By W. Buckel, B. Stritzker (auth.), S. T. Picraux, E. P. EerNisse, F. L. Vook (eds.)
Conferences were held long ago on atomic collision phenomena and at the purposes of ion beams to semiconductors. although, in the earlier 12 months it grew to become obvious that there's a transforming into new zone of lively examine concerning using ion beams to change and learn the elemental houses of metals. hence a topical convention was once geared up to compile for the 1st time scientists with a variety of backgrounds and pursuits concerning this box. This booklet comprises the continue ings of the foreign convention on purposes of Ion Beams to Metals which used to be held in Albuquerque, New Mexico, October 2-4, 1973. a lot of the paintings offered herein represents principles and ideas that have had very little prior publicity within the open literature. the appliance of ion beams to superconducting prop erties for instance is sort of new, as is the bankruptcy on ion triggered floor reactions, which include basically oxidation and corrosion reports of implanted fabrics. those parts, in addition to the bankruptcy on implantation alloy formation, point out vital destiny components of the applying of ion beams to metals. A interpreting of the chapters on superconductivity and on oxida tion and corrosion can serve to convey one brand new on approximately the entire present info in those components of the ion beam mod ification of metals. A huge standpoint of the oxidation sector is given within the invited paper through G. Dearnaley.
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D. Ryan using D. K. Brice, RASE3 and DAMG2: Routines for Ion Implantation Calculations, Sandia Laboratories Report SLA-73-04l6 (April 1973). Diffusion effects at the irradiation temperature have not been taken into account. B. A. Loomis, A. Taylor, T. E. Klippert and S. B. Gerber, Proc. Int. Conf. C. Metals and their Alloys", R. J. Arsenault (editor), Nuclear Metallurgy, vol. 332. J. E. Crow, M. Strongin, R. S. Thompson and O. F. Kammerer. Phys. Letters, 30 A (1969) 161; W. De Sorbo. Phys. , 132 (1963) 107.
If c If I! 0 200 Implantation - Energies Ej 400 600 800 1000 1200 1400 A Penetration Depth Rp Figure 2. Total ion distribution for different implantation rates: NO(E i ) n ~ Ei ' the exponent n being varied as indicated. SUPERCONDUCTING PROPERTIES OF DILUTE MAGNETIC AllOYS for different values of n. implantation rate It is concluded that a constant leads to a constant ion distribution over part of the target-depth. The gradual decrease at high ranges is due to the increasing width of the Gaussian curves.
A: Yes, and we still do. Rutherford backscattering experiments are scheduled to study the interface. However, this problem does not affect the critical temperature results, since the highest T layer shorts the possible lower Tc layers. Also, note that the c transition on the (R,T) curve is sharp, indicating reasonable homogeneity. SUPERCONDUCTING NIOBIUM THIN FILMS 33 Q: (K. L. Merkle) What is the power law for the 6T vs. dose curve? Do you have any explanation for the fact that the observed behavior extends to such high damage doses?
Applications of Ion Beams to Metals by W. Buckel, B. Stritzker (auth.), S. T. Picraux, E. P. EerNisse, F. L. Vook (eds.)