Development of comprehensive and integrated models for by Hassanein, A.; Morozov, V.; Argonne National Lab.; United

By Hassanein, A.; Morozov, V.; Argonne National Lab.; United States. Dept. of Energy.; United States. Dept. of Energy. Office of Scientific and Technical Information

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Extra resources for Development of comprehensive and integrated models for inertial fusion cavity dynamics

Example text

For hydrogen irradiation of carbon, the chemical sputtering significantly depends on the target temperature and the incident energy. As shown by Garcia-Rosales [18], chemical erosion yield reaches its maximum values around 800 K. At low ion energies (100 eV and less), the maximum decreases, and the temperature dependence becomes broader such that at room temperature the chemical sputtering yield may exceed the values of physical sputtering. Higher ion fluxes decrease the chemical sputtering. There is still no comprehensive understanding of the chemical sputtering mechanism.

F. Biggs and R. , Albuquerque, NM (1971). 43 22. F. Biggs and R. Lighthill, "Analytical Approximations for Total and Energy Absorption Cross Sections for Photon-Atom Scattering," SC-PR-720685, Sandia Nat. , Albuquerque, NM (1972). 23. A. Bethe, Ann. Phys, Leipzig, 5 (1930) 325. 24. F. Bloch, Ann. Phys, Leipzig, 16 (1933) 285. 25. J. Lindhard and M. Scharff, "Energy Dissipation by Ions in the keV Region," Phys. Rev 124 (1961) 128. 26. H. F. 3, ed. F. Ziegler, Pergamon, New York (1977) 27. F. Ziegler, "Helium Stopping Powers and Ranges in All Elements," The Stopping and Range of Ions in Matter, Vol.

As shown by Garcia-Rosales [18], chemical erosion yield reaches its maximum values around 800 K. At low ion energies (100 eV and less), the maximum decreases, and the temperature dependence becomes broader such that at room temperature the chemical sputtering yield may exceed the values of physical sputtering. Higher ion fluxes decrease the chemical sputtering. There is still no comprehensive understanding of the chemical sputtering mechanism. For hydrogen bombardment of carbon, Roth et al. 78 eV kT , where a1 − incident ion atomic mass in amu; T − temperature of graphite target, kT in eV; Γ 20 − specific flux of incident particles in 10 1 m ⋅s 2 .

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