1 JBW-NSTX 9/10/02 Reflectometer Measurements of the Plasma Edge in front of the HHFW antennas John Wilgen, David Swain, Greg Hanson, Phil Ryan Oak Ridge.

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1 JBW-NSTX 9/10/02 Reflectometer Measurements of the Plasma Edge in front of the HHFW antennas John Wilgen, David Swain, Greg Hanson, Phil Ryan Oak Ridge National Laboratory Randy Wilson et al. Princeton Plasma Physics Laboratory NSTX Results Review Meeting PPPL September 9 – 11, 2002

2 JBW-NSTX 9/10/02 HHFW Broadband Microwave Reflectometer Purpose: Measure the edge density profile directly in front of the HHFW antenna, primarily in the scrape-off layer in the gap between the outermost flux surface and the antenna Topics to be covered: –Reflectometer access (thru HHFW antenna) –Measurement capability: Profiles & Fluctuations –Current Status of Data Analysis –Examples of profile data obtained for: H-mode conditions Co-CD in Helium Plasma When outer gap --> 0 –Example of fluctuation data –Summary

3 JBW-NSTX 9/10/02 HHFW Reflectometer Access Located Between 2nd and 3rd Straps of the HHFW antenna Location of ORNL microwave reflectometer launchers used for edge density profile measurements

4 JBW-NSTX 9/10/02 Cylindrical Waveguide Antennas - HHFW Reflectometer 1.5” OD Cylindrical Waveguide Antenna  Antennas are recessed 2.5 cm behind BN tiles (& Faraday screen)  Linear polarized launch couples to X- mode propagation in plasma  Launched polarization externally adjustable to match the pitch angle of the magnetic field (typically 35 degrees off vertical)

5 JBW-NSTX 9/10/02 Operational modes for HHFW Reflectometer Can switch between fluctuation & profile modes remotely, between shots Profile Measuring Mode –Sweep time: 100  sec –Frequency range: 5.74 to 26.8 GHz –X-mode polarization ( sweep starts below cyclotron frequency ) –Density range: 0.05 to 6.0 x cm -3 –Due to low starting density, profile reconstruction normally begins at the leading edge of the HHFW antenna –Analyzed profile data is written to the MDSPlus tree –Data taken in 200 ms window; start time can be changed shot-to-shot Fluctuation Measuring Mode –Fluctuation mode - dwell at 2 fixed frequencies, switching every 5 ms –Standard Dwell Frequencies: 14.2 & 20.4 GHz (but can be changed) –Cutoff densities: 1.2 & 3.5 x cm -3 –Fluctuation data was collected for 32 shots from 6 different days –Analyzed fluctuation data is not written to the tree

6 JBW-NSTX 9/10/02 Status of HHFW Reflectometer Data Analysis Data Analysis - Reconstruction of Edge Density Profiles –Automated profile reconstruction for entire shot –Uses accelerated reconstruction to get “quick and dirty” profiles Caution: Not all of the profiles are credible –Up to 1000 profiles written to the tree for each shot –Also write “averaged” density profiles (9-sweep averages, 1.8 ms) –Analysis code has been run on between-shots basis Status of the Profile Data Analysis –Reflectometer data was collected for > 1200 shots; most are on HHFW run days, but also have other data (4/1-5, 4/15-24, 5/8-24, 6/10-14) –We have some earlier data (2/25-26) that can also be analyzed –All since (4/3/02) have been analyzed & written to the tree –Now have > 1.2 million profiles available (not all are credible) –Next Step: Algorithms for assigning confidence factor to each profile

7 JBW-NSTX 9/10/02 Routines to access the data are available Accessing Edge Density Profile Data from the Tree: Option 1: Obtain data from tree as structure a la TS routines –Use NSTX$:[ornlrefl.source]getreflanalyzeddata.pro –getreflanalyzeddata,shotnumber,results,error_flag results - structure with analyzed data, contains: calshot - LONG - calibration shot used in analysis version - TEXT - version of code used in analysis analysisdata - TEXT - analysis date and time comment - TEXT - comment on analysis, data,.... fvector -FLOAT[fdim] - vector of frequencies for phase output rvector - FLOAT[rdim] - vector of radius for density output tvector - FLOAT[nsweeps] - starting times for each reflectometer sweep density - FLOAT[rdim,nsweeps] - density(rvector,tvector) phase - FLOAT[fdim,nsweeps] - phase(fvector,tvector) quality - FLOAT[fdim,nsweeps] - quality of data (fvector,tvector) avgdensity = FLOAT[rdim,avgdim] - density averaged over 9 sweeps avgtvector = FLOAT[avgdim] - time of average density curves error_flag = 0 if data returned OK, = 1 if not

8 JBW-NSTX 9/10/02 Plotting routine for the reflectometer data is also available Option 2: Use analysis code to view various plots of data –Set default area to NSTX$:[ornlrefl.source] –REFLVIEW will start display program (widget-based, needs X-windows) –Set the shot you want, and (optional) the time you want –You can plot: Multiple plots of groups of 9 successive sweeps of phase(frequency) or density(R) Averaged density profiles for entire shot (200 ms) Big plot of phase and density for a specific time (suitable for framing) Contour plot showing averaged profile evolution vs time Bugs exist – let us know when you fine one!

9 JBW-NSTX 9/10/02 Analysis Code Display: Phase Data & Reconstructed Profiles 162 density profiles for , starting at 80 msec Density (10 19 m -3 ) Each box contains data from 9 consecutive sweeps over 1.8 ms period Heavy black line is the average of the nine sweeps (used in contour plot) Can also plot reflectometer phase data in similar manner Radius (m)

10 JBW-NSTX 9/10/02 Analysis Code Display: Average Density Profiles 63 averaged profiles for shot , starting at 180 ms Starting off with L-mode plasma conditions H-mode transition occurs midway thru this frame All H-mode Following the H-mode transition, > density is depleted in scrape-off layer > fluctuations are greatly reduced > consecutive sweeps yield identical profiles > the reflectometer works!!!

11 JBW-NSTX 9/10/02 Analysis Code: Contour Plot of Average density vs. time Fluctuations are reduced at H-mode transition (≈ 237 ms)! Time (ms) Distance From HHFW Antenna (cm) Shot H-mode transition Profiles tend to follow the outer gap Density Contours (x10 19 m -3 )

12 JBW-NSTX 9/10/02 Credibility of Reflectometer Density Profiles L-mode reflectometer data is often problematic, phase data is often phase scrambled with resulting fringe skips –Nevertheless, averaged profiles are useful in revealing trends in the time evolution of the density profile in the scrapeoff layer Three Cases Where Reflectometer Data is Exceptional –Certain H-mode transitions (like shot ) Density is depleted in the scrape-off layer Fluctuations are greatly reduced As many as 20 consecutive sweeps yield identical profiles –Co-current drive phasing in He plasmas Fluctuations are reduced relative to CCD phasing –Certain shots where the Outer Gap --> 0 (like shot ) Profiles are typically very steep (good for EBW emission) Fluctuations are suppressed

13 JBW-NSTX 9/10/02 Profiles Show Reduced Fluctuations After H-mode Transition 15 consecutive sweeps in each frame (ms)(m)

14 JBW-NSTX 9/10/02 Comparison of Co vs Counter-CD Phasing in Helium Plasma Fluctuations in Averaged Profiles are Clearly Reduced for Co-CD Phasing ! Time (msec) 250 HHFW Counter-CD Phasing HHFW Co-CD Phasing This difference was very consistent throughout the entire day (5/21/02) Shot Shot

15 JBW-NSTX 9/10/02 Density Contours Shift Outward When Gap--> 0 Profiles becomes very steep, fluctuations are suppressed ! Time (ms) Distance From HHFW Antenna (cm) Shot Show Profiles Density Contours (x10 19 m -3 )

16 JBW-NSTX 9/10/02 Fluctuations are Suppressed when Outer Gap ---> 0 25 consecutive profiles in each frame T= ms Gap = 5 cm T= ms Gap = 3 cm T= ms Gap = 1 cm T= ms Gap = 1 cm Shot

17 JBW-NSTX 9/10/02 Initial Results from Fluctuation Measurements Density profile information taken on one shot Fluctuation data taken on adjacent shot (need two shots with same properties) Square-wave modulation of reflectometer freq. Fixed at one of two values, 5 ms at each value Sampling rate = 5 MHz Do FFT of time signal for 4 ms to get frequency spectrum of fluctuations -Can FFT amplitude of refl. signal -Or FFT phase of refl. signal Result gives indication of ñ spectra near the cutoff positions of the two frequencies Shot # t = ms f=20.4 GHz f=14.2 GHz

18 JBW-NSTX 9/10/02 L-H transition causes a remarkable drop in fluctuations in plasma edge, seen in profiles and in fluctuation spectra Near 150 ms L-Mode Near 205 ms H-Mode Density fluctuation spectra L-Mode H-Mode Density scans are 200  s apart L-mode gives higher density in scrape-off layer with large fluctuations when RF is on. H-mode plasmas are more quiescent. Fluctuation frequency spectrum shows remarkable decrease in H-mode Density profiles

19 JBW-NSTX 9/10/02 Summary: HHFW Microwave Reflectometer Reflectometer is fully operational –Does not operate all the time, but can be turned on easily for data acquisition when desired –Takes data for 200-ms window, with adjustable start time –Can measure density profiles or fluctuation spectra –Start time and profile/fluctuation mode can be changed between shots All shots from last run with profile data after period have been analyzed and written to the tree (some analysis for shots before ) –Over 10 6 profiles analyzed and available IDL routine is available for easily retrieving data from tree, OR a simple plotting program is available for looking at the data Have started to look at fluctuation mode data Reflectometer works best when fluctuations are reduced

20 JBW-NSTX 9/10/02 Comparison of Co vs Counter-CD Phasing in Helium Plasma Displaying 9 consecutive profiles at 300 msec R (m) HHFW Counter-CD Phasing HHFW Co-CD Phasing Shot t = 300 msec Shot t = 300 msec Outermost flux surface Outermost flux surface