 s of Four 2.4 GHz CPUs, NR < 5%

12. Fluctuations Fluctuations level PSD of the MFL signal Maximum fluctuations level (MFL)

13. Fluctuations Z-Scan of PSD r-Scan of PSD Z r B

14. Conditional Average Sampling (CAS) E×B rotation and Te Probe measurement -1 2 L = FWHM V E×B ~ 1km/s, B~80 mT: E~80 V/m L ~5.5cm, Te~ E L ~ 4.4 eV -1 -1

15. E×B rotation and B . × E E B B E×B is responsible for the rotation of the plasma column

16. Summary The intensified fast camera is able to image plasma with spatial resolution of 2cm and temporal resolution of 4µs. .Plasma emissivity profiles are reconstructed using pixel methode and singular value decomposition approach. Fourier analysis of the reconstructed images show presence of a distinct mode at ~4 kHz which is radially extended between -3cm<r<2 cm and vertically located at the bottom. CASed images show rotation of the structures associated with the mode due to E×B drift.

17. Outlooks Structural analysis of the reconstructed emissivity profiles to estimate plasma transport. The establishment of comparisons between the experimental plasma transport related to the plasma structures with theoretical predictions and confirmation using probe data.

18. Thank you

19. Extra slides

20. Tomographic reconstruction of the plasma emissivity profile in TORPEX

21. Tomographic reconstruction of the plasma emissivity profile in TORPEX Before reconstruction After reconstruction