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Journal articles on the topic 'Weakly ionized plasma'

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Author: Grafiati

Published: 10 December 2022

Last updated: 28 January 2023

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1

Kiss'ovski, Zh, and A. Shivarova. "Plasma permittivity of weakly ionized inhomogeneous magnetized plasmas." Plasma Physics and Controlled Fusion 37, no. 10 (October 1, 1995): 1119–32. http://dx.doi.org/10.1088/0741-3335/37/10/004.

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2

Sudan, R. N., A. V. Gruzinov, W. Horton, and N. Kukharkin. "Convective turbulence in weakly ionized plasma." Physics Reports 283, no. 1-4 (April 1997): 95–119. http://dx.doi.org/10.1016/s0370-1573(96)00055-5.

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3

Lee, Myoung-Jae, and Young-Dae Jung. "Symmetric and Anti-Symmetric Damping Modes of Trivelpiece–Gould Waves in Weakly and Completely Ionized Plasma Waveguides." Symmetry 13, no. 4 (April 16, 2021): 699. http://dx.doi.org/10.3390/sym13040699.

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The collision effects on the low-frequency ion-acoustic Trivelpiece–Gould wave are investigated in weakly and completely ionized plasma waveguides by using the normal mode analysis. In weakly ionized plasma waveguides, it is found that the dependence of the harmonic mode on the absolute value of the scaled damping rate shows the opposite tendency for large and small radii of the cylindrical waveguide. It is also is found that the scaled damping rates for both weakly and completely ionized plasma waveguides decrease with an increase of the electron temperature. It is interesting to note that the scaled damping rate for weakly ionized plasma waveguides shows anti-symmetric behavior when the Trivelpiece–Gould wave propagates in the negative-z direction. However, it is found that the scaled damping rate for completely ionized plasma waveguides shows the symmetric behavior when the Trivelpiece–Gould wave propagates in the negative-z direction.

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4

Pavlov, V. A. "Weakly ionized plasma in a supersonic plasma flow." Plasma Physics Reports 28, no. 6 (June 2002): 479–83. http://dx.doi.org/10.1134/1.1485651.

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5

DAS, CHANDRA. "Evolution of magnetic moment in the interaction of waves with kinetically described plasmas." Journal of Plasma Physics 57, no. 2 (February 1997): 343–48. http://dx.doi.org/10.1017/s002237789600493x.

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The non-oscillating part of the magnetic moment field (called the inverse Faraday effect (IFE) for this field from a circularly polarized wave in a medium) is calculated for the interaction of an elliptically polarized wave with a weakly ionized magnetized plasma in a kinetic theory model and with unmagnetized Vlasov plasmas. For a weakly ionized magnetized plasma, the induced field increases with both temperature and ambient magnetic field. For an unmagnetized plasma, it increases parabolically with temperature. The induced magnetic field is found to vary parabolically with temperature in the case of an unmagnetized Vlasov plasma.

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6

Alharbi, A., I. Ballai, V. Fedun, and G. Verth. "Waves in weakly ionized solar plasmas." Monthly Notices of the Royal Astronomical Society 511, no. 4 (February 18, 2022): 5274–86. http://dx.doi.org/10.1093/mnras/stac444.

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ABSTRACT Here, we study the nature and characteristics of waves propagating in partially ionized plasmas in the weakly ionized limit, typical for the lower part of the solar atmosphere. The framework in which the properties of waves are discussed depends on the relative magnitude of collisions between particles, but also on the relative magnitude of the collisional frequencies compared to the gyro-frequency of charged particles. Our investigation shows that the weakly ionized solar atmospheric plasma can be divided into two regions, and this division occurs, roughly, at the base of the chromosphere. In the solar photosphere, the plasma is non-magnetized and the dynamics can described within the three-fluid framework, where acoustic waves associated to each species can propagate. Due to the very high concentration of neutrals, the neutral sound waves propagates with no damping, while for the other two modes the damping rate is determined by collisions with neutrals. The ion- and electron-related acoustic modes propagate with a cut-off determined by the collisional frequency of these species with neutrals. In the weakly ionized chromosphere, only electrons are magnetized, however, the strong coupling of charged particles reduces the working framework to a two-fluid model. The disassociation of charged particles creates electric currents that can influence the characteristic of waves. The propagation properties of waves with respect to the angle of propagation are studied with the help of polar diagrams.

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7

Graves, David B., and Richard A. Gottscho. "Computer Applications in Plasma Materials Processing." MRS Bulletin 16, no. 2 (February 1991): 16–22. http://dx.doi.org/10.1557/s0883769400057602.

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In manufacturing microelectronic and optoelectronic devices, thin solid films of various sorts are routinely deposited and etched using low pressure, weakly ionized plasmas. The term “plasma” in this context implies an ionized gas with nearly equal numbers of positive and negative charges. This definition is not very restrictive, so. there are an enormous number of phenomena that are termed plasmas. For example, very hot, magnetized, fully ionized plasmas exist in stellar environments and thermonuclear fusion experiments. High temperature electric arcs are a form of plasma as well. In contrast, the plasmas used in electronic materials processing are near room temperature and the gas is usually weakly ionized. Indeed, due to the sensitivity of electronic devices to high temperatures, their low operating temperature is one of the major advantages of plasma processes.Plasma processing is attractive because of two important physiochemical effects: energetic free electrons in the plasma (heated by applied electric fields) dissociate the neutral gas in the plasma to create chemically reactive species; and free positive ions are accelerated by the plasma electric fields to surfaces bounding the plasma. Reactive species created in the plasma diffuse to surfaces and adsorb; wafers to be processed are typically placed on one of these surfaces.The combination of neutral species adsorption and positive ion bombardment results in surface chemical reaction. If the products of the surface reaction are volatile, they leave the surface and etching results. If the products are involatile, a surface film grows.

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8

Leake, James E., Vyacheslav S. Lukin, and Mark G. Linton. "Magnetic reconnection in a weakly ionized plasma." Physics of Plasmas 20, no. 6 (June 2013): 061202. http://dx.doi.org/10.1063/1.4811140.

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9

Zagorodny, A. G., A. V. Filippov, A. F. Pal', A. N. Starostin, and A. I. Momot. "Macroparticle screening in a weakly ionized plasma." Journal of Physical Studies 11, no. 2 (2007): 158–64. http://dx.doi.org/10.30970/jps.11.158.

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10

Stiele, H., H. Lesch, and F. Heitsch. "Thermal instability in a weakly ionized plasma." Monthly Notices of the Royal Astronomical Society 372, no. 2 (October 21, 2006): 862–68. http://dx.doi.org/10.1111/j.1365-2966.2006.10909.x.

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11

V.Reddy, Ramireddygari, Kunihiko Watanabe, Tomohiko Watanabe, and Tetsuya Sato. "Impulsive Alfven Coupling between the Fully-Ionized Plasma and the Weakly-Ionized Plasma." Journal of the Physical Society of Japan 64, no. 1 (January 15, 1995): 124–35. http://dx.doi.org/10.1143/jpsj.64.124.

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12

Furkal, E., A. Smolyakov, and A. Hirose. "Nonlocal electron kinetics in a weakly ionized plasma." Physical Review E 58, no. 1 (July 1, 1998): 965–75. http://dx.doi.org/10.1103/physreve.58.965.

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13

Ren, Haijun, Jintao Cao, and Zhengwei Wu. "MAGNETOROTATIONAL INSTABILITY IN A COLLISIONAL WEAKLY IONIZED PLASMA." Astrophysical Journal 754, no. 2 (July 17, 2012): 128. http://dx.doi.org/10.1088/0004-637x/754/2/128.

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14

Peurrung, A. J., and S. E. Barlow. "Characteristics of a weakly ionized non‐neutral plasma." Physics of Plasmas 3, no. 8 (August 1996): 2859–63. http://dx.doi.org/10.1063/1.871645.

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15

Farina, D., M. Lontano, and R. Pozzoli. "Radiofrequency current drive in a weakly ionized plasma." Nuclear Fusion 27, no. 1 (January 1, 1987): 155–58. http://dx.doi.org/10.1088/0029-5515/27/1/015.

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16

Sosenko, P. P., and M. Poleni. "Global drift waves in weakly ionized plasma column." Journal of Physical Studies 6, no. 3 (2002): 310–16. http://dx.doi.org/10.30970/jps.06.310.

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17

Suetsugu, Yusuke, Akio Komori, and Yoshinobu Kawai. "Collisional Drift Instability in a Weakly Ionized Plasma." Journal of the Physical Society of Japan 54, no. 10 (October 15, 1985): 3664–67. http://dx.doi.org/10.1143/jpsj.54.3664.

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18

Wemlinger, Erik C., and Patrick D. Pedrow. "Acetylene Deposition Using Atmospheric Pressure Weakly Ionized Plasma." IEEE Transactions on Plasma Science 42, no. 6 (June 2014): 1602–6. http://dx.doi.org/10.1109/tps.2014.2320268.

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19

Rohlena, Karel, and Helge R. Skullerud. "Transport coefficients in a weakly ionized nonequilibrium plasma." Physical Review E 51, no. 6 (June 1, 1995): 6028–35. http://dx.doi.org/10.1103/physreve.51.6028.

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20

Karashtin, A. N., A. V. Gurevich, and K. P. Zybin. "Density irregularities in the weakly ionized nonuniform plasma." Physics of Plasmas 4, no. 11 (November 1997): 4090–102. http://dx.doi.org/10.1063/1.872529.

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21

Mishin, G. I. "Structure of a weakly ionized gas-discharge plasma." Technical Physics Letters 24, no. 6 (June 1998): 448–50. http://dx.doi.org/10.1134/1.1262162.

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22

Chu, J. H., and Lin I. "Coulomb lattice in a weakly ionized colloidal plasma." Physica A: Statistical Mechanics and its Applications 205, no. 1-3 (April 1994): 183–90. http://dx.doi.org/10.1016/0378-4371(94)90498-7.

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23

Yu, Pengcheng, Yu Liu, Xiangqun Liu, and Jiuhou Lei. "Sheath expansion effect of double flush mounted probe in weakly ionized plasma." Physics of Plasmas 29, no. 9 (September 2022): 093508. http://dx.doi.org/10.1063/5.0099065.

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Sheath expansion is a distinctive feature of the double flush mounted probe because of the embedded configuration. Previously, the sheath expansion effect was usually neglected in weakly ionized plasma dominated by collisions between charged particles and neutrals. In this work, we investigated the sheath expansion effect of the double flush mounted probe in weakly ionized plasma. Results indicate that measurements using the double flush mounted probe were also influenced to a certain extent by the sheath expansion effect in weakly ionized plasma. To eliminate the influence, an empirical analytical formula has been presented to eliminate the influence of sheath expansion. In addition, a fitting curve is given based on experimental data, which indicates that sheath expansion should be considered in processing the measured data when the plasma pressure is lower than 200 Pa. In summary, this work indicates that the ion–neutral collision is a crucial factor that affects sheath expansion in addition to the radius parameter and probes' bias, which can be extended to double flush mounted probe diagnostics in collisional plasma such as the reentry plasma sheath and high-powered plasma thruster.

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24

Lee, Yonghoon, Xianglei Mao, George C. Y. Chan, Jhanis Gonzalez, Richard E. Russo, and Vassilia Zorba. "Spatial and temporal distribution of metal atoms and their diatomic oxide molecules in femtosecond laser-induced plasmas." Journal of Analytical Atomic Spectrometry 33, no. 11 (2018): 1875–83. http://dx.doi.org/10.1039/c8ja00150b.

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Distribution of atoms and diatomic metal oxide molecules in femtosecond laser-induced plasmas generated at and after the laser beam focal plane, where nonlinear phenomena give rise to the formation of weakly ionized air plasma channels.

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25

MENDONÇA, J. T., J. LOUREIRO, and H. TERÇAS. "Waves in Rydberg plasmas." Journal of Plasma Physics 75, no. 6 (April 16, 2009): 713–19. http://dx.doi.org/10.1017/s0022377809007971.

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AbstractWe define as the Rydberg plasma the weakly ionized gas produced in magneto-optical traps. In such a plasma, the neutral atoms can be excited in Rydberg states. Wave propagation in Rydberg plasmas and the mutual influence of plasma dispersion and atomic dispersion are considered. New dispersion relations are established, showing new instability regimes and new cut-off frequencies.

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26

Oksuz, L., and N. Hershkowitz. "Plasma, presheath, collisional sheath and collisionless sheath potential profiles in weakly ionized, weakly collisional plasma." Plasma Sources Science and Technology 14, no. 1 (February 1, 2005): 201–8. http://dx.doi.org/10.1088/0963-0252/14/1/022.

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27

He, Chuan, Thomas C. Corke, and Mehul P. Patel. "Plasma Flaps and Slats: An Application of Weakly Ionized Plasma Actuators." Journal of Aircraft 46, no. 3 (May 2009): 864–73. http://dx.doi.org/10.2514/1.38232.

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28

Furkal, E., A. Smolyakov, and A. Hirose. "Nonlocal ion transport in a weakly ionized nonequilibrium plasma." IEEE Transactions on Plasma Science 26, no. 2 (April 1998): 198–207. http://dx.doi.org/10.1109/27.669628.

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29

Xia, Hengyang, Ying Wang, Chengxun Yuan, Zhongxiang Zhou, A. A. Kudryavtsev, Xiaoou Wang, Bin Xu, Kun Xue, Hui Li, and Jian Wu. "Measurement of Microwave Propagation in Weakly Ionized Dusty Plasma." IEEE Transactions on Plasma Science 47, no. 1 (January 2019): 109–12. http://dx.doi.org/10.1109/tps.2018.2887244.

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30

Hatami, M. M., A. R. Niknam, B. Shokri, and A. A. Rukhadze. "Nonlinear thermocurrent beam instability of a weakly ionized plasma." Physics of Plasmas 15, no. 2 (February 2008): 022107. http://dx.doi.org/10.1063/1.2842364.

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31

Lucken, R., A. Tavant, A. Bourdon, M. A. Lieberman, and P. Chabert. "Saturation of the magnetic confinement in weakly ionized plasma." Plasma Sources Science and Technology 29, no. 6 (June 24, 2020): 065014. http://dx.doi.org/10.1088/1361-6595/ab38b2.

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32

Ahmed Marzouk, Osama. "Multi-Physics Mathematical Model of Weakly-Ionized Plasma Flows." American Journal of Modern Physics 7, no. 2 (2018): 87. http://dx.doi.org/10.11648/j.ajmp.20180702.14.

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33

Sato, Eiichi, Yasuomi Hayashi, Rudolf Germer, Etsuro Tanaka, Hidezo Mori, Toshiaki Kawai, Takashi Inoue, et al. "X-ray Spectra from Weakly Ionized Linear Copper Plasma." Japanese Journal of Applied Physics 45, no. 6A (June 8, 2006): 5301–6. http://dx.doi.org/10.1143/jjap.45.5301.

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34

Lisin, E. A., O. S. Vaulina, O. F. Petrov, and V. E. Fortov. "Dust-particle charge in weakly ionized gas-discharge plasma." EPL (Europhysics Letters) 97, no. 5 (March 1, 2012): 55003. http://dx.doi.org/10.1209/0295-5075/97/55003.

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35

Belevtsev, A. A. "Charge kinetics in weakly ionized plasma of electronegative gases." High Temperature 51, no. 4 (July 2013): 435–42. http://dx.doi.org/10.1134/s0018151x13040020.

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36

Krasovitskii, D. V., and V. F. Papakin. "Electrostatic-perturbation collisional damping in a weakly ionized plasma." Radiophysics and Quantum Electronics 31, no. 10 (October 1988): 841–46. http://dx.doi.org/10.1007/bf01040015.

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37

Vranjes, J., S. Poedts, B. P. Pandey, and B. De Pontieu. "Energy flux of Alfvén waves in weakly ionized plasma." Astronomy & Astrophysics 478, no. 2 (November 20, 2007): 553–58. http://dx.doi.org/10.1051/0004-6361:20078274.

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38

Perevoznikov, E. N. "Short-Wave Charge Instabilities of Weakly Ionized Plasma Flows." Journal of Engineering Physics and Thermophysics 86, no. 6 (November 2013): 1474–80. http://dx.doi.org/10.1007/s10891-013-0975-z.

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39

Martinović, M. M., A. Zaslavsky, M. Maksimović, and S. Šegan. "Electrostatic thermal noise in a weakly ionized collisional plasma." Radio Science 52, no. 1 (January 2017): 70–77. http://dx.doi.org/10.1002/2016rs006189.

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40

SOSENKO, PETRO P., GÉRARD BONHOMME, and THIÉRY PIERRE. "Global drift waves in weakly ionized magnetized plasmas: theory and observations." Journal of Plasma Physics 63, no. 2 (February 2000): 157–90. http://dx.doi.org/10.1017/s002237789900803x.

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41

Baksht, F. G., and V. F. Lapshin. "Electron heat transport through the plasma-electrode boundary in weakly ionized plasma." Plasma Physics Reports 38, no. 13 (December 2012): 1019–24. http://dx.doi.org/10.1134/s1063780x1208003x.

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42

Numano, M., Y. Murakami, and T. Nitta. "Effects of non-uniformities on electrical conduction in weakly ionized plasmas." Journal of Plasma Physics 42, no. 1 (August 1989): 177–85. http://dx.doi.org/10.1017/s0022377800014252.

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The effect of non-uniformities on the flow of electric current in weakly ionized plasmas is investigated by taking into account the ion slip as well as the Hall current. An Ohm's law for a non-uniform plasma is derived, from which the formula previously obtained by Numano, i.e. an extension of Rosa's equation, is obtainable as a special case. Making use of this new Ohm's law, the effective electrical conductivity and the effective Hall parameter are determined for isotropically turbulent plasmas. It is found that when the ion-slip effect is absent they are in good agreement with the results obtained previously.

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43

SOHBATZADEH, F., S. MIRZANEJHAD, and M. GHALANDARI. "Optical guiding in a plasma channel having top-hat refractive index radial profile." Journal of Plasma Physics 78, no. 1 (August 4, 2011): 39–45. http://dx.doi.org/10.1017/s0022377811000341.

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AbstractIn this paper, intense laser pulse guiding through a weakly ionized plasma channel is studied numerically. The radial profile of the channel refractive index is assumed to be top-hat. The propagating intense laser pulses are Gaussian TEM00 and Laguerre–Gaussian LG01 modes. The analysis includes the effects of plasma density inhomogeneity, diffraction, further ionization by the propagating laser pulse and nonlinearity arising from the nonlinear Kerr effect. Matched conditions are obtained for both TEM00 and LG01 laser modes for a top-hat refractive index profile. It is seen that the electron density profile changes the matched condition in the transmission of the laser pulse through the plasma channel. It is also shown that the nonlinear Kerr effect changes the matched condition and becomes the dominant effect in intense laser pulse propagation through the weakly ionized plasma channel.

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44

Shao, Chun, Deyang Tian, Kun Qian, and Weifang Chen. "Numerical Simulation of Weakly Ionized Dynamic Plasma for Reentry Vehicles." Journal of Spacecraft and Rockets 53, no. 5 (September 2016): 900–911. http://dx.doi.org/10.2514/1.a33525.

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45

Josyula, Eswar, and William F. Bailey. "Governing Equations for Weakly Ionized Plasma Flowfields of Aerospace Vehicles." Journal of Spacecraft and Rockets 40, no. 6 (November 2003): 845–57. http://dx.doi.org/10.2514/2.7036.

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46

Grach, V. S. "Interaction between two conducting spheres in weakly ionized collisional plasma." Plasma Physics Reports 43, no. 5 (May 2017): 555–65. http://dx.doi.org/10.1134/s1063780x17050051.

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47

Kompaneets, Roman, Yuriy O. Tyshetskiy, and Sergey V. Vladimirov. "Ion response in a weakly ionized plasma with ion flow." Physics of Plasmas 20, no. 4 (April 2013): 042108. http://dx.doi.org/10.1063/1.4737145.

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48

Hou, Lei, and Wei Shi. "Fast Terahertz Continuous-Wave Detector Based on Weakly Ionized Plasma." IEEE Electron Device Letters 33, no. 11 (November 2012): 1583–85. http://dx.doi.org/10.1109/led.2012.2214471.

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49

Babič, D., I. Poberaj, and M. Mozetič. "Fiber optic catalytic probe for weakly ionized oxygen plasma characterization." Review of Scientific Instruments 72, no. 11 (November 2001): 4110–14. http://dx.doi.org/10.1063/1.1409567.

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50

Ebne abbasi, Zeinab, and Abdolrasoul Esfandyari-Kalejahi. "Transport coefficients of a weakly ionized plasma with nonextensive particles." Physics of Plasmas 26, no. 1 (January 2019): 012301. http://dx.doi.org/10.1063/1.5051585.

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