Radiation Effects in Materials 2016
DOI: 10.5772/62731
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Ion Bombardment-Induced Surface Effects in Materials

Abstract: This chapter deals with the experimental research and computer simulation of low-and medium-energy (E 0 = 1-30 keV) ion collisions on the surface of a solid and of the accompanying effects, namely scattering, sputtering, and surface implantation. Experimental and computer simulation studies of low-energy (Е 0 = 80-500 eV) Cs + ions scattering on Ta, W, Re target surfaces and K + ions scattering on Ti, V, Cr target surfaces have been performed for more accurate definition of mechanism of scattering, with a purp… Show more

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Cited by 5 publications
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“…The lack of a zero resistance state is likely due to backscattering and ion implantation damaging YBCO structure from the angled ion beam. 28 If we assume elastic scattering, then the backscattering length estimate is the thickness of the scattering wall (photoresist + YBCO film thickness) × tan (ion beam incidence angle), that is, (1.5 μm) × tan(75°) = 5.6 μm. Because the scattering "wall" is not perpendicular to the substrate (SR in Figure 1a), the backscattering length would be even larger.…”
Section: ■ Sawtooth Ratchet Characterizationmentioning
confidence: 99%
“…The lack of a zero resistance state is likely due to backscattering and ion implantation damaging YBCO structure from the angled ion beam. 28 If we assume elastic scattering, then the backscattering length estimate is the thickness of the scattering wall (photoresist + YBCO film thickness) × tan (ion beam incidence angle), that is, (1.5 μm) × tan(75°) = 5.6 μm. Because the scattering "wall" is not perpendicular to the substrate (SR in Figure 1a), the backscattering length would be even larger.…”
Section: ■ Sawtooth Ratchet Characterizationmentioning
confidence: 99%