Measurements of Mode Converted ICRF Waves with Phase Contrast Imaging in Alcator C-Mod
|
|
- John Arnold
- 5 years ago
- Views:
Transcription
1 Measurements of Mode Converted ICRF Waves with Phase Contrast Imaging in Alcator C-Mod N. Tsujii, M. Porkolab, E.M. Edlund, L. Lin, Y. Lin, J.C. Wright, S.J. Wukitch MIT Plasma Science and Fusion Center *Work supported by US DOE under DE-FG02-94-ER54235 and DE-FC02-99-ER54512
2 Introduction The Phase Contrast Imaging(PCI) system in Alcator C-Mod is used to measure MHD modes, turbulence and RF waves The system was absolutely calibrated for the heterodyne measurement of the RF waves Mode converted ion cyclotron waves(icw) were observed by PCI around the ion-ion hybrid layer in a D- 3 He plasma The PCI measurements were compared with the full wave simulation code TORIC
3 Wave Propagation in an Axisymmetric Plasma The local dispersion relation takes the form, : wavevector parallel to the magnetic field : wavevector perpendicular to the magnetic field The toroidal mode number n is conserved, : wavevector in the toroidal direction In terms of wavevector in the poloidal direction,
4 3 He-D Mode Conversion Scenario(1) Mode conversion from fast magnetosonic wave to hot plasma waves occurs around the ion-ion hybrid layer The mode conversion occurs around a narrow region, and the inhomogeneity can be considered 1D, mainly from the variation of the toroidal magnetic field The local dispersion relation can be solved in terms of wavevector in the direction of inhomogeneity, k R
5 3 He-D Mode Conversion Scenario(2) k R [cm -1 ] Ion species concentration, D 78%, 3 He 9%, H 4% I p = 0.83 MA, R 0 = m, B 0 = 4.9 T, n e0 = 1.5 * m -3, T e0 = 2.1 kev Dispersion curves at and above the midplane, for n = IBW MC R[m] z = 0.01 m FW 3 He Fund. k R [cm -1 ] MC ICW 3 He Fund R[m] z = 0.17 m
6 TORIC simulation(1) TORIC Full wave solver in axisymmetric geometry Electric field solution (n = 8, for MW of power absorbed) ICW IBW FW
7 TORIC simulation(2) Power deposition profile (n = 8, for MW of power absorbed) Power absorbed by 3 He at fundamental cyclotron resonance Power absorbed by electrons
8 Phase Contrast Imaging Laser beam propagating through the plasma acquires phase delay proportional to the line-integrated electron density : PCI laser wavelength By introducing π/2 phase delay to the unscattered component of the beam, phase variation is converted to beam intensity variation
9 PCI System in C-Mod(1) The laser beam is focused on the phase plate with an off-axis parabolic mirror π/2 phase delay is introduced by a reflective phase plate with a λ/8 groove at the center λ/8 groove phase plate Line integrated density fluctuation is imaged onto the 32 channel photodiode detector array
10 PCI System in C-Mod(2) Laser: 60 W CO 2 CW λ = 10.6 μm TEM 00 Wave number: k R = cm -1 Frequency: 2 khz 5 MHz Heterodyne frequency: MHz Localization: R = cm
11 Absolute Calibration Sound wave pattern of the calibration source was measured with a calibrated microphone The source is used as a reference for calibrating PCI density fluctuation level 15 khz loudspeaker
12 Optical Heterodyne System Laser beam amplitude is modulated with RF frequency using acousto-optic shifters The mixing of the RF fluctuation with this modulation reduces the frequency to ~1 MHz No need for fast detector array Less RF pick up compared to electronic heterodyne
13 Heterodyned RF Signal on PCI RF frequency 50 MHz PCI beam intensity modulation MHz signal at 1.79 MHz ch22 signal (R = 0.66[m]) Coherent fluctuation is observed at the expected frequency, which shows the excitation of mode converted ion cyclotron wave Strong flow drive is observed in this shot [Y. Lin. BI ] RF power[mw] time[s]
14 Observed RF Fluctuation Profile Density fluctuation profile at 1790 khz Radial structure Wavenumber structure
15 Simulation of PCI Signal with Particle number conservation, TORIC Major contributions to the electron velocity are, where Z is the Fried-Conte plasma dispersion function
16 P abs [MW/kA 2 ] Toroidal Mode Number n Dependence Phasing +90 Total power coupled 1 MW Simulated wave amplitude is normalized to coupled power real wave amplitude Power absorption efficiency P abs [MW] Antenna spectrum antenna current x n n Power absorbed
17 Comparison of TORIC simulation with PCI measurement density fluctuation[(10 16 m -2 ) 2 ] R[m] : Line-integrated density fluctuation from TORIC * : PCI measurement The simulation and experiment are within factors of 2-3 density fluctuation[(10 16 m -2 ) 2 /cm -1 ] 3.5 x k R [cm -1 ]
18 Future Work Expected PCI signal for different 3 He concentrations density fluctuation[(10 16 m -2 ) 2 ] % 20 % 30 % R[m] Future experimental plans include scanning the minority concentration and comparing the experimental measurements with these predictions
19 Summary PCI signal in the mode conversion experiment has been simulated with TORIC The simulation and the experiment are within factors of 2-3 Comparisons will be made for different minority concentrations For a more detailed comparison, PCI channel response has to be calibrated more accurately Simulation of PCI signal with AORSA is planned
Measurement of Mode Converted ICRF Waves with Phase Contrast Imaging and Comparison with Full-wave Simulations on Alcator C-Mod
Measurement of Mode Converted ICRF Waves with Phase Contrast Imaging and Comparison with Full-wave Simulations on Alcator C-Mod N. Tsujii 1, M. Porkolab 1, P.T. Bonoli 1, Y. Lin 1, J.C. Wright 1, S.J.
More informationICRF Mode Conversion Flow Drive Studies with Improved Wave Measurement by Phase Contrast Imaging
57 th APS-DPP meeting, Nov. 2015, Savannah, GA, USA ICRF Mode Conversion Flow Drive Studies with Improved Wave Measurement by Phase Contrast Imaging Yijun Lin, E. Edlund, P. Ennever, A.E. Hubbard, M. Porkolab,
More informationICRF mode conversion in three-ion species heating experiment and in flow drive experiment on the Alcator C- Mod tokamak
ICRF mode conversion in three-ion species heating experiment and in flow drive experiment on the Alcator C- Mod tokamak The MIT Faculty has made this article openly available. Please share how this access
More informationICRF Mode Conversion Physics in Alcator C-Mod: Experimental Measurements and Modeling
Work supported by the US DOE ICRF Mode Conversion Physics in Alcator C-Mod: Experimental Measurements and Modeling S.J. Wukitch Presented at the 46th Annual Meeting of the Division of Plasma Physics November
More informationDetection of Lower Hybrid Waves on Alcator C-Mod with Phase Contrast Imaging Using Electro-Optic Modulators
Detection of Lower Hybrid Waves on Alcator C-Mod with Phase Contrast Imaging Using Electro-Optic Modulators K. Arai, M. Porkolab, N. Tsujii, P. Koert, R. Parker, P. Woskov, S. Wukitch MIT Plasma Science
More informationRF Physics: Status and Plans
RF Physics: Status and Plans Program Advisory Committee meeting February 6-7, 2002 S. J. Wukitch Outline: 1. Overview of RF Physics issues 2. Review of antenna performance and near term modifications.
More informationC-Mod ICRF Research Program
C-Mod ICRF Research Program C-Mod Ideas Forum December 2-6, 2004 MIT PSFC Presented by Steve Wukitch Outline: 1. Overview of ICRF program 2. Summary of MP s and proposals ICRF Highlights Antenna Performance
More informationICRF Mode Conversion Flow Drive on Alcator C-Mod and Projections to Other Tokamaks
ICRF Mode Conversion Flow Drive on Alcator C-Mod and Projections to Other Tokamaks The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters.
More informationUpper limit on turbulent electron temperature fluctuations on Alcator C-Mod APS DPP Meeting Albuquerque 2003
Upper limit on turbulent electron temperature fluctuations on Alcator C-Mod APS DPP Meeting Albuquerque 2003 Christopher Watts, Y. In (U. Idaho), A.E. Hubbard (MIT PSFC) R. Gandy (U. Southern Mississippi),
More informationDetection and application of Doppler and motional Stark features in the DNB emission spectrum in the high magnetic field of the Alcator C-Mod tokamak
Detection and application of Doppler and motional Stark features in the DNB emission spectrum in the high magnetic field of the Alcator C-Mod tokamak I. O. Bespamyatnov a, W. L. Rowan a, K. T. Liao a,
More informationDiagnostic development to measure parallel wavenumber of lower hybrid waves on Alcator C-Mod
Diagnostic development to measure parallel wavenumber of lower hybrid waves on Alcator C-Mod S. G. Baek, T. Shinya*, G. M. Wallace, S. Shiraiwa, R. R. Parker, Y. Takase*, D. Brunner MIT Plasma Science
More informationC-Mod ICRF Program. Alcator C-Mod PAC Meeting January 25-27, 2006 MIT Cambridge MA. Presented by S.J. Wukitch
C-Mod ICRF Program Alcator C-Mod PAC Meeting January 5-7, 006 MIT Cambridge MA Presented by S.J. Wukitch Outline: 1. Overview of ICRF program. Antenna performance evaluation and coupling 3. Mode conversion
More informationHelicon Wave Current Drive in KSTAR Plasmas
Daejeon Helicon Wave Current Drive in KSTAR Plasmas S. J. Wanga, H. J. Kima, Jeehyun Kima, V. Vdovinb, B. H. Parka, H. H. Wic, S. H. Kimd, and J. G. Kwaka anational Fusion Research Institute, Daejeon,
More informationAdvanced Tokamak Program and Lower Hybrid Experiment. Ron Parker MIT Plasma Science and Fusion Center
Advanced Tokamak Program and Lower Hybrid Experiment Ron Parker MIT Plasma Science and Fusion Center Alcator C-Mod Program Advisory Meeting 23-24 February 2004 Main Goals of the Alcator C-Mod AT Program
More informationStructure and Characteristics of the Quasi-Coherent Mode
Structure and Characteristics of the Quasi-Coherent Mode in EDA H-mode Plasmas I. Cziegler, J. L. Terry, L. Lin, M. Porkolab,J. A. Snipes MIT Plasma Science and Fusion Center American Physical Society
More informationIon Heating Arising from the Damping of Short Wavelength Fluctuations at the Edge of a Helicon Plasma Source
Ion Heating Arising from the Damping of Short Wavelength Fluctuations at the Edge of a Helicon Plasma Source Division of Plasma Physics American Physical Society October 2012 Providence, RI Earl Scime,
More informationEvaluation of a Field Aligned ICRF Antenna in Alcator C-Mod
Evaluation of a Field Aligned ICRF Antenna in Alcator C-Mod 24th IAEA Fusion Energy Conference San Diego, USA October 8-13 2012 S.J. Wukitch, D. Brunner, M.L. Garrett, B. Labombard, C. Lau, Y. Lin, B.
More informationInvestigation of RF-enhanced Plasma Potentials on Alcator C-Mod
PSFC/JA-13-3 Investigation of RF-enhanced Plasma Potentials on Alcator C-Mod Ochoukov, R., Whyte, D.G., Brunner, D., Cziegler *, I., LaBombard, B., Lipschultz, B., Myra **, J., Terry, J., Wukitch, S *
More informationSOL Reflectometer for Alcator C-Mod
Alcator C-Mod SOL Reflectometer for Alcator C-Mod C. Lau 1 G. Hanson 2, J. B. Wilgen 2, Y. Lin 1, G. Wallace 1, and S. J. Wukitch 1 1 MIT Plasma Science and Fusion Center, Cambridge, MA 02139 2 Oak Ridge
More informationWhistlers, Helicons, Lower Hybrid Waves: the Physics of RF Wave Absorption for Current Drive Without Cyclotron Resonances
Whistlers, Helicons, Lower Hybrid Waves: the Physics of RF Wave Absorption for Current Drive Without Cyclotron Resonances R.I. Pinsker General Atomics 100 50 Presented at the 56 th Annual Division of Plasma
More informationStudy of Ion Cyclotron Emissions due to DD Fusion Product Ions on JT-60U
1 Study of Ion Cyclotron Emissions due to DD Fusion Product Ions on JT-6U M. Ichimura 1), M. Katano 1), Y. Yamaguchi 1), S. Sato 1), Y. Motegi 1), H. Muro 1), T. Ouchi 1), S. Moriyama 2), M. Ishikawa 2),
More informationField Aligned ICRF Antenna Design for EAST *
Field Aligned ICRF Antenna Design for EAST * S.J. Wukitch 1, Y. Lin 1, C. Qin 2, X. Zhang 2, W. Beck 1, P. Koert 1, and L. Zhou 1 1) MIT Plasma Science and Fusion Center, Cambridge, MA USA. 2) Institute
More informationField-Aligned ICRF Antenna Characterization and Performance in Alcator C-Mod*
Field-Aligned ICRF Antenna Characterization and Performance in Alcator C-Mod* 54th APS DPP Annual Meeting Providence, RI USA October 9-Nov, 0 S.J. Wukitch, D. Brunner, P. Ennever, M.L. Garrett, A. Hubbard,
More informationLower Hybrid. Ron Parker Alcator C-Mod PAC Meeting January January 2006 Alcator C-Mod PAC Meeting 1
Lower Hybrid Ron Parker Alcator C-Mod PAC Meeting 25-27 January 2006 25-27 January 2006 Alcator C-Mod PAC Meeting 1 Goal of Lower Hybrid Current Drive Experiments Use Lower Hybrid Current Drive to supplement
More informationICRF Physics in KSTAR Steady State
ICRF Physics in KSTAR Steady State Operation (focused on the base line operation) Oct. 24, 2005 Jong-gu Kwak on the behalf of KSTAR ICRF TEAM Korea Atomic Energy Research Institute Contents Roles of ICRF
More informationOverview of ICRF Experiments in Alcator C-Mod
Overview of ICRF Experiments in Alcator C-Mod 50 th APS Plasma Physics Conference November 17-1, 008 S.J. Wukitch, Y.Lin, P.T. Bonoli, A. Hubbard, B. LaBombard, B. Lipschultz, M. Porkolab, J.E. Rice, D.
More informationDevelopment of C-Mod FIR Polarimeter*
Development of C-Mod FIR Polarimeter* P.XU, J.H.IRBY, J.BOSCO, A.KANOJIA, R.LECCACORVI, E.MARMAR, P.MICHAEL, R.MURRAY, R.VIEIRA, S.WOLFE (MIT) D.L.BROWER, W.X.DING (UCLA) D.K.MANSFIELD (PPPL) *Supported
More informationNovel Reactor Relevant RF Actuator Schemes for the Lower Hybrid and the Ion Cyclotron Range of Frequencies
Novel Reactor Relevant RF Actuator Schemes for the Lower Hybrid and the Ion Cyclotron Range of Frequencies P. T. Bonoli, S. G. Baek, B. LaBombard, Y. Lin, T. Palmer, R. R. Parker, M. Porkolab, S. Shiraiwa,
More informationInitial Active MHD Spectroscopy Experiments Exciting Stable Alfvén Eigenmodes in Alcator C-Mod
PSFC/JA-03-26 Initial Active MHD Spectroscopy Experiments Exciting Stable Alfvén Eigenmodes in Alcator C-Mod J.A. Snipes, D. Schmittdiel, A. Fasoli*, R.S. Granetz, R.R. Parker 16 December 2003 Plasma Science
More informationImproved core transport triggered by off-axis ECRH switch-off on the HL-2A tokamak
Improved core transport triggered by off-axis switch-off on the HL-2A tokamak Z. B. Shi, Y. Liu, H. J. Sun, Y. B. Dong, X. T. Ding, A. P. Sun, Y. G. Li, Z. W. Xia, W. Li, W.W. Xiao, Y. Zhou, J. Zhou, J.
More informationHelicon mode formation and rf power deposition in a helicon source
Helicon mode formation and rf power deposition in a helicon source Michael Krämer & Kari Niemi Institut für Experimentalphysik II, Ruhr-Universität D-4478 Bochum, Germany Helicon Mini-Conference APS-DPP,
More informationOverview of ICRF Experiments on Alcator C-Mod*
49 th annual APS-DPP meeting, Orlando, FL, Nov. 2007 Overview of ICRF Experiments on Alcator C-Mod* Y. Lin, S. J. Wukitch, W. Beck, A. Binus, P. Koert, A. Parisot, M. Reinke and the Alcator C-Mod team
More informationImportance of edge physics in optimizing ICRF performance
Importance of edge physics in optimizing ICRF performance D. A. D'Ippolito and J. R. Myra Research Corp., Boulder, CO Acknowledgements D. A. Russell, M. D. Carter, RF SciDAC Team Presented at the ECC Workshop
More informationVariation of N and its Effect on Fast Wave Electron Heating on LHD
J. Plasma Fusion Res. SERIES, Vol. 6 (004) 6 (004) 64 646 000 000 Variation of N and its Effect on Fast Wave Electron Heating on LHD TAKEUCHI Norio, SEKI Tetsuo 1, TORII Yuki, SAITO Kenji 1, WATARI Tetsuo
More informationInvestigation of ion toroidal rotation induced by Lower Hybrid waves in Alcator C-Mod * using integrated numerical codes
Investigation of ion toroidal rotation induced by Lower Hybrid waves in Alcator C-Mod * using integrated numerical codes J.P. Lee 1, J.C. Wright 1, P.T. Bonoli 1, R.R. Parker 1, P.J. Catto 1, Y. Podpaly
More informationAbstract. G.D. Garstka 47 th APS-DPP Denver October 27, Pegasus Toroidal Experiment University of Wisconsin-Madison
Abstract The PEGASUS Toroidal Experiment provides an attractive opportunity for investigating the physics and implementation of electron Bernstein wave (EBW) heating and current drive in an overdense ST
More informationKinetic Ray Tracing in Toroidal Geometry with Application to Mode-Converted Ion-Bernstein Waves. Ram, A. K.; Bers, A. August 1989
PFC/JA-89-37 Kinetic Ray Tracing in Toroidal Geometry with Application to Mode-Converted Ion-Bernstein Waves Ram, A. K.; Bers, A. August 1989 Plasma Fusion Center Massachusetts Institute of Technology
More informationStatus of C-Mod Diagnostics. Presented by Jim Irby For the C-Mod Group
Status of C-Mod Diagnostics Presented by Jim Irby For the C-Mod Group Outline Diagnostic Availability Selected Diagnostics PAC 2009 PAC 2009 Diagnostic Availability UCLA Polarimetry Dual FIR lasers operational
More informationDevelopment of the frequency scanning reflectometry for the registration of Alfvén wave resonances in the TCABR tokamak
Development of the frequency scanning reflectometry for the registration of Alfvén wave resonances in the TCABR tokamak L. F. Ruchko, R. M. O. Galvão, A. G. Elfimov, J. I. Elizondo, and E. Sanada Instituto
More informationPedestal Turbulence Dynamics in ELMing and ELM-free H-mode Plasmas
Pedestal Turbulence Dynamics in ELMing and ELM-free H-mode Plasmas Z. Yan1, G.R. McKee1, R.J. Groebner2, P.B. Snyder2, T.H. Osborne2, M.N.A. Beurskens3, K.H. Burrell2, T.E. Evans2, R.A. Moyer4, H. Reimerdes5
More informationMicrowave Imaging in the Large Helical Device
Microwave Imaging in the Large Helical Device T. Yoshinaga 1), D. Kuwahara 2), K. Akaki 3), Z.B. Shi 4), H. Tsuchiya 1), S. Yamaguchi 5), Y. Kogi 6), S. Tsuji-Iio 2), Y. Nagayama 1), A. Mase 3), H. Hojo
More informationResults from Alcator C-Mod ICRF Experiments
Results from Alcator C-Mod ICRF Experiments 18 th Topical Conference on RF Power in Plasmas June 4-7, 009 S.J. Wukitch, Y.Lin and the Alcator C-Mod Team Key Results: 1. First demonstration of efficient
More informationParticle Simulation of Lower Hybrid Waves in Tokamak Plasmas
Particle Simulation of Lower Hybrid Waves in Tokamak Plasmas J. Bao 1, 2, Z. Lin 2, A. Kuley 2, Z. X. Wang 2 and Z. X. Lu 3, 4 1 Fusion Simulation Center and State Key Laboratory of Nuclear Physics and
More informationECRF Heating on CS Reactors
ECRF Heating on CS Reactors T.K. Mau UC-San Diego With input from L.P. Ku (PPPL), J.F. Lyon (ORNL), X.R. Wang (UCSD) ARIES Project Meeting May 6-7, 2003 Livermore, California 1 OUTLINE ECH scenario studies
More informationAlcator C-Mod ICRF Research Program
Alcator C-Mod ICRF Research Program MIT Plasma Science and Fusion Center February 4-6, 2009 S.J. Wukitch Overall Themes 1. Develop ICRF heating and flow/current drive actuators for optimization i i of
More informationEffect of ICRF Mode Conversion at the Ion-Ion Hybrid Resonance on Plasma Confinement in JET
EFDA JET CP()- A.Lyssoivan, M.J.Mantsinen, D.Van Eester, R.Koch, A.Salmi, J.-M.Noterdaeme, I.Monakhov and JET EFDA Contributors Effect of ICRF Mode Conversion at the Ion-Ion Hybrid Resonance on Plasma
More informationTheoretical Studies of Toroidal Rotation Induced by Lower Hybrid Wave Fields
Theoretical Studies of Toroidal Rotation Induced by Lower Hybrid Wave Fields RF SciDAC meeting 2010(PPPL) Jungpyo(J.P.) Lee -MIT John Wright MIT Peter Catto MIT Paul Bonoli MIT Felix Parra Oxford Christ
More informationStructural Analysis of High-field-Side RF antennas during a disruption on the Advanced Divertor experiment (ADX)
Structural Analysis of High-field-Side RF antennas during a disruption on the Advanced Divertor experiment (ADX) J. Doody, B. LaBombard, R. Leccacorvi, S. Shiraiwa, R. Vieira, G.M. Wallace, S.J. Wukitch,
More informationR. J. Jones College of Optical Sciences OPTI 511L Fall 2017
R. J. Jones College of Optical Sciences OPTI 511L Fall 2017 Active Modelocking of a Helium-Neon Laser The generation of short optical pulses is important for a wide variety of applications, from time-resolved
More informationParticle Simulation of Radio Frequency Waves in Fusion Plasmas
1 TH/P2-10 Particle Simulation of Radio Frequency Waves in Fusion Plasmas Animesh Kuley, 1 Jian Bao, 2,1 Zhixuan Wang, 1 Zhihong Lin, 1 Zhixin Lu, 3 and Frank Wessel 4 1 Department of Physics and Astronomy,
More informationInitial Results from the C-Mod Prototype Polarimeter/Interferometer
Initial Results from the C-Mod Prototype Polarimeter/Interferometer K. R. Smith, J. Irby, R. Leccacorvi, E. Marmar, R. Murray, R. Vieira October 24-28, 2005 APS-DPP Conference 1 Abstract An FIR interferometer-polarimeter
More informationCRITICAL PROBLEMS IN PLASMA HEATING/ CD IN LARGE FUSION DEVICES AND ITER
CRITICAL PROBLEMS IN PLASMA HEATING/ CD IN LARGE FUSION DEVICES AND ITER Vdovin V.L. RRC Kurchatov Institute Nuclear Fusion Institute Moscow, Russia 22nd IAEA Fusion Energy Conference 13-18 October 2008
More informationINITIAL RESULTS FROM THE MULTI-MEGAWATT 110 GHz ECH SYSTEM FOR THE DIII D TOKAMAK
GA A22576 INITIAL RESULTS FROM THE MULTI-MEGAWATT 110 GHz ECH SYSTEM by R.W. CALLIS, J. LOHR, R.C. O NEILL, D. PONCE, M.E. AUSTIN, T.C. LUCE, and R. PRATER APRIL 1997 This report was prepared as an account
More informationStatus of the rf Current Drive Systems on MST
Status of the rf Current Drive Systems on MST John A. Goetz for A. Almagri, J.K. Anderson, D.R. Burke, M.M. Clark, W.A. Cox, C.B. Forest, R. Ganch, M.C. Kaufman, J.G. Kulpin, P. Nonn, R. O Connell, S.P.
More informationHigh Temporal Resolution Polarimetry on the MST Reversed Field Pinch
High Temporal Resolution Polarimetry on the MST Reversed Field Pinch W.X. Ding, S.D. Terry, D.L. Brower Electrical Engineering Department University of California, Los Angeles J.K. Anderson, C.B. Forest,
More informationLaser Beam Analysis Using Image Processing
Journal of Computer Science 2 (): 09-3, 2006 ISSN 549-3636 Science Publications, 2006 Laser Beam Analysis Using Image Processing Yas A. Alsultanny Computer Science Department, Amman Arab University for
More informationResonance Cones in Magnetized Plasma
Resonance Cones in Magnetized Plasma C. Riccardi, M. Salierno, P. Cantu, M. Fontanesi, Th. Pierre To cite this version: C. Riccardi, M. Salierno, P. Cantu, M. Fontanesi, Th. Pierre. Resonance Cones in
More informationSimulation Studies of Field-Reversed Configurations with Rotating Magnetic Field Current Drive
Simulation Studies of Field-Reversed Configurations with Rotating Magnetic Field Current Drive E. V. Belova 1), R. C. Davidson 1), 1) Princeton University Plasma Physics Laboratory, Princeton NJ, USA E-mail:ebelova@pppl.gov
More informationElectromagnetic Field Simulation for ICRF Antenna and Comparison with Experimental Results in LHD
Electromagnetic Field Simulation for ICRF Antenna and Comparison with Experimental Results in LHD Takashi MUTOH, Hiroshi KASAHARA, Tetsuo SEKI, Kenji SAITO, Ryuhei KUMAZAWA, Fujio SHIMPO and Goro NOMURA
More information3D full wave code modelling of ECRF plasma heating in tokamaks and ITER at fundamental and second harmonics
3D full wave code modelling of ECRF plasma heating in tokamaks and ITER at fundamental and second harmonics Vdovin V.L. RRC Kurchatov Institute Tokamak Physics Institute vdov@nfi.kiae.ru Abstract We present
More informationComparisons of Edge/SOL Turbulence in L- and H-mode Plasmas of Alcator C-Mod
Comparisons of Edge/SOL Turbulence in L- and H-mode Plasmas of Alcator C-Mod J.L. Terry a, S.J. Zweben b, O. Grulke c, B. LaBombard a, M.J. Greenwald a, T. Munsat b, B. Veto a a Plasma Science and Fusion
More informationExternal Stimulation of Edge Modes
External Stimulation of Edge Modes Alan Binus, Willy Burke, Ambrogio Fasoli, Theodore Golfinopoulos, Robert Granetz, Martin Greenwald, Jerry Hughes, Yijun Lin, Brian LaBombard, Rick Leccacorvi, Ronald
More informationDensity and temperature maxima at specific? and B
Density and temperature maxima at specific? and B Matthew M. Balkey, Earl E. Scime, John L. Kline, Paul Keiter, and Robert Boivin 11/15/2007 1 Slide 1 Abstract We report measurements of electron density
More informationLevitated Dipole Experiment
Microwave Interferometer Density Diagnostic for the Levitated Dipole Experiment Columbia University A. Boxer, J. Kesner MIT PSFC M.E. Mauel, D.T. Garnier, A.K. Hansen, Columbia University Presented at
More informationRadio Frequency Current Drive for Small Aspect Ratio Tori
(?onlf-970+/0a- Radio Frequency Current Drive for Small Aspect Ratio Tori M.D. Carter, E.F. Jaeger, D.B. Batchelor, D.J. S&cMer, R. Majeski" Oak Ridge National Laboratoly, Oak Ridge, Tennessee 378314071
More informationPoloidal Transport Asymmetries, Edge Plasma Flows and Toroidal Rotation in Alcator C-Mod
Poloidal Transport Asymmetries, Edge Plasma Flows and Toroidal Rotation in B. LaBombard, J.E. Rice, A.E. Hubbard, J.W. Hughes, M. Greenwald, J. Irby, Y. Lin, B. Lipschultz, E.S. Marmar, K. Marr, C.S. Pitcher,
More informationICRF-Edge and Surface Interactions
ICRF-Edge and Surface Interactions D. A. D Ippolito and J. R. Myra Lodestar Research Corporation Presented at the ReNeW Taming the Plasma Material Interface Workshop, UCLA, March 4-5, 2009 Introduction
More informationLaser-Produced Sn-plasma for Highvolume Manufacturing EUV Lithography
Panel discussion Laser-Produced Sn-plasma for Highvolume Manufacturing EUV Lithography Akira Endo * Extreme Ultraviolet Lithography System Development Association Gigaphoton Inc * 2008 EUVL Workshop 11
More informationTOROIDAL ALFVÉN EIGENMODES
TOROIDAL ALFVÉN EIGENMODES S.E. Sharapov Euratom/CCFE Fusion Association, Culham Science Centre, Abingdon, Oxfordshire OX14 3DB, UK OUTLINE OF LECTURE 4 Toroidicity induced frequency gaps and Toroidal
More informationSpectral broadening of lower hybrid waves produced by parametric instability in current drive experiments of tokamak plasmas
INSTITUTE OF PHYSICS PUBLISHING and INTERNATIONAL ATOMIC ENERGY AGENCY NUCLEAR FUSION Nucl. Fusion 46 (2006) 462 476 doi:10.1088/0029-5515/46/4/007 Spectral broadening of lower hybrid waves produced by
More informationInvestigating High Frequency Magnetic Activity During Local Helicity Injection on the PEGASUS Toroidal Experiment
Investigating High Frequency Magnetic Activity During Local Helicity Injection on the PEGASUS Toroidal Experiment Nathan J. Richner M.W. Bongard, R.J. Fonck, J.L. Pachicano, J.M. Perry, J.A. Reusch 59
More informationCollective Thomson Scattering Study using Gyrotron in LHD
Collective Thomson Scattering Study using Gyrotron in LHD Shin KUBO, Masaki NISHIURA, Kenji TANAKA, Takashi SHIMOZUMA, Yasuo YOSHIMURA, Hiroe IGAMI, Hiromi TAKAHASHI, Takashi MUTOH National Institute for
More informationLong-distance propagation of short-wavelength spin waves. Liu et al.
Long-distance propagation of short-wavelength spin waves Liu et al. Supplementary Note 1. Characterization of the YIG thin film Supplementary fig. 1 shows the characterization of the 20-nm-thick YIG film
More informationIncreased Stable Beta in DIII D by Suppression of a Neoclassical Tearing Mode Using Electron Cyclotron Current Drive and Active Feedback
1 EX/S1-3 Increased Stable Beta in DIII D by Suppression of a Neoclassical Tearing Mode Using Electron Cyclotron Current Drive and Active Feedback R.J. La Haye, 1 D.A. Humphreys, 1 J. Lohr, 1 T.C. Luce,
More informationInitial Data of Digital Correlation ECE with a Giga Hertz Sampling Digitizer
EPJ Web of Conferences 87, 3 (25) DOI:.5/ epjconf/ 25873 C Owned by the authors, published by EDP Sciences, 25 Initial Data of Digital Correlation ECE with a Giga Hertz Sampling Digitizer Hayato Tsuchiya,a,
More informationCritical Problems in Plasma Heating/CD in large fusion devices and ITER
Critical Problems in Plasma Heating/CD in large fusion devices and ITER V.L. Vdovin RRC Kurchatov Institute, Institute of Nuclear Fusion Russia vdov@pike.pike.ru Abstract We identify critical problems
More informationGA A25836 PRE-IONIZATION EXPERIMENTS IN THE DIII-D TOKAMAK USING X-MODE SECOND HARMONIC ELECTRON CYCLOTRON HEATING
GA A25836 PRE-IONIZATION EXPERIMENTS IN THE DIII-D TOKAMAK USING X-MODE SECOND HARMONIC ELECTRON CYCLOTRON HEATING by G.L. JACKSON, M.E. AUSTIN, J.S. degrassie, J. LOHR, C.P. MOELLER, and R. PRATER JULY
More informationICRF-Edge and Surface Interactions
ICRF-Edge and Surface Interactions D. A. D Ippolito and J. R. Myra Lodestar Research Corporation Presented at the 19 th PSI Meeting, San Diego, CA, May 24-28, 2009 Introduction Heating and current drive
More informationToroidal Rotation and Ion Temperature Validations in KSTAR Plasmas
Toroidal Rotation and Ion Temperature Validations in KSTAR Plasmas S. G. Lee 1, H. H. Lee 1, W. H. Ko 1, J. W. Yoo 2, on behalf of the KSTAR team and collaborators 1 NFRI, Daejeon, Korea 2 UST, Daejeon,
More informationThe Lightwave Model 142 CW Visible Ring Laser, Beam Splitter, Model ATM- 80A1 Acousto-Optic Modulator, and Fiber Optic Cable Coupler Optics Project
The Lightwave Model 142 CW Visible Ring Laser, Beam Splitter, Model ATM- 80A1 Acousto-Optic Modulator, and Fiber Optic Cable Coupler Optics Project Stephen W. Jordan Seth Merritt Optics Project PH 464
More informationTHE ELECTROMAGNETIC FIELD THEORY. Dr. A. Bhattacharya
1 THE ELECTROMAGNETIC FIELD THEORY Dr. A. Bhattacharya The Underlying EM Fields The development of radar as an imaging modality has been based on power and power density It is important to understand some
More informationObservation of Toroidal Flow on LHD
17 th International Toki conference / 16 th International Stellarator/Heliotron Workshop 27 Observation of Toroidal Flow on LHD M. Yoshinuma, K. Ida, M. Yokoyama, K. Nagaoka, M. Osakabe and the LHD Experimental
More informationTheory and Applications of Frequency Domain Laser Ultrasonics
1st International Symposium on Laser Ultrasonics: Science, Technology and Applications July 16-18 2008, Montreal, Canada Theory and Applications of Frequency Domain Laser Ultrasonics Todd W. MURRAY 1,
More informationJ.Shafii, J.N. Talmadge, R.J. Vernon, HSX team HSX Plasma Laboratory, University of Wisconsin-Madison T. S. Bigelow, ORNL K.M.
J.Shafii, J.N. Talmadge, R.J. Vernon, HSX team HSX Plasma Laboratory, University of Wisconsin-Madison T. S. Bigelow, ORNL K.M. Likin, Fusion Division, CIEMAT Outline Abstract HSX ECH system Introduction
More informationReflectometry for density and fluctuation measurement on EAST
Reflectometry for density and fluctuation measurement on EAST *, Shoubiao Zhang, Fei Wen, Hao Qu, Yumin Wang, Xiang Han, Defeng Kong, Xiang Gao and EAST contributor Institute of Plasma Physics, Chinese
More informationPedestal Turbulence Dynamics in ELMing and ELM-free H-mode Plasmas
1 Pedestal Turbulence Dynamics in ELMing and ELM-free H-mode Plasmas Z. Yan 1), G.R. McKee 1), R.J. Groebner 2), P.B. Snyder 2), T.H. Osborne 2), M.N.A. Beurskens 3), K.H. Burrell 2), T.E. Evans 2), R.A.
More informationFirst Results From the Alcator C-Mod Lower Hybrid Experiment.
First Results From the Alcator C-Mod Lower Hybrid Experiment. R. Parker 1, N. Basse 1, W. Beck 1, S. Bernabei 2, R. Childs 1, N. Greenough 2, M. Grimes 1, D. Gwinn 1, J. Hosea 2, J. Irby 1, D. Johnson
More information2D Physical optics simulation of fluctuation reflectometry
3rd Intl. Reflectometer Wksp. for Fusion Plasmas. Madrid, May 1997. Informes Técnicos Ciemat 838 39 2D Physical optics simulation of fluctuation reflectometry GDConway Plasma Physics Lab., University of
More informationWall Conditioning Strategy for Wendelstein7-X. H.P. Laqua, D. Hartmann, M. Otte, D. Aßmus
Wall Conditioning Strategy for Wendelstein7-X H.P. Laqua, D. Hartmann, M. Otte, D. Aßmus 1 Outline 1. Physics background 2. Experience from different experiments (LHD, Wega. Tore Supra) 3. Strategy for
More informationRF, Disruption and Thermal Analyses of EAST Antennas*
RF, Disruption and Thermal Analyses of EAST Antennas* L. Zhou, W.K. Beck, P. Koert, J. Doody, R.F. Vieira, S.J. Wukitch, R.S. Granetz, and J.H. Irby Plasma Science and Fusion Center (PSFC) Massachusetts
More informationAdvanced Density Profile Reflectometry; the State-of-the-Art and Measurement Prospects for ITER
Advanced Density Profile Reflectometry; the State-of-the-Art and Measurement Prospects for ITER by E.J. Doyle With W.A. Peebles, L. Zeng, P.-A. Gourdain, T.L. Rhodes, S. Kubota and G. Wang Dept. of Electrical
More informationHeterodyne Sweeping Radiometer
46 Robezu str. LV-1004 Riga, Latvia Fax: +371-7-065102 Mm-wave Division in St. Petersburg, Russia Fax: +7-812- 326-10-60 Tel: +7-812-326-59-24 E-mail: ivanovph@nnz.ru Heterodyne Sweeping Radiometer Operation
More informationHigh Field Side Lower Hybrid Current Drive Launcher Design for DIII-D
High Field Side Lower Hybrid Current Drive Launcher Design for DIII-D by G.M. Wallace (MIT PSFC) Presented at the American Physical Society Division of Plasma Physics Annual Meeting October 23, 2017 On
More informationCHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT
CHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT In this chapter, the experimental results for fine-tuning of the laser wavelength with an intracavity liquid crystal element
More informationGA A24030 ECE RADIOMETER UPGRADE ON THE DIII D TOKAMAK
GA A24030 ECE RADIOMETER UPGRADE ON THE DIII D TOKAMAK by M.E. AUSTIN, and J. LOHR AUGUST 2002 DISCLAIMER This report was prepared as an account of work sponsored by an agency of the United States Government.
More informationICRF Operation with Improved Antennas in a Full W-wall ASDEX Upgrade, Status and Developments
1 EX/P5-19 ICRF Operation with Improved Antennas in a Full W-wall ASDEX Upgrade, Status and Developments V. Bobkov 1*, M. Balden 1, F. Braun 1, R. Dux 1, A. Herrmann 1, H. Faugel 1, H. Fünfgelder 1, L.
More informationFusion Engineering and Design (1997) First results from the three-view far-infrared interferometer for the H1 heliac
ELSEVIER Fusion Engineering and Design 34-35 (1997)387-391 Fusion Engineering and Design First results from the three-view far-infrared interferometer for the H1 heliac George B. Warr, Boyd D. Blackwell,
More informationPhotonic Signals. and Systems. An Introduction. NabeelA.Riza/Ph.D. Department of Electrical and Electronic Engineering University College Cork
Photonic Signals and Systems An Introduction NabeelA.Riza/Ph.D. Department of Electrical and Electronic Engineering University College Cork Cork, Ireland New York Chicago San Francisco Lisbon London Madrid
More informationInterdependence of Magnetic Islands, Halo Current and Runaway Electrons in T-10 Tokamak
IAEA-CN-77/EXP2/02 Interdependence of Magnetic Islands, Halo Current and Runaway Electrons in T-10 Tokamak N.V. Ivanov, A.M. Kakurin, V.A. Kochin, P.E. Kovrov, I.I. Orlovski, Yu.D.Pavlov, V.V. Volkov Nuclear
More information1. Introduction. 2. Concept. reflector. transduce r. node. Kraftmessung an verschiedenen Fluiden in akustischen Feldern
1. Introduction The aim of this Praktikum is to familiarize with the concept and the equipment of acoustic levitation and to measure the forces exerted by an acoustic field on small spherical objects.
More information