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Journal articles on the topic 'High energy deposition'

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Author: Grafiati

Published: 14 March 2023

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1

Busza, W., and R. Ledoux. "Energy Deposition in High-Energy Proton-Nucleus Collisions." Annual Review of Nuclear and Particle Science 38, no. 1 (December 1988): 119–59. http://dx.doi.org/10.1146/annurev.ns.38.120188.001003.

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2

Taylor, R. D., A. W. Ali, and S. P. Slinker. "Energy deposition in O+by high‐energy electron beams." Journal of Applied Physics 66, no. 11 (December 1989): 5216–27. http://dx.doi.org/10.1063/1.343707.

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3

Fabris, D., G. Nebbia, G. Viesti, M. Lunardon, M. Cinausero, E. Fioretto, D. R. Napoli, et al. "Energy deposition in reactions at." Journal of Physics G: Nuclear and Particle Physics 23, no. 10 (October 1, 1997): 1377–82. http://dx.doi.org/10.1088/0954-3899/23/10/027.

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4

Desbois, J., O. Granier, and C. Ng�. "Critical energy deposition in nuclei." Zeitschrift f�r Physik A Atomic Nuclei 325, no. 2 (June 1986): 245–46. http://dx.doi.org/10.1007/bf01289659.

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5

Zheng-Ming, Luo, Gou Cheng-Jun, and Wolfram Laub. "The penetration, diffusion and energy deposition of high-energy photon." Chinese Physics 12, no. 7 (June 24, 2003): 803–8. http://dx.doi.org/10.1088/1009-1963/12/7/319.

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6

Meinander, K., K. Nordlund, and J. Keinonen. "Size dependent epitaxial cluster deposition: The effect of deposition energy." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 242, no. 1-2 (January 2006): 161–63. http://dx.doi.org/10.1016/j.nimb.2005.08.028.

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7

Wesch, W., A. Kamarou, and E. Wendler. "Effect of high electronic energy deposition in semiconductors." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 225, no. 1-2 (August 2004): 111–28. http://dx.doi.org/10.1016/j.nimb.2004.04.188.

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8

Chorush, Russell A., Ilan Vidavsky, and Fred W. McLafferty. "Surface-induced ion neutralization with high energy deposition." Organic Mass Spectrometry 28, no. 10 (October 1993): 1016–20. http://dx.doi.org/10.1002/oms.1210281008.

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9

Cai, Zilin, Feng Gao, Hongyu Wang, Cenrui Ma, and Thomas Yang. "Numerical Study on Transverse Jet Mixing Enhanced by High Frequency Energy Deposition." Energies 15, no. 21 (November 4, 2022): 8264. http://dx.doi.org/10.3390/en15218264.

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Supersonic incoming flow has a large momentum, which makes it difficult for transverse jets to have a large penetration depth due to the strong compression of the incoming flow. This impacts the mixing efficiency of the jet in the supersonic combustor. This paper proposes a method to improve the mixing efficiency of a rectangular flow field model using pulsed energy deposition, which is verified numerically. In the simulations, the Navier–Stokes equations with an energy source are solved to simulate the effects of energy deposition with various distributions on the fuel mixture. The results show that the energy deposition increases the turbulent kinetic energy, which enlarges the scale of the flow vortex and improves the fuel mixing performance. The energy deposition is distributed upstream and significantly improves the mixing performance. Energy deposition can improve the penetration depth of fuel, which is more significant when the energy deposition is distributed downstream of the jet orifice. The energy deposition also slightly reduces the total pressure recovery coefficient. In general, an energy deposition that is distributed upstream of the jet has the best effect on the mixing efficiency.

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10

Huizenga, H., and P. R. M. Storchi. "Numerical calculation of energy deposition by broad high-energy electron beams." Physics in Medicine and Biology 34, no. 10 (October 1, 1989): 1371–96. http://dx.doi.org/10.1088/0031-9155/34/10/003.

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11

Huizenga, H., and P. R. M. Storchi. "Numerical calculation of energy deposition by broad high-energy electron beams." Physics in Medicine and Biology 35, no. 10 (October 1, 1990): 1445. http://dx.doi.org/10.1088/0031-9155/35/10/508.

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12

Taylor, R. D., S. P. Slinker, and A. W. Ali. "Energy deposition in N and N+by high‐energy electron beams." Journal of Applied Physics 64, no. 3 (August 1988): 982–93. http://dx.doi.org/10.1063/1.341806.

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13

Ur Rahman, N., L. Capuano, S. Cabeza, M. Feinaeugle, A. Garcia-Junceda, M. B. de Rooij, D. T. A. Matthews, G. Walmag, I. Gibson, and G. R. B. E. Römer. "Directed energy deposition and characterization of high-carbon high speed steels." Additive Manufacturing 30 (December 2019): 100838. http://dx.doi.org/10.1016/j.addma.2019.100838.

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14

Schaible, Jonathan, David Hausch, Thomas Schopphoven, and Constantin Häfner. "Deposition strategies for generating cuboid volumes using extreme high-speed directed energy deposition." Journal of Laser Applications 34, no. 4 (November 2022): 042034. http://dx.doi.org/10.2351/7.0000770.

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Extreme high-speed directed energy deposition (EHLA) is a variant of directed energy deposition (DED-LB) developed at Fraunhofer ILT in cooperation with RWTH Aachen University. Because of a powder gas jet setup that is aimed at melting particles in the laser beam before they enter the melting pool, high process speeds of up to several hundred meters per minute and a layer thickness as thin as 25 μm can be achieved. EHLA is generally applied for rotationally symmetric coating applications. In previous experiments on a prototype machine of ponticon GmbH, EHLA was used for building up dense volumes, thus qualifying its use for additive manufacturing, now termed EHLA 3D. In this work, using iron-base alloy 1.4404 and a process speed of 40 m/min, cubic volumes are produced with EHLA 3D. Different deposition strategies commonly used in DED-LB are tested for their transferability to EHLA 3D. The results of different deposition strategies achieving the best near net shape geometry are shown in comparison to DED-LB. Furthermore, the influence of the deposition strategy and used technology on thermal management and microstructure are investigated. The best near net shape is achieved in this comparison using a contour-hatch strategy with 1.5 contours per layer and a 90° rotation of the hatch, both for EHLA and DED-LB. The microstructure of EHLA 3D built cubes is more similar to a typical laser powder bed fusion microstructure than to a typical DED-LB microstructure with respect to grain size and structure.

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15

Klauser-Baumgärtner, Detlef, Thomas Reichel, and John-Are Hansen. "Regional paleodepositional environment of the Cretaceous in the Great Australian Bight – a support for frontier exploration." APPEA Journal 59, no. 2 (2019): 891. http://dx.doi.org/10.1071/aj18055.

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To reveal the development of the depositional environment in the Great Australian Bight, regional and high-resolution 3D-seismic interpretation and palynological evidence from well data was integrated with tectonic plate- and paleo topographical-reconstructions. Results from that work explain the drainage patterns and changes in the sedimentary evolution. A maximum transgression at the Cenomanian–Turonian boundary causes the deposition of the expected main source rock interval at the base of the Tiger mega-sequence. This is supported by Integrated Ocean Drilling Program wells (2017), asphalite strandings and dredge samples from the basin. A relative sea-level drop in the mid-Turonian initiates a forced regression and sand deposition in more distal parts of the basin. As a third mega-sequence the Hammerhead Formation progrades into the basin, depositing several thousand metres of deltaic sandstones and lagoonal shales. Our source to sink model based on our gross depositional environment maps could explain the presence of source rocks and reservoir intervals within this frontier exploration basin.

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16

Suschke, Konrad, René Hübner, Peter Murmu, Prasanth Gupta, John Futter, and Andreas Markwitz. "High Energy Radial Deposition of Diamond-Like Carbon Coatings." Coatings 5, no. 3 (July 24, 2015): 326–37. http://dx.doi.org/10.3390/coatings5030326.

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17

Xia, Xianming, Cheng‐Feng Du, Shien Zhong, Yu Jiang, Hong Yu, Wenping Sun, Hongge Pan, Xianhong Rui, and Yan Yu. "Homogeneous Na Deposition Enabling High‐Energy Na‐Metal Batteries." Advanced Functional Materials 32, no. 10 (November 24, 2021): 2110280. http://dx.doi.org/10.1002/adfm.202110280.

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18

Wallace, Jon M. "Nonlocal Energy Deposition in High-Intensity Laser-Plasma Interactions." Physical Review Letters 55, no. 7 (August 12, 1985): 707–10. http://dx.doi.org/10.1103/physrevlett.55.707.

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19

Dellasega, D., V. Russo, A. Pezzoli, C. Conti, N. Lecis, E. Besozzi, M. Beghi, C. E. Bottani, and M. Passoni. "Boron films produced by high energy Pulsed Laser Deposition." Materials & Design 134 (November 2017): 35–43. http://dx.doi.org/10.1016/j.matdes.2017.08.025.

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20

Gorbunov, S. A., N. A. Medvedev, P. N. Terekhin, and A. E. Volkov. "Electron–lattice coupling after high-energy deposition in aluminum." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 354 (July 2015): 220–25. http://dx.doi.org/10.1016/j.nimb.2014.11.053.

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21

Knight, Doyle, and Nadia Kianvashrad. "Review of Energy Deposition for High-Speed Flow Control." Energies 15, no. 24 (December 19, 2022): 9645. http://dx.doi.org/10.3390/en15249645.

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Energy deposition for flow and flight control has received significant interest in the past several decades due to its potential application to high-speed flow and flight control. This paper reviews recent progress and recommends future research.

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22

Lee, E. M., G. W. Shin, K. Y. Lee, H. S. Yoon, and D. S. Shim. "Study of High Speed Steel AISI M4 Powder Deposition using Direct Energy Deposition Process." Transactions of Materials Processing 25, no. 6 (December 1, 2016): 353–58. http://dx.doi.org/10.5228/kstp.2016.25.6.353.

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23

Siva Prasad, Himani, Frank Brueckner, and Alexander F. H. Kaplan. "Powder incorporation and spatter formation in high deposition rate blown powder directed energy deposition." Additive Manufacturing 35 (October 2020): 101413. http://dx.doi.org/10.1016/j.addma.2020.101413.

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24

Liu, Yang, Zhen Ni Xing, and Guo Zheng Zhu. "Low-Flux Neutron Radiation Detection Technology with High Sensitivity." Applied Mechanics and Materials 668-669 (October 2014): 924–27. http://dx.doi.org/10.4028/www.scientific.net/amm.668-669.924.

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Boron-containing plastic scintillator detectors have a high detection efficiency for low-intensity thermal neutrons and fast neutrons which is currently the preferred types of neutron detector. This article is based on Monte Carlo method, studied boron-containing plastic scintillator for neutron detection performance, and analysis the energy deposition flux characteristics and detection efficiency when low intensity fission neutron incident to the boron plastic scintillator. We obtain the low-flux neutron detector performance in a variety of neutron source energy, boron-containing plastic scintillator diameter and length. Results showed that, when the boron-containing plastic scintillator lengths increase, the energy deposition flux will increase. When the length and diameter is constant, increasing source strength can increase the energy deposition flux brought by the recoil proton to a certain extent. When the source intensity over after thermal neutrons, due to the decrease of the cross section, the energy deposition fluxes brought by the react of neutrons and will decrease. The results provide help for low intensity fission neutron radiation detection technology with high sensitivity.

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25

Ali, Syed Haroon, Osman M. Abdullatif, Lamidi O. Babalola, Fawwaz M. Alkhaldi, Yasir Bashir, S. M. Talha Qadri, and Ali Wahid. "Sedimentary facies, depositional environments and conceptual outcrop analogue (Dam Formation, early Miocene) Eastern Arabian Platform, Saudi Arabia: a new high-resolution approach." Journal of Petroleum Exploration and Production Technology 11, no. 6 (May 15, 2021): 2497–518. http://dx.doi.org/10.1007/s13202-021-01181-7.

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AbstractThis paper presents the facies and depositional environment of the early Miocene Dam Formation, Eastern Arabian platform, Saudi Arabia. Deposition of Dam Formation (Fm.) was considered as a restricted shallow marine deposition. Few studies suggest the role of sea-level change in its deposition but were without decisive substantiation. Here, we describe the facies and high-resolution model of Dam Fm. under varying depositional conditions. The depositional conditions were subjected to changing relative sea level and tectonics. High-resolution outcrop photographs, sedimentological logs, and thin sections present that the mixed carbonate–siliciclastic sequence was affected by a regional tectonics. The lower part of Dam Fm. presents the development of carbonate ramp conditions that are represented by limestones and marl. The depositional conditions fluctuated with the fall of sea level, and uplift in the region pushed the siliciclastic down-dip and covered the whole platform. The subsequent rise in sea level was not as pronounced and thus allowed the deposition of microbial laminites and stromatolitic facies. The southeast outcrops, down-dip, are more carbonate prone as compared to the northwest outcrop, which allowed the deposition of siliciclastic-prone sedimentation up-dip. All facies, architecture, heterogeneity, and deposition were controlled by tectonic events including uplift, subsidence, tilting, and syn-sedimentary faulting, consequently affecting relative sea level. The resulting conceptual outcrop model would help to improve our understanding of mixed carbonate–siliciclastic systems and serve as an analogue for other stratigraphic units in the Arabian plate and region. Our results show that Dam Fm. can be a good target for exploration in the Northern Arabian Gulf.

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26

Saha, Janapriya, Paul Wilson, Peter Thieberger, Derek Lowenstein, Minli Wang, and Francis A. Cucinotta. "Biological Characterization of Low-Energy Ions with High-Energy Deposition on Human Cells." Radiation Research 182, no. 3 (August 6, 2014): 282. http://dx.doi.org/10.1667/rr13747.1.

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27

Bocchetta, Patrizia, Domenico Frattini, Miriana Tagliente, and Filippo Selleri. "Electrochemical Deposition of Polypyrrole Nanostructures for Energy Applications: A Review." Current Nanoscience 16, no. 4 (August 20, 2020): 462–77. http://dx.doi.org/10.2174/1573413715666190717113600.

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By collecting and analyzing relevant literature results, we demonstrate that the nanostructuring of polypyrrole (PPy) electrodes is a crucial strategy to achieve high performance and stability in energy devices such as fuel cells, lithium batteries and supercapacitors. In this critic and comprehensive review, we focus the attention on the electrochemical methods for deposition of PPy, nanostructures and potential applications, by analyzing the effect of different physico-chemical parameters, electro-oxidative conditions including template-based or template-free depositions and cathodic polymerization. Diverse interfaces and morphologies of polymer nanodeposits are also discussed.

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28

Bursill, L. A., Peng JuLin, V. N. Gurarie, A. V. Orlov, and S. Prawer. "Carbon nitride films produced by high-energy shock plasma deposition." Journal of Materials Research 10, no. 9 (September 1995): 2277–85. http://dx.doi.org/10.1557/jmr.1995.2277.

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High-energy shock plasma deposition techniques are used to produce carbon-nitride films containing both crystalline and amorphous components. The structures are examined by high-resolution transmission electron microscopy, parallel-electron-energy loss spectroscopy, and electron diffraction. The crystalline phase appears to be face-centered cubic with a unit cell parameter approx. a = 0.63 nm, and it may be stabilized by calcium and oxygen at about 1–2 at. % levels. 85 at. % of the carbon atoms appear to have trigonal bonding for the crystalline phase, the remaining 15 at.% having tetrahedral bonding. The amorphous carbon-nitride film component varies from essentially nanocrystalline graphite, containing virtually no nitrogen, to amorphous carbon-nitride containing up to 10 at. % N, where the fraction of sp3 bonds ranges up to approx. 85 at. %. There is PEELS evidence that the nitrogen atoms have sp2 trigonal bonds in both the amorphous and crystalline phases.

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29

Tsukakoshi, Osamu, Saburo Shimizu, Seiji Ogata, Naruyasu Sasaki, and Hiroyuki Yamakawa. "A high-current low-energy multi-ion beam deposition system." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 55, no. 1-4 (April 1991): 355–58. http://dx.doi.org/10.1016/0168-583x(91)96193-o.

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30

Arnault, J. C., J. Delafond, C. Templier, J. Chaumont, and O. Enea. "First stages study of high energy ion beam assisted deposition." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 80-81 (January 1993): 1384–87. http://dx.doi.org/10.1016/0168-583x(93)90804-f.

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31

Rao, D. S., and K. J. McCracken. "Effect of feed intake on protein and energy retention of boars of high genetic potential for lean growth." Proceedings of the British Society of Animal Production (1972) 1990 (March 1990): 92. http://dx.doi.org/10.1017/s0308229600018730.

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The daily rate of lean deposition achieved by growing pigs is a function of a wide range of factors including genotype, gender, liveweight and intake of energy/protein. The review of ARC (1981) highlighted the controversy surrounding the effects of liveweight and energy intake on lean deposition. Recent publications suggest that there are interactions between these factors and also with genotype. In contrast to the linear/plateau relationship between energy intake and protein deposition proposed by Whittemore and Fawcett (1976), Campbell and Taverner (1988) observed a linear response in protein deposition up to the highest energy intake achieved, with pigs of improved genotype. The slope of the relationship was much greater than that observed in previous studies (ARC 1981). In a recent experiment, McCracken and Rao (1989) have shown that high-lean pedigree boars can achieve protein deposition rates as high as 200 g/d over the liveweight range of 33 to 88 kg. At present there is no published information on the response of such pigs to energy intake though the low rates of fat deposition observed suggest that energy intake could be limiting protein deposition. The experiment described below was designed to measure the response of protein deposition to energy intake at a series of liveweights between 33 and 88 kg. The diet and the treatments were chosen to obtain a wide range of energy intakes above and below those observed with dry, pelleted diets.

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32

Mitsuishi, K., Z. Q. Liu, M. Shimojo, M. Han, and K. Furuya. "Dynamic profile calculation of deposition resolution by high-energy electrons in electron-beam-induced deposition." Ultramicroscopy 103, no. 1 (April 2005): 17–22. http://dx.doi.org/10.1016/j.ultramic.2004.11.011.

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33

Tekumalla, Sravya, Riccardo Tosi, Xipeng Tan, and Matteo Seita. "Directed energy deposition and characterization of high‐speed steels with high vanadium content." Additive Manufacturing Letters 2 (April 2022): 100029. http://dx.doi.org/10.1016/j.addlet.2022.100029.

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34

OKAMOTO, Erika, Kengo AIZAWA, Hideki AOYAMA, Masahiro UEDA, and Kazuo YAMAZAKI. "Development of High-accuracy, High-efficiency, and High-quality Modeling System Using Direct Energy Deposition." Journal of the Japan Society for Precision Engineering 88, no. 5 (May 5, 2022): 409–14. http://dx.doi.org/10.2493/jjspe.88.409.

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35

Debelle, A., G. Gutierrez, A. Boulle, I. Monnet, and L. Thomé. "Effect of energy deposition on the disordering kinetics in dual-ion beam irradiated single-crystalline GaAs." Journal of Applied Physics 132, no. 8 (August 28, 2022): 085905. http://dx.doi.org/10.1063/5.0096764.

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The damage induced in GaAs crystals irradiated with dual-ion beam (low-energy I2+ and high-energy Fe9+), producing simultaneous nuclear ( Sn) and electronic ( Se) energy depositions, was investigated using several characterization techniques. Analysis of the damage buildup shows that Sn alone (single 900 keV ion beam) leads, in a two-step process, to full amorphization of the irradiated layer (at a fluence of 1.5 nm−2) and to the development of a high (2.2%) elastic strain. Conversely, only one step in the disordering process is observed upon dual-ion beam irradiation (i.e., 900 keV I2+ and 27 MeV Fe9+, Sn& Se); hence, amorphization is prevented and the elastic strain remains very weak (below 0.2%). These results provide a strong evidence that, in GaAs, the electronic energy deposition can induce an efficient dynamic annealing of the damage created in collision cascades formed during nuclear energy deposition.

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36

Azziz, N., H. H. K. Tang, and G. R. Srinivasan. "A microscopic model of energy deposition in silicon slabs exposed to high‐energy protons." Journal of Applied Physics 62, no. 2 (July 15, 1987): 414–18. http://dx.doi.org/10.1063/1.339813.

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37

Huijsmans, G. T. A., and A. Loarte. "Non-linear MHD simulation of ELM energy deposition." Nuclear Fusion 53, no. 12 (November 26, 2013): 123023. http://dx.doi.org/10.1088/0029-5515/53/12/123023.

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38

Kim, Kang-Hyung, Chan-Hyun Jung, Dae-Yong Jeong, and Soong-Keun Hyun. "Preventing Evaporation Products for High-Quality Metal Film in Directed Energy Deposition: A Review." Metals 11, no. 2 (February 19, 2021): 353. http://dx.doi.org/10.3390/met11020353.

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Directed energy deposition (DED), a type of additive manufacturing (AM) is a process that enables high-speed deposition using laser technology. The application of DED extends not only to 3D printing, but also to the 2D surface modification by direct laser-deposition dissimilar materials with a sub-millimeter thickness. One of the reasons why DED has not been widely applied in the industry is the low velocity with a few m/min, but thin-DED has been developed to the extent that it can be over 100 m/min in roller deposition. The remaining task is to improve quality by reducing defects. Thus far, defect studies on AM, including DED, have focused mostly on preventing pores and crack defects that reduce fatigue strength. However, evaporation products, fumes, and spatters, were often neglected despite being one of the main causes of porosity and defects. In high-quality metal deposition, the problems caused by evaporation products are difficult to solve, but they have not yet caught the attention of metallurgists and physicists. This review examines the effect of the laser, material, and process parameters on the evaporation products to help obtain a high-quality metal film layer in thin-DED.

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39

Olson, R. E. "Energy deposition by energetic heavyions in matter." Radiation Effects and Defects in Solids 110, no. 1-2 (October 1989): 1–5. http://dx.doi.org/10.1080/10420158908214151.

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40

Bret, A., A. R. Piriz, and N. A. Tahir. "Imprint reduction in rotating heavy ions beam energy deposition." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 733 (January 2014): 200–202. http://dx.doi.org/10.1016/j.nima.2013.05.069.

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41

Kadri, O., V. N. Ivanchenko, F. Gharbi, and A. Trabelsi. "GEANT4 simulation of electron energy deposition in extended media." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 258, no. 2 (May 2007): 381–87. http://dx.doi.org/10.1016/j.nimb.2007.02.088.

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42

Auricchio, Mayara Maria Beltani, Paulo Roberto Mei, and Osmar Roberto Bagnato. "Soldering of silicon to Invar for double-crystal monochromators." Journal of Synchrotron Radiation 26, no. 5 (August 23, 2019): 1565–71. http://dx.doi.org/10.1107/s1600577519008191.

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At the Brazilian Synchrotron Light Laboratory (LNLS), new double-crystal monochromators are under development for use at the new Brazilian fourth-generation synchrotron, Sirius. The soldering technique used for the double-crystal monochromators ensures the union of monocrystalline silicon with FeNi alloy, Invar36 (64Fe–36Ni) from Grupo Metal and Invar39 (61Fe–39Fe) from Scientific Alloys, through SnSb (92.8Sn–7.2Sb), SnCu (Sn–0.3Cu) and SnBiCu (Sn–1.4Bi–0.7Cu) alloys from Nihon Superior. Following soldering tests and quantitative analysis, the Invar39/SnBiCu/Si samples were selected using base materials coated with different depositions – gold and copper. X-ray diffraction identified the formation of intermetallic compounds, such as AuSn2 and AuSn4 in base materials coated with gold and Cu3Sn and Cu6Sn5 with copper. Before thermal cycling, the average force obtained in shear tests was 1131 N with copper deposition and 499 N with gold deposition. After five consecutive thermal cycles from room temperature down to cryogenic temperature (−196.15°C), specimens with gold deposition presented cracks in the interface region and those with copper deposition showed no defects. Based on this, qualitative and semi-quantitative analyses of specimens with copper deposition were carried out by scanning electron microscopy and energy-dispersive spectroscopy techniques to identify the composition, distribution and morphology of the elements.

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43

Kim, Chan Kyu, Jae Il Jeong, Si Geun Choi, Jong Hyoung Kim, and Young Tae Cho. "High-throughput directed energy deposition process with an optimized scanning nozzle." Journal of Materials Processing Technology 295 (September 2021): 117165. http://dx.doi.org/10.1016/j.jmatprotec.2021.117165.

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44

Sun Shizhuang, 孙诗壮, 金春水 Jin Chunshui, 喻波 Yu Bo, 郭涛 Guo Tao, 姚舜 Yao Shun, 李春 Li Chun, and 邓文渊 Deng Wenyuan. "Reflection and Resputtering of Mo/Si Atoms During High-Energy Deposition." Acta Optica Sinica 40, no. 11 (2020): 1102001. http://dx.doi.org/10.3788/aos202040.1102001.

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45

Knight, D. "Survey of Aerodynamic Drag Reduction at High Speed by Energy Deposition." Journal of Propulsion and Power 24, no. 6 (November 2008): 1153–67. http://dx.doi.org/10.2514/1.24595.

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46

Deshpande, N. G., Y. G. Gudage, J. C. Vyas, F. Singh, and Ramphal Sharma. "Studies on the high electronic energy deposition in polyaniline thin films." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 266, no. 9 (May 2008): 2002–8. http://dx.doi.org/10.1016/j.nimb.2008.03.087.

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Boschker, Jos E., Erik Folven, Åsmund F. Monsen, Erik Wahlström, Jostein K. Grepstad, and Thomas Tybell. "Consequences of High Adatom Energy during Pulsed Laser Deposition of La0.7Sr0.3MnO3." Crystal Growth & Design 12, no. 2 (January 11, 2012): 562–66. http://dx.doi.org/10.1021/cg201461a.

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Zemek, J., F. Černý, M. Závětová, M. Vaněček, and V. Železný. "Silicon nitride films prepared by high energy ion beam enhanced deposition." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 86, no. 3-4 (April 1994): 293–97. http://dx.doi.org/10.1016/0168-583x(94)95292-2.

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Maliy, Liubov, Anatoliy Mamaev, and Vera Mamaeva. "Electrochemical high-energy deposition of CdSe nanostructures: modelling, synthesis and characterization." Journal of Applied Electrochemistry 47, no. 9 (July 21, 2017): 1073–82. http://dx.doi.org/10.1007/s10800-017-1106-x.

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Hatch, Spencer M., James LaBelle, William Lotko, Christopher C. Chaston, and Binzheng Zhang. "IMF Control of Alfvénic Energy Transport and Deposition at High Latitudes." Journal of Geophysical Research: Space Physics 122, no. 12 (December 2017): 12,189–12,211. http://dx.doi.org/10.1002/2017ja024175.

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