Widely changing probability of surface damage creation induced by a single ion in the MeV ion energy range

Author(s):  
Hisato Ogiso
1991 ◽  
Vol 70 (10) ◽  
pp. 5623-5628 ◽  
Author(s):  
W. M. Lau ◽  
I. Bello ◽  
X. Feng ◽  
L. J. Huang ◽  
Qin Fuguang ◽  
...  

2020 ◽  
Author(s):  
Bin Li

<div>Low‐energy ions of ionospheric origin with energies below 10s of electron volt dominate most</div><div>of the volume and mass of the terrestrial magnetosphere. However, sunlit spacecraft often become</div><div>positively charged to several 10s of volts, which prevents low‐energy ions from reaching the particle</div><div>detectors on the spacecraft. Magnetospheric Multiscale spacecraft (MMS) observations show that</div><div>ultralow‐frequency (ULF) waves drive low‐energy ions to drift in the E × B direction with a drift velocity</div><div>equal to VE×B, and low‐energy ions were accelerated to suffificient total energy to be measured by the</div><div>MMS/Fast Plasma Investigation Dual Ion Spectrometers. The maximum low‐energy ion energy flflux peak</div><div>seen in MMS1's dual ion spectrometer measurements agreed well with the theoretical calculation of H+ ion</div><div>E × B drift energy. The density of ions in the energy range below minimum energy threshold was</div><div>between 1 and 3 cm−3 in the magnetosphere subsolar region in this event.</div>


1971 ◽  
Vol 49 (4) ◽  
pp. 480-482 ◽  
Author(s):  
H. Stocker ◽  
E. H. Berkowitz

The ratio, F2∞/F3∞, of equilibrium charge state fractions has been measured for 6Li2+,3+ ions in thin carbon foils and found to vary from 14%–1% over the ion energy range from 5.87–16.45 MeV. The measured ratio varies inversely with the fifth power of the ion velocity.


1988 ◽  
Vol 128 ◽  
Author(s):  
R. Burke ◽  
M. Guillermet ◽  
L. Vallier ◽  
E. Voisin

ABSTRACTThe Microwave Multipolar Plasma (MMP) offers unique features for plasma assisted deposition by combining multipolar magnetic confinement and microwave excitation. Independent control of the plasma-surface interaction parameters (neutral flux, ion flux and ion impact energy) has led to low temperature (400–800°C) silicon epitaxial growth in pure or H2 diluted silane MMPs.Prior to the epitaxial growth of Si, a plasma cleaning is applied to remove 0 and C atoms contaminant from the substrate surface. Ar and H2 were tested on 2 and 4 inch, (100) oriented, silicon wafers loaded “as received” and heated at the deposition temperature. The cleaning is effective in both cases giving a pure Si Auger spectrum. However, a LEED signature is only observed when operating at very low bias of the sample (low energy ions) and the lower the substrate temperature, the lower the energy allowed to obtain a LEED pattern. The cleaning process is also checked and inspected by post-deposition analyses, including TEM, RBS, SIMS and Secco etch.Various layer thicknesses were grown according to the characterization method. Specular epitaxial films are obtained for a large range of plasma and substrate parameters. The temperature may be as low as 400°C but the best results are obtained in the 600–700°C range. Interestingly, epitaxy is lost when the ion energy is increased. These results show a compromise between ion energy and substrate temperature. One needs to work at low ion energy to enhance the surface reaction while avoiding surface damage, but the temperature has to be sufficiently high to restructure the surface. Preliminary results on intentional doping reveal further potentialities of this low energy controlled interaction for low temperature plasma processing.


1969 ◽  
Vol 22 (11) ◽  
pp. 2275 ◽  
Author(s):  
NA McAskill

The ion-molecule reactions of ions in methyl chloride were studied in the gas phase at source pressures of up to 120 μ in a mass spectrometer using ions having exit energies which ranged from 0.2 to 2.0 eV. The ions produced by secondary processes included CH4Cl+, CH2Cl+, and C2H6Cl+. The rate constant for the reaction of CH3Cl+ was found to be independent of the ion energy in the energy range studied. A theoretical rate constant which is independent of the ion energy was also derived for reactions between ions and polar molecules. Negative ion spectra were briefly examined.


2010 ◽  
Vol 1265 ◽  
Author(s):  
Aurelien Debelle ◽  
Frederico Garrido ◽  
Lionel Thome

AbstractThe behavior of two nuclear materials, namely cubic zirconia and urania, is investigated under different irradiation conditions in the low and medium ion energy range (tens of keV to a few MeV). In each case, these materials display a multi-step damage build-up, as revealed by both RBS/C and XRD measurements. It is demonstrated that each step exhibits characteristic features such as damage fraction, elastic strain, nature of defects, and thus presents a specific microstructure. The transition from one step to the following involves radiation defect re-organization which arises to lower the energy of the system.


NANO ◽  
2017 ◽  
Vol 12 (08) ◽  
pp. 1750099
Author(s):  
Junho Yoon ◽  
Jeongyun Lee ◽  
Won Jong Yoo

During plasma etching for fin patterning in the three-dimensional (3D) FinFET structure, the exposure of the Si surface to plasma with reactive ions can induce physical damages, resulting in the degradation of electrical properties of the device. In this study, we evaluated the damage with a measurable value by simulation and surface damage analyses using HR-TEM and RBS. As a result, the degree of the damaged layer was strongly dependent on the energy of the ions bombarding the Si substrate during plasma etching. The damage was quantified with the interface defect density measured by the charge pumping method. Plasma etching with high ion energy showed approximately one order of magnitude higher defect density than that with low ion energy and/or wet etching with no ion bombardment. We introduced Si soft treatment (with very low ion energy) to remove the damaged layer. The Si soft treatment was very effective to remove the damage on a highly damaged silicon surface. However, the Si soft treatment itself increased the number of defects for a low damage silicon surface.


1966 ◽  
Vol 44 (1) ◽  
pp. 57-65 ◽  
Author(s):  
Masud Hussain ◽  
Larkin Kerwin

Ionization probability curves for Ar and Kr have been examined up to 1.5 eV above the ionization threshold using an electrostatic electron selector. Structure is observed between the Kr+ "ground" doublet levels and beyond the Ar+J = 1/2 level.Some of this structure is found to affect the 1001 collision cross section for these ions, which were measured in the primary ion energy range of 500–1 300 eV. The cross section for the J = 1/2 state is found to be larger than that for the J = 3/2 state in the case of Ar, while the reverse appears to be true for Kr.


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