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Journal articles on the topic 'Helicon wave'

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Published: 10 December 2022

Last updated: 28 January 2023

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1

Petržílka, V. "Variations of Helicon Wave-induced Radial Plasma Transport in Different Experimental Conditions." Australian Journal of Physics 47, no. 3 (1994): 315. http://dx.doi.org/10.1071/ph940315.

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Variations of the helicon wave-induced radial plasma transport are presented depending on values of the plasma radius, magnetostatic field, plasma density and the frequency of the helicon wave. It is shown that the value of the helicon wave-induced transport may be significant for plasma confinement; this is demonstrated, for the experiments BASIL and SHEILA. Whereas m = +1 helicons induce an inward-directed transport and thus improve the confinement, m = -1 helicons induce an outward-directed transport velocity.

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2

Lau, Cornwall, Michael Brookman, Andris Dimits, Ben Dudson, Elijah Martin, Robert I. Pinsker, Matt Thomas, and Bart Van Compernolle. "Helicon full-wave modeling with scrape-off-layer turbulence on the DIII-D tokamak." Nuclear Fusion 61, no. 12 (November 25, 2021): 126072. http://dx.doi.org/10.1088/1741-4326/ac36f3.

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Abstract Helicon waves have been recently proposed as an off-axis current drive actuator due to their expected high current drive efficiency in the mid-radius region in high beta tokamaks. This paper focuses on a numerical study to better understand effects of scrape-off-layer (SOL) turbulence on helicon wave propagation and absorption on the DIII-D tokamak using a recently developed helicon full-wave model with turbulent density inputs from synthetic single wavelength SOL turbulence and first-principles HERMES multi-wavelength turbulence models. With both input turbulence models, three key effects are observed: the helicon wave can scatter to undesirable locations in the plasma, large helicon wave electric fields can form in localized regions near the SOL turbulence, and the helicon wave can mode convert to slow waves in the SOL. This is shown to cause helicon wave refraction to undesirable locations and strong helicon wave absorption in the SOL resulting in significantly less helicon wave power in the core plasma. Using synthetic SOL turbulence, the simulations additionally show that high amplitudes and long wavelengths greater than a few cm on average have the largest effect on modifying the helicon wave propagation and absorption; the modeling predicts, for example, that approximately 60% of helicon power can be absorbed in the SOL for ñ/n ∼ 0.8 and lambda_perp ∼ 0.05 m. Several potential physical mechanisms that may explain the interaction of helicon waves with SOL turbulence in these simulations are discussed.

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3

Light, Max, and Francis F. Chen. "Helicon wave excitation with helical antennas." Physics of Plasmas 2, no. 4 (April 1995): 1084–93. http://dx.doi.org/10.1063/1.871461.

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4

Zhu, Wanying, Ruilin Cui, Feng He, Tianliang Zhang, and Jiting Ouyang. "On the mechanism of density peak at low magnetic field in argon helicon plasmas." Physics of Plasmas 29, no. 9 (September 2022): 093511. http://dx.doi.org/10.1063/5.0091471.

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Helicon plasma density may show a non-monotonic dependence on the magnetic field at low strength, so-called “low-field peak (LFP).” We presented the multiple LFPs and the formation mechanism in argon helicon plasmas in this paper. Propagating conditions of helicon (H) and Trivelpiece–Gould (TG) waves in collisional plasmas were calculated based on the dispersion relation. It is demonstrated that there are two mechanisms during mode transition responsible for LFP, i.e., resonance of H- and TG-waves and anti-resonance of TG-wave. Especially, H-TG resonance of the highest axial mode in the helicon plasma results in a density jump rather than a density peak due to the mode transition from non-wave to co-H/TG-wave mode. Higher plasma density in lower magnetic fields is helpful for achievement of multiple LFPs in argon helicon plasmas.

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5

JANKAUSKAS, ZIGMANTAS, VYGAUDAS KVEDARAS, and SAULIUS BALEVIČIUS. "RAMAN SCATTERING IN THE MAGNETIZED SEMICONDUCTOR PLASMA." International Journal of Modern Physics B 18, no. 27n29 (November 30, 2004): 3825–29. http://dx.doi.org/10.1142/s0217979204027530.

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Radio frequency (RF) magnetoplasmic waves known as helicons will propagate in solid-state plasmas when a strong magnetic field is applied. In our device the helicons were excited by RFs (the range 100-2000 MHz) much higher than the helicon generation frequency (the main peak at 20 MHz). The excitation of helicons in this case may be described by the effect similar to the Combination Scattering (Raman effect) when a part of the high RF wave energy that passes through the active material is absorbed and re-emitted by the magnetized solid-state plasma. It is expedient to call this experimental device a Helicon Maser (HRM) and the higher frequency e/m field - a pumping field. In full analogy with the usual Raman maser (or laser) the magnetized semiconductor sample plays the role of active material and the connecting cable - the role of high quality external resonator.

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6

Vountesmery, V. S., and Yu V. Vountesmery. "Quarter-wave helicon resonator." Visnyk NTUU KPI Seriia - Radiotekhnika Radioaparatobuduvannia, no. 67 (December 30, 2016): 25–29. http://dx.doi.org/10.20535/radap.2016.67.25-29.

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7

Petržílka, V., and RL Dewar. "Chirality-dependent Plasma Density Profile Changes from Helicon Wave Ponderomotive Forces." Australian Journal of Physics 48, no. 4 (1995): 691. http://dx.doi.org/10.1071/ph950691.

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It is shown that nonresonant helicon-wave-induced transport may result in significant changes in the plasma density radial profile; this is illustrated using parameters appropriate to the cylindrical experiment BASIL and the toroidal experiment SHEILA. Whereas m = +1 helicon waves induce an inward-directed transport and change the density profile to a more centrally peaked one with a higher density on the axis, m = −1 helicon waves induce an outward-directed transport velocity and change the density profile to a hollow one. This may be the clue to the puzzle as to why m = −1 helicon waves are frequently difficult or impossible to excite, as the plasma column is effectively blown off to the discharge chamber walls by the ponderomotive force density of the waves with this chirality (sense of rotation of the wavevector with respect to the axial or toroidal magnetic field).

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8

Nakamura, Keiji, Keiji Suzuki, and Hideo Sugai. "Helicon Wave Measurements in an Inductively Coupled Magnetoplasma." Australian Journal of Physics 48, no. 3 (1995): 461. http://dx.doi.org/10.1071/ph950461.

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Small-amplitude test waves at 30-100 MHz are externally excited in an inductive rf plasma for a magnetic field of rv100 G, to obtain a full dispersion relation for helicon waves. Measured wavelengths agree well with theoretical ones, not only for the test waves but also for largeamplitude principal waves at the discharge frequency of 13�56 MHz. Absolute measurements of the radial magnetic field B; of the large-amplitude helicon wave are carried out, and the r, q and z components of the wave electric field are estimated to be E; rv Eo rv 8 V cm-1 and Ez rv 0�7Vcm-1 at an rf power of 800 W.

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9

Shoucri, M. "Helicon waves in a cylindrical plasma column." Journal of Plasma Physics 52, no. 3 (December 1994): 465–70. http://dx.doi.org/10.1017/s0022377800027264.

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Helicon waves have been used for efficiently coupling radio-frequency power to plasmas, and are studied for their potential application for low-frequency current drive in tokamks. In this paper the electromagnetic field components and the dispersion relation for azimuthally independent helicon-wave oscillations in a cylindrical plasma column are derived. The coupling of transverse electric TE and transverse magnetic TM modes associated with these oscillations is discussed. The effect of the collisional damping on determining the nature of the TM mode (either surface wave or body wave) is analysed.

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10

Paul, Manash Kr, and Dhiraj Bora. "Wave-induced helicity current drive by helicon waves." Physics of Plasmas 14, no. 8 (August 2007): 082507. http://dx.doi.org/10.1063/1.2762130.

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11

Podesta, M. de, and M. Springford. "Helicon wave studies in potassium." Journal of Physics F: Metal Physics 17, no. 3 (March 1987): 639–56. http://dx.doi.org/10.1088/0305-4608/17/3/010.

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12

Lau, C., L. A. Berry, E. F. Jaeger, and N. Bertelli. "Cold plasma finite element wave model for helicon waves." Plasma Physics and Controlled Fusion 61, no. 4 (February 26, 2019): 045008. http://dx.doi.org/10.1088/1361-6587/aafd04.

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13

Seok-Min Yun, Jung-Hyung Kim, and Hong-Young Chang. "Electrical characteristics of helicon wave plasmas." IEEE Transactions on Plasma Science 26, no. 2 (April 1998): 159–66. http://dx.doi.org/10.1109/27.669619.

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14

Kitagawa, H., A. Tsunoda, H. Shindo, and Y. Horiike. "Etching characteristics in helicon wave plasma." Plasma Sources Science and Technology 2, no. 1 (February 1, 1993): 11–13. http://dx.doi.org/10.1088/0963-0252/2/1/003.

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15

Kushwaha, Manvir S. "Helicon Wave Propagation in Semiconductor Superlattices." physica status solidi (b) 136, no. 2 (August 1, 1986): 757–62. http://dx.doi.org/10.1002/pssb.2221360245.

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16

Kushwaha, M. S. "Helicon Wave Propagation in Semiconductor Magnetoplasma." physica status solidi (b) 130, no. 1 (July 1, 1985): K37—K41. http://dx.doi.org/10.1002/pssb.2221300149.

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17

PAUL, MANASH KUMAR, and DHIRAJ BORA. "Radial characterization of wave magnetic field components during helicon discharge in a small aspect ratio torus." Journal of Plasma Physics 76, no. 1 (April 15, 2009): 39–48. http://dx.doi.org/10.1017/s0022377809008010.

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AbstractWave magnetic field components are measured across the radius (−10 cm ≤ r ≤ 10 cm) for a low-pressure (0.3 mbar) helicon discharge, in a toroidal vacuum chamber of small aspect ratio. Radial variation of the wave magnetic field components, measured during the helicon mode of the discharge, exhibit strong poloidal asymmetry which contribute significantly to the wave-induced helicity. The rise in the magnitude of the radial electric field with radiofrequency power, observed during discharge mode transition, supports better radial confinement of the plasma during the helicon mode of the discharge. The strong dependence of the plasma current on the helicon mode of the discharge has been observed during the present experimental study.

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18

MORIMOTO, Katsuki, Hideo OKAYAMA, and Akiyoshi NAGATA. "Preparation of SOFC Grown by Helicon Wave Excited Plasma Sputtering. Energy Control of Helicon Wave Excited Plasma." SHINKU 44, no. 5 (2001): 539–43. http://dx.doi.org/10.3131/jvsj.44.539.

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19

Kushwaha, Manvir S. "Surface-wave instability in helicon wave propagation in layered structures." Solid-State Electronics 29, no. 1 (January 1986): 31–37. http://dx.doi.org/10.1016/0038-1101(86)90195-4.

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20

Miljak, David G., and Francis F. Chen. "Helicon wave excitation with rotating antenna fields." Plasma Sources Science and Technology 7, no. 1 (February 1, 1998): 61–74. http://dx.doi.org/10.1088/0963-0252/7/1/009.

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21

Achar, B. N. Narahari. "Helicon-wave damping in a periodic structure." Physical Review B 36, no. 15 (November 15, 1987): 8147–50. http://dx.doi.org/10.1103/physrevb.36.8147.

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22

Hanna, Jeremy, and Christopher Watts. "Alfvén wave propagation in a helicon plasma." Physics of Plasmas 8, no. 9 (September 2001): 4251–54. http://dx.doi.org/10.1063/1.1386801.

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23

Scharer, J., A. Degeling, G. Borg, and R. Boswell. "Measurements of helicon wave propagation and ArIIemission." Physics of Plasmas 9, no. 9 (September 2002): 3734–42. http://dx.doi.org/10.1063/1.1501475.

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24

Achar, B. N. Narahari. "Helicon-wave propagation in a periodic structure." Physical Review B 35, no. 14 (May 15, 1987): 7334–37. http://dx.doi.org/10.1103/physrevb.35.7334.

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25

Petržílka, V. "On helicon wave induced radial plasma transport." Czechoslovak Journal of Physics 43, no. 12 (December 1993): 1203–11. http://dx.doi.org/10.1007/bf01590188.

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26

Jiwari, Nobuhiro, Hiroaki Iwasawa, Akira Narai, Hiroyuki Sakaue, Haruo Shindo, Tatsuo Shoji, and Yasuhiro Horiike. "Al Etching Characteristics Employing Helicon Wave Plasma." Japanese Journal of Applied Physics 32, Part 1, No. 6B (June 30, 1993): 3019–22. http://dx.doi.org/10.1143/jjap.32.3019.

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27

Loewenhardt, P. K., B. D. Blackwell, and S. M. Hamberger. "Helicon wave propagation in the SHEILA heliac." Plasma Physics and Controlled Fusion 37, no. 3 (March 1, 1995): 229–54. http://dx.doi.org/10.1088/0741-3335/37/3/005.

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28

Ellingboe, A. R., and R. W. Boswell. "Capacitive, inductive and helicon‐wave modes of operation of a helicon plasma source." Physics of Plasmas 3, no. 7 (July 1996): 2797–804. http://dx.doi.org/10.1063/1.871713.

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29

Ellingboe, A. R., R. W. Boswell, J. P. Booth, and N. Sadeghi. "Electron beam pulses produced by helicon‐wave excitation." Physics of Plasmas 2, no. 6 (June 1995): 1807–9. http://dx.doi.org/10.1063/1.871334.

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30

Shah, H. A., I. U. R. Durrani, and T. Abdullah. "Nonlinear helicon-wave propagation in a layered medium." Physical Review B 47, no. 4 (January 15, 1993): 1980–84. http://dx.doi.org/10.1103/physrevb.47.1980.

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31

Jiwari, Nobuhiro, Takayuki Fukasawa, Hiroshi Kawakami, Haruo Shindo, and Yasuhiro Horiike. "Helicon wave plasma reactor employing single‐loop antenna." Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films 12, no. 4 (July 1994): 1322–27. http://dx.doi.org/10.1116/1.579315.

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32

Fischer, B., M. Kramer, and T. Enk. "Helicon wave coupling to a finite plasma column." Plasma Physics and Controlled Fusion 36, no. 12 (December 1, 1994): 2003–20. http://dx.doi.org/10.1088/0741-3335/36/12/004.

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33

Mouzouris, Y., and J. E. Scharer. "Wave propagation and absorption simulations for helicon sources." Physics of Plasmas 5, no. 12 (December 1998): 4253–61. http://dx.doi.org/10.1063/1.873161.

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34

Krämer, M., Yu M. Aliev, A. B. Altukhov, A. D. Gurchenko, E. Z. Gusakov, and K. Niemi. "Anomalous helicon wave absorption and parametric excitation of electrostatic fluctuations in a helicon-produced plasma." Plasma Physics and Controlled Fusion 49, no. 5A (March 28, 2007): A167—A175. http://dx.doi.org/10.1088/0741-3335/49/5a/s14.

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35

ARONOV, IGOR E., ILYA V. KRIVE, SERGEY A. NAFTULIN, and GÖRAN WENDIN. "ELECTROMAGNETIC WAVES IN A NONSUPERCONDUCTING ANYON MATTER." Modern Physics Letters B 08, no. 18 (August 10, 1994): 1135–42. http://dx.doi.org/10.1142/s0217984994001138.

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Normal modes of free electromagnetic oscillations in a two-dimensional anyon gas above the critical temperature of the superconducting phase transition are considered. Making use of the average statistical field approximation we derive the long wave effective Lagrangian for the electromagnetic field in anyon medium and analyze the dependence of thermodynamic parameters entering into the Lagrangian (zero frequency dielectric and magnetic permeabilities, the "Hall conductivity" and the electrostatic screening length) on the temperature, particle density, and statistical parameter θ. It is shown that the only propagating electromagnetic excitation in a nonsuperconducting anyon medium is the chiral helicon wave analogous to the magnetic helicon found previously in the quantum Hall systems.

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36

Lau, C., E. F. Jaeger, N. Bertelli, L. A. Berry, D. L. Green, M. Murakami, J. M. Park, R. I. Pinsker, and R. Prater. "AORSA full wave calculations of helicon waves in DIII-D and ITER." Nuclear Fusion 58, no. 6 (April 11, 2018): 066004. http://dx.doi.org/10.1088/1741-4326/aab96d.

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37

Jung-Hyung Kim, Seek-Min Yun, and Hong-Yeung Chang. "m=±1 and m=±2 mode helicon wave excitation." IEEE Transactions on Plasma Science 24, no. 6 (1996): 1364–70. http://dx.doi.org/10.1109/27.553202.

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38

Kline, J. L., E. E. Scime, R. F. Boivin, A. M. Keesee, and X. Sun. "Slow wave ion heating in the HELIX helicon source." Plasma Sources Science and Technology 11, no. 4 (September 23, 2002): 413–25. http://dx.doi.org/10.1088/0963-0252/11/4/308.

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39

Bose, D., and T. R. Govindan. "Wave currents in a helicon plasma source-model results." IEEE Transactions on Plasma Science 33, no. 2 (April 2005): 374–75. http://dx.doi.org/10.1109/tps.2005.845306.

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40

Chang, L., M. J. Hole, J. F. Caneses, G. Chen, B. D. Blackwell, and C. S. Corr. "Wave modeling in a cylindrical non-uniform helicon discharge." Physics of Plasmas 19, no. 8 (August 2012): 083511. http://dx.doi.org/10.1063/1.4748874.

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41

Li, Jingchun, X. T. Ding, J. Q. Dong, and S. F. Liu. "Helicon wave heating and current drive in toroidal plasmas." Plasma Physics and Controlled Fusion 62, no. 9 (August 5, 2020): 095013. http://dx.doi.org/10.1088/1361-6587/aba367.

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42

Sato, Genta, Wataru Oohara, and Rikizo Hatakeyama. "Experimental Evidence ofm=-1 Helicon Wave Cutoff in Plasmas." Journal of the Physical Society of Japan 75, no. 4 (April 15, 2006): 043501. http://dx.doi.org/10.1143/jpsj.75.043501.

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43

Narahari Achar, B. N. "Nonlocal effects in helicon wave propagation in a superlattice." Superlattices and Microstructures 3, no. 6 (January 1987): 641–43. http://dx.doi.org/10.1016/0749-6036(87)90193-5.

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44

Kim, Jung-Hyung, Seok-Min Yun, and Hong-Young Chang. "M = +1 mode helicon wave excitation using solenoid antenna." Physics Letters A 221, no. 1-2 (September 1996): 94–98. http://dx.doi.org/10.1016/0375-9601(96)00462-8.

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45

Kushwaha, Manvir S. "Instability mechanism in helicon-wave propagation in layered structures." Physical Review B 33, no. 2 (January 15, 1986): 1257–64. http://dx.doi.org/10.1103/physrevb.33.1257.

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46

Takahata, Satoru, Takashi Imao, Hisayuki Nakanishi, Mutsumi Sugiyama, and Shigefusa F. Chichibu. "Helicon-wave-excited plasma sputtering deposition of CuAlO2thin films." physica status solidi (c) 5, no. 9 (July 2008): 3101–3. http://dx.doi.org/10.1002/pssc.200779181.

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47

Cao, Ming Lu, Jia Cheng, Chuan Kun Han, and Lin Hong Ji. "The Current Status of Development and Applications of Wave-Heated Discharge Plasma Sources." Advanced Materials Research 1006-1007 (August 2014): 193–99. http://dx.doi.org/10.4028/www.scientific.net/amr.1006-1007.193.

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Wave-heated discharges are well known as high-efficiency methods to generate high-density plasma at low pressures. In this paper, three types of plasma sources based on different wave-heated discharge principles are introduced systematically. Electron cyclotron resonance plasma, helicon wave plasma, and surface wave plasma systems are promising to be the next generation of plasma sources to meet increasingly strict requirements in microelectronics industry due to their remarkable advantages over conventional plasma sources.

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48

Ping, Lan-Lan, Xin-Jun Zhang, Hua Yang, Guo-Sheng Xu, Lei Chang, Dong-Sheng Wu, Hong Lyu, et al. "Optimal design of helicon wave antenna and numerical investigation into power deposition on helicon physics prototype experiment." Acta Physica Sinica 68, no. 20 (2019): 205201. http://dx.doi.org/10.7498/aps.68.20182107.

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49

Lundin, B., and C. Krafft. "Ion sense of polarization of the electromagnetic wave field in the electron whistler frequency band." Annales Geophysicae 20, no. 8 (August 31, 2002): 1153–65. http://dx.doi.org/10.5194/angeo-20-1153-2002.

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Abstract. It is shown that the left-hand (or ion-type) sense of polarization can appear in the field interference pattern of two plane electron whistler waves. Moreover, it is demonstrated that the ion-type polarized wave electric fields can be accompanied by the presence at the same observation point of electron-type polarized wave magnetic fields. The registration of ion-type polarized fields with frequencies between the highest ion gyrofrequency and the electron gyrofrequency in a cold, overdense plasma is a sufficient indication for the existence of an interference wave pattern, which can typically occur near artificial or natural reflecting magnetospheric plasma regions, inside waveguides (as in helicon discharges, for example), in fields resonantly emitted by beams of charged particles or, in principle, in some self-sustained, nonlinear wave field structures. A comparison with the conventional spectral matrix data processing approach is also presented in order to facilitate the calculations of the analyzed polarization parameters.Key words. Ionosphere (wave propagation) Radio science (waves in plasma) Space plasma physics (general or miscellaneous)

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50

Shinohara, Shunjiro, Yoko Miyauchi, and Yoshinobu Kawai. "Dynamic Formation of Excited Helicon Wave Structure and Estimation of Wave Energy Flux Distribution." Japanese Journal of Applied Physics 35, Part 2, No. 6A (June 1, 1996): L731—L734. http://dx.doi.org/10.1143/jjap.35.l731.

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