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Journal articles on the topic 'Hydrogen bombardment'

Author: Grafiati

Published: 4 June 2021

Last updated: 1 February 2022

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1

Pisarev, A. A., A. V. Varava, V. M. Smirnov, and E. R. Dryanina. "Hydrogen recycling constant during ion bombardment." Journal of Nuclear Materials 176-177 (December 1990): 418–21. http://dx.doi.org/10.1016/0022-3115(90)90082-x.

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2

Zaluzhnyi, A. G., V. P. Kopytin, and M. V. Tcherednichenko-Alchevskiy. "Hydrogen penetration through structural materials during hydrogen ion bombardment." Fusion Engineering and Design 41, no. 1-4 (September 1998): 129–34. http://dx.doi.org/10.1016/s0920-3796(98)00129-x.

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3

Strauven, H., A. Stesmans, J. Winters, J. Spinnewijn, and O. B. Verbeke. "Hydrogen incorporation mechanisms in the preparation of a-Si:H by ion bombardment-activated reactive evaporation." Journal of Materials Research 3, no. 2 (April 1988): 335–43. http://dx.doi.org/10.1557/jmr.1988.0335.

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Here a-Si:H is prepared by ion bombardment-activated reactive evaporation of Si in a H2O residual gas pressure ranging from 10−9 to 10−7 Torr. The Si+ ions (2.7keV) are bombarding the substrate and the walls during evaporation. Two hydrogen incorporation mechanisms are revealed by H evolution experiments, depending on the H2O residual gas pressure during evaporation. In the first mechanism H is sputtered from the walls of the system by the ion bombardment; this mechanism contributes 10 at. % to the hydrogen content. In a second mechanism Si+ bombardment on the growing layer injects H from H2O molecules adsorbed on the film surface; at least 5 at. % H is incorporated by this process. The second mechanism has a remarkable influence on the microstructure as revealed from the electrical conductivity, electron spin resonance, and infrared transmission. Indeed, Si+ bombardment-induced injection of H changes the conductivity type from variable range hopping to an activated behavior, while the dangling bond density remains low (< 1018 cm −3). The growth of [SiH2]n bundles, observed by the resonance frequency and absorption strength of the stretch mode of the Si–H dipole, is also a consequence of the H injection mechanism. It is concluded that the properties of the a-Si:H, prepared by ion bombardment-activated reactive evaporation, are explained by a microstructure, dependent on the specific hydrogen incorporation mechanism.

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4

Larionov, V. V., N. N. Nikitenkov, and Yu I. Tyurin. "Hydrogen diffusion in steels under electron bombardment." Technical Physics 61, no. 5 (May 2016): 793–97. http://dx.doi.org/10.1134/s1063784216050133.

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5

Seager, C. H., R. A. Anderson, and J. K. G. Panitz. "The diffusion of hydrogen in silicon and mechanisms for “unintentional” hydrogenation during ion beam processing." Journal of Materials Research 2, no. 1 (February 1987): 96–106. http://dx.doi.org/10.1557/jmr.1987.0096.

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Experiments are described in which hydrogen is injected into silicon by various techniques and detected by the neutralization of boron acceptor sites. Wet chemical etching is shown to inject protons several microns in a few seconds; this experiment is used to set a lower limit on the diffusivity of hydrogen of ⋍2⊠10−11 cm2/s at 300 K, a number in reasonable agreement with prior estimates deduced by Van Wieririgen and Warmholtz from high-temperature permeation measurements. A number of experiments are reported to elucidate the mechanism for “unintentional” hydrogenation occurring during argon ion bombardment. The data suggest that this effect is caused by bombardment-induced injection of hydrogen from surface H2O/hydrocarbon contaminants.

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6

Zaluzhnyi, A. G., V. P. Kopytin, O. M. Storozhuk, and M. V. Tcherednichenko-Alchevskyi. "Hydrogen penetration through structural materials under ion bombardment." Journal of Nuclear Materials 233-237 (October 1996): 1148–53. http://dx.doi.org/10.1016/s0022-3115(96)00081-5.

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7

Som, Tapobrata, Sankar Dhar, Shiraz N. Minwalla, and Vishwas N. Kulkarni. "Hydrogen depletion from KH2PO4 under He+ ion bombardment." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 122, no. 2 (February 1997): 244–46. http://dx.doi.org/10.1016/s0168-583x(96)00777-x.

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8

Abdul-Kader, A. M., Andrzej Turos, Jacek Jagielski, Lech Nowicki, Renata Ratajczak, Anna Stonert, and Mariam A. Al-Ma’adeed. "Hydrogen release in UHMWPE upon He-ion bombardment." Vacuum 78, no. 2-4 (May 2005): 281–84. http://dx.doi.org/10.1016/j.vacuum.2005.01.039.

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9

Belyaeva, A. I., A. F. Bardamid, J. W. Davis, A. A. Haasz, V. G. Konovalov, A. D. Kudlenko, M. Poon, K. A. Slatin, and V. S. Voitsenya. "Hydrogen ion bombardment damage in stainless steel mirrors." Journal of Nuclear Materials 345, no. 2-3 (October 2005): 101–8. http://dx.doi.org/10.1016/j.jnucmat.2005.04.066.

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10

Lopes, J. L., J. A. Greer, and M. Seidl. "Sputtering of negative hydrogen ions by cesium bombardment." Journal of Applied Physics 60, no. 1 (July 1986): 17–23. http://dx.doi.org/10.1063/1.337800.

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11

Iwahashi, Hideki, Goroh Itoh, Katsuhiro Saitoh, and Takahiro Shikagawa. "Analysis on Behavior of Hydrogen in Ion-Plated Pure Aluminum." Advanced Materials Research 409 (November 2011): 47–50. http://dx.doi.org/10.4028/www.scientific.net/amr.409.47.

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An increasing interest has been being taken in hydrogen as a clean energy for solving the global environmental problems. In order to use the hydrogen in safety, investigation on the hydrogen behavior is required. Although hydrogen microprint technique (HMPT) has been known to be effective to investigate the hydrogen behavior, the low detection efficiency for hydrogen was reported. Ion-plating (IP) was reported to increase the detection efficiency in HMPT emitted from the specimen by plastic deformation. On the other hand, no such increase was found for hydrogen permeating through the specimen ion-plated with substrate heating in the previous study by the authors. In the present study, the sheet samples of pure aluminum with 99.99% purity were dehydrogenated and subjected to (a) holding in the IP chamber, (b) bombardment with Ar ions, (c) substrate heating after the bombardment and (d) holding in air. Hydrogen behavior in these samples has been investigated by means of thermal desorption spectroscopy (TDS). The amount of desorbed hydrogen was evidently larger in the conditions of (a) and (b) than in (d). However, the amount of desorbed hydrogen was decreased by the substrate heating (c) to the same level as in (d).

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12

Horn, M. W., J. M. Heddleson, and S. J. Fonash. "Permeation of hydrogen into silicon during low‐energy hydrogen ion beam bombardment." Applied Physics Letters 51, no. 7 (August 17, 1987): 490–92. http://dx.doi.org/10.1063/1.98376.

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13

Salonen, E., K. Nordlund, J. Tarus, T. Ahlgren, J. Keinonen, and C. H. Wu. "Suppression of carbon erosion by hydrogen shielding during high-flux hydrogen bombardment." Physical Review B 60, no. 20 (November 15, 1999): R14005—R14008. http://dx.doi.org/10.1103/physrevb.60.r14005.

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14

Zaluzhnyi, A. G., V. P. Kopytin, and O. M. Storozhuk. "Hydrogen permeability of polycrystalline nickel during the process of hydrogen-ion bombardment." Soviet Atomic Energy 65, no. 2 (August 1988): 648–52. http://dx.doi.org/10.1007/bf01270806.

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15

Shao, Hong, Xin Hu, Keqin Xu, Changyu Tang, Yuanlin Zhou, Maobing Shuai, Jun Mei, Yan Zhu, and Woon-ming Lau. "Enhanced water vapor barrier property of poly(chloro-p-xylylene) film by formation of dense surface cross-linking layer via hyperthermal hydrogen treatment." RSC Advances 5, no. 69 (2015): 55713–19. http://dx.doi.org/10.1039/c5ra07557b.

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16

Aboudarham, J., and J. C. Henoux. "Electron Beam as Origin of White-Light Solar Flares." International Astronomical Union Colloquium 104, no. 1 (1989): 19–30. http://dx.doi.org/10.1017/s025292110003178x.

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AbstractWe study the effect of chromospheric bombardment by an electron beam during solar flares. Using a semi-empirical flare model, we investigate energy balance at temperature minimum level and in the upper photosphere. We show that non-thermal hydrogen ionization (i.e., due to the electrons of the beam) leads to an increase of chromospheric hydrogen continuum emission, H− population, and absorption of photo-spheric and chromospheric continuum radiation. So, the upper photosphere is radiatively heated by chromospheric continuum radiation produced by the beam. The effect of hydrogen ionization is an enhanced white-light emission both at chromospheric and photospheric level, due to Paschen and H− continua emission, respectively. We then obtain white-light contrasts compatible with observations, obviously showing the link between white-light flares and atmospheric bombardment by electron beams.

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17

Brown, Stephen J., Jack M. Miller, Roger Theberge, and James H. Clark. "A fast atom bombardment mass spectrometry study of H-bonded complexes of imidazole with various electron donors." Canadian Journal of Chemistry 64, no. 7 (July 1, 1986): 1227–29. http://dx.doi.org/10.1139/v86-211.

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18

Kalantaryan, O. V., V. T. Kolesnik, S. I. Kononenko, V. I. Muratov, and V. E. Storizhko. "Silicon luminescence induced by bombardment with fast hydrogen ions." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 129, no. 1 (June 1997): 77–79. http://dx.doi.org/10.1016/s0168-583x(97)00158-4.

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19

Salonen, E., K. Nordlund, J. Keinonen, and C. H. Wu. "Chemical sputtering of amorphous silicon carbide under hydrogen bombardment." Applied Surface Science 184, no. 1-4 (December 2001): 387–90. http://dx.doi.org/10.1016/s0169-4332(01)00524-4.

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20

Verma, Sunita, Steven C. Pomerantz, Satinder K. Sethi, and James A. McCloskey. "Fast atom bombardment mass spectrometry following hydrogen-deuterium exchange." Analytical Chemistry 58, no. 14 (December 1986): 2898–902. http://dx.doi.org/10.1021/ac00127a002.

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21

Goebel, D. M., J. Bohdansky, R. W. Conn, Y. Hirooka, B. LaBombard, W. K. Leung, R. E. Nygren, J. Roth, and G. R. Tynan. "Erosion of graphite by high flux hydrogen plasma bombardment." Nuclear Fusion 28, no. 6 (June 1, 1988): 1041–52. http://dx.doi.org/10.1088/0029-5515/28/6/007.

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22

Kalin, B. A., V. L. Yakushin, V. I. Polsky, and Yu S. Virgilev. "Sputtering of surface-boronized graphite by hydrogen ion bombardment." Journal of Nuclear Materials 212-215 (September 1994): 1206–10. http://dx.doi.org/10.1016/0022-3115(94)91022-7.

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23

Bitensky, I., E. Parilis, S. Della-Negra, and Y. Le Beyec. "Emission of hydrogen ions under multiply charged ion bombardment." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 72, no. 3-4 (December 1992): 380–86. http://dx.doi.org/10.1016/0168-583x(92)95132-b.

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24

Okuyama, F., H. Muto, H. Tsujimaki, and Y. Fujimoto. "Palladium nanoparticles grown by hydrogen and deuterium ion bombardment." Surface Science 355, no. 1-3 (June 1996): L341—L344. http://dx.doi.org/10.1016/0039-6028(96)00511-0.

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25

Tsuge, Masashi, Chih-Yu Tseng, and Yuan-Pern Lee. "Spectroscopy of prospective interstellar ions and radicals isolated in para-hydrogen matrices." Physical Chemistry Chemical Physics 20, no. 8 (2018): 5344–58. http://dx.doi.org/10.1039/c7cp05680j.

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26

Abdul-Kader, A. M., and Andrzej Turos. "Ion Beam Induced Modifications of Biocompatible Polymer." Solid State Phenomena 239 (August 2015): 149–60. http://dx.doi.org/10.4028/www.scientific.net/ssp.239.149.

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Ion beam bombardment has shown great potential for improving the surface properties of polymers. In this paper, the ion beam-polymer interaction mechanisms are briefly discussed. The main objective of this research was to study the effects of H-ion beam on physico-chemical properties of Ultra-high-molecular-weight polyethylene (UHMWPE) as it is frequently used in biomedical applications. UHMWPE was bombarded with 65 keV H-ions to fluences ranging from 1x1014–2x1016 ions/cm2. Changes of surface layer composition produced by ion bombardment of UHMWPE samples were studied. The hydrogen release and oxygen uptake induced by ion beam bombardment were determined by Nuclear reaction analysis (NRA) using the 1H(15N, αγ)12C and Rutherford backscattering spectrometry (RBS), respectively. Tribological and hardness properties at the polymer near surface region were studied by means of friction coefficient and micro-hardness testers, respectively. Wettability of the bombarded surfaces was determined by measuring the contact angle for distilled water. The obtained results showed that the ion bombardment induced hydrogen release increases with the increasing ion fluence. An important effect observed, was the rapid oxidation of samples, which occurs after exposure of bombarded samples to air. These effects resulted in important modifications of the surface properties of bombarded material such as change of friction coefficient, hardness and improved wettability.

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27

Boutard, D., and W. Möller. "Isotopic effects in a–C:(H/D) films deposited from methane/hydrogen RF plasmas." Journal of Materials Research 5, no. 11 (November 1990): 2451–55. http://dx.doi.org/10.1557/jmr.1990.2451.

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Hard amorphous hydrocarbon films have been deposited by RF glow discharges in methane/hydrogen mixtures with different hydrogen isotopes. For CH4 + D2 and CD4 + H2 gas mixtures, the film growth rate, the density, the refractive index, and the isotopic hydrogen content are obtained as functions of the process gas composition. Further, the hydrogen loss induced by 15 keV helium ions is studied. The results are qualitatively interpreted in terms of different effects of ion bombardment during film deposition which influence the properties of the resulting films.

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28

Fang, C., Z. Xu, and M. D. Ding. "Diagnostics of Non-thermal Particles in Solar Chromospheric Flares." Symposium - International Astronomical Union 219 (2004): 171–75. http://dx.doi.org/10.1017/s0074180900182087.

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Particle beam bombardment on the solar chromosphere produces non-thermal ionization and excitation. The effect on hydrogen lines is investigated by using non-LTE theory and semi-empirical flare models. It has been found that in the case of electron bombardment, the Hα line is widely broadened and enhanced. Significant enhancements at the wings of Lyα and Lyβ lines are also predicted. In the case of proton bombardment, less strong broadening and less central reversal are expected. We found that the total energy flux of the particle beam and the atmospheric condition give much influence on the line profiles, which, however, are less sensitive to the power index. Based on the Hα line profile measurement, a method to deduce the total energy flux of the particle beam is proposed.

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29

Tsuge, Masashi, and Yuan-Pern Lee. "Infrared spectra of HSCS+, c-HSCS, and HCS2− produced on electron bombardment of CS2 in solid para-hydrogen." Physical Chemistry Chemical Physics 19, no. 14 (2017): 9641–53. http://dx.doi.org/10.1039/c7cp00988g.

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We report infrared spectra of HSCS⁺, c-HSCS, HCS₂⁻, and other species produced on electron bombardment of a mixture of CS₂ and para-hydrogen during deposition at 3.2 K.

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30

Tsuge, Masashi, Mohammed Bahou, Yu-Jong Wu, Louis Allamandola, and Yuan-Pern Lee. "Infrared spectra of ovalene (C32H14) and hydrogenated ovalene (C32H15˙) in solid para-hydrogen." Physical Chemistry Chemical Physics 18, no. 41 (2016): 28864–71. http://dx.doi.org/10.1039/c6cp05701b.

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31

Kushita, K. N., K. Hojou, S. Furuno, and H. Otsu. "In situ EELS observation of diamond during hydrogen-ion bombardment." Journal of Nuclear Materials 191-194 (September 1992): 346–50. http://dx.doi.org/10.1016/s0022-3115(09)80063-9.

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32

Brown, W. L., G. Foti, L. J. Lanzerotti, J. E. Bower, and R. E. Johnson. "Delayed emission of hydrogen from ion bombardment of solid methane." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 19-20 (January 1987): 899–902. http://dx.doi.org/10.1016/s0168-583x(87)80180-5.

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33

Okuyama, F., and H. Takamori. "Meltdown of palladium nanoparticles due to prolonged hydrogen ion bombardment." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 267, no. 5 (March 2009): 773–76. http://dx.doi.org/10.1016/j.nimb.2008.12.011.

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34

Zhurenko, Vitaliy P., Oganes V. Kalantaryan, and Sergiy I. Kononenko. "Change of silica luminescence due to fast hydrogen ion bombardment." Nukleonika 60, no. 2 (June 1, 2015): 289–92. http://dx.doi.org/10.1515/nuka-2015-0063.

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AbstractThis paper deals with the luminescence of silica (KV-type) induced by beam of hydrogen ions with the energy of 210 keV per nucleon. An average implantation dose of up to 3.5 × 1021cm−3(5 × 1010Gy) was accumulated during irradiation over an extended period. The luminescent spectra consisted of the blue band (maximum at 456 nm) and the red band (650 nm) in the visible range. It was shown that increase in the absorption dose had an effect on the silica luminescence. It was found that the most significant changes in the spectrum occurred during the dose accumulation in the region of 550–700 nm. The shape of the spectrum of the luminescent radiation in this wavelength range was affected both by the oxygen deficient centres (blue band) and non-bridging oxygen hole centers (red band). Mathematical processing of the experimental spectra permitted to identify contributions to the luminescent radiation coming from both types of defects.

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35

Lee, Chin Shuang, Yun Hueng Chen, and Ya Chun Liu. "The hydrogen radiation induced by OH2+ and H3+ ion bombardment." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 198, no. 1-2 (December 2002): 37–42. http://dx.doi.org/10.1016/s0168-583x(02)01383-6.

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36

Li, W., S. Sato, H. Akima, and M. Sakuraba. "Hydrogen Atom Desorption Induced by Electron Bombardment on Si Surface." ECS Transactions 69, no. 31 (December 28, 2015): 35–38. http://dx.doi.org/10.1149/06931.0035ecst.

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37

Nagai, Y., Y. Saito, and N. Matuda. "Hydrogen desorption from copper during ion bombardment measured by SIMS." Vacuum 47, no. 6-8 (June 1996): 737–39. http://dx.doi.org/10.1016/0042-207x(96)00147-9.

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38

Sugai, H., H. Toyoda, S. Ohshita, S. Yoshida, and A. Sagara. "Hydrogen recycling control by helium ion bombardment onto carbonized surfaces." Journal of Nuclear Materials 162-164 (April 1989): 1035–39. http://dx.doi.org/10.1016/0022-3115(89)90405-4.

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39

KUSHITA, K. "In situ EELS observation of diamond during hydrogen-ion bombardment." Journal of Nuclear Materials 191-194 (September 1992): 346–50. http://dx.doi.org/10.1016/0022-3115(92)90783-h.

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40

Yamamoto, T., S. Tsukui, S. Okuda, and Kouji Kawabata. "Driving Force of Hydrogen Up-Hill Migration Induced by Ion-Bombardment with Another Hydrogen Isotope." Defect and Diffusion Forum 95-98 (January 1993): 365–68. http://dx.doi.org/10.4028/www.scientific.net/ddf.95-98.365.

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41

Guo, Y. P., K. L. Lam, K. M. Lui, R. W. M. Kwok, and K. C. Hui. "Growth of diamond and diamond-like films using a low energy ion beam." Journal of Materials Research 13, no. 8 (August 1998): 2315–20. http://dx.doi.org/10.1557/jmr.1998.0323.

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Ion beam deposition provides an additional control of ion beam energy over the chemical vapor deposition methods. We have used a low energy ion beam of hydrogen and carbon to deposit carbon films on Si(100) wafers. We found that graphitic films, amorphous carbon films, and oriented diamond microcrystallites could be obtained separatedly at different ion beam energies. The mechanism of the formation of the oriented diamond microcrystallites was suggested to include three components: strain release after ion bombardment, hydrogen passivation of sp3 carbon, and hydrogen etching. Such a process can be extended to the heteroepitaxial growth of diamond films.

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42

Hirooka, Y., W. K. Leung, R. W. Conn, D. M. Goebel, B. Labombard, R. Nygren, and K. L. Wilson. "Hydrogen pumping and release by graphite under high‐flux plasma bombardment." Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films 6, no. 5 (September 1988): 2965–77. http://dx.doi.org/10.1116/1.575461.

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43

Krieger, K., and J. Roth. "Synergistic effects by simultaneous bombardment of tungsten with hydrogen and carbon." Journal of Nuclear Materials 290-293 (March 2001): 107–11. http://dx.doi.org/10.1016/s0022-3115(00)00611-5.

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44

Tsuchiya, B., K. Morita, S. Yamamoto, S. Nagata, N. Ohtsu, T. Shikama, and H. Naramoto. "Re-emission of hydrogen implanted into graphite by helium ion bombardment." Journal of Nuclear Materials 313-316 (March 2003): 274–78. http://dx.doi.org/10.1016/s0022-3115(02)01341-7.

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45

Taylor, Ramona S., and Barbara J. Garrison. "Hydrogen Abstraction Reactions in the Kiloelectronvolt Particle Bombardment of Organic Films." Journal of the American Chemical Society 116, no. 10 (May 1994): 4465–66. http://dx.doi.org/10.1021/ja00089a041.

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46

Brown, Ian M., and T. C. Sandreczki. "Hydrogen-atom bombardment of monomers and polymers: maleimides, bismaleimides, and succinimide." Macromolecules 23, no. 23 (November 1990): 4918–24. http://dx.doi.org/10.1021/ma00225a006.

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47

Kašparová, J., and P. Heinzel. "Diagnostics of electron bombardment in solar flares from hydrogen Balmer lines." Astronomy & Astrophysics 382, no. 2 (February 2002): 688–98. http://dx.doi.org/10.1051/0004-6361:20011599.

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48

Lomidze, M. A., S. L. Kanashenko, A. E. Gorodetsky, V. Kh Alimov, and A. P. Zakharov. "Evolution of hydrogen-containing traps in graphite under helium ion bombardment." Journal of Nuclear Materials 212-215 (September 1994): 1483–87. http://dx.doi.org/10.1016/0022-3115(94)91074-x.

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49

Rudolph, W., D. Grambole, R. Groetzschel, C. Heiser, F. Herrmann, P. Knothe, and C. Neelmeijer. "Hydrogen, oxygen and carbon losses during 15N bombardment of PMMA layers." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 33, no. 1-4 (June 1988): 803–7. http://dx.doi.org/10.1016/0168-583x(88)90687-8.

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50

Pirronello, Valerio. "On the Mechanism of H2 Formation in the Interstellar Medium." Symposium - International Astronomical Union 120 (1987): 167–69. http://dx.doi.org/10.1017/s0074180900153975.

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The problem of the formation of molecular hydrogen in interstellar clouds is revisited. the role played by cosmic ray bombardment under certain circumstances is considered mainly in the light of the low formation rate of H2 on grains due to the reduced mobility of adsorbed H atoms on their amorphous surfaces at interstellar temperatures.

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