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Journal articles on the topic 'Gas discharge physics'

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Published: 4 June 2021
Last updated: 4 February 2022

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1

Rycroft, M. J. "Gas discharge physics." Journal of Atmospheric and Terrestrial Physics 55, no. 10 (August 1993): 1487. http://dx.doi.org/10.1016/0021-9169(93)90114-e.

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2

Galechyan, G. A. "Gas-flow-controlled gas-discharge laser." Laser Physics 17, no. 10 (September 2007): 1209–12. http://dx.doi.org/10.1134/s1054660x07100039.

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3

Eletskii, Aleksandr V., and Boris M. Smirnov. "Nonuniform gas discharge plasma." Uspekhi Fizicheskih Nauk 166, no. 11 (1996): 1197. http://dx.doi.org/10.3367/ufnr.0166.199611c.1197.

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4

Eletskii, Aleksandr V., and Boris M. Smirnov. "Nonuniform gas discharge plasma." Physics-Uspekhi 39, no. 11 (November 30, 1996): 1137–56. http://dx.doi.org/10.1070/pu1996v039n11abeh000179.

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5

Smirnov, Boris M. "Modeling gas discharge plasma." Uspekhi Fizicheskih Nauk 179, no. 6 (2009): 591. http://dx.doi.org/10.3367/ufnr.0179.200906e.0591.

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6

Garscadden, A., M. J. Kushner, and J. G. Eden. "Plasma physics issues in gas discharge laser development." IEEE Transactions on Plasma Science 19, no. 6 (1991): 1013–31. http://dx.doi.org/10.1109/27.125028.

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7

WANG, XINXIN, YUAN HU, and XINHAI SONG. "Gas discharge in a gas peaking switch." Laser and Particle Beams 23, no. 4 (October 2005): 553–58. http://dx.doi.org/10.1017/s0263034605050743.

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The gas discharge in a gas peaking switch was experimentally studied and numerically simulated. For simulation, the discharge was divided into two phases, gas breakdown and voltage collapse. The criterion for an electron avalanche to transit to streamer was considered as the criterion of gas breakdown. The spark channel theory developed by Rompe-Weizel was used to calculate the spark resistance. It was found that the prepulse considerably lowers the voltage pulse applied to the gap. Even for a given input pulse, the voltage pulse applied to a peaking gap is different for different gap distance due to existence of a different prepulse. In this case, the breakdown voltage of a gas peaking gap depends on gas pressure and gap distance, individually. For nitrogen pressure varying from 3 MPa to 10 MPa and gap distance from 0.6 mm to 1.2 mm, the peak electric field higher than 2 MV/cm was achieved when breakdown. The output 10% to 90% rise time, tr, varies from 145 ps to 192 ps. As gas pressure increases, tr decreases, which can be explained by the fact that the breakdown field increases with the increase of gas pressure. It was found in experiment that the jitter in tr could be attributed to the jitter in breakdown field. Instead of getting longer, the averaged experimental tr gets shorter as gap distance increases from 0.6 mm to 1.2 mm, which differs from the results of calculation and indicates there may exist something, other than electric field, that is also related to tr. The reason for this difference may lies in the inverse coefficient of spark resistance varying with gap distance. On the whole, the results from the calculations agree with the experimental ones.
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8

Smirnov, Boris M. "Modeling of gas discharge plasma." Physics-Uspekhi 52, no. 6 (June 30, 2009): 559–71. http://dx.doi.org/10.3367/ufne.0179.200906e.0591.

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9

Brown, KL, and J. Fletcher. "Electronic Energy Distribution Function at High Electron Swarm Energies in Neon." Australian Journal of Physics 48, no. 3 (1995): 479. http://dx.doi.org/10.1071/ph950479.

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Electron swarms moving through a gas under the influence of an applied electric field have been extensively investigated. Swarms at high energies, as measured by the ratio of the applieq field to the gas number density, E/N, which are predominant in many applications have, in general, been neglected. Discharges at E/N in the range 300 < E/N < 2500 Td have been investigated in neon gas in the pressure range 6 < po < 133 Pa using a differentially pumped vacuum system in which the swarm electrons are extracted from the discharge and energy analysed in both a parallel plate retarded potential analyser and a cylindrical electrostatic analyser. Both pre-breakdown and post-breakdown discharges have been studied. Initial results indicate that as the discharge traverses breakdown no sudden change in the nature of the discharge occurs and that the discharge can be described by both a Monte Carlo simulation and by a Boltzmann treatment given by Phelps et al. (1987).
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10

Gherardi, Nicolas, Gamal Gouda, Eric Gat, André Ricard, and François Massines. "Transition from glow silent discharge to micro-discharges in nitrogen gas." Plasma Sources Science and Technology 9, no. 3 (July 13, 2000): 340–46. http://dx.doi.org/10.1088/0963-0252/9/3/312.

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11

TAUSCHWITZ, A., R. BIRKNER, R. KNOBLOCH, S. NEFF, C. NIEMANN, D. PENACHE, R. PRESURA, D. PONCE, and S. YU. "Stability of gas discharge channels for final beam transport." Laser and Particle Beams 20, no. 3 (July 2002): 503–9. http://dx.doi.org/10.1017/s0263034602203286.

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Discharge plasma channels have been investigated in recent years at Gesellschaft für Schwerionenforschung–Darmstadt (GSI) and at the Lawrence Berkeley National Laboratory in Berkeley, California, in a number of experiments. A short summary of the experimental work at Berkeley and GSI is given. Different initiation mechanisms for gas discharges of up to 60 kA were studied and compared. In the Berkeley experiments, laser ionization of organic vapors in a buffer gas was used to initiate and direct the discharge while at GSI, laser gas heating and ion-beam-induced gas ionization were tested as initiation mechanisms. These three initiation techniques are compared and the stability of the resulting discharge channels is discussed. A discharge current of 50 kA, a channel diameter well below 1 cm, a pointing stability better than 200 μm, and MHD stability of more than 10 μs have been demonstrated simultaneously in the recent experiments. These parameters are sufficient or close to the requirements of a reactor application depending on the details of the target design. The experimental results show that transport channels work with sufficient stability, reproducibility, and ion optical properties for a wide pressure range of discharge gases and pressures.
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12

Osipov, V. V., V. V. Lisenkov, and A. N. Orlov. "Space discharge and gas lasers." Laser Physics 16, no. 1 (January 2006): 1–12. http://dx.doi.org/10.1134/s1054660x06010014.

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13

Aramyan, A. R., G. A. Galechyan, and G. V. Manukyan. "Gas-discharge acoustically induced laser." Laser Physics 17, no. 9 (September 2007): 1129–32. http://dx.doi.org/10.1134/s1054660x07090046.

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14

Paunska, Ts, H. Schl ter, A. Shivarova, and Kh Tarnev. "Surface-wave produced discharges in hydrogen: II. Modifications of the discharge structure for varying gas-discharge conditions." Plasma Sources Science and Technology 12, no. 4 (September 11, 2003): 608–18. http://dx.doi.org/10.1088/0963-0252/12/4/312.

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15

Lebedev, Yuri A. "Microwave Discharges in Liquid Hydrocarbons: Physical and Chemical Characterization." Polymers 13, no. 11 (May 21, 2021): 1678. http://dx.doi.org/10.3390/polym13111678.

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Microwave discharges in dielectric liquids are a relatively new area of plasma physics and plasma application. This review cumulates results on microwave discharges in wide classes of liquid hydrocarbons (alkanes, cyclic and aromatic hydrocarbons). Methods of microwave plasma generation, composition of gas products and characteristics of solid carbonaceous products are described. Physical and chemical characteristics of discharge are analyzed on the basis of plasma diagnostics and 0D, 1D and 2D simulation.
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16

Nouri, Anne, and Christian Schmeiser. "Streamers in gas discharge devices." ZAMP Zeitschrift f�r angewandte Mathematik und Physik 47, no. 4 (July 1996): 553–66. http://dx.doi.org/10.1007/bf00914871.

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17

Fletcher, J., and PH Purdie. "Spatial Non-uniformity in Discharges in Low Pressure Helium and Neon." Australian Journal of Physics 40, no. 3 (1987): 383. http://dx.doi.org/10.1071/ph870383.

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Low current, low pressure, steady state Townsend discharges in helium and neon gas have been investigated using the photon flux technique. Such discharges have been found to exhibit spatial non-uniformity resulting in luminous layers throughout the discharge. The separation and structure of these layers has been investigated experimentally in both gases along with the wavelength distribution of the photon flux. A Monte Carlo simulation of the discharge in neon has been used to gain information on the cross sections necessary to describe these discharges. It is found that direct excitaton of ground state atoms to the resonance level of each gas is less than indicated by some published cross section data.
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18

Vikharev, A. L., A. M. Gorbachev, and D. B. Radishev. "Physics and application of gas discharge in millimeter wave beams." Journal of Physics D: Applied Physics 52, no. 1 (October 24, 2018): 014001. http://dx.doi.org/10.1088/1361-6463/aae3a3.

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19

Aktas, K., S. Acar, and B. G. Salamov. "Hydrogen discharges operating at atmospheric pressure in a semiconductor gas discharge system." Plasma Sources Science and Technology 20, no. 4 (June 3, 2011): 045010. http://dx.doi.org/10.1088/0963-0252/20/4/045010.

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20

Kurt, H., E. Koc, and B. G. Salamov. "Atmospheric Pressure DC Glow Discharge in Semiconductor Gas Discharge Electronic Devices." IEEE Transactions on Plasma Science 38, no. 2 (February 2010): 137–41. http://dx.doi.org/10.1109/tps.2009.2036920.

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21

Dong, Lifang, Weili Fan, Yafeng He, and Fucheng Liu. "Self-Organized Gas-Discharge Patterns in a Dielectric-Barrier Discharge System." IEEE Transactions on Plasma Science 36, no. 4 (August 2008): 1356–57. http://dx.doi.org/10.1109/tps.2004.924588.

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22

Aramyan, A. R., and G. A. Galechyan. "Vortices in a gas-discharge plasma." Physics-Uspekhi 50, no. 11 (November 30, 2007): 1147–69. http://dx.doi.org/10.1070/pu2007v050n11abeh006400.

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23

Abramov, A. V., E. A. Pankratova, I. S. Surovtsev, and D. Yu Zolototrubov. "Characteristics of a localized gas discharge." Technical Physics 61, no. 1 (January 2016): 47–52. http://dx.doi.org/10.1134/s1063784216010023.

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24

Zanin, A. L., A. W. Liehr, A. S. Moskalenko, and H. G. Purwins. "Voronoi diagrams in barrier gas discharge." Applied Physics Letters 81, no. 18 (October 28, 2002): 3338–40. http://dx.doi.org/10.1063/1.1518775.

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25

Korzec, Dariusz, Florian Hoppenthaler, and Stefan Nettesheim. "Piezoelectric Direct Discharge: Devices and Applications." Plasma 4, no. 1 (December 28, 2020): 1–41. http://dx.doi.org/10.3390/plasma4010001.

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The piezoelectric direct discharge (PDD) is a comparatively new type of atmospheric pressure gaseous discharge for production of cold plasma. The generation of such discharge is possible using the piezoelectric cold plasma generator (PCPG) which comprises the resonant piezoelectric transformer (RPT) with voltage transformation ratio of more than 1000, allowing for reaching the output voltage >10 kV at low input voltage, typically below 25 V. As ionization gas for the PDD, either air or various gas mixtures are used. Despite some similarities with corona discharge and dielectric barrier discharge, the ignition of micro-discharges directly at the ceramic surface makes PDD unique in its physics and application potential. The PDD is used directly, in open discharge structures, mainly for treatment of electrically nonconducting surfaces. It is also applied as a plasma bridge to bias different excitation electrodes, applicable for a broad range of substrate materials. In this review, the most important architectures of the PDD based discharges are presented. The operation principle, the main operational characteristics and the example applications, exploiting the specific properties of the discharge configurations, are discussed. Due to the moderate power achievable by PCPG, of typically less than 10 W, the focus of this review is on applications involving thermally sensitive materials, including food, organic tissues, and liquids.
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26

RAZHEV A M, RAZHEV A. M., and CHURKIN D. S. CHURKIN D S. "Pulsed inductive discharge gas lasers." Optics and Precision Engineering 19, no. 2 (2011): 237–51. http://dx.doi.org/10.3788/ope.20111902.0237.

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27

Xue-Chen, Li, and Wang Long. "Discharge Characteristics in Atmospheric Pressure Glow Surface Discharge in Helium Gas." Chinese Physics Letters 22, no. 2 (January 27, 2005): 416–19. http://dx.doi.org/10.1088/0256-307x/22/2/041.

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28

HUANG, JiaYu, LiFang DONG, Rong HAN, and YiQian CUI. "Square superlattice pattern by interaction of surface discharge in gas discharge." SCIENTIA SINICA Physica, Mechanica & Astronomica 48, no. 12 (October 8, 2018): 125202. http://dx.doi.org/10.1360/sspma2018-00125.

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29

Zola, J. G. "Gas Discharge Tube Modeling With PSpice." IEEE Transactions on Electromagnetic Compatibility 50, no. 4 (November 2008): 1022–25. http://dx.doi.org/10.1109/temc.2008.2004808.

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30

MI, JUNFENG, DEXUAN XU, XIMEI TIAN, YINGHAO SUN, and XIAOYU ZHANG. "COMPARATIVE INVESTIGATIONS ON MAGNETICAL ENHANCED NEGATIVE- AND POSITIVE-CORONA DISCHARGES." International Journal of Modern Physics B 23, no. 26 (October 20, 2009): 5131–42. http://dx.doi.org/10.1142/s0217979209053710.

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The magnetically enhanced negative- and positive-corona discharges were compared in the current study. In the magnetically enhanced corona discharges, some small permanent magnets were employed to form the local magnetic fields on the corona discharge region, in which the Larmor movements of free electrons enhance ionizations of the gas molecules. The characteristics of discharge current changing in the magnetically enhanced corona discharges were firstly revealed here. The experimental results showed that the relative increases of corona discharge currents had a maximum value in both the magnetically enhanced negative- and positive-corona discharges, when a magnetic field was fixed and the inter-electrode voltages were changed. The reasons for the maximum values were analyzed in detail. In addition, comparing with the magnetically enhanced positive-corona discharge, the inter-electrode voltage for the maximum value is lower for the negative one, because the intensity of inter-electrode electric field was altered by the accumulations of positive or negative ions.
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31

Starikovskiy, Andrey, Nickolay Aleksandrov, and Aleksandr Rakitin. "Plasma-assisted ignition and deflagration-to-detonation transition." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 370, no. 1960 (February 13, 2012): 740–73. http://dx.doi.org/10.1098/rsta.2011.0344.

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Non-equilibrium plasma demonstrates great potential to control ultra-lean, ultra-fast, low-temperature flames and to become an extremely promising technology for a wide range of applications, including aviation gas turbine engines, piston engines, RAMjets, SCRAMjets and detonation initiation for pulsed detonation engines. The analysis of discharge processes shows that the discharge energy can be deposited into the desired internal degrees of freedom of molecules when varying the reduced electric field, E / n , at which the discharge is maintained. The amount of deposited energy is controlled by other discharge and gas parameters, including electric pulse duration, discharge current, gas number density, gas temperature, etc. As a rule, the dominant mechanism of the effect of non-equilibrium plasma on ignition and combustion is associated with the generation of active particles in the discharge plasma. For plasma-assisted ignition and combustion in mixtures containing air, the most promising active species are O atoms and, to a smaller extent, some other neutral atoms and radicals. These active particles are efficiently produced in high-voltage, nanosecond, pulse discharges owing to electron-impact dissociation of molecules and electron-impact excitation of N 2 electronic states, followed by collisional quenching of these states to dissociate the molecules. Mechanisms of deflagration-to-detonation transition (DDT) initiation by non-equilibrium plasma were analysed. For longitudinal discharges with a high power density in a plasma channel, two fast DDT mechanisms have been observed. When initiated by a spark or a transient discharge, the mixture ignited simultaneously over the volume of the discharge channel, producing a shock wave with a Mach number greater than 2 and a flame. A gradient mechanism of DDT similar to that proposed by Zeldovich has been observed experimentally under streamer initiation.
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32

Lister, G. G. "Low-pressure gas discharge modelling." Journal of Physics D: Applied Physics 25, no. 12 (December 14, 1992): 1649–80. http://dx.doi.org/10.1088/0022-3727/25/12/001.

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33

Sternberg, Natalia, Valery Godyak, and Daniel Hoffman. "Magnetic field effects on gas discharge plasmas." Physics of Plasmas 13, no. 6 (June 2006): 063511. http://dx.doi.org/10.1063/1.2214537.

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34

Godyak, Valery. "Hot plasma effects in gas discharge plasma." Physics of Plasmas 12, no. 5 (May 2005): 055501. http://dx.doi.org/10.1063/1.1887171.

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35

Taylor, R. S., and K. E. Leopold. "Magnetic-spiker excitation of gas-discharge lasers." Applied Physics B Lasers and Optics 59, no. 5 (November 1994): 479–508. http://dx.doi.org/10.1007/bf01082392.

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36

Dubinov, Alexander E., Victor D. Selemir, and Vladimir P. Tarakanov. "A Gas-Discharge Vircator: Results of Simulation." IEEE Transactions on Plasma Science 49, no. 6 (June 2021): 1834–41. http://dx.doi.org/10.1109/tps.2021.3080987.

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37

Salamov, B. G., K. Çolakoǧlu, Ş. Altındal, and M. Özer. "A Stable Discharge Glow in Gas Discharge System with Semiconducting Cathode." Journal de Physique III 7, no. 4 (April 1997): 927–36. http://dx.doi.org/10.1051/jp3:1997160.

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38

Wang, Xinxin, Haiyun Luo, and Yuan Hu. "Numerical Simulation of the Gas Discharge in a Gas Peaking Switch." IEEE Transactions on Plasma Science 35, no. 3 (June 2007): 702–8. http://dx.doi.org/10.1109/tps.2007.896963.

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39

Liang, Jian-Ping, Zi-Lu Zhao, Xiong-Feng Zhou, De-Zheng Yang, Hao Yuan, Wen-Chun Wang, and Jun-Jie Qiao. "Comparison of gas phase discharge and gas-liquid discharge for water activation and methylene blue degradation." Vacuum 181 (November 2020): 109644. http://dx.doi.org/10.1016/j.vacuum.2020.109644.

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40

Gerasimov, V. A., and A. V. Pavlinskii. "Collisional thulium vapour gas-discharge laser." Quantum Electronics 34, no. 1 (January 31, 2004): 5–7. http://dx.doi.org/10.1070/qe2004v034n01abeh002570.

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41

Tsendin, Lev D. "Nonlocal electron kinetics in gas-discharge plasma." Physics-Uspekhi 53, no. 2 (May 11, 2010): 133–57. http://dx.doi.org/10.3367/ufne.0180.201002b.0139.

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42

Matsunaga, Yasushi, and Tomokazu Kato. "Analysis of Nonlinear Oscillation in Gas Discharge." Journal of the Physical Society of Japan 63, no. 12 (December 15, 1994): 4396–405. http://dx.doi.org/10.1143/jpsj.63.4396.

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43

Bozhinova, I., S. Kolev, Tsv Popov, A. Pashov, and M. Dimitrova. "Metal hydrides studied in gas discharge tube." Journal of Physics: Conference Series 715 (May 2016): 012002. http://dx.doi.org/10.1088/1742-6596/715/1/012002.

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44

Lebedeva, N. N., V. I. Orbukh, and Ch A. Sultanov. "Gas-discharge system with a zeolite electrode." Technical Physics 55, no. 4 (April 2010): 565–68. http://dx.doi.org/10.1134/s1063784210040225.

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45

Shuaibov, A. K., A. I. Minya, Z. T. Gomoki, A. G. Kalyuzhnaya, and A. I. Shchedrin. "Ultraviolet gas-discharge lamp on iodine molecules." Technical Physics 55, no. 8 (August 2010): 1222–25. http://dx.doi.org/10.1134/s1063784210080232.

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46

Shuaibov, A. K., and I. A. Grabovaya. "Short-wavelength XeBr-Br gas discharge lamp." Technical Physics Letters 33, no. 5 (May 2007): 447–49. http://dx.doi.org/10.1134/s1063785007050264.

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47

Tazmeev, G. K., R. N. Tazmeeva, and B. K. Tazmeev. "Gas discharge between two liquid electrolyte electrodes." Journal of Physics: Conference Series 1588 (July 2020): 012050. http://dx.doi.org/10.1088/1742-6596/1588/1/012050.

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48

Kleymenov, E. Yu, S. A. Klemeshev, P. A. Saveliev, and N. A. Kryukov. "Formation of Xe2molecules in glow gas discharge." Journal of Physics: Conference Series 397 (December 6, 2012): 012036. http://dx.doi.org/10.1088/1742-6596/397/1/012036.

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49

Gershman, S., and A. Belkind. "Electrical discharge in gas bubbles in gel." Journal of Applied Physics 128, no. 13 (October 7, 2020): 133302. http://dx.doi.org/10.1063/5.0016273.

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50

Jeništa, J. "Dynamic behaviour of electric arc gas discharge." Czechoslovak Journal of Physics 44, no. 1 (January 1994): 19–33. http://dx.doi.org/10.1007/bf01691747.

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