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Journal articles on the topic 'Plasma interactions'

Author: Grafiati

Published: 4 June 2021

Last updated: 20 February 2023

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1

Kallenbach, A., M. Balden, R. Dux, T. Eich, C. Giroud, A. Huber, G. P. Maddison, et al. "Plasma surface interactions in impurity seeded plasmas." Journal of Nuclear Materials 415, no. 1 (August 2011): S19—S26. http://dx.doi.org/10.1016/j.jnucmat.2010.11.105.

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2

Bruggeman, P. J., A. Bogaerts, J. M. Pouvesle, E. Robert, and E. J. Szili. "Plasma–liquid interactions." Journal of Applied Physics 130, no. 20 (November 28, 2021): 200401. http://dx.doi.org/10.1063/5.0078076.

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3

Boeuf, J. P., P. Belenguer, and T. Hbid. "Plasma particle interactions." Plasma Sources Science and Technology 3, no. 3 (August 1, 1994): 407–17. http://dx.doi.org/10.1088/0963-0252/3/3/026.

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4

Goeckner, M. J., C. T. Nelson, S. P. Sant, A. K. Jindal, E. A. Joseph, B. S. Zhou, G. Padron-Wells, B. Jarvis, R. Pierce, and L. J. Overzet. "Plasma-surface interactions." Journal of Physics: Conference Series 133 (October 1, 2008): 012010. http://dx.doi.org/10.1088/1742-6596/133/1/012010.

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5

Lafleur, Trevor, Julian Schulze, and Zoltan Donkó. "Plasma-surface interactions." Plasma Sources Science and Technology 28, no. 4 (April 16, 2019): 040201. http://dx.doi.org/10.1088/1361-6595/ab1380.

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6

Hess, Dennis W. "Plasma–material interactions." Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films 8, no. 3 (May 1990): 1677–84. http://dx.doi.org/10.1116/1.576829.

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7

F�lthammar, Carl-Gunne. "Magnetospheric plasma interactions." Astrophysics and Space Science 214, no. 1-2 (April 1994): 3–17. http://dx.doi.org/10.1007/bf00982321.

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8

Neubauer, F. M. "Satellite plasma interactions." Advances in Space Research 10, no. 1 (January 1990): 25–38. http://dx.doi.org/10.1016/0273-1177(90)90083-c.

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9

Chang, J. P., and J. W. Coburn. "Plasma–surface interactions." Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films 21, no. 5 (September 2003): S145—S151. http://dx.doi.org/10.1116/1.1600452.

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10

Neyts, Erik C. "Plasma-Surface Interactions in Plasma Catalysis." Plasma Chemistry and Plasma Processing 36, no. 1 (October 16, 2015): 185–212. http://dx.doi.org/10.1007/s11090-015-9662-5.

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11

MacGowan, B. J., B. B. Afeyan, C. A. Back, R. L. Berger, G. Bonnaud, M. Casanova, B. I. Cohen, et al. "Laser–plasma interactions in ignition‐scale hohlraum plasmas." Physics of Plasmas 3, no. 5 (May 1996): 2029–40. http://dx.doi.org/10.1063/1.872000.

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12

Froula, D. H., D. T. Michel, I. V. Igumenshchev, S. X. Hu, B. Yaakobi, J. F. Myatt, D. H. Edgell, et al. "Laser–plasma interactions in direct-drive ignition plasmas." Plasma Physics and Controlled Fusion 54, no. 12 (November 21, 2012): 124016. http://dx.doi.org/10.1088/0741-3335/54/12/124016.

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13

Constantin, C. G., H. A. Baldis, M. B. Schneider, D. E. Hinkel, A. B. Langdon, W. Seka, R. Bahr, and S. Depierreux. "Laser-plasma interactions in high-energy density plasmas." Journal de Physique IV (Proceedings) 133 (June 2006): 243–46. http://dx.doi.org/10.1051/jp4:2006133049.

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14

Bogaerts, Annemie, Evi Bultinck, Maxie Eckert, Violeta Georgieva, Ming Mao, Erik Neyts, and Laurent Schwaederlé. "Computer Modeling of Plasmas and Plasma-Surface Interactions." Plasma Processes and Polymers 6, no. 5 (May 15, 2009): 295–307. http://dx.doi.org/10.1002/ppap.200800207.

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15

Bogaerts, Annemie, Christophe De Bie, Maxie Eckert, Violeta Georgieva, Tom Martens, Erik Neyts, and Stefan Tinck. "Modeling of the plasma chemistry and plasma–surface interactions in reactive plasmas." Pure and Applied Chemistry 82, no. 6 (April 20, 2010): 1283–99. http://dx.doi.org/10.1351/pac-con-09-09-20.

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In this paper, an overview is given of modeling activities going on in our research group, for describing the plasma chemistry and plasma–surface interactions in reactive plasmas. The plasma chemistry is calculated by a fluid approach or by hybrid Monte Carlo (MC)–fluid modeling. An example of both is illustrated in the first part of the paper. The example of fluid modeling is given for a dielectric barrier discharge (DBD) in CH4/O2, to describe the partial oxidation of CH4 into value-added chemicals. The example of hybrid MC–fluid modeling concerns an inductively coupled plasma (ICP) etch reactor in Ar/Cl2/O2, including also the description of the etch process. The second part of the paper deals with the treatment of plasma–surface interactions on the atomic level, with molecular dynamics (MD) simulations or a combination of MD and MC simulations.

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16

Myra, J. R., D. A. D'Ippolito, D. A. Russell, L. A. Berry, E. F. Jaeger, and M. D. Carter. "Nonlinear ICRF-plasma interactions." Nuclear Fusion 46, no. 7 (June 21, 2006): S455—S468. http://dx.doi.org/10.1088/0029-5515/46/7/s08.

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17

Luna, E., and A. Hitt. "Cytoskeleton--plasma membrane interactions." Science 258, no. 5084 (November 6, 1992): 955–64. http://dx.doi.org/10.1126/science.1439807.

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18

Stillwell, R. P., N. J. Stevens, G. K. Crawford, S. R. Strader, and J. R. Valles. "AC system-plasma interactions." IEEE Transactions on Nuclear Science 35, no. 6 (1988): 1394–99. http://dx.doi.org/10.1109/23.25470.

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19

Tsytovich, V. N., R. Bingham, J. M. Dawson, and H. A. Bethe. "Collective neutrino-plasma interactions." Astroparticle Physics 8, no. 4 (April 1998): 297–307. http://dx.doi.org/10.1016/s0927-6505(97)00044-3.

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20

Umstadter, Donald. "Relativistic laser plasma interactions." Journal of Physics D: Applied Physics 36, no. 8 (April 3, 2003): R151—R165. http://dx.doi.org/10.1088/0022-3727/36/8/202.

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21

Zarka, P. "Planet–star plasma interactions." EAS Publications Series 41 (2010): 441–54. http://dx.doi.org/10.1051/eas/1041036.

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22

Silva, L. O., R. Bingham, J. M. Dawson, J. T. Mendonça, and P. K. Shukla. "Collective neutrino–plasma interactions." Physics of Plasmas 7, no. 5 (May 2000): 2166–72. http://dx.doi.org/10.1063/1.874037.

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23

Silva, L. O., R. Bingham, J. T. Mendon�a, W. B. Mori, and P. K. Shukla. "Neutrino Beam Plasma Interactions." Physica Scripta T107, no. 5 (2004): 9. http://dx.doi.org/10.1238/physica.topical.107a00009.

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24

Westhoff, R., G. Trapaga, and J. Szekely. "Plasma-particle interactions in plasma spraying systems." Metallurgical Transactions B 23, no. 6 (December 1992): 683–93. http://dx.doi.org/10.1007/bf02656448.

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25

Heidari, E. "Relativistic Laser-Plasma Interactions. Moving Solitary Waves in Plasma Channels and the Kinetic Dispersion Relation of Cherenkov Radiation." Ukrainian Journal of Physics 62, no. 12 (December 2017): 1017–23. http://dx.doi.org/10.15407/ujpe62.12.1017.

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26

Renner, O., R. Liska, and F. B. Rosmej. "Laser-produced plasma-wall interaction." Laser and Particle Beams 27, no. 4 (December 2009): 725–31. http://dx.doi.org/10.1017/s0263034609990504.

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AbstractJets of laser–generated plasma represent a flexible and well-defined model environment for investigation of plasma interactions with solid surfaces (walls). The pilot experiments carried out on the iodine laser system (5–200 J, 0.44 µm, 0.25–0.3 ns, <1×1016 W/cm2) at the PALS Research Centre in Prague are reported. Modification of macroscopic characteristics of the Al plasma jets produced at laser-irradiated double-foil Al/Mg targets is studied by high-resolution, high-dispersion X-ray spectroscopy. The spatially variable, complex satellite structure observed in emission spectra of the Al Lyα group proves a formation of rather cold dense plasma at the laser-exploded Al foil, an occurrence of the hot plasma between both foils and subsequent thermalization, deceleration and trapping of Al ions in the colliding plasma close to the Mg foil surface. The spectra interpretation based on the collisional-radiative code is complemented by 1D and 2D hydrodynamic modeling of the plasma expansion and interaction of counter-propagating Al/Mg plasmas. The obtained results demonstrate a potential of high resolution X-ray diagnostics in investigation of the laser-produced plasma–wall interactions.

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27

Hamaguchi, S., and R. T. Farouki. "Plasma–particulate interactions in nonuniform plasmas with finite flows." Physics of Plasmas 1, no. 7 (July 1994): 2110–18. http://dx.doi.org/10.1063/1.870608.

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28

Černý, Pavel, Stanislav Novák, and Rudolf Hrach. "Dynamics of plasma–surface interactions in chemically active plasmas." Vacuum 84, no. 1 (August 2009): 97–100. http://dx.doi.org/10.1016/j.vacuum.2009.06.010.

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29

Kasperczuk, Andrzej, Tadeusz Pisarczyk, Tomasz Chodukowski, Zofia Kalinowska, Sergiey Yu Gus'kov, Nikolay N. Demchenko, Jiri Ullschmied, et al. "Interactions of plastic plasma with different atomic number plasmas." Physica Scripta T161 (May 1, 2014): 014034. http://dx.doi.org/10.1088/0031-8949/2014/t161/014034.

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30

Doerner, R. P., S. C. Luckhardt, R. Seraydarian, F. C. Sze, and D. G. Whyte. "Plasma Interactions with Mixed-Material Plasma Facing Components." Physica Scripta T81, no. 1 (1999): 35. http://dx.doi.org/10.1238/physica.topical.081a00035.

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31

BATANI, DIMITRI, SABRINA BIAVA, SERGIO BITTANTI, and FABIO PREVIDI. "A cellular automaton model of laser–plasma interactions." Laser and Particle Beams 19, no. 4 (October 2001): 631–42. http://dx.doi.org/10.1017/s0263034601194103.

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This paper deals with the realization of a CA model of the physical interactions occurring when high-power laser pulses are focused on plasma targets. The low-level and microscopic physical laws of interactions among the plasma and the photons in the pulse are described. In particular, electron–electron interaction via the Coulomb force and photon–electron interaction due to ponderomotive forces are considered. Moreover, the dependence on time and space of the index of refraction is taken into account, as a consequence of electron motion in the plasma. Ions are considered as a fixed background. Simulations of these interactions are provided in different conditions and the macroscopic dynamics of the system, in agreement with the experimental behavior, are evidenced.

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32

Oinuma, Gaku, Gaurav Nayak, Yanjun Du, and Peter J. Bruggeman. "Controlled plasma–droplet interactions: a quantitative study of OH transfer in plasma–liquid interaction." Plasma Sources Science and Technology 29, no. 9 (September 4, 2020): 095002. http://dx.doi.org/10.1088/1361-6595/aba988.

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33

BINGHAM, R., L. O. SILVA, J. T. MENDONCA, P. K. SHUKLA, W. B. MORI, and A. SERBETO. "PLASMA WAKES DRIVEN BY NEUTRINOS, PHOTONS AND ELECTRON BEAMS." International Journal of Modern Physics B 21, no. 03n04 (February 10, 2007): 343–50. http://dx.doi.org/10.1142/s0217979207042112.

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There is considerable interest in the propagation dynamics of intense electron and photon neutrino beams in a background dispersive medium such as dense plasmas, particularly in the search for a mechanism to explain the dynamics of type II supernovae. Neutrino interactions with matter are usually considered as single particle interactions. All the single particle mechanisms describing the dynamical properties of neutrino's in matter are analogous with the processes involving single electron interactions with a medium such as Compton scattering, and Cerenkov radiation etc. However, it is well known that beams of electrons moving through a plasma give rise to a new class of processes known as collective interactions such as two stream instabilities which result in either the absorption or generation of plasma waves. Intense photon beams also drive collective interactions such as modulational type instabilities. In both cases relativistic electron beams of electrons and photon beams can drive plasma wakefields in plasmas. Employing the relativistic kinetic equations for neutrinos interacting with dense plasmas via the weak force we explore collective plasma streaming instabilities driven by Neutrino electron and photon beams and demonstrate that all three types of particles can drive wakefields.

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34

Sunkara, Mahendra Kumar. "Plasma-molten Metal and/or Liquid Interactions for Materials/Chemical Processing." ECS Meeting Abstracts MA2020-01, no. 17 (May 1, 2020): 1106. http://dx.doi.org/10.1149/ma2020-01171106mtgabs.

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Several grand challenges in energy storage and conversion need the discovery of functional materials that many agree will be composed of complex compositions at nanoscale. In this regard, plasma based materials processing has been shown to be promising for combinatorial techniques and scalable processing. The use of plasma oxidation of liquid precursors allows for creation of metastable complex oxide particles with compositional control.1 A number of examples will be discussed in which the above two techniques are currently being used for accelerating the development of a variety of catalysts including electrocatalysts and materials for storage applications. This talk will highlight our efforts to understand the role of plasmas under two categories: (a) the synergistic effects hydrogen and nitrogen plasma interactions with molten metals;2 and (b) the oxygen plasma-liquid droplet interactions.3 To gain insights into these mechanisms we have studied the interaction of hydrogen and nitrogen plasmas with low melting point metals, primarily with gallium. Absorption/desorption experiments as well as theoretical-computational calculations were performed. Experiments have shown an increment of adsorbed gaseous species into the molten metal in the presence of plasmas. In the case of oxygen plasma-liquid droplet interactions for creating complex oxides, the role of solvated electrons, oxygen radicals and heating effects will be discussed. Finally, the use of plasmas for achieving liquid phase epitaxial growth of GaN and related materials will be discussed.4 Author acknowledge primary funding support from NSF Solar Project (DMS 1125909), and NSF EPSCoR (1355438). References 1. P. Ajayi, S. Kumari, D. Jaramillo-Cabanzo, J. Spurgeon, J. Jasinski and M.K. Sunkara, “A rapid and scalable method for making mixed metal oxide alloys for enabling accelerated materials discovery”, J. of Materials Research, 31 (11), 1596-1607(2016) 2. L. Carreon, D.F. Jaramillo-Cabanzo, I. Chaudhuri, M. Menon and M.K. Sunkara, “Synergistic interactions of H2 and N2 with molten gallium in the presence of plasma”, Journal of Vacuum Science and Technology A, 36, 021303 (2018). 3. P. Ajayi, M. Z. Akram, W. H. Paxton, J. B. Jasinski and M. K. Sunkara, “Nucleation and Growth Mechanisms During Complex Oxide Formation Using Plasma Oxidation of Liquid Precursors”, Submitted (2019) 4. Jaramillo, J. Jasinski and M. Sunkara, “Liquid Phase Epitaxial Growth of Gallium Nitride”, Crystal Growth and Design, 19, 11, 6577-6585(2019)

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35

SETSUHARA, Yuichi. "Plasma Interactions with Soft Materials." Journal of The Surface Finishing Society of Japan 64, no. 12 (2013): 628–33. http://dx.doi.org/10.4139/sfj.64.628.

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36

Federici, G. "Plasma wall interactions in ITER." Physica Scripta T124 (April 27, 2006): 1–8. http://dx.doi.org/10.1088/0031-8949/2006/t124/001.

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37

Shukla, P. K., and B. Eliasson. "Collective nonlinear dust–plasma interactions." Plasma Physics and Controlled Fusion 49, no. 5A (March 29, 2007): A211—A220. http://dx.doi.org/10.1088/0741-3335/49/5a/s17.

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38

Uckan, Taner. "Plasma‐materials interactions test facility." Review of Scientific Instruments 58, no. 1 (January 1987): 17–19. http://dx.doi.org/10.1063/1.1139558.

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39

Parker, R. "Plasma-wall interactions in ITER." Journal of Nuclear Materials 241-243, no. 1 (February 11, 1997): 1–26. http://dx.doi.org/10.1016/s0022-3115(96)00491-6.

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40

Parker, R., G. Janeschitz, H. D. Pacher, D. Post, S. Chiocchio, G. Federici, and P. Ladd. "Plasma-wall interactions in ITER." Journal of Nuclear Materials 241-243 (February 1997): 1–26. http://dx.doi.org/10.1016/s0022-3115(97)80027-x.

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41

Jones, Jonathan C. R., and Kathleen J. Green. "Intermediate filament plasma membrane interactions." Current Opinion in Cell Biology 3, no. 1 (February 1991): 127–32. http://dx.doi.org/10.1016/0955-0674(91)90175-x.

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42

Chang, C. T. "Pellet-plasma interactions in tokamaks." Physics Reports 206, no. 4 (August 1991): 143–96. http://dx.doi.org/10.1016/0370-1573(91)90053-o.

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43

Gibbon, P., and E. Förster. "Short-pulse laser - plasma interactions." Plasma Physics and Controlled Fusion 38, no. 6 (June 1, 1996): 769–93. http://dx.doi.org/10.1088/0741-3335/38/6/001.

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44

Bourke, P., D. Ziuzina, L. Han, P. J. Cullen, and B. F. Gilmore. "Microbiological interactions with cold plasma." Journal of Applied Microbiology 123, no. 2 (June 22, 2017): 308–24. http://dx.doi.org/10.1111/jam.13429.

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45

Bastasz, R., and W. Eckstein. "Plasma–surface interactions on liquids." Journal of Nuclear Materials 290-293 (March 2001): 19–24. http://dx.doi.org/10.1016/s0022-3115(00)00557-2.

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46

Dylla, H. F., TFTR Team, M. G. Bell, W. R. Blanchard, P. P. Boody, N. Bretz, R. Budny, et al. "Plasma-material interactions in TFTR." Journal of Nuclear Materials 145-147 (February 1987): 48–60. http://dx.doi.org/10.1016/0022-3115(87)90309-6.

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47

Stancampiano, Augusto, Tommaso Gallingani, Matteo Gherardi, Zdenko Machala, Paul Maguire, Vittorio Colombo, Jean-Michel Pouvesle, and Eric Robert. "Plasma and Aerosols: Challenges, Opportunities and Perspectives." Applied Sciences 9, no. 18 (September 14, 2019): 3861. http://dx.doi.org/10.3390/app9183861.

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The interaction of plasmas and liquid aerosols offers special advantages and opens new perspectives for plasma–liquid applications. The paper focuses on the key research challenges and potential of plasma-aerosol interaction at atmospheric pressure in several fields, outlining opportunities and benefits in terms of process tuning and throughputs. After a short overview of the recent achievements in plasma–liquid field, the possible application benefits from aerosol injection in combination with plasma discharge are listed and discussed. Since the nature of the chemicophysical plasma-droplet interactions is still unclear, a multidisciplinary approach is recommended to overcome the current lack of knowledge and to open the plasma communities to scientists from other fields, already active in biphasic systems diagnostic. In this perspective, a better understanding of the high chemical reactivity of gas–liquid reactions will bring new opportunities for plasma assisted in-situ and on-demand reactive species production and material processing.

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48

Krasik, Yakov, John Leopold, Guy Shafir, Yang Cao, Yuri Bliokh, Vladislav Rostov, Valery Godyak, et al. "Experiments Designed to Study the Non-Linear Transition of High-Power Microwaves through Plasmas and Gases." Plasma 2, no. 1 (March 8, 2019): 51–64. http://dx.doi.org/10.3390/plasma2010006.

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The interaction of powerful sub-picosecond timescale lasers with neutral gas and plasmas has stimulated enormous interest because of the potential to accelerate particles to extremely large energies by the intense wakefields formed and without being limited by high accelerating gradients as in conventional accelerator cells. The interaction of extremely high-power electromagnetic waves with plasmas is though, of general interest and also to plasma heating and wake-field formation. The study of this subject has become more accessible with the availability of sub-nanosecond timescale GigaWatt (GW) power scale microwave sources. The interaction of such high-power microwaves (HPM) with under-dense plasmas is a scale down of the picosecond laser—dense plasma interaction situation. We present a review of a unique experiment in which such interactions are being studied, some of our results so far including results of our numerical modeling. Such experiments have not been performed before, self-channeling of HPM through gas and plasma and extremely fast plasma electron heating to keV energies have already been observed, wakefields resulting from the transition of HPM through plasma are next and more is expected to be revealed.

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49

Boyd, T. J. M. "Laser–plasma interaction physics in underdense coronal plasmas." Canadian Journal of Physics 64, no. 8 (August 1, 1986): 944–55. http://dx.doi.org/10.1139/p86-163.

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After a brief review of stimulated Raman scattering and two-plasmon decay, which dominate the physics of laser–plasma interactions at and below the quarter-critical density, we summarize some of the principal characteristics of emission from targets at half-harmonics of the laser frequency. Two mechanisms in particular are thought to contribute to the emission; Raman conversion and the direct linear conversion of plasmons generated by two-plasmon decay. Both processes are reviewed and the implications of each for the emission spectra examined.The effect of strong self-generated magnetic fields on harmonic generation is considered briefly and attention is drawn to ways in which the coincidence of interactions in the underdense plasma may influence their basic characteristics. A finite-amplitude ion wave, for example, modifies the spectrum of Raman scattered light, including significant frequency splitting.

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50

Rhee, Tongnyeol, Minho Woo, and Chang-Mo Ryu. "Simulation Study of Plasma Emission in Beam-Plasma Interactions." Journal of the Korean Physical Society 54, no. 9(5) (January 15, 2009): 313–16. http://dx.doi.org/10.3938/jkps.54.313.

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