Abstract
The common method of Rutherford backscattering and channeling of light energetic ions is in general not suited to lattice location studies of impurity atoms having a mass similar to or lower than the host. While specific nuclear reactions are sometimes available they usually require high beam doses and yield high backgrounds of scattered particles. In two such situations we have used ion induced x-ray yields to determine lattice location viz. for 32S and 31P implants in Ge single crystals. In the course of this work we have had to identify and optimize a number of experimental parameters, in particular how the beam type affects (a) ψ1/2,xmin and crystal damage rates, (b) x-ray yields (P-K, S-K, Ge-L and Ge-K), target bremsstrahlung and recoil-induced molecular x-ray intensities. Choice of detector geometry, aperture and window also proved to be important. Detection limits for P and S are now certainly better than 1 x 1014 atoms.cm-2 in a thick Ge target for 0.5 MeV proton excitation. We have found that a room temperature implant of 40 keV 31P annealed at 450oC is highly (93%) substitutional in Ge for a dose of 0.7 x 1015 ions.cm-2, but shows a much lower fraction at 2.7 x 1015 ions.cm. Lattice location of S implanted into Ge parallels the pattern from Group VI impurities implanted and annealed in Si, showing ≤ 50% xmin. values for the S signals in <110> and <111> directions. A different distribution for S is implied by <100> channeling data and <111> and <110> angular scans.
This is a condensed version of a longer two-part paper that has been submitted to the Journal of Applied Physics.
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References
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Chemin, J.F., Mitchell, I.V., Saris, F.W. (1973). Lattice Location of Low-Z Impurities in Medium-Z Targets Using Ion-Induced X-Rays. In: Crowder, B.L. (eds) Ion Implantation in Semiconductors and Other Materials. The IBM Research Symposia Series. Springer, Boston, MA. https://doi.org/10.1007/978-1-4684-2064-7_26
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DOI: https://doi.org/10.1007/978-1-4684-2064-7_26
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