1. The 2 nd A3 Workshop on ST January 6 th ~8 th, 2014 Hyunyeong Lee, Jong Gab Jo, D. H. Choi, Y. H. An, S. H. Kim, K. J. Chung and Y. S. Hwang NUPLEX, Dept. of Nuclear, Seoul National University, San 56-1, Shilim-dong, Gwanak-gu, Seoul 151-742, Korea brbbebbero@snu.ac.kr Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device Center for Advance Research in Fusion Reactor Engineering Department of Nuclear Engineering Seoul National University

2. 2 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University Contents  Experiment Result - Feasibility of EBW mode conversion - Density profile along the magnetic field - HFSX, LFSX and LFSO injection along the wall position  Summary  Introduction - Motivation and Objectives - Electron Bernstein Wave(EBW) mode conversion  Experiment Setup - Experiment setup, Diagnostics  Pre-ionization experiment in VEST - XB mode conversion in pre-ionization - Comparison between O&X mode injection  Simulation Result(COMSOL) - Comparison between the CMA diagram - The simulation based on diagnosis of the experiment

3. 3 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University Introduction Motivation & Objectives  Electron Cyclotron Heating(ECH) is widely used for various purposes in fusion device that the pre-ionization, local heating and current drive to control the pedestal and the instabilities such as sawtooth, NTM etc.  Especially non-inductive current drive and startup using ECH/CD is essential for Spherical Torus (ST) which has difficulty in start-up due to lack of space for the center stack.  In ST devices which have characteristics of high beta operation and consequent low cutoff density, alternative method using the Electron Bernstein Wave (EBW) which is no cutoff density has been studied.  In most previous works, EBW mode conversion for the wall covered with the chamber has not been studied in detail. The investigation of this EBW mode conversion is essential for the fusion plasma research including ST.

4. 4 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University  Electron Bernstein Wave(EBW) - Electrostatic wave that has no high density cutoff - Electromagnetic wave(ECH) is converted to the electrostatic wave(EBW) only inside the plasma.  Conventional ECH is not suitable to ST due to low cutoff density - EBW : Attractive for heating and CD in ST  EBW mode conversion coefficient : [1]  Budden parameter : Schematic of the EBW assisted plasma current start-up in MAST [2] Maximum mode conversion efficiency C versus L n at NSTX [1] [1] Heinrich Peter Laqua, PPCF, 49, R1-R42, 2007 [2] V.F. Shevchenko et.al., Nuclear Fusion, 50, 022004, 2010 Introduction Electron Bernstein Wave Mode Conversion

5. 5 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University Quartz HFSLFS 875G ` WR284WR284 Pump System 3 Stub Tuner 2.45 GHz Magnetron Hydrogen Injection Quartz Tube Stainless Steel Wall MW Loss Protection Bent Magnetic Field(B T ) LFS Injection HFS Injection Experiment Setup Magnetic Field and Waveguide System  Objective Confirm the effect of ECH & EBW mode conversion  Small cylindrical device with axial magnetic field bent similar to tokamak  Possible to change the direction of microwave(LFS&HFS and O&X mode)  Easily changeable to the magnetic field and MW power  Antenna : open waveguide(WR284) Magnetron

6. 6 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University Experiment Setup Diagnostics – Langmuir Probe  Diagnostics – Radial Langmuir probe Planar type tip(r=1.5mm) Measured in Z=0cm from the center T e (linear fit slope of the log scale V-I curve) n e (the ion saturation current & T e )  Comparison between Interferometer & Probe To confirm the density measurement Assuming that parabolic density profile due to the line integrating density using interferometer The result shows the similar tendency of the density In this result the diagnostics was utilized by this probe. 2 2 3 43 4 1 Axial Probe Radial Probe Interferometer

7. 7 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University Experiment Setup The Wall with X/O Polarized Slit  Objective Confirm the effect of EBW mode conversion on the wall reflection with polarized slit  The wall is possible to change the position along the injection and opposite side.  X/O slit : The wall with slits that reflects the X/O mode wave Formation of polarized wave with specific direction to radiate the electric field of wave perpendicular/parallel on the magnetic field The other wave with different direction will pass through the slit Center Axial Probe Radial Probe 2.45GHz Hydrogen Injection Pump System BtBt E 1 ┴B t perpendicular E1E1 O slit wall ∥ parallel X slit wall

8. 8 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University  In case of HFS injection, the O/X(L) cutoff layer exists in CMA diagram.  O mode cutoff density : ~7.5×10 16 #/m 3 X(L) mode cutoff density : ~1.5×10 17 #/m 3  The result of COMSOL simulation also shows the cutoff layer. Simulation Result CMA Diagram – the cutoff from HFS injection 1 1 Resonance R(X) cutoff O cut off X(L) cut off UHR HFS LFS : Cutoff(reflection) 0 1E16 5E16 3E17 HFSX injection HFSO injection 0 1E16 5E16 3E17 Background Plasma

9. 9 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University  Also in case of LFS injection, the O/X(R) cutoff layer exists in CMA diagram.  O mode cutoff density : 7.5×10 16 #/m 3 X(L) mode cutoff density : ~1.5×10 17 #/m 3 X(R) mode cutoff density : ~2.5×10 16 #/m 3  The result of COMSOL simulation also shows the cutoff density. Simulation Result CMA Diagram – the cutoff from LFS injection 1 1 Resonance R(X) cutoff O cut off X(L) cut off UHR HFS LFS : Cutoff(reflection) 0 1E16 5E16 3E17 LFSX injection LFSO injection 0 1E16 5E16 3E17 Background Plasma

10. 10 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University  In HFS case, the injected microwave does not exceed the cutoff density as same as COMSOL result.  In LFSX case, over dense plasma generates which overcomes the cutoff layer.  In LFSO case, the tendency of the density is similar but weak tendency of the LFSX injection.  The feasibility of EBW mode conversion(XB/OXB) has been shown. Experiment Result The Feasibility of EBW Mode Conversion 1 1 Resonance R(X) cutoff O cut off X(L) cut off UHR HFS LFS : Cutoff(reflection) : XB conversion

11. 11 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University 700W LFSX injection  The density profile is measured for moving the probe shot by shot.  Due to the limit of the probe size, it was impossible to measure near the quartz wall, so the presumption of the density profile is shown in the dashed line.  Higher plasma density with the low magnetic field not in the ECR, but near the UHR(dashed line)  The density is higher with the lower magnetic field Broader and higher density in the UHR(steep density gradient due to the narrow chamber) Feasibility of XB conversion Experiment Result The Density Profile along the Magnetic Field UHR Layer

12. 12 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University  The result of COMSOL simulation is conducted with the experiment result(density).  In case of HFS injection, the density from the experiment does not exceed the X(L) cutoff density.  The microwave from LFSO meet the cutoff layer, but LFSX injection overcomes the cutoff layer.  It might be occurred due to the steep density gradient near the UHR. The feasibility of EBW mode conversion Simulation Result The Feasibility of EBW Mode Conversion 1 1 Resonance R(X) cutoff O cut off X(L) cut off UHR HFS LFS : Cutoff(reflection) : XB conversion HFSO/X injection LFSO/X injection

13. 13 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University Experiment Result HFSX Injection  In case of HFSX injection, the density does not exceed the X(L) cutoff layer.  In all cases of injection side wall, opposite side wall and both wall, the density has the similar tendency – single pass absorption. 1 1 Resonance R(X) cutoff O cut off X(L) cut off UHR HFSX ECR

14. 14 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University Experiment Result LFSX Injection – XB Mode Conversion  In case of LFSX injection  XB mode conversion might be occurred directly. -Steep density gradient near UHR.  The wall positioned in the opposite side of the wave injection affects to the multiple reflection – multi pass absorption. 1 1 Resonance R(X) cutoff O cut off X(L) cut off UHR LFS LFSX ECR

15. 15 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University Experiment Result LFSX Injection with Polarized Wall  In case of LFSX injection  XB mode conversion and multi pass power absorption due to the wall reflection.  Oslit wall has the similar tendency with the none wall case – no effect of the reflected O wave  Xslit wall – similar to the full wall(XB conversion) 1 1 Resonance R(X) cutoff O cut off X(L) cut off UHR LFS LFSX ECR

16. 16 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University Experiment Result LFSO Injection – OXB Mode Conversion  Opposite side & both wall - The feasibility of OXB mode conversion - OX conversion : O cutoff & wall reflection - Multi pass absorption due to the opposite wall  Injection side & None wall - No overcomes the X(L) cutoff density  Further research is required to understand the wave movement after MW meets the O cutoff layer. 1 1 Resonance R(X) cutoff O cut off X(L) cut off UHR LFS LFSO ECR

17. 17 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University Experiment Result LFSO Injection with Polarized Slit 1 1 Resonance R(X) cutoff O cut off X(L) cut off UHR LFS LFSO ECR  In case of LFSO injection  Xslit & Full wall - The feasibility of OXB mode conversion - the similar density tendency  Oslit & None wall - No existence of the reflected X wave - XB conversion does not occurs.

18. 18 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University  Based on the linear device experiment, the pre-ionization experiment in VEST is conducted with only TF field.  Initial breakdown occurs in ECR with low ECH power, and then UHR moves outward increasing ECH power that means the electron density buildup.  The density profile in VEST shows that the electron density peak exists near the UHR which has the steep density gradient and it means the feasibility of XB mode conversion. R cutoff UHR Pre-ionization experiment in VEST XB Mode Conversion in Pre-ionization LFSX Injection

19. 19 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University  The density and temperature of LFS O mode injection is similar to LFS X.  Reflected MW diagnostics shows OX and no XO mode conversion. Only X-mode O-mode X-mode Pre-ionization experiment in VEST Comparison Between O & X Mode Injection

20. 20 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University Summary  To confirm the effect of ECH and EBW mode conversion on the wall reflection, the experiment is prepared.  With the simulation named as COMSOL based on the experiment result, the feasibility of EBW mode conversion near the steep density gradient is found.  In LFS injection, the feasibility of XB & OXB mode conversion is confirmed and higher plasma density with the low magnetic field not in the ECR, but near the UHR as same as the simulation result.  In case of LFSX injection, XB mode conversion is occurred directly due to the steep density gradient and multi pass power absorption with opposite side wall and in case of LFSO, OXB mode conversion may occur in the UHR and O cutoff layer.  The pre-ionization experiment in VEST is conducted and the result also shows the feasibility of XB and OXB mode conversion near the UHR.

21. Back up

22. 22 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University LFSX injection Leakage MW power monitoring Preliminary ECH Experiment Result(3)  X_Slit/O_Slit : The wall with X/O mode MW radiation when reflection is occurred in the wall  Density : Wall > X_Slit > O_Slit > No_Wall  Over dense plasma and X mode polarized wave effect shows the evidence of the EBW mode conversion(XB)  The result of monitoring the leakage MW No_wall > O_Slit > X_slit

23. 23 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University Future Work  7.9GHz MW source installation Inboard startup using trapped particle configuration – the peak density of the pre- ionization plasma near the inboard side. Study for the ECH harmonic efficiency  EBW mode conversion experiment Closed flux surface formation in trapped particle configuration – the possibility of the steep density gradient to make EBW mode conversion In conventional startup, the steep density gradient will be made using local limiter in front of the waveguide launcher  Non-inductive current drive experiment In steady state plasma, the possibility of the ECCD/EBCD will be investigated. 00.20.40.60.81 -1.5 -0.5 0 0.5 1 1.5 Coil Geometry R (m) Z (m) Various EC Resonance Layer in VEST O-mode cutoff 7.5GHz FHM 2.45GHz FHM 7.5GHz THM 2.45GHz UHR 7.5GHz SHM

24. 24 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University 1e16 LFSX 5e16 LFSX injectionLFSO injectionExperiment SetupLFSX injection

25. 25 /20 LHY_A3_JAN07 Study on the effect of ECH/EBW mode conversion on the wall reflection in linear device on January 07 th 2014, at Tsinghua University