1 edition of Sputtering of condensed gases by keV-electrons and ions found in the catalog.
Sputtering of condensed gases by keV-electrons and ions
|The Physical Object|
|Number of Pages||175|
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Sputtering of solid Ne with the hydrogen ions H + 1, H + 2 and H + 3 in the energy range 1–10 keV/atom has been studied by means of a quartz microbalance technique. No enhancement in the yield per atom for molecular ions was found.
The results for hydrogen ions are compared with data for keV by: Nuclear Instruments and Methods in Physics Research Sputtering of condensed gases by keV-electrons and ions book () North-Holland, Amsterdam Section VIIL Sputtering of condensed gases ELECTRONIC SPUTI'ERING OF SOLID ARGON AND KRYPTON BY keV HYDROGEN IONS J.
SCHOU, R. PEDRYS *, O. ELLEGAARD and H. SORENSEN Association Euratom- Riso National Laboratory, Riso National Laborato~.,Cited by: 3. Most sputtering is done by energetic sulfur ions (s of keV to MeV), but most of the O2 and H2 production is done by cold oxygen ions (temperature ˜ eV, total energy ˜ eV).
Abstract. A number of common features for the erosion of condensed gases by ion or electron bombardment are discussed. The overall pattern shows many similarities for erosion via electronic transitions induced by primary electrons and light by: 2.
The sputtering yield induced by keV hydrogen ions measured at CERN and at Risø National Laboratory for solid H2 and D2 at temperatures below K decreases with increasing film thickness from. Sputtering and Desorption from Icy Surfaces.
Authors; Authors and affiliations the study of the sputtering of surfaces composed of low- temperature condensed gases. Sputtering of such materials is of R.A., Pedrys, R., Oostra, D.J., Haring, A., de Vries, A.E.
(b) Reactive sputtering of simple condensed gases by keV ions II: Mass Cited by: Radiolysis of biomolecules by fast ions has interest in medical applications and astrobiology.
The radiolysis of solid D-valine (–2 μm thick) was performed at room temperature by MeV H+, He+, N+, and MeV S15+ ion beams. The samples were prepared by spraying/dropping valine-water-ethanol solution on ZnSe substrate.
Radiolysis was monitored by infrared spectroscopy (FTIR) through Author: Cíntia A. da Costa, Gabriel S. Vignoli Muniz, Philippe Boduch, Hermann Rothard, Enio F. da Silvei. The electron is a subatomic particle with a negative charge, equal to x t, or the rate of flow of charge, is defined such that one coulomb, so 1/x, or x10 18 electrons flowing past a point per second give a current of one charge on an electron is often given as -e.
note that charge is always considered positive, so the charge of an. This banner text can have markup. web; books; video; audio; software; images; Toggle navigation. How did life begin on Earth.
And is there life elsewhere in the Cosmos. Challenging questions, indeed. The series of conferences established by NoR CEL inaddresses these very same questions. The basis for this paper is the summary report of oral presentations that were delivered by NoR CEL’s network members during the Athens conference and, as such, disseminates the latest Cited by: 1.
Full text of "Processing and characterization of copper indium selenide for photovoltaic applications" See other formats. You can write a book review and share your experiences. Other readers will always be interested in your opinion of the books you've read.
Whether you've loved the book or not, if you give your honest and detailed thoughts then people will find new books that are right for them. Chapter 1 Basic Semiconductor Physics and Technology 44 Silicon nitride can be deposited using plasma-enhanced chemical vapour deposition (PECVD) or low-pressure chemical vapour deposition (LPCVD), using silane and ammonia gases NH 3, although the former is the technique of choice for glassivation purposes because it allows a lower processing.
The UNT Digital Library is a centralized repository for the rich collections held by the libraries, colleges, schools, and departments at the University of North Texas. In this study, we have fabricated nanofuses from thin-film, arc-deposited carbon for use in permanent data storage.
Thin-film carbon fuses have fewer fabrication barriers and retain the required resistivity and structural stability to act as a data-storage medium. Carbon thin films were characterized for their electrical, microstructural, and chemical bonding by: 1. The energy of the ions were varied from 50 keV to 80 keV to obtain the distribution of implanted ions in the silicon nanowire.
The simulation were also carried out using different straggling models. The presence of Fe and Co ions are expected to facilitate the formation of. Therefore we look at the energy dissipated by both 30 keV electrons and ions in a silicon substrate.
For simulating the eﬀect of energetic ions on matter a program called 2 For example for platinum, IBID and EBID as deposited purities are around. Experimental Beam Studies of Plasma-generated Species Interaction with Polymeric Materials and Biomolecules by Ting-Ying Chung A dissertation submitted in partial satisfaction of.
Egerton R.F. Electron Energy-Loss Spectroscopy in the Electron Microscope Egerton R.F. Electron Energy-Loss Spectroscopy in the Electron Microscope. Electron Energy-Loss Spectroscopy in theElectron MicroscopeThird Edition. R.F. EgertonElectron Energy-LossSpectroscopy in theElectron MicroscopeThird Edition The p a function is known with considerable accuracy for practically all neutral atoms and ions: for lighter atoms via Hartree-Fock methods, and for heavier atoms via the Thomas-Fermi approximation.
In Fig. (a) the / a functions for some atoms are shown. Physics at Surfaces is a unique introduction to the physics and chemical physics of solid surfaces, and atoms and molecules that interact with solid surfaces. This book provides a synthesis of the entire field of surface physics from the perspective of a modern condensed matter physicist with a healthy interest in chemical physics.
Physics Research Publications from the Research School of Physics and Engineering. From Molecules to Condensed Phases Springer, Netherlands () 28 keV electrons Nuclear Instruments and Methods in Physics Research: Section B () Hydrogen outgassing was induced by repeated pulses (60 s duration) of 60 keV electrons onto anode material samples and recording the H2 signal with a line of sight RGA.
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